Finding the generator of a transformation

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The discussion focuses on finding the generator of a transformation for the Hamiltonian ##\mathscr{H} = \frac12 p^2 + \frac12 x^2##, which is invariant under infinitesimal rotations in phase space. The transformation is defined as ##\bar{p} = p - \epsilon x## and ##\bar{x} = p \epsilon + x##, which is confirmed to be canonical through the Poisson bracket calculations. The differential equations for the generator ##g## lead to the conclusion that ##g(x,p) = \frac12 x^2 + \frac12 p^2 + C##, indicating that the generating function resembles the Hamiltonian. The discussion concludes that the generator's form aligns with the nature of phase space trajectories for this system.
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Homework Statement


Consider ##\mathscr{H} = \frac12 p^2 + \frac12 x^2, ## which is invariant under infinitesimal rotations in phase space ( the ##x-p## plane). Find the generator of this transformation (after verifying that it is canonical).

Homework Equations

The Attempt at a Solution



So the transformation to ##\bar{x}, \ \bar{p}## is
$$\bar{p} = p - \epsilon x, \ \bar{x} = p \epsilon + x$$.
This is canonical as clearly ##\{ \bar{x}, \bar{x} \} = \{ \bar{p}, \bar{p} \} = 0## and $$\{\bar{x},\bar{p} \} = 1 \times 1 +\epsilon \epsilon = 1$$
if we work only to first order in ##\epsilon##.

The differential equations for the generator ##g## are
$$ \frac{\partial g}{\partial x} = x, \ \frac{\partial g}{\partial p} = p.$$

Thus ##g(x,p) = \frac12 x^2 + \frac12 p^2 + C.##

This seems to make sense, but I'm not sure if this is correct.
 
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I think it's correct. So, the generating function is essentially the Hamiltonian in this case (no need to keep ##C##). That should make sense if you think about the phase space trajectories for this system.
 
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