Research Article  Open Access
J. M. Cabarcas, J. Duarte, J.Alexis Rodriguez, "Sources of FCNC in Models", Advances in High Energy Physics, vol. 2012, Article ID 657582, 12 pages, 2012. https://doi.org/10.1155/2012/657582
Sources of FCNC in Models
Abstract
There are different models which are based on the gauge symmetry (331), and some of them include exotic particles, and others are constructed without any exotic charges assigned to the fermionic spectrum. Each model buildup on 331 symmetry has its own interesting properties according to the representations of the gauge group used for the fermionic spectrum, that is, the main reason to explore and identify the possible sources of flavor changing neutral currents and lepton flavor violation at tree level.
1. Introduction
The standard model (SM) [1ā3] has been successful to describe leptons, quarks, and their interactions. But in any case, the SM leaves open questions concerning to the electroweak symmetry breaking sector of the model, as well as the particle content of the model: why there are three generations of quarks and leptons? These questions, among others, are the motivation to consider the SM as one important attempt to understand the elementary particles of nature and their interactions but not to consider the SM as the ultimate theory of nature. A common alternative to look for new physics beyond the SM is enlarging the gauge symmetry group, one of these alternatives is the gauge symmetry (331) [4ā11]. There are many motivations for this new gauge symmetry group, one of them is that there are some of models are based on 331 symmetry that explain why the family number must be three. This result is obtained from the anomalyfree condition which is satisfied when equal number of triplets and antitriplets (taking into account the ) are present and requiring the sum of all fermion charges to vanish, but even that each generation is anomalous and the anomaly cancellation is given for three generations or multiply of three. Other motivation is concerned with the feature that in this model should be less than , it is related to the ratio of the coupling constants and of and , in this model, there is an energy scale at which the perturbative character is lost, and the energy scale is found using the condition and it is order of āTeV [12].
On the other hand, in the breaking symmetry of the 331 gauge symmetry to the gauge group of the SM and then to the , some new bosons appear such as a new neutral boson which is heavier than the SM gauge bosons and in all the 331 models it can mediate flavor changing process at tree level. In contrast, in the framework of the SM it is well known that flavor changing neutral currents (FCNC) are strongly suppressed, because they appear only at one loop level. Therefore, these FCNC processes can help to put stringent bounds on the parameter space of these kind of models [13ā20]. Our aim in this work is to review the possible models that can be built on the basis of extended gauge symmetry 331 and identify the different sources of FCNC in the quark sector as well as the lepton sector.
2. 331 Models
The gauge group to be consider is . Lefthanded particles are into triplets, there are the usual quarks and leptons plus new exotic particles, and the anomalyfree condition constrains the allowed fermion representations (3 or ) and the quantum numbers. To describe the particle content of the model and to identify specific types of 331 models is important and so is how defined the electric charge operator, which can be written as a linear combination of the diagonal generators of the group where is a parameter that characterizes the specific particle structure. The parameter can be chosen or , obtaining 331 models with exotic electric charges or 331 models without exotic electric charges, and by exotic charges we mean charges different from those that appear in the SM framework.
Since each lepton family has three states, taking massless neutrinos, they can be arranged into antitriplets , where is a family index. The first two components corresponds to the ordinary electroweak doublet. This model corresponds to [4ā11] for the charge operator in (2.1). Therefore each lepton family will be in the representation of . With these assumptions, there are no new leptons in the 331 model, and all three lepton families are treated identically. In contrast, one of the three quark families transform differently from the other two which is required to anomaly cancellation. Anomaly cancellation requires that two families of quarks transform as triplets , and the third one transforms as an antitriplet . The righthanded spectrum is put in singlets in the usual way for the first two families and for the third one. It is worth to notice that in general the assumption that one quark family is transforming differently to the other two families is a general condition in the framework of 331 models, and it is generally assumed that the unique generation corresponds to the third generation, and then, it could explain the heavy top quark mass.
In the gauge sector, five new gauge bosons beyond the SM are found. The new gauge bosons form a complex doublet of dileptons with hypercharge 3 and a singlet . The gauge boson mixes with the gauge boson from the to form the hypercharge boson and a new neutral boson.
In order to break the symmetry spontaneously, four Higgs multiplets are necessary. Three triplets in representations , , and for the breaking of in order to give masses to all quarks, and a sextet is required for the lepton masses [4ā11].
In this first model [4ā11], there are new sources of FCNC processes at tree level coming from the new boson in the quark sector, because the families are treated differently. Also, at one loop level appears new contributions coming from the charged bileptons and the charged scalar sector [21ā26]. In this model, there are FCNC in the lepton sector, and they are mediated by the charged bileptons [21ā26].
A possible variation of this original model is to consider a new lepton assignment using a heavy lepton instead of the and adding and as singlets [27]. With this model, it is easy to generate small neutrino masses and lepton number violation can occur and one property of this model version is that bileptons only couple standard to exotic leptons [27].
On the other hand, it is possible to obtain models based on the gauge 331 symmetry but without new exotic charges for the fermions. One version of that is the model proposed by Ćzer [28], where it is introduced a righthanded neutrino. A systematic study of these kind of models was done in [29, 30]. According to the value in (2.1), it is possible to get six different set of fermions and the fermion structure in order to avoid the quiral anomalies producing different 331 models. The fermion sets are four lepton sets and two quark sets.
The first set of leptons is using as the family index and , and are the SM fermions and , and are the exotic ones.
The second set is where there is a neutral exotic particle. For the third leptonic set, where there is a charged exotic particle and four new exotic neutral ones. Finally, for the forth set with three exotic charged particles and three neutral.
Now, the quark sets are The anomaly contribution for each set is presented in Table 1.

On the basis of Table 1, it is possible to build up many models asking for the anomaly free condition. There are two one family models and eight three family models, referring to how cancel out the anomalies if it is needed one family or the three families. There are two one family models composed by the sets and . These models were studied in [29ā31] and their relation with the grand unified theories established. For the three family models, there are the combinations , , and , and there are other two models particularly interesting, because they treat the three family leptons completely different, they are the combinations and [31, 32].
In the gauge sector, there are 17 gauge bosons, one gauge boson associated to , eight gluons associated to and eight gauge fields from the . The gauge bosons associated with transform according to the adjoint representation of the group, and they can be written as where are the GellMann matrices, and the electric charges of and are given by and , respectively.
In general, it is convenient to rotate the neutral gauge bosons , and into new states , , and , given by where the angle is defined by , , being the coupling constants associated to the groups and , respectively, (, etc.). In the new basis, (the photon) is the gauge boson corresponding to the generator , while can be identified with the SM boson. As in the SM, the extended electroweak symmetry is spontaneously broken in 331 models by the presence of elementary scalars having nonzero vacuum expectation values [33ā37]. The symmetry breakdown follows a hierarchy in which two VEV scales and , with , are introduced. The photon is kept as the only massless gauge boson, while the remaining neutral gauge bosons get mixed. In this way, and turn out to be only approximate mass eigenstates.
3. FCNC in 331 Models
First of all, the extension of the gauge group which embedded the SM group implies a new neutral gauge boson, which in general in all the 331 models presented generates FCNC at treelevel. This fact is that because in 331 models it is not possible to accommodate all the SM spectrum in multiplets with the same quantum numbers; therefore, the couplings are not universal for all the fermions, and that is the origin of a new source of FCNC. Particularly, to treat in a different manner the third generation, as is usually assumed, to the other two generations produces FCNC contributions. This property is common to all the 331 models in the quark sector. It is worth to mention that even in the lefthanded couplings of the standard fermions to the neutral boson appear FCNC at tree level through the mixing of and also coming from the mixing between the standard quarks and the exotic ones included in each case. Moreover, the mixing between neutral gauge bosons should take into account the gauge bosons which transform according to the adjoint representation of the , some noted and gauge bosons for the charged sector and neutral sector (they are related to ). In order to notice these effects clearly, the Lagrangian for the new boson with a arbitrary is the following: where , , , , and the exotic quarks with electric charges are given by and . There is explicitly shown the no universal couplings between the quarks , and the boson, and it is because one family is in the 3 representation, while the other two are in the (or vice versa). As a consequence, the FCNCs arise once the fields and are rotated to the mass eigenstates. The number of extra fermions upquark type or downquark type depends on the parameter , for will have and and for will have and . Therefore, there is not only FCNC at tree level through the boson, but also the usual boson due to the mix of these new exotic quarks with the ordinary ones. To notice this, for the case of , the following definitions are useful , , , and . Meanwhile, for the case , the definitions are , , , and . With this vector notation, the Lagrangian for neutral currents is where the sum is over , , , and . The couplings depends on the parameter . With , the interaction is where the no universality of the left handed quarks is clear, while the righthanded couplings drive for are universals.
In a similar way for the boson, the couplings are
At this point, it is important to mention that the couplings in (3.2)ā(3.4) are in the interaction basis, thus to obtain the mass eigenstates, it is necessary to get the rotation matrices which diagonalize the mass matrices in the Yukawa sector. Therefore, the mass eigenstates and are defined by with matrices of dimensions and , respectively. It is useful to write the matrices as using submatrices in such a way that and in general the CKM matrix is not unitary.
In addition, the models include new gauge bosons which coupled to the left handed fermions, the couplings in (3.2) for the boson when are And when for the boson, they are
It is often assumed that the vacuum expectation values of the scalar fields are real, and this assumption implies that there is not any spontaneous CP symmetry breaking. In that case, the state decouples and therefore turn into an exact mass eigenstate. However, the bosons , and mix, and it is possible to get the mass basis , and through an orthogonal matrix which depends on the vacuum expectation values of the Higgs bosons, and therefore, the Lagrangian can be rewritten as where is the electric charge and the coupling constants are and the matrices are given by
Finally, about the sources of FCNC in the framework of the 331 models, they are two models which are very interesting, because they have some special properties from the phenomenological point of view. They are the models build up with the fermionic sets and . They not only differentiate the quark generations, doing one family specially different, but they also do in the leptonic sector. These models will have the usual FCNC at tree level in 331 models in the quark sector through the boson but also they present FCNC in the leptonic sector through the scalar fields and through the boson [32]. To notice the new sources of FCNC arising in these models, the neutral current Lagrangian is going to be obtained. First of all, the spectrum should be specified where , and note that one of the leptonic triplets is in the adjoint representation respect to the other two then FCNC at tree level will arise through the boson. Using vector notation, the neutral current Lagrangian in this case is Defining the vector , the couplings are where , and it is worthwhile to point out that the right handed couplings are not universal, and it is a new feature of this model. Usually, in the framework of the 331 models, only the lefthanded couplings are not universal, but the righthanded are universal as it was shown in (3.1).
For the neutral sector, is defined, and the lefthanded couplings are
4. Summary
One of the most intriguing options to consider physics beyond the SM consists of extending the gauge symmetry group to . There are many models which are based on the 331 symmetry, and one intriguing feature of these models is the presence of FCNC at tree level, but the source of that new interactions is not unique and depends on how the model is built up. In the PleitezFrampton model, the first one proposed, it was established the presence of FCNC at tree level coming from the new boson and due to the different assignment of the quark representation for one of the quark families; doing the lefthanded couplings between quarks and the boson not universal. On the other hand, it is possible to build up models on the basis of 331 symmetry contrary to the PleitezFrampton model without any exotic charges for the new particles in the spectrum. These kind of models correspond to a in the electric charge operator (2.1). These models include new exotic upquark type and downquark type which are going to mix with the standard quarks. In one version appears five up quark type and four down quark type, and another version include fourup quark type and fivedown quark type; also, these models include extra charged leptons in one case and neutral leptons in the other one. The mixing obtained is a source of FCNC at tree level when the quark fields are written in the mass basis. There are also a new source of FCNC which is coming from the mixing in the gauge sector between the bosons . The mixing in this sector is usually reduced to the mixing between and . If we consider the mixing between the quarks and the mixing , then the FCNC interactions appear through the and the mediation. In the leptonic sector, something similar is going to happen. Finally, there are models which not only treat different the quark families but the leptonic families too. One of these models is presented and the neutral current Lagrangian obtained, and one interesting new and additional feature is the nonuniversal couplings in the righthanded sector through the and bosons. This new contributions to the FCNC processes could help to relax the bounds obtained on the Boson mass.
Acknowledgment
The authors thank Professor V. Pleitez for useful discussions. J. Duarte acknowledges IFTUniversidade Estadual Paulista for the financial support and J.A. Rodriguez for its hospitality while this work was finished.
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Copyright © 2012 J. M. Cabarcas et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.