query: Different forms for the energy operator
positive_passages.docid: 26896
positive_passages.text: Why can't $ i\hbar\frac{\partial}{\partial t}$ be considered the Hamiltonian operator?
negative_passages.docid: 28062
negative_passages.text: Something special about energy eigenstates when it comes to time evolution?
negative_passages.docid: 116718
negative_passages.text: Motivating the ansatz for the infinitesimal translation operator
negative_passages.docid: 58072
negative_passages.text: The formal solution of the time-dependent Schrödinger equation
negative_passages.docid: 86295
negative_passages.text: Creation and annihilation operators in the hydrogen atom
negative_passages.docid: 44747
negative_passages.text: Finding the effective Hamiltonian in a certain subspace
negative_passages.docid: 45071
negative_passages.text: Having the derivative be an operator
negative_passages.docid: 24004
negative_passages.text: General form of a linear transformation
negative_passages.docid: 158387
negative_passages.text: Find eigen energies of time-independent Schrödinger equation
negative_passages.docid: 32606
negative_passages.text: Is the operator $T((x_1,x_2,...,x_n))=(x_1,\frac{x_2}2,\frac{x_3}3,...)$ on $\ell^2$ self-adjoint and unitary
negative_passages.docid: 98535
negative_passages.text: Are eigenstates of the position operator continuous?
negative_passages.docid: 116314
negative_passages.text: On-shell and off-shell transformations in Noether's theorem
negative_passages.docid: 152750
negative_passages.text: Is there a time operator in quantum mechanics?
negative_passages.docid: 119684
negative_passages.text: Is a contraction idempotent operator self-adjoint?
negative_passages.docid: 145626
negative_passages.text: Normalisation of free particle wavefunction
negative_passages.docid: 17785
negative_passages.text: Variational Derivation of Schrodinger Equation
negative_passages.docid: 148088
negative_passages.text: What is the energy of a superposition of energy eigenstates?