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(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.

Short Answer

Expert verified

a) Infinite square well.

b) Finite rectangular barrier.

c) Finite square well.

Step by step solution

01

Example of a Hamiltonian that has a discrete spectrum

a)

The infinite square well Hamiltonian is an example of a Hamiltonian with a discrete spectrum. Recall that all energies Encorresponding to this Hamiltonian are discrete.

02

Example of a Hamiltonian that has a continuous spectrum

b)

The finite rectangular barrier Hamiltonian is an example of a Hamiltonian with a continuous spectrum. Recall that all energies corresponding to this Hamiltonian are continuous.

03

Example of a Hamiltonian that has both continuous and discrete spectrum

c)

The finite square well Hamiltonian is an example of a Hamiltonian with both a continuous and discrete spectrum. Recall that this Hamiltonian admits both bound (discrete spectrum) and scattering (continuous spectrum) status.

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Most popular questions from this chapter

Extended uncertainty principle.The generalized uncertainty principle (Equation 3.62) states that

ฯƒA2ฯƒB2โ‰ฅ14<C>2

whereC^โ‰ก-i[A^,B^ฬ‚]..

(a) Show that it can be strengthened to read

ฯƒA2ฯƒB2โ‰ฅ14(<C>2+<D>2) [3.99]

whereD^โ‰กA^B^+B^A^-2โŸจAโŸฉโŸจBโŸฉ.. Hint: Keep the term in Equation 3.60

(b) Check equation 3.99 for the caseB=A(the standard uncertainty principle is trivial, in this case, sinceC^=0; unfortunately, the extended uncertainty principle doesn't help much either).

(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).

Consider the wave functionฮจ(x,0)={12vฮปei2ฯ€x/ฮป,-nฮป<x<nฮป0,

wherenis some positive integer. This function is purely sinusoidal (with wavelengthฮป)on the interval-nฮป<x<nฮป, but it still carries a range of momenta, because the oscillations do not continue out to infinity. Find the momentum space wave functionฮฆ(p,0). Sketch the graphs of|ฮจ(x,0)|2and|ฮฆ(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 asnโ†’โˆž. Usingwxandwpas estimates ofโˆ†xandโˆ†p, check that the uncertainty principle is satisfied. Warning: If you try calculatingฯƒp, you're in for a rude surprise. Can you diagnose the problem?

A harmonic oscillator is in a state such that a measurement of the energy would yield either(1/2)hฯ‰or (3/2) hฯ‰, with equal probability. What is the largest possible value of in such a state? If it assumes this maximal value at time t=0 , what is ฯˆ(x,t) ?

Is the ground state of the infinite square well an eigenfunction of momentum? If so, what is its momentum? If not, why not?

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