The Higgs and Leptophobic Force at the LHC

The Higgs boson could provide the key to discover new physics at the Large Hadron Collider. We investigate novel decays of the Standard Model (SM) Higgs boson into leptophobic gauge bosons which can be light in agreement with all experimental constraints. We study the associated production of the SM Higgs and the leptophobic gauge boson that could be crucial to test the existence of a leptophobic force. Our results demonstrate that it is possible to have a simple gauge extension of the SM at the low scale, without assuming very small couplings and in agreement with all the experimental bounds that can be probed at the LHC.


Introduction
The discovery of the Standard Model (SM) Higgs boson with a mass of 125 GeV at the Large Hadron Collider (LHC) [1,2] can be considered one of the most important discoveries in physics. We now understand how most of the elementary particles acquire mass through the Higgs mechanism and how the electroweak symmetry is spontaneously broken in nature. Thanks to the great effort of the experimental collaborations at the LHC we know well the properties of the SM Higgs and there exist experimental constraints on its decays and production mechanisms, see for example Ref. [3] for a detailed discussion.
The Higgs boson could open a door to a new physics sector since it can have new interactions that can provide information about a theory for physics beyond the Standard Model. The LHC could discover new decays and/or production channels for the Higgs boson and combining different searches we could have access to new interactions and discover new particles with masses below the TeV scale. See Ref. [4] for a report on future studies at the LHC.
In this article, we investigate new possible decays and production mechanisms of the Higgs boson due to the existence of a new interaction with a leptophobic gauge boson. A leptophobic gauge boson is predicted in simple theories where baryon number is a local gauge symmetry spontaneously broken at the low scale. See Refs. [5][6][7][8] for realistic models predicting a leptophobic gauge boson and Ref. [9] for a review. In our studies we show that one can have a large branching ratio for the Higgs decays into two leptophobic gauge bosons if they are kinematically allowed. The leptophobic gauge boson can be very light with mass below the electroweak scale in agreement with all experimental bounds and without assuming a very small gauge coupling.
When the new Higgs decays are highly suppressed or not allowed we investigate the associated Higgs-Leptophobic gauge boson production mechanism at the LHC. We find that, using this production mechanism, one can obtain large number of events with multiphotons and two quarks that can be used to test the existence of a new interaction of the Higgs boson with this new gauge boson. As in the case of the Higgs decays, the production cross-sections can be generically large due to the fact that the leptophobic gauge boson can be light in agreement with all experimental bounds. The possible existence of a leptophobic gauge boson at the low scale tells us that a gauge theory where baryon number is a local symmetry [5][6][7][8] can describe physics below the TeV scale.
This article is organized as follows: In Section 2, we review all current collider constraints on a leptophobic gauge boson and discuss the impact of these bounds on the predictions for production cross-sections at the LHC. In Section 3, we show the predictions for the new Higgs decay channels into two leptophobic gauge bosons taking into account all the experimental constraints. In Section 4, we discuss the associated production channel proton-proton to the leptophobic gauge boson and the SM Higgs, pp → Z * B → Z B h, and investigate the different signatures at the LHC. We present our conclusions in Section 5. Appendices A and B contain analytic results for all the processes considered in this work. In Appendix C, we discuss the bounds on the kinetic mixing between the Z and the new gauge boson.

Leptophobic Gauge Boson at the LHC
In simple extensions of the SM where baryon number is a local symmetry [5][6][7][8] spontaneously broken one predicts the existence of a leptophobic gauge boson Z B . For phenomenological studies of these models and dark matter see Refs. [10][11][12][13], while for a mechanism for baryogenesis in this scenario see Ref. [14]. The coupling between the SM quarks and Z B in our convention is given by As we show in the following, the local baryon number can be broken at the low scale, even at energies below the electroweak scale.
The main strategy to search for a heavy Z B at the LHC is by looking for a dijet resonance. However, at low masses this search loses sensitivity due to the large QCD backgrounds. Nonetheless, recent experimental searches for a boosted leptophobic gauge boson decaying into jets along with initial state radiation of a photon have been performed at CMS to place exclusion bounds down to a mass of 10 GeV for Z B [15]. This further motivates a study in the low mass region.
In Fig. 1 we summarize the current collider bounds for the leptophobic gauge boson in the g B −M Z B plane. As this figure shows, there is a large region in the parameter space that remains unconstrained. Specifically, for a light Z B with mass between 25 and 50 GeV the gauge coupling can take relatively large values. For smaller couplings, i.e. g B 0.1, almost any value in the window 25 GeV < M Z B < 1 TeV is allowed. Therefore, there is hope to produce this gauge boson at the LHC with large cross-sections and study its properties.    In the left panel in Fig. 2 we show the decay width of Z B for different values of the gauge coupling g B as a function of its mass. In red we show the regions that are ruled out by the collider bounds shown in Fig. 1. From this we can conclude what are the allowed values for the decay width of the leptophobic gauge boson. Moreover, with this information of the decay width we can predict the different cross-sections relevant for different collider searches. In the right panel in Fig. 2 we present contours of Γ Z B in the g B vs M Z B plane. The region shaded in red is excluded by collider searches of the Z B and we conclude that a Γ Z B of order GeV is already mostly excluded.
In Fig. 3 we present our results for the production cross-section for different channels that involve at least one Z B , fixing the gauge coupling to g B = 0.2. These results correspond to the LHC with center-of-mass energy of 14 TeV and the number of events shown on the right vertical axis correspond to an integrated luminosity of 300 fb −1 . The model has been implemented in FeynRules 2.0 [22] and the cross-sections obtained using MadGraph5aMC@NLO -v2.7.0 [23], we cross-checked our results in a Mathematica notebook and the use of the MSTW2008 [24] set of parton distribution functions. In Appendices A and B we provide analytic results for all the processes we have considered.
From Fig. 3 one can see that the dijet cross-section dominates across the plot, and in the region M Z B > 2M t the process pp → Z B → tt can be large as well. The process pp → Z B q can be significant, since there is a large contribution from the parton distribution function of the gluon in the initial state. For the pp → Z B γ, Z B q and Z B g channels we impose the following cuts on the rapidity and the transverse momentum: |η| < 2.5, and p T > 150 GeV. These three channels are relevant for searches in the low mass regime.

Exotic Decays of the SM-like Higgs
In extensions of the SM with a leptophobic gauge boson [5][6][7][8], its mass generation comes from the vacuum expectation of a new Higgs boson with non-zero baryon number, and hence, the models have two Higgs scalars. After spontaneous symmetry breaking, the SM- like Higgs will have the following coupling to the leptophobic Z B gauge boson where θ B is the mixing angle in the scalar sector, and Q B is the baryon number of the second scalar. Since the leptophobic gauge boson can be light, the SM-like Higgs can have the following decays   depending on the Z B mass, see Fig. 4. In order to calculate these decays one needs to know the coupling between the SM quarks and Z B , the couplings between the SM-like Higgs and SM particles will scale by a factor cos θ B . With this information we can calculate the impact of these novel decays of the SM-like Higgs by computing the total Higgs decay width Γ h = cos 2 θ B Γ SM + Γ BSM , where in our case Γ BSM corresponds to the decays into two leptophobic gauge bosons. Collider searches of a new scalar mixing with the SM Higgs combined with measurements of the SM Higgs properties provide constraints on the mixing angle. In our study we take the bound sin θ B ≤ 0.3 [25]. Current LHC measurements of the properties of the SM-like Higgs boson give the following constraint on its branching ratio into BSM particles [26] BR(h → BSM) < 0.34 at 95% CL, (3.2) which is obtained assuming the production of the Higgs in the SM. Therefore, we scale the bound by the ratio between the production cross-section for the Higgs in this model with the one in the SM, which is given by BR(h → BSM) < 0.34 × σ SM h /σ h = 0.34/ cos 2 θ B . We have computed the two-body and three-body decay and provide analytic expressions in Appendix A. In Fig. 5 we present our results for the branching ratios for the decay channels h → Z B Z B and h → Z B qq of the SM Higgs. The latter includes both, the on-shell and the off-shell contribution from the Z B . In the region with M Z B ≤ M h /2 ≈ 62.5 GeV the channel h → Z B Z B becomes the dominant decay channel and the Higgs decay can become of order GeV. In this region the bound on BR(h → BSM) < 0.34 gives a strong constraint shown by the area shaded in red.
On the other hand, when M Z B ≥ M h /2 the two-body decay is kinematically closed and the three-body decay gives a much smaller contribution to the Higgs width. In this regime, experiments can search for the associated Higgs Z B production to probe the existence of these interactions, as we discuss in the following section.
The experimental bound on the branching ratio of Higgs decays to BSM particles can be translated to the g B vs M Z B plane. Nevertheless, we note that this bound also depends on the scalar mixing. In Fig. 6 we present our results for two different mixing angles. For sin θ B = 0.1 this constraint is strong in the region M Z B ≤ M h /2 and excludes g B 0.03 for M Z B = 25 GeV. In order to relax this bound one needs to go to very small mixing angles, sin θ B < 0.05, as shown in the right panel. It is important to emphasize that the SM-like Higgs can have a large branching ratio into two leptophobic gauge bosons in agreement with all current experimental bounds.

Higgs-Leptophobic Gauge Boson Associated Production
In the previous section we discussed the possible new Higgs decays due to the existence of a leptophobic gauge boson. In the scenarios where these Higgs decays are not allowed or highly suppressed, one can study the associated production to test the existence of the new h−Z B −Z B interaction. See Fig. 8 for the relevant Feynman graph.
The production cross-section for this process is given by Eq. (B.4). In Fig. 7 we show the numerical predictions for the associated production p p → Z * B → Z B h in the g B − M Z B plane, in the maximal mixing scenario where θ B = 0.3 and with center-of-mass energy of √ s = 14 TeV. The region shaded in red is excluded by the experimental bound on the branching ratio of the SM Higgs into BSM particles. The different colored dotted regions correspond to the predictions in different ranges: σ < 0.1 fb (blue dots), 0.1 fb < σ < 1 fb (orange dots), 1 fb < σ < 10 fb (yellow dots), 10 fb < σ < 100 fb (cyan dots), and σ > 100 fb (purple dots). The region shaded in gray is excluded by the collider bounds discussed in Section 2. The associated cross-section is proportional to sin 2 θ B . Therefore, although in the above figure we show only the predictions for θ B = 0.3, one can easily find the allowed values for other mixing angles. It is important to mention that the associated production can be very large due to the fact that the gauge coupling can be large and the mass of the leptophobic gauge boson can be below the electroweak scale.  Figure 9: Predictions for the number of events at the LHC with center-of-mass energy of 14 TeV assuming that the integrated luminosity is L = 3000 fb −1 and using the maximal allowed value for the mixing angle θ B = 0.3. We show the number of events for the most relevant channels: γγ tt, γγ bb, γγ jj, bbbb, bbtt, and bbjj. The gray region is excluded by the LHC bounds, while the red region is excluded by the bound on the branching ratio of the new Higgs decays.
Knowing the possible h and Z B decays we can show the predictions for the number of events at the LHC for the following channels: γγ tt, γγ bb, γγ jj, bbbb, bbtt, and bbjj.
The number of events for each of these channels is given by In Fig. 9 we show the predictions for the expected number of events assuming that the integrated luminosity is L = 3000 fb −1 as planned for the High-Luminosity LHC [27], and using the maximal allowed value for the mixing angle θ B = 0.3. The gray regions in Fig. 9 are excluded by the collider bounds discussed in Section 2, while the regions in red are excluded by the experimental bound on the branching ratio of SM Higgs exotic decays. One can notice that a large number of events for these channels can be predicted and then one can hope to test these predictions in the near future at the LHC. A dedicated analysis for these signatures is required but it is beyond the scope of this article.

Summary
The SM Higgs boson can open a doorway to new physics and there is a chance to discover a new sector from the existence of new interactions with the Higgs. In this article, we investigated the possibility that the Higgs can have a new interaction with a leptophobic gauge boson. In this scenario, Higgs decays can have a large branching ratio into two leptophobic gauge bosons if they are kinematically allowed. The leptophobic gauge boson can be very light, with mass below the electroweak scale, in agreement with all experimental bounds and without assuming a very small gauge coupling.
In the case where the new Higgs decays are highly suppressed or not allowed, we investigated the associated Higgs-Leptophobic gauge boson production mechanism at the LHC. We showed that from this channel it is possible to obtain a large number of events with multi-photons and two quarks, which can be used to probe the existence of the interaction of the Higgs with the new gauge boson. As in the case of the exotic Higgs decays, the production cross-sections can be generically large due to the fact that the leptophobic gauge boson can be light in agreement with all experimental bounds. It is relevant to mention that the possible existence of a leptophobic gauge boson at the low scale tells us that it is possible to have a simple gauge theory where baryon number is a local gauge symmetry [5][6][7][8] describing physics below the TeV scale. The partial decay width of the leptophobic gauge boson Z B with mass M Z B is given by

A Decays Widths
where M q is the mass of a given quark.
• New Higgs Decays: The width for the new two-body decays, h → Z B Z B , of the SM Higgs boson is . The three-body decay, h → Z B (p 1 ) q(p 2 )q(p 3 ), is given by Neglecting the quark masses we have that where p ij = (p i + p j ) 2 and the spin-averaged squared amplitude is given by (A.6)

B Production Cross-sections
The hadronic production cross-section reads as where σ(qq → XY )(ŝ) corresponds to the partonic cross-section and The parameter τ =ŝ/s, whereŝ is the partonic center-of-mass energy squared, s is the hadronic center-of-mass energy squared, τ 0 = (M X + M Y ) 2 /s is the production threshold, and µ is the factorization scale. In what follows we give the analytic results for the partonic cross-sections.
• Di-quark production: q q q q Z * B Figure 11: Di-quark production channel.
The di-quark production cross-section through the leptophobic gauge boson, is given by where we have neglected the quark masses in the initial state.
• Associated Production: The associated Z B − h production, is relevant to test the existence of the new Higgs interaction with the leptophobic gauge boson.
The cross-section at the partonic level is given by where the U(1) B charge of the new scalar is taken as Q B = 3 as in the minimal models [5][6][7][8].
• Di-boson production: Taking quarks to be massless, the cross-section for the process qq → Z B V where V = Z, W ± , Z B is given by where the overall factor n = 1(= 1/2) corresponds to having distinguishable (indistinguishable) particles in the final state, and the coefficients C V and C A correspond to the vector and axial couplings of the gauge bosons respectively, • For the process qq → Z B γ the averaged squared amplitude is given by, , where Q q corresponds to the electric charge of the quark. In order to compute the proton-proton cross-section we include the cuts on the transverse momentum and the rapidity of the photon (also gluon and quark) as it is explained in the main text.
• For the process qq → Z B g we have where g S corresponds to the strong coupling the SM. • For the process qg → Z B q, the averaged squared amplitude is given by and we follow the same procedure as above to compute the proton-proton crosssection.

C Constraints from Kinetic Mixing
In this Appendix, we study the kinetic mixing between the U(1) Y and U(1) B gauge groups, see Refs. [5][6][7][8] for realistic theories where baryon number is a local gauge symmetry. This parameter can be constrained by studying the properties of the Z boson in the SM, see e.g. [28,29]. The most general Lagrangian that can be written under the gauge group SU(3) c ⊗ SU(2) L ⊗ U(1) Y ⊗ U(1) B involving the neutral gauge bosons of the theory is given by where Y L/R are the hypercharges of the left/right-handed fields interacting with the hypercharge gauge boson B µ , Q B = 1/3 is the charge of the gauge quarks under the baryon force, µ B = 3g B v B is the mass term generated after the spontaneously breaking of U(1) B and sin parametrizes the kinetic mixing between both Abelian gauge bosons B µ and B µ .
There are different paths to bring the kinetic terms in the first line of Eq. (C.1) to an orthonormal form via a non-orthogonal transformation. For convenience, we choose a change of basis that does not modify the well-known relation between the neutral SM gauge bosons, this can be achieved through the following transformation of the B µ and B µ fields: which renders the kinetic Lagrangian for the gauge bosons orthonormalized and leads to the following Lagrangian mass terms with the mass matrix in the neutral gauge boson basis (W 3 µ , B µ , B µ ) Now, by rotating the W µ 3 and B µ fields as it is done in the SM,    , and sin θ 0 W ≡ g 1 the photon decouples and we are left with the following mass matrix for the still unphysical neutral gauge bosons C µ and B µ : The above mass matrix defines the angle of the final rotation towards the physical basis, C µ = cos ξ Z µ + sin ξ Z Bµ B µ = − sin ξ Z µ + cos ξ Z Bµ (C.7) given by tan2ξ = 2g 1 g 2 1 + g 2 2 tan v 2 0 4µ 2 B sec 2 + g 2 1 tan 2 v 2 0 − (g 2 1 + g 2 2 )v 2 0 , (C. 8) with the following eigenvalues defining their masses: M 2 Z,Z B = 1 8 g 2 1 sec 2 + g 2 2 v 2 0 + 1 2 µ 2 B sec 2 ± 1 8 4µ 2 B sec 2 + (g 2 1 sec 2 + g 2 2 )v 2 0 2 − 16(g 2 1 + g 2 2 )µ 2 B v 2 0 sec 2 , (C.10) as expected, in the limit → 0 we recover the original masses in the Lagrangian for Z and Z B . We can now apply the high precision measurement of the Z boson mass to constrain the kinetic mixing parameter, sin . The mass of the Z boson has been measured to be [3] ∆M where the last number is the one standard deviation uncertainty in the experimentally measured Z boson mass and will constrain the shift induced by the kinetic mixing. In Fig. 14 we show this constraint in the M Z B vs sin plane. As one can see in Fig. 14 that the kinetic mixing has to be very small and it does not change the main results in our paper. A recent study by the CMS [30] collaboration finds stronger constraints for this mixing parameter for M Z B ≤ 200 GeV by searching for the direct production of a new gauge boson.