12 Parabolic Cylinder FunctionsProperties

§12.8 Recurrence Relations and Derivatives

Contents
  1. §12.8(i) Recurrence Relations
  2. §12.8(ii) Derivatives

§12.8(i) Recurrence Relations

12.8.1 z⁢U⁡(a,z)−U⁡(a−1,z)+(a+12)⁢U⁡(a+1,z) =0,
12.8.2 U′⁡(a,z)+12⁢z⁢U⁡(a,z)+(a+12)⁢U⁡(a+1,z) =0,
12.8.3 U′⁡(a,z)−12⁢z⁢U⁡(a,z)+U⁡(a−1,z) =0,
12.8.4 2⁢U′⁡(a,z)+U⁡(a−1,z)+(a+12)⁢U⁡(a+1,z) =0.

(12.8.1)–(12.8.4) are also satisfied by U¯⁡(a,z).

12.8.5 z⁢V⁡(a,z)−V⁡(a+1,z)+(a−12)⁢V⁡(a−1,z) =0,
12.8.6 V′⁡(a,z)−12⁢z⁢V⁡(a,z)−(a−12)⁢V⁡(a−1,z) =0,
12.8.7 V′⁡(a,z)+12⁢z⁢V⁡(a,z)−V⁡(a+1,z) =0,
12.8.8 2⁢V′⁡(a,z)−V⁡(a+1,z)−(a−12)⁢V⁡(a−1,z) =0.

§12.8(ii) Derivatives

For m=0,1,2,…,

12.8.9 dmdzm⁡(e14⁢z2⁢U⁡(a,z))=(−1)m⁢(12+a)m⁢e14⁢z2⁢U⁡(a+m,z),
12.8.10 dmdzm⁡(e−14⁢z2⁢U⁡(a,z))=(−1)m⁢e−14⁢z2⁢U⁡(a−m,z),
12.8.11 dmdzm⁡(e14⁢z2⁢V⁡(a,z))=e14⁢z2⁢V⁡(a+m,z),
12.8.12 dmdzm⁡(e−14⁢z2⁢V⁡(a,z))=(−1)m⁢(12−a)m⁢e−14⁢z2⁢V⁡(a−m,z).