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Comment on ``Spin and cyclotron energies of electrons in GaAs/GaAlAs quantum wells''
In a recent publication, Pfeffer and Zawadzki [cond-mat/0607150; Phys. Rev. B
74, 115309 (2006)] attempted a calculation of electron g factor in III-V
heterostructures. The authors emphasize that their outcome is in strong
discrepancy with our original result [Ivchenko and Kiselev, Sov. Phys.
Semicond. 26, 827 (1992)] and readily conclude that ``the previous theory of
the g factor in heterostructures is inadequate''. We show here that the entire
discrepancy can be tracked down to an additional contribution missing in the
incomplete elimination procedure of Pfeffer and Zawadzki. This mistake equally
affects their ``exact'' and approximate results. When the overlooked terms
stemming from the nondiagonal Zeeman interaction between light hole and
spin-orbit-split valence states are taken into account in the effective
electron dispersion, the results of the both approaches applied to the
three-level kp model become identical.Comment: 5 pages, no figure
Resonant Fibonacci Quantum Well Structures
We propose a resonant one-dimensional quasicrystal, namely, a multiple
quantum well (MQW) structure satisfying the Fibonacci-chain rule with the
golden ratio between the long and short inter-well distances. The resonant
Bragg condition is generalized from the periodic to Fibonacci MQWs. A
dispersion equation for exciton-polaritons is derived in the two-wave
approximation, the effective allowed and forbidden bands are found. The
reflection spectra from the proposed structures are calculated as a function of
the well number and detuning from the Bragg condition.Comment: 5 pages, 3 figures, submitted to Phys. Rev.
Chiral Lagrangians at finite temperature and the Polyakov Loop
Heat kernel expansions at finite temperature of massless QCD and chiral quark
models generate effective actions relevant for both low and high temperature
QCD. The key relevance of the Polyakov Loop to maintain the large and
non-perturbative gauge invariance at finite temperature is stressed.Comment: Talk given at 6th Conference on Quark Confinement and the Hadron
Spectrum, Villasimius, Sardinia, Italy, 21-25 Sep 200
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