Help with a formula in Weinberg

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    Formula Weinberg
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Discussion Overview

The discussion revolves around a specific formula in Weinberg's derivation of the matter part of the Lagrangian for electroweak theory, particularly focusing on equation (21.3.20) in volume II. Participants express confusion regarding the correctness of the formula and its implications, exploring the derivation and potential errors in signs and terms.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant expresses confusion about Weinberg's notation and derivation, suggesting a possible error in the original formula.
  • Another participant proposes an alternative formulation that includes additional terms and different signs, indicating a discrepancy with Weinberg's version.
  • Some participants question the clarity of Weinberg's text, suggesting it assumes prior knowledge that may not be accessible to all readers.
  • A later reply challenges the correctness of Weinberg's formula, asserting that it contains mistakes related to signs and missing terms.
  • There are humorous remarks about the difficulty of learning electroweak theory from Weinberg, despite his contributions to the field.
  • One participant seeks clarification on whether the original poster has resolved their confusion or agrees with the proposed corrections.

Areas of Agreement / Disagreement

Participants do not reach a consensus; there are multiple competing views regarding the correctness of Weinberg's formula and the proposed corrections. Some believe there are errors in the original text, while others express uncertainty about the resolution of these issues.

Contextual Notes

Participants highlight potential limitations in Weinberg's derivation, including unclear definitions and assumptions that may not be explicitly stated. The discussion reflects varying levels of familiarity with the material, which may influence interpretations of the formulas.

Jim Kata
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Alright, I'm trying to follow Weinberg's derivation of the matter part of the Lagrangian for electroweak theory, and I am all confused. This is equation (21.3.20) in volume II.

He writes:

[tex] iL_e = - \left( {\begin{array}{*{20}c}<br /> {\bar \upsilon _e } \\<br /> {\bar e} \\<br /> <br /> \end{array} } \right)\sum\limits_\alpha {\gamma _\mu A^\mu _\alpha } t_\alpha \left( {\begin{array}{*{20}c}<br /> {\upsilon _e } \\<br /> e \\<br /> <br /> \end{array} } \right)[/tex]

but I think he meant to write

[tex] iL_e = - \left( {\begin{array}{*{20}c}<br /> {\bar \upsilon _e } \\<br /> {\bar e} \\<br /> <br /> \end{array} } \right)\sum\limits_\alpha {\gamma _\mu \left( {A^\mu _\alpha t_{\alpha L} + B^\mu y} \right)} \left( {\begin{array}{*{20}c}<br /> {\upsilon _e } \\<br /> e \\<br /> <br /> \end{array} } \right)[/tex]

He defines his left handed and right handed parts different than Itzykson and Zuber

Namely [tex]e_L = \frac{1}{2}\left( {1 + \gamma _5 } \right)[/tex] and [tex] e_R = \frac{1}<br /> {2}\left( {1 - \gamma _5 } \right)[/tex]

but whatever

From this I was able to derive next line

Namely

[tex] \begin{gathered}<br /> - \left( {\begin{array}{*{20}c}<br /> {\bar \upsilon _e } \\<br /> {\bar e} \\<br /> <br /> \end{array} } \right)[\frac{1}<br /> {{\sqrt 2 }}\gamma _\mu W^\mu \left( {t_{1L} - it_{2L} } \right) + \frac{1}<br /> {{\sqrt 2 }}\gamma _\mu W^{*\mu } \left( {t_{1L} + it_{2L} } \right) \hfill \\<br /> + \gamma _\mu Z^\mu \left( {t_{3L} \cos \theta _W + y\sin \theta _W } \right) + \gamma _\mu A^\mu \left( { - t_{3L} \sin \theta _W + y\cos \theta _W } \right)]\left( {\begin{array}{*{20}c}<br /> {\upsilon _e } \\<br /> e \\<br /> <br /> \end{array} } \right) \hfill \\ <br /> \end{gathered} [/tex]

but when I tried to go to the final line of his derivation I got an opposite sign and some different stuff, namely I got

[tex] \begin{gathered}<br /> - \frac{g}<br /> {{\sqrt 2 }}\left( {\bar e\gamma _\mu W^\mu \left( {\frac{{1 + \gamma _5 }}<br /> {2}} \right)\upsilon _e } \right) - \frac{g}<br /> {{\sqrt 2 }}\left( {\bar \upsilon _e \gamma _\mu W^{*\mu } \left( {\frac{{1 + \gamma _5 }}<br /> {2}} \right)e} \right) \hfill \\<br /> + \frac{1}<br /> {2}\sqrt {g^2 + g'^2 } \bar \upsilon _e \gamma _\mu Z^\mu \left( {\frac{{1 + \gamma _5 }}<br /> {2}} \right)\upsilon _e - \frac{1}<br /> {2}\frac{{\left( {g^2 - g'^2 } \right)}}<br /> {{\sqrt {g^2 + g'^2 } }}\bar e\gamma _\mu Z^\mu \left( {\frac{{1 + \gamma _5 }}<br /> {2}} \right)e \hfill \\<br /> - g'\sin \theta _W \bar e\gamma _\mu Z^\mu \left( {\frac{{1 - \gamma _5 }}<br /> {2}} \right)e - \left( {\begin{array}{*{20}c}<br /> {\bar \upsilon _e } \\<br /> {\bar e} \\<br /> <br /> \end{array} } \right)\gamma _\mu A^\mu \left( { - t_{3L} \sin \theta _W + y\cos \theta _W } \right)\left( {\begin{array}{*{20}c}<br /> {\upsilon _e } \\<br /> e \\<br /> <br /> \end{array} } \right) \hfill \\ <br /> \end{gathered} [/tex]

The first four terms I got are similar to his, but with a different sign, and I understand he uses a Gell Mann Nishijima equation to get last part, but how do you get

[tex] - g'\bar e\gamma _\mu Z^\mu \left( {\frac{{1 - \gamma _5 }}<br /> {2}} \right)e + e\left( {\bar e\gamma _\mu A^\mu e} \right)[/tex]

from
[tex] - \left( {\begin{array}{*{20}c}<br /> {\bar \upsilon _e } \\<br /> {\bar e} \\<br /> <br /> \end{array} } \right)[\gamma _\mu Z^\mu \left( {\frac{{1 - \gamma _5 }}<br /> {2}} \right)\sin \theta _W + \gamma _\mu \left( { - t_{3L} \sin \theta _W + y\cos \theta _W } \right)\left( {\begin{array}{*{20}c}<br /> {\upsilon _e } \\<br /> e \\<br /> <br /> \end{array} } \right)[/tex]

even with

[tex] q = - \sin \theta _W t_3 + \cos \theta _W y[/tex]
 
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Anybody? Help!
 
trying to learn EW theory from Weinberg?... not a good choice! :smile:
sorry don't have a copy of Weinberg at hand
 
Last edited:
Plain and simple, I think his formula is wrong. He got his signs backwards and he is missing a
[tex]\sin \theta _W[/tex] term in

[tex]- g'\bar e\gamma _\mu Z^\mu \left( {\frac{{1 - \gamma _5 }}<br /> {2}} \right)e[/tex]

It should read:

[tex]- g'\sin \theta_W \bar e\gamma _\mu Z^\mu \left( {\frac{{1 - \gamma _5 }}<br /> {2}} \right)e[/tex]
 
mjsd said:
trying to learn EW theory from Weinberg?... not a good choice! :smile:
The funny thing is that Weinberg is the guy who discovered EW theory. Moreover, he received the Nobel prize for it. :smile:
 
Demystifier said:
The funny thing is that Weinberg is the guy who discovered EW theory. Moreover, he received the Nobel prize for it. :smile:

And the most amusing part is that that book assumes that you know "the entire thing" before you start reading... I guess that's what make him the Nobel laureate. you need to be ahead of your time :smile:
 
mjsd said:
And the most amusing part is that that book assumes that you know "the entire thing" before you start reading... I guess that's what make him the Nobel laureate. you need to be ahead of your time :smile:
I have a general rule: If you want to learn the basics of something, never ask the best experts for that to explain it to you!
 
Jim Kata said:
Anybody? Help!

Jim, have you resolved the issue to your satisfaction? Do you agree with him now or are you now convinced there is a mistake? I am asking because I was considering double checking this.
 
kdv said:
Jim, have you resolved the issue to your satisfaction? Do you agree with him now or are you now convinced there is a mistake? I am asking because I was considering double checking this.

I think there is a mistake, take a look
 

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