Preview. Results were computed and written by AI models; statements labelled 'agent-proof' have been read by a second AI model but not checked by a person.

Worked examples

Six equations, each with the kind of answer it gets. A link opens the result on the page Solve; where the catalogue has no report for the exact text, the engine computes it, in the browser or on the server.

Kuramoto–Sivashinsky

u_t + u*u_x + u_xx + u_xxxx = 0

A published theorem gives the class of all meromorphic solutions of the travelling-wave equation (rational, simply periodic or elliptic, with one pole in a period), and the list within that class is complete: the constants and two simply periodic families.

Fisher at the speed 5/√6

w'' + 5/sqrt(6) w' + w - w^2 = 0

At this speed the travelling-wave equation has, besides the constants and a simply periodic family, a family of solutions with d = 2: an exponential times a Weierstrass function of an exponential.

A nonlinear Schrödinger equation

i q_t + q_xx + g |q|^2 q = 0

Typed as an evolution equation for a complex field: the envelope reduction q = w(z)·exp(iθ) leads to a real equation of second order with a cubic term, and all its meromorphic solutions are listed.

The φ⁶ equation

w'' = a w + b w^3 + c w^5

For c ≠ 0 the only meromorphic solutions are constants; the square u = w² satisfies an equation that has nonconstant meromorphic solutions, and the result lists them.

Swift–Hohenberg, stationary

w'''' + 2 w'' + (1 - r) w + w^3 = 0

Every meromorphic solution is rational, simply periodic or elliptic with at most two poles in a period; the engine in the browser lists those with one pole and reports those with two as not computed.

A forced Korteweg–de Vries wave

w''' = 12 w w' + 1

Every solution with a pole is a first Painlevé transcendent, so d = 3: the result describes these solutions through an earlier record and gives no closed form.