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Variational method (quantum mechanics): Revision history


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  • curprev 20:1420:14, 30 November 2022 35.40.123.60 talk 13,046 bytes +29 Clarifying that the corresponding state is both the ground state and an eigenstate of the Hamiltonian (H). undo
  • curprev 20:1220:12, 30 November 2022 35.40.123.60 talk 13,017 bytes −2 The corresponding state would be the ground state, which is an energy eigenstate, meaning it is an eigenstate of the Hamiltonian (H). E_0 is a number, and H is an operator. Quantum states are not eigenstates of numbers, but they are eigenstates of operators. undo

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  • curprev 17:1117:11, 5 April 2019 Kungchuan.hsu talk contribs m 12,032 bytes −20 Remove the summation in the first equation, which is redundant. Replace "\alpha_i" with "\mathbf{\alpha}" as the variable in the \psi states, since the dependency should be on all \alpha_i's, which is grouped up as a single vector variable \bm{\alpha}. undo

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