Skip to main content

Determination of Fermi contour and spin polarization of composite fermions via ballistic commensurability measurements

Author(s): Kamburov, D; Mueed, MA; Jo, I; Liu, Yang; Shayegan, Mansour; et al

Download
To refer to this page use: http://arks.princeton.edu/ark:/88435/pr1f86q
Full metadata record
DC FieldValueLanguage
dc.contributor.authorKamburov, D-
dc.contributor.authorMueed, MA-
dc.contributor.authorJo, I-
dc.contributor.authorLiu, Yang-
dc.contributor.authorShayegan, Mansour-
dc.contributor.authorPfeiffer, LN-
dc.contributor.authorWest, KW-
dc.contributor.authorBaldwin, KW-
dc.contributor.authorLee, JJD-
dc.contributor.authorWinkler, R-
dc.date.accessioned2021-10-08T20:17:09Z-
dc.date.available2021-10-08T20:17:09Z-
dc.date.issued2014-12en_US
dc.identifier.citationKamburov, D, Mueed, MA, Jo, I, Liu, Yang, Shayegan, M, Pfeiffer, LN, West, KW, Baldwin, KW, Lee, JJD, Winkler, R. (2014). Determination of Fermi contour and spin polarization of composite fermions via ballistic commensurability measurements. Physical Review B, 90 (23), 10.1103/PhysRevB.90.235108en_US
dc.identifier.issn1098-0121-
dc.identifier.urihttp://arks.princeton.edu/ark:/88435/pr1f86q-
dc.description.abstractWe report ballistic transport commensurability minima in the magnetoresistance of ν=3/2 composite fermions (CFs). The CFs are formed in high-quality two-dimensional electron systems confined to wide GaAs quantum wells and subjected to an in-plane, unidirectional periodic potential modulation. We observe a slight asymmetry of the CF commensurability positions with respect to ν=3/2, which we explain quantitatively by comparing three CF density models and concluding that the ν=3/2 CFs are likely formed by the minority carriers in the upper energy spin state of the lowest Landau level. Our data also allow us to probe the shape and size of the CF Fermi contour. At a fixed electron density of ≃1.8×1011 cm-2, as the quantum well width increases from 30 to 60 nm, the CFs show increasing spin polarization. We attribute this to the enhancement of the Zeeman energy relative to the Coulomb energy in wider wells where the latter is softened because of the larger electron layer thickness. The application of an additional parallel magnetic field (B||) leads to a significant distortion of the CF Fermi contour as B|| couples to the CFs' out-of-plane orbital motion. The distortion is much more severe compared to the ν=1/2 CF case at comparable B||. Moreover, the applied B|| further spin-polarizes the ν=3/2 CFs as deduced from the positions of the commensurability minima.en_US
dc.language.isoen_USen_US
dc.relation.ispartofPhysical Review Ben_US
dc.rightsAuthor's manuscripten_US
dc.titleDetermination of Fermi contour and spin polarization of composite fermions via ballistic commensurability measurementsen_US
dc.typeJournal Articleen_US
dc.identifier.doidoi:10.1103/PhysRevB.90.235108-
dc.date.eissued2014-12-02en_US
dc.identifier.eissn1550-235X-
pu.type.symplectichttp://www.symplectic.co.uk/publications/atom-terms/1.0/journal-articleen_US

Files in This Item:
File Description SizeFormat 
Determination of Fermi contour and spin polarization of ν= 32 composite fermions via ballistic commensurability measurements.pdf4.53 MBAdobe PDFView/Download


Items in OAR@Princeton are protected by copyright, with all rights reserved, unless otherwise indicated.