A.16 The adiabatic theorem

An adiabatic system is a system whose Hamiltonian changes slowly in time. Despite the time dependence of the Hamiltonian, the wave function can still be written in terms of the energy eigenfunctions $\psi_{\vec n}$ of the Hamiltonian, because the eigenfunctions are complete. But since the Hamiltonian changes with time, so do the energy eigenfunctions. And that affects how the coefficients of the eigenfunctions evolve in time.

In particular, in the adiabatic approximation, the wave function of a system can be written as, {D.34}:

\Psi = \sum_{\vec n}c_{{\vec n}}(0)...
...angle\psi_{\vec n}\vert\psi_{\vec n}'\rangle{\,\rm d}t
$} %
\end{displaymath} (A.74)

where the $c_{{\vec n}}(0)$ are constants. The angle $\theta_{\vec n}$ is called the “dynamic phase” while the angle $\gamma_{\vec n}$ is called the “geometric phase.” Both phases are real. The prime on $\psi_{\vec n}$ indicates the time derivative of the eigenfunction.

Note that if the Hamiltonian does not depend on time, the above expression simplifies to the usual solution of the Schrö­din­ger equation as given in chapter 7.1.2. In particular, in that case the geometric phase is zero and the dynamic phase is the usual $-E_{{\vec n}}t$$\raisebox{.5pt}{$/$}$$\hbar$.

Even if the Hamiltonian depends on time, the geometric phase is still zero as long as the Hamiltonian is real. The reason is that real Hamiltonians have real eigenfunctions; then $\gamma_{\vec n}$ can only be real, as it must be, if it is zero.

If the geometric phase is nonzero, you may be able to play games with it. Suppose first that Hamiltonian changes with time because some single parameter $\lambda$ that it depends on changes with time. Then the geometric phase can be written as

\gamma_{\vec n}= {\rm i}\int
\langle\psi_{\vec n}\vert
...gle{\,\rm d}\lambda
\equiv \int f(\lambda) {\,\rm d}\lambda

It follows that if you bring the system back to the state it started out at, the total geometric phase is zero, because the limits of integration will be equal.

But now suppose that not one, but a set of parameters $\vec\lambda$ $\vphantom0\raisebox{1.5pt}{$=$}$ $(\lambda_1,\lambda_2,\ldots)$ changes during the evolution. Then the geometric phase is

\gamma_{\vec n}= {\rm i}\int
\langle\psi_{\vec n}\vert\n...
f_2(\lambda_1,\lambda_2,\ldots) {\,\rm d}\lambda_2 + \ldots

and that is not necessarily zero when the system returns to the same state it started out at. In particular, for two or three parameters, you can immediately see from the Stokes’ theorem that the integral along a closed path will not normally be zero unless $\nabla_{\vec\lambda}\times\vec{f}$ $\vphantom0\raisebox{1.5pt}{$=$}$ 0. The geometric phase that an adiabatic system picks up during such a closed path is called “Berry’s phase.”

You might assume that it is irrelevant since the phase of the wave function is not observable anyway. But if a beam of particles is sent along two different paths, the phase difference between the paths will produce interference effects when the beams merge again.

Systems that do not return to the same state when they are taken around a closed loop are not just restricted to quantum mechanics. A classical example is the Foucault pendulum, whose plane of oscillation picks up a daily angular deviation when the motion of the earth carries it around a circle. Such systems are called “nonholonomic” or anholonomic.