Jacobian in path integral equal to one?

geoduck
Messages
257
Reaction score
2
Consider:

\int d\phi e^{iS[\phi]}=\int d\phi' J e^{iS'[\phi']}

where J is the Jacobian. If the transformation of variables to phi' is a symmetry of the action [i.e., S'=S], then this becomes:

\int d\phi e^{iS[\phi]}=\int d\phi' J e^{iS[\phi']}

But doesn't this imply that the Jacobian has to equal one?

But surely that doesn't have to be true in general? If the action has a symmetry, and you perform the change of coordinates corresponding to the symmetry transformation, then does the Jacobian of that transformation have to equal one?
 
Last edited:
Physics news on Phys.org
I think you miss that, in general, \mathrm{d} \phi \neq \mathrm{d} \phi'.

For a simple example, consider S=\frac{1}{2}\phi^2. Obviously, this is invariant under the inversion \phi \rightarrow \phi'=-\phi, for which \mathrm{d}\phi'=-\mathrm{d}\phi and J=\frac{\partial \phi'}{\partial \phi}=-1.
 
Hypersphere said:
I think you miss that, in general, \mathrm{d} \phi \neq \mathrm{d} \phi'.

For a simple example, consider S=\frac{1}{2}\phi^2. Obviously, this is invariant under the inversion \phi \rightarrow \phi'=-\phi, for which \mathrm{d}\phi'=-\mathrm{d}\phi and J=\frac{\partial \phi'}{\partial \phi}=-1.

The Jacobian should take care of differences in measure, so what happens to

∫ e-x^2 dx from -∞ to ∞

under y=-x is:

∫ e-y^2 dx/dy dy from ∞ to -∞

which equals ∫ e-y^2 (-1) dy from ∞ to -∞

so it's the change of the order of the limits in the integration that allows the Jacobian to not have to be equal to 1.

Maybe a stronger statement is true: If the limits in an integration are unchanged by a transformation, then the Jacobian must equal one?
 
geoduck said:
so it's the change of the order of the limits in the integration that allows the Jacobian to not have to be equal to 1.

I guess that is the more common way of putting it, yeah.

Maybe a stronger statement is true: If the limits in an integration are unchanged by a transformation, then the Jacobian must equal one?

I don't have an explicit example, but couldn't we have a local transformation y=f(x) that doesn't change the endpoints (i.e. limits) and J=\frac{\partial f}{\partial x} \not\equiv 1?

I think your statement should hold for linear functions f(x) though.
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
Back
Top