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Buzz's user avatar
Buzz
  • Member for 4 years
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  • The American South
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Finite-dimensional representations of quantum $SU(2)$
When, many years ago, I took a seminar class on this (based on, e.g. arxiv.org/abs/q-alg/9603025 ), I remember that many of the modules that arose naturally were indeed completely reducible, in a form very similar to the $q=0$ versions.
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Reference request for $\phi^{4}_{d}$ theory - where to begin?
I think the real answer is that you should learn more about quantum mechanics and quantum field theory as general subjects. (The fact that you have never seen $\phi^{4}$ theory in $d=1$ indicates that you do not have much grounding in the physics.) If you are having trouble making the connections between apparently different formalisms used in different sources, that is probably because they assume a certain level of understanding of the physics that motivates the mathematics.
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What is the Lie superalgebra generated by permutations?
It sounds like what you need is the structure of the Schur superalgebra: arxiv.org/abs/1209.6327
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Resources on the stationary Schrödinger equation with the soliton potential
A further nice pedagogical paper on the reflectionless potentials, solved via supersymmetry operators, is physics.smu.edu/scalise/P6335fa19/notes/…
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Hamiltonian, energy, and conservation laws of nonlinear PDEs
I included some thoughts on this in the first two sections of arXiv:1902.04643 . It doesn't get into the actual structure of the of the infinite hierarchy of conservation laws, but it discussed why, qualitatively, a soliton equation has to have countably many conserved quantities.
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