Is the Hamiltonian Equation of Motion Gauge Dependent?

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The discussion centers on the implications of gauge dependence in the Hamiltonian formulation derived from a specific Lagrangian. The Euler-Lagrange equations yield the Lorentz force, which is gauge invariant, yet the resulting Hamiltonian appears to introduce gauge dependence in the equations of motion. Participants clarify that while the Hamiltonian itself may be gauge-dependent, the physical solutions, particularly the equations of motion, remain gauge invariant when expressed in terms of electric and magnetic fields. The distinction between canonical momentum and kinetic momentum is emphasized, with the latter being the physically relevant quantity. Ultimately, the gauge dependence of the Hamiltonian does not undermine the physical observables derived from the equations of motion.
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If we consider the following Lagrangian:
L = m * (dot x)^2 / 2 - e A dot x - e phi
with A the vectorpotential and phithe scalar potential, then
the Euler-Lagrange equations, reduce to the known formula
of Lorentz-force:
m ddot x = e dot x X B + e E
know, this equation is invariant under gauge transformations:
A->A + nabla F
phi -> phi - parcd phi / parcd t
Know this is great, but if we construct the Hamiltonian with the
usual Legendre transform we will get
H = (p+eA)^2 / 2m + e phi
My problem with this is, if a write the (Hamiltonian) equation of
motion now, it seems gauge dependent:
dot x = (p + eA)/m

Isn't this a problem? What's the resolution?
 
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A Hamiltonian is always gauge-dependent. Remember the arbitrary constant C that can be added to the scalar potential? It is of the same nature.
 
The gauge dependence of the Hamiltonian is not my problem. My problem is that, from these equations of motion, the velocity, which is something that should be mesurable, also seems to be gauge dependent...
 
No, the equation solutions are gauge invariant. Moreover, the equations themselves, expressed via EM filed tensions, are gauge invariant.
 
I don't see why the solutions should be gauge independent when A(and not its curl or something) is explicitly in the equations of motion...
 
If you speak of velocity equation, it contains also p which is gauge-dependent. Write the equation for acceleration d2x/dt2. You will see that this equation will contain the electric and magnetic fields rather than potentials.
 
You are right. And if I understand it correctly p is no longer a physical quantity, only p+eA is.
 
Yes, there are two momenta: a canonically conjugated p (a formal mathematical construction) and a kinetic P = p + eA (physical quantity).
 
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