Origin of the value of the vacuum v ~ 246 GeV

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Discussion Overview

The discussion revolves around the origin of the vacuum expectation value (vev) in the electroweak theory, specifically the value of v ~ 246 GeV, and its connection to the Fermi Constant G_F. Participants explore the relationship between the Higgs potential parameters and the electroweak symmetry breaking mechanism, as well as the methods for measuring G_F.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants note that the Higgs vev can be expressed in terms of the parameters mu and lambda, as well as in terms of the W mass and the coupling constant g.
  • There is a question about the connection between the Higgs vacuum and G_F, specifically whether this connection can be established a priori or requires specific calculations involving processes like muon decay.
  • One participant suggests that the decay rate in muon decay is proportional to 1/v^2, which can be used to relate the vev to G_F.
  • Another participant mentions that one-loop corrections to muon decay are generally considered for a more accurate determination of the vev in relation to G_F.
  • There is a discussion about the best methods for measuring G_F, with muon decay being highlighted as a precise experimental process, while also noting that other parameters could be used as input.
  • Some participants clarify their terminology regarding the treatment of the W mass in calculations, indicating a shared understanding of the nuances involved.

Areas of Agreement / Disagreement

Participants express varying views on the connection between the Higgs vev and G_F, with some suggesting that specific calculations are necessary while others imply a more general understanding. The discussion remains unresolved regarding the best measurement methods for G_F and the implications of different approaches.

Contextual Notes

Participants acknowledge the complexity of the relationship between the Higgs potential parameters and the electroweak interactions, as well as the need for careful consideration of corrections in theoretical calculations.

Sleuth
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Hi guys,
I have a very very simple and naive question, which I hope I shouldn't be ashamed to ask, but I would like to clarify an issue in my mind.

We hear everywhere that the value of the ew vacuum is v ~ 246GeV, fixed by the Fermi Constant G_F, v = (\sqrt(2)*G_F)^(-1/2).

Now this is also the vacuum of the Higgs potential in the standard model, which is determined by the two parameters, say mu^2 and \lambda, in the Higgs potential, schematically

V(\phi) = mu^2 phi^2 + \lambda \phi^4.

The mechanism does not have anything to do with G_F at this point, it exists completely independently of the rest of the Lagrangian which can contain any other interactions.

Therefore the question is, at which step of the implementation of the mechanism in the EW SU(2)xU(1) and how exactly do we get to say that this v is actually connected to G_F, and in particular it is exactly equal to (\sqrt(2)*G_F)^(-1/2)? Does one necessarily need to compute, for example, the process

\mu -> \nu + \bar{\nu} + e^+

in the SM in terms of the parameter v, then take the limit M_W->\infty, get the corresponding "effective" 4-point interaction and then compare it to what Fermi had called G_F, or can one somehow make this statement"a priori" from more general considerations?

Also, once one agrees on this, what is the most precise method to measure G_F?

Thanks guys and sorry if this sounds a bit silly...
Sleuth
 
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The Higgs vev is mu/sqrt(lambda), but it's also 2M_W/g. You calculate the W mass and get vg/2.
 
Sleuth said:
Hi guys,
I have a very very simple and naive question, which I hope I shouldn't be ashamed to ask, but I would like to clarify an issue in my mind.

We hear everywhere that the value of the ew vacuum is v ~ 246GeV, fixed by the Fermi Constant G_F, v = (\sqrt(2)*G_F)^(-1/2).

Now this is also the vacuum of the Higgs potential in the standard model, which is determined by the two parameters, say mu^2 and \lambda, in the Higgs potential, schematically

V(\phi) = mu^2 phi^2 + \lambda \phi^4.

The mechanism does not have anything to do with G_F at this point, it exists completely independently of the rest of the Lagrangian which can contain any other interactions.

Therefore the question is, at which step of the implementation of the mechanism in the EW SU(2)xU(1) and how exactly do we get to say that this v is actually connected to G_F, and in particular it is exactly equal to (\sqrt(2)*G_F)^(-1/2)? Does one necessarily need to compute, for example, the process

\mu -> \nu + \bar{\nu} + e^+

in the SM in terms of the parameter v, then take the limit M_W->\infty, get the corresponding "effective" 4-point interaction and then compare it to what Fermi had called G_F, or can one somehow make this statement"a priori" from more general considerations?

Also, once one agrees on this, what is the most precise method to measure G_F?

Thanks guys and sorry if this sounds a bit silly...
Sleuth
See the last part (equations 36-40) of the post
https://www.physicsforums.com/threads/why-su-2-times-u-1-for-the-sm.846099/#post-5320206
 
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One doesn't really send mw-> infinity, but rather ignore the electron mass and also the momentum transfer in muon decay. Then you get a decay rate proportional to 1/vev^2 from muon decay (as people point out related to the W boson coupling to a lepton su2 doublet). Then this decay rate is used to eliminate the vev in terms of gf as measured from muon decay.

This is the general procedure. To be more accurate, people actually generally consider the one loop corrections to muon decay, and eliminate the vev this way.
 
Thanks for the answers! Sending m_W to infinity would be the sensible thing to do for me, if one wants to recover the Fermi 4-point like interaction, but I guess this is only matter of language.

Does anyone know exactly what is the best measurement of G_F (and therefore of v)? I guess one could measures the muon decay rate and the muon, or is there anything better?
 
Sleuth said:
Sending m_W to infinity would be the sensible thing to do for me, if one wants to recover the Fermi 4-point like interaction,

If you do that, you recover it with strength zero.
 
Yes well, I meant keeping the first non-zero order in 1/m_W of course...
Thanks again
 
;) I knew what you meant, but just thought it was sloppy terminology.

For sure, just drop the momentum dependence of the interaction.

Muon decay is the most precisely measured experimental process for extracting and vev. People have also been computing corrections to this process (weak, qed, effective field theory corrections etc.) so it's also theoretically well motivated to use it.

Note that this is just a choice of input parameters. One could just quite as well use m_w , electric charge, m_z. It's just that m_w is a couple of orders of magnitude less precisely known
 
Thanks RGevo. Yes I was being a bit sloppy, but I thought that was clear enough.

I wanted to make sure I knew what was going on regarding the value of v. The discussion helped clarifying my mind :)
 

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