almost symplectic structure, metaplectic structure, metalinear structure
geometric quantization, higher geometric quantization
geometric quantization higher geometric quantization
geometry of physics: Lagrangians and Action functionals + Geometric Quantization
prequantum circle n-bundle = extended Lagrangian
prequantum 1-bundle = prequantum circle bundle, regularcontact manifold,prequantum line bundle = lift of symplectic form to differential cohomology
The archetypical example of a mechanical system is a particle propagating on a manifold $\Sigma$. The phase space of this particular system happens to be canonically identified with the cotangent bundle $X \coloneqq T^* \Sigma$ of $\Sigma$. Here the covector $(x,p)$ in $X$ over a point $x \in \Sigma$ is physically interpretd as describing a state of the system where the particle is at position $x \in \Sigma$ and has momentum (essentially: speed) as given by $p$.
Therefore locally for coordinate patch $\phi : \mathbb{R}^{2n} \simeq \mathbb{R}^n \times \mathbb{R}^n \to T^* \Sigma$ the $2n$-canonical coordinates of the Cartesian space $\mathbb{R}^n$ are naturally thought of as decomposed into $n$ “canonical coordinates” on the first $n$ factors and a set of “canonical momenta”, being the canonical coordinates on the second $\mathbb{R}^n$-factor.
Notice that “canonical” here refers (at best) to the canonical coordinates of the Cartesian space $\mathbb{R}^n$ once $\phi$ has been chosen. The choice of $\phi$ however is arbitrary. Hence, despite the (standard) term, there is nothing much canonical about these “canonical coordinates” and “canonical momenta”.
In general, the phase space of a physical system is a symplectic manifold which need not be a cotangent bundle as for the particle sigma-model.
But locally over a coordinate patch every symplectic manifold looks like $\mathbb{R}^{2n} \simeq \mathbb{R}^n \times \mathbb{R}^n$ such that under this identification the symplectic form reads $\sum_{i = 1}^n d q_i \wedge d p^i$, for $\{q_i\}$ the canonical coordinates on one $\mathbb{R}^n$ and $\{p^i\}$ for the other.
Therefore generally, in the context of mechanics, with such a local identification one calls $p^i$ the canonical momentum of the coordinate (or sometimes “canonical coordinate”) $q_i$.
Globally the notion of canonical momenta may not exist at all. The notion that does exist globally is that of a polarization of a symplectic manifold. See there for more details.
Discussion of how there is a flat connection on the bundle of spaces of quantum states over the space of choices of polarizations of a symplectic vector space and how this reproduces the traditional relation between canonical coordinates and canonical momenta by Fourier transformation? is in (Kirwin-Wu 04).
Last revised on September 13, 2013 at 19:29:18. See the history of this page for a list of all contributions to it.