000059397 001__ 59397 000059397 005__ 20200423204545.0 000059397 0247_ $$2pmid$$apmid:21691008 000059397 0247_ $$2DOI$$a10.1088/0953-8984/19/18/186227 000059397 0247_ $$2WOS$$aWOS:000246556500033 000059397 0247_ $$2Handle$$a2128/23010 000059397 037__ $$aPreJuSER-59397 000059397 041__ $$aeng 000059397 082__ $$a530 000059397 084__ $$2WoS$$aPhysics, Condensed Matter 000059397 1001_ $$0P:(DE-Juel1)VDB54416$$aPerroni, C. A.$$b0$$uFZJ 000059397 245__ $$aRashba quantum wire: exact solution and ballistic transport 000059397 260__ $$aBristol$$bIOP Publ.$$c2007 000059397 300__ $$a186227 000059397 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000059397 3367_ $$2DataCite$$aOutput Types/Journal article 000059397 3367_ $$00$$2EndNote$$aJournal Article 000059397 3367_ $$2BibTeX$$aARTICLE 000059397 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000059397 3367_ $$2DRIVER$$aarticle 000059397 440_0 $$03703$$aJournal of Physics: Condensed Matter$$v19$$x0953-8984 000059397 500__ $$aRecord converted from VDB: 12.11.2012 000059397 520__ $$aThe effect of Rashba spin-orbit interaction in quantum wires with hard-wall boundaries is discussed. The exact wavefunction and eigenvalue equation are worked out, pointing out the mixing between the spin and spatial parts. The spectral properties are also studied within perturbation theory with respect to the strength of the spin-orbit interaction and diagonalization procedure. A comparison is made with the results of a simple model, the two-band model, that takes account only of the first two sub-bands of the wire. Finally, the transport properties within the ballistic regime are analytically calculated for the two-band model and through a tight-binding Green function for the entire system. Single and double interfaces separating regions with different strengths of spin-orbit interaction are analysed by injecting carriers into the first and the second sub-band. It is shown that in the case of a single interface the spin polarization in the Rashba region is different from zero, and in the case of two interfaces the spin polarization shows oscillations due to spin-selective bound states. 000059397 536__ $$0G:(DE-Juel1)FUEK414$$2G:(DE-HGF)$$aKondensierte Materie$$cP54$$x0 000059397 588__ $$aDataset connected to Web of Science, Pubmed 000059397 650_7 $$2WoSType$$aJ 000059397 7001_ $$0P:(DE-HGF)0$$aBercioux, D.$$b1 000059397 7001_ $$0P:(DE-HGF)0$$aMarigliano Ramaglia, V.$$b2 000059397 7001_ $$0P:(DE-HGF)0$$aCataudella, V.$$b3 000059397 773__ $$0PERI:(DE-600)1472968-4$$a10.1088/0953-8984/19/18/186227$$gVol. 19, p. 186227$$p186227$$q19<186227$$tJournal of physics / Condensed matter$$v19$$x0953-8984$$y2007 000059397 8567_ $$uhttp://dx.doi.org/10.1088/0953-8984/19/18/186227 000059397 8564_ $$uhttps://juser.fz-juelich.de/record/59397/files/0701508.pdf$$yOpenAccess 000059397 8564_ $$uhttps://juser.fz-juelich.de/record/59397/files/0701508.pdf?subformat=pdfa$$xpdfa$$yOpenAccess 000059397 909CO $$ooai:juser.fz-juelich.de:59397$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire 000059397 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt bis 2009 000059397 9141_ $$y2007 000059397 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000059397 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed 000059397 9201_ $$0I:(DE-Juel1)VDB781$$d31.12.2010$$gIFF$$kIFF-1$$lQuanten-Theorie der Materialien$$x1 000059397 970__ $$aVDB:(DE-Juel1)93441 000059397 980__ $$aVDB 000059397 980__ $$aConvertedRecord 000059397 980__ $$ajournal 000059397 980__ $$aI:(DE-Juel1)PGI-1-20110106 000059397 980__ $$aUNRESTRICTED 000059397 9801_ $$aFullTexts 000059397 981__ $$aI:(DE-Juel1)PGI-1-20110106