About the meaning "on-shell" vs "off-shell" in Hamiltonian mechanics

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Discussion Overview

The discussion revolves around the meanings of "on-shell" and "off-shell" in the context of Hamiltonian and Lagrangian mechanics, as well as their implications in quantum mechanics. Participants explore the definitions and applications of these concepts within theoretical frameworks.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that "on-shell" and "off-shell" are involved in the derivation of Hamiltonian mechanics, specifically relating to four-momentum in special relativity.
  • Another participant suggests that a trajectory in phase space is considered "on-shell" if it satisfies the equation ##\frac{dq_i}{dt} = \frac{\partial H}{\partial p_i}##, indicating a relationship between coordinates and momenta as defined by the Hamiltonian.
  • It is proposed that "off-shell" refers to arbitrary paths through phase space where coordinates and momenta are treated as independent variables, not necessarily adhering to the Hamiltonian constraints.
  • A participant mentions that "on-shell" trajectories are constrained by Hamilton's equations, while "off-shell" paths are relevant in quantum mechanics, particularly in path integral evaluations.
  • Discussion includes the notion that off-shell analysis can involve "virtual" paths and is applicable in scenarios like quantum tunneling and W boson transitions, where conservation laws permit certain transitions that would otherwise be forbidden.

Areas of Agreement / Disagreement

Participants express varying interpretations of the concepts of "on-shell" and "off-shell," with some agreement on their definitions in Hamiltonian mechanics, but differing views on their implications in quantum mechanics. The discussion remains unresolved regarding the broader implications and applications of these concepts.

Contextual Notes

Some statements rely on specific definitions of "on-shell" and "off-shell" that may vary across contexts, and there are unresolved aspects regarding the relationship between these concepts in classical versus quantum frameworks.

cianfa72
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TL;DR
About the meaning "on-shell" vs "off-shell" in the context of Hamiltonian/Lagrangian mechanics
In the derivation of Hamiltonian mechanics, the concept of "on-shell" vs "off-shell" is involved in the calculation.

I searched it for like off-shelf, however it seems it makes sense in the context of four-momentum in special relativity.

What is the meaning of that concept in the context of Hamiltonian/Lagrangian mechanics ? Thanks.
 
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cianfa72 said:
TL;DR Summary: About the meaning "on-shell" vs "off-shell" in the context of Hamiltonian/Lagrangian mechanics

In the derivation of Hamiltonian mechanics, the concept of "on-shell" vs "off-shell" is involved in the calculation.

I searched it for like off-shelf, however it seems it makes sense in the context of four-momentum in special relativity.

What is the meaning of that concept in the context of Hamiltonian/Lagrangian mechanics ? Thanks.
I'm not an expert on Hamiltonian Mechanics but as I understand it, we have a phase space with coordinates ##(q_i,p_i)##. A trajectory is a path through phase space parametrized by time.

Such a path is considered on shell if ##\frac{dq_i}{dt} = \frac{\partial H}{\partial p_i}##.

With a typical Hamiltonian of ##H = m/2\sum p_i^2 + V(q_i)## this just reduces to ##\frac{dq_i}{dt} = p_i/m = \dot{q_i}##.

TLDR, On shell is restricted to paths where q and p are related via the Hamiltonian and off-shell refers to an arbitrary path through phase space where q and p aren't necessarily related and are treated as independent variables.
 
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Ah ok, so basically the "time evolution" of an "on-shell" trajectory through phase space is "constrained" from Hamilton's equations.
 
cianfa72 said:
Ah ok, so basically the "time evolution" of an "on-shell" trajectory through phase space is "constrained" from Hamilton's equations.
Mostly on-shell and off-shell are used to distinguish between different kinds of path integral evaluations in quantum mechanics. In quantum mechanics, paths that would be forbidden by conservation laws are still possible so long as the end point where an observation if made complies with the relevant conservation laws.

In particular, off-shell analysis considers "virtual" paths from one state to another, sometimes involving "virtual particles." One of the most common cases where an off-shell analysis is needed is in quantum tunneling situations, and in W boson transitions where the system lacks the mass-energy to create a real, on-shell W boson in an intermediate step.
 

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