# 0.4: Time evolution of the state vector

• • Contributed by Mark E. Tuckerman
• Professor (Chemistry and Mathematics) at New York University

The time evolution of the state vector is prescribed by the Schrödinger equation where H is the Hamiltonian operator. This equation can be solved, in principle, yielding where is the initial state vector. The operator is the time evolution operator or quantum propagator. Let us introduce the eigenvalues and eigenvectors of the Hamiltonian H that satisfy The eigenvectors for an orthonormal basis on the Hilbert space and therefore, the state vector can be expanded in them according to where, of course, , which is the amplitude for obtaining the value at time t if a measurement of H is performed. Using this expansion, it is straightforward to show that the time evolution of the state vector can be written as an expansion: Thus, we need to compute all the initial amplitudes for obtaining the different eigenvalues of H, apply to each the factor and then sum over all the eigenstates to obtain the state vector at time t.

If the Hamiltonian is obtained from a classical Hamiltonian H(x,p), then, using the formula from the previous section for the action of an arbitrary operator A(X,P) on the state vector in the coordinate basis, we can recast the Schrödiner equation as a partial differential equation. By multiplying both sides of the Schrödinger equation by , we obtain If the classical Hamiltonian takes the form then the Schrödinger equation becomes which is known as the Schrödinger wave equation or the time-dependent Schrödinger equation.

In a similar manner, the eigenvalue equation for H can be expressed as a differential equation by projecting it into the X basis: where is an eigenfunction of the Hamiltonian.