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Let Q^be an operator with a complete set of orthonormal eigenvectors:localid="1658131083682" Q^en>=qnen(n=1,2,3,....) Show thatQ^can be written in terms of its spectral decomposition:Q^=nqnen><en|

Hint: An operator is characterized by its action on all possible vectors, so what you must show is thatQ^={nqnen><en|} for any vector α>.

Short Answer

Expert verified

The operator can be written as a spectral decomposition operator Q^=nqnen><en|.

Step by step solution

01

Spectral decomposition operator

The underlying vector space on which the operator functions is further decomposed canonically by the spectral decomposition, which is provided by the spectral theorem. Every real, symmetric matrix is diagonalizable according to the spectral theorem for symmetric matrices, which was established by Augustin-Louis Cauchy.

02

Write the operator as a spectral decomposition operator

Consider an operatorQ^with a complete, orthonormal set of eigenvectors, that is:

Q^em>=qmem>

Whereqmis the eigenvalue. Write the operator as a spectral decomposition operator.

First, write any vectorα>in terms of the eigenvectors set, since the eigenvectors of form a complete, orthonormal set:

α>=mamem>

Here amis the coefficient of the basis vector em>. Now apply Q^on this equation and get the result as:

Q^α>=mamqmem>

Write Q^as:

Q^=nqne><en|

then:

role="math" localid="1658132420035" Q^α>=nqnen><en|mamem>=n,mqnamδnme><em|=mamqmem>

So:

Q=nqnen><en|

Thus, the operator can be written as a spectral decomposition operator Q=nqnen><en|.

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Most popular questions from this chapter

Consider a three-dimensional vector space spanned by an Orthonormal basis 1>,2>,3>. Kets α>and β>are given by

|α=i|1-2|2-i|3,|β>=i|1+2|3.

(a)Construct<αand <β(in terms of the dual basis

1|,2|,3|).
(b) Find αβandβα,and confirm that

βα=αβ*.
(c)Find all nine matrix elements of the operatorA|αβ|, in this basis, and construct the matrix A. Is it hermitian?

(a) Cite a Hamiltonian from Chapter 2 (other than the harmonic oscillator) that has only a discrete spectrum.

(b) Cite a Hamiltonian from Chapter 2 (other than the free particle) that has only a continuous spectrum.

(c) Cite a Hamiltonian from Chapter 2 (other than the finite square well) that has both a discrete and a continuous part to its spectrum.

Consider the operator Q^=d2/dϕ2, where (as in Example 3.1)ϕ is the azimuthal angle in polar coordinates, and the functions are subject to Equation 3.26. Is Q^Hermitian? Find its eigenfunctions and eigenvalues. What is the spectrum of Q^? Is the spectrum degenerate?

Coherent states of the harmonic oscillator. Among the stationary states of the harmonic oscillator (Equation 2.67) only n = 0 hits the uncertainty limit (σxσp=h/2); in general, σxσp=(2n+1)h/2, as you found in Problem 2.12. But certain linear combinations (known as coherent states) also minimize the uncertainty product. They are (as it turns out) Eigen functions of the lowering operator

ψn=1n!(a^+)nψ0(2.68).

a_|α>=α|a>(the Eigen value α can be any complex number).

(a)Calculate <x>,<x2>,<p>,<p2>in the state |α〉. Hint: Use the technique in Example 2.5, and remember that is the Hermitian conjugate of a-. Do not assume α is real.

(b) Find σx; show that σxσp=h/2.

(c) Like any other wave function, a coherent state can be expanded in terms of energy Eigen states: |α>=n=0Cn|n>.

Show that the expansion coefficients arecn=αnn!c0.

(d) Determine by normalizing |α〉. Answer: exp(-α2/2)

(e) Now put in the time dependence: |n>e-iEntIh|n>,

and show that |αt|remains an Eigen state of a-, but the Eigen value evolves in time:α(t)=e-iωt So a coherent state stays coherent, and continues to minimize the uncertainty product.

(f) Is the ground state (n=0>)itself a coherent state? If so, what is the Eigen value?

(a) Check that the eigenvalues of the hermitian operator in Example 3.1 are real. Show that the eigenfunctions (for distinct eigenvalues) are orthogonal.

(b) Do the same for the operator in Problem 3.6.

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