2003
DOI: 10.1016/s1386-9477(02)01040-8
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Continuous transformation from spin- to pseudospin-type excitation

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Cited by 11 publications
(14 citation statements)
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“…We have then calculated how the excitation energy changes as the sample is tilted. Our formula has explained quite well the activation energy anomaly found by Murphy et al 11 at the balanced point by excitations of pseudospins, and also found by Sawada et al 14 at various values of 0 by simultaneous excitations of spins and pseudospins. Though our formulas are derived for sufficiently smooth skyrmions, they have turned out to be quite good at least with the use of phenomenological values of N spin and N ppin .…”
Section: Discussionsupporting
confidence: 88%
See 2 more Smart Citations
“…We have then calculated how the excitation energy changes as the sample is tilted. Our formula has explained quite well the activation energy anomaly found by Murphy et al 11 at the balanced point by excitations of pseudospins, and also found by Sawada et al 14 at various values of 0 by simultaneous excitations of spins and pseudospins. Though our formulas are derived for sufficiently smooth skyrmions, they have turned out to be quite good at least with the use of phenomenological values of N spin and N ppin .…”
Section: Discussionsupporting
confidence: 88%
“…It is natural that a pseudospin texture evolves into an isospin texture and then regresses to a spin texture in this process. The corresponding continuous transformation of the activation energy has already been observed experimentally by Sawada et al [13,14,15]. In this paper we explain these experimental data [11,14,15] based on the excitation of SU(4) skyrmions.…”
Section: Introductionsupporting
confidence: 69%
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“…A Hartree-Fock calculation of the behavior of the bimeron energy in tilted magnetic field reproduces qualitatively the features found in the experiment. 11 Sawada et al 3 measured the activation energy of the 2DEG in a DQWS as a function of a parallel magnetic field and electrical bias between the layers. They define the imbalance parameter σ = (n L − n R )/(n L + n R ) where n R(L) is the density in the right(left) layer of the DQWS.…”
Section: Introductionmentioning
confidence: 99%
“…The ν = 1 balanced bilayer QHS also possesses a vortex excitation; however, on account of the symmetry of the system, such an excitation becomes a pair of half-charged vortices owing to pseudospins (where a pseudospin is a layer degree of freedom). As the density imbalance of the bilayer QHS increases, it is known that the system continuously evolves to the monolayer QHS [1,2]. In earlier studies pertaining to the ν = 1 bilayer QHS, the spin degree of freedom was often neglected because of the simple assumption that a strong magnetic field leads to the generation of fully polarized spins.…”
mentioning
confidence: 99%