Consider a Hamiltonian (hat{H}(p)) only (no (x) dependence). What are the operators in the theory that evolve
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Consider a Hamiltonian \(\hat{H}(p)\) only (no \(x\) dependence). What are the operators in the theory that evolve nontrivially in the Heisenberg picture? What about in a possible interaction picture, if \(\hat{H}(p)\) can be separated into two parts?
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