Invariant Lagrangian or action

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    Invariant Lagrangian
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Discussion Overview

The discussion centers around the relationship between the invariance of the Lagrangian and the invariance of the action in the context of theoretical physics. Participants explore whether these concepts are equivalent and how they relate to different types of symmetries, particularly in field theories and the Standard Model.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that the invariance of the Lagrangian and the invariance of the action are not equivalent, noting that the Lagrangian can vary by a total derivative while leaving the action invariant.
  • Others argue that there is a distinction between a Lagrangian being invariant and it "transforming as," questioning the implications for underlying symmetries.
  • A participant mentions that for space-time transformations, the Lagrangian experiences a variation, while for the symmetries of the Standard Model, the Lagrangian remains invariant.
  • There is a suggestion to generalize the transformation properties of the Lagrangian to all external and internal symmetry transformations, particularly in the context of writing a thesis.
  • One participant references a specific condition for action invariance under spacetime symmetries, indicating that the action is invariant if a certain relationship involving the Lagrangian holds.

Areas of Agreement / Disagreement

Participants express differing views on the equivalence of Lagrangian invariance and action invariance, indicating that multiple competing views remain. The discussion does not reach a consensus on the implications of these concepts for symmetry in physics.

Contextual Notes

Participants express uncertainty regarding terminology and clarity in their discussions, particularly in relation to their academic work. There are indications of confusion stemming from the complexity of the topic.

Physiana
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"invariant" Lagrangian or action

Hello everyone,

I tried to describe my question but it seems getting too complicated and confusing to write down my thoughts in detail, so I am trying to start with the following question...

Are invariance of the Lagrangian under a transformation and invariance of the action equivalent to each other? or even the same?

Physiana

P.S.: I know it sounds stupid. But I was wondering if there is a difference in physics by demanding the Lagrangian being invariant or just transforming in a certain way. As for example for time dilatation [itex] t \rightarrow t' = \lambda t[/itex] the Lagrangian transforms as[itex] L \rightarrow L'= \frac{L}{\lambda}[/itex] which is not "exactly" invariant, although "a" is constant and probably does not really matter. So I wondered if there are more transformations that "change" the Lagrangian but leave the action invariant.
 
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They're not quite the same, the Lagrangian can vary by a total derivative which would leave the action invariant, since it can be integrated over the boundary by stokes' theorem, and it is normally assumed fields all go to zero at infinity.

The variation of the lagrangian [itex]\delta L[/itex] contributes one term to the Noether current of that symmetry.
 


So there is a difference between a Lagrangian being invariant and it "transforming as".

Does it say anything about the underlying symmetry, if a Lagrangian is invariant or "only" transforming as? (e.g. space-time, external, internal)

In field theories one generally speaks of invariance, right?

It is just, I have read too much these days and I ram starting to get really confused and loose what I believed to know/ understand.
 


To specify; For space time transformations I get a [itex]\delta L[/itex], while for all the symmetries of the Standard model (QCD, GWS and chiral) the Lagrangian remains invariant. Space time symmetries are external symmetries, while QCD, GWS and chiral symmetries are internal symmetries. So can I generalize the above "observed" transformation properties of the Lagrangian to all external resp. internal symmetry transformations?

I just ask because I am writing my thesis and I am not exactly sure which words to use and it is important to me to be as clear as possible in my use of words.
 


Physiana said:
To specify; For space time transformations I get a [itex]\delta L[/itex], while for all the symmetries of the Standard model (QCD, GWS and chiral) the Lagrangian remains invariant. Space time symmetries are external symmetries, while QCD, GWS and chiral symmetries are internal symmetries. So can I generalize the above "observed" transformation properties of the Lagrangian to all external resp. internal symmetry transformations?

I just ask because I am writing my thesis and I am not exactly sure which words to use and it is important to me to be as clear as possible in my use of words.

Under a spacetime symmetry the action is invariant if and only if

[tex]\delta \mathcal{L} + \partial_{\mu}(\delta x^{\mu} \mathcal{L}) = 0[/tex]

For internal symmetries; [itex]\delta x^{\mu} = 0[/itex], therefore, the action is invariant if and only if the Lagrangian is invariant. See post #12 in

www.physicsforums.com/showthread.php?t=172461

regards

sam
 
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:) Thank you.
 

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