Search for doubly-charged Higgs bosons in like-sign dilepton final states at sqrt(s) = 7 TeV with the ATLAS detector

A search for doubly-charged Higgs bosons decaying to pairs of electrons and/or muons is presented. The search is performed using a data sample corresponding to an integrated luminosity of 4.7 fb-1 of pp collisions at sqrt(s) = 7 TeV collected by the ATLAS detector at the LHC. Pairs of prompt, isolated, high-pT leptons with the same electric charge (ee, emu, mumu) are selected, and their invariant mass distribution is searched for a narrow resonance. No significant excess over Standard Model background expectations is observed, and limits are placed on the cross section times branching ratio for pair production of doubly-charged Higgs bosons. The masses of doubly-charged Higgs bosons are constrained depending on the branching ratio into these leptonic final states. Assuming pair production, coupling to left-handed fermions, and a branching ratio of 100% for each final state, masses below 409 GeV, 375 GeV, and 398 GeV are excluded for ee, emu, mumu, respectively.

Eur. Phys. J. C manuscript No. Abstract A search for doubly-charged Higgs bosons decaying to pairs of electrons and/or muons is presented. The search is performed using a data sample corresponding to an integrated luminosity of 4.7 fb −1 of pp collisions at √ s = 7 TeV collected by the ATLAS detector at the LHC. Pairs of prompt, isolated, high-p T leptons with the same electric charge (e ± e ± , e ± µ ± , µ ± µ ± ) are selected, and their invariant mass distribution is searched for a narrow resonance. No significant excess over Standard Model background expectations is observed, and limits are placed on the cross section times branching ratio for pair production of doublycharged Higgs bosons. The masses of doubly-charged Higgs bosons are constrained depending on the branching ratio into these leptonic final states. Assuming pair production, coupling to left-handed fermions, and a branching ratio of 100% for each final state, masses below 409 GeV, 375 GeV, and 398 GeV are excluded for e ± e ± , e ± µ ± , and µ ± µ ± , respectively.
Several extensions of the Standard Model (SM) predict the existence of doubly-charged Higgs bosons (H ±± ) as part of an extended Higgs sector where a triplet of Higgs bosons is present [1][2][3][4]. In addition to the neutral Higgs boson, charged and doubly-charged Higgs bosons are part of this triplet. The origin of neutrino masses and mixing can be attributed to this triplet, which can couple to Higgs and lepton doublets. Dirac neutrino mass terms are generated via the Yukawa couplings of the left-handed leptons to the Higgs triplet. This is commonly known as the "type II seesaw" mechanism [5][6][7][8]. A H ±± -like particle can also occur as a singlet as proposed in the Zee-Babu model [9][10][11], where it is postulated for the purpose of generating Majorana neutrino masses.
The main production mechanisms of H ±± bosons at hadron colliders are pair production via an s-channel Zboson or photon exchange and associated production with a H ± boson via a W -boson exchange. The latter process de-pends on the mass of the H ± boson, which is generally unknown, and is not considered here. Doubly-charged Higgs bosons can couple to either left-handed or right-handed fermions. In left-right symmetric models [12][13][14][15] [16].
The H ±± boson may decay to a pair of like-sign leptons whose invariant mass is consistent with the mass of the H ±± boson, denoted m(H ±± ). The partial decay width to leptons is given by where k = 2 if both leptons have the same flavour ( = ) and k = 1 if they have a different flavour. The factor h is the coupling parameter. Only prompt decays of the H ±± boson (cτ < 10 µm) are considered in this letter, corresponding to h > 3 × 10 −6 for m(H ±± ) > 50 GeV. Direct searches for H ±± have been performed by experiments at the LEP, HERA, Tevatron, and LHC colliders [17][18][19]. The mass limits obtained for the H ±± bosons depend on the branching ratio (BR) assumed. The most stringent limits were set by the CMS Collaboration [19], excluding at 95% confidence level (CL) masses below 382 GeV, 391 GeV, and 395 GeV for e ± e ± , µ ± µ ± , and e ± µ ± final states, respectively, assuming left-handed couplings and a 100% branching ratio to each final state. Low-energy constraints exist on the product of some of the coupling parameters. The 90% CL upper limit on the muon decay branching ratio BR(µ + → e + e − e + ) < 1.0×10 −12 provides the tightest constraint, h ee h eµ /m(H ±± ) 2 < 4.7 × 10 −11 GeV −2 [20], but the individual couplings are not constrained. More details on constraints from non-collider experiments can be found in Ref. [21]. This letter presents a search for a H ±± boson decaying to pairs of electrons and/or muons with the same electric charge (H ±± → e ± e ± , H ±± → µ ± µ ± , and H ±± → e ± µ ± ). The search is performed using a data sample corresponding to 4.7 ± 0.2 fb −1 [22,23] of integrated luminosity (L ) collected by the ATLAS detector [24]. The event selection and background estimates follow those used by the inclusive search for anomalous production of like-sign leptons described in Ref. [25] and are summarized only briefly here.
Events are collected using single-lepton triggers with transverse momentum (p T ) thresholds of 18 GeV for muons and either 20 GeV or 22 GeV for electrons, depending on the running period. To ensure no efficiency loss for electrons with very high p T , a trigger with a threshold of 45 GeV and looser requirements for the electron identification is also used. Electrons are identified as showers in the electromagnetic calorimeter matched to a track in the inner detector using the tight criteria described in Ref. [26]. Muons are reconstructed from combined tracks in the inner tracking system and the muon detector [24]. Leptons must have a transverse momentum above 20 GeV, be in the angular range covered by the inner tracking system, be well isolated, and have impact parameters consistent with originating from the primary event vertex. In pairs where the higher-p T lepton is an electron, it is required to have p T > 25 GeV. All pairs of electrons or muons with the same electric charge are considered, so more than one lepton pair may be reconstructed per event. The invariant mass of the lepton pair must be larger than 15 GeV, and for e ± e ± the region close to the Z-boson mass (70 GeV < m(e ± e ± ) < 110 GeV) is excluded due to a large background from Z → e + e − events with an electron charge misidentification, as described below.
SM backgrounds in this search are divided into three categories: prompt, non-prompt, and conversion sources. The dominant source of prompt like-sign lepton pairs is W Z production, and smaller sources include ZZ, like-sign WW , ttW , and ttZ production. The expected prompt background contribution is derived from MC simulation normalised to cross-section calculations performed at next-to-leading order in the strong coupling constant. The background due to non-prompt leptons comes primarily from semileptonic band c-hadron decays for muons, while for electrons, an additional background comes from charged pions that shower early in the calorimeter and neutral pions decaying to two photons, where one of the photons converts to an e + e − pair. This background is derived by extrapolating from data regions where one or both leptons fail part of the selection criteria. The extrapolation factors are derived in events dominated by non-prompt leptons and are dependent on the p T and pseudorapidity (η) of the leptons. The origin of the background due to photon conversions, important for the electron channels, includes W γ and Zγ production and cases where one of the electrons in an e + e − pair is reconstructed with the wrong charge (electron charge flip) after radiating a photon that subsequently converts. The background from conversions is derived using MC simulation, where the electron charge-flip rate has been corrected based on comparison between data and simulation for Z → ee events. The chargeflip background due to the finite curvature resolution is small compared to that from conversion sources.
Several control regions are selected to validate the background estimates. In all cases, the dilepton mass spectrum observed in data agrees with the background prediction within the systematic uncertainties [25].
The H ±± process is simulated using PYTHIA8 [27] to estimate the acceptance and efficiency for reconstructing H ±± bosons with masses between 50 GeV and 1000 GeV. The kinematic properties of H ±± L and H ±± R bosons are identical; only their cross sections differ. Windows in the reconstructed dilepton mass are defined to ensure optimal signal sensitivity across the full mass range. In each window, the number of observed events is compared to the expected background and signal yields to derive a limit on the signal contribution. The expected observable width of the H ±± resonance is dominated by detector resolution effects. The detector resolution of the momentum measurement is roughly 1.2-1.8% for high-p T electrons, depending on η, and for muons ranges from about 2% for p T = 20 GeV to 10% for p T = 1 TeV. For the e ± e ± final state, lepton pairs with a mass within ±4% of the tested mass value are selected. For µ ± µ ± and e ± µ ± , the window size is ±(6 + 0.007 × m(H ±± )/GeV)% around the tested mass to account for the coarser resolution. With the selection described above, the acceptance times efficiency to reconstruct a H ±± boson in these mass windows is about 27% for e ± e ± , 36% for e ± µ ± , and 43% for µ ± µ ± for m(H ±± ) = 100 GeV. For m(H ±± ) = 400 GeV it is about 50% for all three final states.
Among the dominant systematic uncertainties on the background yields are the ±12% uncertainties on the W Z and ZZ cross sections. The cross-section uncertainties on the ttW , ttZ, and like-sign WW processes are ±50%, but the contribution from these backgrounds is small. The nonprompt and conversion background uncertainties are also significant: at low mass, they are about ±40% and stem mainly from the uncertainty in the extrapolation factor used for the non-prompt estimate and uncertainty in the rate of photon-to-electron conversions. At higher mass, the uncertainties on all backgrounds are dominated by the limited size of MC or data samples used in their estimates. Smaller uncertainties arise from the lepton identification, isolation, and trigger efficiencies, which also apply to the H ±± signal acceptance. For the signal, an additional uncertainty of ±1.6% is estimated from the parton distribution functions by using the uncertainties provided by the MSTW 2008 90% CL set [28] added in quadrature to the difference between the central value of this set and the CTEQ6L PDF set.
The dilepton mass distribution observed in data is shown for the e ± e ± , µ ± µ ± , and e ± µ ± channels in Fig. 1 and is compared to the background expectation and four hypothetical H ±± signals normalised to their respective cross sections (assuming a branching ratio to the given lepton flavour of 100%). The data show no clear peak structure and agree well with the background estimate in all three channels.
A limit on the number of lepton pairs originating from H ±± bosons (N rec ) in each mass window is derived using a CLs technique [29]. It is converted to a limit on the cross section times branching ratio for doubly-charged Higgs production using the acceptance times efficiency values derived from MC simulation. Since this analysis counts lepton pairs and each event contains two H ±± bosons, the cross section times branching ratio for pair production is given by where A × ε is the acceptance times efficiency to detect a lepton pair from H ±± decay within a given mass window.
The integrated luminosity L is 4.7 fb −1 . The 95% CL expected and observed upper limits on the cross section times branching ratio as a function of the H ±± boson mass are shown in Fig. 2. The expected limit is determined as the median outcome of simulated pseudoexperiments in the absence of any signal. Also shown are the theoretical cross sections calculated at next-to-leading order (NLO) for H ±± production with left-and right-handed couplings [16]. The uncertainty on these cross sections is ±10% due to scale dependence in the NLO calculation, parton distribution function uncertainties, and neglecting higher-order electroweak corrections.
At low mass, the expected cross-section limits are most stringent for the µ ± µ ± channel due to the low background levels in this channel. At high mass, the expected e ± e ± and µ ± µ ± limits are comparable while the e ± µ ± limit is about 30% worse due to the larger background from W Z production. In general the observed and expected limits agree well with each other. The largest deviations of the observed limit from the expected limit are within the 2σ uncertainty on the expected limit. The cross-section limits range from 25 fb (in the e ± e ± channel at low mass) to 0.6 fb (in all channels at high mass).
Comparison of the cross-section limits with the theoretical production cross section places constraints on m(H ±± ). The lower limits on the H ±± mass at 95% CL are listed in Table 1 for the three final states when BR(H ±± → ± ± ) = 100%, as well as branching ratios of 33%, 22%, and 11%. For a democratic scenario where the BR to each pair of lepton flavours is the same, the branching ratio is 22% for the Observed 95% CL upper limit Expected 95% CL upper limit  Fig. 2 Upper limit at 95% CL on the cross section times branching ratio for pair production of H ±± bosons decaying to (a) e ± e ± , (b) µ ± µ ± , and (c) e ± µ ± pairs. The observed and median expected limits are shown along with the 1σ and 2σ variations in the expected limits. In the range 70 < m(H ±± ) < 110 GeV, no limit is set in the e ± e ± channel. Also shown are the theoretical predictions at next-to-leading order for the pp → H ±± H ∓∓ cross section for H ±± L and H ±± R bosons. The variation from bin to bin in the expected limits is due to fluctuations in the background yields derived from small MC samples. Table 1 Lower mass limits at 95% CL on H ±± bosons decaying to e ± e ± , µ ± µ ± , or e ± µ ± pairs. Mass limits are derived assuming branching ratios to a given decay mode of 100%, 33%, 22%, or 11%. Both expected and observed limits are given.
exp e ± e ± and µ ± µ ± final states and 11% for the e ± µ ± final state. In addition, the same mass limits can be placed on the singlet H ±± in the Zee-Babu model as its production cross sections and decay kinematics are the same as for H ±± L . Figure 3 shows the mass limits as a function of the branching ratio into each of the three final states.
In conclusion, a search for doubly-charged Higgs bosons decaying to e ± e ± , e ± µ ± , or µ ± µ ± has been performed by searching for a narrow resonance peak in the dilepton mass distribution. No such peak was observed in a data sample corresponding to an integrated luminosity of 4.7 fb −1 of pp collisions at √ s = 7 TeV recorded by the ATLAS detector at the LHC in 2011. Cross-section limits between 17 fb and 0.6 fb are set depending on the mass of the H ±± boson and the final state. Assuming pair production, couplings to lefthanded fermions, and a branching ratio of 100% for each final state, masses below 409 GeV, 398 GeV, and 375 GeV are excluded at 95% CL for e ± e ± , µ ± µ ± , and e ± µ ± final states, respectively. Lower mass limits are also set for scenarios with right-handed couplings or smaller branching ratios. The limits on H ±± L bosons also apply to the singlet in the Zee-Babu model.  Fig. 3 The mass limits as a function of the branching ratio for the H ±± decaying to e ± e ± , e ± µ ± , and µ ± µ ± for (a) H ±±