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This is the Past Exam of Quantum Mechanics which includes Wavefunction for Particle, Valid Wavefunction, Stern Gehrlach Device, Square Barrier, Spin System etc. Key important points are: Spin System, Energy Eigenstates and Eigenvectors, Hamiltonian Transform, Eigenstate Transform, Rotationally Invariant, Half-Integer Value, Hilbert Space, Clebsch Gordan Coefficients, Harmonic Oscillator
Typology: Exams
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Time: Tuesday 24 oktober, 2006, 8: Place: V-huset Examiner: Stellan Ostlund (0708-723201) (on travel)¨ Ling Bao (031-7723184) Additional material: Your course text. You may not have extensive handwrit- ten notes in the book. If you do, you will be asked to ex- change the book for one without notes. You may also borrow BETA , if necessary from each other if absolutely necessary.
I strongly suggest you go directly to the problems you know how to do and get them out of the way. Think about substituting a symmetry or physical argument instead of messy algebra; the algebra can thereby be drastically reduced in most of these problems. Please choose one of Problem 6-alt 1 or Problem 6-alt 2 and indicate on the front which of those two you want us to correct.
The Hamiltonian for a spin-1 system is given by
H = AS z^2 + B(S x^2 − S^2 y )
The Hamiltonian for three spins is given by
H = SA · SB + SB · SC + SC · SA
For arbitrary value integer and half-integer value of the spin S,
For the Zeeman-like Hamiltonian
HZ = α L · S + β(Lz + Sz )
write down exactly the eigenvalues and eigenfunctions in the | lz , sz 〉 basis for the case l = 1 and s = 1/2. The prefactor in front of Sz should really be 2, but I have made it 1 to keep the problem simple.
Compute exactly the eigenvalues of the following Hamiltonian
H = a†a + λ(a + a†)
where [ a, a†^ ] = 1.
Unpolarized spin 1/2 atoms are coming out of an oven in three identical distinct beams. Each beam A,B and C is passed through a filter, each selecting atoms with polarization 120 degrees from each other, resulting in density matrices ρA , ρB and ρC. Assume that beam A is polarized along z. Recall the formula for entropy of a mixture S = −k T r ρ ln( ρ ).
Now insert the mixture of B and C into a magnetic field B ˆx corresponding to a Hamiltonian H = μBSx.