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12 Parabolic Cylinder FunctionsProperties

§12.4 Power-Series Expansions

12.4.1 U⁡(a,z)=U⁡(a,0)⁢u1⁡(a,z)+U′⁡(a,0)⁢u2⁡(a,z),
12.4.2 V⁡(a,z)=V⁡(a,0)⁢u1⁡(a,z)+V′⁡(a,0)⁢u2⁡(a,z),

where the initial values are given by (12.2.6)–(12.2.9), and u1⁡(a,z) and u2⁡(a,z) are the even and odd solutions of (12.2.2) given by

12.4.3 u1⁡(a,z)=e−14⁢z2⁢(1+(a+12)⁢z22!+(a+12)⁢(a+52)⁢z44!+⋯),
12.4.4 u2⁡(a,z)=e−14⁢z2⁢(z+(a+32)⁢z33!+(a+32)⁢(a+72)⁢z55!+⋯).

Equivalently,

12.4.5 u1⁡(a,z)=e14⁢z2⁢(1+(a−12)⁢z22!+(a−12)⁢(a−52)⁢z44!+⋯),
12.4.6 u2⁡(a,z)=e14⁢z2⁢(z+(a−32)⁢z33!+(a−32)⁢(a−72)⁢z55!+⋯).

These series converge for all values of z.