Table 7F.1 The spherical harmonics Ym (0,0) 1/2 4 (유) 1/2 3 1 cose 1/2 3 ±1 sinde*i 1/2 (3 cos'0-1) 16T 1/2 15 ±1 cose sinde*i tip 1/2 15 +2 32n 1/2 7 (5 cos'e-3cose) 3 16T 1/2 21 ±1 (5 cos'e-1)sin Oe** 64T 1/2 105 ±2 sin'e coseei0 32n 1/2 35 13 sin'de* 64T 2. Table 8A.1 Hydrogenic radial wavefunctions R(r) 3/2 (). 1 e P2 a 3/2 2 1 Z. 81/2 (2-p)e-p/2 a 3/2 2 1 PI2 242a 1 3/2 2432 a -) (6-6p+p²)e¯/2 3 1. 3/2 1 486 (4-p)pe-p12 台。 3 1. 3/2 24302 a p = (2Z/na)r with a = 4ne,h*/µe². For an infinitely heavy nucleus (or one that may be assumed to be), µ = m, and a = a, the Bohr radius. en

Table 7F.1 The spherical harmonics Ym (0,0) 1/2 4 (유) 1/2 3 1 cose 1/2 3 ±1 sindei 1/2 (3 cos'0-1) 16T 1/2 15 ±1 cose sindei tip 1/2 15 +2 32n 1/2 7 (5 cos'e-3cose) 3 16T 1/2 21 ±1 (5 cos'e-1)sin Oe** 64T 1/2 105 ±2 sin'e coseei0 32n 1/2 35 13 sin'de* 64T 2. Table 8A.1 Hydrogenic radial wavefunctions R(r) 3/2 (). 1 e P2 a 3/2 2 1 Z. 81/2 (2-p)e-p/2 a 3/2 2 1 PI2 242a 1 3/2 2432 a -) (6-6p+p²)e¯/2 3 1. 3/2 1 486 (4-p)pe-p12 台。 3 1. 3/2 24302 a p = (2Z/na)r with a = 4ne,h*/µe². For an infinitely heavy nucleus (or one that may be assumed to be), µ = m, and a = a, the Bohr radius. en

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