nLab
de Donder-Weyl formalism

under construction

Contents

Idea

The formalism of de Donder-Weyl is a formulation of variational calculus related to multisymplectic geometry.

For L a local Lagrangian of fields {ϕ i} on a space Σ, and their first derivatives μϕ i, the Euler-Lagrange equations

μδLδ( μϕ i)=δLδϕ i\partial_\mu \frac{\delta L }{\delta (\partial_\mu \phi^i)} = \frac{\delta L}{ \delta \phi^i}

are equivalently rewritten, under the generalized Legendre transform (if it exists)

H:=π i μ μϕ iLH := \pi^\mu_i \partial_\mu \phi^i - L

(with π i μ the ”μ-th momentum of the i-th field” ) as the first-order system of “covariant” Hamilton equations?

δHδπ i μ= μϕ i,δHδϕ i= μπ i μ.\frac{\delta H}{\delta \pi_i^\mu} = \partial_\mu \phi^i \,, \;\;\;\; \frac{\delta H}{ \delta \phi^i} = - \partial_\mu \pi^\mu_i \,.

This H is also called the de Donder-Weyl Hamiltonian.

In terms of the multisymplectic form

Ω:=dπ i μdϕ i(ι μvol Σ)+dHvol Σ\Omega := d \pi^\mu_i \wedge d \phi^i \wedge (\iota_{\partial_\mu} vol_\Sigma) + d H \wedge vol_\Sigma

the critical field configurations are precisely those whose top-degree multi-tangent spaces annihilate Ω.

(…)

References

Reviews include

See also

  • I.V. Kanatchikov, DeDonder-Weyl theory and a hypercomplex extension of quantum mechanics to field theory , (arXiv:hep-th/9810165)

For more see the references at multisymplectic geometry.

Revised on March 8, 2013 01:18:57 by Urs Schreiber (131.174.40.92)