Home > Research > Publications & Outputs > Crossing of cyclotron and spin resonances in a ...

Research

Links

Text available via DOI:

View graph of relations

Crossing of cyclotron and spin resonances in a 2D electron gas

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Published

Standard

Crossing of cyclotron and spin resonances in a 2D electron gas. / Falko, Vladimir.
In: Surface Science, Vol. 305, No. 1-3, 20.03.1994, p. 290-294.

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Harvard

Falko, V 1994, 'Crossing of cyclotron and spin resonances in a 2D electron gas', Surface Science, vol. 305, no. 1-3, pp. 290-294. https://doi.org/10.1016/0039-6028(94)90903-2

APA

Falko, V. (1994). Crossing of cyclotron and spin resonances in a 2D electron gas. Surface Science, 305(1-3), 290-294. https://doi.org/10.1016/0039-6028(94)90903-2

Vancouver

Falko V. Crossing of cyclotron and spin resonances in a 2D electron gas. Surface Science. 1994 Mar 20;305(1-3):290-294. doi: 10.1016/0039-6028(94)90903-2

Author

Falko, Vladimir. / Crossing of cyclotron and spin resonances in a 2D electron gas. In: Surface Science. 1994 ; Vol. 305, No. 1-3. pp. 290-294.

Bibtex

@article{3f775c03f5ca4a538daf69d122aafe9e,
title = "Crossing of cyclotron and spin resonances in a 2D electron gas",
abstract = "We compare anticrossing of the cyclotron and spin resonances in spin-polarized and non-polarized phases of the degenerate two-dimensional Coulomb gas subjected to a strong tilted magnetic field. The spin-orbit coupling splits these resonances into three lines with the gaps between them exactly equal to delta2n+1 = v(so)p(F) and delta2n = v(so)p(F)/square-root 2 at odd- and even- integer filling factors, respectively. The 1/square-root 2 difference between delta2n and delta2n+1 comes from the existence of an additional spin-density wave excitation in the polarized phase of interacting electrons at nu = 2n and can be treated as a means to indicate the re-entrance of the system into it.",
author = "Vladimir Falko",
year = "1994",
month = mar,
day = "20",
doi = "10.1016/0039-6028(94)90903-2",
language = "English",
volume = "305",
pages = "290--294",
journal = "Surface Science",
issn = "0039-6028",
publisher = "Elsevier",
number = "1-3",

}

RIS

TY - JOUR

T1 - Crossing of cyclotron and spin resonances in a 2D electron gas

AU - Falko, Vladimir

PY - 1994/3/20

Y1 - 1994/3/20

N2 - We compare anticrossing of the cyclotron and spin resonances in spin-polarized and non-polarized phases of the degenerate two-dimensional Coulomb gas subjected to a strong tilted magnetic field. The spin-orbit coupling splits these resonances into three lines with the gaps between them exactly equal to delta2n+1 = v(so)p(F) and delta2n = v(so)p(F)/square-root 2 at odd- and even- integer filling factors, respectively. The 1/square-root 2 difference between delta2n and delta2n+1 comes from the existence of an additional spin-density wave excitation in the polarized phase of interacting electrons at nu = 2n and can be treated as a means to indicate the re-entrance of the system into it.

AB - We compare anticrossing of the cyclotron and spin resonances in spin-polarized and non-polarized phases of the degenerate two-dimensional Coulomb gas subjected to a strong tilted magnetic field. The spin-orbit coupling splits these resonances into three lines with the gaps between them exactly equal to delta2n+1 = v(so)p(F) and delta2n = v(so)p(F)/square-root 2 at odd- and even- integer filling factors, respectively. The 1/square-root 2 difference between delta2n and delta2n+1 comes from the existence of an additional spin-density wave excitation in the polarized phase of interacting electrons at nu = 2n and can be treated as a means to indicate the re-entrance of the system into it.

U2 - 10.1016/0039-6028(94)90903-2

DO - 10.1016/0039-6028(94)90903-2

M3 - Journal article

VL - 305

SP - 290

EP - 294

JO - Surface Science

JF - Surface Science

SN - 0039-6028

IS - 1-3

ER -