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
, where a, b, and c are real numbers.
(a) If the system starts out in the state what is ?
(b) If the system starts out in the state what is ?
An anti-Hermitian (or skew-Hermitian) operator is equal to minus its Hermitian conjugate:
(a) Show that the expectation value of an anti-Hermitian operator is imaginary. (b) Show that the commutator of two Hermitian operators is anti-Hermitian. How about the commutator of two anti-Hermitian operators?
Supposefor constants Aand 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.
Extended uncertainty principle.The generalized uncertainty principle (Equation 3.62) states that
where.
(a) Show that it can be strengthened to read
[3.99]
where. Hint: Keep the term in Equation 3.60
(b) Check equation 3.99 for the case(the standard uncertainty principle is trivial, in this case, since; unfortunately, the extended uncertainty principle doesn't help much either).
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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