PTL NANO ||Quantum Dot Source-Drain Transport Response at Microwave Frequencies PTL NANO HOME JOURNALS PRICING AND PLANS SUBMIT Locked Heading 4 Submitted - 06 November 2022 Reviewed - 02 February 2023 Accepted - 20 March 2023 Sunday, March 26, 2023 at 6:30:00 AM UTC I'm a paragraph. Click here to add your own text and edit me. It's easy. Apply Now Heading 6 Heading 6 BACK TO TOP Quantum Dot Source-Drain Transport Response at Microwave Frequencies Harald Havir,1 Subhomoy Haldar,1 Waqar Khan,1 Sebastian Lehmann,1 Kimberly A. Dick, 1, 2 Claes Thelander,1 Peter Samuelsson,3 Ville F. Maisi1 PTL NANO "Acknolowdgement NA" Keyword Highlighted quantum, quantum technologies, centre for quantum technologies, quantum computer (literature subject) Unlock Only Read-only this publication This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. 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Unlock us Quick View Newly listed Tphysletters A Unifying Bag Model of Composite Fermionic Structures in a Cold Genesis Theory Regular Price $700.00 Sale Price $400.00 Excluding Sales Tax Quick View TphysicsLetters Detection of the large-scale tidal field with galaxy multiplet alignment in the Regular Price $1,900.00 Sale Price $950.00 Excluding Sales Tax Quick View Newly listed Tphysletters Violation of γ in Brans-Dicke gravity Regular Price $1,000.00 Sale Price $600.00 Excluding Sales Tax Quick View Astrophysics Observations and detectability of young Suns’ flaring and CME activity in optica Regular Price $1,000.00 Sale Price $450.00 Excluding Sales Tax Quick View TphysicsLetters Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S Regular Price $2,000.00 Sale Price $400.00 Excluding Sales Tax Quick View New Thphysletters Bayesian and frequentist investigation of prior effects in EFTofLSS analyses of Regular Price $3,000.00 Sale Price $370.00 Excluding Sales Tax Quick View New Thphysletters A search for faint resolved galaxies beyond the Milky Way in DES Year 6: A new f Regular Price $1,900.00 Sale Price $750.00 Excluding Sales Tax Quick View New X-ray polarization properties of partially ionized equatorial obscurers around a Regular Price $800.00 Sale Price $350.00 Excluding Sales Tax Quick View New Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Regular Price $1,200.00 Sale Price $400.00 Excluding Sales Tax Quick View New SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural N Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View New Rapid neutron star cooling triggered by accumulated dark matter Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View Newly listed Tphysletters Searching for Radio Outflows from M31* with VLBI Observations Price $300.00 Excluding Sales Tax Load More Abstract Quantum dots are frequently used as charge sensitive devices in low temperature experiments to probe electric charge in mesoscopic conductors where the current running through the quantum dot is modulated by the nearby charge environment. Recent experiments have been operating these detectors using reflectometry measurements up to GHz frequencies rather than probing the low frequency current through the dot. In this work, we use an on-chip coplanar waveguide resonator to measure the source-drain transport response of two quantum dots at a frequency of 6 GHz, further increasing the bandwidth limit for charge detection. Similar to the low frequency domain, the response is here predominantly dissipative. For large tunnel coupling, the response is still governed by the low frequency conductance, in line with Landauer-Büttiker theory. For smaller couplings, our devices showcase two regimes where the high frequency response deviates from the low frequency limit and Landauer-Büttiker theory: When the photon energy exceeds the quantum dot resonance linewidth, degeneracy dependent plateaus emerge. These are reproduced by sequential tunneling calculations. In the other case with large asymmetry in the tunnel couplings, the high frequency response is two orders of magnitude larger than the low frequency conductance G, favoring the high frequency readout. Inroduction The ability to detect single electrons in the solid state is useful for a variety of applications, including spin qubit readout [1–4], electrical current and capacitance standards [5, 6], studying cooper pair breaking [7–9], single-shot photodetection [10–13], and nanothermodynamics and fluctuations [14– 19]. While many methods exist to detect charge, one of the main ways are by utilizing quantum dots (QD). These systems make excellent charge detectors due to their high sensitivity and well-established transport theory [20, 21], allowing detectors to be made predictable and with a well-understood operation principle. Originally, measurements were performed at DC, relying on a difference in current for the readout resulting in a bandwidth up to some kHz [6, 22]. In the last two decades, the readout methods have moved towards measuring the reflected power in a high-frequency tank circuit with resonant frequency in the 100 MHz - 1 GHz range. This results in bandwidths in the MHz range allowing for µs time resolution [23–25]. The response of the system in these studies is still governed by the low frequency response of the system, i.e. the admittance Y(ω) is equal to the DC conductance G of the system. In this article, we increase the QD sensor frequency to the 4 - 8 GHz frequency range where the cavity photon energy h¯ω is greater than the thermal energy kT [26]. This opens up the avenue to increase the bandwidth correspondingly by an order of magnitude, yielding possibly a time resolution sufficient to probe the electron position in DQD systems within the recently achieved coherence times [27, 28]. The pioneering works have considered the dispersive response of the QD at these frequencies motivated mostly by quantum capacitance effects [29]. In this article, we focus on the dissipative part that yields a stronger response, making it useful for charge readout [26]. We present experimental results for two devices and show that for both of them at sufficiently large tunnel couplings that we are lifetime broadened, Γ > kT, the low frequency result of Y(ω) = G still applies. However, when the device is tuned to the thermally broadened limit where the tunnel couplings Γ < kT, the measured admittance is qualitatively different from the DC conductance, displaying a linewidth of 2h¯ω in the QD level tuning and a factor two difference in admittance depending on the direction of the level shift of the quantum dot relative to the leads ε, attributed to spin degeneracy. These results are well captured by sequential tunneling theory, directly evaluating the admittance for a QD subjected to a time-periodic drive [30], or using P(E) theory in which the admittance is inferred from the absorption in the cavity [31, 32]. Lastly, we show in the other device which exhibits asymmetric tunnel couplings where the DC transport is suppressed while remaining lifetime broadened, the AC response in this device remains large, in line with Ref. 26, indicating a potentially useful consequence of probing QD devices at high frequencies. This response falls in a regime where neither non-interacting scattering theory nor sequential tunneling models are applicable. Conclusion In summary, we studied the high frequency source-drain response of a quantum dot. We showed experimentally that the low frequency result of Y(ω) = G holds for quantum dots tuned to sufficiently large tunnel couplings in line with the slow-drive limit. However, when the tunnel couplings are tuned to be smaller than the photon energy, the measured linewidth of the admittance Y(ω) is set by the photon energy. This response is well-described by sequential tunneling theory. Additionally, the low-frequency limit does not hold when the drive amplitude is made sufficiently large or with large asymmetry in tunnel couplings of the junctions. For the highly asymmetric case, it is also shown that the admittance Y(ω) can be orders of magnitude larger than the conductance G, indicating a potential benefit of measuring at high frequencies, as the readout strength remains large even for weakly conducting dots. References [1] B. E. Kane, Nature 393, 133 (1998). [2] D. Loss and D. P. DiVincenzo, Phys. Rev. A 57, 120 (1998). [3] L. M. K. Vandersypen, H. Bluhm, J. S. Clarke, A. S. Dzurak, R. Ishihara, A. Morello, D. J. Reilly, L. R. Schreiber, and M. Veldhorst, npj Quantum Information 3, 34 (2017). [4] R. Hanson, L. P. Kouwenhoven, J. R. Petta, S. Tarucha, and L. M. K. Vandersypen, Rev. Mod. Phys. 79, 1217 (2007). [5] M. W. Keller, A. L. Eichenberger, J. M. Martinis, and N. M. Zimmerman, Science 285, 1706 (1999), https://www.science.org/doi/pdf/10.1126/science.285.5434.1706 . [6] J. P. Pekola, O.-P. Saira, V. F. Maisi, A. Kemppinen, M. Möttönen, Y. A. Pashkin, and D. V. Averin, Rev. Mod. Phys. 85, 1421 (2013). [7] D. J. van Woerkom, A. Geresdi, and L. P. Kouwenhoven, Nature Physics 11, 547 (2015). [8] E. T. Mannila, P. Samuelsson, S. Simbierowicz, J. T. Peltonen, V. Vesterinen, L. Grönberg, J. Hassel, V. F. Maisi, and J. P. Pekola, Nature Physics 18, 145 (2022). [9] A. Ranni, F. Brange, E. T. Mannila, C. Flindt, and V. F. Maisi, Nature Communications 12, 6358 (2021). [10] S. Gustavsson, M. Studer, R. Leturcq, T. Ihn, K. Ensslin, D. C. Driscoll, and A. C. Gossard, Phys. Rev. Lett. 99, 206804 (2007). [11] A. Ghirri, S. Cornia, and M. Affronte, Sensors 20 (2020), 10.3390/s20144010. [12] W. Khan, P. P. Potts, S. Lehmann, C. Thelander, K. A. Dick, P. Samuelsson, and V. F. Maisi, Nature Communications 12, 5130 (2021). [13] S. Cornia, V. Demontis, V. Zannier, L. Sorba, A. Ghirri, F. Rossella, and M. Affronte, Advanced Functional Materials n/a, 2212517, https://onlinelibrary.wiley.com/doi/pdf/10.1002/adfm.202212517 . [14] J. V. Koski, V. F. Maisi, J. P. Pekola, and D. V. Averin, PNAS 111, 13786 (2014). [15] J. V. Koski, V. F. Maisi, T. Sagawa, and J. P. Pekola, Phys. Rev. Lett. 113, 030601 (2014). [16] D. Barker, M. Scandi, S. Lehmann, C. Thelander, K. A. Dick, M. Perarnau-Llobet, and V. F. Maisi, Phys. Rev. Lett. 128, 040602 (2022). [17] R. Garreis, J. D. Gerber, V. Stará, C. Tong, C. Gold, M. Röösli, K. Watanabe, T. Taniguchi, K. Ensslin, T. Ihn, and A. Kurzmann, Phys. Rev. Res. 5, 013042 (2023). [18] B. Küng, C. Rössler, M. Beck, M. Marthaler, D. S. Golubev, Y. Utsumi, T. Ihn, and K. Ensslin, Phys. Rev. X 2, 011001 (2012). [19] G. Manzano, D. Subero, O. Maillet, R. Fazio, J. P. Pekola, and E. Roldán, Phys. Rev. Lett. 126, 080603 (2021). [20] T. Ihn, “Semiconductor nanostructures: Quantum states and electronic transport,” (2009). [21] J. H. Davies, The Physics of Low-Dimensional Semiconductors - An Introduction (2006). [22] P. Lafarge, P. Joyez, D. Esteve, C. Urbina, and M. H. Devoret, Phys. Rev. Lett. 70, 994 (1993). [23] R. J. Schoelkopf, P. Wahlgren, A. A. Kozhevnikov, P. Delsing, and D. E. Prober, Science 280, 1238 (1998), https://www.science.org/doi/pdf/10.1126/science.280.5367.1238 . [24] E. J. Connors, J. Nelson, and J. M. Nichol, Phys. Rev. Appl. 13, 024019 (2020). [25] Y.-Y. Liu, S. Philips, L. Orona, N. Samkharadze, T. McJunkin, E. MacQuarrie, M. Eriksson, L. Vandersypen, and A. Yacoby, Phys. Rev. Appl. 16, 014057 (2021). [26] Y. Li, S.-X. Li, F. Gao, H.-O. Li, G. Xu, K. Wang, H. Liu, G. Cao, M. Xiao, T. Wang, J.-J. Zhang, and G.-P. Guo, J. of Appl. Phys. 123, 174305 (2018). [27] X. Mi, J. V. Cady, D. M. Zajac, P. W. Deelman, and J. R. Petta, Science 355, 156 (2017), https://www.science.org/doi/pdf/10.1126/science.aal2469 . [28] A. Stockklauser, P. Scarlino, J. V. Koski, S. Gasparinetti, C. K. Andersen, C. Reichl, W. Wegscheider, T. Ihn, K. Ensslin, and 6 A. Wallraff, Phys. Rev. X 7, 011030 (2017). [29] T. Frey, P. J. Leek, M. Beck, J. Faist, A. Wallraff, K. Ensslin, T. Ihn, and M. Büttiker, Phys. Rev. B 86, 115303 (2012). [30] C. Bruder and H. Schoeller, Phys. Rev. Lett. 72, 1076 (1994). [31] G.-L. Ingold and Y. V. Nazarov, “Charge tunneling rates in ultrasmall junctions,” in Single Charge Tunneling: Coulomb Blockade Phenomena In Nanostructures, edited by H. Grabert and M. H. Devoret (Springer US, Boston, MA, 1992) pp. 21– 107. [32] J.-R. Souquet, M. J. Woolley, J. Gabelli, P. Simon, and A. A. Clerk, Nature Communications 5, 5562 (2014). [33] M. Göppl, A. Fragner, M. Baur, R. Bianchetti, S. Filipp, J. M. Fink, P. J. Leek, G. Puebla, L. Steffen, and A. Wallraff, Journal of Applied Physics 104, 113904 (2008), https://doi.org/10.1063/1.3010859 . [34] K. A. Dick, J. Bolinsson, M. E. Messing, S. Lehmann, J. Johansson, and P. Caroff, Journal of Vacuum Science & Technology B 29, 04D103 (2011), https://doi.org/10.1116/1.3593457 . [35] I.-J. Chen, S. Lehmann, M. Nilsson, P. Kivisaari, H. Linke, K. A. Dick, and C. Thelander, Nano Letters 17, 902 (2017). [36] M. Nilsson, L. Namazi, S. Lehmann, M. Leijnse, K. A. Dick, and C. Thelander, Phys. Rev. B 93, 195422 (2016). [37] D. Barker, S. Lehmann, L. Namazi, M. Nilsson, C. Thelander, K. A. Dick, and V. F. Maisi, Applied Physics Letters 114, 183502 (2019), https://doi.org/10.1063/1.5089275 . [38] R. Wang, R. S. Deacon, D. Car, E. P. A. M. Bakkers, and K. Ishibashi, Applied Physics Letters 108, 203502 (2016), https://doi.org/10.1063/1.4950764 . [39] Prêtre, Thomas, and Büttiker, Physical review. B, Condensed matter 54 11, 8130 (1996). [40] L. P. Kouwenhoven, S. Jauhar, J. Orenstein, P. L. McEuen, Y. Nagamune, J. Motohisa, and H. Sakaki, Phys. Rev. Lett. 73, 3443 (1994). [41] S. Cornia, F. Rossella, V. Demontis, V. Zannier, F. Beltram, L. Sorba, M. Affronte, and A. Ghirri, Scientific Reports 9 (2019). [42] T. Frey, P. J. Leek, M. Beck, K. Ensslin, A. Wallraff, and T. Ihn, Applied Physics Letters 98, 262105 (2011), https://doi.org/10.1063/1.3604784 . [43] J. M. Sage, V. Bolkhovsky, W. D. Oliver, B. Turek, and P. B. Welander, Journal of Applied Physics 109, 063915 (2011), https://doi.org/10.1063/1.3552890 . [44] S. Haldar, H. Havir, W. Khan, S. Lehmann, C. Thelander, K. A. Dick, and V. F. Maisi, Phys. Rev. Lett. 130, 087003 (2023). [45] S. J. Chorley, J. Wabnig, Z. V. Penfold-Fitch, K. D. Petersson, J. Frake, C. G. Smith, and M. R. Buitelaar, Phys. Rev. Lett. 108, 036802 (2012). [46] M. Ridley, N. W. Talarico, D. Karlsson, N. L. Gullo, and R. Tuovinen, Journal of Physics A: Mathematical and Theoretical 55, 273001 (2022). [47] A. Hofmann, V. F. Maisi, C. Gold, T. Krähenmann, C. Rössler, J. Basset, P. Märki, C. Reichl, W. Wegscheider, K. Ensslin, and T. Ihn, Phys. Rev. Lett. 117, 206803 (2016). [48] T. Ihn, “Semiconductor nanostructures,” (Oxford University Press, New York, 2010). [49] V. F. Maisi, “Andreev tunneling and quasiparticle excitations in mesoscopic normal metal - superconductor structures,” (PhD thesis, Aalto University, 2014) pp. 21 – 107. [50] S. M. Girvin, in Quantum Machines: Measurement and Control of Engineered Quantum Systems: Lecture Notes of the Les Houches Summer School: Volume 96, July 2011 (Oxford University Press, 2014). [51] L. Childress, A. S. Sørensen, and M. D. Lukin, Phys. Rev. A 69, 042302 (2004). [52] C. Altimiras, O. Parlavecchio, P. Joyez, D. Vion, P. Roche, D. Esteve, and F. Portier, Phys. Rev. Lett. 112, 236803 (2014).

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Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT Locked Tphysicsletters/6981/11/1490/3728tpl/Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S, Se, Te) electrocatalysts via hydrothermal methods: insight into optimizing the electrocatalytic performance for hydrogen generation Citation (0) Sunday, February 25, 2024 at 6:30:00 AM UTC Request Open Apply Now Article Rating by Publisher 8 T. Physics Article Rating by Readers 10 https://doi.wikipt.org/11/1490/3728tpl Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S, Se, Te) electrocatalysts via hydrothermal methods: insight into optimizing the electrocatalytic performance for hydrogen generation Zhexu Xi Theoretical Physics Letters 2024 ° 25(02) ° 0690-3728 www.wikipt.org TphysicsLetters Physics Tomorrow Theoretical Physics Letters publications TOA Abstract Introduction Conclusion ACKNOWLEDGMENTS Not Applicable. Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters Abstract Hydrogen Evolution Reaction (HER) has always gained wide attention as one of the eco-friendly and sustainable pathways for efficient hydrogen generation and storage; also, two-dimensional molybdenum dichalcogenide (MoX2, where X stands for S, Se, Te) layers have emerged as a class of quasi-ideal electrocatalysts because of their large surface area, rich reserves and outstanding conductivity. However, besides greater HER activity, the maturity and diversity of modification strategies result in a more puzzling relationship between electrocatalytic mechanisms and the corresponding practical performance. In this article, based on a comprehensive review of fundamentals, principles and interconnected similarities of the MoX2 family, we focus on the structure-activity correlation of layered MoX2 for HER enhancement via hydrothermal synthesis. This method is summarized from different experimental systems to efficiently modulate the crystal structure and surface for boosted HER activity. Here, with the adjustment of three key experimental parameters: the categories of MoX2, reaction temperature and the molar amount of added reactants, the optimum HER performance can be obtained at the best conditions (MoSe2 species, 180℃ and a vast ratio of the reductant or metal precursor), and more microscopically, a controlled structure-activity relationship can be inducted. This summary may pave a new path for the controllable synthesis and modification of MoX2-based catalyst materials. Introduction As the environmental pollution and energy crisis become increasingly severe, hydrogen, owing to its tiptop energy density, renewability, high purity and zero-polluting combustion byproduct (water), has received greater attention as an ideal energy carrier to reduce the dependence on traditional fossil energy [1-3]. Over various hydrogen generation pathways (in Fig. 1), water splitting via electrochemical approaches has been regarded as a low-cost, eco-friendly and sustainable industrial pathway for high-efficiency hydrogen conversion and storage[4,5]. So far, numerous experimental studies about high-speed and efficient hydrogen evolution have been gradually categorized into two classes: 1) identifying HER mechanisms in pursuit of more strategies for accelerating HER reaction rates, especially at a wide range of pH containing neutral and alkaline electrolyte environments (theoretically) [6-12]; 2) the discovery and design of new kinds of durable and high-activity HER electrocatalysts (experimentally) [13-18]. Considering the class 1), the key to understanding the HER mechanism is to explore the inherent relationship between the microscopic viewpoint of intermediate adsorbed states (including intermediate species and the triggered activation and adsorption energy change) and the macroscopic reaction rates [19]. Although the perplexing principle of the HER process in different pH conditions (mainly referring to acidic, neutral and alkaline conditions) is still under heated debate, especially considering which factor plays a predominant role including the source of proton donors[6,7], the interfacial H*-M (hydrogen-metal) band intensity with the changed activation barriers[8,9], the availability of surface sites and electron trapping states[10], Hupd[11], pzfc (the potential of zero free charge) with the changed reorganizational energy[12], there is a common consensus based on the competing relationship between the extra water dissociation and activation step and the hydrogen adsorption/desorption step. Specifically, from the perspective of catalyst design, several feasible strategies should be implemented to accomplish two goals (as Fig.2 depicts[20]): improving the reaction thermodynamics by lessening the activation barrier from dissociated water molecules (e.g. creating more oxophilic sites); promoting the reaction kinetics by tuning the H*-M interactions (e.g. modulating the electronic structures)[20,21]. Accordingly, no matter what the respective value of two goals are in HER, more micro-to-macro relationship can be established between the HER-related principles and the apparent HER activity by taking theoretically well-defined surface structures and electronic band levels of a certain electrocatalyst into account. Another class of research entails the real-world design of a certain kind of high-activity electrocatalysts. Although noble metals with their compounds, especially platinum (Pt), exhibit the optimum HER activity according to the Sabatier principles[22], their rare reserves and exorbitant prices largely restricts the large-scale hydrogen production. With a comparably low overpotential, a low Tafel slope and a moderate ΔGH* (not too big or too small) to Pt, various materials have adequate potentialities to replace the Pt-based HER catalysts, including chalcogenides[13,14], oxides[15], phosphides[16], nitrides[17] and carbides[18] ranging from bulk to nanoscale. Fully considering important structural or physical properties like surface area, crystallinity, porosity, thickness, electron conductivity and layered assemblies, molybdenum dichalcogenides (MoX2) have superior activity and long-term durability to defeat other structured catalyst materials[23-26]. Accordingly, the suitable choice of MoX2 help govern and regulate the apparent reactivity and kinetics of HER by designing a practically high-performance electrocatalyst with controlled surfaces and morphologies from a theoretically well-defined catalyst surface based on the HER principles. Consequently, our work aims to provide a comprehensive structure-activity analysis of MoX2-based electrocatalysts to present a clear mapping between the sluggish-rate-related HER energetics of two intermediate thermodynamic states (produced by two competing steps: the extra water dissociation step and hydrogen adsorption with interfacial H*-M interactions, as shown in Fig. 3 (b)[27,28]) and the practical design of a high-activity electrocatalyst. Based on the aforementioned correlations among hydrogen generation and two classes of viewpoints (simplified in ........... Purchase to read more. Conclusion The low concentration of proton donors in alkaline HER, subsequently leading to the extra water adsorption and dissociation steps, identifies the value of active sites (edge and basal sites) and crystal phases in lowering the extra activation barrier and/or optimizing the H* adsorption kinetics; in addition, the outstanding morphology-based features (surface area, thickness, defects, disorders and crystallinity) of layered molybdenum dichalcogenide families pinpoint the roles of active sites and phases for more interpretable and feasible structure-activity analysis. In this context, hydrothermal synthetic method is used to exhibit a clear mapping between the nanostructure/nanosurface design and the practical HER performance by adjusting key experimental parameters. In this article, MoX2 nanostructures in different species (X = S, Se, Te), the molar ratio of added reactants (the Se metal precursor and the NaBH4 reducing agency) and hydrothermal temperature are considered for the modulated structure and the optimized HER performance. The tunability of the hydrothermal method can be well confirmed with regard to its structure-activity relationship and the underlying mechanism. A system of MoX2-based samples delivery their excellent HER activity, stability and kinetics, with the optimal value of overpotential η, exchange current density j0, Tafel slope b and charge transfer resistance Rct, which are well tuned by these parameters above. For better comprehensions of the parameter-tunable structure-activity correlations, the role of active sites and phases are crucially highlighted. In detail, different chalcogenide species are indicative of different exposure of surface defects as active sites on nanoscale; the concentration of the added precursor/reductant determines the specific content of metallic 1T/1T’ phase by inducing a 2H-to-1T(1T’) conversion; hydrothermal temperatures regulates the phase and defect structure simultaneously by generating a controlled core/shell-like structure with mixed phases. Furthermore, the tunable procedures contribute to more revelation in the weigh of the roles of structural factors (edge sites, bulk conductivity for in-plane activation and phases). The crystal phase plays the predominant role as the phase transition also results in the altered densities of active sites and intrinsic activity of basal plane. To conclude, with higher tunability and scalability, the hydrothermal method can pave a novel path for the oriented, rational design of higher-activity transition-metal-based electrocatalysts and better understandings of the underlying design rules and mechanisms. TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow [1] Zheng, Y.; Jiao, Y.; Jaroniec, M.; Qiao, S. Advancing the Electrochemistry of the Hydrogen Evolution Reaction through Combining Experiment and Theory. Angew. Chem. Int. Ed. 2015, 54, 52-65. [1] Liu, Y.; Wu, J.; Hackenberg, K. P.; Zhang, J.; Wang, Y. M.; Yang, Y.; Keyshar, K.; Gu, J.; Ogitsu, T.; Vajtai, R. Self-Optimizing, Highly Surface-Active Layered Metal Dichalcogenide Catalysts for Hydrogen Evolution. Nat. Energy 2017, 2, 17127. [2] Jaramillo, T. F.; Jørgensen, K. P.; Bonde, J.; Nielsen, J. H.; Horch, S.; Chorkendorff, I. Identification of Active Edge Sites for Electrochemical H2 Evolution from MoS2 Nanocatalysts. Science 2007, 317, 100-102. [3] Gillis, R. J.; Al-Ali, K.; Green, W. H. Thermochemical Production of Hydrogen from Hydrogen Sulfide with Iodine Thermochemical Cycles. Int. J. Hydrog. Energy 2018, 43, 12939-12947. [4] Zou, X.; Zhang, Y. Noble Metal-Free Hydrogen Evolution Catalysts for Water Splitting. Chem. Soc. Rev. 2015, 44, 5148-5180. [5] Tarasevich, M. R.; Korchagin, O. V. Electrocatalysis and pH (a Review). Russ. J. Electrochem. 2013, 49, 600-618. [6] Auinger, M.; Katsounaros, I.; Meier, J. C.; Klemm S. O.; Biedermann, P. U.; Topalov, A. A.; Rohwerdera, M.; Mayrhofer, K. J. Near-Surface Ion Distribution and Buffer Effects During Electrochemical Reactions. Phys. Chem. Chem. Phys. 2011, 13, 16384-16394. [7] Strmcnik, D.; Uchimura, M.; Wang, C.; Subbaraman, R.; Danilovic, N.; Van Der Vliet, D.; Paulikas, A. P.; Stamenkovic, V. R.; Markovic, N. M. Improving the Hydrogen Oxidation Reaction Rate by Promotion of Hydroxyl Adsorption. Nature Chem. 2013, 5, 300-306. [8] Zhu, S.; Qin, X.; Yao, Y.; Shao, M. pH-Dependent Hydrogen and Water Binding Energies on Platinum Surfaces as Directly Probed through Surface-Enhanced Infrared Absorption Spectroscopy. J. Am. Chem. Soc. 2020, 142, 8748-8754. [9] Danilovic, N.; Subbaraman, R.; Strmcnik, D.; Chang, K. -C.; Paulikas, A. P.; Stamenkovic, V. R.; Markovic, N. M. Enhancing the Alkaline Hydrogen Evolution Reaction Activity through the Bifunctionality of Ni(OH)2/Metal Catalysts. Angew. Chem. Int. Ed. 2012, 51, 12495-12498. [10] Cheng, T.; Wang, L.; Merinov, B. V.; Goddard III, W. A. Explanation of Dramatic pH-Dependence of Hydrogen Binding on Noble Metal Electrode: Greatly Weakened Water Adsorption at High pH. J. Am. Chem. Soc. 2018, 140, 7787-7790. [11] Yang, X.; Nash, J.; Oliveira, N.; Yan, Y.; Xu, B. Understanding the pH Dependence of Underpotential Deposited Hydrogen on Platinum. Angew. Chem. Int. Ed. 2019, 58, 17718-17723. [12] Wang, R.; Yan, J.; Zu, M.; Yang, S.; Cai, X.; Gao, Q.; Fang, Y.; Zhang, S. Facile Synthesis of Interlocking g-C3N4/CdS Photoanode for Stable Photoelectrochemical Hydrogen Production. Electrochim. Acta 2018, 279, 74-83. [13] Shi, X.; Fields, M.; Park, J.; McEnaney, J. M.; Yan, H.; Zhang, Y.; Tsai, C.; Jaramillo, T. F.; Sinclair, R.; Norskov, J. K.; Zheng, X. Rapid Flame Doping of Co to WS2 for Efficient Hydrogen Evolution. Energy Environ. Sci. 2018, 11, 2270-2277. [14] Wang, L.; Tsang, C.; Liu, W.; Zhang, X.; Zhang, K.; Ha, E.; Kwok, W. M.; Park, J. H.; Lee, L. Y. S.; Wong, K. Y. Disordered Layers on WO3 Nanoparticles Enable Photochemical Generation of Hydrogen from Water. J. Mater. Chem. A 2019, 7, 221-227. [15] Kanda, Y.; Kawanishi, K.; Tsujino, T.; Al-otaibi, A.; Uemichi, Y. Catalytic Activities of Noble Metal Phosphides for Hydrogenation and Hydrodesulfurization Reactions. Catalysts 2018, 8, 160. [16] Miao, J.; Lang, Z.; Zhang, X.; Kong, W.; Peng, O.; Yang, Y.; Wang, S.; Cheng, J.; He, T.; Amini, A.; Wu, Q.; Zheng, Z.; Tang, Z.; Cheng, C. Polyoxometalate-Derived Hexagonal Molybdenum Nitrides (MXenes) Supported by Boron, Nitrogen Codoped Carbon Nanotubes for Efficient Electrochemical Hydrogen Evolution from Seawater. Adv. Funct. Mater. 2019, 29, 1970046. [17] Kou, Z.; Wang, T.; Wu, H.; Zheng, L.; Mu, S.; Pan, Z.; Lyu, Z.; Zang, W.; Pennycook, S. J.; Wang, J. Twinned Tungsten Carbonitride Nanocrystals Boost Hydrogen Evolution Activity and Stability. Small 2019, 15, 1900248. [18] Wang, X.; Zheng, Y.; Sheng, W.; Xu, Z. J.; Jaroniec, M.; Qiao, S. Z. Strategies for Design of Electrocatalysts for Hydrogen Evolution under Alkaline Conditions. Mater. Today 2020, 36, 125-138. [19] Jiao, Y.; Zheng, Y.; Davey, K.; Qiao, S. Z. Activity Origin and Catalyst Design Principles for Electrocatalytic Hydrogen Evolution on Heteroatom-Doped Graphene. Nat. Energy 2016, 1, 16130. [20] Skúlason, E.; Jónsson, H. Atomic Scale Simulations of Heterogeneous Electrocatalysis: Recent Advances. Adv. Phys. 2017, 2, 481-495. [21] Parsons, R. The Rate of Electrolytic Hydrogen Evolution and the Heat of Adsorption of Hydrogen. Trans. Faraday Soc. 1958, 54, 1053-1063. [22] Wang, R.; Han, J.; Zhang, X.; Song, B. Synergistic Modulation in MX2 (where M = Mo or W or V, and X = S or Se) for an Enhanced Hydrogen Evolution Reaction. J. Mater. Chem. A 2018, 6, 21847-21858. [23] Deng, S.; Yang, F.; Zhang, Q.; Zhong, Y.; Zeng, Y.; Lin, S.; Wang, X.; Lu, X.; Wang, C.-Z.; Gu, L.; Xia, X.; Tu, J. Phase Modulation of (1T-2H)-MoSe2/TiC-C Shell/Core Arrays via Nitrogen Doping for Highly Efficient Hydrogen Evolution Reaction. Adv. Mater. 2018, 30, 1802223. [24] Vikraman, D.; Akbar, K.; Hussain, S.; Yoo, G.; Jang, J.-Y.; Chun, S.-H.; Jung, J.; Park, H. J. Direct Synthesis of Thickness-Tunable MoS2 Quantum Dot Thin Layers: Optical, Structural and Electrical Properties and Their Application to Hydrogen Evolution. Nano Energy 2017, 35, 101-114. [25] Guo, W.; Chen, Y.; Wang, L.; Xu, J.; Zeng, D.; Peng, D. -L. Colloidal Synthesis of MoSe2 Nanonetworks and Nanoflowers with Efficient Electrocatalytic Hydrogen-Evolution Activity. Electrochim. Acta 2017, 231, 69-76. [26] Wei, J.; Zhou, M.; Long, A.; Xue, Y.; Liao, H.; Wei, C.; Xu, Z. J. Heterostructured Electrocatalysts for Hydrogen Evolution Reaction Under Alkaline Conditions. Nano-Micro Lett. 2018, 10, 75. [27] Zheng, Y.; Jiao, Y.; Zhu, Y.; Li, L. H.; Han, Y.; Chen, Y.; Jaroniec, M.; Qiao, S. Z. High Electrocatalytic Hydrogen Evolution Activity of an Anomalous Ruthenium Catalyst. J. Am. Chem. Soc. 2016, 138, 16174-16181. [28] Zhang, B.; Liu, J.; Wang, J.; Ruan, Y.; Ji, X.; Xu, K.; Chen, C.; Wan, H.; Miao, L.; Jiang, J. Interface Engineering: the Ni(OH)2/MoS2 Heterostructure for Highly Efficient Alkaline Hydrogen Evolution. Nano Energy 2017, 37, 74-80. [29] Zhen, C.; Zhang, B.; Zhou, Y.; Du, Y.; Xu, P. Hydrothermal Synthesis of Ternary MoS2xSe2(1-x) Nanosheets for Electrocatalytic Hydrogen Evolution. Inorg. Chem. Front. 2018, 5, 1386-1390. [30] Gao, M.; Xu, Y.; Jiang, J.; Yu, S. Nanostructured Metal Chalcogenides: Synthesis, Modification, and Applications in Energy Conversion and Storage Devices. Chem. Soc. Rev. 2013, 42, 2986-3017. [31] Liu, Z.; Gao, Z.; Liu, Y.; Xia, M.; Wang, R.; Li, N. Heterogeneous Nanostructure Based on 1T-Phase MoS2 for Enhanced Electrocatalytic Hydrogen Evolution. ACS Appl. Mater. Interfaces 2017, 9, 25291-25297. [32] Fu, Q.; Han, J.; Wang, X.; Xu, P.; Yao, T.; Zhong, J.; Zhong, W.; Liu, S.; Gao, T.; Zhang, Z.; Xu, L.; Song, B. 2D Transition Metal Dichalcogenides: Design, Modulation, and Challenges in Electrocatalysis. Adv. Mater. 2021, 33, 1907818. [33] Strmcnik, D.; Lopes, P. P.; Genorio, B.; Stamenkovic, V. R.; Markovic, N. M. Design Principles for Hydrogen Evolution Reaction Catalyst Materials. Nano Energy 2016, 29, 29-36. [34] Durst, J.; Siebel, A.; Simon, C.; Hasche, F.; Herranz, J.; Gasteiger, H. A. New Insights into the Electrochemical Hydrogen Oxidation and Evolution Reaction Mechanism. Energy Environ. Sci. 2014, 7, 2255-2260. [35] Wei, C.; Sun, Y.; Scherer, G. G.; Fisher, A. C.; Sherburne, M.; Ager, J. W.; Xu, Z. J. Surface Composition Dependent Ligand Effect in Tuning the Activity of Nickel-Copper Bimetallic Electrocatalysts toward Hydrogen Evolution in Alkaline. J. Am. Chem. Soc. 2020, 142, 7765-7775. [36] Wang, X.; Xu, C.; Jaroniec, M.; Zheng, Y.; Qiao, S. -Z. Anomalous Hydrogen Evolution Behavior in High-pH Environment Induced by Locally Generated Hydroniumions. Nat. Commun. 2019, 10, 4876. [37] Cheng, T.; Wang, L.; Merinov, B. V.; Goddard, W. A. Explanation of Dramatic pH-Dependence of Hydrogen Binding on Noble Metal Electrode: Greatly Weakened Water Adsorption at High pH. J. Am. Chem. Soc. 2018, 140, 7787-7790. [38] Ruqia, B.; Choi, S. I. Pt and Pt-Ni(OH)2 Electrodes for the Hydrogen Evolution Reaction in Alkaline Electrolytes and Their Nanoscaled Electrocatalysts. ChemSusChem 2018, 11, 2643-2653. [39] Feng, X. J.; Wu, J. Q.; Tong, Y. X.; Li, G. R. Efficient Hydrogen Evolution on Cu Nanodots-Decorated Ni3S2 Nanotubes by Optimizing Atomic Hydrogen Adsorption and Desorption. J. Am. Chem. Soc. 2018, 140, 610-617. [40] Voiry, D.; Yang, J.; Chhowalla, M. Recent Strategies for Improving the Catalytic Activity of 2D TMD Nanosheets toward the Hydrogen Evolution Reaction. Adv. Mater. 2016, 28, 6197-6206. [41] Gushchin, A. L.; Laricheva, Y. A.; Sokolov, M. N.; Llusar, R. Tri-and Tetranuclear Molybdenum and Tungsten Chalcogenide Clusters: on the Way to New Materials and Catalysts. Russ. Chem. Rev. 2018, 87, 670-706. [42] Zhong, W.; Xiao, B.; Lin, Z.; Wang, Z.; Huang, L.; Shen, S.; Zhang, Q.; Gu, L. RhSe2: a Superior 3D Electrocatalyst with Multiple Active Facets for Hydrogen Evolution Reaction in Both Acid and Alkaline Solutions. Adv. Mater. 2021, 33, 2007894. [43] McGlynn, J. C.; Cascallana-Matías, I.; Fraser, J. P.; Roger, I.; McAllister, J.; Miras, H. N.; Symes, M. D.; Ganin, A. Y. Molybdenum Ditelluride Rendered into an Efficient and Stable Electrocatalyst for the Hydrogen Evolution Reaction by Polymorphic Control. Energy Technol. 2018, 6, 345-350. [44] Bhat, K. S.; Nagaraja, H. S. Performance Evaluation of Molybdenum Dichalcogenide (MoX2; X = S, Se, Te) Nanostructures for Hydrogen Evolution Reaction. Int. J. Hydrog. Energy 2019, 44, 17878-17886. [45] Wang, H.; Yuan, H.; Hong, S. S.; Li, Y.; Cui, Y. Physical and Chemical Tuning of Two-Dimensional Transition Metal Dichalcogenides. Chem. Soc. Rev. 2015, 44, 2664-2680. [46] Hinnemann, B.; Moses, P. G.; Bonde, J.; Jørgensen, K. P.; Nielsen, J. H.; Horch, S.; Chorkendorff, I.; Nørskov, J. K. Biomimetic Hydrogen Evolution: MoS2 Nanoparticles as Catalyst for Hydrogen Evolution. J. Am. Chem. Soc. 2005, 127, 5308-5309. [47] Luo, Z.; Ouyang, Y.; Zhang, H.; Xiao, M.; Ge, J.; Jiang, Z.; Wang, J.; Tang, D.; Cao, X.; Liu, C.; Xing, W. Chemically Activating MoS2 via Spontaneous Atomic Palladium Interfacial Doping towards Efficient Hydrogen Evolution. Nat. Commun. 2018, 9, 2120. [48] (a) Yu, Y.; Huang, S. -Y.; Li, Y.; Steinmann, S. N.; Yang, W.; Cao, L. Layer-Dependent Electrocatalysis of MoS2 for Hydrogen Evolution. Nano Lett. 2014, 14, 553-558.; (b) Janik, J. M.; McCrum, I. T.; Koper, M. T. M. On the Presence of Surface Bound Hydroxyl Species on Polycrystalline Pt Electrodes in the “Hydrogen Potential Region” (0-0.4 V-RHE). J. Catal. 2018, 367, 332-337; (c) Qian, Z.; Jiao, L.; Xie, L. Phase Engineering of Two-Dimensional Transition Metal Dichalcogenides. Chin. J. Chem. 2020, 38, 753-760. [49] Khossossi, N.; Singh, D.; Ainane, A.; Ahuja, R. Recent Progress of Defect Chemistry on 2D Materials for Advanced Battery Anodes. Chem. Asian J. 2020, 15, 3390-3404. [50] Coleman, J. N.; Lotya, M.; O’Neill, A.; Bergin, S. D.; King, P. J.; Khan, U.; Young, K.; Gaucher, A.; De, S.; Smith, R. J.; Shvets, I. V.; Arora, S. K.; Stanton, G.; Kim, H. -Y.; Lee, K.; Kim, G. T.; Duesberg, G. S.; Hallam, T.; Boland, J. J.; Wang, J. J.; Donegan, J. F.; Grunlan, J. C.; Moriarty, G.; Shmeliov, A.; Nicholls, R. J.; Perkins, J. M.; Grieveson, E. M.; Theuwissen, K.; McComb, D. W.; Nellist, P. D.; Nicolosi, V. Two-Dimensional Nanosheets Produced by Liquid Exfoliation of Layered Materials. Science 2011, 331, 568. [51] Kong, D.; Wang, H.; Cha, J. J.; Pasta, M.; Koski, K. J.; Yao, J.; Cui, Y. Synthesis of MoS2 and MoSe2 Films with Vertically Aligned Layers. Nano Lett. 2013, 13, 1341-1347. [52] Lukowski, M. A.; Daniel, A. S.; Meng, F.; Forticaux, A.; Li, L. S.; Jin, S. Enhanced Hydrogen Evolution Catalysis from Chemically Exfoliated Metallic MoS2 Nanosheets. J. Am. Chem. Soc. 2013, 135, 10274-10277. [53] Vattikuti, S. P.; Devarayapalli, K. C.; Nagajyothi, P. C.; Shim, J. Microwave Synthesized Dry Leaf-Like Mesoporous MoSe2 Nanostructure as an Efficient Catalyst for Enhanced Hydrogen Evolution and Supercapacitor Applications. Microchem. J. 2020, 153, 104446. [54] Lei, Z.; Xu, S.; Wu, P. Ultra-Thin and Porous MoSe2 Nanosheets: Facile Preparation and Enhanced Electrocatalytic Activity towards the Hydrogen Evolution Reaction. Phys. Chem. Chem. Phys. 2016, 18, 70-74. [55] Jaramillo, T. F.; Jorgensen, K. P.; Bonde, J.; Nielsen, J. H.; Horch, S.; Chorkendorff, I. Identification of Active Edge Sites for Electrochemical H2 Evolution from MoS2 Nanocatalysts. Science 2007, 317, 100-102. [56] Nguyen, T. P.; Choi, S.; Jeon, J. M.; Kwon, K. C.; Jang, H. W.; Kim, S. Y. Transition Metal Disulfide Nanosheets Synthesized by Facile Sonication Method for the Hydrogen Evolution Reaction. J. Phys. Chem. C 2016, 120, 3929-3935. [57] Ambrosi, A.; Sofer, Z.; Pumera, M. Lithium Intercalation Compound Dramatically Influences the Electrochemical Properties of Exfoliated MoS2. Small 2015, 11, 605-612. [58] Attanayake, N. H.; Thenuwara, A. C.; Patra, A.; Aulin, Y. V.; Tran, T. M.; Chakraborty, H.; Borguet, E.; Klein, M. L.; Perdew, J. P.; Strongin, D. R. Effect of Intercalated Metals on the Electrocatalytic Activity of 1T-MoS2 for the Hydrogen Evolution Reaction. ACS Energy Lett. 2017, 3, 7-13. [59] Lin, S.; Kuo, J. Activating and Tuning Basal Planes of MoO2, MoS2, and MoSe2 for Hydrogen Evolution Reaction. Phys. Chem. Chem. Phys. 2015, 17, 29305-29310. [60] Ouyang, Y.; Ling, C.; Chen, Q.; Wang, Z.; Shi, L.; Wang, J. Activating Inert Basal Planes of MoS2 for Hydrogen Evolution Reaction through the Formation of Different Intrinsic Defects. Chem. Mater. 2016, 28, 4390-4396. [61] Vasu, K.; Meiron, O. E.; Enyashin, A. N.; Bar-Ziv, R.; Bar-Sadan, M. Effect of Ru Doping on the Properties of MoSe2 Nanoflowers. J. Phys. Chem. C 2019, 123, 1987-1994. [62] Voiry, D.; Mohiteb, A.; Chhowalla, M. Phase Engineering of Transition Metal Dichalcogenides. Chem. Soc. Rev. 2015, 44, 2702-2712. [63] Wang, Q. H.; Kalantar-Zadeh, K.; Kis, A.; Coleman, J. N.; Strano, M. S. Electronics and Optoelectronics of Two-Dimensional Transition Metal Dichalcogenides. Nat. Nanotechnol. 2012, 7, 699-712. [64] Lukowski, M. A.; Daniel, A. S.; Meng, F.; Forticaux, A.; Li, L.; Jin, S. Enhanced Hydrogen Evolution Catalysis from Chemically Exfoliated Metallic MoS2 Nanosheets. J. Am. Chem. Soc. 2013, 135, 10274-10277. [65] Wang, D.; Zhang, X.; Bao, S.; Zhang, Z.; Fei, H.; Wu, Z. Phase-Engineering of Multiphasic 1T/2H MoS2 Catalyst for Highly Efficient Hydrogen Evolution. J. Mater. Chem. A 2017, 5, 2681-2688. [66] Wang, H.; Wang, X.; Wang, L.; Wang, J.; Jiang, D.; Li, G.; Zhang, Y.; Zhong, H.; Jiang, Y. Phase Transition Mechanism and Electrochemical Properties of Nanocrystalline MoSe2 as Anode Materials for the High Performance Lithium-Ion Battery. J. Phys. Chem. C 2015, 119, 10197-10205. [67] Li, X.; Sun, M.; Cheng, S.; Ren, X.; Zang, J.; Xu, T.; Wei, X.; Li, S,; Chen, Q.; Shan, C. Crystallographic-Orientation Dependent Li Ion Migration and Reactions in Layered MoSe2. 2D Mater. 2019, 6, 035027. [68] Li, H.; Tsai, C.; Koh, A. L.; Cai, L.; Contryman, A. W.; Fragapane, A. H.; Zhao, J.; Han, H. S.; Manoharan, H. C.; Abild-Pedersen, F.; Nørskov, J. K.; Zheng, X. Activating and Optimizing MoS2 Basal Planes for Hydrogen Evolution through the Formation of Strained Sulphur Vacancies. Nat. Mater. 2016, 15, 48-53. [69] Duerloo, K. A. N.; Li, Y.; Reed, E. J. Structural Phase Transitions in Two-Dimensional Mo- and W- Dichalcogenide Monolayers. Nat. Ccommun. 2014, 5, 4214. [70] Lee, J.; Kim, C.; Choi, K.; Seo, J.; Choi, Y.; Choi, W.; Kim, Y. -M.; Jeong, H.; Lee, J. H.; Kim, G.; Park, H. In-situ Coalesced Vacancies on MoSe2 Mimicking Noble Metal: Unprecedented Tafel Reaction in Hydrogen Evolution. Nano Energy 2019, 63, 103846. [71] Tan, C.; Luo, Z.; Chaturvedi, A.; Cai, Y.; Du, Y.; Gong, Y.; Huang, Y.; Lai, Z.; Zhang, X.; Zheng, L.; Qi, X.; Goh, M. H.; Wang, J.; Han, S.; Wu, X. -J.; Gu, L.; Kloc, C.; Zhang, H. Preparation of High-Percentage 1T-Phase Transition Metal Dichalcogenide Nanodots for Electrochemical Hydrogen Evolution. Adv. Mater. 2018, 30, 1705509. [72] Cai, L.; Cheng, W.; Yao, T.; Huang, Y.; Tang, F.; Liu, Q.; Liu, W.; Sun, Z.; Hu, F.; Jiang, Y.; Yan, W; Wei, S. High Content Metallic 1T Phase in MoS2-Based Electrocatalyst for Efficient Hydrogen Evolution. J. Phys. Chem. C 2017, 121, 15071-15077. [73] He, Y.; Boubeche, M.; Zhou, Y.; Yan, D.; Zeng, L.; Wang, X.; Yan, K.; Luo, H. Topologically Nontrivial 1T’-MoTe2 as Highly Efficient Hydrogen Evolution Electrocatalyst. J. Phys. Mater. 2020, 4, 014001. [74] Chen, M.; Zhu, L.; Chen, Q.; Miao, N.; Si, C.; Zhou, J.; Sun, Z. Quantifying the Composition Dependency of the Ground-State Structure, Electronic Property and Phase-Transition Dynamics in Ternary Transition-Metal-Dichalcogenide Monolayers. J. Mater. Chem. C 2020, 8, 721-733. [75] Voiry, D.; Salehi, M.; Silva, R.; Fujita, T.; Chen, M.; Asefa, T.; Shenoy, V. B.; Eda, G.; Chhowalla, M. Conducting MoS2 Nanosheets as Catalysts for Hydrogen Evolution Reaction. Nano Lett. 2013, 13, 6222-6227. [76] Xie, J.; Qi, J.; Lei, F.; Xie, Y. Modulation of Electronic Structures in Two-Dimensional Electrocatalysts for the Hydrogen Evolution Reaction. Chem. Commun. 2020, 56, 11910-11930. [77] Xie, J.; Liu, W.; Zhang, X.; Guo, Y.; Gao, L.; Lei, F.; Tang, B.; Xie, Y. Constructing Hierarchical Wire-On-Sheet Nanoarrays in Phase-Regulated Cerium-Doped Nickel Hydroxide for Promoted Urea Electro-Oxidation. ACS Mater. Lett. 2019, 1, 103-110. [78] Hu, X.; Zhang, Q.; Yu, S. Theoretical Insight into the Hydrogen Adsorption on MoS2 (MoSe2) Monolayer as a Function of Biaxial Strain/External Electric Field. Appl. Surf. Sci. 2019, 478, 857-865. [79] Yin, Y.; Han, J.; Zhang, Y.; Zhang, X.; Xu, P.; Yuan, Q.; Samad, L.; Wang, X.; Wang, Y.; Zhang, Z.; Zhang, P.; Cao, X.; Song, B.; Jin, S. Contributions of Phase, Sulfur Vacancies, and Edges to the Hydrogen Evolution Reaction Catalytic Activity of Porous Molybdenum Disulfide Nanosheets. J. Am. Chem. Soc. 2016, 13, 7965-7972. [80] Joo, J.; Kim, T.; Lee, J.; Choi, S. I.; Lee, K. Morphology-Controlled Metal Sulfides and Phosphides for Electrochemical Water Splitting. Adv. Mater. 2019, 31, 1806682. [81] Staszak-Jirkovský, J.; Malliakas, C. D.; Lopes, P. P.; Danilovic, N.; Kota, S. S.; Chang, K. -C.; Genorio, B.; Strmcnik, D.; Stamenkovic, V. R.; Kanatzidis, M. G.; Markovic, N. M. Design of Active and Stable Co-Mo-Sx Chalcogels as pH-Universal Catalysts for the Hydrogen Evolution Reaction. Nat. Mater. 2016, 15, 197-203. [82] Ge, Y.; Gao, S. -P.; Dong, P.; Baines, R.; Ajayan, P. M.; Ye, M.; Shen, J. Insight into the Hydrogen Evolution Reaction of Nickel Dichalcogenide Nanosheets: Activities Related to Non-Metal Ligands. Nanoscale 2017, 9, 5538-5544. [83] Rasmussen, F. A.; Thygesen, K. S. Computational 2D Materials Database: Electronic Structure of Transition-Metal Dichalcogenides and Oxides. J. Phys. Chem. C 2015, 119, 13169-13183. [84] De Silva, U.; Masud, J.; Zhang, N.; Hong, Y.; Liyanage, W. P. R.; Asle Zaeem, M.; Nath, M. Nickel Telluride as a Bifunctional Electrocatalyst for Efficient Water Splitting in Alkaline Medium. J. Mater. Chem. 2018, 6, 7608-7822. [85] Kosmala, T.; Coy Diaz, H.; Komsa, H. P.; Ma, Y.; Krasheninnikov, A. V.; Batzill, M.; Agnoli, S. Metallic Twin Boundaries Boost the Hydrogen Evolution Reaction on the Basal Plane of Molybdenum Selenotellurides. Adv. Energy Mater. 2018, 8, 1800031. [86] Seok, J.; Lee, J. H.; Bae, D.; Ji, B.; Son, Y. W.; Lee, Y. H.; Yang, H.; Cho, S. Hybrid Catalyst with Monoclinic MoTe2 and Platinum for Efficient Hydrogen Evolution. APL Mater. 2019, 7, 071118. [87] Yoo, D.; Kim, M.; Jeong, S.; Han, J.; Cheon, J. Chemical Synthetic Strategy for Single-Layer Transition-Metal Chalcogenides. J. Am. Chem. Soc. 2014, 136, 14670-14673. [88] Balasingam, S. K.; Lee, J. S.; Jun, Y. Few-Layered MoSe2 Nanosheets as an Advanced Electrode Material for Supercapacitors. Dalton Trans. 2015, 44, 15491-15498. [89] Jiang, M.; Zhang, J.; Wu, M.; Jian, W.; Xue, H.; Ng, T. -W.; Lee, C. -S.; Xu, J. Synthesis of 1T-MoSe2 Ultrathin Nanosheets with an Expanded Interlayer Spacing of 1.17 nm for Efficient Hydrogen Evolution Reaction. J. Mater. Chem. A 2016, 4, 14949-14953. [90] Zhou, R.; Wang, H.; Chang, J.; Yu, C.; Dai, H.; Chen, Q.; Zhou, J.; Yu, H.; Sun, G.; Huang, W. Ammonium Intercalation Induced Expanded 1T-Rich Molybdenum Diselenides for Improved Lithium Ion Storage. ACS Appl. Mater. Interfaces 2021, 13, 17459-17466. [91] Yi, Y.; Sun, Z.; Li, C.; Tian, Z.; Lu, C.; Shao, Y.; Li, J.; Sun, J.; Liu, Z. Designing 3D Biomorphic Nitrogen-Doped MoSe2/Graphene Composites toward High-Performance Potassium-Ion Capacitors. Adv. Funct. Mater. 2020, 30, 1903878. [92] Bhat, K. S.; Nagaraja, H. S. Performance Evaluation of Molybdenum Dichalcogenide (MoX2; X= S, Se, Te) Nanostructures for Hydrogen Evolution Reaction. Int. J. Hydrog. Energy 2019, 44, 17878-17886. [93] Hu, C.; Zhang, L.; Zhao, Z. J.; Luo, J.; Shi, J.; Huang, Z.; Gong, J. Edge Sites with Unsaturated Coordination on Core-Shell Mn3O4@MnxCo3xO4 Nanostructures for Electrocatalytic Water Oxidation. Adv. Mater. 2017, 29, 1701820. [94] Chia, X.; Pumera, M. Inverse Opal-Like Porous MoSex Films for Hydrogen Evolution Catalysis: Overpotential-Pore Size Dependence. ACS Appl. Mater. Interfaces 2018, 10, 4937-4945. [95] Bhat, K. S.; Barshilia, H. C.; Nagaraja, H. S. Porous Nickel Telluride Nanostructures as Bifunctional Electrocatalyst towards Hydrogen and Oxygen Evolution Reaction. Int. J. Hydrog. Energy 2017, 42, 24645-24655. [96] Ndala, Z.; Shumbula, N.; Nkabinde, S.; Kolokoto, T.; Nchoe, O.; Shumbula, P.; Tetana, Z. N.; Linganiso, E. C.; Gqoba, S. S.; Moloto, N. Evaluating the Effect of Varying the Metal Precursor in the Colloidal Synthesis of MoSe2 Nanomaterials and Their Application as Electrodes in the Hydrogen Evolution Reaction. Nanomaterials 2020, 10, 1786. [97] Kwon, I. S.; Kwak, I. H.; Debela, T. T.; Abbas, H. G.; Park, Y. C.; Ahn, J. P.; Park, J.; Kang, H. S. Se-Rich MoSe2 Nanosheets and Their Superior Electrocatalytic Performance for Hydrogen Evolution Reaction. ACS Nano 2020, 14, 6295-6304. [98] Najafi, L.; Bellani, S.; Oropesa-Nunez, R.; Ansaldo, A.; Prato, M.; Del Rio Castillo, A. E.; Bonaccorso, F. Engineered MoSe2-Based Heterostructures for Efficient Electrochemical Hydrogen Evolution Reaction. Adv. Energy Mater. 2018, 8, 1703212. [99] Xia, B.; Wang, T.; Jiang, X.; Zhang, T.; Li, J.; Xiao, W.; Xi, P.; Gao, D.; Xue, D.; Ding, J. Ar2+ Beam Irradiation-Induced Multivancancies in MoSe2 Nanosheet for Enhanced Electrochemical Hydrogen Evolution. ACS Energy Lett. 2018, 3, 2167-2172. [100] Tang, Q. Tuning the Phase Stability of Mo-based TMD Monolayers through Coupled Vacancy Defects and Lattice Strain. J. Mater. Chem. C 2018, 6, 9561-9568. [101] Yin, Y.; Zhang, Y.; Gao, T.; Yao, T.; Zhang, X.; Han, J.; Wang, X.; Zhang, Z.; Xu, P.; Zhang, P.; Cao, X.; Song, B.; Jin, S. Synergistic Phase and Disorder Engineering in 1T-MoSe2 Nanosheets for Enhanced Hydrogen-Evolution Reaction. Adv. Mater. 2017, 29, 1700311. [102] Zhang, H.; Yu, L.; Chen, T.; Zhou, W.; Lou, X. W. Surface Modulation of Hierarchical MoS2 Nanosheets by Ni Single Atoms for Enhanced Electrocatalytic Hydrogen Evolution. Adv. Funct. Mater. 2018, 28, 1807086. [103] Yu, C.; Cao, Z.; Chen, S.; Wang, S.; Zhong, H. Promoting the Hydrogen Evolution Performance of 1T-MoSe2-Se: Optimizing the Two-Dimensional Structure of MoSe2 by Layered Double Hydroxide Limited Growth. Appl. Surf. Sci. 2020, 509, 145364. [104] Yi, J.; Li, H.; Gong, Y.; She, X.; Song, Y.; Xu, Y.; Deng, J.; Yuan, S.; Xu, H.; Li, H. Phase and Interlayer Effect of Transition Metal Dichalcogenide Cocatalyst toward Photocatalytic Hydrogen Evolution: the Case of MoSe2. Appl. Catal. B-Environ. 2019, 243, 330-336. [105] Zhang, Y.; Gong, Q.; Li, L.; Yang, H.; Li, Y.; Wang, Q. MoSe2 Porous Microspheres Comprising Monolayer Flakes with High Electrocatalytic Activity. Nano Res. 2015, 8, 1108-1115. [106] Duan, X.; Wang, C.; Pan, A.; Yu, R.; Duan, X. Two-Dimensional Transition Metal Dichalcogenides as Atomically Thin Semiconductors: Opportunities and Challenges. Chem. Soc. Rev. 2015, 44, 8859-8876. [107] Takahashi, Y.; Nakayasu, Y.; Iwase, K.; Kobayashi, H.; Honma, I. Supercritical Hydrothermal Synthesis of MoS2 Nanosheets with Controllable Layer Number and Phase Structure. Dalton Trans. 2020, 49, 9377-9384. Zhang, J.; Wang, T.; Liu, P.; Liu, Y.; Ma, J.; Gao, D. Enhanced Catalytic Activities of Metal-Phase-Assisted 1T@2H-MoSe2 Nanosheets for Hydrogen Evolution. Electrochim. Acta 2016, 217, 181-186. Abstract Introduction Conclusion References All Products Quick View Newly listed Tphysletters A Unifying Bag Model of Composite Fermionic Structures in a Cold Genesis Theory Regular Price $700.00 Sale Price $400.00 Excluding Sales Tax Quick View TphysicsLetters Detection of the large-scale tidal field with galaxy multiplet alignment in the Regular Price $1,900.00 Sale Price $950.00 Excluding Sales Tax Quick View Newly listed Tphysletters Violation of γ in Brans-Dicke gravity Regular Price $1,000.00 Sale Price $600.00 Excluding Sales Tax Quick View Astrophysics Observations and detectability of young Suns’ flaring and CME activity in optica Regular Price $1,000.00 Sale Price $450.00 Excluding Sales Tax Quick View TphysicsLetters Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S Regular Price $2,000.00 Sale Price $400.00 Excluding Sales Tax Quick View New Thphysletters Bayesian and frequentist investigation of prior effects in EFTofLSS analyses of Regular Price $3,000.00 Sale Price $370.00 Excluding Sales Tax Quick View New Thphysletters A search for faint resolved galaxies beyond the Milky Way in DES Year 6: A new f Regular Price $1,900.00 Sale Price $750.00 Excluding Sales Tax Quick View New X-ray polarization properties of partially ionized equatorial obscurers around a Regular Price $800.00 Sale Price $350.00 Excluding Sales Tax Quick View New Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Regular Price $1,200.00 Sale Price $400.00 Excluding Sales Tax Quick View New SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural N Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View New Rapid neutron star cooling triggered by accumulated dark matter Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View Newly listed Tphysletters Searching for Radio Outflows from M31* with VLBI Observations Price $300.00 Excluding Sales Tax Quick View New Thphysletters Measurement of the scaling slope of compressible magnetohydrodynamic turbulence Regular Price $680.00 Sale Price $612.00 Excluding Sales Tax Quick View MAKE OPEN ACCESS New method to revisit the gravitational lensing analysis of the Bullet Cluster u Price $1,030.00 Excluding Sales Tax Quick View New Thphysletters New method to revisit the gravitational lensing analysis of the Bullet Cluster u Regular Price $599.00 Sale Price $359.40 Excluding Sales Tax Quick View New Nebular spectra from Type Ia supernova explosion models compared to JWST observa Regular Price $503.00 Sale Price $271.62 Excluding Sales Tax Quick View New Thphysletters The Nature of the 1 MeV-Gamma quantum in a Classic Interpretation of the Quantum Price $399.00 Excluding Sales Tax Quick View Exceptional Classifications of Non-Hermitian Systems Price $399.00 Excluding Sales Tax Quick View New Thphysletters On the occurrence of stellar fission in binary-driven hypernovae Price $399.00 Excluding Sales Tax Quick View New ApplSciLettersA AC frequency influence on pump temperature Price $399.00 Excluding Sales Tax Quick View New ApplSciLett. 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Micro and Nano Physics HOME JOURNALS PRICING AND PLANS SUBMIT mnpl/3659/5548/2023/Quantum capacitance governs electrolyte conductivity in carbon nanotubes Received 17, March 2023 Revised 26, May 2023 Accepted 29, July 2023 Heading 4 Mon Jul 31 2023 06:30:00 GMT+0000 (Coordinated Universal Time) Make this article Open Accessed Apply Now Publisher Rating 10 MNPL Readers Rating 10 Citation (5) 10/1490/55874mnpl Quantum capacitance governs electrolyte conductivity in carbon nanotubes Th´eo Hennequin and Manoel Manghi∗ Laboratoire de Physique Th´eorique, Universit´e Paul Sabatier–Toulouse III, CNRS, France Adrien Noury, Fran¸cois Henn, Vincent Jourdain, and John Palmeri† Laboratoire Charles Coulomb, Universit´e de Montpellier, CNRS, France Micro & Nano Physics J. DOI- https://www.doi.wikipt.org/10/1490/55874mnpl Acknolowdgement NA Keyword Highlighted Quantum capacitance, carbon nanotubes, nano Unlock Only Read-only this publication This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Buy Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. 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By accounting for the coupling between the quantum CNT and the classical electrolyte-filled pore capacitances, we study the case where a gate voltage is applied to the CNT. The computed surface charge and conductivity dependence on reservoir salt concentration and gate voltage are intimately connected to the CNT electronic density of states. This approach provides key insight into why metallic CNTs have larger conductivities than semiconducting ones. Introduction Although much experimental, theoretical, and molecular modeling effort has been devoted over the past years to understanding water and ion (electrolyte) transport through carbon nanotubes (CNTs) [1–3], the origin of the electric charge localized on the surface of industrially important CNT based nanofluidic systems still remains unclear (see Ref. [4] and references therein). It has already been proposed that this surface charge could arise from functional groups at the CNT entrances [5, 6] and/or the specific adsorption of ions, such as OH− [7]. Although the above cited studies lead to the conclusion that this surface charge plays a key role in governing ion transport in CNTs, it is difficult to regulate it directly and one is left to making inferences, for example by studying the variation of ionic conductance G with the pH or salt concentration, cs, of the external bulk reservoirs bounding the CNT. Intriguing results have been obtained, including a power law behavior, G ∝ c α s , with 1/2 ≤ α ≤ 1, which could be interpreted as the manifestation of an underlying surface charge regulation mechanism [8–10]. Through a simplified feasibility study we propose in this work that by biasing a CNT incorporated in a nanofluidic system via an applied gate voltage, Vg, and taking into account explicitly the quantum capacitance (QC) of the quasi-1D CNT structure as well as the nonlinear capacitance of the confined electrolyte ion the pore, it should be possible to quantify the CNT surface charge density σQ and establish a link between the intrinsic CNT electronic properties and ion transport through the same structure, such as the electrolyte conductance through the CNT. A major conclusion it that these intrinsic electronic properties will depend significantly, under certain conditions, on whether the CNT is metallic (M) or semiconducting (SC). Conclusion As an concluding example, we consider the experimental results obtained by Liu et al. [30], who measured, for cs = 1 mol/L, conductances of 61.0 nS for M SWCNTs and 5.6 nS for SC ones with 0.8 ≤ d ≤ 2 nm and 5 ≤ L ≤ 10 nm. Using the DOS given in Fig. 1(a) with d = 1.5 nm and L = 8 nm, we can account for these two conductance values by taking Vg ≃ 0.35 V, a value that we interpret as an environmentally induced shift in the zero of the gate tension. More systematic experiments are clearly needed to ascertain to what extent the charge density and therefore the electrolyte conductivity through SWCNTs can be controlled by an applied gate voltage. Presumably, a more complete model for conductivity would be needed to account for the full complexity of real CNTs, including the influence of pH (via charge regulation), residual geometrical capacitances, and dielectric interactions. Reference [1] S. Guo, E. R. Meshot, T.Tevye Kuykendall, S. Cabrini, and F. Fornasiero, Nanofluidic Transport through Isolated Carbon Nanotube Channels: Advances, Controversies, and Challenges, Adv. Mater., 27, 5726-5737 (2015). [2] J. P. Thiruraman, P. M. Das, and M. Drndic, Ions and Water Dancing through Atom-Scale Holes: A Perspective toward “Size Zero”, ACSNano, 14, 3736-3746 (2020). [3] N. R. Aluru et al., Fluids and Electrolytes under Confinement in Single-Digit Nanopores, Chem. Rev. 2023, 123, 2737-2831 (2023). [4] M. Manghi, J. Palmeri, F. Henn, A. Noury, F. Picaud, G. Herlem, and V. Jourdain, Ionic Conductance of Carbon Nanotubes: Confronting Literature Data with Nanofluidic Theory, J. Phys. Chem. C, 125, 22943-22950 (2021). [5] S. Balme, F. Picaud, M. Manghi, J. Palmeri, M. Bechelany, S. Cabello-Aguilar, A. Abou-Chaaya, P. Miele, E. Balanzat, J.-M. Janot, Ionic transport through sub-10 nm diameter hydrophobic high-aspect ratio nanopores: experiment, theory and simulation, Sc. Rep. 5, 10135 (2015). [6] K. Yazda, S. Tahir, T. Michel, B. Loubet, M. Manghi, J. Bentin, F. Picaud, J. Palmeri, F. Henn, and V. Jourdain, Voltage-activated transport of ions through single-walled carbon nanotubes, Nanoscale 9, 11976 (2017). [7] B. Grosjean, C. Pean, A. Siria, L. Bocquet, R. Vuilleumier, and M.-L. Bocquet, Chemisorption of hydroxide on 2D materials from DFT calculations: graphene versus hexagonal boron nitride, J. Phys. Chem. Lett., 7, 4695- 4700 (2016). [8] E. Secchi, A. Nigues, L. Jubin, A. Siria, L. Bocquet, Scaling Behavior for Ionic Transport and its Fluctuations in Individual Carbon Nanotubes, Phys. Rev. Lett., 116, 154501 (2016). [9] P. M. Biesheuvel and M. Z. Bazant, Analysis of ionic conductance of carbon nanotubes, Phys. Rev. E, 94, 050601(R) (2016). [10] M. Manghi, J. Palmeri, K. Yazda, F. Henn and V. Jourdain, Role of charge regulation and flow slip in the ionic conductance of nanopores: An analytical approach, Phys. Rev. E, 98 012606 (2018). [11] P. Gao and C. R. Martin, Voltage Charging Enhances Ionic Conductivity in Gold Nanotube Membranes, ACSNano, 8, 8266-8272 (2014). [12] I. Heller, J. Kong, K.A. Williams, C. Dekker, and S. G. Lemay, Electrochemistry at Single-Walled Carbon Nanotubes: The Role of Band Structure and Quantum Capacitance, J. Am. Chem. Soc., 128 7353-7359 (2006). [13] I. Heller, A. M. Janssens, J. Mannik, E. D. Minot, S. G. Lemay, and C. Dekker, Identifying the Mechanism of Biosensing with Carbon Nanotube Transistors, Nano Lett., 8 591-595 (2008). [14] I. Heller, S. Chatoor, J. Mannik, M. A. G. Zevenbergen, C. Dekker, and S. G. Lemay, Influence of Electrolyte Composition on Liquid-Gated Carbon Nanotube and Graphene Transistors, J. Am. Chem. Soc. 131 17149- 17156 (2010). [15] S. Rosenblatt, Y. Yaish, J. Park, J. Gore, V. Sazonova, and P. L. McEuen, High Performance Electrolyte Gated Carbon Nanotube Transistors, Nano Lett., 2, 869-872 (2002). [16] J. Li, P. H. Q. Pham, W. Zhou, T. D. Pham, and P. J. Burke, Carbon-Nanotube-Electrolyte Interface: Quantum and Electric Double Layer Capacitance, ACSNano, 12, 9763-9774 (2018). [17] J. Li, and P. J. Burke, Measurement of the combined quantum and electrochemical capacitance of a carbon nanotube, Nature Comm., 10, 3598 (2019). [18] J. Xia, F. Chen, J. Li and N. Tao, Measurement of the quantum capacitance of graphene, Nature Nanotech., 4, 505-509 (2009). [19] T. Fang, A.Konar, H.Xing, and D. Jena, Carrier statistics and quantum capacitance of graphene sheets and ribbons, Appl. Phys. Lett. 91 092109 (2007). [20] Z. Jiang and D. Stein, Electrofluidic Gating of a Chemically Reactive Surface, Langmuir, 28 8161 (2010). [21] Z. Jiang and D. Stein, Charge regulation in nanopore ionic field-effect transistors, Phys. Rev. E, 83 031203 (2011). [22] J.W. Mintmire and C.T. White, Universal Density of States for Carbon Nanotubes, Phys. Rev. Lett., 81 2506 (1998). [23] M.J. Biercuk, S. Ilani, C.M. Marcus, and P.L. McEuen, In Carbon Nanotubes, Eds. A. Jorio, G. Dresselhaus, M.S. Dresselhaus, Electrical Transport in Single-Wall Carbon Nanotubes, Topics Appl. Physics 111, 455 (2008). [24] S. Ilani, L. A. K. Donev, M. Kindermann, and P. L. McEuen, Measurement of the quantum capacitance of interacting electrons in carbon nanotubes, Nature Phys., 2, 687-691 (2006). [25] T. Miyake and S. Saito, Quasiparticle band structure of carbon nanotubes, Phys. Rev. B, 68, 155424 (2003). [26] S. Maruyama web page, The University of Tokyo: http://photon.t.u-tokyo.ac.jp/~maruyama/kataura/ 1D_DOS.html [27] H. Zhang, C. Berthod, H. Berger, T. Giamarchi, A. F. Morpurgo, Band Filling and Cross Quantum Capacitance in Ion-Gated Semiconducting Transition Metal Dichalcogenide Monolayers, Nano Lett., 19, 8836 (2019). [28] C. Berthod, H. Zhang, A. F. Morpurgo, and T. Giamarchi, Theory of cross quantum capacitance, Phys. Rev. Res., 2, 043036 (2021). [29] S. K. Kannam, P. J. Daivis, and B. Todd, Modeling slip and flow enhancement of water in carbon nanotubes, MRS Bull., 42, 283-288 (2017). [30] L. Liu, C. Yang, K. Zhao, J. Li, and H.-C. Wu, Ultrashort single-walled carbon nanotubes in a lipid bilayer as a new nanopore sensor, Nature Comm., 4, 2989 (2013).

Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT Locked Tphysicsletters/6879/10/1490/585470tpl/SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural Networks for Detection of Entanglement Citation (16) Sunday, September 10, 2023 at 2:30:00 PM UTC Request Open Apply Now Article Rating by Publisher 10 Thoeretical Physics Article Rating by Readers 9 Premium doi.wikipt.org/10/1490/585470tpl SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural Networks for Detection of Entanglement Ali Kookani1,3, Yousef Mafi2,3, Payman Kazemikhah2,3 Hossein Aghababa4,5, Kazim Fouladi 1 Masoud Barati6 --------------------------------- 1 School of Engineering, College of Farabi, University of Tehran, Tehran, Iran 2 School of Electrical and Computer Engineering, College of Engineering, University of Tehran, Tehran, Iran 3 Quantum Computation and Communication Laboratory (QCCL), University of Tehran, Tehran, Iran 4 Department of Engineering, Loyola University Maryland, Maryland 5 Founder of Quantum Computation and Communication Laboratory (QCCL), University of Tehran, Tehran, Iran 6 Swanson School of Engineering, Electrical Engineering, University of Pittsburgh, Pittsburgh, Pennsylvania Theoretical Physics Letters 2023 ° 10(09) ° 0631-6367 https://www.wikipt.org/tphysicsletters DOI: https://www.doi.wikipt.org/10/1490/585470tpl TOA Abstract Introduction Conclusion Acknowledgement NA Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters Abstract The application of machine learning models in quantum information theory has surged in recent years, driven by the recognition of entanglement and quantum states, which are the essence of this field. However, most of these studies rely on existing prefabricated models, leading to inadequate accuracy. This work aims to bridge this gap by introducing a custom deep convolutional neural network (CNN) model explicitly tailored to quantum systems. Our proposed CNN model, the so-called SpookyNet, effectively overcomes the challenge of handling complex numbers data inherent to quantum systems and achieves an accuracy of 98.5%. Developing this custom model enhances our ability to analyze and understand quantum states. However, first and foremost, quantum states should be classified more precisely to examine fully and partially entangled states, which is one of the cases we are currently studying. As machine learning and quantum information theory are integrated into quantum systems analysis, various perspectives, and approaches emerge, paving the way for innovative insights and breakthroughs in this field. Introduction In quantum mechanics, an extraordinary phenomenon known as quantum entanglement arises when two or more particles interact so that their quantum states become related [1]. This relation indicates that the particles become correlated and can no longer be described independently [2]. Any change made to one particle will be instantaneously reflected in the others, even if they are far apart [3]. Creating and increasing entanglement in arbitrary qubits for quantum algorithms and quantum information (QI) theory protocols, in which entanglement is a vital resource, plays an influential role [4]. As proof, it excludes undesirable energy levels in quantum annealing [5] and facilitates the exchange of quantum information over long distances [6]. It also provides conditions for transferring classical bits of information with fewer qubits [7]. The first step in creating and increasing entanglement is recognizing its existence and amount. In recent years, various entanglement detection criteria have been proposed [8]. Yet, the positive partial transpose (PPT) criterion determines entanglement only in 2⊗2 and 2⊗3 non-mixed bi-party states by indicating the state is separable if the partial transpose of the density matrix is positive semi-definite [9]. In other words, there are some mixed states that are entangled but still meet the PPT conditions, which are called bound entangled states, as they cannot be used to create a maximally entangled state through local operations and classical communication (LOCC), even though the reduction criterion has been practical here [10]. Moreover, Werner states are another instance in which PPT is violated [11]. Measurement of the scaling slope of compressible magnetohydrodynamic turbulence Buy Now A method for automated regression test in scientific computing libraries: illust Buy Now Conclusion In recent years, quantum information theory has witnessed rapid growth and faced notable challenges. One significant hurdle is applying artificial intelligence (AI) to this field due to the complexity of feeding data with complex numbers into conventional AI models. However, this article presents a groundbreaking solution that addresses this challenge and propels the field forward. The key contribution of this research is the development of an advanced deep Convolutional Neural Network (CNN) model, boasting an impressive accuracy rate of 98.5%. This innovative model successfully overcomes the limitations of handling data with complex numbers, thereby unlocking new possibilities for effectively leveraging advanced machine learning techniques in processing quantum information. TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow References [1] Franck Lalo¨e. Quantum Entanglement, page 189–222. Cambridge University Press, 2 edition, 2019. [2] Pawel Blasiak and Marcin Markiewicz. Entangling three qubits without ever touching. Scientific Reports, 9(1):20131, 2019. [3] Tamoghna Das, Marcin Karczewski, Antonio Mandarino, Marcin Markiewicz, Bianka Woloncewicz, and Marek Zukowski. Comment on ‘single particle nonlocality with completely ˙ independent reference states’. New Journal of Physics, 24(3):038001, 2022. [4] Gary J Mooney, Charles D Hill, and Lloyd CL Hollenberg. Entanglement in a 20-qubit superconducting quantum computer. Scientific reports, 9(1):13465, 2019. [5] Trevor Lanting, Anthony J Przybysz, A Yu Smirnov, Federico M Spedalieri, Mohammad H Amin, Andrew J Berkley, Richard Harris, Fabio Altomare, Sergio Boixo, Paul Bunyk, et al. Entanglement in a quantum annealing processor. Physical Review X, 4(2):021041, 2014. [6] Laszlo Gyongyosi and Sandor Imre. Adaptive routing for quantum memory failures in the quantum internet. Quantum Information Processing, 18:1–21, 2019. [7] Charles Neill, Pedran Roushan, K Kechedzhi, Sergio Boixo, Sergei V Isakov, V Smelyanskiy, A Megrant, B Chiaro, A Dunsworth, K Arya, et al. A blueprint for demonstrating quantum supremacy with superconducting qubits. Science, 360(6385):195–199, 2018. [8] Manuel Gessner, Luca Pezze, and Augusto Smerzi. Efficient entanglement criteria for discrete, continuous, and hybrid variables. Physical Review A, 94(2):020101, 2016 16 [9] Eric Chitambar and Min-Hsiu Hsieh. Relating the resource theories of entanglement and quantum coherence. Physical review letters, 117(2):020402, 2016. [10] Micha l Horodecki and Pawe l Horodecki. Reduction criterion of separability and limits for a class of distillation protocols. Physical Review A, 59(6):4206, 1999. [11] Debbie Leung and William Matthews. On the power of ppt-preserving and non-signalling codes. IEEE Transactions on Information Theory, 61(8):4486–4499, 2015. [12] Ming-Jing Zhao, Teng Ma, Zhen Wang, Shao-Ming Fei, and Rajesh Pereira. Coherence concurrence for x states. Quantum Information Processing, 19:1–9, 2020. [13] Jaydeep Kumar Basak, Debarshi Basu, Vinay Malvimat, Himanshu Parihar, and Gautam Sengupta. Page curve for entanglement negativity through geometric evaporation. SciPost Physics, 12(1):004, 2022. [14] Ludovico Lami and Maksim E Shirokov. Attainability and lower semi-continuity of the relative entropy of entanglement and variations on the theme. In Annales Henri Poincar´e, pages 1–69. Springer, 2023. [15] Spyros Tserkis, Sho Onoe, and Timothy C Ralph. Quantifying entanglement of formation for two-mode gaussian states: Analytical expressions for upper and lower bounds and numerical estimation of its exact value. Physical Review A, 99(5):052337, 2019. [16] Ievgen I Arkhipov, Artur Barasi´nski, and Jiˇr´ı Svozil´ık. Negativity volume of the generalized wigner function as an entanglement witness for hybrid bipartite states. Scientific reports, 8(1):16955, 2018. [17] Yue-Chi Ma and Man-Hong Yung. Transforming bell’s inequalities into state classifiers with machine learning. npj Quantum Information, 4(1):34, 2018. [18] Sirui Lu, Shilin Huang, Keren Li, Jun Li, Jianxin Chen, Dawei Lu, Zhengfeng Ji, Yi Shen, Duanlu Zhou, and Bei Zeng. Separability-entanglement classifier via machine learning. Physical Review A, 98(1):012315, 2018. [19] Philipp Hyllus and Jens Eisert. Optimal entanglement witnesses for continuous-variable systems. New Journal of Physics, 8(4):51, 2006. [20] Xiaofei Qi and Jinchuan Hou. Characterization of optimal entanglement witnesses. Physical Review A, 85(2):022334, 2012. [21] Peng-Hui Qiu, Xiao-Guang Chen, and Yi-Wei Shi. Detecting entanglement with deep quantum neural networks. IEEE Access, 7:94310–94320, 2019. [22] Cillian Harney, Mauro Paternostro, and Stefano Pirandola. Mixed state entanglement classification using artificial neural networks. New Journal of Physics, 23(6):063033, 2021. [23] Antoine Girardin, Nicolas Brunner, and Tam´as Kriv´achy. Building separable approximations for quantum states via neural networks. Physical Review Research, 4(2):023238, 2022. [24] Yiwei Chen, Yu Pan, Guofeng Zhang, and Shuming Cheng. Detecting quantum entanglement with unsupervised learning. Quantum Science and Technology, 7(1):015005, 2021. [25] Naema Asif, Uman Khalid, Awais Khan, Trung Q Duong, and Hyundong Shin. Entanglement detection with artificial neural networks. Scientific Reports, 13(1):1562, 2023. [26] Xuemei Gu, Lijun Chen, Anton Zeilinger, and Mario Krenn. Quantum experiments and graphs. iii. high-dimensional and multiparticle entanglement. Physical Review A, 99(3):032338, 2019. [27] Marco Paini, Amir Kalev, Dan Padilha, and Brendan Ruck. Estimating expectation values using approximate quantum states. Quantum, 5:413, 2021. [28] Sebastian Wouters, Carlos A Jim´enez-Hoyos, Qiming Sun, and Garnet K-L Chan. A practical guide to density matrix embedding theory in quantum chemistry. Journal of chemical theory and computation, 12(6):2706–2719, 2016. [29] HY Huang, R Kueng, and J Preskill. Predicting many properties of a quantum system from very few measurements. arxiv 2020. arXiv preprint arXiv:2002.08953. [30] Maria Schuld and Francesco Petruccione. Machine learning with quantum computers. Springer, 2021. [31] Xingjian Zhen, Rudrasis Chakraborty, Nicholas Vogt, Barbara B Bendlin, and Vikas Singh. Dilated convolutional neural networks for sequential manifold-valued data. In Proceedings of the IEEE/CVF International Conference on Computer Vision, pages 10621–10631, 2019. [32] Hai Wang, Mengjun Shao, Yan Liu, and Wei Zhao. Enhanced efficiency 3d convolution based on optimal fpga accelerator. IEEE Access, 5:6909–6916, 2017. [33] Zhiyuan Li, Tianhao Wang, and Sanjeev Arora. What happens after sgd reaches zero loss?–a mathematical framework. arXiv preprint arXiv:2110.06914, 2021. [34] L Lu, Y Shin, Y Su, GE Karniadakis, and Dying ReLU. Initialization: Theory and numerical examples, 2019. Available: arXiv preprint, 14(1903.06733):v1. [35] Linlin Jia, Benoit Ga¨uz`ere, and Paul Honeine. Graph kernels based on linear patterns: theoretical and experimental comparisons. Expert Systems with Applications, 189:116095, 17 2022. [36] Mohammad Yosefpor, Mohammad Reza Mostaan, and Sadegh Raeisi. Finding semi-optimal measurements for entanglement detection using autoencoder neural networks. Quantum Science and Technology, 5(4):045006, 2020. [37] Christian Szegedy, Wei Liu, Yangqing Jia, Pierre Sermanet, Scott Reed, Dragomir Anguelov, Dumitru Erhan, Vincent Vanhoucke, and Andrew Rabinovich. Going deeper with convolutions. In Proceedings of the IEEE conference on computer vision and pattern recognition, pages 1–9, 2015. [38] Kaiming He, Xiangyu Zhang, Shaoqing Ren, and Jian Sun. Deep residual learning for image recognition. In Proceedings of the IEEE conference on computer vision and pattern recognition, pages 770–778, 2016. [39] Karen Simonyan and Andrew Zisserman. Very deep convolutional networks for large-scale image recognition. arXiv preprint arXiv:1409.1556, 2014. [40] Shibani Santurkar, Dimitris Tsipras, Andrew Ilyas, and Aleksander Madry. How does batch normalization help optimization? Advances in neural information processing systems, 31, 2018. [41] Jiang-Jiang Liu, Qibin Hou, Ming-Ming Cheng, Changhu Wang, and Jiashi Feng. Improving convolutional networks with self-calibrated convolutions. In Proceedings of the IEEE/CVF conference on computer vision and pattern recognition, pages 10096–10105, 2020. 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Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT PTL OPEN Sunday, February 28, 2021 at 5:30:00 AM UTC Request Open Apply Now In search of a new quantum theory: from an electron with a volume to the mechanism of light generation ACCEPTED COPY ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. TOA Abstract Introduction Conclusion Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. 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Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT Locked Tphysicsletters/6698/10/1490/687361tpl/New method to revisit the gravitational lensing analysis of the Bullet Cluster using radio waves Citation (0) Thursday, June 22, 2023 at 6:30:00 AM UTC Request Open Apply Now Article Rating by Publisher 8.6 Theoretical Physics Article Rating by Readers no data DOI: https://doi.wikipt.org/10/1490/687361tpl New method to revisit the gravitational lensing analysis of the Bullet Cluster using radio waves Youngsub Yoon a,b Jong-Chul Park,a,b,1 Ho Seong Hwangc,d ------------------------------------- a Department of Physics and Institute of Quantum Systems (IQS) Chungnam National University, Daejeon 34134, Republic of Korea b Particle Theory and Cosmology Group, Center for Theoretical Physics of the Universe, Institute for Basic Science (IBS), Daejeon, 34126, Republic of Korea c Astronomy Program, Department of Physics and Astronomy, Seoul National University, Seoul 08826, Republic of Korea d SNU Astronomy Research Center, Seoul National University, Seoul 08826, Republic of Korea Theoretical Physics Letters 2023 ° 22(06) ° 0631- 7361 https://www.wikipt.org/tphysicsletters DOI : 10/1490/687361tpl TOA Abstract Introduction Conclusion Acknowledgement We thank Douglas Clowe, Jérémie Francfort, Ruth Durrer, and Han-Gil Choi for helpful discussions. The work is supported by the National Research Foundation of Korea (NRF) [NRF- 2019R1C1C1005073 and NRF-2021R1A4A2001897 (YY, JCP), NRF-2021R1A2C1094577 (HSH)] and by IBS under the project code, IBS-R018-D1 (YY, JCP). Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters Abstract Gravitational lensing studies of the Bullet Cluster suggested convincingly in favour of the existence of dark matter. However, it was performed without the knowledge of the original orientation of each galaxy before gravitational lensing. A potential improvement to this issue lies in the measurement of the original orientation from the polarization direction of radio waves emitted from each galaxy. In this context, Francfort et al. derived a formula that can utilize the information about the original orientation of each galaxy to obtain what is called shear. However, we demonstrate that shear in their formula should be replaced by reduced shear when the change in sizes of images of galaxies is taken into account. As the previous gravitational lensing analysis of the Bullet Cluster used reduced shear, we suggest applying our improved formula directly for the reanalysis once we obtain the polarization direction of radio waves. In particular, we show that our new formula can yield a more accurate analysis than the previous one, if the polarization direction can be measured more precisely than 10◦. To read the full article please purchase. Introduction There are many observational results that favor the existence of dark matter. One of the most convincing results is the gravitational lensing analysis of the Bullet Cluster [1]; matter present in the Bullet Cluster, be it baryonic matter or dark matter, distorts the images of galaxies behind the Bullet Cluster, by its gravitation. The authors of Ref. [1] analyzed such images to reconstruct the mass distribution at the Bullet Cluster, which did not coincide with the baryonic matter distribution obtained by X-ray image. Thus, they concluded that dark matter is responsible for the discrepancy. In order to analyze the gravitational lensing effect, certain assumptions about the original images are necessary since the observed images of galaxies alone cannot determine the distortion. In Ref. [1], it is assumed that the average orientation of the original galactic images in each small patch of sky, where variables related to gravitational lensing are determined, is zero. However, this can lead to errors if there are not enough galaxies in each patch. Although this represents the optimal approach based on the currently available observational data, the analysis requires a sufficient number of galaxies to statistically determine the gravitational lensing effect in each patch. Otherwise, accidental skewing of the original galactic orientations could lead to skewed results. However, it is now possible to determine the original orientation of galaxies from the polarization of the radio waves from each galaxy. The radio emission from each galaxy is known to have a polarization that is perpendicular to the major axis of its ellipticity [2, 3]. While the orientation of a galactic image is rotated by gravitation, polarization is not. Therefore, even if the average original galactic orientations were distorted in a certain direction by accident, possibly due to the small number of galaxies in each small patch of sky, it would not bias the data, as long as we know the original orientation and therefore are able to compensate it. Thus, we can use this information to our advantage to measure the lensing effect more accurately, as pointed out in Refs. [3–5]. Therefore, the position of dark matter at the Bullet Cluster may be corrected if we reanalyze the gravitational lensing effect with the help of the polarization data of radio waves, which would be available in the future [6–8]. Read more relevant articles Nebular spectra from Type Ia supernova explosion models compared to JWST observa Buy Now The Nature of the 1 MeV-Gamma quantum in a Classic Interpretation of the Quantum Buy Now STeP-CiM: Strain-enabled Ternary Precision Computation-in-Memory based on Non-Vo Buy Now Conclusion Let’s estimate σg, the error of 1D g for the new method. We closely follow Ref. [3] where an error estimate for a mathematically similar but contently different case was considered. We will use the following notation: TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow References [1] D. Clowe, M. Bradac, A. H. Gonzalez, M. Markevitch, S. W. Randall, C. Jones and D. Zaritsky, “A direct empirical proof of the existence of dark matter,” Astrophys. J. Lett. 648 (2006), L109-L113 doi:10.1086/508162 [arXiv:astro-ph/0608407 [astro-ph]]. [2] J. M. Stil, M. Krause, R. Beck and A. R. Taylor, “The Integrated Polarization of Spiral Galaxy Disks,” Astrophys. J. 693 (2009), 1392-1403 doi:10.1088/0004-637X/693/2/1392 [arXiv:0810.2303 [astro-ph]]. [3] M. L. Brown and R. A. Battye, “Polarization as an indicator of intrinsic alignment in radio weak lensing,” Mon. Not. Roy. Astron. Soc. 410, 2057 (2011) doi:10.1111/j.1365-2966.2010.17583.x [arXiv:1005.1926 [ astro-ph.CO ]]. [4] J. Francfort, G. Cusin and R. Durrer, “Image rotation from lensing,” Class. Quant. Grav. 38 (2021) no.24, 245008 doi:10.1088/1361-6382/ac33ba [arXiv:2106.08631 [ astro-ph.GA ]]. [5] M. L. Brown and R. A. Battye, “Mapping the dark matter with polarized radio surveys,” Astrophys. J. Lett. 735, L23 (2011) doi:10.1088/2041-8205/735/1/L23 [arXiv:1101.5157 [ astro-ph.CO ]]. [6] D. J. Bacon et al. [SKA], “Cosmology with Phase 1 of the Square Kilometre Array: Red Book 2018: Technical specifications and performance forecasts,” Publ. Astron. Soc. Austral. 37, e007 (2020) doi:10.1017/pasa.2019.51 [arXiv:1811.02743 [ astro-ph.CO ]]. [7] M. L. Brown, D. J. Bacon, S. Camera, I. Harrison, B. Joachimi, R. B. Metcalf, A. Pourtsidou, K. Takahashi, J. A. Zuntz and F. B. Abdalla, et al. “Weak gravitational lensing with the Square Kilometre Array,” PoS AASKA14, 023 (2015) doi:10.22323/1.215.0023 [arXiv:1501.03828 [ astro-ph.CO ]]. [8] G. Heald et al. [SKA Magnetism Science Working Group], “Magnetism Science with the Square Kilometre Array,” Galaxies 8, no.3, 53 (2020) doi:10.3390/galaxies8030053 [arXiv:2006.03172 [ astro-ph.GA ]]. [9] V. Perlick, “Gravitational lensing from a spacetime perspective,” Living Rev. Rel. 7, 9 (2004) [arXiv:1010.3416 [gr-qc]]. [10] N. Kaiser, “Nonlinear cluster lens reconstruction,” Astrophys. J. Lett. 439, L1 (1995) doi:10.1086/187730 [arXiv:astro-ph/9408092 [astro-ph]]. [11] P. Schneider, “Cluster lens reconstruction using only observed local data,” Astron. Astrophys. 302, 639 (1995) [arXiv:astro-ph/9409063 [astro-ph]]. [12] R. D. Blandford, A. B. Saust, T. G. Brainerd and J. V. Villumsen, “The distortion of distant galaxy images by large-scale structure,” Mon. Not. Roy. Astron. Soc. 251, no.4, 600-627 (1991) doi:10.1093/mnras/251.4.600 [13] M. Bartelmann and P. Schneider, “Weak gravitational lensing,” Phys. Rept. 340, 291-472 (2001) doi:10.1016/S0370-1573(00)00082-X [arXiv:astro-ph/9912508 [astro-ph]]. [14] N. Kaiser, G. Squires and T. J. Broadhurst, “A Method for weak lensing observations,” Astrophys. J. 449, 460-475 (1995) doi:10.1086/176071 [arXiv:astro-ph/9411005 [astro-ph]]. [15] D. Clowe, P. Schneider, A. Aragon-Salamanca, M. Bremer, G. De Lucia, C. Halliday, P. Jablonka, B. Milvang-Jensen, R. Pello and B. Poggianti, et al. “Weak lensing mass reconstructions of the eso distant cluster survey,” Astron. Astrophys. 451, 395 (2006) doi:10.1051/0004-6361:20041787 [arXiv:astro-ph/0511746 [astro-ph]]. [16] S. Hou, X. L. Fan and Z. H. Zhu, “Gravitational Lensing of Gravitational Waves: Rotation of Polarization Plane,” Phys. Rev. D 100, no.6, 064028 (2019) doi:10.1103/PhysRevD.100.064028 [arXiv:1907.07486 [gr-qc]]. [17] P. Schneider, “Gravitational lensing as a probe of structure,” [arXiv:astro-ph/0306465 [astro-ph]]. [18] J. Francfort, G. Cusin and R. Durrer, “A new observable for cosmic shear,” JCAP 09, 003 (2022) doi:10.1088/1475-7516/2022/09/003 [arXiv:2203.13634 [ astro-ph.CO ]]. [19] C. Stanghellini, D. Dallacasa, M. Bondi and R. Della Ceca, “Arcsecond scale radio polarization of BL Lacertae objects” Astron. Astrophys. 325, 911 (1997) Suggesting other works Solve the Maxwell’s equations and Schrodinger’s equation but avoiding the Sommer Buy Now Self – Regulated Thermal Process Taking Place during Hardening of Materials ... 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Micro and Nano Physics HOME JOURNALS PRICING AND PLANS SUBMIT mnpl/3659/69800/2023/Room-temperature quantum emission from interface excitons in mixed-dimensional heterostructures Heading 4 Sat Aug 05 2023 06:30:00 GMT+0000 (Coordinated Universal Time) Make this article Open Accessed Apply Now Publisher Rating 9 Micro & Nano Physics J. Readers Rating 9 Citation (3) DOI- https://www.doi.wikipt.org/10/1490/698775mnpl Room-temperature quantum emission from interface excitons in mixed-dimensional heterostructures N. Fang,1, ∗ Y. R. Chang,1 S. Fujii,2, 3 D. Yamashita,2, 4 M. Maruyama,5 Y. Gao,5 C. F. Fong,1 D. Kozawa,1, 2, 6 K. Otsuka,1, 7 K. Nagashio,8 S. Okada,5 and Y. K. Kato1, 2, † 1Nanoscale Quantum Photonics Laboratory, RIKEN Cluster for Pioneering Research, Saitama 351-0198, Japan 2Quantum Optoelectronics Research Team, RIKEN Center for Advanced Photonics, Saitama 351-0198, Japan 3Department of Physics, Keio University, Yokohama 223-8522, Japan 4Platform Photonics Research Center, National Institute of Advanced Industrial Science and Technology (AIST), Ibaraki 305-8568, Japan 5Department of Physics, University of Tsukuba, Ibaraki 305-8571, Japan 6Research Center for Materials, National Institute for Materials Science, Ibaraki 305-0044, Japan 7Department of Mechanical Engineering, The University of Tokyo, Tokyo 113-8656, Japan 8Department of Materials Engineering, The University of Tokyo, Tokyo 113-8656, Japan Micro & Nano Physics J. DOI- https://www.doi.wikipt.org/10/1490/698775mnpl ACKNOWLEDGMENTS Parts of this study are supported by JSPS (KAKENHI JP22K14624, JP22K14625, JP21K14484, JP22F22350, JP22K14623, JP22H01893, JP21H05233, JP23H00262, JP20H02558) and MEXT (ARIM JPMXP1222UT1135). Y.R.C. is supported by JSPS (International Research Fellow). N.F. and C.F.F. are supported by RIKEN Special Postdoctoral Researcher Program. We thank the Advanced Manufacturing Support Team at RIKEN for technical assistance. Keyword Highlighted quantum emission, Room-temperature, van der Waals (vdW) materials, carbon nanotubes, silicon carbide Unlock Only Read-only this publication This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Buy Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Unlock us Quick View Newly listed Tphysletters A Unifying Bag Model of Composite Fermionic Structures in a Cold Genesis Theory Regular Price $700.00 Sale Price $400.00 Excluding Sales Tax Quick View TphysicsLetters Detection of the large-scale tidal field with galaxy multiplet alignment in the Regular Price $1,900.00 Sale Price $950.00 Excluding Sales Tax Quick View Newly listed Tphysletters Violation of γ in Brans-Dicke gravity Regular Price $1,000.00 Sale Price $600.00 Excluding Sales Tax Quick View Astrophysics Observations and detectability of young Suns’ flaring and CME activity in optica Regular Price $1,000.00 Sale Price $450.00 Excluding Sales Tax Quick View TphysicsLetters Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S Regular Price $2,000.00 Sale Price $400.00 Excluding Sales Tax Quick View New Thphysletters Bayesian and frequentist investigation of prior effects in EFTofLSS analyses of Regular Price $3,000.00 Sale Price $370.00 Excluding Sales Tax Quick View New Thphysletters A search for faint resolved galaxies beyond the Milky Way in DES Year 6: A new f Regular Price $1,900.00 Sale Price $750.00 Excluding Sales Tax Quick View New X-ray polarization properties of partially ionized equatorial obscurers around a Regular Price $800.00 Sale Price $350.00 Excluding Sales Tax Quick View New Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Regular Price $1,200.00 Sale Price $400.00 Excluding Sales Tax Quick View New SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural N Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View New Rapid neutron star cooling triggered by accumulated dark matter Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View Newly listed Tphysletters Searching for Radio Outflows from M31* with VLBI Observations Price $300.00 Excluding Sales Tax Load More Abstract The development of van der Waals heterostructures has introduced unconventional phenomena that emerge at atomically precise interfaces. For example, interlayer excitons in two-dimensional transition metal dichalcogenides show intriguing optical properties at low temperatures. Here we report on room-temperature observation of interface excitons in mixed-dimensional heterostructures consisting of two-dimensional tungsten diselenide and one-dimensional carbon nanotubes. Bright emission peaks originating from the interface are identified, spanning a broad energy range within the telecommunication wavelengths. The effect of band alignment is investigated by systematically varying the nanotube bandgap, and we assign the new peaks to interface excitons as they only appear in type-II heterostructures. Room-temperature localization of low-energy interface excitons is indicated by extended lifetimes as well as small excitation saturation powers, and photon correlation measurements confirm single-photon emission. With mixed-dimensional van der Waals heterostructures where band alignment can be engineered, new opportunities for quantum photonics are envisioned. Introduction The discovery of van der Waals (vdW) materials, including two-dimensional (2D) transition metal dichalcogenides (TMDs) and graphene, has brought about a revolution in the assembly of artificial heterostructures by allowing for the combination of two different materials without the constraints of lattice matching. Such an unprecedented level of flexibility in heterostructure design has led to the emergence of novel properties not seen in individual materials. A prime example is twisted bilayer graphene at magic angles, which exhibits exotic phases such as correlated insulating states [1] and superconductivity [2]. Another notable development is the stacking of two TMDs, resulting in the observation of unique excitons known as interlayer excitons, characterized by electrons and holes located in separate layers [3–6]. The spatially indirect nature of interlayer excitons imparts them with distinct properties, including long exciton lifetimes [3], extended diffusion lengths [7], large valley polarization [8], and significant modulation by moir´e potentials [9, 10]. The existing vdW heterostructures comprise of 2D materials with similar lattice structure, excitonic characteristics, and inherently identical dimensions. Development of vdW heterostructures that encompass lower dimen- sional materials may give rise to unique interface exciton states resulting from the mixed dimensionality. Carbon nanotubes (CNTs), a typical one-dimensional (1D) material, are ideal for such heterostructures as they have all bonds confined to the tube itself [11, 12]. CNTs interact with 2D materials through weak vdW forces, resulting in well-defined, atomically sharp interfaces [13, 14]. The chirality-dependent bandgap of CNTs can be utilized to tune the band alignment [15], allowing for unambiguous identification of excitonic states at the 1D-2D interface. Conclusion Air-suspended carbon nanotubes. We prepare airsuspended CNTs using trenched SiO2/Si substrates [11]. First, we pattern alignment markers and trenches with lengths of 900 µm and widths ranging from 0.5 to 3.0 µm onto the Si substrates using electron-beam lithography, followed by dry etching. We then thermally oxidize the substrate to form a SiO2 film, with a thickness ranging from 60 to 70 nm. Another electron-beam lithography process is used to define catalyst regions along the edges of the trenches. A 1.5 ˚A thick iron (Fe) film is deposited as a catalyst for CNT growth using an electron beam evaporator. CNTs are synthesized by alcohol chemical vapor deposition at 800◦C for 1 minute. The Fe film thickness is optimized to control the yield for preparing isolated CNTs. We select isolated, fully suspended chirality-identified CNTs with lengths ranging from 0.5 to 2.0 µm to form the heterostructures with WSe2. Anthracene crystal growth. For transferring WSe2 flakes onto CNTs, we grow anthracene crystals through an in-air sublimation process [17, 18]. Anthracene powder is heated to 80◦C on a glass slide, while another glass slide is placed 1 mm above the anthracene source. Thin and large-area single crystals are then grown on the glass surface. To promote the growth of large-area single crystals, we pattern the glass slides using ink from commercial markers. The typical growth time for anthracene crystals is 10 hours. Transfer of WSe2 by anthracene crystals. First, WSe2 (HQ graphene) flakes are prepared on 90-nm-thick SiO2/Si substrates using mechanical exfoliation, and the layer number is determined by optical contrast. An anthracene single crystal is picked up with a glasssupported PDMS sheet to form an anthracene/PDMS stamp. Next, the WSe2 flakes are picked up by pressing the anthracene/PDMS stamp against a substrate with the target WSe2 flakes. The stamp is quickly separated (> 10 mm/s) to ensure that the anthracene crystal remains attached Reference [1] Y. Cao, V. Fatemi, A. Demir, S. Fang, S. L. Tomarken, J. Y. Luo, J. D. Sanchez-Yamagishi, K. Watanabe, T. Taniguchi, E. Kaxiras, R. C. Ashoori, and P. JarilloHerrero, Correlated insulator behaviour at half-filling in magic-angle graphene superlattices, Nature 556, 80 (2018). [2] Y. Cao, V. Fatemi, S. Fang, K. Watanabe, T. Taniguchi, E. Kaxiras, and P. Jarillo-Herrero, Unconventional superconductivity in magic-angle graphene superlattices, Nature 556, 43 (2018). [3] P. Rivera, J. R. Schaibley, A. M. Jones, J. S. Ross, S. Wu, G. Aivazian, P. Klement, K. Seyler, G. Clark, N. J. Ghimire, J. Yan, D. G. Mandrus, W. Yao, and X. Xu, Observation of long-lived interlayer excitons in monolayer MoSe2-WSe2 heterostructures, Nat. Commun. 6, 6242 (2015). [4] R. Xiong, J. H. Nie, S. L. Brantly, P. Hays, R. Sailus, K. Watanabe, T. Taniguchi, S. Tongay, and C. Jin, Correlated insulator of excitons in MoSe2-WSe2 moir´e superlattices, Science 380, 860 (2023). [5] X. Sun, Y. Zhu, H. Qin, B. Liu, Y. Tang, T. L¨u, S. Rahman, T. Yildirim, and Y. Lu, Enhanced interactions of interlayer excitons in free-standing heterobilayers, Nature 610, 478 (2022). [6] N. Ubrig, E. Ponomarev, J. Zultak, D. Domaretskiy, V. Z´olyomi, D. Terry, J. Howarth, I. Guti´errez-Lezama, A. Zhukov, Z. R. Kudrynskyi, Z. D. Kovalyuk, A. Patan´e, T. Taniguchi, K. Watanabe, R. V. Gorbachev, V. I. Fal’ko, and A. F. Morpurgo, Design of van der Waals interfaces for broad-spectrum optoelectronics, Nat. Mater. 19, 299 (2020). [7] D. Unuchek, A. Ciarrocchi, A. Avsar, K. Watanabe, T. Taniguchi, and A. Kis, Room-temperature electrical control of exciton flux in a van der Waals heterostructure, Nature 560, 340 (2018). [8] P. Rivera, K. L. Seyler, H. Yu, J. R. Schaibley, J. Yan, D. G. Mandrus, W. Yao, and X. Xu, Valley-polarized exciton dynamics in a 2D semiconductor heterostructure, Science 351, 688 (2016). [9] C. Jin, E. C. Regan, A. Yan, M. I. B. Utama, D. Wang, S. Zhao, Y. Qin, S. Yang, Z. Zheng, S. Shi, K. Watanabe, T. Taniguchi, S. Tongay, A. Zettl, and F. Wang, Observation of moir´e excitons in WSe2/WS2 heterostructure superlattices, Nature 567, 76 (2019). [10] K. L. Seyler, P. Rivera, H. Yu, N. P. Wilson, E. L. Ray, D. G. Mandrus, J. Yan, W. Yao, and X. Xu, Signatures of moir´e-trapped valley excitons in MoSe2/WSe2 heterobilayers, Nature 567, 66 (2019). [11] A. Ishii, M. Yoshida, and Y. K. Kato, Exciton diffusion, end quenching, and exciton-exciton annihilation in individual air-suspended carbon nanotubes, Phys. Rev. B 91, 125427 (2015). [12] A. Ishii, M. Yoshida, and Y. K. Kato, High efficiency dark-to-bright exciton conversion in carbon nanotubes, Phys. Rev. X 9, 041048 (2019). [13] D. Jariwala, T. J. Marks, and M. C. Hersam, Mixeddimensional van der Waals heterostructures, Nat. Mater. 16, 170 (2016). [14] N. Fang, K. Otsuka, A. Ishii, T. Taniguchi, K. Watanabe, K. Nagashio, and Y. K. Kato, Hexagonal boron nitride as an ideal substrate for carbon nanotube photonics, ACS Photonics 7, 1773 (2020). [15] N. Fang, D. Yamashita, S. Fujii, M. Maruyama, Y. Gao, Y.-R. Chang, C. F. Fong, K. Otsuka, K. Nagashio, S. Okada, and Y. K. Kato, Resonant exciton transfer in mixed-dimensional heterostructures for overcoming dimensional restrictions in optical processes, arXiv:2307.07124 (2023). [16] J. Lefebvre, Y. Homma, and P. Finnie, Bright band gap photoluminescence from unprocessed single-walled carbon nanotubes, Phys. Rev. Lett. 90, 217401 (2003). [17] K. Otsuka, N. Fang, D. Yamashita, T. Taniguchi, K. Watanabe, and Y. K. Kato, Deterministic transfer of optical-quality carbon nanotubes for atomically defined technology, Nat. Commun. 12, 3138 (2021). [18] N. Fang, D. Yamashita, S. Fujii, K. Otsuka, T. Taniguchi, K. Watanabe, K. Nagashio, and Y. K. Kato, Quantization of mode shifts in nanocavities integrated with atom- 8 ically thin sheets, Adv. Opt. Mater. 10, 2200538 (2022). [19] M. Jiang, Y. Kumamoto, A. Ishii, M. Yoshida, T. Shimada, and Y. K. Kato, Gate-controlled generation of optical pulse trains using individual carbon nanotubes, Nat. Commun. 6, 6335 (2015). [20] T. Uda, M. Yoshida, A. Ishii, and Y. K. Kato, Electricfield induced activation of dark excitonic states in carbon nanotubes, Nano Lett. 16, 2278 (2016). [21] K. Otsuka, A. Ishii, and Y. K. Kato, Super-resolution fluorescence imaging of carbon nanotubes using a nonlinear excitonic process, Opt. Express 27, 17463 (2019). [22] R. Matsunaga, K. Matsuda, and Y. Kanemitsu, Origin of low-energy photoluminescence peaks in single carbon nanotubes: K-momentum dark excitons and triplet dark excitons, Phys. Rev. B 81, 033401 (2010). [23] D. Kozawa, X. Wu, A. Ishii, J. Fortner, K. Otsuka, R. Xiang, T. Inoue, S. Maruyama, Y. Wang, and Y. K. Kato, Formation of organic color centers in air-suspended carbon nanotubes using vapor-phase reaction, Nat. Commun. 13, 2814 (2022). [24] B. Yu, S. Naka, H. Aoki, K. Kato, D. Yamashita, S. Fujii, Y. K. Kato, T. Fujigaya, and T. Shiraki, ortho-substituted aryldiazonium design for the defect configuration-controlled photoluminescent functionalization of chiral single-walled carbon nanotubes, ACS Nano 16, 21452 (2022). [25] Q. Tan, A. Rasmita, S. Li, S. Liu, Z. Huang, Q. Xiong, S. A. Yang, K. Novoselov, and W.-b. Gao, Layerengineered interlayer excitons, Sci. Adv. 7, 1 (2021). [26] Y. Bai, L. Zhou, J. Wang, W. Wu, L. J. McGilly, D. Halbertal, C. F. B. Lo, F. Liu, J. Ardelean, P. Rivera, N. R. Finney, X.-C. Yang, D. N. Basov, W. Yao, X. Xu, J. Hone, A. N. Pasupathy, and X. Zhu, Excitons in straininduced one-dimensional moir´e potentials at transition metal dichalcogenide heterojunctions, Nat. Mater. 19, 1068 (2020). [27] S. Settele, F. J. Berger, S. Lindenthal, S. Zhao, A. A. El Yumin, N. F. Zorn, A. Asyuda, M. Zharnikov, A. H¨ogele, and J. Zaumseil, Synthetic control over the binding configuration of luminescent sp3 -defects in single-walled carbon nanotubes, Nat. Commun. 12, 2119 (2021). [28] K. Shinokita, Y. Miyauchi, K. Watanabe, T. Taniguchi, and K. Matsuda, Resonant coupling of a moir´e exciton to a phonon in a WSe2/MoSe2 heterobilayer, Nano Lett. 21, 5938 (2021). [29] M. Nirmal, B. O. Dabbousi, M. G. Bawendi, J. Macklin, J. Trautman, T. Harris, and L. E. Brus, Fluorescence intermittency in single cadmium selenide nanocrystals, Nature 383, 802 (1996). [30] W. E. Moerner and M. Orrit, Illuminating single molecules in condensed matter, Science 283, 1670 (1999). [31] G. Sallen, A. Tribu, T. Aichele, R. Andr´e, L. Besombes, C. Bougerol, S. Tatarenko, K. Kheng, and J. P. Poizat, Exciton dynamics of a single quantum dot embedded in a nanowire, Phys. Rev. B 80, 085310 (2009). [32] T. T. Tran, K. Bray, M. J. Ford, M. Toth, and I. Aharonovich, Quantum emission from hexagonal boron nitride monolayers, Nat. Nanotechnol. 11, 37 (2016). [33] K. Gao, I. Solovev, M. Holmes, M. Arita, and Y. Arakawa, Nanosecond-scale spectral diffusion in the single photon emission of a gan quantum dot, AIP Adv. 7, 125216 (2017). [34] A. Ishii, M. Yoshida, and Y. K. Kato, Roomtemperature single-photon emission from micrometerlong air-suspended carbon nanotubes, Phys. Rev. Applied 8, 054039 (2017). [35] T. M. Babinec, B. J. Hausmann, M. Khan, Y. Zhang, J. R. Maze, P. R. Hemmer, and M. Lonˇcar, A diamond nanowire single-photon source, Nat. Nanotechnol. 5, 195 (2010). [36] S. Castelletto, B. C. Johnson, V. Iv´ady, N. Stavrias, T. Umeda, A. Gali, and T. Ohshima, A silicon carbide room-temperature single-photon source, Nat. Mater. 13, 151 (2014). [37] X. Ma, N. F. Hartmann, J. K. S. Baldwin, S. K. Doorn, and H. Htoon, Room-temperature single-photon generation from solitary dopants of carbon nanotubes, Nat. Nanotechnol. 10, 671 (2015). [38] L. Linhart, M. Paur, V. Smejkal, J. Burgd¨orfer, T. Mueller, and F. Libisch, Localized intervalley defect excitons as single-photon emitters in WSe2, Phys. Rev. Lett. 123, 146401 (2019). [39] S. Zhang, C.-G. Wang, M.-Y. Li, D. Huang, L.-J. Li, W. Ji, and S. Wu, Defect structure of localized excitons in a WSe2 monolayer, Phys. Rev. Lett. 119, 046101 (2017). [40] K. Parto, S. I. Azzam, K. Banerjee, and G. Moody, Defect and strain engineering of monolayer WSe2 enables site-controlled single-photon emission up to 150 K, Nat. Commun. 12, 3585 (2021). [41] B. G. Shin, G. H. Han, S. J. Yun, H. M. Oh, J. J. Bae, Y. J. Song, C.-Y. Park, and Y. H. Lee, Indirect bandgap puddles in monolayer MoS2 by substrate-induced local strain, Adv. Mater. 28, 9378 (2016). [42] S. Zhao, Z. Li, X. Huang, A. Rupp, J. G¨oser, I. A. Vovk, S. Y. Kruchinin, K. Watanabe, T. Taniguchi, I. Bilgin, A. S. Baimuratov, and A. H¨ogele, Excitons in mesoscopically reconstructed moir´e heterostructures, Nat. Nanotechnol. 18, 572 (2023).

Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT PTL OPEN Citation (0) moshe_segal@yahoo.com Sunday, May 23, 2021 at 2:00:00 PM UTC Request Open Apply Now DOI - 10.1490/100235.100ptl A New Theory Expands Einstein's General Relativity Theory to Include Both Electric Charge and Mass Entities Moshe Segal ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. TOA Abstract Introduction Conclusion Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow ! Widget Didn’t Load Check your internet and refresh this page. If that doesn’t work, contact us. Abstract Introduction Conclusion References All Products Quick View Newly listed Tphysletters A Unifying Bag Model of Composite Fermionic Structures in a Cold Genesis Theory Regular Price $700.00 Sale Price $400.00 Excluding Sales Tax Quick View TphysicsLetters Detection of the large-scale tidal field with galaxy multiplet alignment in the Regular Price $1,900.00 Sale Price $950.00 Excluding Sales Tax Quick View Newly listed Tphysletters Violation of γ in Brans-Dicke gravity Regular Price $1,000.00 Sale Price $600.00 Excluding Sales Tax Quick View Astrophysics Observations and detectability of young Suns’ flaring and CME activity in optica Regular Price $1,000.00 Sale Price $450.00 Excluding Sales Tax Quick View TphysicsLetters Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S Regular Price $2,000.00 Sale Price $400.00 Excluding Sales Tax Quick View New Thphysletters Bayesian and frequentist investigation of prior effects in EFTofLSS analyses of Regular Price $3,000.00 Sale Price $370.00 Excluding Sales Tax Quick View New Thphysletters A search for faint resolved galaxies beyond the Milky Way in DES Year 6: A new f Regular Price $1,900.00 Sale Price $750.00 Excluding Sales Tax Quick View New X-ray polarization properties of partially ionized equatorial obscurers around a Regular Price $800.00 Sale Price $350.00 Excluding Sales Tax Quick View New Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Regular Price $1,200.00 Sale Price $400.00 Excluding Sales Tax Quick View New SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural N Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View New Rapid neutron star cooling triggered by accumulated dark matter Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View Newly listed Tphysletters Searching for Radio Outflows from M31* with VLBI Observations Price $300.00 Excluding Sales Tax Quick View New Thphysletters Measurement of the scaling slope of compressible magnetohydrodynamic turbulence Regular Price $680.00 Sale Price $612.00 Excluding Sales Tax Quick View MAKE OPEN ACCESS New method to revisit the gravitational lensing analysis of the Bullet Cluster u Price $1,030.00 Excluding Sales Tax Quick View New Thphysletters New method to revisit the gravitational lensing analysis of the Bullet Cluster u Regular Price $599.00 Sale Price $359.40 Excluding Sales Tax Quick View New Nebular spectra from Type Ia supernova explosion models compared to JWST observa Regular Price $503.00 Sale Price $271.62 Excluding Sales Tax Quick View New Thphysletters The Nature of the 1 MeV-Gamma quantum in a Classic Interpretation of the Quantum Price $399.00 Excluding Sales Tax Quick View Exceptional Classifications of Non-Hermitian Systems Price $399.00 Excluding Sales Tax Quick View New Thphysletters On the occurrence of stellar fission in binary-driven hypernovae Price $399.00 Excluding Sales Tax Quick View New ApplSciLettersA AC frequency influence on pump temperature Price $399.00 Excluding Sales Tax Quick View New ApplSciLett. Perturbative aspects of mass dimension one fermions non-minimally coupled to ele Regular Price $399.00 Sale Price $319.20 Excluding Sales Tax Quick View ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Price $200.00 Excluding Sales Tax Quick View New Thphysletters Magnetic reconnection as an erosion mechanism for magnetic switchbacks Price $490.00 Excluding Sales Tax Quick View New Thphysletters Calculation of the Hubble Constant, the Minimum Mass, and the Proton Charge Radi Price $499.00 Excluding Sales Tax Featured Changeover the Schrödinger Equation $100.00 Price Excluding Sales Tax View Details

Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT Locked Tphysicsletters/6879/10/1490/587850tpl/Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Citation (43) Sunday, September 3, 2023 at 11:00:00 AM UTC Request Open Apply Now Article Rating by Publisher 9 Astrophysics Experimental Article Rating by Readers 10 doi.wikipt.org/10/1490/588796tpl Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Olag Pratim Bordoloi,1★ Yuri A. Shchekinov,2 † P. Shalima,3‡ M. Safonova4 § and Rupjyoti Gogoi1 ¶ 1Tezpur University, Napaam, Assam, India, 784028 2Raman Research Institute, Bengaluru, India, 560080 3Manipal Centre for Natural Sciences, Centre of Excellence, Manipal Academy of Higher Education, Manipal, Karnataka, India, 576104 4 Indian Institute of Astrophysics, Bengaluru, India, 560034 Theoretical Physics Letters 2023 ° 03(09) ° 0631-66982 https://www.wikipt.org/tphysicsletters DOI: https://www.doi.wikipt.org/10/1490/588796tpl TOA Abstract Introduction Conclusion OPB and RG are thankful to Science & Engineering Research Board (SERB), Department of Science & Technology (DST), Government of India for financial support (EMR/2017/003092). OPB acknowledges the help received during this work from his colleagues Anshuman Borgohain and Hritwik Bora. SP acknowledges Manipal Centre for Natural Sciences, Centre of Excellence, Manipal Academy of Higher Education (MAHE) for facilities and support. MS acknowledges the financial support by the DST, Government of India, under the Women Scientist Scheme (PH) project reference number SR/WOS-A/PM-17/2019. YS acknowledges the hospitality of the Raman Research Institute, Bengaluru, India. Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters Abstract Holmberg II – a dwarf galaxy in the nearby M81 group – is a very informative source of distribution of gas and dust in the interstellar discs. High-resolution observations in the infrared (IR) allows us to distinguish isolated star-forming regions, photodissociation (PDR) and HII regions, remnants of supernovae (SNe) explosions and, as such, can provide information about more relevant physical processes. In this paper we analyse dust emission in the wavelength range 4.5 to 160 𝜇m using the data from IR space observatories at 27 different locations across the galaxy. We observe that the derived spectra can be represented by multiple dust populations with different temperatures, which are found to be independent of their locations in the galaxy. By comparing the dust temperatures with the far ultraviolet (FUV) intensities observed by the UVIT instrument onboard AstroSat, we find that for locations showing a 100 𝜇m peak, the temperature of cold (20 to 30 K) dust grains show a dependence on the FUV intensities, while such a dependence is not observed for the other locations. We believe that the approach described here can be a good tool in revealing different dust populations in other nearby galaxies with available high spatial resolution data. Introduction Dwarfs galaxies (DG) – galaxies with baryonic mass of 𝑀𝑏∼109𝑀⊙, are commonly thought to be the building blocks for the entire hierarchy of mass distribution in the Universe, being progressed during its evolution since post-recombination epochs through merging process (White & Rees 1978). Within this concept, DG in local Universe can serve as laboratories for understanding the details of physical processes regulating formation of the very first galaxies in early Universe (see review by Tolstoy et al. 2009, and more recent discussions in Henkel et al. (2022); Annibali & Tosi (2022)). Among the most important traits of DGs are their metal-poor interstellar medium (ISM) and, correspondingly, a low dust content (Henkel et al. 2022) – the features that are also commonly expected for early Universe galaxies. Observations of bright galaxies at 𝑧 > 10 conducted first by the Hubble Space Telescope (HST), and subsequently by the James Webb Space Telescope (JWST), have indeed indicated a deficient amount of dust in a set of high-𝑧 galaxies (see discussion in Finkelstein et al. 2022; Ferrara et al. 2023). In order for local DGs to indeed provide relevant information for understanding of their more distant congeners, the comparative analysis of their global emission characteristics, along with the respective properties on smaller scales, is of a high importance (relevant discussion can be found in Izotov et al. 2021; Henkel et al. 2022). A good example of a DG in local Universe is the Holmberg II (Ho II) galaxy belonging to the nearby M81 group at a distance of ≃ 3.4 Mpc. Its modest inclination angle (≈27◦ ; Sánchez-Salcedo et al. (2014)) makes Ho II a very informative source of distribution of gas and dust in the interstellar discs. Spitzer and Herschel space telescopes with the angular resolution of ∼ 2 ′′ − 5 ′′ can probe the Ho II interstellar disc with a high scrutiny. Scanning the interstellar medium (ISM) with such resolution can allow to distinguish isolated star forming regions (SFR), photodissociation (PDR) and HII regions, supernovae remnants, and can provide information about relevant physical processes. In this Letter we analyze spectra of dust emission in the range 𝜆𝜆 = 4.5, . . . 160 𝜇m from Spitzer and Herschel archival data, focusing on a few rather small-area locations. It allows us to distinguish IR emission which cannot be attributed to the isothermal dust, thus requiring existence of at least two populations of dust with different temperatures.Since the primary source of dust heating is the absorption of UV/optical photons by the dust grains, we have also utilised the highest available resolution (1.2 ′′ −1.6 ′′) FUV observations of Ho II galaxy obtained by the UVIT instrument of India’s AstroSat mission (Singh et al. 2014) as part of this study. The data correspond to 3 epochs in 2016, 2 epochs in 2019, and 3 epochs in 2020 (Vinokurov et al. 2022). These observations are crucial in understanding the UV radiation fields, responsible for modifying the dust populations and © their thermal IR emission profiles at these locations. READ MORE ARTICLES On the occurrence of stellar fission in binary-driven hypernovae Buy Now Exceptional Classifications of Non-Hermitian Systems Buy Now Conclusion We present for the first time analysis of IR dust emission in the galaxy Holmberg II to detect spatial variations of dust parameters on small physical scales of ∼ 82 pc (corresponding to a circular area of 5′′-radius) using high angular resolution data from Spitzer and Herschel. (ii) In several locations, connected to physically distinct regions, we found spectra that can represent several – up to five, dust populations with different temperatures. Spectral characteristics are not sensitive to the HI column density, except for the cold dust component with 𝑇𝑑 = 10 − 15 K which concentrates predominantly in HI deficient regions. Preliminary inspection shows that this cold dust population does not show a dependence on FUV intensity. (iii) Similarly, the cold dust in those regions with spectra peaking at 70 𝜇m has temperatures nearly in the same range as the HI voids with little dependence on FUV intensity. However, for those locations with the peak intensity at 100 𝜇m, the temperature of the cold dust component (𝑇𝑑 = 20 − 30 K) increases with FUV intensity. (iv) The estimated dust mass manifests signs of anti-correlation with its temperature, as formerly reported for dwarf star-forming galaxies by Izotov et al. (2014). TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow References Annibali F., Tosi M., 2022, Nature Astronomy, 6, 48 Banerjee A., Jog C. J., Brinks E., Bagetakos I., 2011, MNRAS, 415, 687 Bordoloi O. P., Shalima P., Safonova M., Shchekinov Y., Gogoi R., 2023, in preparation Compiègne M., Abergel A., Verstraete L., Habart E., 2008, A&A, 491, 797 Cortese L., et al., 2012, A&A, 540, A52 Draine B. T., 2011, Physics of the Interstellar and Intergalactic Medium Draine B. T., Lee H. M., 1984, ApJ, 285, 89 Draine B. T., Li A., 2007, ApJ, 657, 810 Drozdov S. A., 2021, Astrophysics, 64, 126 Drozdov S. A., Shchekinov Y. A., 2019, Astrophysics, 62, 540 Dwek E., 1986, ApJ, 302, 363 Dwek E., Arendt R. G., 1992, ARA&A, 30, 11 Egorov O. V., et al., 2023, ApJ, 944, L16 Fazio G. G., et al., 2004, ApJS, 154, 10 Ferrara A., Pallottini A., Dayal P., 2023, MNRAS, 522, 3986 Finkelstein S. L., et al., 2022, ApJ, 940, L55 Galliano F., Galametz M., Jones A. P., 2018, ARA&A, 56, 673 Galliano F., et al., 2021, A&A, 649, A18 Helou G., et al., 2004, ApJS, 154, 253 Henkel C., Hunt L. K., Izotov Y. I., 2022, Galaxies, 10, 11 Hildebrand R. H., 1983, QJRAS, 24, 267 Izotov Y. I., Guseva N. G., Fricke K. J., Krügel E., Henkel C., 2014, A&A, 570, A97 Izotov Y. I., Guseva N. G., Fricke K. J., Henkel C., Schaerer D., Thuan T. X., 2021, A&A, 646, A138 Jura M., 1999, ApJ, 515, 706 Kennicutt Robert C. J., et al., 2003, PASP, 115, 928 Kennicutt R. C., et al., 2011, PASP, 123, 1347 Lagadec E., Mékarnia D., de Freitas Pacheco J. A., Dougados C., 2005, A&A, 433, 553 Li A., 2020, Nature Astronomy, 4, 339 Nath B. B., Shchekinov Y., 2013, ApJ, 777, L12 Rieke G. H., et al., 2004, ApJS, 154, 25 Sánchez-Salcedo F. J., Hidalgo-Gámez A. M., Martínez-García E. E., 2014, Rev. Mex. Astron. Astrofis., 50, 225 Singh K. P., et al., 2014, in Takahashi T., den Herder J.-W. A., Bautz M., eds, Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series Vol. 9144, Space Telescopes and Instrumentation 2014: Ultraviolet to Gamma Ray. p. 91441S, doi:10.1117/12.2062667 Tolstoy E., Hill V., Tosi M., 2009, ARA&A, 47, 371 Uzpen B., Kobulnicky H. A., Semler D. R., Bensby T., Thom C., 2008, ApJ, 685, 1157 Vinokurov A., et al., 2022, Astrophysical Bulletin, 77, 231 Walter F., et al., 2007, ApJ, 661, 102 White S. D. M., Rees M. J., 1978, MNRAS, 183, 341 Zhou L., Shi Y., Diaz-Santos T., Armus L., Helou G., Stierwalt S., Li A., 2016, MNRAS, 458, 772 Abstract Introduction Conclusion References All Products Quick View Newly listed Tphysletters A Unifying Bag Model of Composite Fermionic Structures in a Cold Genesis Theory Regular Price $700.00 Sale Price $400.00 Excluding Sales Tax Quick View TphysicsLetters Detection of the large-scale tidal field with galaxy multiplet alignment in the Regular Price $1,900.00 Sale Price $950.00 Excluding Sales Tax Quick View Newly listed Tphysletters Violation of γ in Brans-Dicke gravity Regular Price $1,000.00 Sale Price $600.00 Excluding Sales Tax Quick View Astrophysics Observations and detectability of young Suns’ flaring and CME activity in optica Regular Price $1,000.00 Sale Price $450.00 Excluding Sales Tax Quick View TphysicsLetters Tunable structure-activity correlations of molybdenum dichalcogenides (MoX2; X=S Regular Price $2,000.00 Sale Price $400.00 Excluding Sales Tax Quick View New Thphysletters Bayesian and frequentist investigation of prior effects in EFTofLSS analyses of Regular Price $3,000.00 Sale Price $370.00 Excluding Sales Tax Quick View New Thphysletters A search for faint resolved galaxies beyond the Milky Way in DES Year 6: A new f Regular Price $1,900.00 Sale Price $750.00 Excluding Sales Tax Quick View New X-ray polarization properties of partially ionized equatorial obscurers around a Regular Price $800.00 Sale Price $350.00 Excluding Sales Tax Quick View New Unravelling multi-temperature dust populations in the dwarf galaxy Holmberg II Regular Price $1,200.00 Sale Price $400.00 Excluding Sales Tax Quick View New SpookyNet: Advancement in Quantum System Analysis through Convolutional Neural N Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View New Rapid neutron star cooling triggered by accumulated dark matter Regular Price $1,500.00 Sale Price $500.00 Excluding Sales Tax Quick View Newly listed Tphysletters Searching for Radio Outflows from M31* with VLBI Observations Price $300.00 Excluding Sales Tax Quick View New Thphysletters Measurement of the scaling slope of compressible magnetohydrodynamic turbulence Regular Price $680.00 Sale Price $612.00 Excluding Sales Tax Quick View MAKE OPEN ACCESS New method to revisit the gravitational lensing analysis of the Bullet Cluster u Price $1,030.00 Excluding Sales Tax Quick View New Thphysletters New method to revisit the gravitational lensing analysis of the Bullet Cluster u Regular Price $599.00 Sale Price $359.40 Excluding Sales Tax Quick View New Nebular spectra from Type Ia supernova explosion models compared to JWST observa Regular Price $503.00 Sale Price $271.62 Excluding Sales Tax Quick View New Thphysletters The Nature of the 1 MeV-Gamma quantum in a Classic Interpretation of the Quantum Price $399.00 Excluding Sales Tax Quick View Exceptional Classifications of Non-Hermitian Systems Price $399.00 Excluding Sales Tax Quick View New Thphysletters On the occurrence of stellar fission in binary-driven hypernovae Price $399.00 Excluding Sales Tax Quick View New ApplSciLettersA AC frequency influence on pump temperature Price $399.00 Excluding Sales Tax Quick View New ApplSciLett. 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Theoretical Physics Letters HOME JOURNALS PRICING AND PLANS SUBMIT Locked Tphysicsletters/6879/10/1490/584587tpl/Rapid neutron star cooling triggered by accumulated dark matter Citation (10) Sunday, September 10, 2023 at 12:45:00 PM UTC Request Open Apply Now Article Rating by Publisher 10 Astrophysics Experimental Article Rating by Readers 9 Premium doi.wikipt.org/10/1490/584587tpl Rapid neutron star cooling triggered by accumulated dark matter Afonso Avila ´ 1 ∗ Edoardo Giangrandi1,2 † Violetta Sagun1 ‡ Oleksii Ivanytskyi3 § and Constan¸ca Providˆencia 1¶ ---------------------------------------- 1CFisUC, Department of Physics, University of Coimbra, Rua Larga P-3004-516, Coimbra, Portugal 2 Institut f¨ur Physik und Astronomie, Universit¨at Potsdam, Karl-Liebknecht-Str.24-25, Potsdam, Germany and 3 Incubator of Scientific Excellence—Centre for Simulations of Superdense Fluids, University of Wroc law, 50-204, Wroclaw, Poland Theoretical Physics Letters 2023 ° 10(09) ° 0631-9870 https://www.wikipt.org/tphysicsletters DOI: https://www.doi.wikipt.org/10/1490/584587tpl TOA Abstract Introduction Conclusion Acknowledgement The work is supported by the FCT – Funda¸c˜ao para a Ciˆencia e a Tecnologia, within the project No. EXPL/FIS-AST/0735/2021. A.A., E.G., V.S., and ´ C.P. acknowledge the support from FCT within the projects No. UIDB/04564/2020, UIDP/04564/2020. E.G. also acknowledges the support from Project No. PRT/BD/152267/2021. C.P. is supported by project No. PTDC/FIS-AST/28920/2017. The work of O.I. was supported by the program Excellence Initiative–Research University of the University of Wroc law of the Ministry of Education and Science. Unlock Only Changeover the Schrödinger Equation This option will drive you towards only the selected publication. If you want to save money then choose the full access plan from the right side. Unlock all Get access to entire database This option will unlock the entire database of us to you without any limitations for a specific time period. This offer is limited to 100000 clients if you make delay further, the offer slots will be booked soon. Afterwards, the prices will be 50% hiked. Buy Unlock us Newsletters Abstract We study the effect of asymmetric fermionic dark matter (DM) on the thermal evolution of neutron stars (NSs). No interaction between DM and baryonic matter is assumed, except the gravitational one. Using the two-fluid formalism, we show that DM accumulated in the core of a star pulls inwards the outer baryonic layers of the star, increasing the baryonic density in the NS core. As a result, it significantly affects the star’s thermal evolution by triggering an early onset of the dir ect Urca process and modifying the photon emission from the surface caused by the decrease of the radius. Thus, due to the gravitational pull of DM, the direct Urca process becomes kinematically allowed for stars with lower masses. Based on these results, we discuss the importance of NS observations at different distances from the Galactic center. Since the DM distribution peaks towards the Galactic center, NSs in this region are expected to contain higher DM fractions that could lead to a different cooling behavior. Introduction Extremely high gravitational field and compactness inside neutron stars (NSs) make them a perfect laboratory to study the strongly interacting matter, test General Relativity and physics beyond the Standard Model [1, 2]. Throughout the entire stellar evolution, NSs could accumulate a sizeable amount of dark matter (DM) in their interior, which will impact the matter distribution, masses, radii, etc. [3–7]. At the end of its evolution, a main sequence star of 8-20 M⊙ undergoes a supernova explosion, creating an NS [8]. The former is from the gravitational collapse of molecular cloud regions, which exceed the Jeans limit. The proto-cloud may already present traces of DM, facilitating the collapse and giving rise to newly born stars with a sizeable amount of DM [9]. Once the star is born, DM particles could be further accreted from a surrounding medium, leading to an even higher DM fraction inside the object [10, 11]. At the end of the stellar evolution, the star eventually reaches the iron-core stage, undergoing a core-collapse supernova explosion. During this incredibly energetic event, DM might be created and further accrued inside the remnant, i.e. an NS [12]. More exotic scenarios can also be taken into account, e.g. mergers of baryonic matter (BM) stars with boson stars, and accretion of DM clumps [13]. Once the DM is trapped in the gravitational field of an NS, it may lead to different configurations depending on the DM properties: a core or halo configuration. In the former scenario, DM forms a compact core in the inner regions of an NS. A stronger gravitational pull by the inner Conclusion In this study, we focus on the effects of asymmetric fermionic DM on the NS thermal evolution. Despite asymmetric DM that interacts with BM only gravitationally contributes neither to neutrino, and photon emission directly nor deposits energy to the system, it alters the thermal evolution of NSs indirectly. We demonstrate that an accumulated DM pulls inwards BM from the outer layers, significantly increasing the central density, hence modifying the BM distribution. Consequently, the onset of the DU process is triggered at lower NS masses, leading to a highly efficient and rapid cooling, which is substantially different from the case when it is forbidden. At the same time, the proton fraction corresponding to the DU onset remains the same, as for the pure BM star with the same central BM density. We show that despite the DU process is kinematically allowed only at 1.91 M⊙ for the IST EoS and 1.92 M⊙ for the FSU2R EoS, an accumulation of DM particles with mχ = 1 GeV of fχ ≃ 0.161% (IST EoS) and fχ = 0.378% (FSU2R EoS) triggers the previously forbidden process. An increase of the DM particle’s mass mχ ≥ 3 GeV and/or DM fraction fχ ≥ 2 % shifts the DU onset even below 1.6 M⊙. This effect is also illustrated on the compact object in the center of the Cas A. Indeed, the surface temperature drop of Cas A could be explained by the rapid DU cooling triggered at a lower mass in comparison to the pure BM star. An additional effect of DM is related to the pull of BM inward, creating a more compact core and reduction of the baryonic radius. Thus, the total surface of the star is reduced leading to a lower photon luminosity. This effect is clearly visible at the photon-dominated stage when the neutrino emission takes a subdominant role. TOC (TphysicsLetters) TOC (TphysicsLetters) The Nature of the 1 MeV-Gamma Quantum in a Classic Interpretation of the Quantum Nebular spectra from Type Ia supernov Physics Tomorrow TOC HIGHLIGHTS 2023 TOC HIGHLIGHTS 2023 Theoretical Physics Letters Physics Tomorrow ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS ZZ Ceti stars of the southern ecliptic hemisphere re-observed by TESS Physics Tomorrow References [1] G. Baym, T. Hatsuda, T. Kojo, P. D. Powell, Y. Song, and T. Takatsuka, Rept. Prog. Phys. 81, 056902 (2018), [2] M. Kramer et al., Phys. Rev. X 11, 041050 (2021), arXiv:2112.06795 [astro-ph.HE]. [3] O. Ivanytskyi, V. Sagun, and I. Lopes, Phys. Rev. D 102, 063028 (2020), arXiv:1910.09925 [astro-ph.HE]. [4] V. Sagun, E. Giangrandi, O. Ivanytskyi, I. Lopes, and K. A. Bugaev, PoS PANIC2021, 313 (2022), arXiv:2111.13289 [astro-ph.HE]. [5] E. Giangrandi, V. Sagun, O. Ivanytskyi, C. Providˆencia, and T. Dietrich, Astrophys. J. 953, 115 (2023), arXiv:2209.10905 [astro-ph.HE]. [6] R. F. Diedrichs, N. Becker, C. Jockel, J.-E. Christian, L. Sagunski, and J. Schaffner-Bielich, arxiv (2023), arXiv:2303.04089 [gr-qc]. [7] D. R. Karkevandi, S. Shakeri, V. Sagun, and O. Ivanytskyi, Phys. Rev. D 105, 023001 (2022), arXiv:2109.03801 [astro-ph.HE]. [8] A. Heger, C. L. Fryer, S. E. Woosley, N. Langer, and D. H. Hartmann, The Astrophysical Journal 591, 288 (2003). [9] W. Yang, H. Chen, and S. Liu, AIP Adv. 10, 075003 (2020). [10] R. Brito, V. Cardoso, and H. Okawa, Physical Review Letters 115 (2015), 10.1103/physrevlett.115.111301. [11] C. Kouvaris and P. Tinyakov, Phys. Rev. D 83, 083512 (2011), arXiv:1012.2039 [astro-ph.HE]. [12] M. Meyer and T. Petrushevska, Phys. Rev. Lett. 124, 231101 (2020), [Erratum: Phys.Rev.Lett. 125, 119901 (2020)], arXiv:2006.06722 [astro-ph.HE]. [13] Y. Dengler, J. Schaffner-Bielich, and L. Tolos, Phys. Rev. D 103, 109901 (2021). [14] J. Ellis, A. Hektor, G. H¨utsi, K. Kannike, L. Marzola, M. Raidal, and V. Vaskonen, Phys. Lett. B 781, 607 (2018), arXiv:1710.05540 [ astro-ph.CO ]. [15] M. Bezares, D. Vigan`o, and C. Palenzuela, Phys. Rev. D 100, 044049 (2019), arXiv:1905.08551 [gr-qc]. [16] G. F. Giudice, M. McCullough, and A. Urbano, JCAP 10, 001 (2016), arXiv:1605.01209 [hep-ph]. [17] M. Emma, F. Schianchi, F. Pannarale, V. Sagun, and T. Dietrich, Particles 5, 273 (2022), arXiv:2206.10887 [grqc]. [18] M. Punturo et al., Class. Quant. Grav. 27, 194002 (2010). [19] C. Mills, V. Tiwari, and S. Fairhurst, Phys. Rev. D 97, 104064 (2018), arXiv:1708.00806 [gr-qc]. [20] K. Ackley et al., Publ. Astron. Soc. Austral. 37, e047 (2020), arXiv:2007.03128 [astro-ph.HE]. [21] V. Sagun, E. Giangrandi, O. Ivanytskyi, C. Providˆencia, and T. Dietrich, EPJ Web Conf. 274, 07009 (2022), arXiv:2211.10510 [astro-ph.HE]. [22] S. Shakeri and D. R. Karkevandi, arxiv (2022), arXiv:2210.17308 [astro-ph.HE]. [23] T. Sales, O. Louren¸co, M. Dutra, and R. Negreiros, Astron. Astrophys. 642, A42 (2020), arXiv:2004.05019 [astro-ph.HE]. [24] D. Page, J. M. Lattimer, M. Prakash, and A. W. Steiner, Astrophys. J. Suppl. 155, 623 (2004), arXiv:astroph/0403657. [25] J. M. Lattimer, K. A. van Riper, M. Prakash, and M. Prakash, Astrophys. J. 425, 802 (1994). [26] D. Page, U. Geppert, and F. Weber, Nucl. Phys. A 777, 497 (2006), arXiv:astro-ph/0508056. [27] J. M. Lattimer, M. Prakash, C. J. Pethick, and P. Haensel, Phys. Rev. Lett. 66, 2701 (1991). [28] A. Y. Potekhin, J. A. Pons, and D. Page, Space Sci. Rev. 191, 239 (2015), arXiv:1507.06186 [astro-ph.HE]. [29] R. Wijnands, N. Degenaar, and D. Page, J. Astrophys. Astron. 38, 49 (2017), arXiv:1709.07034 [astro-ph.HE]. 10 [30] D. N. Aguilera, J. A. Pons, and J. A. Miralles, Astrophys. J. Lett. 673, L167 (2008), arXiv:0712.1353 [astroph]. [31] G. Baym, D. Beck, P. Geltenbort, and J. Shelton, Physical Review Letters 121 (2018), 10.1103/physrevlett.121.061801. [32] T. F. Motta, P. A. M. Guichon, and A. W. Thomas, Journal of Physics G: Nuclear and Particle Physics 45, 05LT01 (2018). [33] T. F. Motta, P. A. M. Guichon, and A. W. Thomas, International Journal of Modern Physics A 33, 1844020 (2018). [34] J. M. Berryman, S. Gardner, and M. Zakeri, Symmetry 14, 518 (2022), arXiv:2201.02637 [hep-ph]. [35] R. Garani and S. Palomares-Ruiz, JCAP 05, 042 (2022), arXiv:2104.12757 [hep-ph]. [36] T. Dietrich and K. Clough, Phys. Rev. D 100, 083005 (2019), arXiv:1909.01278 [gr-qc]. [37] A. Sedrakian, Phys. Rev. D 93, 065044 (2016), arXiv:1512.07828 [astro-ph.HE]. [38] M. Buschmann, R. T. Co, C. Dessert, and B. R. Safdi, Phys. Rev. Lett. 126, 021102 (2021), arXiv:1910.04164 [hep-ph]. [39] M. Buschmann, C. Dessert, J. W. Foster, A. J. Long, and B. R. Safdi, Phys. Rev. Lett. 128, 091102 (2022), arXiv:2111.09892 [hep-ph]. [40] A. de Lavallaz and M. Fairbairn, Phys. Rev. D 81, 123521 (2010), arXiv:1004.0629 [ astro-ph.GA ]. [41] M. Angeles P´erez-Garc´ıa, H. Grigorian, C. Albertus, ´ D. Barba, and J. Silk, Phys. Lett. B 827, 136937 (2022), arXiv:2202.00702 [hep-ph]. [42] K. Hamaguchi, N. Nagata, and K. Yanagi, Phys. Lett. B 795, 484 (2019), arXiv:1905.02991 [hep-ph]. [43] C. Kouvaris, Physical Review D 77 (2008), 10.1103/physrevd.77.023006. [44] S. Chatterjee, R. Garani, R. K. Jain, B. Kanodia, M. S. N. Kumar, and S. K. Vempati, Phys. Rev. D 108, L021301 (2023), arXiv:2205.05048 [astro-ph.HE]. [45] V. V. Sagun, A. I. Ivanytskyi, K. A. Bugaev, and I. N. Mishustin, Nucl. Phys. A 924, 24 (2014), arXiv:1306.2372 [nucl-th]. [46] V. V. Sagun, K. A. Bugaev, A. I. Ivanytskyi, I. P. Yakimenko, E. G. Nikonov, A. V. Taranenko, C. Greiner, D. B. Blaschke, and G. M. Zinovjev, Eur. Phys. J. A 54, 100 (2018), arXiv:1703.00049 [hep-ph]. [47] K. A. Bugaev et al., Int. J. Mod. Phys. A 36, 2141009 (2021), arXiv:2104.05351 [hep-ph]. [48] V. V. Sagun, K. A. Bugaiev, A. I. Ivanytskyi, D. R. Oliinychenko, and I. N. Mishustin, EPJ Web Conf. 137, 09007 (2017), arXiv:1611.07071 [nucl-th]. [49] V. V. Sagun, I. Lopes, and A. I. Ivanytskyi, Astrophys. J. 871, 157 (2019), arXiv:1805.04976 [astro-ph.HE]. [50] V. Sagun, G. Panotopoulos, and I. Lopes, Phys. Rev. D 101, 063025 (2020). [51] L. Tolos, M. Centelles, and A. Ramos, Publ. Astron. Soc. Austral. 34, e065 (2017), arXiv:1708.08681 [astroph.HE]. [52] W.-C. Chen and J. Piekarewicz, Phys. Rev. C 90, 044305 (2014), arXiv:1408.4159 [nucl-th]. [53] P. Danielewicz, R. Lacey, and W. G. Lynch, Science 298, 1592 (2002), arXiv:nucl-th/0208016. [54] A. I. Ivanytskyi, K. A. Bugaev, V. V. Sagun, L. V. Bravina, and E. E. Zabrodin, Phys. Rev. C 97, 064905 (2018), arXiv:1710.08218 [nucl-th]. [55] B. P. Abbott et al. (The LIGO Scientific Collaboration and the Virgo Collaboration), Phys. Rev. Lett. 121, 1611012013Sci...340..448A (2018). [56] B. P. Abbott et al. (LIGO Scientific, Virgo), Astrophys. J. Lett. 892, L3 (2020), arXiv:2001.01761 [astro-ph.HE]. [57] M. C. Miller et al., Astrophys. J. Lett. 887, L24 (2019), arXiv:1912.05705 [astro-ph.HE]. [58] T. E. Riley et al., Astrophys. J. Lett. 887, L21 (2019), arXiv:1912.05702 [astro-ph.HE]. [59] G. Raaijmakers et al., Astrophys. J. Lett. 893, L21 (2020), arXiv:1912.11031 [astro-ph.HE]. [60] M. C. Miller et al., Astrophys. J. Lett. 918, L28 (2021), arXiv:2105.06979 [astro-ph.HE]. [61] T. E. Riley et al., Astrophys. J. Lett. 918, L27 (2021), arXiv:2105.06980 [astro-ph.HE]. [62] P. Haensel and J. L. Zdunik, Astron. and Astrophys. 227, 431 (1990). [63] J. W. Negele and D. Vautherin, Nucl. Phys. A 207, 298 (1973). [64] A. Nelson, S. Reddy, and D. Zhou, JCAP 07, 012 (2019), arXiv:1803.03266 [hep-ph]. [65] R. C. Tolman, Phys. Rev. 55, 364 (1939). [66] J. R. Oppenheimer and G. M. Volkoff, Phys. Rev. 55, 374 (1939). [67] J. Antoniadis et al., Science 340, 6131 (2013), arXiv:1304.6875 [astro-ph.HE]. [68] R. W. Romani, D. Kandel, A. V. Filippenko, T. G. Brink, and W. Zheng, Astrophys. J. Lett. 908, L46 (2021), arXiv:2101.09822 [astro-ph.HE]. [69] R. W. Romani, D. Kandel, A. V. Filippenko, T. G. Brink, and W. Zheng, Astrophys. J. Lett. 934, L17 (2022), arXiv:2207.05124 [astro-ph.HE]. [70] G. Raaijmakers, S. K. Greif, K. Hebeler, T. Hinderer, S. Nissanke, A. Schwenk, T. E. Riley, A. L. Watts, J. M. Lattimer, and W. C. G. Ho, Astrophys. J. Lett. 918, L29 (2021), arXiv:2105.06981 [astro-ph.HE]. [71] B. P. Abbott et al. (LIGO Scientific, Virgo), Phys. Rev. Lett. 121, 161101 (2018), arXiv:1805.11581 [gr-qc]. [72] V. Doroshenko, V. Suleimanov, G. P¨uhlhofer, and et al., Nature Astronomy 6, 1444 (2022). [73] J. Bardeen, L. N. Cooper, and J. R. Schrieffer, Phys. Rev. 108, 1175 (1957). [74] D. Page, “NSCool: Neutron star cooling code,” Astrophysics Source Code Library, record ascl:1609.009 (2016), ascl:1609.009. [75] W. C. G. Ho, K. G. Elshamouty, C. O. Heinke, and A. Y. Potekhin, Phys. Rev. C 91, 015806 (2015), arXiv:1412.7759 [astro-ph.HE]. [76] M. V. Beznogov and D. G. Yakovlev, Mon. Not. Roy. Astron. Soc. 447, 1598 (2015), arXiv:1411.6803 [ astroph.SR ]. [77] R. Negreiros, L. Tolos, M. Centelles, A. Ramos, and V. Dexheimer, Astrophys. J. 863, 104 (2018), arXiv:1804.00334 [astro-ph.HE]. [78] S. Tsiopelas and V. Sagun, Particles 3, 693 (2020), arXiv:2006.06351 [astro-ph.HE]. [79] S. Tsiopelas and V. Sagun, Astron. Nachr. 342, 332 (2021). [80] A. Schwenk, B. Friman, and G. E. Brown, Nucl. Phys. A 713, 191 (2003), arXiv:nucl-th/0207004. [81] J. M. C. Chen, J. W. Clark, R. D. Dav´e, and V. V. Khodel, Nucl. Phys. A 555, 59 (1993). [82] V. Sagun, E. Giangrandi, T. Dietrich, O. Ivanyt- 11 skyi, R. Negreiros, and C. Providˆencia, (2023), arXiv:2306.12326 [astro-ph.HE]. [83] W. C. G. Ho and C. O. Heinke, Nature 462, 71 (2009), arXiv:0911.0672 [astro-ph.HE]. [84] C. O. Heinke and W. C. G. Ho, Astrophys. J. Lett. 719, L167 (2010), arXiv:1007.4719 [astro-ph.HE]. [85] P. S. Shternin, D. G. Yakovlev, C. O. Heinke, W. C. G. Ho, and D. J. Patnaude, Mon. Not. Roy. Astron. Soc. 412, L108 (2011), arXiv:1012.0045 [ astro-ph.SR ]. [86] K. G. Elshamouty, C. O. Heinke, G. R. Sivakoff, W. C. G. Ho, P. S. Shternin, D. G. Yakovlev, D. J. Patnaude, and L. David, Astrophys. J. 777, 22 (2013), arXiv:1306.3387 [astro-ph.HE]. [87] M. J. P. Wijngaarden, W. C. G. Ho, P. Chang, C. O. Heinke, D. Page, M. Beznogov, and D. J. Patnaude, Mon. Not. Roy. Astron. Soc. 484, 974 (2019), arXiv:1901.01012 [astro-ph.HE]. [88] P. S. Shternin, D. D. Ofengeim, C. O. Heinke, and W. C. G. Ho, Mon. Not. Roy. Astron. Soc. 518, 2775 (2022), arXiv:2211.02526 [astro-ph.HE]. [89] D. Page, M. Prakash, J. M. Lattimer, and A. W. Steiner, Phys. Rev. Lett. 106, 081101 (2011), arXiv:1011.6142 [astro-ph.HE]. [90] G. Taranto, G. F. Burgio, and H. J. Schulze, Mon. Not. Roy. Astron. Soc. 456, 1451 (2016), arXiv:1511.04243 [nucl-th]. [91] D. Blaschke, H. Grigorian, D. N. Voskresensky, and F. Weber, Phys. Rev. C 85, 022802 (2012), arXiv:1108.4125 [nucl-th]. [92] K. Hamaguchi, N. Nagata, K. Yanagi, and J. Zheng, Phys. Rev. D 98, 103015 (2018), arXiv:1806.07151 [hepph]. [93] T. Takatsuka, Progress of Theoretical Physics 48, 1517 (1972), https://academic.oup.com/ptp/articlepdf/48/5/1517/5328994/48-5-1517.pdf . [94] R. Cassano et al., arXiv (2018), arXiv:1807.09080 [astroph.HE]. [95] J. J. M. in ’t Zand et al. (eXTP), Sci. China Phys. Mech. Astron. 62, 029506 (2019), arXiv:1812.04023 [astroph.HE]. [96] P. S. Ray et al. (STROBE-X Science Working Group), arxiv (2019), arXiv:1903.03035 [ astro-ph.IM ]. 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