New Resonances Along with Cyclotron Resonance in Heterostructures

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dc.creatorShrivastava, Keshav N.
dc.date2003-05-18
dc.date.accessioned2026-07-07T02:51:24Z
dc.date.available2026-07-07T02:51:24Z
dc.descriptionThe usual cyclotron resonance occurs at ω_c=eB/m*c which is independent of spin. The new resonances depend on spin. The new resonances occur at ω_{c\pm}=(1/2)g_{\pm}eB/m*c where (1/2)g_{\pm}= {\it l}+(1/2)\pm s/(2{\it l}+1). The energy in the centre of two new frequencies varies as the square root of the 2-dimensional electrons due to spin excess in the Gaussian model. The frequencies ω_{c\pm} are linearly proportional to the magnetic field except near crossing point where the linear combination of wave functions must be made.
dc.description4 pages TeX
dc.identifierhttps://arxiv.org/abs/cond-mat/0305415
dc.identifierhttp://arxiv.org/abs/cond-mat/0305415
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/21439
dc.subjectMesoscale and Nanoscale Physics
dc.subjectStatistical Mechanics
dc.titleNew Resonances Along with Cyclotron Resonance in Heterostructures
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