Group 14 element-based non-centrosymmetric quantum spin Hall insulators with large bulk gap
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Aijun Du | Thomas Heine | Liangzhi Kou | A. Du | L. Kou | T. Heine | Yandong Ma | Yandong Ma | Liangzhi Kou
[1] Baibiao Huang,et al. Halogenated two-dimensional germanium: candidate materials for being of Quantum Spin Hall state , 2012 .
[2] E. Krasovskii,et al. Experimental realization of a three-dimensional topological insulator phase in ternary chalcogenide TlBiSe₂. , 2010, Physical review letters.
[3] Ying Dai,et al. Intriguing Behavior of Halogenated Two-Dimensional Tin , 2012 .
[4] Hasan Sahin,et al. Monolayer honeycomb structures of group-IV elements and III-V binary compounds: First-principles calculations , 2009, 0907.4350.
[5] Binghai Yan,et al. Single Dirac cone topological surface state and unusual thermoelectric property of compounds from a new topological insulator family. , 2010, Physical review letters.
[6] K. Novoselov,et al. Control of Graphene's Properties by Reversible Hydrogenation: Evidence for Graphane , 2008, Science.
[7] Shuichi Murakami,et al. Quantum spin Hall effect and enhanced magnetic response by spin-orbit coupling. , 2006, Physical review letters.
[8] Ying Dai,et al. Strain-induced quantum spin Hall effect in methyl-substituted germanane GeCH3 , 2014, Scientific Reports.
[9] Cheng-Cheng Liu,et al. Quantum spin Hall insulators and quantum valley Hall insulators of BiX/SbX (X = H, F, Cl, and Br) monolayers with a record bulk band gap , 2014 .
[10] G. Sullivan,et al. Evidence for helical edge modes in inverted InAs/GaSb quantum wells. , 2011, Physical review letters.
[11] E. J. Mele,et al. Quantum spin Hall effect in graphene. , 2004, Physical review letters.
[12] Tanmoy Das,et al. Prediction of large-gap two-dimensional topological insulators consisting of bilayers of group III elements with Bi. , 2014, Nano letters.
[13] Thomas Frauenheim,et al. Robust two-dimensional topological insulators in methyl-functionalized bismuth, antimony, and lead bilayer films. , 2015, Nano letters.
[14] Thomas Frauenheim,et al. Robust 2D topological insulators in van der Waals heterostructures. , 2014, ACS nano.
[15] Xi Dai,et al. Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface , 2009 .
[16] Binghai Yan,et al. Large-gap quantum spin Hall insulators in tin films. , 2013, Physical review letters.
[17] L. Molenkamp,et al. Quantum Hall effect from the topological surface states of strained bulk HgTe. , 2011, Physical review letters.
[18] Z. K. Liu,et al. Experimental Realization of a Three-Dimensional Topological Insulator , 2010 .
[19] Cheng-Cheng Liu,et al. Low-energy effective Hamiltonian involving spin-orbit coupling in silicene and two-dimensional germanium and tin , 2011, 1108.2933.
[20] H. Monkhorst,et al. SPECIAL POINTS FOR BRILLOUIN-ZONE INTEGRATIONS , 1976 .
[21] Bing-Lin Gu,et al. Functionalized germanene as a prototype of large-gap two-dimensional topological insulators , 2014, 1401.4100.
[22] G. Kresse,et al. Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set , 1996 .
[23] R. Arita,et al. Emergence of non-centrosymmetric topological insulating phase in BiTeI under pressure , 2011, Nature Communications.
[24] Shou-Cheng Zhang,et al. Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells , 2006, Science.
[25] G. Scuseria,et al. Hybrid functionals based on a screened Coulomb potential , 2003 .
[26] G. Barber,et al. Graphane: a two-dimensional hydrocarbon , 2006, cond-mat/0606704.
[27] Joel E Moore,et al. The birth of topological insulators , 2010, Nature.
[28] R. Cava,et al. Observation of a large-gap topological-insulator class with a single Dirac cone on the surface , 2009 .
[29] E. Akturk,et al. Two- and one-dimensional honeycomb structures of silicon and germanium. , 2008, Physical review letters.
[30] Z. Hussain,et al. Discovery of a single topological Dirac fermion in the strong inversion asymmetric compound BiTeCl , 2013, Nature Physics.
[31] G. Kresse,et al. From ultrasoft pseudopotentials to the projector augmented-wave method , 1999 .
[32] C. Felser,et al. A large-energy-gap oxide topological insulator based on the superconductor BaBiO3 , 2013, Nature Physics.
[33] Burke,et al. Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.
[34] Kresse,et al. Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. , 1996, Physical review. B, Condensed matter.
[35] X. Dai,et al. Transition-Metal Pentatelluride ZrTe 5 and HfTe 5 : A Paradigm for Large-Gap Quantum Spin Hall Insulators , 2013, 1309.7529.
[36] L. Molenkamp,et al. Quantum Spin Hall Insulator State in HgTe Quantum Wells , 2007, Science.
[37] C. Kane,et al. Topological Insulators , 2019, Electromagnetic Anisotropy and Bianisotropy.
[38] L. Fu,et al. Quantum Spin Hall Effect and Topological Field Effect Transistor in Two-Dimensional Transition Metal Dichalcogenides , 2014, 1406.2749.
[39] Ping Li,et al. Epitaxial growth of large-gap quantum spin Hall insulator on semiconductor surface , 2014, Proceedings of the National Academy of Sciences.
[40] Ashvin Vishwanath,et al. Subject Areas : Strongly Correlated Materials A Viewpoint on : Topological semimetal and Fermi-arc surface states in the electronic structure of pyrochlore iridates , 2011 .
[41] L. Fu,et al. Quantum spin Hall effect in two-dimensional transition metal dichalcogenides , 2014, Science.
[42] Cheng-Cheng Liu,et al. Quantum spin Hall effect in silicene and two-dimensional germanium. , 2011, Physical review letters.