Poisson Brackets
In Hamiltonian mechanics, consider a symplectic manifold M with a smooth Hamiltonian over it (for field theories, M would be infinite-dimensional).
Suppose we have some constraints
for n smooth functions
These will only be defined chartwise in general. Suppose that everywhere on the constrained set, the n derivatives of the n functions are all linearly independent and also that the Poisson brackets
- { fi, fj }
and
- { fi, H }
all vanish on the constrained subspace. This means we can write
for some smooth functions
- cijk
(there is a theorem showing this) and
for some smooth functions
- vij.
This can be done globally, using a partition of unity. Then, we say we have an irreducible first-class constraint (irreducible here is in a different sense from that used in representation theory).
Read more about this topic: First Class Constraint