1990
DOI: 10.1142/0936
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Quantum Theory of the Optical and Electronic Properties of Semiconductors

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Cited by 646 publications
(628 citation statements)
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“…These Coulomb collisions come from a binary process in which a photoexcited electron collides with a background carrier, 62,63 and also a collective process in which the photoexcited electron interacts with the thermal plasma of background carriers. 64,65 The energy relaxation of photoexcited electrons due to Coulomb collisions is effective in the X and L valleys but not in the Γ valley. This difference stems from the effective mass as explained in Sec.…”
Section: Physical Picturementioning
confidence: 99%
“…These Coulomb collisions come from a binary process in which a photoexcited electron collides with a background carrier, 62,63 and also a collective process in which the photoexcited electron interacts with the thermal plasma of background carriers. 64,65 The energy relaxation of photoexcited electrons due to Coulomb collisions is effective in the X and L valleys but not in the Γ valley. This difference stems from the effective mass as explained in Sec.…”
Section: Physical Picturementioning
confidence: 99%
“…Having obtained a model expression for ρ ν (z, t), it is straightforward to obtain S(z, t) using Eqns. (18) and (19).…”
Section: Theorymentioning
confidence: 99%
“…[1], we now want to include some measure of screening in the wavefunction φ k . This is possible by using the Hulthén potential [5][6][7][8][9]12]…”
Section: Hulthén Fundamental Wavefunctionsmentioning
confidence: 99%
“…In the present study however, we are interested in the lowest-lying bound state only. In real space, its eigenfunction reads [8] …”
Section: Hulthén Fundamental Wavefunctionsmentioning
confidence: 99%
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