Schrödinger Equation: Difference between revisions
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In this chapter, we introduce the Schrödinger equation, the most fundamental equation in quantum mechanics. Given a Hamiltonian <math>\mathcal{H}</math>, this equation describes how the wave function evolves in time. In [[States, Dirac Bra-Ket Notation|Dirac bra-ket notation]], the Schrödinger equation is | In this chapter, we introduce the Schrödinger equation, the most fundamental equation in quantum mechanics. Given a Hamiltonian <math>\mathcal{H}</math>, this equation describes how the wave function evolves in time. In [[States, Dirac Bra-Ket Notation|Dirac bra-ket notation]], the Schrödinger equation is | ||
<math>i\hbar\frac{\partial}{\partial t} | <math> i\hbar\frac{\partial}{\partial t}|\Psi(t)\rangle=\mathcal{H}|\Psi(t)\rangle. </math> | ||
If the Hamiltonian does not depend on time, then the wave function can be written as | |||
<math> |\Psi(t)\rangle=e^{-iEt/\hbar}|\psi\rangle, </math> | |||
and the Schrödinger equation becomes | |||
<math> \mathcal{H}|\psi\rangle=E|\psi\rangle. </math> | |||
<b>Chapter Contents</b> | <b>Chapter Contents</b> |
Revision as of 11:58, 6 March 2013
In this chapter, we introduce the Schrödinger equation, the most fundamental equation in quantum mechanics. Given a Hamiltonian , this equation describes how the wave function evolves in time. In Dirac bra-ket notation, the Schrödinger equation is
If the Hamiltonian does not depend on time, then the wave function can be written as
and the Schrödinger equation becomes
Chapter Contents