Abstract
Transport is called linear if the current is proportional to the driving force. The forces might be electric fields F, temperature gradients ∇T, or density gradients ∇n. Examples of linear transport relations are j = σF or Q = K (∇T), where the currents j (electrical) or Q (heat) are determined in terms of macroscopic coefficients σ (electrical conductivity) or K (thermal conductivity). These coefficients can be measured experimentally and calculated theoretically, which provides the meeting ground between experiment and theory. The theoretical calculation of σ and K can be done by using equilibrium Green’s functions.(1–2) A set of theoretical techniques for linear transport, based on equilibrium Green’s functions, have been developed and are widely used.
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© 1992 Springer Science+Business Media New York
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Mahan, G.D. (1992). Green’s Function Methods: Quantum Boltzmann Equation for Linear Transport. In: Ferry, D.K., Jacoboni, C. (eds) Quantum Transport in Semiconductors. Physics of Solids and Liquids. Springer, Boston, MA. https://doi.org/10.1007/978-1-4899-2359-2_6
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DOI: https://doi.org/10.1007/978-1-4899-2359-2_6
Publisher Name: Springer, Boston, MA
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