A ''which-path'' (welcher Weg) measurement necessarily destroys the fr
inges in a double-slit interference experiment. We show that in all in
stances one may attribute this destruction to a disturbance of the par
ticle's momentum by an amount equal to at least pi h/2d, where d is th
e slit separation, in accordance with the uncertainty principle. Howev
er, this momentum transfer need not be local; that is, it need not act
at either of the slits through which the particle passes. For well-kn
own welcher Weg measurements such as Einstein's recoiling slit and Fey
nman's light microscope, the disturbance can be understood in terms of
random classical momentum kicks that act locally. In some recent prop
osals, including that by Scully, Englert, and Walther [Nature (London)
351, 111 (1991)], the momentum transfer is of a peculiarly quantum, n
onlocal nature. In this paper we introduce a formalism based on the Wi
gner function, as this describes both the local and nonlocal momentum
transfer caused by any welcher Weg measurement. We show that for some
examples, such as that of Scully, Englert, and Walther, there is no mo
mentum disturbance at the slits even though the nonlocal momentum dist
urbance is sufficient to destroy the interference pattern. Finally, we
discuss the experimental signatures of nonlocal versus local momentum
transfer and demonstrate a strong similarity to the nonlocality of th
e Aharonov-Bohm effect.