We show that in calculating the semiclassical energy levels of electrons in
metals located in a magnetic field, one must determine whether or not the
corresponding electron paths in the space of wave vectors k are attached to
a band degeneracy line. Calculations in the two possible cases, i.e., with
and without such attachment, differ by \e\(h) over bar/2m*c, where e is th
e electron charge and m* is the cyclotron mass of the electron. This shift
in the energy levels is of a topological nature, and its existence depends
neither on the specific form of the electron dispersion relation epsilon(k)
near the electron path nor on the shape or size of this path. The reason f
or this shift lies in the fact that the electron orbit is attached to the b
and degeneracy line, which is the line of singular points of the Bloch wave
functions. In many respects this effect is similar to the Aharonov-Bohm ef
fect if the band degeneracy line is considered an infinitely thin "solenoid
." This shift in energy levels should become apparent in studies of oscilla
tion phenomena in metals. We give examples of metals in which the condition
s for observing the shift is probably the most favorable. (C) 1998 American
Institute of Physics. [S1063-7761(98)01510-8].