W_L-W_R Mixing in the Left-Right Symmetric Model

In summary, the conversation discusses how to get the mass term for the W Gauge bosons in the Left Right Symmetric Model (LRSM). The main struggle is with the Left-Right Mixing part. The LRSM has the gauge group SU(2)_L\times SU(2)_R \times U(1)_{B-L} and with an additional discrete symmetry, the left and right gauge couplings can be made equal. The Higgs sector of the theory has Vacuum Expectation Values (VEV) for the doublet $\phi$ and the triplets $\Delta_L$ and $\Delta_R$. The mass term for the W bosons is obtained from the kinetic term in the lagrangian, which involves the interaction
  • #1
andres0l1
2
0

Homework Statement



The question is how to get the mass term for the W Gauge bosons within the Left Right Symmetric Model (LRSM). My main struggle is with the Left-Right Mixing part.
So the LRSM has the gauge group $SU(2)_L\times SU(2)_R \times U(1)_{B-L}$ and with an additional discrete symmetry, we can make the left and right gauge couplings to be equal $g_L=g_R=g$. Now, the Higgs sector of the theory has the following Vacuum Expectation Values (VEV):
$$
\ev{\phi}=\left(\begin{array}{c c }
k_1 & 0 \\
0 & k_2
\end{array}\right), \,\, \ev{\Delta_{L,R}}=\left(\begin{array}{c c }
0 & 0 \\
\kappa_{L,R} & 0
\end{array}\right),
$$
Where the $\phi$ is a doublet under both $SU(2)_L$ and $SU(2)_R$, the $\Delta_L$ is a triplet under $SU(2)_L$ and transform in the trivial representation of $SU(2)_R$ and vice versa for the $\Delta_R$ Higgs. Therefore, $\tau^a=\frac{\sigma^a}{2}$ for the $\phi$ terms.
What is the mass term for the W bosons? in particular the mixing term?

2. Homework Equations


$$
D_\mu\phi=\partial_\mu\phi + ig_LW_{L,\mu}^a \tau^a\phi + ig_RW_{R,\mu}^a \tau^a+ ig'(B-L)B_\mu\phi
$$
$$
D_\mu\Delta_L=\partial_\mu + ig_LW_{L,\mu}^a \tau^a\Delta_L + ig'(B-L)B_\mu\Delta_L
$$
$$
D_\mu\Delta_R=\partial_\mu + ig_RW_{R,\mu}^a \tau^a\Delta_R + ig'(B-L)B_\mu\Delta_R
$$
The kinetic term in the lagrangian which gives mass to the gauge bosons is
$$
\mathcal{L}=Tr[(D^\mu\phi)^\dagger(D_\mu\phi) + (D^\mu\Delta_L)^\dagger(D_\mu\Delta_L) +
(D^\mu\Delta_R)^\dagger(D_\mu\Delta_R)]
$$
where the Tr is over the 2x2 matrices.

3. The Attempt at a Solution


So if we only focus on the $W^1,W^2$ terms which are the ones that give mass to the charged W bosons. I get pairs of the type $W_L,W_L$ and $W_RW_R$
The mixing will be given by the interacion with the $\phi$ field so let us only focus on it.
Within it, the mixing terms are of the form

$$W_L^aW_R^b\sigma^a\sigma^b +W^a_RW^b_L\sigma^a\sigma^b$$.

Using the properties of the sigma matrices, this is reduced to the unitary matrix multiply by $2W_L^1W_R^1 + W_L^2W_R^2 + W_L^3W_R^3$ which, when multiply by the $\phi$ at its VEV's gives

$$(k_1^2 +k_2^2)2[W_L^1W_R^1 + W_L^2W_R^2 + W_L^3W_R^3]$$

When I should be getting something of the type

$$(k_1k_2)2[W_L^1W_R^1 + W_L^2W_R^2] + 2(k_1^2+k_2^2)W_L^3W_R^3$$

What am I doing wrong?
 

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  • #2
Found the solution! I think this can be deleted. Thanks!
 

1. What is the W_L-W_R Mixing in the Left-Right Symmetric Model?

The W_L-W_R Mixing in the Left-Right Symmetric Model is a phenomenon that occurs in particle physics models where the left-handed and right-handed gauge bosons, W_L and W_R, mix with each other. This mixing is a result of the symmetry breaking in the model and can have important implications for particle interactions and decays.

2. Why is W_L-W_R Mixing important?

W_L-W_R Mixing is important because it can lead to the violation of parity, which is a fundamental symmetry in particle physics. It also affects the interactions and decays of particles, providing important insights into the underlying structure of the model and potential new physics beyond the Standard Model.

3. How is W_L-W_R Mixing studied?

W_L-W_R Mixing is studied through experiments, where scientists observe the interactions and decays of particles to measure the strength of the mixing. Theoretical calculations and simulations are also used to understand the implications of W_L-W_R Mixing in different scenarios and models.

4. What are the potential consequences of W_L-W_R Mixing?

The consequences of W_L-W_R Mixing can vary depending on the specific model and parameters. It can lead to the violation of parity and potentially open up new avenues for exploring physics beyond the Standard Model. It can also affect the decay rates and properties of particles, providing important clues for understanding the underlying mechanisms of the model.

5. How does W_L-W_R Mixing relate to other physics concepts?

W_L-W_R Mixing is closely related to other concepts in particle physics, such as symmetry breaking, gauge bosons, and parity violation. It is also relevant to current research on the search for new physics beyond the Standard Model, such as the search for dark matter and the study of neutrino physics.

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