A Show Lagrangian is invariant under a Lorentz transformation without using generators

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considering directly coordinate transformations and how to consider boost-translation
This is probably a stupid question but, I want to show that a Lagrangian written in field theory is Lorentz invariant WITHOUT using the Lorentz transformation representation / generators. I know we know that a Lorentz scalar is automatically Lorentz invariant, but, I want to show this by considering the coordinate expressions directly.

I.e to plug in :

##t’=\gamma (t-\frac{vx}{c^2}),##

##x’=\gamma(x-vt) ##(1)

and expanding out the fields.

So I expand out ##L[\phi(x,t), \partial_{mu}\phi(x,t)] ->L'[\phi(x',t'), \partial_{mu}\phi(x',t')]##

(where I just wrote ##\phi(x,t),## rather than ##x^{\mu}## just because of the transformation written as (1)).

1 )And then I think, for everything to be consistent, it should then come out that for ##L ##to be Lorentz-invariant ##\phi## would have to satisfy the known transformation laws for field theory (Since, in contrast to a Galilean invariant Lagranigan, where one has to uniquely decipher the way a wavefunction needs to transform in order to get Galilean invariance for the Lagrangian), the way fields transform are already predetermined).

(So a Lorentz transformation is defined by: ##g'^{\mu \nu}=\Lambda^{\mu}_{\alpha}\Lambda^{\nu}_{\beta}g^{\alpha \beta}=g^{\mu \nu}##, and where a vector must satisfy: ##x'^{\mu}=\Lambda^{\mu}_{\alpha}x^{\alpha}##). So, I think, I would expect to find that for ##L## to be Lorentz invariant, this should give an expansion for ##\phi## in terms of ##\Lambda^{\mu}_{\alpha}## expanded out for a boost- it would agree with ##\phi## in terms of ##\Lambda^{\mu}_{\alpha}## expressed in terms of boost generators and expanded out

2) How would I show that Lorentz boost and translation do not commute for a Lagrangian in field theory when we have Lorentz scalars so everything is invariant w.r.t boost translations and boosts . I want to consider performing a boost then a translation and vice versa..
 
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I showed you how to do that in the non-relativistic case,

https://www.physicsforums.com/threa...slation-on-a-wave-function-or-fields.1066552/

As I pointed out there, it's important to understand how the transformations of the group (or infinitesimally, from the algebra) act on the wave function. So under a boost or translation, one has for a scalar field that ##\phi'(t',x') = \phi(t,x)##. So that's not going to give you information about the (non)commutativity of the algebra. That's why I explained in post #3 how these transformations act on the wavefunction. The same goes for the relativistic operators on the scalar field ##\phi(t,x)##.

Also, you should transform the derivative in the Lagrangian. That transforms as a covector.
 
If you don't respond to comments in your own topics, then it will be a hard time helping you. Good luck.
 
haushofer said:
If you don't respond to comments in your own topics, then it will be a hard time helping you. Good luck.
i went back to the old thread and replied there 2 days ago which has not been replied to
 
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