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relation to Fuchsian equation

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1: 29.2 Differential Equations
§29.2 Differential Equations
§29.2(i) Lamé’s Equation
§29.2(ii) Other Forms
For the Weierstrass function see §23.2(ii). …
2: 30.2 Differential Equations
§30.2 Differential Equations
§30.2(i) Spheroidal Differential Equation
With ζ = γ z Equation (30.2.1) changes toIf μ 2 = 1 4 , Equation (30.2.2) reduces to the Mathieu equation; see (28.2.1). …
3: 31.2 Differential Equations
§31.2 Differential Equations
§31.2(i) Heun’s Equation
§31.2(v) Heun’s Equation Automorphisms
Composite Transformations
4: 15.10 Hypergeometric Differential Equation
§15.10 Hypergeometric Differential Equation
15.10.1 z ( 1 z ) d 2 w d z 2 + ( c ( a + b + 1 ) z ) d w d z a b w = 0 .
This is the hypergeometric differential equation. … The three pairs of fundamental solutions given by (15.10.2), (15.10.4), and (15.10.6) can be transformed into 18 other solutions by means of (15.8.1), leading to a total of 24 solutions known as Kummer’s solutions. …
5: 32.2 Differential Equations
§32.2 Differential Equations
The six Painlevé equations P I P VI  are as follows: … The six equations are sometimes referred to as the Painlevé transcendents, but in this chapter this term will be used only for their solutions. … An equation is said to have the Painlevé property if all its solutions are free from movable branch points; the solutions may have movable poles or movable isolated essential singularities (§1.10(iii)), however. … The fifty equations can be reduced to linear equations, solved in terms of elliptic functions (Chapters 22 and 23), or reduced to one of P I P VI . …
6: 28.2 Definitions and Basic Properties
A solution with the pseudoperiodic property (28.2.14) is called a Floquet solution with respect to ν . … leads to a Floquet solution. …
§28.2(vi) Eigenfunctions
Table 28.2.2 gives the notation for the eigenfunctions corresponding to the eigenvalues in Table 28.2.1. …
7: 28.20 Definitions and Basic Properties
§28.20(i) Modified Mathieu’s Equation
28.20.1 w ′′ ( a 2 q cosh ( 2 z ) ) w = 0 ,
§28.20(ii) Solutions Ce ν , Se ν , Me ν , Fe n , Ge n
Then from §2.7(ii) it is seen that equation (28.20.2) has independent and unique solutions that are asymptotic to ζ 1 / 2 e ± 2 i h ζ as ζ in the respective sectors | ph ( i ζ ) | 3 2 π δ , δ being an arbitrary small positive constant. …
§28.20(iv) Radial Mathieu Functions Mc n ( j ) , Ms n ( j )
8: 31.14 General Fuchsian Equation
§31.14 General Fuchsian Equation
§31.14(i) Definitions
The general second-order Fuchsian equation with N + 1 regular singularities at z = a j , j = 1 , 2 , , N , and at , is given by …
Normal Form
An algorithm given in Kovacic (1986) determines if a given (not necessarily Fuchsian) second-order homogeneous linear differential equation with rational coefficients has solutions expressible in finite terms (Liouvillean solutions). …
9: 6.11 Relations to Other Functions
§6.11 Relations to Other Functions
Incomplete Gamma Function
Confluent Hypergeometric Function
6.11.2 E 1 ( z ) = e z U ( 1 , 1 , z ) ,
10: 16.7 Relations to Other Functions
§16.7 Relations to Other Functions