Undergrad Temperature in quantum systems

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SUMMARY

The discussion centers on the thermodynamics of quantum systems, specifically the behavior of quantum harmonic oscillators at zero and finite temperatures. Participants clarify that Hamiltonians, such as those for the H-atom and harmonic oscillator, model systems at absolute zero temperature, while finite temperatures are analyzed using density operators and canonical ensembles. The ground state at zero temperature is identified as a coherent state, while thermal coherent states emerge at finite temperatures. The conversation emphasizes that Fock states, although excited, do not correspond to a meaningful nonzero temperature.

PREREQUISITES
  • Understanding of quantum mechanics and Hamiltonians
  • Familiarity with statistical mechanics concepts, particularly canonical ensembles
  • Knowledge of coherent states and Fock states in quantum systems
  • Basic principles of thermodynamics as applied to quantum systems
NEXT STEPS
  • Study the role of density operators in quantum statistical mechanics
  • Explore the concept of thermal coherent states in detail
  • Learn about the implications of temperature in quantum harmonic oscillators
  • Investigate the mathematical formulation of the partition function Z in statistical mechanics
USEFUL FOR

Quantum physicists, researchers in thermodynamics of quantum systems, and students studying quantum mechanics and statistical mechanics will benefit from this discussion.

lfqm
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Hi!

These days I've been studying thermodynamics of quantum systems, and in so a very basic doubt come to me... I hope you guys can help me:

When we study the usual hamiltonians of quantum mechanics (H-atom, harmonic oscillator, etc.)... Are these hamiltonians modeling the system at temperature 0? How can the temperature be adjusted in the hamiltonian?

More concretely: How do I study a quantum harmonic oscillator at temperature 0 and how do I do it at finite temperature?

Thanks!
 
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lfqm said:
How do I study a quantum harmonic oscillator at temperature 0 and how do I do it at finite temperature?
At zero temperature by looking at wave functions (ground states and excited states), at finite temperature by looking at density operators - in the simplest case canonical ensembles.
 
So, the hamiltonian isn't modified?
At 0 temperature I study the usual spectrum of the hamiltonian and at finite temperature I use the density operador given in statistical mechanics?
 
The hamiltonian is the same. At zero temperature the ground state is a gaussian with a minimal width (a coherent state). if you enlarge it, you get the ground state at a finite temperature (it is then a thermal coherent state). If you translate it in the phase space the temperature does not change but you are no more in the vacuum.
Inside a black body you have a thermal coherent state It is well explained in the wiki link.
 
Ok, at 0 tenperature the ground state is a coherent state with Alfa=0... But, the first excited state at 0 temperature is the fock state |1>? i.e. the usual spectrum.
 
As the single-particle Fock state ##|1 \rangle## has a greater energy than the ground state it is an excitation but it is not a thermal coherent state. Have you seen this http://www.iqst.ca/quantech/wiggalery.php ? I am not sure that there is a notion of temperature for this state. You are talking about the first excited state. if you translate the vacuum by a small complex ##\alpha## you get a coherent state with an energy which can be less than the energy of ##|1 \rangle##
I recently discovered this notion of thermal quantum state please correct my eventual errors.
 
naima said:
I am not sure that there is a notion of temperature for this Fock state.

In this old thread
Xepma said:
Let's first focus on the idea of a single particle in a quantum mechanical system which is set at some temperature T. When a system is at some temperature T it means that its energy is not fixed. The particle can sit in each energy eigenstate, and the probability that it does so is given by ##e^{-E/(kT)}/Z##
This would mean that a Fock state with a well defined energy is not at a precise temperature. This is the case with the harmonic oscillator hamiltonian.
 
naima said:
a Fock state with a well defined energy is not at a precise temperature.
Conventionally, Fock states are considered as (excited) zero temperature states. It is impossible to assign it a meaningful nonzero temperature, not even an imprecise one.
 

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