The second transition is the well-known vortex phase transition. from the ACS website, either in whole or in part, in either machine-readable form or any other form ‐TaS x��=M�$�qw�sL���M6���#8�n��";:�J��!�>M���*����2Yz=M�X��*Vx������Ï_n?~x�������}���/_~��>|���Ӈ?����×��ۇ?��I�����姿�ﷷO���w�~��o�ܾ�������o�m�u7o�������/��Z���?�~���Sß�����? The low-energy 1D vortex spectrum can be utilized to distinguish between HOTI (with chiral hinge states) from a conventional TI. Structure, Preparation, and Applications of 2D Material‐Based Metal–Semiconductor Heterostructures. Superconducting simulators are used to investigate dynamical phase transitions, revealing their applications in quantum metrology. <> Find more information about Crossref citation counts. %PDF-1.5 2. Sample preparation for 1T-TaS2 flakes; low-temperature Raman characterization for a 1T-TaS2 flake before and after annealing (PDF). endobj Jan Ravnik, Igor Vaskivskyi, Yaroslav Gerasimenko, Michele Diego, Jaka Vodeb, Viktor Kabanov. Learn More ». stream The monolayer 2H-TaS2 on bulk 1T-TaS2 exhibits a superconducting transition temperature (Tc) of 2.1 K, which is significantly enhanced compared to that of bulk 2H-TaS2. In this work, we show that the phenomenology in higher-order topological insulators (HOTIs) can be qualitatively distinct. without permission from the American Chemical Society. 2 We believe our work provides new phenomenology that can help identify HOTIs, as well as illustrating a promising platform for the realization of MZMs. of phase transitions is the way it to materialize. Experimental observations and density functional simulations on the structural transition behavior of a two-dimensional transition-metal dichalcogenide. *���O�����o>�s�yM7��b������m��Ϳ��uĺ��f��}���v������?���M��۶l+Ī}^f]�:�7���y5�WN��G N�2S)���3��L릗�O���j1�@�gG`o��3�.,[���Yb��������DOʦMձ;!ml��avU����}�K��w���.=7�������!�w�����{���/�����0����cW��c��=����y��xK�■������:�w�=䱾̃� B�L[c�K� ���p��w�_�Jx�P�_����H�Z���Q@���t�[��t�$:�$�A�4:,���&$A��LG�G�1�ƣ�8|E���ɧ�9��]��2Mk�7&�¾��=��C�7�8/�Vϼ�I���n5����e��?w�sOx�(D�vj>�kk6|˻4� Z�w���;�1,z�;� ��p���j)����_�e�8&�/��^m>#�纸ȦLp�D��a랇��. This parameter vanishes at the transition between two topological superconducting phases with opposite Chern numbers, see figure 3(b) . in situ (e) Hinge modes, (f) surface phase transition at μc,1, (g) Majorana zero modes, (h) vortex phase transition at μc,2. Through this difficult time APS and the Physical Review editorial office are fully equipped and actively working to support researchers by continuing to carry out all editorial and peer-review functions and publish research in the journals as well as minimizing disruption to journal access. Subscription Scanning tunneling microscopy measurements reveal a 3 × 3 charge density wave (CDW) in the phase-switched monolayer at 4.5 K. The enhanced Tc is explained by the suppressed 3 × 3 CDW and a charge-transfer doping from the 1T substrate. (e)–(h) The evolution of the probability density profile of the lowest energy states when a vortex is inserted perpendicular to the y−z surface and μ is tuned. Your Mendeley pairing has expired. In such a field, the system acts as a chain of S-I-N junctions. Enhanced Superconductivity in Few-Layer TaS2 due to Healing by Oxygenation. Files available from the ACS website may be downloaded for personal use only. Construction of Ta-Cu7S4 negative electrode for high-performance all-solid-state asymmetric supercapacitor. Department of Chemistry, Centre for Advanced 2D Materials, National University of Singapore, Singapore 117543, State Key Laboratory of High Performance Ceramics and Superfine Microstructure, Shanghai Institute of Ceramics, Chinese Academy of Sciences, Shanghai 201899, China, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Science, Changchun 130033, China, National Synchrotron Radiation Laboratory, University of Science and Technology of China, Hefei 230026, China, Surface-Limited Superconducting Phase Transition on 1. The existence of t… H. H. Huang, Xiaofeng Fan, David J. Singh, W. T. Zheng. M=−2, t1=1, t2=1(HOTI), δ0=0.2. Duan Zhang, Yecun Wu, Yu-Hsin Su, Ming-Chien Hsu, Cormac Ó Coileáin, Jiung Cho, Miri Choi, Byong Sun Chun, Yao Guo, Ching-Ray Chang, Han-Chun Wu. https://doi.org/10.1103/PhysRevLett.125.037001, Physical Review Physics Education Research, Log in with individual APS Journal Account », Log in with a username/password provided by your institution », Get access through a U.S. public or high school library ». The second transition is the well-known vortex phase transition. For instance, all superconductors have exactly zero resistivity to low applied currents when there is no magnetic field present or if the applied field does not exceed a critical value. redistribute this material, requesters must process their own requests via the RightsLink permission The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. heating and electron beam irradiation. The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/acsnano.8b07379. In particular, we find two distinct features. In particular case of normal – superconducting phase transitions we have shown that (1) the norm al and superconduc ting crystal structur es are … In particular case of normal – superconducting phase transitions we have shown that (1) the normal and superconducting crystal structures are not identical, (2) the phase transition between them proceeds by a structuralepitaxial Junyang Tan, Shisheng Li, Bilu Liu, Hui-Ming Cheng. And we hope you, and your loved ones, are staying safe and healthy. Yahuan Huan, Jianping Shi, Xiaolong Zou, Yue Gong, Chunyu Xie, Zhongjie Yang, Zhepeng Zhang, Yan Gao, Yuping Shi, Minghua Li, Pengfei Yang, Shaolong Jiang, Min Hong, Lin Gu, Qing Zhang, Xiaoqin Yan. 3 0 obj Ruicong Xie, Min Hu, Dongqi Liu, Yanying Yu, Chao Li, Jia He, Jun Luo. This article is cited by Thickness-Controlled Synthesis of CoX2 (X = S, Se, and Te) Single Crystalline 2D Layers with Linear Magnetoresistance and High Conductivity. endobj Please reconnect. Scalable Production of Two-Dimensional Metallic Transition Metal Dichalcogenide Nanosheet Powders Using NaCl Templates toward Electrocatalytic Applications. http://pubs.acs.org/page/copyright/permissions.html, https://doi.org/10.1021/acs.nanolett.0c00871, https://doi.org/10.1021/acs.chemmater.9b04416, https://doi.org/10.1016/j.cej.2020.126471, https://doi.org/10.1038/s41598-020-75240-0, https://doi.org/10.1107/S2052252520011021, https://doi.org/10.1007/s40843-018-9398-1. The observed surface-limited superconducting phase transition offers a convenient way to prepare robust 2D superconductivity on bulk 1T-TaS2 crystal, thereby bypassing the need to exfoliate monolayer samples. Surface phase transition in a superconducting HOTI. ISSN 1079-7114 (online), 0031-9007 (print). Yao Xiao, Mengyue Zhou, Jinglu Liu, Jing Xu, Lei Fu. (d) μc,1 versus t2. Find more information on the Altmetric Attention Score and how the score is calculated. We further show that the monolayer 2H-TaS2 could be switched back to 1T phase by applying a voltage pulse. Environmental Control of Charge Density Wave Order in Monolayer 2H-TaS2. 2 Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Users are Such quantum transition can occur if the magnetic field is tuned such that it suppresses superconductivity in the islands with the weaker critical field, while the islands with stronger energy gap remain superconducting. Recent progress of TMD nanomaterials: phase transitions and applications. P Tsuppayakorn-aek, W Pungtrakool, U Pinsook, T Bovornratanaraks. (a)–(c) The evolution of surface states in the y−z plane for μ=0.1, 0.33, 0.4, respectively. Phase engineering of two-dimensional transition metal dichalcogenides. Information. 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