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?

Short Answer

Expert verified

Yes Q^is Hermitian.

The eigenvalues of the function are q=-n2,(n=0,1,2,)

There are two eigenfunctions which are the plus sign or the minus sign, in the exponent Therefore, the spectrum is doubly degenerate. A special case for n=0, which is not degenerate.

Step by step solution

01

Concept used

For a Hermitian operator (say Q), the following condition must be satisfied:

abg*Qfdx=abf(Qg)*dx

02

Calculate the eigenfunctions and eigenvalues

For a Hermitian operator (say Q), the following condition must be satisfied:

abg*Qfdx=abf(Qg)*dx

This condition can be written as follows using the more compact bracket notation:

gQ^f=Q^gf

Consider the operator,

Q^=d2dϕ2

Where, ϕis the azimuthal angle in polar coordinates. We must demonstrate that this operator is Hermitian, as follows:

fQ^g=02πf*d2gdϕ2dϕ=f*dgdϕ02π-02πdf*dϕdgdϕdϕ=f*dgdϕ02π-df*dϕg02π+02πd2f*dϕ2gdϕ

Due to the function's periodicity, the values of f(ϕ)and f(ϕ)are the same at 0 and 2π, so:

So, yes Q^is Hermitian.

Now we'll look for the operator's eigenvalues:

d2fdϕ2=q2f

This problem has two linearly independent solutions:

f1=eqϕ

f2=e-qϕ

The periodicity condition requires that:

f1(0)=f1(2π)

1=e2πq

We can deduct from this that q must be imaginary and is limited to the value:

q=ni

So, the eigenvalues are:

q=-n2,(n=0,1,2,)

For a given nthere are two eigenfunctions which are the plus sign or the minus sign, in the exponent Therefore, the spectrum is doubly degenerate. A special case for n=0, which is not degenerate.

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Most popular questions from this chapter

(a) Suppose that f(x)and g(x)are two eigenfunctions of an operatorQ^ , with the same eigenvalue q . Show that any linear combination of f andgis itself an eigenfunction of Q^, with eigenvalue q .

(b) Check that f(x)=exp(x)andg(x)=exp(-x) are eigenfunctions of the operatord2/dx2 , with the same eigenvalue. Construct two linear combinations of and that are orthogonal eigenfunctions on the interval(-1.1) .

(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.

Show that if hQ^h=Q^hhfor all functionsh(in Hilbert space), thenfQ^g=Q^fgfor allrole="math" localid="1655395250670" fandg(i.e., the two definitions of "Hermitian" -Equations 3.16 and 3.17- are equivalent).

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>.

Consider the wave functionΨ(x,0)={12ei2πx/λ,-<x<0,

wherenis some positive integer. This function is purely sinusoidal (with wavelengthλ)on the interval-<x<, but it still carries a range of momenta, because the oscillations do not continue out to infinity. Find the momentum space wave functionΦ(p,0). Sketch the graphs of|Ψ(x,0)|2and|Φ(p,0)|2, and determine their widths,wxandwp(the distance between zeros on either side of the main peak). Note what happens to each width asn. Usingwxandwpas estimates ofxandp, check that the uncertainty principle is satisfied. Warning: If you try calculatingσp, you're in for a rude surprise. Can you diagnose the problem?

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