Difference between revisions of "Quantum Qual Problems"
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<math>H_1= \begin{pmatrix} 0 & v \\ v & 0\end{pmatrix}</math> | <math>H_1= \begin{pmatrix} 0 & v \\ v & 0\end{pmatrix}</math> | ||
where v is real. | where v is real. | ||
| + | Find the exact values of the energies of the new Hamitonlian, <math>H=H_0 + H_1</math> | ||
| − | + | ||
| + | b.) Assume that <math>w_1 - w_2 >> |v|</math> | ||
Revision as of 21:10, 17 August 2007
1.) Given a quantum mechanical particle of mass confined inside a box of sides . The particle is allowed to move freely between and .
- Use the time-independent Schrodinger equation for this problem to obtain the general form for the eigenfunctions of the particle
- Now apply boundary conditions to obtain the specific eigenfunctions and eigenenergies for this specific problem.
- Assume and find the first 6 eigenenergies of the problem in terms of the box side length (), the particle mass () and standard constants. What are their quantum number? Make a sketch of the eigenvalue spectrum, a table listing these eigenenergies and the quantum numbers of all the states that correspond to them.
Solution: Qal_QuantP1S
2.) A system has two energy eigenstate with eigenvalues and . Assume that . Representing the enegy eigenstate by and . The Hamiltonian can be written as
a.) We introduce and interaction whose matrix elements, using the above basis vectors, are where v is real. Find the exact values of the energies of the new Hamitonlian,
b.) Assume that