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Description
Dusk Shine Jumpscares
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The unstable solution is “scary.” The quantum case shows that the force is one of repulsion, a “jump.”
The comic is a “jumpscare.”
Lol
Alright, it’s been after twelve hours. Time for the answer.
In the classical canonical ensemble, the solution is unstable—the Coulomb potential energy is unbounded below at the origin. In the quantum case of this example, it only works if they satisfy Fermi–Dirac statistics.
The particles provided in the example are implied to be fermions, when making some informed assumptions about how they would act from the given description.
The stability notion for the interaction Phi is essential in quantum statistical mechanics as much as is the case for the canonical ensemble for a classical system.
The interaction would be stable in the case where there is a constant Beta such that the Schrodinger operator H for the two particles is satisfied if the two particles were identical, which they are not. This is illustrated with the use of combinatorial coefficients, to attribute the distinction between them.
While there is no symmetry property with respect to the mixed permutations of both particles, the symmetries and antisymmetries hold true with respect to the given variables of each of the two particles.
These statistics give a glimpse at the sorts of interactions that are absent in Classical Statistical Mechanics for describing Fermionic systems.
On that it kind of makes sense(but still way to slow to work), on this it doesn’t as it’s a bunch of still images.
If someone doesn’t work it out in the next twelve hours, then I’ll post up the answer.
I’m still waiting for someone to work it out.
https://derpiboo.ru/824033
Thirded.
Agreed.
I think you have the wrong idea what that means.