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Harvard University. Physics 143b: Quantum Mechanics II. Practice Final exam. 1. We refer to the states of a qubit using the eigenstates |T>, |+> of σz, ...
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Harvard University
Practice Final exam
V (x) =
{ 0 , 0 < x < L/ 2 V 0 , L/ 2 < x < L ,^0 < t < T,^ (1)
where V 0 is small, and the potential returns to V (x) = 0 for t > T. What is the probability that a measurement of the energy of the particle at some time t > T yields the value E 2? You need only determine this to order V 02 , using time-dependent perturbation theory. (c) Now consider instead the situation in which the particle was in the state ψ 1 (x) at time t = 0, and for t > 0 the potential in the box became time-dependent but remained space-independent
V (x, t) = f (t) for t > 0 and 0 < x < L (2)
where f (t) is an arbitrary function of time, but is independent of x. What is the exact wavefunction for all t > 0? Do not use perturbation theory here, but obtain the answer by exactly integrating the time-dependent Schr¨odinger equation.
x d dx +^ mσ
z
) Ψ(x) = EΨ(x) (3)
where σx,z^ are the Pauli matrices, the wavefunction Ψ(x) has 2 components, and we have set c = 1. (a) Show that the wavefunction of a particle with energy E = √p^2 + m^2 can be written as Ψ(x) =
( cos(θ/2) sin(θ/2)
) eipx/¯h^ (4) where tan θ = p/m. Here, and below, we assume that the symbol p is positive, so that Eq. (4) represents a particle moving to the right. (b) Similarly show that the wavefunction of a particle with momentum −p i.e. a particle moving to the left, is
Ψ(x) =
( cos(θ/2) − sin(θ/2)
) e−ipx/¯h^ (5)
(c) As shown in the class notes, the current carried by such a particle is J = Ψ†σxΨ. Determine J for the states in (a) and (b). Interpret your result in terms of the group velocity of a wave packet.