Search for supersymmetry at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}=13$$\end{document}s=13 TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector

A search for strongly produced supersymmetric particles is conducted using signatures involving multiple energetic jets and either two isolated leptons (e or \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mu $$\end{document}μ) with the same electric charge or at least three isolated leptons. The search also utilises b-tagged jets, missing transverse momentum and other observables to extend its sensitivity. The analysis uses a data sample of proton–proton collisions at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s}= 13$$\end{document}s=13 TeV recorded with the ATLAS detector at the Large Hadron Collider in 2015 corresponding to a total integrated luminosity of 3.2 fb\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$^{-1}$$\end{document}-1. No significant excess over the Standard Model expectation is observed. The results are interpreted in several simplified supersymmetric models and extend the exclusion limits from previous searches. In the context of exclusive production and simplified decay modes, gluino masses are excluded at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$95\,\%$$\end{document}95% confidence level up to 1.1–1.3 TeV for light neutralinos (depending on the decay channel), and bottom squark masses are also excluded up to 540 GeV. In the former scenarios, neutralino masses are also excluded up to 550–850 GeV for gluino masses around 1 TeV.


Introduction
Supersymmetry (SUSY) [1][2][3][4][5][6] is one of the most studied frameworks to extend the Standard Model (SM) beyond the electroweak scale; a general review can be found in Ref. [7]. In its minimal realisation (MSSM) [8,9] it predicts a new bosonic (fermionic) partner for each fundamental SM fermion (boson), as well as an additional Higgs doublet. If Rparity is conserved [10] the lightest supersymmetric particle (LSP) is stable and is typically the lightest neutralino 1χ 0 1 . Only such scenarios are considered in this paper. In many models, the LSP can be a viable dark matter candidate [11,12] and produce collider signatures with large missing transverse momentum. e-mail: atlas.publications@cern.ch In order to address the SM hierarchy problem with SUSY models [13][14][15][16], TeV-scale masses are required [17,18] for the partners of the gluons (gluinosg) and of the top quark chiral degrees of freedom (top squarkst L andt R ), due to the large top Yukawa coupling. The latter also favours significantt L -t R mixing, so that the lighter mass eigenstatet 1 is in many scenarios lighter than the other squarks [19,20]. Bottom squarks may also be light, being bound to top squarks by SU (2) L invariance. This leads to potentially large production cross-sections for gluino pairs (gg), top-antitop squark pairs (t 1t * 1 ) and bottom-antibottom squark pairs (b 1b * 1 ) at the Large Hadron Collider (LHC) [21]. Production of isolated leptons may arise in the cascade decays of those superpartners to SM quarks and neutralinosχ 0 1 , via intermediate neutralinosχ 0 2,3,4 or charginosχ ± 1,2 that in turn lead to W , Z or Higgs bosons, or to lepton superpartners (sleptons). Lighter third-generation squarks would also enhanceg → tt * 1 org → bb * 1 branching ratios over the generic decays involving light-flavour squarks, favouring the production of heavy flavour quarks and, in the case of top quarks, additional leptons. This paper presents a search for SUSY in final states with two leptons (electrons or muons) of the same electric charge (referred to as same-sign (SS) leptons) [22] or three leptons (3L) in any charge combination, jets and missing transverse momentum ( p miss T , whose magnitude is referred to as E miss T ). It is an extension to √ s = 13 TeV of an earlier search performed by ATLAS with √ s = 8 TeV data [23], and uses the data collected by the ATLAS experiment [24] in protonproton ( pp) collisions during 2015. Despite the much lower integrated luminosity collected at √ s = 13 TeV compared to that collected at √ s = 8 TeV, a similar or improved sensitivity at √ s = 13 TeV is expected due to the much larger crosssections predicted for the production of SUSY particles with 1 The SUSY partners of the Higgs and electroweak gauge bosons mix to form the mass eigenstates known as charginos (χ ± l , l = 1, 2 ordered by increasing mass) and neutralinos (χ 0 m , m = 1, . . . , 4 ordered by increasing mass). masses at the TeV scale. A similar search for SUSY in this topology was also performed by the CMS Collaboration [25] at √ s = 8 TeV. While the same-sign leptons signature is present in many scenarios of physics beyond the SM (BSM), SM processes leading to such final states have very small cross-sections. Compared to many other BSM searches, analyses based on same-sign leptons therefore allow the use of looser kinematic requirements (for example, on E miss T or the momentum of jets and leptons), preserving sensitivity to scenarios with small mass differences between gluinos/squarks and the LSP, or in which R-parity is not conserved [23].
The sensitivity to a wide range of models is illustrated by the interpretation of the results in the context of four different SUSY benchmark processes that may lead to samesign or three-lepton signatures. The first two scenarios focus on gluino pair production with generic decays into light quarks and multiple leptons, either involving light sleptons, g → qqχ 0 2 → qq ˜ * → qq + −χ 0 1 (Fig. 1a), or mediated by a cascade involvingχ ± 1 andχ 0 2 ,g → qq χ ± 1 → qq W ±χ 0 2 → qq W ± Zχ 0 1 (Fig. 1b). The other two scenarios are motivated by the expectation that the third-generation squarks are lighter than the other squarks and target the direct production ofb 1b * 1 pairs with subsequent chargino-mediated b 1 → t W −χ 0 1 decays (Fig. 1c) or the production ofgg pairs decaying asg → ttχ 0 1 via an off-shell top squark (Fig. 1d). Four signal regions (SRs) are designed to achieve good sensitivity for these SUSY scenarios, mainly characterised by the number of b-tagged jets or reconstructed leptons. They are detailed in Sect. 4, preceded by descriptions of the experimental apparatus (Sect. 2) and the simulated samples (Sect. 3). Section 5 is devoted to the estimation of the contribution from SM processes to the signal regions, validated by comparisons with data in dedicated regions. The results are presented in Sect. 6, together with the statistical tests used to interpret the results in the context of the SUSY benchmark scenarios. Finally, Sect. 7 summarises the main conclusions of this paper.

The ATLAS detector
The ATLAS experiment [24] is a multi-purpose particle detector with a forward-backward symmetric cylindrical geometry and nearly 4π coverage in solid angle. 1 The inter-1 ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point (IP) in the centre of the detector and the zaxis along the beam pipe. The x-axis points from the IP to the centre of the LHC ring, and the y-axis points upward. Cylindrical coordinates (r , φ) are used in the transverse plane, φ being the azimuthal angle around the beam pipe. The pseudorapidity is defined in terms of the polar angle θ as η = −ln tan(θ/2). Rapidity is defined as y = 0.5 ln (E + p z )/(E − p z ) where E denotes the energy and p z is the component of the momentum along the beam direction. action point is surrounded by an inner detector (ID), a calorimeter system, and a muon spectrometer.
The ID provides precision tracking of charged particles for pseudorapidities |η| < 2.5 and is surrounded by a superconducting solenoid providing a 2 T axial magnetic field. It consists of pixel and silicon-microstrip detectors inside a transition radiation tracker. One significant upgrade for the √ s = 13 TeV running period is the presence of the Insertable B-Layer [26], an additional pixel layer close to the interaction point, which provides high-resolution hits at small radius to improve the tracking performance.
The muon spectrometer consists of three large superconducting toroids with eight coils each, a system of trigger and precision-tracking chambers, which provide triggering and tracking capabilities in the ranges |η| < 2.4 and |η| < 2.7, respectively.
A two-level trigger system is used to select events. The first-level trigger is implemented in hardware and uses a subset of the detector information. This is followed by the software-based High-Level Trigger stage, which can run offline reconstruction and calibration software, reducing the event rate to about 1 kHz.

Dataset and simulated event samples
The data were collected by the ATLAS detector during 2015 with a peak instantaneous luminosity of L = 5.2 × 10 33 cm −2 s −1 , a bunch spacing of 25 ns, and a mean number of additional pp interactions per bunch crossing (pile-up) in the dataset of μ = 14. After the application of beam, detector and data quality requirements, the integrated luminosity considered in this analysis corresponds to 3.2 fb −1 with an uncertainty of ±5 %. The luminosity and its uncertainty are derived following a methodology similar to that detailed in Ref.
[27] from a preliminary calibration of the luminosity scale using a pair of x-y beam separation scans performed in August 2015.
Monte Carlo (MC) simulated event samples are used to aid in the estimation of the background from SM processes and to model the SUSY signal. The MC samples are processed through an ATLAS detector simulation [28] based on Geant4 [29] or a fast simulation using a parameterisation of the calorimeter response and Geant4 for the other parts of the detector [30] and are reconstructed in the same manner as the data. Diboson processes with four charged leptons ( ), three charged leptons and one neutrino, or two charged leptons and two neutrinos are simulated using the Sherpa v2.1.1 generator [31], and are described in detail in Ref. [32]. The matrix elements contain the doubly resonant W W , W Z and Z Z processes and all other diagrams with four or six electroweak vertices (such as same-electric-charge W boson production in association with two jets, W ± W ± j j). Fully leptonic triboson processes (W W W , W W Z, W Z Z and Z Z Z) with up to six charged leptons are also simulated using Sherpa v2.1.1 and described in Ref. [32]. The 4 and 2 +2ν processes are calculated at next-to-leading order (NLO) for up to one additional parton; final states with two and three additional partons are calculated at leading order (LO The signal SUSY processes are generated from LO matrix elements with up to two extra partons, using the Mad-Graph v2.2.3 generator interfaced to Pythia 8.186 with the A14 tune for the modelling of the SUSY decay chain, parton showering, hadronisation and the description of the underlying event. Parton luminosities are provided by the NNPDF23LO PDF set. Jet-parton matching is realised following the CKKW-L prescription [47], with a matching scale set to one quarter of the pair-produced superpartner mass. Signal cross-sections are calculated to NLO in the strong coupling constant, adding the resummation of soft gluon emission at next-to-leading-logarithmic accuracy (NLO+NLL) [48-52]. The nominal cross-section and the uncertainty are taken from an envelope of cross-section predictions using different PDF sets and factorisation and renormalisation scales, as described in Ref.

Event selection
Candidate events are required to have a reconstructed vertex [57], with at least two associated tracks with p T > 400 MeV, and the vertex with the highest sum of squared transverse momentum of the tracks is considered as primary vertex. In order to perform background estimations using data, two categories of electrons and muons are defined: "candidate" and "signal" (the latter being a subset of the "candidate" leptons satisfying tighter selection criteria).
Electron candidates are reconstructed from an isolated electromagnetic calorimeter energy deposit matched to an ID track and are required to have |η| < 2.47, a transverse momentum p T > 10 GeV, and to pass a loose likelihoodbased identification requirement [58,59]. The likelihood input variables include measurements of calorimeter shower shapes and measurements of track properties from the ID. Candidates within the transition region between the barrel and endcap electromagnetic calorimeters, 1.37 < |η| < 1.52, are removed. The track matched with the electron must have a significance of the transverse impact parameter with respect to the reconstructed primary vertex, d 0 , of Muon candidates are reconstructed in the region |η| < 2.5 from muon spectrometer tracks matching ID tracks. All muons must have p T > 10 GeV and must pass the medium identification requirements defined in Ref.
[60], based on selections on the number of hits in the different ID and muon spectrometer subsystems, and the significance of the charge to momentum ratio q/ p [60].
Jets are reconstructed with the anti-k t algorithm [61] with radius parameter R = 0.4, using three-dimensional energy clusters in the calorimeter [62] as input. All jets must have p T > 20 GeV and |η| < 2.8. Jets are calibrated as described in Ref. [63]. In order to reduce the effects of pile-up, for jets with p T < 50 GeV and |η| < 2.4 a significant fraction of the tracks associated with each jet must have an origin compatible with the primary vertex, as defined by the jet vertex tagger [64]. Furthermore, for all jets the expected average energy contribution from pile-up clusters is subtracted according to the jet area After object identification, overlaps between objects are resolved. Any jet within a distance R y = ( y) 2 + ( φ) 2 = 0.2 of an electron candidate is discarded, unless the jet has a value of the MV2c20 discriminant larger than the value corresponding to approximately an 80 % b-tagging efficiency, in which case the electron is discarded since it is likely originating from a semileptonic b-hadron decay. Any remaining electron within R y = 0.4 of a jet is discarded. Muons within R y = 0.4 of a jet are also removed. However, if the jet has fewer than three associated tracks, the muon is kept and the jet is discarded instead to avoid inefficiencies for high-energy muons undergoing significant energy loss in the calorimeter.
Signal electrons must satisfy a tight likelihood-based identification requirement [58,59] and have |η| < 2 to reduce the impact of electron charge mis-identification. Signal muons must fulfil the requirement of |d 0 |/σ (d 0 ) < 3. The track associated to the signal leptons must have a longitudinal impact parameter with respect to the reconstructed primary vertex, z 0 , satisfying |z 0 sin θ | < 0.5 mm. Isolation requirements are applied to both the signal electrons and muons. The scalar sum of the p T of tracks within a variable-size cone around the lepton, excluding its own track, must be less than 6 % of the lepton p T . The track isolation cone radius for electrons (muons) R η = ( η) 2 + ( φ) 2 is given by the smaller of R η = 10 GeV/p T and R η = 0.2 (0.3), that is, a cone of size 0.2 (0.3) at low p T but narrower for highp T leptons. In addition, in the case of electrons the energy of calorimeter energy clusters in a cone of R η = 0.2 around the electron (excluding the deposition from the electron itself) must be less than 6 % of the electron p T . Simulated events are corrected to account for minor differences in the lepton trigger, reconstruction and identification efficiencies between data and MC simulation.
The missing transverse momentum p miss T is defined as the negative vector sum of the transverse momenta of all identified physics objects (electrons, photons, muons, jets) and an additional soft term. The soft term is constructed from all tracks that are not associated with any physics object, and that are associated with the primary vertex. In this way, the E miss T is adjusted for the best calibration of the jets and the other identified physics objects above, while maintaining pile-up independence in the soft term [67,68].
Events are selected using a combination (logical OR) of dilepton and E miss T triggers, the latter being used only for events with E miss T > 250 GeV. The trigger-level requirements on E miss T and the leading and subleading lepton p T are looser than those applied offline to ensure that trigger efficiencies are constant in the relevant phase space. Events of interest are selected if they contain at least two signal leptons with p T > 20 GeV. If the event contains exactly two signal leptons, they are required to have the same electric charge.
To maximise the sensitivity in different signal models, four overlapping signal regions are defined as shown in Table 1, with requirements on the number of signal leptons (N signal lept ), the number of b-jets with p T > 20 GeV (N 20 b−jets ), the number of jets with p T > 50 GeV regardless of their flavour (N 50 jets ), E miss T and the effective mass (m eff ), defined as the scalar sum of the p T of the signal leptons and jets (regardless of their flavour) in the event plus the E miss T . Each signal region is motivated by a different SUSY scenario. The SR0b3j and SR0b5j signal regions are sensitive to gluino-mediated and directly produced squarks of the first and second generations leading to final states particularly rich in leptons (Fig. 1a) or in jets (Fig. 1b), but with no enhancement of the production of b-quarks. Third-generation squark models resulting in final states with two b-quarks, such as direct bottom squark production (Fig. 1c), are targeted by the SR1b signal region. Finally, the signal region SR3b targets gluino-mediated top squark production resulting in final states with four b-quarks (Fig. 1d).
The values of acceptance times efficiency of the SR selections for the SUSY signal models in Fig. 1 typically range between 1 and 6 % for mg = 1.2 TeV or mb 1 = 600 GeV, and a lightχ 0 1 .

Background estimation
Three main sources of SM background can be distinguished in this analysis. A first category consists of events with two same-sign prompt leptons or at least three prompt leptons, mainly from tt V and diboson processes. Other types of background events include those containing electrons with mismeasured charge, mainly from the production of top quark pairs, and those containing at least one non-prompt or fake lepton, which mainly originate from hadron decays in events containing top quarks or of W bosons in association with jets.

Background estimation methods
The estimation of the SM background processes with two same-sign prompt leptons or at least three prompt leptons is performed using the MC samples described in Sect. 3. Since diboson and tt V events are the main backgrounds in the signal regions, dedicated validation regions with an enhanced contribution from these processes are defined to verify the background predictions (see Sect. 5.3).
Background events due to charge mis-identification, dominated by electrons having emitted a hard bremsstrahlung photon which subsequently converted to an electron-positron pair, are referred to as "charge-flip". The probability of misidentifying the charge of a muon is checked in both data and MC simulation, and found to be negligible in the kinematic range relevant to this analysis. The contribution of chargeflip events is estimated using data. The electron charge-flip probability is extracted in a Z /γ * → ee data sample using a likelihood fit which takes as input the numbers of same-sign and opposite-sign electron pairs observed in the sample. The charge-flip probability is a free parameter of the fit and is extracted as a function of the electron p T and η. The event yield of this background in the signal or validation regions is obtained by applying the measured charge-flip probability to data regions with the same kinematic requirements as the signal or validation regions but with opposite-sign lepton pairs.
The contribution from fake or non-prompt (FNP) leptons (such as hadrons mis-identified as leptons, leptons originating from heavy-flavour decays, and electrons from photon conversions) is also estimated from data with a matrix method similar to that described in Ref. [23]. In this method, two types of lepton identification criteria are defined: "tight", corresponding to the signal lepton criteria described in Sect. 4, and "loose", corresponding to candidate leptons. The matrix method relates the number of events containing prompt or FNP leptons to the number of observed events with tight or loose-not-tight leptons using the probability for loose prompt or FNP leptons to satisfy the tight criteria. The probability for loose prompt leptons to satisfy the tight selection criteria is obtained using a Z /γ * → data sample and is modelled as a function of the lepton p T and η. The probability for loose FNP leptons to satisfy the tight selection criteria is determined from data in a SS control region enriched in non-prompt leptons originating from heavy-flavour decays. This region contains events with at least one b-jet, one tight muon with p T > 40 GeV (likely prompt) and an additional loose electron or muon (likely FNP). The contribution from prompt leptons and charge mis-measured electrons to this region is subtracted from the observed event yields.
The data-driven background estimates are cross-checked with an MC-based technique. In this method, the contributions from processes with FNP leptons and electron charge mis-identification are obtained from MC simulation and normalised to data in dedicated control regions at low jet multiplicity, low E miss T , and either with or without b-jets. The normalisation is performed using five multipliers: one to correct  Table 2 summarises the contributions of the different sources of systematic uncertainty in the total SM background predictions in the signal regions. The systematic uncertainties related to the same-sign prompt leptons background estimation arise from the accuracy of the theoretical and experimental modelling in the MC simulation. The primary sources of systematic uncertainties are related to the jet energy scale calibration, the jet energy resolution, b-tagging efficiency, and MC modelling and theoretical cross-section uncertainties. The cross-sections used to normalise the MC samples are varied according to the uncertainty in the cross-section calculation, that is, 6 % for diboson, 13 % for tt W and 12 % tt Z production [43]. Additional uncertainties are assigned to these backgrounds to account for the modelling of the kinematic distributions in the MC simulation. For tt W and tt Z, the predictions from the Mad-Graph and Sherpa generators are compared, leading to a ∼30 % uncertainty for these processes after the SR selections. For dibosons, uncertainties are estimated by varying the renormalisation, factorisation and resummation scales used to generate these samples, leading to a ∼30 % uncertainty for these processes after the SR selections. For tribo-son, tth, tttt and t Z production processes, which constitute a small background in all signal regions, a 50 % uncertainty on the event yields is assumed.

Systematic uncertainties on the background estimation
Uncertainties in the FNP lepton background estimate are assigned due to the limited number of data events with loose and tight leptons. In addition, systematic uncertainties of 50-60 % are assigned to the probabilities for loose FNP leptons to satisfy the tight signal criteria to account for potentially different FNP compositions (heavy flavour, light flavour or conversions) between the regions used to measure these probabilities and the SRs, as well as the contamination from prompt leptons in the former regions. This leads to overall FNP background uncertainties in the total background estimates of 18-21 % depending on the signal region.
For the charge-flip background prediction, the main uncertainties originate from the statistical uncertainty of the charge-flip probability measurements and the background contamination of the sample used to extract the charge-flip probability.

Validation of background estimates
To check the validity and robustness of the background estimates, the distributions of several discriminating variables in data are compared with the predicted background after various requirements on the number of jets and b-jets. Events are categorised based on the flavours of the selected leptons, and the different flavour channels are compared separately. Examples of such distributions are shown in Fig. 2a, c and illustrate that the predictions and data agree fairly well. The background estimates in a kinematic region close to the signal regions can also be observed in Fig. 3, which shows the The statistical uncertainties in the background prediction are included in the uncertainty band, as well as the theory uncertainties for the backgrounds with prompt SS/3L, and the full systematic uncertainties for data-driven backgrounds. The last bin includes overflows. The "Fake leptons" category corresponds to FNP leptons (see text), and the "Rare" category contains the contributions from associated production of tt with h/W W/t/tt, as well as t Z, W h, Zh, and triboson production. The lower part of the figures a-d shows the ratio of data to the background prediction for the backgrounds with prompt SS/3L, and the full systematic uncertainties for data-driven backgrounds. The "Fake leptons" category corresponds to FNP leptons (see text), and the "Rare" category contains the contributions from associated production of tt with h/W W/t/tt, as well as t Z, W h, Zh, and triboson production E miss T distributions in the signal regions before applying the E miss T requirements. Dedicated validation regions (VRs) are defined to test the estimate of the rare SM processes contributing to the signal regions, whose cross-sections have not yet been measured at √ s = 13 TeV. The corresponding selections are summarised in Table 3. In these regions, upper bounds are placed on E miss T and m eff to reduce signal contamination, and the small residual overlap with the signal regions is resolved by vetoing events that contribute to the signal regions. To further reduce contributions from electron charge mis-identification, events are also vetoed if one of the two leading leptons is an electron with |η| > 1.37, since contributions from charge-flip electrons are smaller in the central region due to the lower amount of crossed material. The purity of the targeted processes in these regions ranges from about 40 to 80 %. The VR-ttV and VR-ttZ regions overlap with each other, with 30 % of the tt V events in VR-ttV also present in VR-ttZ, and the contributions from the tt Z and tt W processes is similar in VR-ttV.
The observed yields in these validation regions, compared with the background predictions and uncertainties, can be seen in Table 4, and the effective mass distributions are shown in Fig. 2d, f. There is fair agreement between data and the estimated background for the validation regions, with the largest deviations being observed in VR-ttV with a 1.5σ deviation. Figure 3 shows the data E miss T distributions after the signal region selections (beside that on E miss T ) in data together with the expected contributions from all the SM backgrounds with their total statistical and systematic uncertainties. For illustration, a typical SUSY signal distribution corresponding to the most relevant benchmark scenario in each SR is displayed.

Results
80 < m SFOS < 100 GeV All VRs Veto events belonging to any SR, or if 1 or 2 is an electron with |η| > 1.37 (except in VR-WZ) The detailed yields for data and the different sources of SM background in the signal regions are presented in Table 5.
The uncertainties amount to 22-34 % of the total background depending on the signal region. In all four SRs the number of data events exceeds the expectation but is consistent within the uncertainties, the smallest p-value for the SM-only hypothesis being 0.04 for SR0b5j. Out of the 14 events in the SRs, 2 of the events in SR1b and the 3 events in SR0b3j contain three leptons. None of those events contain three leptons of equal charge, or are present in more than one SR. In the absence of any significant deviations from the SM predictions, upper limits on possible BSM contributions to the signal regions are computed, in particular in the context of the SUSY benchmark scenarios described in Sect. 1. The HistFitter framework [70], which utilises a profile-likelihood-ratio test [71], is used to establish 95 % confidence intervals using the CL s prescription [72]. The likelihood is built as the product of a Poisson probability density function describing the observed number of events in the signal region and Gaussian distributions constraining the nuisance parameters associated with the systematic uncertainties whose widths correspond to the sizes of these uncertainties; Poisson distributions are used instead for MC statistical uncertainties. Correlations of a given nuisance parameter across the different sources of backgrounds and the signal are taken into account when relevant. The statistical tests are performed independently for each of the signal regions. Table 6 presents 95 % confidence level (CL) modelindependent upper limits on the number of BSM events, N BSM , that may contribute to the signal regions. Normalising these by the integrated luminosity L of the data sample, they can be interpreted as upper limits on the visible BSM cross- Table 5 The number of observed data events and expected background contributions in the signal regions. The p-value of the observed events for the background-only hypothesis is denoted by p(s = 0). The "Rare" category contains the contributions from associated production of tt with h/W W/t/tt, as well as t Z, W h, Zh, and triboson production.
Background categories shown as "−" denote that they cannot contribute to a given region (charge flips or W ± W ± j j in 3-lepton regions). The individual uncertainties can be correlated and therefore do not necessarily add up in quadrature to the total systematic uncertainty section σ vis , defined as the product σ prod × A × = N BSM /L of production cross-section, acceptance and reconstruction efficiency.
Exclusion limits are also set on the masses of the superpartners involved in the four SUSY benchmark scenarios considered in this analysis. Simplified models corresponding to a single production mode and with 100 % branching ratio to a specific decay chain are used, with the masses of the SUSY particles not involved in the process set to very high values. Figure 4 shows the limits on the mass of theχ 0 1 as a function of theg orb 1 mass. In some cases, the new limits set by this analysis can be compared with the existing limits set by the combination of ATLAS SUSY searches with 8 TeV data [73,74]. For parts of the parameter space, the sensitivity reached with the 13 TeV dataset exceeds that of the 8 TeV dataset, and additional parameter space regions can be excluded, especially for large neutralino masses.

Conclusion
A search for supersymmetry in events with exactly two samesign leptons or at least three leptons, multiple jets, b-jets and E miss T is presented. The analysis is performed with protonproton collision data at √ s = 13TeV collected with the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 3.2 fb −1 . With no significant excess over the Standard Model expectation observed, results are interpreted in the framework of simplified models featuring gluino and bottom squark production. In thẽ gg simplified models considered, mg 1.