001     1044177
005     20250912110200.0
024 7 _ |a 10.1103/h8v9-sl53
|2 doi
024 7 _ |a 2469-9950
|2 ISSN
024 7 _ |a 2469-9977
|2 ISSN
024 7 _ |a 0163-1829
|2 ISSN
024 7 _ |a 0556-2805
|2 ISSN
024 7 _ |a 1095-3795
|2 ISSN
024 7 _ |a 1098-0121
|2 ISSN
024 7 _ |a 1538-4489
|2 ISSN
024 7 _ |a 1550-235X
|2 ISSN
024 7 _ |a 2469-9969
|2 ISSN
024 7 _ |a 10.34734/FZJ-2025-03066
|2 datacite_doi
024 7 _ |a WOS:001539380900006
|2 WOS
037 _ _ |a FZJ-2025-03066
082 _ _ |a 530
100 1 _ |a Bagchi, Mahasweta
|0 P:(DE-HGF)0
|b 0
245 _ _ |a Quasiparticle interference on the surface of Bi 2 Se 3 -terminated (PbSe) 5 ( Bi 2 Se 3 ) 6
260 _ _ |a Woodbury, NY
|c 2025
|b Inst.
336 7 _ |a article
|2 DRIVER
336 7 _ |a Output Types/Journal article
|2 DataCite
336 7 _ |a Journal Article
|b journal
|m journal
|0 PUB:(DE-HGF)16
|s 1752737752_21156
|2 PUB:(DE-HGF)
336 7 _ |a ARTICLE
|2 BibTeX
336 7 _ |a JOURNAL_ARTICLE
|2 ORCID
336 7 _ |a Journal Article
|0 0
|2 EndNote
520 _ _ |a Among the family of topological superconductors derived from Bi 2 Se 3 , Cux (PbSe) 5 (Bi 2 Se 3 ) 6 is unique in its surface termination of a single quintuple layer (QL) of the topological insulator (TI) Bi 2 Se 3 on an ordinaryinsulator PbSe. Here, we report a combined scanning tunneling microscopy (STM) and density functional theory (DFT) characterization of the cleaved surface of the parent compound (PbSe)5 (Bi 2 Se 3 ) 6 (PSBS). Interestingly,the potential disorder due to the random distribution of native defects is only ∼ 4 meV, comparable to the smallest reported for TIs. Performing high-resolution quasiparticle interference imaging (QPI) near the Fermienergy (E − EF = −1 to 0.6 eV) we reconstruct the dispersion relation of the dominant spectral feature and our ab initio calculations show that this surface feature originates from two bands with Rashba-like splitting dueto strong spin-orbit coupling and inversion symmetry breaking. Moreover, only a small hexagonal distortion of the calculated Fermi surface is seen in the full momentum space distribution of the measured scattering data.Nevertheless, the scattering pattern at lower energies transforms into a flowerlike shape with suppressed intensity along the K direction. We show that this effect is not due to the forbidden backscattering in the spin-momentumlocked surface state in Bi 2 Se 3 but reflects the threefold symmetry of the scattering potential.
536 _ _ |a 5211 - Topological Matter (POF4-521)
|0 G:(DE-HGF)POF4-5211
|c POF4-521
|f POF IV
|x 0
588 _ _ |a Dataset connected to CrossRef, Journals: juser.fz-juelich.de
700 1 _ |a Rüssmann, Philipp
|0 P:(DE-Juel1)157882
|b 1
|u fzj
700 1 _ |a Bihlmayer, Gustav
|0 P:(DE-Juel1)130545
|b 2
|e Corresponding author
700 1 _ |a Blügel, Stefan
|0 P:(DE-Juel1)130548
|b 3
700 1 _ |a Ando, Yoichi
|0 P:(DE-HGF)0
|b 4
700 1 _ |a Brede, Jens
|0 P:(DE-HGF)0
|b 5
773 _ _ |a 10.1103/h8v9-sl53
|g Vol. 112, no. 4, p. 045411
|0 PERI:(DE-600)2844160-6
|n 4
|p 045411
|t Physical review / B
|v 112
|y 2025
|x 2469-9950
856 4 _ |u https://juser.fz-juelich.de/record/1044177/files/h8v9-sl53.pdf
|y OpenAccess
909 C O |o oai:juser.fz-juelich.de:1044177
|p openaire
|p open_access
|p VDB
|p driver
|p dnbdelivery
910 1 _ |a Physics Institute II, University of Cologne, D-50937 Köln, Germany
|0 I:(DE-HGF)0
|b 0
|6 P:(DE-HGF)0
910 1 _ |a Forschungszentrum Jülich
|0 I:(DE-588b)5008462-8
|k FZJ
|b 1
|6 P:(DE-Juel1)157882
910 1 _ |a Institute for Theoretical Physics and Astrophysics, University of Würzburg, 97074 Würzburg, Germany
|0 I:(DE-HGF)0
|b 1
|6 P:(DE-Juel1)157882
910 1 _ |a Forschungszentrum Jülich
|0 I:(DE-588b)5008462-8
|k FZJ
|b 2
|6 P:(DE-Juel1)130545
910 1 _ |a Forschungszentrum Jülich
|0 I:(DE-588b)5008462-8
|k FZJ
|b 3
|6 P:(DE-Juel1)130548
910 1 _ |a Physics Institute II, University of Cologne, D-50937 Köln, Germany
|0 I:(DE-HGF)0
|b 4
|6 P:(DE-HGF)0
910 1 _ |a Physics Institute II, University of Cologne, D-50937 Köln, Germany
|0 I:(DE-HGF)0
|b 5
|6 P:(DE-HGF)0
913 1 _ |a DE-HGF
|b Key Technologies
|l Natural, Artificial and Cognitive Information Processing
|1 G:(DE-HGF)POF4-520
|0 G:(DE-HGF)POF4-521
|3 G:(DE-HGF)POF4
|2 G:(DE-HGF)POF4-500
|4 G:(DE-HGF)POF
|v Quantum Materials
|9 G:(DE-HGF)POF4-5211
|x 0
914 1 _ |y 2025
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0200
|2 StatID
|b SCOPUS
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0160
|2 StatID
|b Essential Science Indicators
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)1230
|2 StatID
|b Current Contents - Electronics and Telecommunications Collection
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0600
|2 StatID
|b Ebsco Academic Search
|d 2024-12-10
915 _ _ |a American Physical Society Transfer of Copyright Agreement
|0 LIC:(DE-HGF)APS-112012
|2 HGFVOC
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)1150
|2 StatID
|b Current Contents - Physical, Chemical and Earth Sciences
|d 2024-12-10
915 _ _ |a WoS
|0 StatID:(DE-HGF)0113
|2 StatID
|b Science Citation Index Expanded
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0150
|2 StatID
|b Web of Science Core Collection
|d 2024-12-10
915 _ _ |a IF < 5
|0 StatID:(DE-HGF)9900
|2 StatID
|d 2024-12-10
915 _ _ |a OpenAccess
|0 StatID:(DE-HGF)0510
|2 StatID
915 _ _ |a Peer Review
|0 StatID:(DE-HGF)0030
|2 StatID
|b ASC
|d 2024-12-10
915 _ _ |a JCR
|0 StatID:(DE-HGF)0100
|2 StatID
|b PHYS REV B : 2022
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0300
|2 StatID
|b Medline
|d 2024-12-10
915 _ _ |a DBCoverage
|0 StatID:(DE-HGF)0199
|2 StatID
|b Clarivate Analytics Master Journal List
|d 2024-12-10
920 _ _ |l yes
920 1 _ |0 I:(DE-Juel1)PGI-1-20110106
|k PGI-1
|l Quanten-Theorie der Materialien
|x 0
980 _ _ |a journal
980 _ _ |a VDB
980 _ _ |a UNRESTRICTED
980 _ _ |a I:(DE-Juel1)PGI-1-20110106
980 1 _ |a FullTexts


LibraryCollectionCLSMajorCLSMinorLanguageAuthor
Marc 21