Deep impurity levels in semiconductor superlattices

1988 ◽  
Vol 38 (15) ◽  
pp. 10677-10692 ◽  
Author(s):  
Shang Yuan Ren ◽  
John D. Dow ◽  
Jun Shen
Keyword(s):  
Semiconductor Superlattices ◽  
Deep Impurity

RAMAN PROBING OF PHONONS AND INTERFACES IN SEMICONDUCTOR SUPERLATTICES

1984 ◽  
Vol 45 (C5) ◽  
pp. C5-131-C5-137 ◽  
Author(s):  
M. V. Klein ◽  
C. Colvard ◽  
R. Fischer ◽  
H . Morkoç
Keyword(s):  
Semiconductor Superlattices

EXPERIMENTAL INVESTIGATIONS OF THE QUANTUM PHOTOVOLTAIC EFFECT IN InAs-GaSb SEMICONDUCTOR SUPERLATTICES

1987 ◽  
Vol 48 (C5) ◽  
pp. C5-183-C5-186
Author(s):  
J. BLEUSE ◽  
P. VOISIN ◽  
M. VOOS ◽  
L. L. CHANG ◽  
L. ESAKI
Keyword(s):  
Photovoltaic Effect ◽  
Experimental Investigations ◽  
Semiconductor Superlattices

Strong Coupling of Electron and Nuclear Spins: Outlook and Prospects

2018 ◽  
Author(s):  
M. M. Glazov
Keyword(s):  
Energy Spectrum ◽  
Charge Carrier ◽  
Strong Coupling ◽  
Nuclear Spin ◽  
Spin Dynamics ◽  
Spin Polaron ◽  
Nuclear Spins ◽  
Deep Impurity ◽  
Impurity Centers ◽  
Ordered State

In this chapter, some prospects in the field of electron and nuclear spin dynamics are outlined. Particular emphasis is put ona situation where the hyperfine interaction is so strong that it leads to a qualitative rearrangement of the energy spectrum resulting in the coherent excitation transfer between the electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized, for example in the case of deep impurity centers in semiconductors or in isotopically purified systems. We also discuss the effect of the nuclear spin polaron, that is ordered state, formation at low enough temperatures of nuclear spins, where the orientation of the carrier spin results in alignment of the spins of nucleus interacting with the electron or hole.

Synergistic effects of nonmetal co-doping with sulfur in anatase TiO2: a DFT + U study

2015 ◽  
Vol 17 (5) ◽  
pp. 3426-3434 ◽  
Author(s):  
Qing-Lu Liu ◽  
Zong-Yan Zhao ◽  
Qing-Ju Liu
Keyword(s):  
Electric Field ◽  
Synergistic Effects ◽  
Anatase Tio2 ◽  
Local Electric Field ◽  
Energy Bands ◽  
Deep Impurity ◽  
Co Doping

S + NM co-doping could induce a stronger local electric field and eliminate the deep impurity energy bands of S mono-doped TiO2.

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