2015
DOI: 10.1016/j.optcom.2014.09.004
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Nonlinear optical absorption in parabolic quantum well via two-photon absorption process

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Cited by 32 publications
(5 citation statements)
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“…The main trend that can be observed here is that with increasing magnetic field the resonant peaks shift to higher energies and their amplitudes increase. This behavior of the MOAC is similar to that in a semiconductor quantum well [79] and in graphene [44,45,62]. This can be qualitatively explained in the one-particle picture as originating from the LL spectrum as follows: With the increase of the magnetic field, the LL spacing increases giving upswing to a higher energy of the absorbed photon.…”
Section: A Intrinsic Acoustic Phononssupporting
confidence: 62%
“…The main trend that can be observed here is that with increasing magnetic field the resonant peaks shift to higher energies and their amplitudes increase. This behavior of the MOAC is similar to that in a semiconductor quantum well [79] and in graphene [44,45,62]. This can be qualitatively explained in the one-particle picture as originating from the LL spectrum as follows: With the increase of the magnetic field, the LL spacing increases giving upswing to a higher energy of the absorbed photon.…”
Section: A Intrinsic Acoustic Phononssupporting
confidence: 62%
“…GaAs and Ga 0.7 Al 0.3 As quantum wells, as well as in the one-and two-photon absorption processes. The present result is in good agreement with the results of previous papers [33,34,[39][40][41][42][43]. This increase behavior of the half-width is explained from the increase of the probability of electron−phonon interaction when magnetic field increases.…”
Section: Quantitiessupporting
confidence: 93%
“…In the case of this potential, the term U P ( z ) is revealed by 47–50 U P ( z ) = m *( ω P z ) 2 z 2 /2,where m * and ω P z are symbols of the effective mass of the charge-carrier and the characteristic confining frequency of the parabolic-well electron. In this case, the eigenfunctions ( χ P ( z )) and the corresponding eigenvalues ( E P n , ) of the parabolic-well electron are given byandwhere the Hermite polynomials of order are symbolized by H ( z / λ z ), = 0, 1, 2, …, and λ z = ( ℏ /( m * ω P z )) 1/2 .…”
Section: Electron–acoustic-phonon Interaction Matrix Elements In Para...mentioning
confidence: 99%