# 07 - Physics 6210/Spring 2007/Lecture 7 Lecture 7 Relevant sections in text 1.6 Observables with continuous and/or unbounded values We are now

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Physics 6210/Spring 2007/Lecture 7 Lecture 7 Relevant sections in text: § 1.6 Observables with continuous and/or unbounded values We are now ready to turn to the quantum mechanical description of a (non-relativistic) particle. We shall deﬁne a (spinless) particle as a system that is completely characterized by the position and linear momentum, which are the basic observables in this model. This means that all observables are functions of position and momentum. While it is possible that the position and momentum variables take a discrete set of values (as angular momentum and – often – energy do), there is currently no experimental evidence of this. We therefore create a model in which these observables can take a continuous, unbounded set of values. Evidently, we need to deﬁne a Hilbert space that admits self-adjoint operators with a continuous, unbounded spectrum. Neither of these features are possible on ﬁnite- dimensional vector spaces, and so here we are forced into the inﬁnite-dimensional setting ( i.e., spaces of functions). This leads to some mathematical subtleties that we need to be wary of. I shall not try to be perfectly rigorous in our discussion since that would take us too far aﬁeld. But I will try to give you a reasonably fool-proof – if somewhat formal – treatment. First, let me give you a recipe for dealing with the situation. Then let me give you a ﬂavor of the underlying mathematics which makes the formal recipe work (and also which shows where it can become tricky). Formal recipe We want to deﬁne an observable A with a continuous, unbounded set of values a R , say. We postulate the existence of a self-adjoint linear operator, again denoted A , and a continuous set of vectors | a i such that A | a i = a | a i . We say that A has a “continuous” spectrum. These vectors are to be “orthonormal in the delta-function sense”: h a | a 0 i = δ ( a, a 0 ) . You can think of this as a continuum generalization of the usual orthonormality expressed via the Kronecker delta. The vectors | a i are to form a basis, that is, they provide a continuous resolution of the identity: I = Z -∞ da | a ih a | , 1

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Physics 6210/Spring 2007/Lecture 7 so that we can write | ψ i = Z -∞ da | a ih a | ψ i . Using quotation marks to indicate where the underlying mathematics is considerably more subtle than the words indicate, we can say the following. We interpret the “eigenval- ues” a as the possible values of an outcome of the measurement of A , the vectors | a i are “states” in which A has the value a with certainty. The scalar |h a | ψ i| 2 da is the probability for ﬁnding A to have the value in the range [ a, a + da ] in the state | ψ i . In particular, the probability that the observable A
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## This note was uploaded on 02/18/2012 for the course PHYSICS 6210 taught by Professor M during the Spring '07 term at AIU Online.

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07 - Physics 6210/Spring 2007/Lecture 7 Lecture 7 Relevant sections in text 1.6 Observables with continuous and/or unbounded values We are now

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