kakarukeys
- 187
- 0
Given a system,
H = H_0 + V
V is a small perturbation that does not depend on time.
the system is in |E_0> at time t_0
H_0 |E_n> = E_n |E_n>
H_0 |E_0> = E_0 |E_0>
Let |\Psi(t)> be the solution of the system.
Let |\Phi(t)> be the solution of the system without perturbation.
Let |u(t)> = |\Psi(t)> - |\Phi(t)>.
Show that |<E_n|u(t)>|^2 = 4 |V_{n0}|^2 [{{\sin(t - t_0)(E_n - E_0)/\hbar}\over{E_n - E_0}}]^2
at lowest order
No matter how many times I try, the answer I get is
|<E_n|u(t)>|^2 = 2 |V_{n0}|^2 [{{1 - \cos(t - t_0)(E_n - E_0)/\hbar}\over{E_n - E_0}}]^2
Please help!
H = H_0 + V
V is a small perturbation that does not depend on time.
the system is in |E_0> at time t_0
H_0 |E_n> = E_n |E_n>
H_0 |E_0> = E_0 |E_0>
Let |\Psi(t)> be the solution of the system.
Let |\Phi(t)> be the solution of the system without perturbation.
Let |u(t)> = |\Psi(t)> - |\Phi(t)>.
Show that |<E_n|u(t)>|^2 = 4 |V_{n0}|^2 [{{\sin(t - t_0)(E_n - E_0)/\hbar}\over{E_n - E_0}}]^2
at lowest order
No matter how many times I try, the answer I get is
|<E_n|u(t)>|^2 = 2 |V_{n0}|^2 [{{1 - \cos(t - t_0)(E_n - E_0)/\hbar}\over{E_n - E_0}}]^2
Please help!