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DLMF: §31.10 Integral Equations and Representations ‣ Properties ‣ Chapter 31 Heun Functions
§31.10 Integral Equations and Representations
Contents
§31.10(i) Type I
§31.10(ii) Type II
§31.10(i) Type I
If w ( z ) is a solution of Heun’s equation, then another solution W ( z )
(possibly a multiple of w ( z ) ) can be represented as
31.10.1
W ( z ) = ∫ C 𝒦 ( z , t ) w ( t ) ρ ( t ) d t
for a suitable contour C . The weight function is given by
31.10.2
ρ ( t ) = t γ − 1 ( t − 1 ) δ − 1 ( t − a ) ϵ − 1 ,
and the kernel 𝒦 ( z , t ) is a solution of the partial differential
equation
where 𝒟 z is Heun’s operator in the variable z :
31.10.4
𝒟 z = z ( z − 1 ) ( z − a ) ( ∂ 2 / ∂ z 2 ) + ( γ ( z − 1 ) ( z − a ) + δ z ( z − a ) + ϵ z ( z − 1 ) ) ( ∂ / ∂ z ) + α β z .
The contour C must be such that
31.10.5
p ( t ) ( ∂ 𝒦 ∂ t w ( t ) − 𝒦 d w ( t ) d t ) | C = 0 ,
where
31.10.6
p ( t ) = t γ ( t − 1 ) δ ( t − a ) ϵ .
Kernel Functions
Set
31.10.7
cos θ
= ( z t a ) 1 / 2 ,
sin θ cos ϕ
= i ( ( z − a ) ( t − a ) a ( 1 − a ) ) 1 / 2 ,
sin θ sin ϕ
= ( ( z − 1 ) ( t − 1 ) 1 − a ) 1 / 2 .
The kernel 𝒦 must satisfy
31.10.8
sin 2 θ ( ∂ 2 𝒦 ∂ θ 2 + ( ( 1 − 2 γ ) tan θ + 2 ( δ + ϵ − 1 2 ) cot θ ) ∂ 𝒦 ∂ θ − 4 α β 𝒦 ) + ∂ 2 𝒦 ∂ ϕ 2 + ( ( 1 − 2 δ ) cot ϕ − ( 1 − 2 ϵ ) tan ϕ ) ∂ 𝒦 ∂ ϕ = 0 .
The solutions of (31.10.8 ) are given in terms of the Riemann
P -symbol (see §15.11(i) ) as
31.10.9
𝒦 ( θ , ϕ ) = P { 0 1 ∞ 0 1 2 − δ − σ α cos 2 θ 1 − γ 1 2 − ϵ + σ β } P { 0 1 ∞ 0 0 − 1 2 + δ + σ cos 2 ϕ 1 − ϵ 1 − δ − 1 2 + ϵ − σ } ,
where σ is a separation constant . For integral equations
satisfied by the Heun polynomial 𝐻𝑝 n , m ( z ) we have
σ = 1 2 − δ − j , j = 0 , 1 , … , n .
For suitable choices of the branches of the P -symbols in
(31.10.9 ) and the contour C , we can obtain both integral
equations satisfied by Heun functions, as well as the integral representations of
a distinct solution of Heun’s equation in terms of a Heun function (polynomial,
path-multiplicative solution).
Example 1
Let
31.10.10
𝒦 ( z , t ) = ( z t − a ) 1 2 − δ − σ F 1 2 ( 1 2 − δ − σ + α , 1 2 − δ − σ + β γ ; z t a ) × F 1 2 ( − 1 2 + δ + σ , − 1 2 + ϵ − σ δ ; a ( z − 1 ) ( t − 1 ) ( a − 1 ) ( z t − a ) ) ,
where ℜ γ > 0 , ℜ δ > 0 , and C be the
Pochhammer double-loop contour about 0 and 1 (as in §31.9(i) ). Then
the integral equation (31.10.1 ) is satisfied by w ( z ) = w m ( z ) and
W ( z ) = κ m w m ( z ) , where
w m ( z ) = ( 0 , 1 ) 𝐻𝑓 m ( a , q m ; α , β , γ , δ ; z )
and κ m is the corresponding eigenvalue.
Example 2
Fuchs–Frobenius solutions W m ( z ) = κ ~ m z − α H ℓ ( 1 / a , q m ; α , α − γ + 1 , α − β + 1 , δ ; 1 / z ) are
represented in terms of Heun functions
w m ( z ) = ( 0 , 1 ) 𝐻𝑓 m ( a , q m ; α , β , γ , δ ; z )
by (31.10.1 ) with W ( z ) = W m ( z ) , w ( z ) = w m ( z ) , and with kernel
chosen from
31.10.11
𝒦 ( z , t ) = ( z t − a ) 1 2 − δ − σ ( z t / a ) − 1 2 + δ + σ − α × F 1 2 ( 1 2 − δ − σ + α , 3 2 − δ − σ + α − γ α − β + 1 ; a z t ) × P { 0 1 ∞ 0 0 − 1 2 + δ + σ ( z − a ) ( t − a ) ( 1 − a ) ( z t − a ) 1 − ϵ 1 − δ − 1 2 + ϵ − σ } .
Here κ ~ m is a normalization constant and C is the contour of
Example 1.
§31.10(ii) Type II
If w ( z ) is a solution of Heun’s equation, then another solution W ( z )
(possibly a multiple of w ( z ) ) can be represented as
31.10.12
W ( z ) = ∫ C 1 ∫ C 2 𝒦 ( z ; s , t ) w ( s ) w ( t ) ρ ( s , t ) d s d t
for suitable contours C 1 , C 2 . The weight function is
31.10.13
ρ ( s , t ) = ( s − t ) ( s t ) γ − 1 ( ( 1 − s ) ( 1 − t ) ) δ − 1 ( ( 1 − ( s / a ) ) ( 1 − ( t / a ) ) ) ϵ − 1 ,
and the kernel 𝒦 ( z ; s , t ) is a solution of the partial differential
equation
31.10.14
( ( t − z ) 𝒟 s + ( z − s ) 𝒟 t + ( s − t ) 𝒟 z ) 𝒦 = 0 ,
where 𝒟 z is given by (31.10.4 ). The contours C 1 ,
C 2 must be chosen so that
31.10.15
p ( t ) ( ∂ 𝒦 ∂ t w ( t ) − 𝒦 d w ( t ) d t ) | C 1
= 0 ,
and
31.10.16
p ( s ) ( ∂ 𝒦 ∂ s w ( s ) − 𝒦 d w ( s ) d s ) | C 2
= 0 ,
where
p ( t ) is given by (31.10.6 ).
Kernel Functions
Set
31.10.17
u
= ( s t z ) 1 / 2 a ,
v
= ( ( s − 1 ) ( t − 1 ) ( z − 1 ) 1 − a ) 1 / 2 ,
w
= i ( ( s − a ) ( t − a ) ( z − a ) a ( 1 − a ) ) 1 / 2 .
The kernel 𝒦 must satisfy
31.10.18
∂ 2 𝒦 ∂ u 2 + ∂ 2 𝒦 ∂ v 2 + ∂ 2 𝒦 ∂ w 2 + 2 γ − 1 u ∂ 𝒦 ∂ u + 2 δ − 1 v ∂ 𝒦 ∂ v + 2 ϵ − 1 w ∂ 𝒦 ∂ w = 0 .
This equation can be solved in terms of cylinder functions 𝒞 ν ( z )
(§10.2(ii) ):
31.10.19
𝒦 ( u , v , w ) = u 1 − γ v 1 − δ w 1 − ϵ 𝒞 1 − γ ( u σ 1 ) 𝒞 1 − δ ( v σ 2 ) 𝒞 1 − ϵ ( i w σ 1 + σ 2 ) ,
where σ 1 and σ 2 are separation constants.
Transformation of Independent Variable
A further change of variables, to spherical coordinates,
31.10.20
u
= r cos θ ,
v
= r sin θ sin ϕ ,
w
= r sin θ cos ϕ ,
leads to the kernel equation
31.10.21
∂ 2 𝒦 ∂ r 2 + 2 ( γ + δ + ϵ ) − 1 r ∂ 𝒦 ∂ r + 1 r 2 ∂ 2 𝒦 ∂ θ 2 + ( 2 ( δ + ϵ ) − 1 ) cot θ − ( 2 γ − 1 ) tan θ r 2 ∂ 𝒦 ∂ θ + 1 r 2 sin 2 θ ∂ 2 𝒦 ∂ ϕ 2 + ( 2 δ − 1 ) cot ϕ − ( 2 ϵ − 1 ) tan ϕ r 2 sin 2 θ ∂ 𝒦 ∂ ϕ = 0 .
This equation can be solved in terms of hypergeometric functions
(§15.11(i) ):
31.10.22
𝒦 ( r , θ , ϕ ) = r m sin 2 p θ P { 0 1 ∞ 0 0 a cos 2 θ 1 2 ( 3 − γ ) c b } P { 0 1 ∞ 0 0 a ′ cos 2 ϕ 1 − ϵ 1 − δ b ′ } ,
with
31.10.23
m 2 + 2 ( α + β ) m − σ 1 = 0 ,
p 2 + ( α + β − γ − 1 2 ) p − 1 4 σ 2 = 0 ,
a + b
= 2 ( α + β + p ) − 1 ,
a b
= p 2 − p ( 1 − α − β ) − 1 4 σ 1 ,
c
= γ − 1 2 − 2 ( α + β + p ) ,
a ′ + b ′
= δ + ϵ − 1 ,
a ′ b ′
= − 1 4 σ 2 ,
and σ 1 and σ 2 are separation constants.
For integral equations for special confluent Heun functions (§31.12 )
see Kazakov and Slavyanov (1996 ) .