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bznm
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I have solved this exercise, but I'm not sure that it is good. Please, can you check it? A lot of thanks!
1. Homework Statement
The hamiltonian is ##H_0=\epsilon |1><1|+5/2 \epsilon (|2><2|+|3><3|)##
The perturbation is given by ##\Delta(|2><3|+|3><2|)##
Discuss the degeneration of H0.
Using perturbation theory, find energy-level shift and their eigenvectors.
Solve *exaclty* the problem with ##H=H_0+V##
Consider ##\Delta=\epsilon/2## . In t=0, the system is described by ##|s(0)>=|2>##,. Find ##|s(t)>##2. The attempt at a solution
H is degenerative: the eigenvalue relative to the vector |1> is epsilon. But vectors |2> and |3> have the same eigenvalue.
The energy level related to |1> hasn't energy shift produced by V.
Energy shifts for |2> and |3> are ##\pm \Delta##
For ##\lambda=\Delta## the eigenvector is ##|v_1>=1/ \sqrt 2 (|2>+|3>)##
For ##\lambda=- \Delta## the eigenvector is ##|v_2>=1/ \sqrt 2 (|2>-|3>)##
The exactly resolution of the problem, give me the eigenvalues: ##\lambda_1= \epsilon##, ##\lambda_2= 5/2 \epsilon + \Delta##, ##\lambda_3= \epsilon##. The corresponding eigenvectors are ##v_0=|1>##, ##|v_1>=1/ \sqrt 2 (|2>+|3>)## ,##|v_2>=1/ \sqrt 2 (|2>-|3>)##
The last point is the one that I'm not so sure that could be good:
I have written |2> as linear combination of |v_1> and v_2>:
##|2>= 1/ \sqrt 2 (|V_1>+|v_2>##, so
##|s(t)>=e^{-iHt/ \hbar} 1/ \sqrt 2 (|V_1>+|v_2>)= 1/ \sqrt 2 e^{-i2 \epsilon t / \hbar} (|v_2>+e^{-i \epsilon t / \hbar} |v_1>)##
1. Homework Statement
The hamiltonian is ##H_0=\epsilon |1><1|+5/2 \epsilon (|2><2|+|3><3|)##
The perturbation is given by ##\Delta(|2><3|+|3><2|)##
Discuss the degeneration of H0.
Using perturbation theory, find energy-level shift and their eigenvectors.
Solve *exaclty* the problem with ##H=H_0+V##
Consider ##\Delta=\epsilon/2## . In t=0, the system is described by ##|s(0)>=|2>##,. Find ##|s(t)>##2. The attempt at a solution
H is degenerative: the eigenvalue relative to the vector |1> is epsilon. But vectors |2> and |3> have the same eigenvalue.
The energy level related to |1> hasn't energy shift produced by V.
Energy shifts for |2> and |3> are ##\pm \Delta##
For ##\lambda=\Delta## the eigenvector is ##|v_1>=1/ \sqrt 2 (|2>+|3>)##
For ##\lambda=- \Delta## the eigenvector is ##|v_2>=1/ \sqrt 2 (|2>-|3>)##
The exactly resolution of the problem, give me the eigenvalues: ##\lambda_1= \epsilon##, ##\lambda_2= 5/2 \epsilon + \Delta##, ##\lambda_3= \epsilon##. The corresponding eigenvectors are ##v_0=|1>##, ##|v_1>=1/ \sqrt 2 (|2>+|3>)## ,##|v_2>=1/ \sqrt 2 (|2>-|3>)##
The last point is the one that I'm not so sure that could be good:
I have written |2> as linear combination of |v_1> and v_2>:
##|2>= 1/ \sqrt 2 (|V_1>+|v_2>##, so
##|s(t)>=e^{-iHt/ \hbar} 1/ \sqrt 2 (|V_1>+|v_2>)= 1/ \sqrt 2 e^{-i2 \epsilon t / \hbar} (|v_2>+e^{-i \epsilon t / \hbar} |v_1>)##