What is Quantum Statistical Mechanics?

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SUMMARY

Quantum Statistical Mechanics (QSM) applies Quantum Mechanics (QM) to mixed states rather than pure states, introducing thermodynamic concepts such as temperature and the thermodynamic limit. Unlike non-relativistic Quantum Field Theory (NRQFT), which describes quantum many-body systems using quasiparticles, QSM focuses on statistical properties of systems in thermodynamic equilibrium. The discussion emphasizes that QSM is essential for understanding systems far from equilibrium and highlights the significance of local temperature fields in nonequilibrium thermodynamics. Key references include Danielewicz's papers on nonequilibrium processes and Linda Reichl's statistical physics book.

PREREQUISITES
  • Understanding of Quantum Mechanics (QM) principles
  • Familiarity with Quantum Field Theory (QFT) concepts
  • Knowledge of thermodynamic principles, particularly temperature and equilibrium
  • Basic grasp of statistical mechanics and its applications
NEXT STEPS
  • Study Danielewicz's papers on Quantum Theory of Nonequilibrium Processes
  • Explore Linda Reichl's book on statistical physics for deeper insights
  • Research the concept of quasiparticles and their role in NRQFT
  • Investigate the implications of superselection rules in quantum mechanics
USEFUL FOR

Researchers and students in theoretical physics, particularly those focusing on quantum mechanics, statistical mechanics, and thermodynamics. This discussion is beneficial for anyone looking to deepen their understanding of quantum many-body systems and nonequilibrium phenomena.

  • #31
Demystifier said:
I believe they prepare them all the time, but they just don't know it because the states are ... well, unobservable.
Hm, I still don't know, what you mean by "unobservable states". If a state is (in principal) unobservable, then it's not a state. So an "unobservable state" seems to be a constradictio in adjecto. The only thing, I'm aware of are superselection rules which forbid certain states, but that means that they simply do not exist (e.g., the charge superselection rules forbidding superpositions of states of different charge or the angular-momentum superselection rule forbidding superpositions of half-integer with integer angular momenta).
 
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  • #32
A. Neumaier said:
Whatever will be preparable any time in the future must be a state that comes from partial tracing of the state of a bigger system including its environment. Thus it is covered by my definition of the states that can appear in Nature. Whereas one cannot observe a state that doesn't occur in Nature, and one cannot prepare such a state.
Well, If I prepare a cup of coffee and leave it at rest a while on my desk, I don't trace anything but prepare a thermal-equilibrium state by just waiting long enough. That's an easy preparation without in any way tracing out anything.
 
  • #33
vanhees71 said:
Well, If I prepare a cup of coffee and leave it at rest a while on my desk, I don't trace anything but prepare a thermal-equilibrium state by just waiting long enough. That's an easy preparation without in any way tracing out anything.
To be able to say what you said you traced out the whole universe except for the coffee in the cup. For only that part is in equilibrium. If you wait longer, maybe the bigger system consisting of coffee, cup and desk will be in thermal equilibrium. But as long as you are in the room, the whole room will not be in equilibrium. Thus you need to trace out at least yourself. And the outside of the building your desk is in. And your computer if it is running...
 
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  • #34
Wow, I'm a very mighty being, being able to trace out the whole universe by cooking a cup of coffee ;-)), but when I come to thermal equilibrium with my environment, I'm dead. So I better don't trace myself out...
 
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