query: Non-hermitian hamiltonians and symmetry properties of $\partial_t$
positive_passages.docid: 26896
positive_passages.text: Why can't $ i\hbar\frac{\partial}{\partial t}$ be considered the Hamiltonian operator?
negative_passages.docid: 157191
negative_passages.text: Conjugate Variables, Noether's Theorem and QM
negative_passages.docid: 112216
negative_passages.text: Geometric description of canonical commutation relation
negative_passages.docid: 13137
negative_passages.text: Why are Hermitian operators linked to observables?
negative_passages.docid: 22279
negative_passages.text: Local and Global Symmetries
negative_passages.docid: 35509
negative_passages.text: Noether's Theorem: Lie groups vs. Lie algebras; finite vs. infinitesimal symmetries
negative_passages.docid: 156636
negative_passages.text: The Existence of the $^1D$ term and the non-existence of the $^3D$ term?
negative_passages.docid: 44953
negative_passages.text: Gauge symmetries and elementary particles
negative_passages.docid: 99789
negative_passages.text: Beyond Hamiltonian and Lagrangian mechanics
negative_passages.docid: 47301
negative_passages.text: Hermitian Matrix
negative_passages.docid: 68267
negative_passages.text: $SU(3)$ irreducible representations with tensor method
negative_passages.docid: 143157
negative_passages.text: Perturbation theory: justifying expansion in terms of eigenstates of the basis Hamiltonian
negative_passages.docid: 99285
negative_passages.text: Why is the change in Hamiltonian for an active infinitesimal canonical transformation defined the way it is?
negative_passages.docid: 83832
negative_passages.text: Time as a Hermitian operator in quantum mechanics
negative_passages.docid: 89004
negative_passages.text: Where does the partial derivative come from in Sakurai's derivation of the momentum operator?
negative_passages.docid: 26125
negative_passages.text: Does the canonical commutation relation fix the form of the momentum operator?
negative_passages.docid: 5058
negative_passages.text: Eigenvalues of the rank one matrix $uv^T$