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Therefore, N acts as deep center localized above extended conduction band states of the host semiconductor.
This results in the accumulation of electrons in extended conduction band, which can serve as hydrogen formation site.
In Ce TiO2, the photogenerated electrons are excited from the valence band to extended conduction band where electrons are trapped effectively by Ce4+/Ce3+ couple.
The presence of N in a host III-V material restructures the conduction band of the host material, and this modification has been well explained using the interaction between the localized N level and the extended conduction band state of the host material in terms of the band anti-crossing model[4].
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Therefore, extended state conduction is most likely to take place.
Discussions are extended to the conduction mechanisms in the partially crystallized states.
The mechanics of structure genome has been extended to heat conduction problem of composite materials with a general linear thermal imperfect interface model.
Also, it made full use of principles of thermal insulation and gradient heat conduction, and extended the scope of thermal gradient in asphalt layers.
The major conclusion of this work is that for stationary heat conduction through extended surfaces, the DTM solution can be obtained in a closed series solution which does not necessitate an iterative method such as the Newton Raphson methods for the determination of the initial value of temperature transform function.
The distributions of interface states having high density tails that extend to the conduction band can significantly impact the subthreshold performance in both the surface channel design and the implant-free quantum-well HEMT-like structure with no δ-doping.
Helmholtz, Thomson, Henry, Gustav Kirchhoff, and Sir George Gabriel Stokes also extended the theory of the conduction and propagation of electric effects in conductors.
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