# relation to Fuchsian equation

(0.003 seconds)

## 1—10 of 920 matching pages

##### 1: 29.2 Differential Equations
###### §29.2(ii) Other Forms
For the Weierstrass function $\wp$ see §23.2(ii). …
##### 2: 30.2 Differential Equations
###### §30.2(i) Spheroidal Differential Equation
With $\zeta=\gamma z$ Equation (30.2.1) changes toIf $\mu^{2}=\frac{1}{4}$, Equation (30.2.2) reduces to the Mathieu equation; see (28.2.1). …
##### 3: 31.2 Differential Equations
###### §31.2(i) Heun’s Equation
31.2.1 $\frac{{\mathrm{d}}^{2}w}{{\mathrm{d}z}^{2}}+\left(\frac{\gamma}{z}+\frac{% \delta}{z-1}+\frac{\epsilon}{z-a}\right)\frac{\mathrm{d}w}{\mathrm{d}z}+\frac{% \alpha\beta z-q}{z(z-1)(z-a)}w=0,$ $\alpha+\beta+1=\gamma+\delta+\epsilon$.
##### 4: 15.10 Hypergeometric Differential Equation
###### §15.10(i) Fundamental Solutions
15.10.1 $z(1-z)\frac{{\mathrm{d}}^{2}w}{{\mathrm{d}z}^{2}}+\left(c-(a+b+1)z\right)\frac% {\mathrm{d}w}{\mathrm{d}z}-abw=0.$
This is the hypergeometric differential equation. …
##### 5: 32.2 Differential Equations
###### §32.2 Differential Equations
The six Painlevé equations $\mbox{P}_{\mbox{\scriptsize I}}$$\mbox{P}_{\mbox{\scriptsize VI}}$ are as follows: … The six equations are sometimes referred to as the Painlevé transcendents, but in this chapter this term will be used only for their solutions. … An equation is said to have the Painlevé property if all its solutions are free from movable branch points; the solutions may have movable poles or movable isolated essential singularities (§1.10(iii)), however. … The fifty equations can be reduced to linear equations, solved in terms of elliptic functions (Chapters 22 and 23), or reduced to one of $\mbox{P}_{\mbox{\scriptsize I}}$$\mbox{P}_{\mbox{\scriptsize VI}}$. …
##### 6: 28.2 Definitions and Basic Properties
###### §28.2(i) Mathieu’s Equation
This is the characteristic equation of Mathieu’s equation (28.2.1). … leads to a Floquet solution. …
##### 7: 28.20 Definitions and Basic Properties
###### §28.20(ii) Solutions $\operatorname{Ce}_{\nu}$, $\operatorname{Se}_{\nu}$, $\operatorname{Me}_{\nu}$, $\operatorname{Fe}_{n}$, $\operatorname{Ge}_{n}$
Then from §2.7(ii) it is seen that equation (28.20.2) has independent and unique solutions that are asymptotic to $\zeta^{\ifrac{1}{2}}e^{\pm 2\mathrm{i}h\zeta}$ as $\zeta\to\infty$ in the respective sectors $|\operatorname{ph}\left(\mp\mathrm{i}\zeta\right)|\leq\tfrac{3}{2}\pi-\delta$, $\delta$ being an arbitrary small positive constant. …
##### 8: 31.14 General Fuchsian Equation
###### §31.14(i) Definitions
The general second-order Fuchsian equation with $N+1$ regular singularities at $z=a_{j}$, $j=1,2,\dots,N$, and at $\infty$, 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: 16.25 Methods of Computation
Methods for computing the functions of the present chapter include power series, asymptotic expansions, integral representations, differential equations, and recurrence relations. They are similar to those described for confluent hypergeometric functions, and hypergeometric functions in §§13.29 and 15.19. There is, however, an added feature in the numerical solution of differential equations and difference equations (recurrence relations). …Instead a boundary-value problem needs to be formulated and solved. …