In differential geometry, a **caustic** is the envelope of rays either reflected or refracted by a manifold. It is related to the concept of caustics in geometric optics. The ray's source may be a point (called the radiant) or parallel rays from a point at infinity, in which case a direction vector of the rays must be specified.

More generally, especially as applied to symplectic geometry and singularity theory, a caustic is the critical value set of a Lagrangian mapping (*π* ○ *i*) : *L* ↪ *M* ↠ *B*; where *i* : *L* ↪ *M* is a Lagrangian immersion of a Lagrangian submanifold *L* into a symplectic manifold *M*, and *π* : *M* ↠ *B* is a Lagrangian fibration of the symplectic manifold *M*. The caustic is a subset of the Lagrangian fibration's base space *B*.^{[1]}

## Catacaustic

A **catacaustic** is the reflective case.

With a radiant, it is the evolute of the orthotomic of the radiant.

The planar, parallel-source-rays case: suppose the direction vector is and the mirror curve is parametrised as . The normal vector at a point is ; the reflection of the direction vector is (normal needs special normalization)

Having components of found reflected vector treat it as a tangent

Using the simplest envelope form

which may be unaesthetic, but gives a linear system in and so it is elementary to obtain a parametrisation of the catacaustic. Cramer's rule would serve.

### Example

Let the direction vector be (0,1) and the mirror be Then

and has solution ; *i.e.*, light entering a parabolic mirror parallel to its axis is reflected through the focus.

## References

**^**Arnold, V. I.; Varchenko, A. N.; Gusein-Zade, S. M. (1985).*The Classification of Critical Points, Caustics and Wave Fronts: Singularities of Differentiable Maps, Vol 1*. Birkhäuser. ISBN 0-8176-3187-9.