Lagrangian Mechanics, Continuous Particle Paths and QFT

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Discussion Overview

The discussion revolves around the relationship between Lagrangian mechanics, continuous particle paths, and Quantum Field Theory (QFT). Participants explore the implications of these concepts in the context of quantum mechanics, particularly focusing on the nature of particle movement and the application of Lagrangian mechanics in quantum contexts.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants reference a previous discussion asserting that questions about a particle's movement between measurements in Quantum Mechanics do not constitute scientific inquiries, as noted by PeroK.
  • One participant questions how this view reconciles with Lagrangian mechanics, which is perceived to imply continuous particle movement in QFT.
  • Another participant clarifies that Lagrangian mechanics is a generalized approach not strictly tied to continuous paths, emphasizing that in field theory, the Lagrangian applies to fields rather than particles.
  • A participant suggests that fields in the field-theoretic application of Lagrangian mechanics are quantized rather than continuous, prompting further discussion.
  • It is noted that while quantum fields are generally continuous, the energy levels in systems like the quantum harmonic oscillator are quantized, indicating a distinction between the continuity of wave functions and the quantization of energy.
  • Some participants argue that QFT does not posit continuous particle movement, challenging the assumption that it does.
  • One participant introduces Huygens' principle to explain wave function propagation in quantum theory, asserting that quantum theory does not provide information about particle paths but rather about measurement expectations.

Areas of Agreement / Disagreement

Participants express differing views on the continuity of particle movement in quantum mechanics and QFT. There is no consensus on whether Lagrangian mechanics implies continuous paths in quantum contexts, and multiple competing interpretations are presented.

Contextual Notes

Participants highlight the complexity of quantum fields and the distinction between classical and quantum interpretations of Lagrangian mechanics. The discussion reveals uncertainties regarding the definitions and implications of continuity and quantization in quantum theories.

Islam Hassan
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How are Lagrangian mechanics --which posit a continuous particle path-- integrated within the framework of QFT if continuity of a particle's movement is not established/addressed in QM.
In the following thread:

https://www.physicsforums.com/threads/particle-movement-in-quantum-mechanics.1054807/

the discussion established/confirmed that the matter of a particle’s continuity of movement in Quantum Mechanics QM is not a scientific question in QM, refer to PeroK post # 6:

“Orthodox QM goes further than that. Asking what a particle does between measurements makes no sense as a scientific question. For example, only measurements of position make sense. Asking where a particle was when you didn't measure its position is not a scientific question.”

How is the foregoing reconciled with the application of Lagrangian mechanics in Quantum Field Theory which ––if I understand correctly–– posits continuous particle movement?


IH
 
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Islam Hassan said:
How is the foregoing reconciled with the application of Lagrangian mechanics in Quantum Field Theory which ––if I understand correctly–– posits continuous particle movement?
Lagrangian mechanics is a generalised approach, which is not tied to continuous classical paths. In any case, in field theory, the Lagrangian applies to the fields themselves. Here's an example where the Lagrangian applies to the Schroedinger field (effectively wave functions):

https://en.wikipedia.org/wiki/Schrödinger_field
 
Maybe I misunderstood regarding the requirement for continuous paths in Lagrangian mechanics...will check.

In the field-theoretic application of Lagrangian mechanics, I suppose the fields are taken as quantised and not continuous then?


IH
 
Islam Hassan said:
In the field-theoretic application of Lagrangian mechanics, I suppose the fields are taken as quantised and not continuous then?
A field in physics is, by assumption, generally continuous - including quantum fields. A quantum field is a complicated object, as described here:

https://www.damtp.cam.ac.uk/user/tong/whatisqft.html

Let's take a simple example of the quantum harmonic oscillator. It's the energy that is quantized. A measurement of energy on a quantum harmonic oscillator must obtain an integer number of the lowest energy. The system itself still has a continuous (and infinitely differentiable) wave function.
 
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Islam Hassan said:
Lagrangian mechanics --which posit a continuous particle path
Only in the classical version, not in the quantum version. In the quantum version, the paths in the path integral formulation are not "particle paths"; they are one way of computing probability amplitudes.
 
Islam Hassan said:
Quantum Field Theory which ––if I understand correctly–– posits continuous particle movement?
QFT does not posit continuous particle movement. I have no idea why do you think it does.
 
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Islam Hassan said:
How is the foregoing reconciled with the application of Lagrangian mechanics in Quantum Field Theory which ––if I understand correctly–– posits continuous particle movement?

IH
In quantum (field) theory you basically apply Huygens' principle,

https://en.wikipedia.org/wiki/Huygens–Fresnel_principle

I.e. the propagation of the wave function can be derived from treating every point on a wave front as a new wave front. Every configuration is weighed with a certain amount with a phase factor, and this phase factor is determined by the action.

But quantum (field) theory doesn't tell you anything about paths. It tells you what you can expect if you perform a measurement (unless you adhere to other interpretations). So "continuous particle movement" in ordinary quantum mechanics is as well-defined as the colour of the wind.
 

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