General Generator of Lorentz Transformation in Hamiltonian Formalism

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SUMMARY

The discussion focuses on the general generator of Lorentz transformations in the Hamiltonian formalism, specifically exploring the canonical transformations realized through Poisson brackets of phase-space variables. The proposed generator for Lorentz transformations is expressed as $$\mathbf{K}=H\mathbf{r}-t\mathbf{p}$$, which parallels the Galilean boost generator $$\overrightarrow{G}=m\overrightarrow{r}$$ with mass replaced by energy. The conclusion emphasizes that while the traditional $$t=0$$ generator is commonly used, it obscures the physical interpretation of the boost generator, particularly in the context of energy as the source of gravitational fields in relativistic physics.

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  • Understanding of Hamiltonian mechanics
  • Familiarity with Poisson brackets
  • Knowledge of Lorentz transformations
  • Concept of energy-mass equivalence
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  • Research Hamiltonian mechanics and its applications in physics
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The discussion is beneficial for theoretical physicists, students of advanced mechanics, and researchers interested in the foundations of relativistic physics and the implications of energy in gravitational fields.

andresB
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In the Hamiltonian formalism, the space-time transformation are realized via canonical transformation, and the transformations are generated by Poisson brackets of certain functions of phase-space variables.
In Newtonian mechanics, Galilean boosts are generated by the sometimes called dynamic mass moment $$\overrightarrow{G}=m\overrightarrow{r}-t\overrightarrow{p}.$$
Now, in virtually every source I consult, the general generator of the Galilean boosts is not considered. Instead, people just use the ##t=0## generator
$$\overrightarrow{G}=m\overrightarrow{r}$$
The same happen for Lorentz transformations, people just use the ##t=0## generator
$$\overrightarrow{K}=H\overrightarrow{r}$$
where ##H## is the energy.
So, the question is, what is the most general form of ##\overrightarrow{K}##?
 
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How about
t\mathbf{p}-\frac{E}{c^2}\mathbf{r}
which comes from ##(M^{01},M^{02},M^{03})## of angular momentum 4-tensor
M^{\mu\nu}=x^\mu p^\nu-x^\nu p^\mu ?
 
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anuttarasammyak said:
How about
t\mathbf{p}-\frac{E}{c^2}\mathbf{r}
which comes from ##(M^{01},M^{02},M^{03})## of angular momentum 4-tensor
M^{\mu\nu}=x^\mu p^\nu-x^\nu p^\mu ?

So it would have almost the same form of the Galilei boost generator with only ##m## replaced by ##H##? I suppose it's a good Ansatz, I'll have to check the bracket relations of the Poincare group to see if they remain true.
 
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Yes! The conclusion leads to the correct interpretation of the famous "energy-mass equivalence":

In Newtonian physics from invariance under Galilei boosts follows that the center of mass of a closed system moves with constant velocity. The measure for "inertia" is mass.

In relativistic physics invariance under Lorentz boosts implies that the center of energy of a closed system moves with constant velocity and thus the measure of inertia is energy.

Using the equivalence principle this implies that the source of a gravitational field must be energy, not mass, in relativistic physics.
 
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So, yes, ##\mathbf{K}=H\mathbf{r}-t\mathbf{p}## has the same bracket relation than just ##\mathbf{K}=H\mathbf{r}##. Thank you guys for the answer. I do wonder why the ##t=0## generator is preferred for the presentation of the Galilean and the Poincare algebra, it seems to hide some physical interpretation of the boost generator, and it is not much of a simplification in the math.
 
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