000041289 001__ 41289
000041289 005__ 20200423203915.0
000041289 017__ $$aThis version is available at the following Publisher URL: http://prl.aps.org
000041289 0247_ $$2DOI$$a10.1103/PhysRevLett.93.196802
000041289 0247_ $$2WOS$$aWOS:000224924900051
000041289 0247_ $$2Handle$$a2128/1382
000041289 037__ $$aPreJuSER-41289
000041289 041__ $$aeng
000041289 082__ $$a550
000041289 084__ $$2WoS$$aPhysics, Multidisciplinary
000041289 1001_ $$0P:(DE-HGF)0$$aPascual, J. I.$$b0
000041289 245__ $$aRole of Spin in Quasiparticle Interference
000041289 260__ $$aCollege Park, Md.$$bAPS$$c2004
000041289 300__ $$a196802
000041289 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article
000041289 3367_ $$2DataCite$$aOutput Types/Journal article
000041289 3367_ $$00$$2EndNote$$aJournal Article
000041289 3367_ $$2BibTeX$$aARTICLE
000041289 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000041289 3367_ $$2DRIVER$$aarticle
000041289 440_0 $$04925$$aPhysical Review Letters$$v93$$x0031-9007
000041289 500__ $$aRecord converted from VDB: 12.11.2012
000041289 520__ $$aQuasiparticle interference patterns measured by scanning tunneling microscopy can be used to study the local electronic structure of metal surfaces and high-temperature superconductors. Here, we show that even in nonmagnetic systems the spin of the quasiparticles can have a profound effect on the interference patterns. On Bi(110), where the surface state bands are not spin degenerate, the patterns are not related to the dispersion of the electronic states in a simple way. In fact, the features which are expected for the spin-independent situation are absent and the observed interference patterns can be interpreted only by taking spin-conserving scattering events into account.
000041289 536__ $$0G:(DE-Juel1)FUEK242$$2G:(DE-HGF)$$aKondensierte Materie$$cM02$$x0
000041289 588__ $$aDataset connected to Web of Science
000041289 650_7 $$2WoSType$$aJ
000041289 7001_ $$0P:(DE-Juel1)130545$$aBihlmayer, G.$$b1$$uFZJ
000041289 7001_ $$0P:(DE-HGF)0$$aKoroteev, Yu. M.$$b2
000041289 7001_ $$0P:(DE-HGF)0$$aRust, H. P.$$b3
000041289 7001_ $$0P:(DE-HGF)0$$aCeballos, G.$$b4
000041289 7001_ $$0P:(DE-HGF)0$$aHansmann, M.$$b5
000041289 7001_ $$0P:(DE-HGF)0$$aHorn, K.$$b6
000041289 7001_ $$0P:(DE-HGF)0$$aChulkov, E. V.$$b7
000041289 7001_ $$0P:(DE-Juel1)130548$$aBlügel, S.$$b8$$uFZJ
000041289 7001_ $$0P:(DE-HGF)0$$aEchenique, P. M.$$b9
000041289 7001_ $$0P:(DE-HGF)0$$aHofmann, Ph.$$b10
000041289 773__ $$0PERI:(DE-600)1472655-5$$a10.1103/PhysRevLett.93.196802$$gVol. 93, p. 196802$$p196802$$q93<196802$$tPhysical review letters$$v93$$x0031-9007$$y2004
000041289 8567_ $$uhttp://hdl.handle.net/2128/1382$$uhttp://dx.doi.org/10.1103/PhysRevLett.93.196802
000041289 8564_ $$uhttps://juser.fz-juelich.de/record/41289/files/56714.pdf$$yOpenAccess
000041289 8564_ $$uhttps://juser.fz-juelich.de/record/41289/files/56714.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess
000041289 8564_ $$uhttps://juser.fz-juelich.de/record/41289/files/56714.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000041289 8564_ $$uhttps://juser.fz-juelich.de/record/41289/files/56714.jpg?subformat=icon-640$$xicon-640$$yOpenAccess
000041289 909CO $$ooai:juser.fz-juelich.de:41289$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire
000041289 9131_ $$0G:(DE-Juel1)FUEK242$$bMaterie$$kM02$$lKondensierte Materie$$vKondensierte Materie$$x0
000041289 9141_ $$y2004
000041289 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed
000041289 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000041289 9201_ $$0I:(DE-Juel1)VDB30$$d31.12.2006$$gIFF$$kIFF-TH-I$$lTheorie I$$x0
000041289 970__ $$aVDB:(DE-Juel1)56714
000041289 980__ $$aVDB
000041289 980__ $$aJUWEL
000041289 980__ $$aConvertedRecord
000041289 980__ $$ajournal
000041289 980__ $$aI:(DE-Juel1)PGI-1-20110106
000041289 980__ $$aUNRESTRICTED
000041289 980__ $$aFullTexts
000041289 9801_ $$aFullTexts
000041289 981__ $$aI:(DE-Juel1)PGI-1-20110106