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Titlebook: Effective Electron Mass in Low-Dimensional Semiconductors; Sitangshu Bhattacharya,Kamakhya Prasad Ghatak Book 2013 Springer-Verlag Berlin

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https://doi.org/10.1007/978-3-642-31248-9EEM book; EEM review; effective electron mass, EEM; low dimensional semiconductors; non-parabolic Semico
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The EEM in Inversion Layers of Non-Parabolic Semiconductors a one dimensional potential well whose width is of the order of the carrier wavelength, the motion in that particular direction gets quantized while that along the other two directions remains as free.
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The EEM in Nanowires of Non-Parabolic Semiconductorswo infinitely deep one-dimensional (1D) rectangular potential wells, along any two orthogonal directions leading to quantization of the wave vectors along the said directions, allowing 1D carrier transport.
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The EEM in the Presence of Intense Electric Fielddifferent band structures. It appears from the literature that the studies have been made on the assumption that the carrier dispersion laws are invariant quantities in the presence of intense electric field, which is not fundamentally true.
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Die Kernaussagen auf einen Blick,It must be noted that among the various definitions of the effective electron mass (e.g effective acceleration mass, density-of-state effective mass, concentration effective mass, conductivity effective mass, Faraday rotation effective mass, etc) [2], it is the effective momentum mass that should be
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https://doi.org/10.1007/978-3-658-07047-2wo infinitely deep one-dimensional (1D) rectangular potential wells, along any two orthogonal directions leading to quantization of the wave vectors along the said directions, allowing 1D carrier transport.
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