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Advances in High Energy Physics
Volume 2013 (2013), Article ID 915897, 15 pages
Heavy Chiral Fermions and Dark Matter
1Department of Physics and Center for Theoretical Sciences, National Taiwan University, Taipei 10617, Taiwan
2Department of Physics and Center for Mathematics and Theoretical Physics, National Central University, Chungli 32001, Taiwan
Received 22 June 2012; Accepted 4 November 2012
Academic Editor: Tao Han
Copyright © 2013 Johan Alwall and Jusak Tandean. 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.
Dark matter presents perhaps one of the most compelling direct indications of new physics beyond the standard model with three generations of fermions. In this paper, we survey several scenarios for dark matter in association with a fourth generation of chiral matter. The surveyed scenarios include stable heavy neutrino dark matter, composite dark matter consisting of stable heavy quarks, heavy quarks as mediators between the dark and visible sectors, and the four-generation standard model with the minimal addition of a stable real scalar field. We discuss the basic properties of the models, direct search constraints on their dark matter, and their collider phenomenology, as well as the possible effects of dark matter on the searches for a Higgs boson in the presence of four generations. We also comment on the potential implication of the recent observation of a Higgs-like new particle at the LHC.
In recent years, an ever-increasing collection of measurements have been performed and produced data which support the inference that dark matter exists in our Universe. They include the observations of velocities of various astronomical objects and the detailed mapping of the cosmic microwave background radiation . In spite of all this evidence, the identity of the basic constituents of most dark matter has so far remained a mystery, as they are not of any known type of matter. Nevertheless, there are some basic properties that candidates for dark matter need to possess. They must be stable on cosmological time scales, interact very weakly with electromagnetic radiation, and have the right relic density. Furthermore, analyses of structure formation in the Universe suggest that dark matter consists mainly of cold (i.e., nonrelativistic) particles  (for reviews on the nature of, and search strategies for, dark matter, see also [2–4]).
Among the considerable variety of dark matter (DM) candidates, the most popular at present are the so-called weakly interacting massive particles (WIMPs). While the standard model (SM) does contribute weakly interacting stable particles in the form of neutrinos, their being very light precludes them from being abundant enough to be the dominant component of the observed relic density. Many models for new physics have been proposed that contain suitable WIMP candidates, including supersymmetry with -parity, universal extra dimensions with Kaluza-Klein parity, and little Higgs models with -parity. Alternatively, it is possible that the DM candidate naturally yields the correct relic density, but does not have a weak-scale mass or weak interactions. Such a WIMP-less possibility can occur in models which possess sequestered (hidden) sectors with conserved quantum numbers.
In this paper, we will give an of overview of some scenarios for DM in conjunction with heavy chiral quarks and leptons, as well as their respective motivations, cosmology, and collider phenomenology. The considered scenarios are (1)a sequential fourth generation with a stable heavy neutrino, (2)a sequential fourth generation with stable heavy quarks, (3)heavy chiral quarks acting as mediators between the SM sector and a hidden sector, and (4)a sequential fourth generation plus the simplest DM candidate.
We will here briefly describe the models, before continuing to give a more in-depth survey of their properties in the following sections.
The first scenario involves a sequential fourth generation with a neutrino that is heavy and stable. This possibility is natural, as it builds on the existing SM structure, and also fairly economical in that it retains neutrinos as the only source of weakly interacting stable matter in the universe. To guarantee the stability of the heavy neutrino, one may introduce a symmetry under which the neutrino is odd, whereas the SM particles are even, and which may originate from an extra gauge group spontaneously broken at some high scale [5, 6]. If the couplings of the fourth neutrino to the boson are comparable to those of the light neutrinos, the fourth neutrino can make up at most a few tenths of the observed DM abundance and moreover direct searches for DM impose severe constraints [7–10]. However, if the fourth neutrino is mostly right-handed, it may get around these restrictions and saturate the relic density .
The second scenario again involves a sequential fourth generation, but with DM that is predominantly due to a (quasi-)stable heavy anti-up-type quark [12–14]. These stable antiquarks form baryons with charge −2, which are captured by immediately after nucleosynthesis. The resulting “atoms” play the role of DM in structure formation and other observables.
The third scenario is inspired by so-called WIMPless models, where DM resides in a sequestered (hidden) sector [15–19]. In such models, any interactions with the SM sector must come about due to mediators, particles charged under both the hidden and SM sectors. An interesting possibility is that these mediators carry the SM quantum numbers of a pair of chiral quarks, as well as some hidden-sector quantum number(s). Such quark mediators would give rise to sufficient cross-section for DM detection in direct search experiments as well as abundant production at the LHC.
Finally, in the fourth scenario, the SM with four sequential generations (SM4) is slightly expanded by incorporating a real gauge-singlet scalar field which acts as the WIMP candidate . This is the most economical extension of the SM4 with WIMP DM in the case of all the fourth-generation fermions being unstable. Its minimality is reflected in the small number of parameters in its DM sector, which makes it highly testable with recent and ongoing experiments.
The rest of the paper is organized as follows. Section 2 gives details on the scenarios, including their motivation, and cosmological and astrophysical phenomenology. In Section 3, we present the collider phenomenology of the different scenarios. We discuss in Section 4 some of the possible impacts of the DM under consideration on Higgs searches in the SM4. We also comment on the potential implication of the recent observation at the LHC of a new particle compatible with the Higgs boson in the three-generation case (SM3). We finally discuss similarities and differences of the models and present our conclusions in Section 5.
2. Cosmology and Dark Matter Detection
The four scenarios presented here, despite the common features of dark matter and heavy chiral fermions, all have quite different motivation and phenomenology. We will therefore present the models in four separate subsections and will defer the discussion on similarities and differences to Section 5.
2.1. Scenario 1: A Stable Heavy Neutrino
In the presence of the fourth generation, it is natural and economical to regard its neutral member as a potential WIMP candidate. The lower limit, at 95% confidence level (CL), on the mass of a stable fourth-generation neutrino with SM coupling strength is 45.0 (39.5) GeV if it is a Dirac (Majorana) fermion . (In the Majorana case, if the fourth neutrino is the lighter member of a pair of Majorana neutrino eigenstates with masses originating from both Dirac and Majorana contributions, the lower limit can be relaxed to 33.5 GeV .) As it turns out, such a neutrino cannot be a primary candidate for DM because its annihilation cross-section is generally large and leads to relic abundance that is too small to account for the observed DM density . Moreover, constraints from experiments looking directly for DM interacting with nuclei rule out the fourth-generation neutrino with SM couplings as the leading component of the DM in our galactic halo. Specifically, for a stable fourth-generation Dirac neutrino dominating the halo DM, the spin-independent cross-section of the neutrino elastically scattering off a nucleus is much higher than the upper bounds from the direct searches, which excludes masses up to the TeV level. In the Majorana neutrino case, the spin-dependent cross-section is also too large over a comparable, but smaller, mass range. For a heavier neutrino, the cross-sections may agree with the data, but in the higher-mass region perturbative unitarity may be violated . These restrictions can be lessened if the stable heavy neutrino is not assumed to saturate the local halo DM.
It is instructive to review the situation in the context of a specific example in light of recent results from the Higgs and DM direct searches. We adopt the model of  in which the four generations of fermions are sequential with respect to the SM gauge group and a right-handed neutrino state is added to each generation. The neutrino DM is made stable by a symmetry which arises naturally after the spontaneous breaking of an extra Abelian gauge group, . All the quarks and leptons carry charges, and , respectively, for , but the Higgs doublet does not. These charges are chosen to be and , with . One can deduce from these charge assignments that flavor-changing neutral currents at tree level and gauge anomalies are absent. The model also contains extra scalar fields and , which are singlets under the SM gauge group and carry the charges and , respectively. Accordingly, the mass-generating terms for the neutrinos can be expressed as where are summed over, represents the Higgs (left-handed lepton) doublet, and denotes the charge conjugate of the right-handed neutrino . Thus when the vacuum expectation values (VEVs) of become nonzero, , they break , causing the associated gauge boson to get mass given by , and simultaneously the right-handed neutrino fields gain Majorana mass terms. It follows that, after electroweak symmetry breaking, each generation ends up with two Majorana mass eigenstates. Those in the fourth generation are denoted here by and , with masses satisfying and the DM candidate being lighter also than the fourth-generation charged lepton.
The relic density of is related to the cross-section at freeze-out of annihilation into all possible SM4 final states. Assuming that , one calculates the contributions of diagrams mediated by the Higgs or boson in the channel and by or the fourth charged-lepton in the channel. In Figure 1 we display the resulting ratio , where is the observed total DM density , for various values of and the - mixing angle , as the couplings to the Higgs, , and bosons depend on , which varies from 0 to . In the numerical work, is set to unity, the mass to GeV, consistent with constraints from electroweak precision data [22, 23], and the Higgs mass to GeV, outside the 120–600 GeV zone excluded by LHC data at 95% CL [24, 25]. Hence in this model the stable fourth-generation neutrino can constitute up to about half of the total DM density. However, restraints from direct searches for DM may reduce this fraction significantly.
Since can only contribute to a fraction of the observed relic density, it is reasonable to expect that also contributes to a fraction, , of the local halo DM density, . This implies that the spin-independent and spin-dependent cross-sections and , respectively, of elastically scattering off a nucleon need to be rescaled as for comparison with experiment. Under the assumption that the local density of is proportional to its cosmic density, , we show in Figure 2 the predictions of for various values of and . These graphs illustrate how the parameters of this model may affect its predictions which can be probed by ongoing and future DM direct detection experiments. Given the formidable challenges in observing neutral stable particles at the LHC, the DM direct searches may have an edge in the quest for fourth-generation neutrino DM due to its potentially sizable couplings to and .
We turn now to another model which, like the first one, has four sequential generations with right-handed neutrinos and an extra Abelian gauge group, . However, the fermions have charge assignments under this new gauge group that are different from those in the first model. As proposed in , their charges are , , and . This implies that the charge operator of is , where and represent the baryon and fourth-generation lepton numbers, respectively. Another difference lies in the scalar sector which contains, besides the Higgs doublet , one SM-singlet scalar field and one Higgs triplet , both of which carry the charge and couple to the fourth-generation leptons, but not to the other fermions, giving rise to a fourth-generation neutrino mass matrix of the form  where are Yukawa couplings and denote the VEVs of , , and , respectively. By requiring that , one can ensure that the lighter Majorana mass eigenstate, , is mostly right-handed, while the heavier one is predominantly left-handed. In that case, the couplings of to the Higgs and bosons become suppressed, allowing to overcome the obstacles faced by in the previous model.
More specifically, the charge assignments above imply that in the limit has only an axial-vector coupling to the boson which in turn has only vectorial couplings to the quarks. As a consequence, the cross-sections of the -nucleon scattering vanish, thereby automatically satisfying the direct search bounds. On the other hand, the annihilation cross-section is nonzero and can yield relic density of the right amount, especially if the mass is not far from the resonance region, . This is depicted for a couple of examples in Figure 3, where is the coupling constant. Thus this model provides a stable fourth-generation neutrino that can be a good DM candidate. Although the boson is leptophobic with respect to the leptons of the first 3 generations, its couplings to the quarks and fourth-generation charged lepton may allow it to be detectable at colliders.
2.2. Scenario 2: A Stable Heavy Quark
Another possibility is that all members of the fourth generation carry some new, unbroken charge. This can be realized, for example, in grand unified theories with the unification group . In this case, the new heavy quarks can only decay through GUT-scale operators to the lightest member of the fourth generation, typically the neutrino. The lightest of these quasi-stable quarks can easily have a lifetime longer than that of the universe [12–14].
If the heavy quarks receive a baryon asymmetry leaving a predominance of up-type antiquarks , during the cooling of the universe, these antiquarks will mainly form antibaryons (due to strong chromo-Coulomb forces) with charge . Immediately after nucleosynthesis, these negatively charged baryons will bind to nuclei to form , also called “O-helium” or OHe. The resulting OHe atoms act as DM for the remainder of the lifetime of the universe. Due to their short-range nuclear interactions, this DM behaves as slightly “warm” in structure formation.
O-helium has some special implications. One is in nucleosynthesis, where the baryons can act as catalysts for the generation of in the merging of a and a nucleus, as well as for the production of heavier nuclei. Furthermore, the Earth is opaque to O-Helium, which would be slowed down in the Earth’s crust and, through gravitational interactions, sink down to the Earth’s core. Some of the O-helium would be destroyed in reactions, with baryons forming bound states with other nuclei. Such anomalous isotopes could in principle be detected, although the prevalence should be below present experimental limits.
In underground direct detection experiments, the O-helium would be very difficult to detect since it is slowed down by the passage through matter and would release a minimal energy transfer of order eV. Therefore, direct production of pairs in colliders would be the main way to detect this scenario, see further Section 3.2.
2.3. Scenario 3: Mediator Heavy Quarks
A notable property of DM inferred from observations is the so-called “WIMP miracle”, that is, that the observed DM abundance can be explained by a new particle with weak-scale mass and weak-scale interaction cross-section. This observation was taken up in WIMPless models [15–19], where the DM resides in a hidden sector, which receives mass through the same mechanism as the SM sector (such as gauge-mediated supersymmetry breaking) in such a way that the ratio of the mass scale to gauge structure constant is the same as in the SM. This hidden-sector DM will then automatically have a relic density of the correct order of magnitude, independently of the DM mass. The stability of the DM particles is naturally explained by their carrying some unbroken gauge quantum number or a symmetry, forbidding decays into lighter SM particles. The precise cosmology of the model depends on whether the DM experiences long-range interactions through an unbroken symmetry (“self-interacting dark matter”, see [26–28]) or not.
This hidden sector DM can either interact with the SM only through the high-energy supersymmetry breaking mechanism, in which case discovery in direct or indirect detection experiments would be impossible, or through some mediator particles, carrying both hidden-sector and visible-sector quantum numbers. A tantalizing possibility is that the DM is a real scalar particle that couples to the SM sector through heavy chiral quarks (or, to be precise, mirror quarks, since their chirality is opposite to that of the SM quarks) through Yukawa terms
In order to avoid any flavor constraints, we assume the usual Yukawa hierarchy for coupling to the SM generations, giving dominant coupling of the new quarks to 3rd-generation SM quarks. The original motivation for these model choices  was that in this scenario, with a DM mass in the range 1–10 GeV, , and GeV, the model could explain the anomalies reported by the DAMA  and CoGeNT  experiments, while staying marginally consistent with the stringent constraints from other DM detection experiments, see Figure 4.
However, the general scenario, with DM which couples to the SM through heavy (chiral or vector-like) quarks that are charged under a new symmetry and decay to the DM and 3rd-generation quarks, is recovered in many models. Examples include “asymmetric dark matter” models , little Higgs models with unbroken -parity , and extra-dimensional models [34, 35]. These models have identical collider signatures, and they can all be explored at the LHC [36, 37], as detailed in Section 3.3.
2.4. Scenario 4: SM4 with Minimal Dark Matter
If the fourth-generation fermions are all unstable, it will be necessary to invoke extra particles in order to account for the observed DM relic density. The simplest possibility along this line is the SM4+D, which is the SM with four sequential generations slightly expanded with the addition of a real scalar field acting as the WIMP candidate . The stability of , sometimes dubbed darkon, is ensured by requiring it to be a singlet under the SM gauge group and introducing a discrete symmetry, under which is odd, while the SM particles are even. The renormalizable Lagrangian of the darkon has the form where , , and are free parameters and is the Higgs doublet containing the physical Higgs field . This Lagrangian is the same as that in the three-generation case, the SM3+D, which has been much studied in the literature [38–56], but the presence of the fourth generation gives rise to potentially detectable processes which are absent or suppressed in the SM3+D case, as will be discussed later. Clearly the DM sector of SM4+D has a small number of free parameters, only two of which are relevant here: the Higgs-darkon coupling and the darkon mass , where is the Higgs VEV.
Since the term in (4) leads to the darkon relic density, can be extracted from the observed DM density once the darkon and Higgs masses, and , are specified. With determined, one can then predict the cross-section of a darkon elastically scattering off a nucleon. Based on the calculations of [20, 56] with the fourth-generation fermion masses adopted therein, we display in Figure 5 the results for GeV and some illustrative values of . The band widths in Figure 5(a) corresponds to the 90%-CL range of the observed DM density , whereas those in Figure 5(b) reflect mainly the substantial uncertainty of the Higgs-nucleon coupling .
Also shown in Figure 5(b) are data on the spin-independent cross-section of WIMP-nucleon interactions from the leading direct-detection experiments. Evidently the potential WIMP signals measured by DAMA, CoGeNT, and CRESST-II are at odds with the upper bounds reported by CDMS, XENON10, and XENON100. Since the null results of the latter for WIMP masses GeV have been seriously disputed in the literature [58–62], pending a general consensus on this puzzle we will here regard it as an open question and consequently assume that the range 2.5–15 GeV is still viable. (In the SM4+D, most of the GeV region is disallowed by restrictions from the data on a number of kaon and -meson rare decays with missing energy .) It is then interesting to observe that the predictions in Figure 5(b) overlap well with the signal cross-sections suggested by CoGeNT and CRESST-II for this mass range. Thus darkon masses from 15 to ~80 GeV are ruled out by the direct search limits, as the black-dotted portions of the curves in Figure 5(b) indicate. In contrast, most of the GeV region is not yet subject to the existing direct-search bounds, but will be within reach of future searches such as XENON1T. Before moving on, we remark that there is a fresh update on the XENON100 limit , which roughly amounts to lowering the XENON100 curve in Figure 5(b) by up to almost a factor of four.
3. Collider Phenomenology
Detecting stable weakly-interacting neutral particles at a hadron collider is extremely difficult. Typically, the only prompt production mechanisms are through off-shell bosons, on- or off-shell Higgs bosons, or through new heavy gauge bosons . These all have quite low production cross-sections, and the signal, which in all cases consists of missing transverse energy, , recoiling against hadron jets (or possibly other recoils such as photons or weak bosons) all suffer from very large SM backgrounds, including and plus jets, top pair production, and QCD multijet production with missing energy due to mismeasurement and/or heavy flavor decays. (See however  for a model-independent study using effective 4-fermion operators comparing the reach for Majorana fermion DM detection at the Tevatron and the LHC to direct detection experiments, where collider experiments are found to increase the detection reach significantly for several operator types, in particular for very low mass DM. Their study might be directly relevant for scenario 1, and, indirectly, for scenario 4.)
The only hope for distinguishing and identifying the production of DM is therefore usually through the decay of heavier particles, which are either more readily produced or have more easily distinguishable decay modes, such as high-momentum isolated leptons and/or jets. With a significant mass difference between the decaying particle and its decay products (including the DM), the amount of missing can also be increased without requiring recoil against high- initial state radiation (jets or photons).
This type of signatures are by necessity model-dependent, and therefore help distinguish the type of DM scenario. In the following, we will survey the expected collider signatures of the four scenarios of DM and heavy chiral fermions. We leave the comparison and discussion about the possibility to distinguish the scenarios for the concluding section.
3.1. Scenario 1: A Stable Heavy Neutrino
In scenarios with a stable fourth-generation neutrino, the viable collider signatures depend on the details of the model. In the models discussed in Section 2.1, the fourth-generation neutrino is stabilized by a new symmetry which is broken at or above the TeV scale. Furthermore, the fourth-generation neutrino has both Majorana and Dirac mass terms, generating mixing between the left- and right-handed neutrinos, with possibly both mass eigenstates light enough to be within reach of the LHC.
The first model discussed in Section 2.1 (see ) has a mass matrix in the basis of . This means that the lightest neutrino state is predominantly left-handed, with a sizable coupling to the SM boson.
In , the collider phenomenology of a corresponding scenario was analyzed, where the fourth-generation Majorana neutrino states and have comparable masses, and decays as , where indicates an on- or off-shell SM boson. Parts of the and mass plane can in this case be excluded already by existing squark searches at LEP 2. The squark signal considered in the LEP search was , and the search excluded squark masses up to the kinematic limit of LEP 2. The corresponding signal of jets plus missing energy would be generated also by fourth-generation neutrino pair production, , with at least one of and being the heavier neutrino. The resulting exclusion region is given in Figure 6(a).
Turning to the LHC, the cross-section for pair production is far too small to give a distinguishable missing signal at the LHC, but there is an interesting possibility: where indicates on- or off-shell bosons. The production mechanism is assumed to be through an -channel SM boson. The resulting signal is four isolated leptons and missing transverse energy. While this signal is suppressed by the branching ratio into four leptons and the efficiency for detecting four isolated leptons, on the other hand, it is practically background free. In Figure 6(b), cross-section limits in the plane is shown for 30 fb−1 integrated luminosity at the LHC.
In the second model (that of ), the inclusion of the scalar triplet with a nonvanishing VEV renders the lighter fourth-generation neutrino predominantly right-handed. In this case, the coupling of the lighter neutrino to the boson vanishes, which allows the neutrino, on one hand, to have sufficient relic density to make up virtually all the DM and, on the other hand, to escape the DM direct detection bounds. In the model studied in , the mixing between the heavier and lighter fourth-generation neutrinos is furthermore strongly suppressed. As is shown in Figure 3, however, an acceptable relic density requires the mass of the associated to be close to twice the mass of .
This couples to a current, and therefore has a coupling to SM quarks, but not to leptons of the first three generations. The standard dilepton decay channel is therefore closed. Possible detection channels could instead be either diquark (or ) decay, or decay of the to fourth-generation charged leptons . As seen in Figure 7, the present searches in the dijet channel at the LHC do not yet constrain this model.
3.2. Scenario 2: A Stable Heavy Quark
In the model of composite DM consisting of baryons of a stable heavy chiral antiquark combining with Helium nuclei to form O-helium, what would be produced at a hadron collider is pairs. The production cross-section for these pairs is identical to that of regular fourth-generation quarks, and the difference in phenomenology comes solely from the fact that they do not decay, but instead hadronize with light quarks and antiquarks into -baryons and -mesons and then traverse the detector . The phenomenology of these -baryons and -mesons is identical to that of -hadrons [66, 67], in particular hadrons formed with a stable top squark and SM light quarks. The interactions of such heavy hadrons with matter has been thoroughly investigated using GEANT . Note that the difference in spin between stop-hadrons and -hadrons has no impact on the collider phenomenology, which is completely determined by the interaction of the light quarks with the matter of the detector. In this sense, the only function of the spectator heavy constituent is to give mass and momentum to the heavy hadrons.
While the heavy quarks immediately after production hadronize mainly into heavy mesons / and and , while traversing the detector they frequently interact with the nuclear matter. It is kinematically advantageous for a meson to exchange baryon number in the collision, emitting a pion. Therefore, nearly 100% of the mesons transform during their passage through the detector into charge-1 baryons, which is the lightest baryonic state. This means that in a significant fraction of the events, the hadron changes charge from the neutral to the positive (see Figure 8). mesons on the other hand cannot form antibaryons through interactions with the detector material. They can however still change charge (between and 0) through exchange of and quarks.
This gives rise to interesting signals of a slow-moving positively charged particle (the baryon) seen in the muon detector, often with no corresponding track in the inner tracker, together with either (i)a negatively charged inner track with minimal energy deposit in the calorimeters and possibly no corresponding negative track in the muon chamber (due to exchange in the calorimeter), or (ii)a negatively charged track in the muon chambers but no corresponding track in the inner tracker, or (iii)simply missing transverse momentum and no additional tracks on the opposite side of the detector.
Some experimental searches have been done for stable heavy hadrons in particular as well as heavy stable charged particles in general, both at the Tevatron and the LHC [69–72]. If in the future a signal would be seen, it would be necessary to experimentally cover a significant range of charge exchange combinations to fully determine the properties of the heavy stable particle and distinguish different scenarios.
3.3. Scenario 3: Mediator Heavy Quarks
In this scenario, scalar DM particles couple to the SM sector through heavy quarks carrying both SM and dark quantum numbers (due to either a continuous or a discrete symmetry). In order to avoid flavor constraints, these exotic heavy quarks are assumed to couple preferentially to 3rd-generation quarks. The new quarks can then be pair produced at hadron colliders through standard QCD interactions, and then decay to DM and 3rd-generation quarks. The production of new quarks with up-type quantum numbers ( quarks), decaying to scalar DM particles and (possibly off-shell) SM top quarks, was studied in , while the production of decays of heavy down-type quarks , decaying to DM and quarks, was studied in .
Both studies used MadGraph/MadEvent 4  interfaced to Pythia 6.4  and PGS 4  for the simulation of both signals and backgrounds, and investigate the exclusion and discovery potential, at the Tevatron and the LHC, for the parameter plane. The authors optimized the exclusion and discovery reach for each parameter point, using different cut combinations for a number of different signatures.
For production with decay , there are several channels corresponding to the different decays of the top and anti-top quarks: all-hadronic (when both the top and anti-top decay to quarks), semileptonic (when one of the top or anti-top decays to a charged lepton and a neutrino), and doubly leptonic (when both the top and anti-top decay to charged leptons). These channels have quite different background and signal efficiencies and were therefore studied separately. In both cases (as for all signals with large missing transverse energy), the dominant backgrounds are top pair production, + jets production, and (for the all-hadronic case) + jets production.
Contrary to what one might expect, the best limits (and best discovery reach) for production are obtained, not from the semileptonic channel, but from the all-hadronic channel. The reason is that the main backgrounds, semileptonic and + jets, both have a lepton in the final state, while the all-hadronic decay has no missing energy at parton level. Therefore, a large missing cut, large cut on transverse hadronic energy , and a lepton veto combine to efficiently suppress the backgrounds. Furthermore, the all-hadronic mode has larger branching ratio, and does not suffer from the relatively low efficiencies in detecting an isolated lepton. The additional + jets background is not large enough to considerably modify this picture. In order to optimize the exclusion and discovery reach, the cuts on missing , , and number of jets were chosen to maximize the signal significance point-by-point in the parameter space.
Something worth special mentioning in the scenario is the case in which the mass of the is very close to . In this case, the momentum of the particle from the decay and the decay tend to be back-to-back, since the particle is produced nearly at rest in the and rest frames. Therefore, the amount of missing energy is reduced in this region, leading to a considerably worse exclusion reach. However, once , the decay is effectively a 3-body decay , and the phase space for the particle again opens up. This effect is clearly seen in the exclusion regions for production at a 10 TeV LHC run, see Figure 9.
The expected exclusion reach for 300 pb−1 at a 10 TeV LHC run was found to extend beyond 600 GeV mass for GeV, with a maximum reach in at around 220 GeV (for between 430 and 520 GeV), and the maximum evidence reach going up to at 480 GeV for GeV. These numbers roughly correspond to the exclusion and evidence reaches at 1 fb−1 at the 7 TeV LHC run.
For production with decay to , there is only one search channel, -tagged jet(s) associated with large missing transverse energy. Also here, the cuts were optimized point by point in the parameter plane by choosing between a number of cuts on the hardest jet, missing , and summed hadronic and missing transverse momentum . The 7 TeV LHC exclusion limits are shown in Figure 10. The larger mass difference between the produced and the decay products translate larger missing and a significantly better reach in compared to production, while the reach in is comparable to that for for a corresponding integrated luminosity.
3.4. Scenario 4: SM4 with Minimal Dark Matter
The existence of the fourth-generation quarks can offer potentially important means to probe the DM sector of the SM4+D which are lacking or unavailable in the SM3+D. In the SM3 the flavor-changing neutral current (FCNC) top-quark decay is known to have a tiny branching ratio, between and [79–84], but in the SM4 the new quarks can induce an enhancement factor of several orders of magnitude [85, 86]. In the SM4+D the related decay with a darkon pair in the final state, , if kinematically allowed, can be similarly enhanced and therefore may be detectable at the LHC. The analogous processes involving the fourth-generation quarks, and , may also be observable. These decays could, in principle, probe darkon masses all the way up to half the mass difference between the initial and final quarks, , hence covering potentially broader ranges than those covered by some of the DM direct searches in the future.
Some numerical results for these FCNC processes involving the darkon have been obtained in . With GeV and fourth-generation quark masses of order 500 GeV, assuming that the mode dominates the Higgs width leads to the branching ratio . Since estimates suggest that needs to be at least several times in order to be detectable [83, 84], then may be unfeasible to measure. In contrast, its and counterparts are more promising, yielding , , , and . Since and decays with branching ratios between and are expected to be within LHC reach [85, 86], we may expect that these and decays would also be detectable at the LHC despite their final states involving missing energy. Once they are seen, comparing the data with those from DM direct searches could provide further consistency tests for the darkon model.
4. Implications for Higgs Searches
A Higgs boson which has couplings to a pair of dark matter particles can decay into the latter if kinematically allowed. Such a mode will enlarge the rate of its invisible decay, suppressing the Higgs production cross-section into other decay modes and hence its detectability. In this section, we discuss some more details about the effect of dark matter on the Higgs sector in two of the scenarios treated above. We also touch on the implication of the information gained from the recent discovery of a Higgs-like particle at the LHC.
4.1. Stable Heavy Neutrino
If the fourth-generation neutrinos are long-lived or stable and couple nonnegligibly to the Higgs, it may have a significant invisible decay channel into the neutrinos, depending on the Higgs mass [8, 87–89]. This can happen in the first model considered in Section 2.1 in which the stable fourth-generation neutrino is a predominantly left-handed Majorana fermion and has a coupling to the Higgs roughly proportional to the mass . In contrast, the second model discussed in Section 2.1 contains a stable fourth-generation neutrino that is a predominantly right-handed Majorana fermion and has negligible couplings to the Higgs .
To illustrate how large this invisible mode can modify the Higgs branching ratios in the first model, we display in Figure 11 two examples from  for two sets of the masses of and its heavier partner , which are related to their mixing angle by . Evidently tends to be substantial and can approach unity, especially for before the opening of the important channels. One can infer from the bottom plot and Figure 1 that for GeV and the viable range –50 GeV the Higgs can be hidden from view. Since Figure 1 was based on assuming that the local density of is proportional to its cosmic density and on limits from recent DM direct searches, we should note that a different assumption and more stringent data from future searches may yield a different conclusion.
It is worth remarking that for the dominance of the decay into fourth-generation neutrinos will generally persist if there is another Higgs doublet in the scalar sector . Yet the expanded parameter space in that case can accommodate the appearance of a Higgs with SM3-like characteristics.
4.2. SM4 with Minimal Dark Matter
In the SM4+D case, with all the fourth-generation fermions being unstable, the opening of the invisible channel can drastically decrease the Higgs’ visibility [20, 56]. Some examples of this can be seen in Figure 12(a), drawn with the same values of Higgs-darkon coupling and their masses as in Figure 5(a). Like the preceding scenario, the darkon effect is most striking for .
Since the darkon has no gauge interactions and no mixing with the Higgs, in the SM4+D the rates of Higgs decays into visible particles are essentially the same as in the SM4 alone. Therefore their branching ratios in the SM4+D are all subject to the same reduction factor [55, 56] , where is the Higgs width in the SM4 without the darkon. In Figure 12(b) we graph for the same choices as in Figure 12(a). These graphs show that the visible branching ratios can be suppressed by up to 3 orders of magnitude. For , although the SM4 with fourth-generation quark masses of hundreds of GeV predicts Higgs production cross-sections amplified by up to 9 times due to the enlarged coupling , the enhancement would not sufficiently ameliorate the effect of the reduction factor in the SM4+D with GeV, causing the Higgs’ to be highly invisible. On the other hand, for the Higgs is mostly visible and for its decay pattern is no different from that in the SM4.
4.3. Impact of Higgs-Like Boson Discovery
The recent observation at the LHC [92, 93] of a new resonance at ~125-126 GeV, with cross-sections and branching ratios consistent with those of the SM3 Higgs boson, supported by the latest findings from Higgs searches at the Tevatron , has spelled major trouble for the simplest version of the SM with four generations [95–98]. In particular, the large rate of is difficult to accommodate in the SM4 with a minimal Higgs sector. However, the data acquired so far still offer room for the possibility that the discovered particle is some nonstandard boson [99–101]. In the presence of a chiral fourth-generation, specifically, it turns out that one could expand the minimal SM4 with the appropriate extra particles in order to reproduce the current data well. This can be achieved, for instance, by adding another Higgs doublet [90, 102–108]. Such extended four-generation models may also include DM candidates, with phenomenology identical to the scenarios described in the previous sections. These scenarios are therefore still viable in general, once an extended Higgs sector is considered.
5. Summary and Discussion
In this paper, we have discussed some representative scenarios for dark matter in association with a fourth generation of chiral matter. In the first two scenarios, the DM is due to particles within the fourth generation itself (the fourth-generation neutrino and the up-type fourth-generation quark, respectively). This is a minimal solution in the sense that the motivation for the fourth-generation particles can be taken to be DM itself. However, some additional physics is needed to stabilize the DM candidate, typically a new symmetry with its associated gauge boson .
Whereas the detection of direct generation of a stable heavy neutrino at the LHC might be very challenging, one discovery route might be through the decay of the boson and possibly also through the production of heavier fourth-generation charged leptons which decay to the stable neutrino. A parallel detection route, if the stable neutrino has a significant left-handed component, is direct detection. In this case, if the fourth-generation neutrino has a nonnegligible contribution to the DM in our galactic halo, detection should be within reach for the next generation of experiments.
In the case of a stable heavy quark, direct detection of the DM particles is nearly impossible due to the large cross-section of the -Helium composites with terrestrial matter, slowing down the DM particles far below the necessary momentum transfer. However, if the mass of the stable quark is within reach for the LHC, the collider signature would be quite spectacular—massive, slow, highly ionizing particles which change charge as they pass through the detector.
In the third scenario, the DM resides in a hidden sector, and the role of the fourth-generation quarks is to act as mediators between the hidden sector and the visible sector. The quarks are therefore charged under both the hidden-sector and visible-sector gauge groups, and therefore must decay to SM quarks and DM. Comparing to sequential fourth-generation scenarios, due to the new conserved quantum number of these exotic quarks, we do not have any of the regular CKM-inspired decays such as , , and so forth. We focused on the situation where the new quarks couple predominantly to the third generation. The signatures for this scenario are quite similar to those of supersymmetric stop and sbottom production with decay to the lightest neutralino and SM quarks, but the production cross-section is an order of magnitude larger for the same mass, and there are no additional leptonic signatures from new charged electroweak states such as charginos and sleptons (apart from possible decays or if the mass difference between and is larger than the mass).
Lastly, the fourth scenario is that of a sequential fourth generation with the addition of a neutral real scalar singlet, the darkon, coupling only to the SM Higgs field. In this scenario, the decays and other properties of the fourth-generation fermions are unchanged, and the only possibility to produce the darkon is through an (on- or off-shell) Higgs particle. This would therefore (together with scenario 1 of a stable fourth-generation neutrino) be the most difficult scenario to discover (or exclude) at the LHC. However, due to the small number of parameters of the model, most of the parameter space of this scenario can be tested at future direct detection experiments.
The recent discovery of a new resonance compatible with the SM3 Higgs boson seems difficult to accommodate within a fourth-generation scenario with a minimal Higgs sector. Nevertheless, present experimental as well as theoretical uncertainties still allow chiral fourth-generation models beyond the simplest versions, with or without DM, to survive. The viability of such extended models will likely be determined by measurements in the near future.
Finally, it is interesting to note the wide span of collider signatures associated with the scenarios treated in this paper, making them excellent benchmarks for LHC studies. Such benchmark studies, if presented in a model-independent way, can easily be reinterpreted to encompass also other models involving DM and new heavy states.
This work was supported in part by the NSC and NCTS of ROC and the NCU Plan to Develop First-Class Universities and Top-Level Research Centers. J. Alwall is supported by NTU Grant no. 10R1004022.
- J. Beringer, J. F. Arguin, R. M. Barnett, et al., “Review of particle physic,” Physical Review, vol. 86, 2012.
- G. Bertone, D. Hooper, and J. Silk, “Particle dark matter: evidence, candidates and constraints,” Physics Reports, vol. 405, no. 5-6, pp. 279–390, 2005.
- D. Hooper and E. A. Baltz, “Strategies for determining the nature of dark matter,” Annual Review of Nuclear and Particle Science, vol. 58, pp. 293–314, 2008.
- J. L. Feng, “Dark matter candidates from particle physics and methods of detection,” Annual Review of Astronomy and Astrophysics, vol. 48, pp. 495–545, 2010.
- L. M. Krauss and F. Wilczek, “Discrete gauge symmetry in continuum theories,” Physical Review Letters, vol. 62, no. 11, pp. 1221–1223, 1989.
- B. Batell, “Dark discrete gauge symmetries,” Physical Review D, vol. 83, no. 3, 12 pages, 2011.
- G. Jungman, M. Kamionkowski, and K. Griest, “Supersymmetric dark matter,” Physics Report, vol. 267, no. 5-6, pp. 195–373, 1996.
- W. Y. Keung and P. Schwaller, “Long lived fourth generation and the Higgs,” Journal of High Energy Physics, vol. 2011, no. 54, 19 pages, 2011.
- D. Borah, “Abelian extension of standard model with four generations,” Physical Review D, vol. 85, no. 1, 6 pages, 2012.
- Y. F. Zhou, “Probing the fourth generation Majorana neutrino dark matter,” Physical Review D, vol. 85, no. 5, 10 pages, 2012.
- H. S. Lee, Z. Liu, and A. Soni, “Neutrino dark matter candidate in fourth generation scenarios,” Physics Letters B, vol. 704, no. 1-2, pp. 30–35, 2011.
- K. Belotsky, D. Fargion, M. Y. Khlopov, et al., “May Heavy hadrons of the 4th generation be hidden in our Universe while close to detection?” http://arxiv.org/abs/hep-ph/0411271.
- M. Y. Khlopov, “Composite dark matter from 4th generation,” Pis'ma v Zhurnal Eksperimental'noi i Teoreticheskoi Fiziki, vol. 83, p. 3, 2006.
- M. Y. Khlopov, “Physics of dark matter in the light of dark atoms,” Modern Physics Letters A, vol. 26, no. 38, 2011.
- J. L. Feng and J. Kumar, “Dark-matter particles without weak-scale masses or weak interactions,” Physical Review Letters, vol. 101, no. 23, 4 pages, 2008.
- K. Fukushima, J. Kumar, and P. Sandick, “Detection prospects for Majorana fermion WIMPless dark matter,” Physical Review, vol. 84, no. 1, 9 pages, 2011.
- J. L. Feng and Y. Shadmi, “WIMPless dark matter from non-Abelian hidden sectors with anomaly-mediated supersymmetry breaking,” Physical Review D, vol. 83, no. 9, Article ID 095011, 2011.
- J. L. Feng, V. Rentala, and Z. Surujon, “WIMPless dark matter in anomaly-mediated supersymmetry breaking with Hidden QED,” Physical Review D, vol. 84, no. 9, Article ID 095033, 2011.
- J. L. Feng, V. Rentala, and Z. Surujon, “WIMPless dark matter from an anomaly-mediated supersymmetry breaking hidden sector with no new mass parameters,” Physical Review, vol. 85, no. 5, Article ID 055003, 2012.
- X. G. He, S. Y. Ho, J. Tandean, and H. C. Tsai, “Scalar dark matter and standard model with four generations,” Physical Review, vol. 82, 3, Article ID 035016, 11 pages, 2010.
- L. M. Carpenter, “Fourth generation lepton sectors with stable majorana neutrinos: from LEP to LHC,” http://arxiv.org/abs/1010.5502.
- G. D. Kribs, T. Plehn, M. Spannowsky, and T. M. P. Tait, “Four generations and Higgs physics,” Physical Review D, vol. 76, no. 7, Article ID 075016, 11 pages, 2007.
- O. Eberhardt, A. Lenz, and J. Rohrwild, “Less space for a new family of fermions,” Physical Review D, vol. 82, no. 9, Article ID 095006, 20 pages, 2010.
- The ATLAS collaboration, “Update of the combination of Higgs Boson searches in pp collisions at sqrt(s) = 7 TeV with the ATLAS experiment at the LHC,” ATLAS-CONF 2011-135, 2011.
- CMS Collaboration, “SM Higgs combination,” CMS-PAS-HIG 11-011, 2011.
- D. N. Spergel and P. J. Steinhardt, “Observational evidence for self-interacting cold dark matter,” Physical Review Letters, vol. 84, no. 17, p. 3760, 2000.
- R. Dave, D. N. Spergel, P. J. Steinhardt, and B. D. Wandelt, “Halo properties in cosmological simulations of self-interacting cold dark matter,” The Astrophysical Journal, vol. 547, no. 2, 2001.
- C. Kouvaris, “Limits on self-interacting dark matter from neutron stars,” Physical Review Letters, vol. 108, no. 19, Article ID 191301, 2012.
- J.L. Feng, J. Kumar, and L.E. Strigari, “Explaining the DAMA signal with WIMPless dark matter,” Physics Letters B, vol. 670, no. 1, pp. 37–40, 2008.
- R. Bernabei, P. Belli, F. Cappella, et al., “New results from DAMA/LIBRA,” The European Physical Journal C, vol. 67, no. 1-2, pp. 39–49, 2010.
- C. E. Aalseth, P. S. Barbeau, N. S. Bowden, et al., “Results from a search for light-mass dark matter with a p-type point contact germanium detector,” Physical Review Letters, vol. 106, Article ID 131301, 2011.
- B. Dutta and J. Kumar, “Asymmetric dark matter from hidden sector baryogenesis,” Physics Letters B, vol. 699, no. 5, pp. 364–367, 2011.
- H. C. Cheng and I. Low, “Little hierarchy, little higgses, and a little symmetry,” Journal of High Energy Physics, vol. 408, Article ID 061, 2004.
- G. Servant and T. M. P. Tait, “Is the lightest kaluza-klein particle a viable dark matter candidate?” Nuclear Physics B, vol. 650, no. 1-2, pp. 391–419, 2003.
- H. C. Cheng, J. L. Feng, and K. T. Matchev, “Kaluza-Klein Dark Matter,” Physical Review Letters, vol. 89, no. 21, Article ID 211301, 2002.
- J. Alwall, J. L. Feng, J. Kumar, and S. Su, “Dark matter-motivated searches for exotic fourth-generation mirror quarks in tevatron and early LHC data,” Physical Review D, vol. 81, no. 11, Article ID 114027, 2010.
- J. Alwall, J. L. Feng, J. Kumar, and S. Su, “B's with direct decays: Tevatron and LHC discovery prospects in the bb+E/T channel,” Physical Review D, vol. 84, Article ID 074010, 2011.
- V. Silveira and A. Zee, “Scalar Phantoms,” Physics Letters B, vol. 161, no. 1–3, pp. 136–140, 1985.
- J. McDonald, “Gauge singlet scalars as cold dark matter,” Physical Review D, vol. 50, no. 6, pp. 3637–3649, 1994.
- H. Davoudiasl, R. Kitano, T. Li, and H. Murayama, “The new minimal standard model,” Physics Letters B, vol. 609, no. 1-2, pp. 117–123, 2005.
- X. G. He, T. Li, X. Q. Li, and H. C. Tsai, “Scalar dark matter effects in Higgs and top quark decays,” Modern Physics Letters A, vol. 22, pp. 2121–2129, 2007.
- V. Barger, P. Langacker, M. McCaskey, M. J. Ramsey-Musolf, and G. Shaughnessy, “CERN LHC phenomenology of an extended standard model with a real scalar singlet,” Physical Review D, vol. 77, no. 3, Article ID 035005, 2008.
- S. Andreas, T. Hambye, and M. H. G. Tytgat, “WIMP dark matter, Higgs exchange and DAMA,” Journal of Cosmology and Astroparticle Physics, vol. 0810, Article ID 034, 2008.
- X. G. He, T. Li, X. Q. Li, J. Tandean, and H. C. Tsai, “Constraints on scalar dark matter from direct experimental searches,” Physical Review D, vol. 79, no. 2, Article ID 023521, 2009.
- X. G. He, T. Li, X. Q. Li, J. Tandean, and H.-C. Tsai, “The simplest dark-matter model, CDMS II results, and Higgs detection at LHC,” Physics Letters B, vol. 688, no. 4-5, pp. 332–336, 2010.
- S. Andreas, C. Arina, T. Hambye, F. S. Ling, and M. H. G. Tytgat, “Light scalar WIMP through the Higgs portal and CoGeNT,” Physical Review D, vol. 82, no. 4, Article ID 043522, 2010.
- W. L. Guo and Y. L. Wu, “The real singlet scalar dark matter model,” Journal of High Energy Physics, vol. 2010, Article ID 083, 2010.
- K. Ghosh, B. Mukhopadhyaya, and U. Sarkar, “Signals of an invisibly decaying Higgs in a scalar dark matter scenario: a study for the large hadron collider,” Physical Review D, vol. 84, no. 1, Article ID 015017, 2011.
- Y. Mambrini, “Higgs searches and singlet scalar dark matter: combined constraints from XENON 100 and the LHC,” Physical Review D, vol. 84, no. 11, Article ID 115017, 2011.
- M. Raidal and A. Strumia, “Hints for a non-standard Higgs boson from the LHC,” Physical Review D, vol. 84, no. 7, Article ID 077701, 2011.
- O. Lebedev, H. M. Lee, and Y. Mambrini, “Vector Higgs portal dark matter and the invisible Higgs,” Physics Letters B, vol. 707, no. 5, pp. 570–576, 2012.
- A. Djouadi, O. Lebedev, Y. Mambrini, and J. Quevillon, “Implications of LHC searches for Higgs-portal dark matter,” Physics Letters B, vol. 709, no. 1-2, pp. 65–69, 2012.
- M. Kadastik, K. Kannike, A. Racioppi, and M. Raidal, “Implications of the 125 GeV Higgs boson for scalar dark matter and for the CMSSM phenomenology,” Journal of High Energy Physics, vol. 1205, Article ID 061, 2012.
- X. G. He, B. Ren, and J. Tandean, “Hints of standard model Higgs boson at the LHC and light dark matter searches,” Physical Review D, vol. 85, no. 9, Article ID 093019, 2012.
- C. P. Burgess, M. Pospelov, and T. ter Veldhuis, “The minimal model of nonbaryonic dark matter: a singlet scalar,” Nuclear Physics B, vol. 619, no. 1–3, pp. 709–728, 2001.
- X. G. He and J. Tandean, “Hidden Higgs boson at the LHC and light dark matter searches,” Physical Review D, vol. 84, no. 7, Article ID 075018, 2011.
- E. Komatsu, K. M. Smith, J. Dunkley, et al., “Seven-yearwilkinson microwave anisotropy probe(wmap*) observations: cosmological interpretation,” The Astrophysical Journal, vol. 192, no. 2, p. 18, 2011.
- D. Hooper, J. I. Collar, J. Hall, D. McKinsey, and C. Kelso, “Consistent dark matter interpretation for CoGeNT and DAMA/LIBRA,” Physical Review D, vol. 82, no. 12, Article ID 123509, 2010.
- J. I. Collar, “A comparison between the low-energy spectra from CoGeNT and CDMS,” http://arxiv.org/abs/1103.3481.
- J. I. Collar, “A realistic assessment of the sensitivity of XENON10 and XENON100 to light-mass WIMPs,” http://arxiv.org/abs/1106.0653.
- J. I. Collar, “Comments on ‘final analysis and results of the phase II SIMPLE dark matter search’,” http://arxiv.org/abs/1106.3559.
- G. B. Gelmini, “Direct dark matter searches: Fits to WIMP candidates,” http://arxiv.org/abs/1106.3559.
- E. Aprile, M. Alfonsi, K. Arisaka, et al., “Dark matter results from 225 live days of XENON100 data,” Physical Review Letters, vol. 109, no. 18, 6 pages, 2012.
- J. Goodman, M. Ibe, A. Rajaraman, W. Shepherd, T.M.P. Tait, and H. B. Yu, “Constraints on light Majorana dark matter from colliders,” Physics Letters B, vol. 695, no. 1–4, pp. 185–188, 2011.
- K. M. Belostky, M. Y. Khlopov, and K. I. Shibaev, “Accelerator probes for new stable quarks,” arxiv.org/abs/1111.3578.
- A. C. Kraan, “Interactions of heavy stable hadronizing particles,” The European Physical Journal, vol. 37, pp. 91–104, 2004.
- R. Mackeprang and A. Rizzi, “Interactions of coloured heavy stable particles in matter,” The European Physical Journal C, vol. 50, no. 2, pp. 353–362, 2007.
- R. Mackeprang and D. Milstead, “An updated description of heavy-hadron interactions in Geant-4,” The European Physical Journal C, vol. 66, no. 3-4, pp. 493–501, 2010.
- V. M. Abazov, B. Abbott, M. Abolins, et al., “Search for long-lived charged massive particles with the D0 detector,” Physical Review Letters, vol. 102, no. 16, Article ID 161802, 2009.
- T. Aaltonen, J. Adelman, T. Akimoto, et al., “Search for long-lived massive charged particles in 1.96 TeV collisions,” Physical Review Letters, vol. 103, no. 2, Article ID 021802, 2009.
- C. M. S. Collaboration, “Search for heavy stable charged particles in pp collisions at sqrt(s)=7 TeV,” Journal of High Energy Physics, vol. 3, p. 24, 2011.
- G. Aad, B. Abbott, J. Abdallah, et al., “Search for stable hadronising squarks and gluinos with the ATLAS experiment at the LHC,” Physics Letters B, vol. 701, no. 1, pp. 1–19, 2011.
- J. Alwall, P. Demin, S. de Visscher, et al., “MadGraph/MadEvent v4: the new web generation,” Journal of High Energy Physics, vol. 2007, Article ID 028, 2007.
- T. Sjostrand, S. Mrenna, and P. Z. Skands, “PYTHIA 6.4 physics and manual,” Journal of High Energy Physics, vol. 0605, Article ID 026, 2006.
- PGS—Pretty Good Simulator, http://www.physics.ucdavis.edu/~conway/research/software/pgs/pgs4-general.htm.
- T. Aaltonen, B. A. Gonzalez, S. Amerio, et al., “Search for new T′ particles in final states with large jet multiplicities and missing transverse energy in ppbar collisions at sqrt(s) = 1.96 TeV,” Physical Review Letters, vol. 107, Article ID 191803, 2011.
- T. Aaltonen, B. Á. Gonzalez, S. Amerio, et al., “Search for production of heavy particles decaying to top quarks and invisible particles in collisions at TeV,” Physical Review Letters, vol. 106, no. 19, Article ID 191801, 2011.
- G. Aad, B. Abbott, J. Abdallah, et al., “Search for new phenomena in ttbar events with large missing transverse momentum in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector,” Physical Review Letters, vol. 108, no. 4, Article ID 041805, 2012.
- G. Eilam, J. L. Hewett, and A. Soni, “Rare decays of the top quark in the standard and two Higgs doublet models,” Physical Review D, vol. 44, no. 5, Article ID 1473, 1991.
- G. Eilam, J. L. Hewett, and A. Soni, “Erratum: rare decays of the top quark in the standard and two-Higgs-doublet models,” Physical Review D, vol. 59, no. 3, Article ID 039901, 1998.
- J. L. Hewett, T. Takeuchi, and S. D. Thomas, “Indirect probes of new physics,” http://arxiv.org/abs/hep-ph/9603391.
- B. Mele, S. Petrarca, and A. Soddu, “A new evaluation of the t→cH decay width in the standard model,” Physics Letters B, vol. 435, no. 3-4, pp. 401–406, 1998.
- J. A. Aguilar-Saavedra and G. C. Branco, “Probing top flavour-changing neutral scalar couplings at the CERN LHC,” Physics Letters B, vol. 495, no. 3-4, pp. 347–356, 2000.
- J. A. Aguilar-Saavedra, “Top flavour-changing neutral interactions: theoretical expectations and experimental detection,” Acta Physica Polonica B, vol. 35, pp. 2695–2710, 2004.
- G. Eilam, B. Melic, and J. Trampetic, “CP violation and the 4th generation,” Physical Review D, vol. 80, Article ID 116003, 2009.
- A. Arhrib and W. S. Hou, “Flavor changing neutral currents involving heavy quarks with four generations,” Journal of High Energy Physics, vol. 0607, Article ID 009, 2006.
- K. Belotsky, D. Fargion, M. Khlopov, R. Konoplich, and K. Shibaev, “Invisible Higgs boson decay into massive neutrinos of fourth generation,” Physical Review D, vol. 68, no. 5, Article ID 054027, 2003.
- A. N. Rozanov and M. I. Vysotsky, “Tevatron constraints on the Higgs boson mass in the fourth-generation fermion models revisited,” Physics Letters B, vol. 700, no. 5, pp. 313–315, 2011.
- S. A. Cetin, T. Cuhadar-Donszelmann, M. Sahin, S. Sultansoy, and G. Unel, “Impact of the relatively light fourth family neutrino on the Higgs boson search,” Physics Letters B, vol. 710, no. 2, pp. 328–331, 2012.
- N. Chen and H. J. He, “LHC signatures of two-Higgs-doublets with fourth family,” Journal of High Energy Physics, vol. 1204, Article ID 062, 2012.
- Q. Li, M. Spira, J. Gao, and C. S. Li, “Higgs boson production via gluon fusion in the standard model with four generations,” Physical Review D, vol. 83, no. 9, Article ID 094018, 2011.
- G. Aad, T. Abajyan, and B. Abbott, “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, no. 1, pp. 1–29, 2012.
- S. Chatrchyan, V. Khachatryan, A. M. Sirunyan, and A. Tumasyan, “Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC,” Physics Letters B, vol. 716, no. 1, pp. 30–61, 2012.
- T. Aaltonen, V. M. Abazov, B. Abbott, et al., “Evidence for a particle produced in association with weak bosons and decaying to a bottom-antibottom quark pair in Higgs boson searches at the Tevatron,” Physical Review Letters, vol. 109, no. 7, 12 pages, 2012.
- A. Djouadi and A. Lenz, “Sealing the fate of a fourth generation of fermions,” http://arxiv.org/abs/1204.1252.
- E. Kuflik, Y. Nir, and T. Volansky, “Implications of Higgs searches on the four generation standard model,” http://arxiv.org/abs/1204.1975.
- M. Buchkremer, J.M. Gerard, and F. Maltoni, “Closing in on a perturbative fourth generation,” Journal of High Energy Physics, vol. 1206, Article ID 135, 2012.
- O. Eberhardt, A. Lenz, A. Menzel, U. Nierste, and M. Wiebusch, “Status of the fourth fermion generation before ICHEP2012: higgs data and electroweak precision observables,” Physical Review D, vol. 86, no. 7, 5 pages, 2012.
- I. Low, J. Lykken, and G. Shaughnessy, “Have we observed the Higgs (imposter)?” http://arxiv.org/abs/1207.1093.
- P.P. Giardino, K. Kannike, M. Raidal, and A. Strumia, “Is the resonance at 125 GeV the Higgs boson?” http://arxiv.org/abs/1207.1347.
- D. Elander and M. Piai, “The decay constant of the holographic techni-dilaton and the 125 GeV boson,” http://arxiv.org/abs/1208.0546.
- X. G. He and G. Valencia, “An extended scalar sector to address the tension between a fourth generation and Higgs searches at the LHC,” Physics Letters B, vol. 707, no. 3-4, pp. 381–384, 2011.
- M. Geller, S. Bar-Shalom, and G. Eilam, “The need for new search strategies for fourth generation quarks at the LHC,” Physics Letters B, vol. 715, no. 1–3, 2012.
- K. Kumar, R. Vega-Morales, and F. Yu, “Effects from new colored states and the Higgs portal on gluon fusion and Higgs boson decays,” http://arxiv.org/abs/1205.4244.
- L. Bellantoni, J. Erler, J. J. Heckman, and E. Ramirez-Homs, “Masses of a fourth generation with two Higgs doublets,” Physical Review D, vol. 86, no. 3, Article ID 034022, 2012.
- H. S. Lee and A. Soni, “Fourth generation parity,” http://arxiv.org/abs/1206.6110.
- E. Osoba, “Fourth generations with an inert doublet Higgs,” http://arxiv.org/abs/1206.6912.
- S. Bar-Shalom, M. Geller, S. Nandi, and A. Soni, “Two Higgs doublets, a 4th generation and a 125 GeV Higgs: a review,” http://arxiv.org/abs/1208.3195.
- Z. Ahmed, D. S. Akerib, A. Arrenberg, et al., “The CDMS II Collaboration. Dark matter search results from the CDMS II experiment,” Science, vol. 327, pp. 1619–1621, 2010.
- E. Aprile, K. Arisaka, F. Arneodo, et al., “Dark matter results from 100 live days of XENON100 data,” Physical Review Letters, vol. 107, no. 13, Article ID 131302, 2011.
- H. S. Lee, H. C. Bhang, J. H. Choi, et al., “Limits on interactions between weakly interacting massive particles and nucleons obtained with CsI(Tl) crystal detectors,” Physical Review Letters, vol. 99, no. 9, Article ID 091301, 2007.
- D. S. Akerib, M. S. Armel-Funkhouser, M. J. Attisha, et al., “Limits on spin-dependent WIMP-nucleon interactions from the cryogenic dark matter search,” Physical Review D, vol. 73, no. 1, Article ID 011102, 2006.
- J. Angle, E. Aprile, F. Arneodo, et al., “Limits on spin-dependent WIMP-nucleon cross sections from the XENON10 experiment,” Physical Review Letters, vol. 101, no. 9, Article ID 091301, 2008.
- D. S. Akerib, M. J. Attisha, and L. Baudis, “Low-threshold analysis of CDMS shallow-site data,” Physical Review D, vol. 82, no. 12, Article ID 122004, 2010.
- Z. Ahmed, D. S. Akerib, S. Arrenberg, et al., “Results from a low-energy analysis of the CDMS II germanium data,” Physical Review Letters, vol. 106, no. 13, Article ID 131302, 2011.
- J. Angle, E. Aprile, F. Arneodo, et al., “Search for light dark matter in XENON10 data,” Physical Review Letters, vol. 107, no. 5, Article ID 051301, 2011.
- C. Savage, G. Gelmini, P. Gondolo, and K. Freese, “Compatibility of DAMA/LIBRA dark matter detection with other searches,” Journal of Cosmology and Astroparticle Physics, vol. 0904, Article ID 010, 2009.
- G. Angloher, M. Bauer, I. Bavykina, et al., “Results from 730 kg days of the CRESST-II Dark Matter search,” The European Physical Journal C, vol. 72, no. 1971, 2012.
- E. Aprile, “The XENON1T dark matter search experiment,” http://arxiv.org/abs/1206.6288.