This is a special case of this question of mine, which, I think, might have drawn little attention because it was too general. In this question, I would like to consider a specific case.
Take a classical system given by the action S[x]=∫dt[α2¨x2+β2˙x2+γ2x2].
This action is Lagrangian, but it is not what we are usually dealing with in physics, because the Lagrangian contains second time derivatives.
The equations of motion are:
αx⃜
This can be solved as usual by employing Fourier transform:
x(t) = a_1 e^{i \omega_1 t} + a_1^{*} e^{-i \omega_1 t} + a_2 e^{i \omega_2 t} + a_2^{*} e^{-i \omega_2 t},
where \omega_1^2 and \omega_2^2 are the two roots of \alpha \omega^4 + \beta \omega^2 + \gamma, given by
\omega_{1,2}^2 = \frac{- \beta \pm \sqrt{\beta^2 - 4 \alpha \gamma}}{2 \alpha} .
Now by definition the phase space is the space of solutions of equations of motion. In this case it is parametrized by two complex co-ordinates a_{1,2}, meaning that it is 4-dimensional.
I would like to know if there's a natural way to associate the symplectic structure (Poisson bracket) on this phase space. I.e.,
\{a_1, a_1^{*}\} = ? \{a_1, a_2^{*}\} = ? \{a_2, a_1^{*}\} = ? \{a_2, a_2^{*}\} = ? \{a_1, a_2\} = ? \{a_1^{*}, a_2^{*}\} = ?
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