Poisson bracket
Let M be a symplectic manifold with symplectic form Ω. The Poisson bracket is a bilinear operation on the set of differentiable functions on M. In terms of local Darboux coordinates p1,…,pn,q1,…,qn, the Poisson bracket of two functions is defined as follows:
[f,g]=n∑i=1∂f∂qi∂g∂pi-∂f∂pi∂g∂qi |
It can be shown that the value of [f,g] does not depend on the choice of Darboux coordinates. Therefore, the Poisson bracket is a well-defined operation on the symplectic manifold. Also, some authors use a different sign convention — what they call [f,g] is what would be referred to as -[f,g] here.
The Poisson bracket can be defined without reference to a special coordinate system as follows:
[f,g]=Ω-1(df,dg)=2n∑i=1Ωij∂f∂xi∂g∂xj |
Here Ω-1 is the inverse of the symplectic form, and its components in an arbitrary coordinate system are denoted Ωij.
The Poisson bracket sastisfies several important algebraic identities. It is antisymmetric:
[f,g]=-[g,f] |
It is a derivation:
[fg,h]=f[g,h]+g[f,h] |
It satisfies Jacobi’s identitity:
[f,[g,h]]+[g,[h,f]]+[h,[f,g]]=0 |
The Hamilton equations can be expressed elegantly in terms of the Poisson bracket. If X is a smooth function on M, we can describe the time-evolution of X by the equation
dXdt=[X,H] |
If X is a smooth function on ℝ×M, we can describe the time-evolution of X by the more general equation
dXdt=∂X∂t-[X,H] |
Title | Poisson bracket |
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Canonical name | PoissonBracket |
Date of creation | 2013-03-22 14:46:04 |
Last modified on | 2013-03-22 14:46:04 |
Owner | rspuzio (6075) |
Last modified by | rspuzio (6075) |
Numerical id | 11 |
Author | rspuzio (6075) |
Entry type | Definition |
Classification | msc 53D05 |
Related topic | Quantization |
Related topic | CanonicalQuantization |