Superposition at absolute zero

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SUMMARY

The discussion centers on the concept of superposition at absolute zero, highlighting that even at this temperature, coherent superpositions can be disrupted by zero-point fluctuations. The participants explore the implications of a quantum system losing energy to its cold environment and the theoretical possibility of achieving universal superposition at absolute zero. Key references include a paper on decoherence and a quantum physics preprint that delve into these phenomena, emphasizing the relationship between temperature and quantum states.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly superposition and decoherence.
  • Familiarity with the Schrödinger equation and quantum state representation.
  • Knowledge of statistical mechanics, specifically the canonical ensemble and partition function.
  • Basic grasp of zero-point energy and its implications in quantum systems.
NEXT STEPS
  • Research "quantum decoherence and its effects on superposition" for deeper insights.
  • Study "Schrödinger equation applications in quantum mechanics" to understand state evolution.
  • Explore "zero-point energy and its role in quantum systems" to grasp energy loss at absolute zero.
  • Investigate "canonical ensemble and statistical mechanics" to connect temperature with quantum states.
USEFUL FOR

Physicists, quantum mechanics students, and researchers interested in the implications of temperature on quantum states and superposition phenomena.

DirkMan
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I googled a bit about this and managed to find this

http://arxiv.org/abs/quant-ph/0505056
http://physics.bu.edu/~mohanty/physica-decoherence.pdf

Since I can't make much out of them, maybe except this interesting phrase in the first one

"First
of all it is intriguing that even at
absolute zero a coherent superposition of states can get destroyed by zero point fluctuations
."

But this, I don't understand what they mean by this:

"At absolute zero the quantum system
can only lose energy to the
cold environment"

And another question : From what I know, the more atoms you try to put in superposition, you need to get them closer to absolute zero, so can one deduce that theoretically at absolute zero you could have the whole universe in a superposition state ?
 
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For a closed system, if you start in a pure state, you'll always stay in a pure state. In the Schrödinger picture, if ##|\psi_0 \rangle## is the vector, representing a pure state, at later times the vector is (I use natural units with ##\hbar=k_{\text{B}}=c=1##)
$$|\psi(t) \rangle=\exp(-\mathrm{i} \hat{H} t) |\psi_0 \rangle.$$
This has nothing to do with temperature, which makes only sense if you have a system in (maybe local) thermal equilibrium. In the canonical ensemble this state is described by the statistical operator
$$\hat{\rho}_{\text{can}}=\frac{1}{Z} \exp \left (-\frac{\hat{H}}{T} \right ), \quad Z=\mathrm{Tr}\exp \left (-\frac{\hat{H}}{T} \right ) .$$
 

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