Review schrodinger equations not dependent on 3D time in ball coordinates v² + V(f) v(F) = E p(F) 2m With = (r, 0,4) and E is the energy system. Assume the potential is only radial function V (f) = V(r). 'To solve the Schrodinger equation above apply the method p(r,0, q) = R(r)P(0)Q(g) variable separation problem : Show that the solution functions azimuthal Q(p) adalah Q(4) = e±imp With is the separation constant
Review schrodinger equations not dependent on 3D time in ball coordinates v² + V(f) v(F) = E p(F) 2m With = (r, 0,4) and E is the energy system. Assume the potential is only radial function V (f) = V(r). 'To solve the Schrodinger equation above apply the method p(r,0, q) = R(r)P(0)Q(g) variable separation problem : Show that the solution functions azimuthal Q(p) adalah Q(4) = e±imp With is the separation constant
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Transcribed Image Text:Review schrodinger equations not dependent on 3D time in ball coordinates
(
h?
-v² +V(f) )µ(F) = E Þ(F)
2m
With = (r, 0,p) and E is the energy system. Assume the potential is only radial function
V (f) = V(r).
'To solve the Schrodinger equation above apply the method
p(r, 0, q) = R(r)P(0)Q(w)
variable separation
problem : Show that the solution functions azimuthal Q(p) adalah Q(4) = e±imp
With m
is the separation constant
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