(2) n = 2 ~ l = 0 ~ m = 0
Ψ200 (r,θ,φ) = R20 (r) Y0º (θ,φ)
R20(r) = 2(z/2a)³/² (1-[zr/2a]) exp (-zr/2a)
Y0º (θ,φ) = [1/4π]¹/²
Ψ200 (r,θ,φ) = 2[1/4π]¹/²(z/2a)³/² (1-[zr/2a]) exp (-zr/2a)
(3) n = 2 ~ l = 1 ~ m = -1
-1
Ψ21-1 (r,θ,φ) = R21 (r) Y1 (θ,φ)
R21(r) = (1/3)¹/² (z/2a)³/² [zr/a] exp (-zr/2a)
-1
Y1 (θ,φ) = [3/8π]¹/² (sinθ) exp(-iφ)
Ψ21-1 = [1/8π]¹/²(z/2a)³/²[zr/a] (sinθ) exp[-(zr/2a)-iφ]
(4) n = 2 ~ l = 1 ~ m = 0
Ψ210 (r,θ,φ) = R21 (r) Y1º (θ,φ)
Y1º (θ,φ) = [3/4π]¹/² (cosθ)
Ψ210 = [1/4π]¹/² (z/2a)³/² [zr/a] (cosθ) exp (-zr/2a)
(5) n = 2 ~ l = 1 ~ m = 1
Ψ211 (r,θ,φ) = R21 (r) Y1¹ (θ,φ)
Y1¹ (θ,φ) = - [3/8π]¹/² (sinθ) exp(iφ)
Ψ211 (r,θ,φ) =- [1/8π]¹/²(z/2a)³/²[zr/a] (sinθ) exp[-(zr/2a)+iφ]
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