7. (a) What is the energy distribution function n(E) and why is it useful in the context of statistical physics? Consider an ideal gas vs. a "free electron gas", and write the general expression for the energy distribution function n(E) for each case separately. (b) In class, we derived the density of states for a free electron gas (i.e. electrons in a metal) using the model of the 3D infinite potential well which gives energy levels as:, πη E= (n² + n² + n²) 2mL² where L is the side length of a cubical "box". Now suppose instead that we consider physical systems in which the electrons are confined to move in a 2D "sheet" of side length L (e.g. a relevant material system is graphene), which can have energy levels given as: E h²x² ~ 2m² F² (m² + n²) where m* is an "effective mass". Derive the density of states for the 2D electron gas.
7. (a) What is the energy distribution function n(E) and why is it useful in the context of statistical physics? Consider an ideal gas vs. a "free electron gas", and write the general expression for the energy distribution function n(E) for each case separately. (b) In class, we derived the density of states for a free electron gas (i.e. electrons in a metal) using the model of the 3D infinite potential well which gives energy levels as:, πη E= (n² + n² + n²) 2mL² where L is the side length of a cubical "box". Now suppose instead that we consider physical systems in which the electrons are confined to move in a 2D "sheet" of side length L (e.g. a relevant material system is graphene), which can have energy levels given as: E h²x² ~ 2m² F² (m² + n²) where m* is an "effective mass". Derive the density of states for the 2D electron gas.
Classical Dynamics of Particles and Systems
5th Edition
ISBN:9780534408961
Author:Stephen T. Thornton, Jerry B. Marion
Publisher:Stephen T. Thornton, Jerry B. Marion
Chapter7: Hamilton's Principle-lagrangian And Hamiltonian Dynamics
Section: Chapter Questions
Problem 7.36P
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