Does DOS depend on Temperature?

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The discussion centers on the relationship between Density of States (DOS) and temperature (T) within the context of Green Function theory. It is argued that while DOS is typically defined as the number of states per energy and is considered independent of temperature, the Spectral Function, which relates to DOS, does depend on temperature when calculating averages over excited states. The participants explore the implications of this relationship, questioning whether DOS can truly be independent if it is derived from a temperature-dependent Spectral Function. The conversation highlights the complexity of these definitions and their interdependencies, particularly in nonzero temperature conditions. Ultimately, the discussion raises important questions about the fundamental nature of DOS and its relationship to temperature in quantum systems.
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In the Green Function theory. The Spectrum Function can be related to DOS. However, in the nonzero T condition, we can also define Spectrum Function. In the other hand, in my conception, DOS is the independent quantity which is determined by the system.
So, does it mean DOS is actually a function which depends on T?
 
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Diracmai said:
In the Green Function theory. The Spectrum Function can be related to DOS. However, in the nonzero T condition, we can also define Spectrum Function. In the other hand, in my conception, DOS is the independent quantity which is determined by the system.
So, does it mean DOS is actually a function which depends on T?

Can you show me the single-particle spectral function for T=0 and T not zero, and tell me what you think is "different"?

Zz.
 
Well the standard definition of the DOS I have been given is the number of states per energy (number of states not number of occupied states). This is a property of the Hamiltonian so for every example I have seen the DOS does not depend on temperature, but the occupation numbers do. I don't know, there may be other definitions.
 
radium said:
Well the standard definition of the DOS I have been given is the number of states per energy (number of states not number of occupied states). This is a property of the Hamiltonian so for every example I have seen the DOS does not depend on temperature, but the occupation numbers do. I don't know, there may be other definitions.

There is a "lower level" derivation/definition of the DOS when mean-field approximation/Fermi liquid model is valid. If one starts with the single-particle spectral function A(k,w), which is the imaginary part of the single-particle Green's function, then the DOS is the "momentum average" of the spectral function, i.e. you integrate A(k,w) over all possible momentum k and essentially giving you A(w), which corresponds to some form of the density of states.

Zz.
 
ZapperZ said:
Can you show me the single-particle spectral function for T=0 and T not zero, and tell me what you think is "different"?

Zz.

The definition of Spectral Function need us to calculate the average value of commutator(retard or advance green function) according to all the occupied states. In the T=0 condition, we only need to compute the average value in the ground state. So, the function is independent of T. However, if T is a definite value, we need to include partition function to calculate the average value in all the excited states. So, the Spectral Function include the parameter T.

My question is, the definition of DOS seems like an definite quantity which independent of T. So, if we relate DOS to Spectral Function, there must be some contradiction between these two conception.

In your second response, do you means A(k,w) (momentum average) is dependent on T. And if we integrate all the k, the quantity A(w) is actually accord with the definition of DOS and independent of T?
 

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