Associated production of the Higgs boson and a single top quark in the littlest Higgs model at Large Hadron Collier

Associated production of the Higgs boson and a single top quark in the littlest Higgs model at Large Hadron Collier

Shuo Yang Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, China shuoyang@itp.ac.cn
Abstract

In the context of the littlest Higgs model, we study the associated production of the Higgs boson and a top quark ( production) at the CERN Large Hadron Collider (LHC). The cross sections for s-channel, t-channel processes and the relative correction for the total cross section are presented. In a part of parameter space , the cross sections can be distinctly deviated from the predictions of Standard Model. We also investigate the signal and backgrounds for the production at the LHC. However, due to the large QCD backgrounds, it is not very hopeful to directly observe the signal in most of the parameter space of LH model. It is found that with 30 fb of integrated luminosity, in a narrow range of the parameter space and TeV, a statistical significance of 3 can be achieved. More than 30 fb luminosity will enhance the significance and the possibility of detecting the signal.

pacs:

I Introduction

For the Standard Model (SM) Higgs boson, the main discovery modes at hadron colliders are the associated production of or WZH (), the vector boson fusion processes bosonfusion (), the gluon-gluon fusion mode gluonfusion (), and the Higgs associated production with heavy top quark pairs ttH () or bottom quark pairs bbH (). Compared with these modes, the cross section for the production of the Higgs boson associated with a single top quark is small tH (); interference (); tH2 (). ( production Feynman diagrams are shown in Fig.1-Fig.3 .) However, measurements of the total rates for and processes only test the Higgs coupling to and the Yukawa coupling to top. The production contains the important relative phase information of the couplings of the Higgs to and to top, and production is sensitive to some new physics interference (); tH2 (). As a class candidate of physics beyond SM, little Higgs models LHidea (); MiniMoose (); LHM (); SU3 (); LHT (); LHreview (); LHreview2 () predict new bosons, fermions and scalars. These new particles will contribute considerably to Higgs production. The Higgs phenomena in little Higgs models have been extensively studied in the literature higgspheno (); higgsLH (). In this paper, we study the production at the LHC in the frame of the littlest Higgs model.

The rest of this paper is organized as follows. In Sec. II we briefly describe the general features of little Higgs models and then focus on the littlest Higgs model. The Feynman rules and formulas relevant to our computation are also listed in this section. In Sec. III, we study production in the littlest Higgs model at the LHC. Finally, we give our conclusions in Sec. IV.

Ii Littlest Higgs Model

In this section we firstly introduce the general features of little Higgs models and then describe the littlest Higgs model focusing on particle content and the couplings relevant to our computation.

The major motivation of little Higgs theory LHidea () is to cure the hierarchy problem of SM. Little Higgs models suppose that Higgs boson is a Nambu-Goldstone boson (NGB) of some approximate global symmetry and avoid one-loop quadratically divergent through collective breaking mechanism LHidea (). The collective symmetry breaking means that when one interaction breaks some of the global symmetries, it still exits unbroken global symmetry ensuring the Higgs’s identity as an exact NGB. The symmetries protecting Higgs is explicitly broken only when two or more couplings in the lagrangian are present. In this way, the collective symmetry breaking protects the Higgs mass from receiving quadratically divergent radiative corrections at one-loop. The Coleman-Weinberg potential generates the Higgs potential and triggers electroweak symmetry breaking (EWSB). The implementation of collective symmetry breaking results in the prediction of new gauge bosons, new fermions and new scalars at TeV scale. These new particles will be produced at the LHC and contribute derivations to SM processes.

As a realistic implementation of little Higgs idea, the littlest Higgs (LH) model LHM () base on a coset. The global symmetry is spontaneously broken down to global symmetry via a vacuum expectation value (VEV) of order , simultaneously, and the gauge group of is broken down to its diagonal subgroup. The breaks result in new heavy bosons , , and new scalar triplet , which acquire masses of order . In order to implement the collective symmetry breaking mechanism in top sector, LH model also introduces a pair vector-like quarks. After EWSB, the physical states in top sector are the top quark and the heavy quark . We list the Feynman rules and formulas LHhan (); smokinghan () relevant to our computation as below where the terms of order has been neglected:

(1)
(2)
(3)
(4)
(5)
(6)

In these formulas, ( ) is the mixing parameter between the and gauge bosons, is the new symmetry breaking scale, and =/, where and are Yukawa coupling parameters in top sector. The couplings of to fermions are suppressed by and the contribution of to production can be safely ignored, so we do not list the coupling of here.

Figure 1: Feynman diagrams for production in t-channel process.
Figure 2: Feynman diagrams for production in s-channel process.
Figure 3: Feynman diagrams for production in W-associated process.

Iii Production in the littlest Higgs model at the LHC

As shown as in Fig.1 - Fig.3, the Higgs in association with a top quark can be produced at the LHC in t-channel, s-channel and W-associated process. In these Feynman diagrams, represents for SM and represents and for LH model, represents for SM and represents and for LH model. In SM, the t-channel process has the largest cross section and the s-channel has the smallest cross section. However, in LH model both the cross sections in s-channel and t-channel can dominate over the W-associated process in a part of the parameter space as shown below.

Figure 4: Cross section for t-channel production as a function of the parameter for c=0.4 (dot line), c=0.7 (dash line), c=0.8 (solid line).
Figure 5: Cross section for s-channel production as a function of the parameter for c=0.4 (dot line), c=0.5 (dash dot line), c=0.7 (dash line), c=0.8 (solid line).

In our computation (We compute production including both top quark and antitop production.), we have used Madgraph madgraph () package and CTEQ6L cteq6 () parton distribution functions with the factorization scale . The SM input parameters relevant to our computation are taken as GeV topmass (), GeV, GeV, , and pdg ().

Figure 6: Relative correction R of total production as a function of the scale parameter for c=0.4 (dot line), c=0.7 (dash line), c=0.8 (solid line).

In LH model, the new interactions will contribute the production and cause deviation from the cross section of SM. Considering the constraints of the electroweak precision data on LH model LHconstrains (), we assumed , TeV TeV and . A low will result in a light which is disfavored by limit from Tevatron and precision electroweak constrains. This can be resolved by considering alternative embeddings of the two U(1) generators or only gauging a U(1) group, i.e. the gauge group is LHconstrains (). Fig.4 and Fig.5 show the cross sections as a function of the scale parameter for different value of mixing parameter for t-channel and s-channel production, respectively. The computation results are very sensitive to the value of , which because the coupling of to fermions are in proportion to and the cross section for relevant diagrams will be sensitive to . In LH model, the cross section both in s-channel process and t-channel process can reach the level of 70 fb in a part of parameter space. The cross section for W-associated channel is not sensitive to the variation of parameters and in most of the parameter space the deviation from the SM prediction is small, so we don’t show the cross section for W-associated production. Different from the case in SM where the t-channel process has the largest cross section and s-channel has the smallest one, in LH model both the cross sections in s-channel and t-channel can dominate over the W-associated process in a part of the parameter space. This is mainly because the couplings of and are suppressed by mixing parameters as shown in Feynman rules, so the contributes from new particles are very weak in W-associated channel. In t-channel and s-channel, the new contributes mainly come from and which are not suppressed. However, the effects from new particles become weak and the cross sections of production converge to the values of SM as increase and c decrease. In order to describe the deviation of total cross section from the SM prediction, we define a relative correction function

(7)

and show the as a function of for , and in Fig.6. As shown in Fig.6, it is found that in most of the parameter space, the cross section in LH model is larger than the prediction of SM which will enhance the detecting possibility in this mode.

Now we further consider the signature of production at the LHC. In order to provide a efficient lepton trigger the semi-leptonical decay of top is considered, and the decay of is required for the large branching ratio 11footnotetext: In our calculation, we ignored the corrections to branching ratio of ( ) ) in LH model. Because in LH model couplings of fermions and gauge bosons of SM to the Higgs are only shifted by an order of , and only decay widths of , and are modified due to new particles in loops. For a light Higgs, there is no new decay channel and the dominant decay channel is still . So the change of is not distinct in most of the parameter space and the change converges to zero as f increases. Detailed analysis of Higgs decay in LH model have been studied in Ref. higgsLH ().. In this case for t-channel mode the signal is 1 forward jet and for s-channel the signal is . However, ref.tH2 () has pointed that it is difficult to extract the signal 1 forward jet from the large backgrounds and the hopeful signal for t-channel is 1 forward jet where the additional comes from the splitting of virtual gluons into pairs. From a phenomenological point the difference between s-channel 4b signal and t-channel 4b signal is that all the jets are high central jets in s-channel while t-channel signal has a forward jet and a low -jet. We may separate them by rejecting or tagging a forward jet. But the s-channel signal will always be accompanied by a jet coming from QCD radiation. If we consider the s-channel signal and t-channel signal separately, each of them will be the important backgrounds for the other. So, in this paper, we consider the signal is 1jet which include t-channel events and s-channel events with a radiated jet. We study the signal and backgrounds in a idealized case that the top is reconstructed with 100% efficiency, so the coming from top decay can be separated from other quarks.

For the 1jet signal, with decay to pair, are two of the main backgrounds. The process contributes to backgrounds when one of the jets from W decay is missed or in the case that one of the jets from W decay is mistagged as a -jet and another jet ( including ) is missed. Due to the large rate of , when both and quarks from the hadronically decaying W are mistagged, this process also contributes to the backgrounds.

Because for many events in our signal the final particles from new heavy particles’ contributions are more energetic and with high- than the events in SM, So we raise the minimum to 20 GeV and loose the forward jet constrain compared with the cuts in Ref.tH2 (). The cuts are shown as below:

GeV,

GeV,

GeV, ,

At least one pair GeV.

All pairs min 90 GeV

At least one pair GeV means that we require at least one pair ( not including the that reconstructs the top ) accord with GeV. All pairs min 90 GeV means that the invariant mass of all pairs ( not including the that reconstructs the top ) is required in this range.

Signal
cross section (fb) 0.482 0.054 0.039 0.61 0
events with 30 fb 14.5 1.6 1.2 18.3 0
Table 1: Cross section and events with 30 fb of integrated luminosity for the signal and backgrounds for the production. For the signal, the parameter values , TeV, are chosen.

At luminosity 30 fb, only in a very narrow part of the parameter space and TeV of LH model, we can achieve the statistical significance of . We list the cross section and events with 30 fb which pass the cuts for the signal and the important backgrounds in table I, in which for the signal the parameter values , TeV, are taken. The -tagging efficiency , lepton-tagging efficiency and the mistag probability , have been included in computation.

Iv Conclusion

In the frame of the littlest Higgs model we calculate the production of the Higgs bosons associated a top quark at the LHC. Due to the new interactions of new gauge boson and new fermion with Higgs boson, these new particles can contribute to production cross section. We find that in a large part of the parameter space the cross section of in s-channel and t-channel production can deviate largely from the SM prediction. Different from the case in SM, in LH model both the cross sections in s-channel and t-channel are larger than that in W-associated process in a part of the parameter space. We also consider the signal 1jet and backgrounds for the production. However, due to the large QCD backgrounds, it is not very hopeful to observe the signal in most of the parameter space of LH model. It is found that with 30 fb of integrated luminosity, in a narrow range of the parameter space and TeV, a statistical significance of 3 can be achieved. More than 30 fb luminosity will enhance the significance and the possibility of detecting the signal.

Acknowledgements.
The author would like to thank Chun Liu, Jin Min Yang, Chong-Xing Yue and Lei Wang for useful discussions. This work was supported in part by the National Science Foundation of China under Grant No. 90503002 and the Project of Knowledge Innovation Program (PKIP) of Chinese Academy of Sciences, Grant No. KJCX2.YW.W10.

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