Tunneling modes, elementary excitations of a large class of glasses, a
re local dynamical signatures of disorder. There is one tunneling mode
per odd loop (a necklace through odd rings in the network), decoupled
from other loops, and tunneling is forced by gauge invariance of the
structure, the symmetry of disorder. Absence of tunneling modes in tri
valent glasses (a-As or B2O3) is a notable consequence of this model.
It is possible to decompose topologically a tetravalent network into a
trivalent network, and to add a large proportion of boroxol rings wit
h their characteristic but different dynamical signature.