## #001: Classical mechanics as high entropy limit of quantum mechanics

Category: Quantum mechanics - Tags: Quantum information, Classical limit, Entropy

Prove or disprove the following conjecture: any sufficiently high entropy state can be approximated by a statistical mixture of Gaussian wave packets.

Mathematical problem. Denote $$|g(q,p)\rangle$$ a set of Gaussian wave packets centered in phase space at position $$q$$ and momentum $$p$$. We want to show that a density matrix $$\rho$$ with sufficiently high von Neumann entropy $$tr(-\rho \log \rho)$$, allows the approximation:

$\rho \approx \int \hat{\rho}(q,p) |g(q,p)\rangle \langle g(q,p)| dq dp$

for a suitable function $$\hat{\rho}(q,p)$$ of position and momentum. The approximation should also approximate the expectations:

$tr(\rho F(Q,P)) \approx \int \hat{\rho}(q,p) f(q,p) dq dp.$

Note that there are a number of issues that remain vague, and part of the problem is exactly to find the correct specification. For example, the quality of the approximation should increase with the entropy of the mixed state; how this link works (at least in the limit) is part of the problem.

Physical significance. The idea is to show that the classical limit arises without a physical mechanism, but just as an approximation. A single particle in a pure state will have low entropy, and therefore the approximation will fail. A gas of multiple particles at room temperature, however, will have a high entropy, and therefore it can be approximated with a classical mixed state. While we will commit an error in making the approximation, the idea is that such error will be below the uncertainty associated with the high entropy.

The conjecture is motivated by observing that pure quantum states have zero entropy while pure classical states (i.e. microstates) have minus infinite entropy (they are a point over a continuuum, therefore a set of measure zero). The lower bound for entropy is also established by the third law of thermodynamics. Classical statistical states and quantum mixed states, then, must “diverge” as the entropy decreases since they cannot “go to zero” in the same way.