(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) .

Short Answer

Expert verified

(a) The linear combination of f and g is an eigenfunction of the operatorQ^ .

(b) Both of f(x) and g(x) are eigenfunctions of the operator d2/dx2, with the same eigenvalue of l . The two linear combinations of f(x) and g(x) are orthogonal.

Step by step solution

01

Definition of eigenfunction.

The eigenfunction is a function f of an operator A that provides the same function f when operator A is applied on f. Mathematically, it can be written as,

A^f=kf

Here, k is the constant known as eigen value.

02

Prove for part (a).

(a)

Assuming f(x)and g(x)are two eigenfunctions of an operator Q^, with the same eigenvalue q , we must demonstrate that any linear combination of f and g is an eigenfunction of the operator Q^Q^f=qf

And

Q^g=qg

And let us consider a function:

$h(x)=af(x)+bg(x)$

Where a and b are an arbitrary constant.

On solving the Therefore:

Q^h=Q^(af+bg)=a(Q^f)+b(Q^g)=a(qf)+b(qg)=q(af+bg)=qh

So, the linear combination of and is an eigenfunction of the operator Q^.

03

Check for the given function and construction of linear combination

(b)

Check that f(x)=ex and g(x)=e-xare eigenfunctions of the operator d2/dx2, as:

d2fdx2=d2dx2ex=ddxex=ex=f

And for g(x)as:

d2gdx2=d2dx2e-x=ddx-e-x=e-x=g

Therefore, both of f(x) and g(x)are eigenfunctions of the operator d2/dx2, with the same eigenvalue of 1, the two linear combinations of the functions are:

sinh(x)=12ex-e-x=12(f-g)

And,

cosh(x)=12ex+e-x=12(f+g)

Since is odd and is even, then the two linear combinations of f(x)and g(x) are orthogonal in the interval (-1,1).

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Most popular questions from this chapter

Test the energy-time uncertainty principle for the free particle wave packet in Problem 2.43and the observable x , by calculating σHσx , and d<x>/dtexactly.

Find the matrix elements <n|x|n'>a­­­­nd <n|p|n'>in the (orthonormal) basis of stationary states for the harmonic oscillator (Equation 2.67). You already calculated the "diagonal" elements (n=n') in Problem 2.12; use the same technique for the general case. Construct the corresponding (infinite) matrices, X and P . Show that(1/2m)P2+(2/2)X2=His diagonal, in this basis. Are its diagonal elements what you would expect? Partial answer:

<n|x|n'>=h2mω(n'δn,n'-1+nδn,n'-1)

(a) Prove the following commutator identity:

[AB.C]=A[B.C]+[A.C]B

b) Show that

[xn,p]=ihnxn-1

(c) Show more generally that

[f(x),p]=ihdfdx

for any functionf(x).

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?

Apply Equation 3.71 to the following special cases: (a)Q=1; (b)Q=H; (c)Q=x; (d)Q=p. In each case, comment on the result, with particular reference to Equations 1.27,1.33,1.38, and conservation of energy (comments following Equation 2.39).

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