I Uncovering the Mystery Behind SM Lagrangian Sums

  • I
  • Thread starter Thread starter jouvelot
  • Start date Start date
  • Tags Tags
    Lagrangian Sum
AI Thread Summary
The discussion centers on the perplexity surrounding the summation of different components in the Standard Model (SM) Lagrangian without additional coefficients. Participants highlight that while each component has unique coefficients, the overall Lagrangian is formed by simple addition, which raises questions about the underlying mathematical principles. The conversation touches on both quantum and classical systems, noting that the same additive approach applies in both contexts. It is suggested that the coefficients may be represented by coupling constants within the Lagrangian terms, reflecting the additive nature of energy. Ultimately, the simplicity of this summation process is viewed as remarkable and deserving of further exploration.
jouvelot
Messages
51
Reaction score
2
Hello all,

I'm a bit baffled by the fact that the various quite different components of the SM Lagrangian (or other systems, btw) are simply summed up, without even one ponderation coefficient, in the total Lagrangian. I know one reason it is like that is that... it works in practice, but I keep thinking there must be a more profound and/or mathematical reason for this (a rapid Google search on this didn't provide anything really conclusive).

Thanks for your help.

Bye,

Pierre
 
Physics news on Phys.org
I don't quiet understand the question... can you give an example of a Lagrangian you are talking about?
For example I've seen L = - \frac{1}{4} F_{\mu\nu}F^{\mu\nu} ...
 
But each component of the sum has different coefficients. Therefore it has an individuality, even if one can show that the so-called interaction terms are derived from the so-called free fields.
 
Well, for instance, the EM and Higgs Lagrangian subexpressions have their own parameters, of course. But, when one combines them, one just adds them, plus the possible interaction term, without introducing any additional coefficients, something like $$\alpha L_{EM}+\beta L_{Higgs}.$$ I find this sort of miraculous.
 
jouvelot said:
I find this sort of miraculous.

Why? Specifically, why do you find this miraculous in the quantum case but not the classical case?
 
Sure :) As I alluded to in my first post, I have the same issue with classical systems. Just adding stuff, without ponderation or additional parameters, and then minimizing it in the action "just" works in all cases. I find it amazing... Maybe I'm too impressionable :)
 
Maybe this should be moved to General or Classical then, because the exact same thing happens classically. If I have two free particles, the Lagrangian is T1 + T2. If I add an interaction, it's T1 + T2 - U_A. If I add another interaction, it's T1 + T2 - U_A - U_B. Another and it's T1 + T2 - U_A - U_B - U_C.
 
Thanks for the suggestion. I'll put my question there then.

Bye,

Pierre
 
jouvelot said:
Thanks for the suggestion. I'll put my question there then.

Bye,

Pierre
I moved it for you, because I didn't want to lose the already existing part of the discussion.
Please do not create a second one. Thanks.
 
  • #10
Thanks.

Pierre
 
  • #11
Just thinking a little bit more about this, and answering my own question :)

it seems to me that the coefficients I was looking for are, in some sense, embedded in the coupling constants that occur in the various terms of the lagrangian. And then, using non-weighted addition between these terms comes from the additive nature of the notion of energy
 

Similar threads

Back
Top