Thermal populations of atomic energy eigenstates

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SUMMARY

This discussion focuses on calculating the expected population of atomic energy eigenstates in complex atoms at a given temperature, specifically for transition metals with spin-orbit coupling. The relevant formula for this calculation is P(ψ) = (1/Z)e^(Nμ - ε)/kT, where μ is the chemical potential, ε is the energy of the state, N is the number of electrons, T is the temperature, and k is Boltzmann's constant. A recommended resource for understanding these concepts is "An Introduction to Thermal Physics" by Daniel Schroeder, which provides foundational insights into statistical mechanics.

PREREQUISITES
  • Understanding of statistical mechanics principles
  • Familiarity with atomic energy levels and eigenstates
  • Knowledge of Boltzmann's constant and its significance
  • Basic grasp of chemical potential in quantum systems
NEXT STEPS
  • Study the derivation and applications of the formula P(ψ) = (1/Z)e^(Nμ - ε)/kT
  • Read "An Introduction to Thermal Physics" by Daniel Schroeder for foundational knowledge
  • Explore the concept of spin-orbit coupling in transition metals
  • Investigate the role of degeneracies in atomic energy levels
USEFUL FOR

This discussion is beneficial for physicists, chemists, and students studying statistical mechanics, particularly those interested in atomic physics and the behavior of complex atoms at varying temperatures.

Kazza_765
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Basically I have an (infinite) population of isolated atoms with a bunch of discrete energy levels available to them. I want to work out what the expected population of each of the states is at a given temperature.

They're complex atoms (transition metals) and spin-orbit coupling combined with various valance configurations gives me a big spectrum of possible eigenstates, with a number of different degeneracies. I'm sure I should have covered this at some stage in my education, but I always hated statistical physics and skipped most of the lectures.

I'm hoping someone could point me towards the right formula or the right book, or even a paper that has covered this at a basic level and has useful references. The only thing I remember is looking at the fermi level in semi-conductors, but I don't think that applies when we have discrete states.

Thanks
John
 
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The book I always liked for statistical mechanics, at least as an introduction, was "An Introduction to Thermal Physics" by Daniel Schroeder. So you might have a look at that. Basically you're going to need something like
P(\psi) = \frac{1}{Z}e^{(N\mu - \epsilon)/kT}
where \mu is the chemical potential of a given state, \epsilon is its energy, N is the number of electrons in the state, T is the temperature, and k is Boltzmann's constant. I'm not sure if that's the exact notation used in the book but it should be recognizable at least.
 
Terrific, thankyou very much. Off to the library now.

(I reckon it's always better to have someone recommend a good book than just typing "statistical physics" in the catalogue.)
 

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