Chapter 3: Q13P (page 112)
(a) Prove the following commutator identity:
b) Show that
(c) Show more generally that
for any function.
Short Answer
a)
b)
c)
Chapter 3: Q13P (page 112)
(a) Prove the following commutator identity:
b) Show that
(c) Show more generally that
for any function.
a)
b)
c)
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Get started for freeThe Hamiltonian for a certain three-level system is represented by the matrix
Two other observables, A and B, are represented by the matrices ,where ω, , and μ are positive real numbers.
(a)Find the Eigen values and (normalized) eigenvectors of H, A and B.
(b) Suppose the system starts out in the generic staterole="math" localid="1656040462996"
with . Find the expectation values (at t=0) of H, A, and B.
(c) What is ? If you measured the energy of this state (at time t), what values might you get, and what is the probability of each? Answer the same questions for A and for B.
(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.
Prove the famous "(your name) uncertainty principle," relating the uncertainty in position to the uncertainty in energy:
For stationary states this doesn't tell you much-why not?
Suppose for constantsA and a.
(a) Determine A, by normalizing
(b) Find, and(at time).
(c) Find the momentum space wave function, and check that it is normalized.
(d) Useto calculate, and(at time).
(e) Check the Heisenberg uncertainty principle for this state.
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