In perturbation theory, the second corrections to the energy are given by Hm |H'E,n| E ()...

 

Transcribed Image Text:

In perturbation theory, the second corrections to the energy are given by Hm |H'E,n|² E (²) => mfn mn EO) - E -1 + -dE (0) where the first sum is over the discrete energy levels and the second over the continuous energy levels. Considering the case of the helium atom, where H' = e² 47E0712 no one has been able to evaluate the second-order correctness of the ground state (n = 1); Let's see how complex it is to calculate /H'mn Determine, with Z = 2: a) H(200) (100) ² b) H(300)(100) ² In perturbation theory, the second corrections to the energy are given by Hm |H'E,n|² E (²) => mfn mn EO) - E -1 + -dE (0) where the first sum is over the discrete energy levels and the second over the continuous energy levels. Considering the case of the helium atom, where H' = e² 47E0712 no one has been able to evaluate the second-order correctness of the ground state (n = 1); Let's see how complex it is to calculate /H'mn Determine, with Z = 2: a) H(200) (100) ² b) H(300)(100) ²

Answer rating: 100% (QA)

Determine with Z 2 mn H200 100 2 With n1 and m2 H2010 e24 e28 e28 H2... View the full answer