Lagrangian & Hamiltonian of Fields

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Discussion Overview

The discussion revolves around the necessity and sufficiency of specifying the Lagrangian and Hamiltonian for various fundamental forces and fields, including the Higgs field. Participants explore whether these formulations are adequate to describe all possible models in physics, particularly in the context of quantum mechanics and general relativity.

Discussion Character

  • Debate/contested
  • Exploratory
  • Technical explanation

Main Points Raised

  • Some participants assert that one does not need to specify both the Lagrangian and Hamiltonian, as one can be derived from the other through a Legendre transformation.
  • Others emphasize that the Lagrangian encodes the dynamics of a model and that specifying how fields transform under symmetry is crucial.
  • There is a question about whether the Lagrangian and Hamiltonian are sufficient to specify all possible models, with some suggesting that this depends on the definition of "all possible models."
  • Some participants express skepticism about the existence of theories that do not utilize Lagrangian or Hamiltonian formulations, questioning how dynamics could be described without them.
  • Concerns are raised about the potential for "wild theories" that may not conform to traditional Lagrangian or Hamiltonian frameworks, with some participants suggesting that these theories could be more than just "wild."
  • There is a suggestion that a more fundamental description could exist, from which the Hamiltonian and Lagrangian formalisms might emerge as limits.

Areas of Agreement / Disagreement

Participants do not reach consensus on whether the Lagrangian and Hamiltonian are sufficient to describe all models. There are competing views on the necessity of these formulations and the implications of theories that might not adhere to them.

Contextual Notes

Participants express uncertainty regarding the definitions of "possible models" and the implications of theories that may not be described by Lagrangian or Hamiltonian mechanics. The discussion reflects a range of assumptions and interpretations about the nature of dynamics in physics.

cube137
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For each of the four fundamental forces (or fields), must one always specify the Lagrangian and Hamiltonian? What else must one specify for other fields (like the Higgs Fields)?
 
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You cannot specify both. If you specify one the othr follows. Normally, we define a model from its Lagrangian.
 
The Lagrangian/Hamiltonian encodes the dynamics of your model. As Orodruin said, you don't need both since the one is a Legendre transformation of the other [ you can always change from the 1 to the other], something that is true in classical mechanics as well.

Now for your second question, I don't really understand what caused you this confusion:
For example you want to describe a QED model- your Lagrangian will contain both photons and fermions [charged]...you could as well emit the fermions but your model would be unrealistic and boring. So you don't have much to specify about the fields...
As far as I know, the only thing that you need to define your fields with, is to state how they transform under the model (symmetry model) in consideration.
 
ChrisVer said:
The Lagrangian/Hamiltonian encodes the dynamics of your model. As Orodruin said, you don't need both since the one is a Legendre transformation of the other [ you can always change from the 1 to the other], something that is true in classical mechanics as well.

Now for your second question, I don't really understand what caused you this confusion:
For example you want to describe a QED model- your Lagrangian will contain both photons and fermions [charged]...you could as well emit the fermions but your model would be unrealistic and boring. So you don't have much to specify about the fields...
As far as I know, the only thing that you need to define your fields with, is to state how they transform under the model (symmetry model) in consideration.

Is the Lagrangian/Hamiltonian enough to specify all possible models? For example. Is it possible for a model that needs more than the Lagrangian/Hamiltonian to specify it?
 
cube137 said:
Is the Lagrangian/Hamiltonian enough to specify all possible models?
That depends on what you mean by "all possible models". The Lagrangian certainly is enough for all models in Lagrangian mechanics by definition. Of course there may be some wild theories out there not described by Lagrangian mechanics and it would be presumptuous to assume that anything can ever specify "all" models. You need a qualifier for what you consider a "possible model".
 
Orodruin said:
That depends on what you mean by "all possible models". The Lagrangian certainly is enough for all models in Lagrangian mechanics by definition. Of course there may be some wild theories out there not described by Lagrangian mechanics and it would be presumptuous to assume that anything can ever specify "all" models. You need a qualifier for what you consider a "possible model".

For example.. quantum mechanics and general relativity being emergence from another theory that doesn't use Lagrangian or Hamiltonian.. does this statement even makes sense? I'm asking if a theory can exist that doesn't use Lagrangian/Hamiltonian that can unite QM and GR. Any example or papers?
 
To be honest I don't understand Orodruin's point, neither something being not described by a Lagrangian/Hamiltonian... It's like trying to deal with something without caring about the dynamics [the Hamiltonian for example contains information about the energies; kinetic and potential]. I understand the "wild theories", but I'd be confident enough to call those theories more than just "wild".
 
ChrisVer said:
To be honest I don't understand Orodruin's point, neither something being not described by a Lagrangian/Hamiltonian... It's like trying to deal with something without caring about the dynamics [the Hamiltonian for example contains information about the energies; kinetic and potential]. I understand the "wild theories", but I'd be confident enough to call those theories more than just "wild".

Obviously you need a hamiltonian/lagrangian to describe things in Hamilton/Lagrange formalism. Within those formalisms the hamiltonian/lagrangian is all there is by definition.

And yes, most other theories are going to be "wild" and clearly wrong. However, there will always be the possibility that there is some more fundamental type of description from which the Hamilton/Lagrange formalisms would be limits. In such a theory, there would clearly be a new notion of how dynamics appear.
 

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