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Electric charge operator in the $SU(3)_{C} times SU(3)_{L} times U(1)_{X}$ model

Physics Asked on July 26, 2021

The 3-3-1 extension of the Standard Model of the strong and electroweak interactions, with gauge group $SU(3)_{C} times SU(3)_{L} times U(1)_{X}$, provides an attempt to answer the question on family replication. There are several versions of the 3-3-1 models. In one of them, three $SU(3)_L$ lepton triplets are of the form ($nu_l, l, nu_l^c)_L$, where $nu_l^c$ is related to the right-handed component of the neutrino field $nu_l$. The particle content of this model is given as follows:
begin{equation}
psi_{iL} = left( begin{array}{c} nu_i e_i nu_i^c end{array} right)_L sim left( 3, -frac{1}{3} right), e_{iR} sim left( 1, -1 right) , i = 1, 2, 3 tag{1}
end{equation}

begin{equation}
Q_{1L} = left( begin{array}{c} u_1 d_1 U end{array} right)_L sim left( 3, frac{1}{3} right), Q_{alpha L} = left( begin{array}{c} d_alpha -u_alpha D_alpha end{array} right)_L sim left( 3^*, 0 right), alpha = 2, 3 tag{2}
end{equation}

begin{equation}
u_{iR} sim left( 1, frac{2}{3} right), d_{iR} sim left( 1, -frac{1}{3} right), U_{R} sim left( 1, frac{2}{3} right), D_{alpha R} sim left( 1, -frac{1}{3} right). tag{3}
end{equation}

Here, the values in the parentheses denote quantum numbers based on the $left( SU(3)_L, U(1)_X right)$ symmetry. $U$ and $D_alpha$ are exotic quarks whose electric charges are the same as of the usual quarks, i.e. $q_U = frac{2}{3}$ and $q_{D_alpha} = -frac{1}{3}$. In this case, the electric charge operator takes the form
begin{equation}
Q = T_{3} -frac{1}{sqrt{3}}T_8 + X tag{4}
end{equation}

where $T_a (a = 1, 2, …, 8)$ and $X$ stand for $SU(3)_L$ and $U(1)_X$ charges respectively. This paper just lists eq. (4) but does not derive it. I wonder how eq. (4) comes about? Why does the electric charge operator take this form? Besides, I am not very familiar with the $SU(3)_L$ charges. What are the values of $T_a$ especially those of $T_3$ and $T_8$ for the particles involved?

One Answer

Eq. (4) comes about by construction of the model, and should be trivial to check by inspection: it is the reason behind constituting the multiplets this way. The generators of su(3), normalized like all generators, must, therefore, be the Gell-Mann matrices halved, $$ T_3=operatorname{diag} (1/2,-1/2,0), qquad T_8=operatorname{diag} (1,1,-2)/2sqrt{3}, ~~leadsto Q=operatorname{diag} (1/3+x,-2/3+x,1/3+x), $$ where x is the eigenvalue of X given in the parenteses, for the triplets.

For the singlets, of course, omit the su(3) generators, as they are represented by null and the group elements by the identity, and the charge is x. For the antitriplets, just reverse the sign of the above generators.

If you are having trouble with confirming all charges' comportance with this, go back (run!) to your SM and GUT text. But there is hardly anything to be derived!

Correct answer by Cosmas Zachos on July 26, 2021

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