Within the traditional Hilbert space formalism of quantum mechanics, it is
not possible to describe a particle as possessing, simultaneously, a sharp
position value and a sharp momentum value. Is it possible, thought, to desc
ribe a particle as possessing just a sharp position value (or just a sharp
momentum value)? Some, such as Teller, have thought that the answer to this
question is No--that the status of individual continuous quantities is ver
y different in quantum mechanics than in classical mechanics. On the contra
ry, I shall show that the same subtle issues arise with respect to continuo
us quantities in classical quantum mechanics; and that it is , after all, p
ossible to describe a particle as possessing a sharp position value without
altering the standard formalism of quantum mechanics.