Expanding the fields of a laser cavity in a set of orthonormal modes i
s a standard technique in laser theory. Expansion in a normal mode set
is also the basis of the concept of ''photons''. A substantial number
of practical lasers do not, however, support any kind of normal or or
thogonal cavity modes, and thus, their fields cannot be represented (a
t least not easily) in terms of normal modes, or photons. This leads t
o a number of unusual results, including situations in which the fewes
t-order made of a cavity can contain substantially more energy than th
e total energy in the cavity, as well as enhanced quantum spontaneous
emission far stronger than the ''single extra photon'' level character
istic of an ordinary laser oscillator. We review the theoretical origi
ns of these unusual effects and present experimental confirmation of g
reatly enhanced Schawlow-Townes fluctuations in an unstable-resonator
laser with a Petermann-noise enhancement factor of several hundred tim
es.