000860516 001__ 860516
000860516 005__ 20230426083205.0
000860516 0247_ $$2doi$$a10.1103/PhysRevB.93.115415
000860516 0247_ $$2ISSN$$a0163-1829
000860516 0247_ $$2ISSN$$a0556-2805
000860516 0247_ $$2ISSN$$a1050-2947
000860516 0247_ $$2ISSN$$a1094-1622
000860516 0247_ $$2ISSN$$a1095-3795
000860516 0247_ $$2ISSN$$a1098-0121
000860516 0247_ $$2ISSN$$a1538-4489
000860516 0247_ $$2ISSN$$a1550-235X
000860516 0247_ $$2ISSN$$a2469-9950
000860516 0247_ $$2ISSN$$a2469-9969
000860516 0247_ $$2Handle$$a2128/21547
000860516 0247_ $$2WOS$$aWOS:000371734800007
000860516 037__ $$aFZJ-2019-01252
000860516 082__ $$a530
000860516 1001_ $$0P:(DE-HGF)0$$aIshida, H.$$b0
000860516 245__ $$aRelationship between embedding-potential eigenvalues and topological invariants of time-reversal invariant band insulators
000860516 260__ $$aWoodbury, NY$$bInst.$$c2016
000860516 3367_ $$2DRIVER$$aarticle
000860516 3367_ $$2DataCite$$aOutput Types/Journal article
000860516 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1549380249_11543
000860516 3367_ $$2BibTeX$$aARTICLE
000860516 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000860516 3367_ $$00$$2EndNote$$aJournal Article
000860516 520__ $$aThe embedding potential defined on the boundary surface of a semi-infinite crystal relates the value and normal derivative of generalized Bloch states propagating or decaying toward the interior of the crystal. It becomes Hermitian when the electron energy ε is located in a projected bulk band gap at a given wave vector k in the surface Brillouin zone (SBZ). If one plots the real eigenvalues of the embedding potential for a time-reversal invariant insulator in the projected bulk band gap along a path ε=ε0(k) passing between two time-reversal invariant momentum (TRIM) points in the SBZ, then, they form Kramers doublets at both end points. We will demonstrate that the Z2 topological invariant, ν, which is either 0 or 1, depending on the product of time-reversal polarizations at the two TRIM points, can be determined from the two different ways these eigenvalues are connected between the two TRIM points. Furthermore, we will reveal a relation, ν=P mod 2, where P denotes the number of poles that the embedding potential exhibits along the path. We also discuss why gapless surface states crossing the bulk band gap inevitably occur on the surface of topological band insulators from the view point of the embedding theory.
000860516 536__ $$0G:(DE-HGF)POF3-143$$a143 - Controlling Configuration-Based Phenomena (POF3-143)$$cPOF3-143$$fPOF III$$x0
000860516 542__ $$2Crossref$$i2016-03-09$$uhttp://link.aps.org/licenses/aps-default-license
000860516 588__ $$aDataset connected to CrossRef
000860516 7001_ $$0P:(DE-Juel1)131042$$aWortmann, D.$$b1$$ufzj
000860516 77318 $$2Crossref$$3journal-article$$a10.1103/physrevb.93.115415$$bAmerican Physical Society (APS)$$d2016-03-09$$n11$$p115415$$tPhysical Review B$$v93$$x2469-9950$$y2016
000860516 773__ $$0PERI:(DE-600)2844160-6$$a10.1103/PhysRevB.93.115415$$gVol. 93, no. 11, p. 115415$$n11$$p115415$$tPhysical review / B$$v93$$x2469-9950$$y2016
000860516 8564_ $$uhttps://juser.fz-juelich.de/record/860516/files/PhysRevB.93.115415.pdf$$yOpenAccess
000860516 8564_ $$uhttps://juser.fz-juelich.de/record/860516/files/PhysRevB.93.115415.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000860516 909CO $$ooai:juser.fz-juelich.de:860516$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000860516 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131042$$aForschungszentrum Jülich$$b1$$kFZJ
000860516 9131_ $$0G:(DE-HGF)POF3-143$$1G:(DE-HGF)POF3-140$$2G:(DE-HGF)POF3-100$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bEnergie$$lFuture Information Technology - Fundamentals, Novel Concepts and Energy Efficiency (FIT)$$vControlling Configuration-Based Phenomena$$x0
000860516 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS
000860516 915__ $$0StatID:(DE-HGF)0600$$2StatID$$aDBCoverage$$bEbsco Academic Search
000860516 915__ $$0LIC:(DE-HGF)APS-112012$$2HGFVOC$$aAmerican Physical Society Transfer of Copyright Agreement
000860516 915__ $$0StatID:(DE-HGF)0100$$2StatID$$aJCR$$bPHYS REV B : 2017
000860516 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000860516 915__ $$0StatID:(DE-HGF)0110$$2StatID$$aWoS$$bScience Citation Index
000860516 915__ $$0StatID:(DE-HGF)0111$$2StatID$$aWoS$$bScience Citation Index Expanded
000860516 915__ $$0StatID:(DE-HGF)9900$$2StatID$$aIF < 5
000860516 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000860516 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bASC
000860516 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences
000860516 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000860516 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List
000860516 9201_ $$0I:(DE-Juel1)IAS-1-20090406$$kIAS-1$$lQuanten-Theorie der Materialien$$x0
000860516 9201_ $$0I:(DE-Juel1)PGI-1-20110106$$kPGI-1$$lQuanten-Theorie der Materialien$$x1
000860516 9201_ $$0I:(DE-82)080009_20140620$$kJARA-FIT$$lJARA-FIT$$x2
000860516 9201_ $$0I:(DE-82)080012_20140620$$kJARA-HPC$$lJARA - HPC$$x3
000860516 980__ $$ajournal
000860516 980__ $$aVDB
000860516 980__ $$aUNRESTRICTED
000860516 980__ $$aI:(DE-Juel1)IAS-1-20090406
000860516 980__ $$aI:(DE-Juel1)PGI-1-20110106
000860516 980__ $$aI:(DE-82)080009_20140620
000860516 980__ $$aI:(DE-82)080012_20140620
000860516 9801_ $$aFullTexts
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/RevModPhys.82.3045
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/RevModPhys.83.1057
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/0034-4885/75/9/096501
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1002/pssr.201206414
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.95.226801
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1126/science.1133734
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/nphys1270
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/1367-2630/12/6/065013
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1038/nphys1274
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.105.076802
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1209/0295-5075/90/37002
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.105.036404
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.105.136802
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.105.146801
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.105.266401
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.95.146802
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.74.195312
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.75.121306
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.98.106803
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.76.045302
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.78.045426
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1143/JPSJ.76.053702
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.83.035108
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.83.235401
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.84.075119
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1557/mrs.2014.216
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/0022-3719/14/26/015
000860516 999C5 $$1J. E. Inglesfield$$2Crossref$$9-- missing cx lookup --$$a10.1088/978-0-7503-1042-0$$y2015
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/S0010-4655(01)00173-4
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.53.8052
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.81.155439
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.65.165103
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.66.075113
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.63.165409
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.90.235422
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.71.155120
000860516 999C5 $$1D. J. Singh$$2Crossref$$oD. J. Singh Planewaves, Pseudopotentials, and the LAPW Method 2006$$tPlanewaves, Pseudopotentials, and the LAPW Method$$y2006
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.77.3865
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1186/1556-276X-6-126
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.81.115106
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1107/S0365110X62002297
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.72.085410
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.86.115208
000860516 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevB.88.041404