Math 2.0

Special functions Definition

Painlevé transcendents

Builds on Painlevé propertyOrdinary differential equation

Definition

Let α,β,γ,δ\alpha, \beta, \gamma, \delta be complex constants, and let yy be a function of a complex variable tt. The six Painlevé equations are the ordinary differential equations:

  1. PI\mathrm{P_I}: y′′=6y2+ty'' = 6y^2 + t;
  2. PII\mathrm{P_{II}}: y′′=2y3+ty+αy'' = 2y^3 + ty + \alpha;
  3. PIII\mathrm{P_{III}}: y′′=(y′)2y−y′t+αy2+βt+γy3+δyy'' = \frac{(y')^2}{y} - \frac{y'}{t} + \frac{\alpha y^2 + \beta}{t} + \gamma y^3 + \frac{\delta}{y};
  4. PIV\mathrm{P_{IV}}: y′′=(y′)22y+32y3+4ty2+2(t2−α)y+βyy'' = \frac{(y')^2}{2y} + \frac32 y^3 + 4ty^2 + 2(t^2 - \alpha) y + \frac{\beta}{y};
  5. PV\mathrm{P_V}: y′′=(12y+1y−1)(y′)2−y′t+(y−1)2t2(αy+βy)+γyt+δy(y+1)y−1y'' = \left( \frac{1}{2y} + \frac{1}{y - 1} \right) (y')^2 - \frac{y'}{t} + \frac{(y - 1)^2}{t^2} \left( \alpha y + \frac{\beta}{y} \right) + \frac{\gamma y}{t} + \frac{\delta y (y + 1)}{y - 1};
  6. PVI\mathrm{P_{VI}}: y′′=12(1y+1y−1+1y−t)(y′)2−(1t+1t−1+1y−t)y′+y(y−1)(y−t)t2(t−1)2(α+βty2+γ(t−1)(y−1)2+δt(t−1)(y−t)2)y'' = \frac12 \left( \frac1y + \frac{1}{y - 1} + \frac{1}{y - t} \right) (y')^2 - \left( \frac1t + \frac{1}{t - 1} + \frac{1}{y - t} \right) y' + \frac{y (y - 1)(y - t)}{t^2 (t - 1)^2} \left( \alpha + \frac{\beta t}{y^2} + \frac{\gamma (t - 1)}{(y - 1)^2} + \frac{\delta t (t - 1)}{(y - t)^2} \right).

A Painlevé transcendent is a solution of one of these six equations.

Remarks

Each equation has the Painlevé property: the only movable singularities of its solutions are poles. Example: for α=1\alpha = 1, the function y=−1ty = -\frac1t solves PII\mathrm{P_{II}}. Check: y′′=−2t3y'' = -\frac{2}{t^3}, and 2y3+ty+1=−2t3−1+1=−2t32y^3 + ty + 1 = -\frac{2}{t^3} - 1 + 1 = -\frac{2}{t^3}. This solution is rational, so for special parameters some Painlevé transcendents are classical functions; the generic solution is not. Non-example: a solution of y′′=6y2y'' = 6y^2 is not a Painlevé transcendent, since this equation is not one of the six; its nonconstant solutions are translates of the Weierstrass function ℘(t;0,g3)\wp(t; 0, g_3). Each of PI\mathrm{P_I} to PV\mathrm{P_V} is a limit of PVI\mathrm{P_{VI}} under a suitable coalescence of singular points and parameters.

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  1. Ordinary differential equation concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Painlev%C3%A9_transcendents
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MSC33E17, 34M55
DefinesPainlevé transcendents
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