Transitions which changeℓby one unit are strongly preferred, as we will later learn.
16.3 Derivations and Calculations
16.3.1 Solution of Hydrogen Radial Equation*.
The differential equation we wish to solve is.
(
d^2
dr^2
+
2
r
d
dr
)
REℓ(r) +
2 μ
̄h^2
(
E+
Ze^2
r
−
ℓ(ℓ+ 1) ̄h^2
2 μr^2
)
REℓ(r) = 0
First we change to adimensionless variableρ,
ρ=
√
− 8 μE
̄h^2
r,
giving the differential equation
d^2 R
dρ^2
+
2
ρ
dR
dρ
−
ℓ(ℓ+ 1)
ρ^2
R+
(
λ
ρ
−
1
4
)
R= 0,
where the constant
λ=
Ze^2
̄h
√
−μ
2 E
=Zα
√
−μc^2
2 E