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Find the form of operator ˆx1(t

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Quantum Mechanics List of Problems, Section 3 Problem 0 ) A warm up.

Suppose we have a free quantum particle confined in [0, d]. The corresponding Hamiltonian takes the form

H = −¯h2 2m

d2 dx2 ,

acts in L2(0, d) and the functions from its domain satisfy u(0) = u(d) = 0.

Find available energies and associated eigenvectors.

Problem 1)

Assuming that ˆH = 2m1 ˆ~p2 + ˆV (~r), find a) [ˆpj, ˆH] ,

b) [ˆxj, ˆH] , (j = 1, 2, 3).

Problem 2)

Suppose ˆH = 2m1 ˆ~p2 + ˆV (~r). Find the form of operator ˆx1(t) = ˆx(t) in the Heisenberg picture and position representation for

a) a free particle — ˆV (x) = 0,

b) harmonic oscillator — ˆV (x) = m ω222. Problem 3)

Check whether the operators ˆx(t1), ˆx(t2) expressed in the Heisenberg picture commutate.

Hint: use the result of Problem 2.

Problem 4)

Using the Schr¨odinger equation show the continuity equation

∂ρ

∂t + div ~j = 0, where ρ = |ψ(~r, t)|2. Furthermore, show a)

∂t

Z

R3

ρ(~r, t) d3~r = 0, 1

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, b) calculate div~j for the stationary states,

c) calculate ~j(ψp~(~r) where ψ~p(~r) is an eigenfuction of operator ˆp.~ Problem 5)

Find the eigenfuctions and eigenvalues of the energy operator for a particle moving in the potential field

V (x) =

( V0 if 0 ≤ x ≤ a, 0 if x < 0, x > a,

where V0 > 0 a > 0 (the barrier potential). Find the reflection and transition coefficients.

Problem 6)

a) Find the eigenfunctions and eigenvalues of the energy operator for a par- ticle moving in the potential field

V (x) =

( 0 if 0 ≤ x ≤ a, V0 if x < 0, x > a, and V0 > 0 (the well potential).

b) Consider the case V0 → ∞.

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