Rewriting neutral gauge bosons (EW) for vacuum with Y=-1

In summary, the conversation discusses the Higgs mechanism for the electroweak sector of the Standard Model and examines the changes in mass and mass eigenvectors of the Z and photon particles when the vacuum hypercharge is chosen to be -1. The resulting eigenvalues and eigenvectors are calculated and it is found that the choice of -1 for the vacuum hypercharge does not give a massless photon and a massive Z-boson as expected in the Standard Model. This may suggest that there is a deeper reason for choosing a vacuum hypercharge of +1 in the Standard Model.
  • #1
Valeriia Lukashenko
8
1

Homework Statement


So, my textbook proposes a to check what will change in mass and mass eigenvectors of Z and photon in terms of ##W_{3}## and ##B_{\mu}## fields in Higgs mechanism for EW if we choose a vacuum hypercharge to be -1 and compare results to SM (where we know that photon is massless and Z is not)

Homework Equations


Mass term for ##W_{3}## and ##B_{\mu}##:
$$(-gW_{3}+g^{'}Y_{vac}B_{\mu})^2=(W_3, B_{\mu})\Bigg(\begin{matrix}
g^2 & -gg^{'} Y_{vac} \\
-gg^{'} Y_{vac} & g^{'2}
\end{matrix}\Bigg)\Bigg(\begin{matrix}W_3\\
B_{\mu}
\end{matrix}\Bigg)$$

The Attempt at a Solution


Let's find eigenvalues and eigenvectors of $$
\Bigg(\begin{matrix}
g^2 & -gg^{'} Y_{vac} \\
-gg^{'} Y_{vac} & g^{'2}
\end{matrix}\Bigg)
$$
for ##Y_{vac}=-1##
$$
det\Bigg(\begin{matrix}
g^2-\lambda & gg^{'}\\
gg^{'} & g^{'2}-\lambda
\end{matrix}\Bigg)=0
$$
$$(g^2-\lambda)(g^{'2}-\lambda)-(gg^{'})^2=(gg^{'})^2-\lambda g^2 -\lambda g^{'2} + \lambda^2=
\lambda(\lambda-(g^2+g^{'2}))=0$$

There are 2 eigenvalues: ##\lambda=0## and ##\lambda=(g^2+g^{'2})##
For ##\lambda=0## the eigenvector is:
$$g^2x+gg'y=0$$
$$gx=g'y$$
$$x=g', y=g$$
+ normilize it:
$$
\frac{1}{\sqrt{g^2+g^{'2}}}\Bigg(\begin{matrix}
g'\\
g
\end{matrix}\Bigg)=0
$$For ##\lambda=(g^2+g^{'2})## following the same procedure:
$$g^2x-gg'y=g^2x+g^{'2}x$$
$$-gy=g'x$$
$$x=g, y=-g'$$
+ normilize it:
$$
\frac{1}{\sqrt{g^2+g^{'2}}}\Bigg(\begin{matrix}
g\\
-g'
\end{matrix}\Bigg)=0
$$

Eigenvectors describe mass. We have two bosons, one of them is massless (photon) other is not (Z-boson).

In terms ##W_3## and ##B_{\mu}## we can write:
$$A'_{\mu}(photon)=\frac{1}{\sqrt{g^2+g^{'2}}}(g^{'}W_3+gB_{\mu})$$
$$Z'_{\mu}=\frac{1}{\sqrt{g^2+g^{'2}}}(gW_3-g^{'}B_{\mu})$$

BUT!
$$(-g W_{3}-g^{'}B_{\mu})^2 \neq (g^2+g^{'2}) Z'^2_{\mu} +0 \cdot A'^2_{\mu}$$

We need a mass of ##Z## to be equal 0 and photon to survive, because $$A'^{2}_{\mu}=(g^{'}W_3+g B_{\mu})^2=(-g W_{3}-g^{'}B_{\mu})^2$$

For ##Y_{vac}=1## everything works fine, but in this case not! It kind of surprises me, because choice of vacuum hypercharge is described as arbitrary in our lecture notes (however, they say that it becomes clear why it is better to choose +1 if you look at photon coupling with electric charge).

So, my question is: am I missing something in math or everything is fine and -1 hypercharge for vacuum doesn't work already in this case?
 
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  • #2


Your solution looks correct to me. It seems that choosing a vacuum hypercharge of -1 does not work in this case because it does not give a massless photon and a massive Z-boson as we expect in the Standard Model. This may indicate that there is some deeper reason behind why we choose a vacuum hypercharge of +1 in the Standard Model, and this is something that may become clearer as you continue your studies in this topic.
 

1. What are neutral gauge bosons in the context of electroweak unification?

Neutral gauge bosons are particles that mediate the weak nuclear force and are responsible for the unification of the electromagnetic and weak forces in the Standard Model of particle physics. These include the Z boson and the photon, which have different couplings to particles based on their electric charge.

2. What is the significance of rewriting neutral gauge bosons for vacuum with Y=-1?

Rewriting neutral gauge bosons for vacuum with Y=-1 is an important theoretical concept in electroweak theory. It allows for the unification of the electromagnetic and weak forces by assigning a value of -1 to the hypercharge of the vacuum, which is necessary for the consistency of the theory and the generation of mass for particles.

3. How does Y=-1 affect the properties of neutral gauge bosons?

The value of Y=-1 for the vacuum has a significant impact on the properties of neutral gauge bosons. It allows for the generation of mass for the W and Z bosons, which would otherwise be massless. It also affects the couplings of these particles to other particles, resulting in different interaction strengths depending on the electric charge of the particles involved.

4. Can the concept of Y=-1 be experimentally tested?

Yes, the concept of Y=-1 can be experimentally tested through the study of electroweak interactions at high energy particle colliders such as the Large Hadron Collider (LHC). By measuring the properties and interactions of neutral gauge bosons, scientists can confirm the validity of the Y=-1 concept and further refine our understanding of the electroweak force.

5. How does the concept of Y=-1 fit into the larger picture of particle physics?

The concept of Y=-1 is an important piece of the puzzle in the Standard Model of particle physics, which describes the fundamental particles and forces in the universe. By unifying the electromagnetic and weak forces, it helps to explain the behavior of particles at the most fundamental level and provides a framework for understanding the interactions of particles in the universe.

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