Temporary HW

Problem 1

A researcher in spintronics is investigated two devices in order to generate spin-polarized currents. One of those devices has spins comprising the current described by the density matrix:

${\hat{\rho }}_1=\frac{|\uparrow ⟩⟨\uparrow |+|\downarrow ⟩⟨\downarrow |}{2}$,

while the spins comprising the current in the other device are described by the density matrix

${\hat{\rho }}_2=|u⟩⟨u|$ , where $|u⟩=\frac{e^{i\alpha }|\uparrow ⟩+e^{i\beta }|\downarrow ⟩}{\sqrt{2}}$.

Here $|\uparrow ⟩$ and $|\downarrow ⟩$ are the eigenstates of the Pauli spin matrix ${\hat{\sigma }}_z$:

${\hat{\sigma }}_z|\uparrow ⟩=+1|\uparrow ⟩,{\hat{\sigma }}_z|\downarrow ⟩=-1|\downarrow ⟩$.

What is the spin polarization of these two currents? Comment on the physical meaning of the difference between the spin state transported by two currents.

HINT: Compute the x, y, and z components of the spin polarization vector using both of these density matrices following the quantum-mechanical definition of an average value $P_{x,y,z}=⟨{\sigma }_{x,y,z}⟩=\mathrm{T}\mathrm{r}[\hat{\rho }{\hat{\sigma }}_{x,y,z}]$.

Problem 2

The Hamiltonian of a single spin in external magnetic field $\mathbf{𝐁}$ is given by (assuming that gyromagnetic ration is unity):

$\hat{H}=-\frac{\hslash }{2}\mathbf{𝐁}\cdot \mathit{\sigma }$

where $\mathit{\sigma }=({\sigma }_x,{\sigma }_y,{\sigma }_z)$ is the vector of the Pauli matrices. Show that the equation of motion for the density matrix of spin-$\frac{1}{2}$ discussed in the class

$\mathit{\rho }=\frac{1}{2}(1+\mathbf{𝐏}\cdot \mathit{\sigma })$

is can be written as:

$\mathit{\rho }=\frac{1}{2}(1+\mathbf{𝐏}\cdot \mathit{\sigma })$

$\frac{dP}{dt}$