A.12 Heisenberg picture

This book follows the formulation of quantum mechanics as developed by Schrödinger. However, there is another, earlier, formulation due to Heisenberg. This subsection gives a brief description so that you are aware of it when you run into it in literature.

In the Schrödinger picture, physical observables like position and momentum are represented by time-independent operators. The time dependence is in the wave function. This is somewhat counterintuitive because classically position and momentum are time dependent quantities. The Heisenberg picture removes the time dependence from the wave function and absorbs it into the operator.

To see how that works out, consider first the general form of the wave
function. It can be written as

(A.37) |

(A.38) |

(To check the above expression for the wave function, take the initial
wave function to be any energy eigenfunction of energy

Now consider an arbitrary Schrödinger operator

(A.39) |

If the time-dependent exponentials are now peeled off

(A.40) |

The operator

The first and third terms can be recognized as a multiple of the commutator of

(Note that there is no difference between the Hamiltonians

For example, consider the Schrödinger

Those have the exact same form as the equations for the classical position and momentum of the particle.

In fact, the equivalent of the general equation (A.41) is
also found in classical physics: it is derived in advanced mechanics,
with the so-called “Poisson bracket” taking the place of the commutator. As a
simple example, consider one-dimensional motion of a particle. Any
variable

according to the total differential of calculus. And from the classical Hamiltonian

it is seen that the time derivatives of position and momentum obey the classical “Hamiltonian dynamics”

Substituting this into the time derivative of

The first two terms in the right hand side are by definition minus the Poisson bracket

Note that the Poisson bracket, like the commutator, is antisymmetric under exchange of

More generally, the classical Hamiltonian can depend on multiple and non-Cartesian coordinates, generically called “generalized coordinates.” In that case, in the Poisson bracket you must sum over all generalized coordinates and their associated so-called “canonical” momenta. For a Cartesian position coordinate, the canonical momentum is the corresponding linear momentum. For an angular coordinate, it is the corresponding angular momentum. In general, using the so-called Lagrangian formulation usually covered in an engineering education, and otherwise found in addendum {A.1}, the canonical momentum is the derivative of the Lagrangian with respect to the time derivative of the coordinate.

The bottom line is that the Heisenberg equations are usually not easy to solve unless you return to the Schrödinger picture by peeling off the time dependence. In relativistic applications however, time joins space as an additional coordinate, and the Heisenberg picture becomes more helpful. It can also make it easier to identify the correspondence between classical equations and the corresponding quantum operators.

Key Points

- In the Heisenberg picture, operators evolve in time just like their physical variables do in classical physics.