Top Partner Production at Collider in the Littlest Higgs Model with -Parity
In the framework of the littlest Higgs Model with -parity, we discuss the top partner production at future collider. We calculate the cross sections of the top partner production processes and associated production processes of Higgs and top partner under current constraints. Then, we investigate the observability of the -odd top partner pair production through the process in the dilepton channel for two -odd top partner masses GeV at TeV. We analyze the signal significance depending on the integrated luminosity and find that this signal is promising at the future high energy collider.
The discovery of the Higgs boson at the Large Hadron Collider (LHC) [1, 2] is a great step towards understanding the electroweak symmetry breaking (EWSB) mechanism. However, the little hierarchy problem [3, 4], which is essentially from quadratically divergent corrections to the Higgs mass parameter, still exists. In the past, various new physics models have been proposed to solve this problem, and the littlest Higgs Model with -parity (LHT) [5–7] is one of the most promising candidates.
In the LHT model, the Higgs boson is constructed as a pseudo-Nambu-Goldstone particle of the broken global symmetry. The quadratic divergence contributions to Higgs boson mass from the SM top quark loop, gauge boson loops, and the Higgs self-energy are cancelled by the corresponding -parity partners, respectively. Among the partners, the top partner is the most important one since it is responsible for cancelling the largest quadratically divergent correction to the Higgs mass induced by the top quark.
Recently, the ATLAS and CMS collaborations have performed the searches for the vector-like top partner through the pair or single production with three final states , , and and have excluded the top partner with the mass less than about 700 GeV [8–10]. Besides, a search has been performed in pair-produced exotic top partners, each decay to an on-shell top (or antitop) quark and a long-lived undetected neutral particle . Apart from direct searches, the indirect searches for the top partners through their contributions to the electroweak precision observables (EWPOs) [12, 13], -pole observables [14–16], and the flavor physics [17–24] have been extensively investigated. The null results of the top partners, in conjunction with the EWPOs and the recent Higgs data, have tightly constrained the parameter space of the LHT model [25–30].
Compared to the hadron colliders, linear colliders may provide cleaner environments to study productions and decays of various particles. Some design schemes have been put forward, such as the International Linear Collider (ILC) [31–33] and the Compact Linear Collider (CLIC) [34–36]; they can run at the center of mass (c.m.) energy ranging from 500 GeV to 3000 GeV, which enables us to perform precision measurements of the top partner above the threshold. In addition, the polarization of the initial beams at linear colliders will be useful to study the properties of the top partner. Some relevant works have been widely studied in various extensions of the Standard Model (SM) [37–39], including the Little Higgs model [40, 41]. However, the works in Little Higgs model mostly were performed many years ago and before the discovery of the Higgs boson, so it is necessary to revisit this topic. Moreover, the different final states are analyzed in this work.
The paper is organized as follows. In Section 2 we review the top partner in the LHT model. In Section 3 we calculate top partner production cross sections. In Section 4 we investigate signal and discovery potentiality of the top partner production at collider. Finally, we draw our conclusions in Section 5.
2. Top Partner in the LHT Model
The LHT model is a nonlinear model based on the coset space [42–49]. The global group is spontaneously broken into at the scale (TeV) by the vacuum expectation value (VEV) of the field, which is given byThe VEV also breaks the gauged subgroup of down to the diagonal SM electroweak symmetry . After the symmetry breaking, there arise 4 new heavy gauge bosons whose masses are given at by with and being the SM and gauge couplings, respectively. The heavy photon is the lightest -odd particle and can serve as a candidate for dark matter. In order to match the SM prediction for the gauge boson masses, the VEV needs to be redefined as where = 246 GeV.
In the fermion sector, the implementation of -parity requires the existence of mirror partners for each original fermion. In order to do this, two fermion doublets and are introduced and -parity interchanges these two doublets. A -even combination of these doublets is taken as the SM fermion doublet and the -odd combination is its -parity partner. The doublets and are embedded into incomplete multiplets and as and , where . To give the additional fermions masses, an multiplet is also introduced as , whose transformation under the is nonlinear: , where is the unbroken rotation in a nonlinear representation of the . The components of the latter multiplet are the so-called mirror fermions. Then, one can write down the following Yukawa-type interaction to give masses of the mirror fermions: where are the generation indices. The masses of the mirror quarks and mirror leptons up to are given by where are the diagonalized Yukawa couplings.
In the top quark sector, two singlet fields and (and their right-handed counterparts) are introduced to cancel the large radiative correction to the Higgs mass induced by the top quark. Both fields are embedded together with the and doublets into the multiplets: and . The -even combination of is the SM fermion doublet and the other -odd combination is its -parity partner. Then, the -parity invariant Yukawa Lagrangian for the top sector can be written down as follows:where and are the antisymmetric tensors with and , is the image of under -parity, and and are two dimensionless top quark Yukawa couplings. Under -parity, these fields transform as , , and . The above Lagrangian contains the following mass terms: where and . The -parity eigenstates have been defined as , , and . Note that -odd Dirac fermion does not have the tree-level Higgs boson interaction, and thus it does not contribute to the Higgs mass at one-loop level.
The two -even eigenstates and mix with each other so that the mass eigenstates can be defined aswhere the mixing angles and can be defined by the dimensionless ratio as The quark is identified with the SM top quark, and is its -even heavy partner, which is responsible for the cancellation of the quadratic divergence to the Higgs mass induced by the top quark loop.
The Yukawa term generates the masses of the top quark and its partners, which are given at bySince the mass is always larger than the -odd top partner mass, the can decay into in addition to the conventional decay modes ().
The -invariant Lagrangians of the Yukawa interactions of the down-type quarks and charged leptons can be constructed by two possible ways, which are denoted as Case A and Case B, respectively . In the two cases, the corrections to the Higgs couplings with the down-type quarks and charged leptons with respect to their SM values are given at order by
3. Top Partner Production in Collision
In the LHT model, the Feynman diagrams of top partner production are shown in Figure 1, which proceeds through the -channel and exchange diagrams. These processes include -even top partner pair production , -odd top partner pair production , and a -even top partner associating with a top quark production .
The Feynman diagrams of the Higgs and top partner associated production are shown in Figure 2, which has additional diagrams mediated by the -even top partner compared to the process in the SM. These processes include Higgs associating with -even top partner pair production , Higgs associating with -odd top partner pair production , and Higgs associating with a top quark and a -even top partner production .
Before calculating the top partner production cross section, we firstly consider the constraints on the top partner mass from current measurements. We update the constraint on the LHT parameter in our previous works [51, 52], where the global fit of the latest Higgs data, EWPOs, and measurements is performed. Thereinto, the constraints from the direct searches for Higgs data at Tevatron [53, 54] and LHC [55, 56] are obtained by the package HiggsSignals-1.4.0 [57, 58], which is linked to the HiggsBounds-4.2.1 [59–63] library. We compute the values by the method introduced in [64–66] and obtained the constraint on the LHT parameter space. This constraint will lead to the exclusion limits on the top partner masses, which is displayed on the plane for Case A and Case B in Figure 3 at confidence level with . We can see that the combined constraints can, respectively, exclude and up to One can notice that Case B predicts a stronger suppression for the down-type fermion couplings to the Higgs boson, such as , which helps to enhance the branching ratios of , so that Case B is favored by the experimental data .
In the left frame of Figure 4, we show the top partner production cross sections as a function of c.m. energy for GeV and (corresponding to GeV and GeV) in collision with unpolarized beams. The production cross sections are calculated at tree-level by using CalcHEP 3.6.25 [68, 69], where the SM parameters are taken as follows : We can see that the top partner pair production cross sections increase abruptly at threshold and reach a maximum roughly 200 GeV above threshold. Then, the production cross sections fall roughly with the c.m. energy increase due to the -channel suppression. The production usually has a larger cross section than production since the mass is always lighter than the mass in the LHT model. The production cross sections of the associated production of Higgs and top partner have the similar behavior as the top partner pair production, but usually have smaller cross sections due to smaller phase space. The production cross section of the process reaches its maximum when the resonance decay of the top partner emerges.
Considering the polarization of the initial electron and positron beams, the cross section at collider can be expressed as  where is the cross section for completely right-handed polarized beam () and completely left-handed polarized beam (), and other cross sections , , and are defined analogously. We show the top partner production cross sections in polarized beam with and in the right frame of Figure 4 and find that the relevant top partner production cross sections can be enhanced by the polarized beams.
4. Signal and Discovery Potentiality
Take into account the relatively large production cross section; we will perform the Monte Carlo simulation and explore the sensitivity of -odd top partner production in the following section. The -odd top partner has a simple decay pattern, which decays almost 100% into the mode. We will explore the sensitivity of -odd top partner pair production with unpolarized beam through the channel which implies that the events contain one pair of oppositely charged leptons with high transverse momentum, two high transverse momentum -jets, and large missing transverse energy .
The dominant background arises from in the SM. Besides, the most relevant backgrounds come from , , and . Here, the backgrounds , , and are neglected due to their small cross sections. We turn off the parton-level cuts and generate the signal and background events by using MadGraph 5 , where the UFO  format of the LHT model has been obtained by FeynRules  in . We use MadGraph 5 to generate the process by issuing the following commands: generate e- e+ thodd thodd, (thodd t ah, t l+ vl b), (thodd > t ah, t l- vlb) [for signal]; generate e- e+ t t, t l+ vl b, t > l- vl b [for ]; generate e- e+ t t z, t l+ vl b, t > l- vl~ b, z vl vl [for ]; generate e- e+ w- w+ z, w- l- vl, w+ l+ vl, z b b [for ]; generate e- e+ w- w+ h, w- l- vl, w+ l+ vl, h b b [for ].
The parton shower and hadronization are performed with PYTHIA , and the fast detector simulations are performed with Delphes . We use the default card (i.e., delphes_card_ILD) of ILC in Delphes 3.3.3. The -jet tagging efficiency is taken as default value in delphes, where it is parameterized as a function of the transverse momentum and rapidity of the jets. When generating the parton-level events, we assume to be the default event-by-event value. FastJet  is used to define jets via the anti- algorithm  with distance parameter . We use MadAnalysis 5  for analysis, where the (mis)tagging efficiencies and fake rates are assumed to be their default values.
Take into consideration the constraints on the top partner mass from current measurements; we take = 700 GeV, (corresponding to GeV) and GeV, (corresponding to GeV) for two benchmark points in the following calculations. In order to reduce the background contribution and enhance the signal contribution, some cuts of kinematic distributions are needed. In Figure 5, we show the normalized distributions of transverse momentum , the pseudorapidity , , the separation between and , the energy , and the total transverse energy .
Since the dominant background arises from , the cuts that are chosen to suppress the backgrounds should be centered around the background. Firstly, we can apply the cuts of general kinematic distributions, such as , , and , to suppress the backgrounds. For the distribution, there are two peaks in the , backgrounds and one peak in the , backgrounds; we can use the deviation between the signal peak and background peak to suppress the backgrounds. Then, in view of the energy distribution, we can also use the deviation between the signal peak and background peak to reduce the backgrounds. After that, the distribution of the signal can be utilized to remove the background effectively. According to the above analysis, events are selected to satisfy the following cuts:
For easy reading, we summarize the cut-flow cross sections of the signal and backgrounds for c.m. energy = 1.5 TeV in Table 1. To estimate the observability quantitatively, the Statistical Significance () is calculated after final cut by using Poisson formula  where and are the signal and background cross sections and is the integrated luminosity. The results for the values depending on the integrated luminosity for = 1.5 TeV are shown in Figure 6. It is clear from Figure 6 that we can obtain the significance at a luminosity of fb, significance at a luminosity of fb, and significance at a luminosity of fb for = GeV.
In this paper, we discuss the top partner production at future collider in the LHT model. We first consider the constraints on the top partner masses from the current measurements and then calculate the cross sections of various top partner production processes, which include , , and , , and . Next, we investigate the observability of the -odd top partner pair production through the process with the dilepton decay of the top quark pair for = 1.5 TeV. We display the signal significance depending on the integrated luminosity and find that the significance can be obtained at a luminosity of fb for = GeV, which is promising at the future high energy collider with high luminosity.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
This work is supported by the National Natural Science Foundation of China (NNSFC) under Grants no. 11405047 and no. 11404099 and by the Startup Foundation for Doctors of Henan Normal University under Grant no. qd15207.
G. Aad, T. Abajyan, B. Abbott et al., “Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ,” Physics Letters B, vol. 716, p. 1, 2012.View at: Google Scholar
H.-C. Cheng and I. Low, “TeV symmetry and the little hierarchy problem ,” Journal of High Energy Physics, vol. 2003, no. 09, article 051, 2003.View at: Google Scholar
H.-C. Cheng and I. Low, “Little hierarchy, little higgses, and a little symmetry,” Journal of High Energy Physics, vol. 2004, no. 08, article 061, 2004.View at: Google Scholar
I. Low, “T parity and the littlest Higgs,” Journal of High Energy Physics, vol. 2004, no. 10, article 067, 2004.View at: Google Scholar
G. Aad., J. Abbott, J. Abdallah et al., “Search for pair and single production of new heavy quarks that decay to a Z boson and a third-generation quark in pp collisions at TeV with the ATLAS detector ,” Journal of High Energy Physics, vol. 2014, article 104, 2014.View at: Google Scholar
The ATLAS collaboration [ATLAS Collaboration], ATLAS-CONF-2015-012,ATLAS-COM-CONF-2015-012.
B. Yang, X. Wang, and J. Han, “The study of the contribution of the LHT model to coupling,” Nuclear Physics B, vol. 847, no. 1, pp. 1–16, 2011.View at: Google Scholar
J. Hubisz, S. J. Lee, and G. Paz, “The flavor of a little Higgs with T-parity,” Journal of High Energy Physics, vol. 2006, no. 06, article 041, 2006.View at: Google Scholar
M. Blanke, A. J. Buras, A. Poschenrieder, C. Tarantino, S. Uhlig, and A. Weiler, “Particle-antiparticle mixing, , and in the Littlest Higgs model with T-parity,” Journal of High Energy Physics, vol. 2006, no. 12, article 003, 2006.View at: Google Scholar
K. Huitu and H. Waltari, “Higgs sector in NMSSM with right-handed neutrinos and spontaneous R-parity violation,” Journal of High Energy Physics, vol. 2014, article 053, 2014.View at: Google Scholar
J. Reuter and M. Tonini, “Can the 125 GeV Higgs be the Little Higgs? ” Journal of High Energy Physics, vol. 2013, article 77, 2013.View at: Google Scholar
B. F. Yang, G. F. Mi, and N. Liu, “Higgs couplings and Naturalness in the littlest Higgs model with T-parity at the LHC and TLEP,” Journal of High Energy Physics, vol. 2014, no. 10, article 47, 2014.View at: Google Scholar
C. C. Han, A. Kobakhidze, N. Liu, L. Wu, and B. F. Yang, “Constraining top partner and naturalness at the LHC and TLEP,” Nuclear Physics B, vol. 890, pp. 388–399, 2014.View at: Google Scholar
J. Brau, “ILC Collaboration,” arXiv: 0712.19.View at: Google Scholar
E. Accomando and CLIC Physics Working Group Collaboration, hep-ph/0412251, CERN-2004- 005 .
R. Kitano, T. Moroi, and S.-F. Su, “Top-Squark Study at a Future Linear Collider,” Journal of High Energy Physics, vol. 2002, no. 12, p. 011, 2002.View at: Google Scholar
K. Kong and S. C. Park, “Phenomenology of top partners at the ILC ,” Journal of High Energy Physics, vol. 2007, no. 08, article 038, 2007.View at: Google Scholar
K. Harigaya, S. Mastsumoto, M. M. Nojiri, and K. Tobioka, “Magnetic response in the holographic insulator/superconductor transition,” Journal of High Energy Physics, vol. 2012, no. 1, article 135, 2012.View at: Google Scholar
N. Arkani-Hamed, A. G. Cohen, E. Katz, and A. E. Nelson, “The Littlest Higgs ,” Journal of High Energy Physics, vol. 2002, no. 07, article 034, 2002.View at: Google Scholar
N. Arkani-Hamed, A. G. Cohen, E. Katz, A. E. Nelson, T. Gregoire, and J. G. Wacker, “The Minimal Moose for a Little Higgs,” vol. 2012, no. 08, article 021, 2002.View at: Google Scholar
D. E. Kaplan and M. Schmaltz, “The little Higgs from a simple group,” Journal of High Energy Physics, vol. 2003, no. 10, article 039, 2003.View at: Google Scholar
F. Lizzi, P. Vitale, and A. Zampini, “The fuzzy disc,” Journal of High Energy Physics, vol. 2004, no. 08, article 056, 2004.View at: Google Scholar
M. Schmaltz, “The simplest little Higgs,” Journal of High Energy Physics, vol. 2004, no. 8, article 056, 2004.View at: Google Scholar
[ATLAS Collaboration], ATL-CONF-2015-005, ATL-CONF-2015-006.
[CMS Collaboration], CMS-PAS-HIG-14-009, CMS-PAS-HIG-13-001.
P. Bechtle, S. Heinemeyer, O. Stål, T. Stefaniak, and G. Weiglein, “Probing the Standard Model with Higgs signal rates from the Tevatron, the LHC and a future ILC,” Journal of High Energy Physics, vol. 2014, no. 11, article 039, 2014.View at: Google Scholar
P. Bechtle, O. Brein, S. Heinemeyer, G. Weiglein, and K. E. Williams, “HiggsBounds 2.0.0: Confronting neutral and charged Higgs sector predictions with exclusion bounds from LEP and the Tevatron,” Computer Physics Communications, vol. 182, no. 12, pp. 2605–2631, 2011.View at: Google Scholar
P. Bechtle, O. Brein, S. Heinemeyer et al., “Recent Developments in HiggsBounds and a Preview of HiggsSignals,” PoS CHARGED, vol. 2012, p. 024, 2012.View at: Google Scholar
P. Bechtle, O. Brein, S. Heinemeyer et al., “HiggsBounds-4: improved tests of extended Higgs sectors against exclusion bounds from LEP, the Tevatron and the LHC,” The European Physical Journal C, vol. 74, p. 2693, 2014.View at: Google Scholar
J. R. Espinosa, C. Grojean, M. Muhlleitner, and M. Trott, “Baryon electric dipole moments from strong CP violation ,” Journal of High Energy Physics, vol. 2012, no. 12, article 097, 2012.View at: Google Scholar
P. P. Giardino, K. Kannike, M. Raidal, and A. Strumia, “Reconstructing Higgs boson properties from the LHC and Tevatron data,” Journal of High Energy Physics, vol. 2012, no. 6, article 117, 2012.View at: Google Scholar
ATLAS and CMS Collaborations, “Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at and 8 TeV,” Journal of High Energy Physics, vol. 2016, no. 08, p. 045, 2016.View at: Google Scholar
C. Patrignani and Particle Data Group, “Review of Particle Physics,” Chinese Physics C, vol. 40, no. 10, Article ID 100001, 2016.View at: Google Scholar
J. Alwall, R. Frederix, S. Frixione et al., “The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations,” Journal of High Energy Physics, vol. 2014, no. 07, article 079, 2014.View at: Google Scholar
T. Sjostrand, S. Mrenna, and P. Z. Skands, “PYTHIA 6.4 physics and manual,” Journal of High Energy Physics, vol. 2006, no. 5, article 026, 2006.View at: Google Scholar
J. de Favereau, C. Delaere, P. Demin et al., “DELPHES 3: a modular framework for fast simulation of a generic collider experiment,” vol. 2014, no. 2, article 057, 2014.View at: Google Scholar
M. Cacciari, G. P. Salam, and G. Soyez, “The anti-kt jet clustering algorithm,” Journal of High Energy Physics, vol. 2008, no. 04, p. 063, 2008.View at: Google Scholar