Homework Set 1: Difference between revisions

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<math> [\hat{M},f(\hat{M})]=0 </math>.
<math> [\hat{M},f(\hat{M})]=0 </math>.
== Problem 4: Successive measurements on subsystems of composite bipartite quantum system ==
Consider a quantum system composed of two spins, labeled as subsystem ''A'' and ''B''. The quantum state of the composite system is described by the following density matrix in the Hilbert space <math> \mathcal{H}_A \otimes \mathcal{H}_B </math>:
<math> \hat{\rho} = \frac{1}{8} \hat{I} + \frac{1}{2} |\Psi\rangle \langle \Psi| </math>
where <math> \hat{I}  </math> denotes the <math> 4 \times 4 </math> unit matrix in <math> \mathcal{H}_A \otimes \mathcal{H}_B </math> and
<math> |\Psi \rangle = \frac{1}{\sqrt{2}}\left( |\uparrow \rangle \otimes |\downarrow \rangle - |\downarrow \rangle \otimes |\uparrow \rangle \right) </math>
is an entangled state (in the context of spins also called "singlet") of two spins.
Suppose we measure the first spin (subsystem ''A'') along the axis described by the unit vector <math> \mathbf{n} </math>, and the second spin (subsystem ''B'') along the axis described by the unit vector <math> \mathbf{m} </math>, where <math> \mathbf{n} \cdot \mathbf{m} = \cos \theta </math>. ''What is the probability that both spins are "spin-up" along their respective axes?''
'''HINT:''' In general, the probability to measure eigenvalue <math> \lambda </math> of a physical quantity in the quantum state described by the density matrix <math> \hat{\rho} </math> is given by <math> \mathrm{prob} = \mathrm{Tr}[ \hat{\rho} \hat{P}_\lambda]</math>. Here <math> \hat{P}_\lambda </math> is the projection operator on the eigensubspace corresponding to eigenvalue <math> \lambda </math>. To find the probability of measurement on the subsystem, one should use the density matrix of that subsystem, obtained by partial trace over the states
of the second subsystem. This means that the probability asked in the problem is defined by:
<math> \mathrm{prob} = \mathrm{Tr}_B \left\{ \hat{P}_\mathbf{m}^B \hat{\rho}^B \right\} =  \mathrm{Tr}_B \left\{ \hat{P}_\mathbf{m}^B  \mathrm{Tr}_A \left[(\hat{P}_\mathbf{n}^A \otimes \hat{I}^B) \hat{\rho} \right] \right\} </math>.
The eigenprojector for the "spin-up" (i.e., +1) eigenvalue along the <math> \mathbf{n} </math>-axis is simply:
<math> \hat{P}_\mathbf{n}^A = |\uparrow_\mathbf{n} \rangle \langle \uparrow_\mathbf{n}| = \frac{1}{2} \left( \hat{I}^A + \mathbf{n} \cdot \hat{\boldsymbol{\sigma}}^A \right) </math>.
We also use the fact that resulting state of the composite system after the selective measurement on subsystem ''A'' is described by the density matrix <math> \hat{P}_\mathbf{n}^A \hat{\rho} \hat{P}_\mathbf{n}^A </math>, so that subsystem ''B'' after the measurement on system ''A'' is "collapsed" onto the state described by the density matrix  <math> \hat{\rho}^B = \mathrm{Tr}_A [\hat{P}_\mathbf{n}^A \hat{\rho} \hat{P}_\mathbf{n}^A]= \mathrm{Tr}_A [\hat{P}_\mathbf{n}^A \hat{\rho}] </math>.

Revision as of 17:58, 1 March 2016

Problem 1: Pure vs. mixed quantum states

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:


,


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


, where .


Here and Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle |\downarrow\rangle } are the eigenstates of the Pauli spin matrix Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\sigma}_z } :


Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\sigma}_z |\uparrow \rangle = +1 |\uparrow \rangle, \ \hat{\sigma}_z |\downarrow \rangle = -1 |\downarrow \rangle } .


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 expectation value Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle P_{x,y,z} = \langle \sigma_{x,y,z}\rangle =\mathrm{Tr}\, [\hat{\rho} \hat{\sigma}_{x,y,z}] } . The colloquial "spin-polarization" discussed in spintronics literature is Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle |\mathbf{P}| } in precise formal language.

Problem 2: Dynamics of Bloch vector

The Hamiltonian of a single spin of an electron in external magnetic field Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \mathbf{B} } is given by (assuming that gyromagnetic ration is unity):

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{H} = -\frac{\hbar}{2} \mathbf{B} \cdot {\boldsymbol{\sigma}} }

where Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \boldsymbol{\sigma}=(\hat{\sigma}_x,\hat{\sigma}_y,\hat{\sigma}_z) } is the vector of the Pauli matrices. Show that the equation of motion

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle i \hbar \frac{\partial \hat{\rho}}{\partial t} = [\hat{H},\hat{\rho}] }

for the density matrix of spin-Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \frac{1}{2} } discussed in the class

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\rho} = \frac{1}{2} \left( 1 + \mathbf{P} \cdot \boldsymbol{\sigma} \right) }

can be recast into the equation of motion for the spin-polarization (or Bloch) vector

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \frac{d \mathbf{P}}{dt} = -\mathbf{B} \times \mathbf{P} }

since Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \mathbf{\rho} } and Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \mathbf{P} } are in one-to-one correspondence.

HINT: Use the following property of the Pauli matrices:

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\sigma}_\alpha \hat{\sigma}_\beta - \hat{\sigma}_\beta \hat{\sigma}_\alpha = 2 i \epsilon_{\alpha \beta \gamma} \hat{\sigma}_\gamma } .

Problem 3: Does entropy increase in closed quantum systems?

In classical Hamiltonian systems the nonequilibrium entropy

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle S = -k_B \int \rho \ln \rho }

is constant. In this problem we want to demonstrate that in microscopic evolution of an isolated quantum system, the entropy is also time independent, even for general time-dependent density matrix Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\rho} } . That is, using the equation of motion:

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle i \hbar \frac{\partial \hat{\rho}}{\partial t} = [\hat{H},\hat{\rho}] }

prove that von Neumann entropy

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle S(t) =-k_B \mathrm{Tr}[\hat{\rho}(t) \ln \hat{\rho}(t)] }

is time independent for arbitrary density matrix Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{\rho}(t) } .

HINT: Use Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \mathrm{Tr}(\hat{A}\hat{B}\hat{C})=\mathrm{Tr}(\hat{C}\hat{A}\hat{B}) } for any operators Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{A} } , Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{B} } , Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{C} } , as well as that an operator Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle \hat{M} } commutes with any function Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle f(\hat{M}) } :

Failed to parse (SVG with PNG fallback (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle [\hat{M},f(\hat{M})]=0 } .

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