A search is presented for long-lived particles with a mass between 25 and 50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and a lifetime between 2 and 500 ps, using proton–proton collision data corresponding to an integrated luminosity of 2.0fb-1\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{fb}^{-1}$$\end{document}, collected by the LHCb detector at centre-of-mass energies of 7 and 8 TeV. The particles are assumed to be pair-produced in the decay of a 125GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} Standard-Model-like Higgs boson. The experimental signature is a single long-lived particle, identified by a displaced vertex with two associated jets. No excess above background is observed and limits are set on the production cross-section as a function of the mass and lifetime of the long-lived particle.
volume-issue-count12issue-article-count101issue-toc-levels0issue-typeRegularissue-online-date-year2018issue-online-date-month1issue-online-date-day22issue-pricelist-year2017issue-copyright-holderSIF and Springer-Verlag GmbH Germanyissue-copyright-year2017article-contains-esmNoarticle-numbering-styleContentOnlyarticle-toc-levels0article-registration-date-year2017article-registration-date-month9article-registration-date-day1article-grants-typeOpenChoicemetadata-grantOpenAccessabstract-grantOpenAccessbodypdf-grantOpenAccessbodyhtml-grantOpenAccessbibliography-grantOpenAccessesm-grantOpenAccessIntroduction
Various extensions of the Standard Model (SM) feature new particles whose couplings to lighter states are sufficiently small to result in detectable lifetimes. In this paper we report on a search for such long-lived particles, which are assumed to be pair-produced in the decay of a Standard-Model-like Higgs boson, and subsequently decay into a quark–antiquark pair. Such a signature is present in models with a hidden-sector non-Abelian gauge group, where the Standard Model Higgs boson acts as a portal [1–5]. The new scalar particle represents the lightest state in the hidden sector and is called a hidden-valley pion (πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document}) throughout this paper. Experimental constraints on the properties of the Higgs boson of mass 125GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} observed by the ATLAS and CMS collaborations [6, 7] still allow for branching fractions of non-SM decay modes of up to 30% [8].
Data collected with the LHCb experiment in 2011 and 2012 are used for this analysis, restricted to periods in which suitable triggers were available. The data sample analysed corresponds to 0.62fb-1\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{fb}^{-1}$$\end{document} at a centre-of-mass energy of s=7TeV\documentclass[12pt]{minimal}
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\begin{document}$$\sqrt{s}={7}\,\mathrm{TeV}$$\end{document} and 1.38fb-1\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{fb}^{-1}$$\end{document} at s=8TeV\documentclass[12pt]{minimal}
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\begin{document}$$\sqrt{s}={8}\,\mathrm{TeV}$$\end{document}. In simulated events with πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} pairs originating from a Higgs boson decay it is found that in most cases no more than one of the two πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} decays occurs inside the LHCb acceptance. Consequently, the experimental signature is a single πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} particle. The candidate is identified by its decay to two hadronic jets originating from a displaced vertex, with a transverse distance to the proton-proton collision axis (Rxy\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document}) of at least 0.4 mm. The vertex is required to have at least five tracks reconstructed in the LHCb vertex detector. The analysis is sensitive to πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} particles with a mass between 25 and 50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and a lifetime between 2 and 500 ps. The lifetime range is limited due to the presence of large prompt backgrounds at short decay times and the acceptance of the vertex detector for long decay times. The lower boundary on the mass range arises from the requirement to identify two hadronic jets while the upper boundary is driven by the geometric acceptance of the detector.
This paper presents an update of an earlier analysis, which considered only the data set corresponding to an integrated luminosity of 0.62fb-1\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{fb}^{-1}$$\end{document} collected at s=7\documentclass[12pt]{minimal}
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\begin{document}$$\sqrt{s}=7$$\end{document} TeV [9]. Similar searches for hidden-valley particles decaying to jet pairs were performed by the D0 [10], CDF [11], ATLAS [12–14] and CMS [15] collaborations. Compared to these analyses, this search is sensitive to πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} particles with relatively low mass and lifetime. The LHCb collaboration has also performed a search for events with two displaced high-multiplicity vertices [16] and a search for events with a lepton from a high-multiplicity displaced vertex [17] in the context of SUSY models, and several searches for so far unknown long-lived particles in B-meson decays [18–21].
Detector and event simulation
The LHCb detector [22, 23] is a single-arm forward spectrometer covering the pseudorapidity range 2<η<5\documentclass[12pt]{minimal}
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\begin{document}$$2<\eta <5$$\end{document}, designed for the study of particles containing b\documentclass[12pt]{minimal}
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\begin{document}$$b$$\end{document} or c\documentclass[12pt]{minimal}
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\begin{document}$$c$$\end{document} quarks. The detector includes a high-precision tracking system consisting of a silicon-strip vertex detector (VELO) surrounding the pp interaction region, a large-area silicon-strip detector located upstream of a dipole magnet with a bending power of about 4Tm\documentclass[12pt]{minimal}
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\begin{document}$$4{\mathrm {\,Tm}}$$\end{document}, and three stations of silicon-strip detectors and straw drift tubes placed downstream of the magnet. The tracking system provides a measurement of the momentum, p\documentclass[12pt]{minimal}
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\begin{document}$$p$$\end{document}, of charged particles with a relative uncertainty that varies from 0.5% at low momentum to 1.0% at 200GeV/c\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c$$\end{document}. The minimum distance of a track to a primary vertex (PV), the impact parameter (IP), is measured with a resolution of (15+(29GeV/c)/pT)μm\documentclass[12pt]{minimal}
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\begin{document}$$(15+({29}{\,\mathrm{GeV}/c})/p_\mathrm{T})\;{\mu \mathrm{m}}$$\end{document}, where pT\documentclass[12pt]{minimal}
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\begin{document}$$p_\mathrm{T}$$\end{document} is the component of the momentum transverse to the collision axis. Different types of charged hadrons are distinguished using information from two ring-imaging Cherenkov detectors. Photons, electrons and hadrons are identified by a calorimeter system consisting of scintillating-pad (SPD) and preshower detectors, an electromagnetic calorimeter and a hadronic calorimeter. Muons are identified by a system composed of alternating layers of iron and multiwire proportional chambers.
The model for the production of πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} particles through the Higgs portal is fully specified by three parameters: the mass of the Higgs boson and the mass and lifetime of the πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document}. The Higgs boson mass is taken to be 125GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document}, and its production through the gluon-gluon fusion process is simulated with the Pythia8 generator [24], with a specific LHCb configuration [25] and using the CTEQ6 leading-order set of parton density functions [26]. The interaction of the generated particles with the detector, and its response, are implemented using the Geant4 toolkit [27, 28] as described in Ref. [29]. Signal samples with πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} masses of 25, 35, 43 and 50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and lifetimes of 10 and 100 ps are generated. In the simulated events the long-lived particles decay exclusively as πv→bb¯\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}\rightarrow {b\bar{b}}$$\end{document}, since this decay mode is generally preferred in the Higgs portal model. Samples with decays to c\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and a lifetime of 10 ps.
Event selection
The experimental signature for this analysis is a single displaced vertex with two associated jets. Only decays that produce a sufficient number of tracks in the VELO for a vertex to be reconstructed are considered. Due to the geometry of the vertex detector, this restricts the sample to decay points up to about 200 mm from the nominal interaction point along the beam direction, and up to about 30 mm in the transverse direction, thereby limiting the decay time acceptance. The selection strategy is the same as used in the analysis of Ref. [9]. Reconstructed tracks are used to find the decay vertex, and jets are built out of reconstructed particles compatible with originating from that vertex. Constraints on the signal yield are determined from a fit to the dijet invariant mass distribution. The main source of background is displaced vertices from heavy-flavour decays or interactions of particles with detector material. To take into account the strong dependence of the background level on the separation from the beam axis, different selection criteria are used in different bins of Rxy\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document}, and the final fit is performed in bins of this variable.
The selection consists of online (trigger) and offline parts. The trigger [30] is divided into a hardware (L0) and a software (HLT) stage. The L0 requires a muon with high pT\documentclass[12pt]{minimal}
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\begin{document}$$p_\mathrm{T}$$\end{document} or a hadron, photon or electron with high transverse energy in the calorimeters. In order to reduce the processing time of the subsequent trigger stages, events with a large hit multiplicity in the SPD are discarded. The software stage is divided into two parts, which for this analysis differ between the 2011 and 2012 data. In the 2011 sample, the first software stage (HLT1) requires a single high-pT\documentclass[12pt]{minimal}
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\begin{document}$$p_\mathrm{T}$$\end{document} track with a large impact parameter. The HLT1 selection for the 2012 sample was complemented with a two-track vertex signature with looser track quality criteria, in order to improve the efficiency at large displacements. At the second stage of the software trigger (HLT2), events are required to pass either a dedicated inclusive displaced-vertex selection or a standard topological B decay selection, which requires a two-, three- or four-track vertex with a significant displacement from all PVs [30]. The inclusive displaced-vertex selection uses an algorithm similar to that used for the LHCb primary vertex reconstruction [31]. A combination of requirements on the minimum number of tracks in the vertex (at least four), the distance Rxy\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document} of the vertex to the beam axis (at least 0.4 mm), the invariant mass of the particles associated with the vertex (at least 2GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document}) and the scalar sum pT\documentclass[12pt]{minimal}
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\begin{document}$$p_\mathrm{T}$$\end{document} of the tracks that form the vertex (at least 3GeV/c\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c$$\end{document}), is used to define a set of trigger selections with sufficiently low rate.
Before the offline selection can be applied, the displaced vertex corresponding to the decay of the πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} candidate must be reconstructed. For those events in which the HLT2 inclusive displaced-vertex selection was successful, the same vertex candidate found in the trigger is used; this approach differs from that used in the previous LHCb analysis [9] and simplifies the evaluation of systematic uncertainties. For events selected only by the topological B trigger, a modified version of the algorithm is run on the output of the offline reconstruction with the following criteria: vertices with 0.4<Rxy<1mm\documentclass[12pt]{minimal}
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\begin{document}$$0.4< R_{xy}{} < {1}\, \mathrm{mm}$$\end{document} must have at least eight tracks and the invariant mass of the system must exceed 10GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}{} > {5}\, \mathrm{mm}$$\end{document} must have at least five tracks. To exclude background due to interactions with the detector material, vertices inside a veto region around the VELO detector elements are discarded. Events with many parallel displaced tracks, which can arise from machine background, are identified by the azimuthal distribution of hits in the VELO and are also discarded.
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\begin{document}$$\theta $$\end{document} itself, since its efficiency depends less strongly on the boost and the mass of the candidate [35]. The second criterion is that the kinematic separation of the jets should satisfy ΔR=(Δη)2+(Δϕ)2<2.2\documentclass[12pt]{minimal}
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\begin{document}$$\Delta \eta $$\end{document} and Δϕ\documentclass[12pt]{minimal}
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\begin{document}$$\Delta \phi $$\end{document} are the pseudorapidity and azimuthal angle differences between the two jets, respectively. This reduces the tail in the dijet invariant mass distribution by suppressing the remaining back-to-back dijet background.
The overall efficiency to reconstruct and select displaced πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} decays in the simulated samples is summarized in Table 1 for the 2011 and 2012 data taking conditions. A large part of the inefficiency is due to the detector acceptance, which is about 13% (8%) and 6.5% (5.5%) for πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} particles with a lifetime of 10 ps (100 ps) and masses of 25 and 50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document}, respectively. Other important contributions are due to the selection on the displacement from the beamline, requirements on the minimum number of tracks forming the vertex, the material interaction veto, the reduction in VELO tracking efficiency at large displacements, and the jet selection [36]. The efficiency for long-lived particles decaying to s\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} decay vertex.
Number of selected candidates per generated H0→πvπv\documentclass[12pt]{minimal}
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\begin{document}$$H^{0} \rightarrow \pi _{\text {v}}\pi _{\text {v}}$$\end{document} event (efficiency) in percent for different πv→qq¯\documentclass[12pt]{minimal}
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\begin{document}$${\pi _{\text {v}}} \rightarrow {{q}{}{\overline{q}}{}}$$\end{document}, q=b,c,s\documentclass[12pt]{minimal}
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\begin{document}$${q}=b, c, s$$\end{document} models for 2011 and 2012 data taking conditions, as derived from simulation. The relative statistical uncertainty on the efficiency due to the limited size of the simulated sample is less than a few percent
Systematic uncertainties on the efficiency are obtained from studies of data-simulation differences in control samples. They are reported in Tables 2 and 3, for the 2011 and 2012 conditions, respectively, and discussed in more detail below. Uncertainties on the signal efficiency due to parton-density distributions, the simulation of fragmentation and hadronization, and the Higgs boson production cross-section and kinematics are not taken into account.
Overview of the contributions to the relative systematic uncertainty on the signal efficiency and luminosity (in percent) for different signal samples in 2011 conditions. The uncertainty on the total efficiency is obtained by summing the individual contributions in quadrature
Overview of the contributions to the relative systematic uncertainty on the signal efficiency and luminosity (in percent) for different signal samples in 2012 conditions. The uncertainty on the total efficiency is obtained by summing the individual contributions in quadrature
The vertex reconstruction efficiency can be split into two parts, namely the track reconstruction efficiency and the vertex finding efficiency. The track reconstruction efficiency is described by the simulation to within a few percent, including for highly displaced and low-momentum tracks [37–39]. The effect of a systematic change in this efficiency is studied by randomly removing 2% of the signal tracks and reapplying all selection criteria.
The vertex finding algorithm is not fully efficient even if all tracks are reconstructed. In particular, the efficiency to find a low-multiplicity secondary vertex is reduced in the proximity of a high-multiplicity PV. The effect is studied in data and simulation using exclusively reconstructed B0→J/ΨK∗0\documentclass[12pt]{minimal}
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\begin{document}$$B^{0}\rightarrow J/\varPsi K^{*0}$$\end{document} decays, which can be selected with high purity without tight requirements on the vertex. The efficiency for the displaced vertex reconstruction algorithm to find the B0\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document} in data and simulation [36]. The difference, weighted by the Rxy\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document} distribution of the signal candidates, is used to derive a systematic uncertainty.
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\begin{document}$$m/m_\text {corr}$$\end{document} selection and the dijet invariant mass shape. The jet reconstruction efficiency has been studied previously in measurements of the Z+jet\documentclass[12pt]{minimal}
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\begin{document}$${{Z}} \rightarrow {{\mu ^{+}\mu ^{-}}}+\text {jet}$$\end{document} sample is used to study jet-related systematic effects for this analysis as well. To mimic the selection of the particle-flow inputs, the PV associated to the Z\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} reconstruction efficiency and correspond to systematic uncertainties of 2–4%, depending on the πv\documentclass[12pt]{minimal}
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\begin{document}$${Z}\rightarrow {\mu ^{+}\mu ^{-}}$$\end{document} sample triggered by the dimuon L0 selection, which applies only a loose selection on this quantity. An efficiency correction is derived, which is about 90% for 2011 data, and about 85% for 2012 data, with an uncertainty of 2–3%. The difference in the correction between the different πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} models is smaller than the systematic variation. This correction is applied to the overall detection efficiency derived from the simulation and the uncertainty is taken as a systematic uncertainty.
The differences between data and simulation in the HLT1 selection are dominated by the track reconstruction efficiency, which was discussed above, and additional track quality criteria. One such difference is due to a requirement on the number of VELO hits for displaced tracks. It is characterized using B0→J/ΨK∗0\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} decays the final-state track multiplicity is larger, which dilutes effects due to a mismodelling of the single-track efficiency.
The main source of systematic uncertainty in the HLT2 selection is the vertex reconstruction efficiency, which was discussed above. The efficiency of the topological B\documentclass[12pt]{minimal}
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Results
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Results are presented as upper limits on the signal strength μ≡(σ/σgg→H0SM)·B(H0→πvπv)\documentclass[12pt]{minimal}
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\begin{document}$${s\bar{s}}$$\end{document} depending on the final state under study) is assumed to be 100%. If the decay width of the πv\documentclass[12pt]{minimal}
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The CLs\documentclass[12pt]{minimal}
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\begin{document}$$\text {CL}_s$$\end{document} method [42] is used to determine upper limits. The profile likelihood ratio qPLLμ=L(μ,θ^(μ))/L(μ^,θ^)\documentclass[12pt]{minimal}
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\begin{document}$$L(\hat{\mu },\hat{\theta })$$\end{document} is the global maximum likelihood. To estimate the sensitivity of the analysis and the significance of a potential signal, the expected upper limit quantiles in the case of zero signal are also evaluated.
For each value of μ\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document} bin and data taking year, the invariant mass distribution is modelled by the sum of background and signal components. The distribution for the signal is modelled as a Gaussian distribution whose parameters are obtained from fully simulated signal events. For the background distribution an empirical model, outlined below, is adopted.
Background candidates can be categorized into two contributions. The first category is mostly due to the combination of a heavy-flavour decay vertex or an interaction with detector material with particles from a primary interaction. This contribution has a steeply decreasing invariant mass spectrum. Following the approach in Ref. [9], the distribution is modelled by the convolution of a falling exponential distribution with a bifurcated Gaussian. All parameters of this background model are free to vary in the fit.
The second category is due to Standard Model dijet events. These events have candidates with jets that are approximately back-to-back in the transverse plane. It is suppressed by the selection on the dijet opening angle ΔR\documentclass[12pt]{minimal}
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\begin{document}$$\Delta R$$\end{document}. Its remaining contribution has a less steeply falling mass spectrum. It is described in the fit with a similar functional shape as for the first category, but with the parameters and the relative yields in the different bins fixed from a fit to the invariant mass distribution of candidates that fail the ΔR\documentclass[12pt]{minimal}
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\begin{document}$$\Delta R$$\end{document} requirement. In the final fit only the total normalization of this component is varied. The second component is new compared to the model used for the previous analysis [9]. It leads to a better description of the high-mass tail, at the expense of one extra fit parameter for each data taking year. It was found that the result of the fit is not sensitive to the exact ΔR\documentclass[12pt]{minimal}
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\begin{document}$$\Delta R$$\end{document} requirement used to select the events for this component.
All parameters of the fit to the invariant mass distribution are allowed to float independently in each bin, except for the following nuisance parameters: the dijet invariant mass scale, the overall signal efficiency, and the normalization for the second background contribution. All relevant systematic uncertainties are incorporated in the fit model: the overall uncertainty on the efficiency, as described in Sect. 4, the uncertainty on the dijet invariant mass scale, and the uncertainties on the shape parameters and relative normalisation arising from the finite size of the simulated signal samples. Gaussian constraints on these parameters are added to the likelihood.
Alternatives have been considered for the background mass model, in particular with an additional less steeply falling exponential to describe the tail. With these models the estimated background yield at higher mass is similar or larger than with the nominal background model, leading to tighter limits on the signal. As the nominal model gives the most conservative limit, no additional systematic uncertainty is assigned for background modeling.
There is no significant excess of signal in the data. Upper limits at 95% confidence level (CL) as a function of lifetime for hidden-valley models with different πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} mass and decay mode are shown in Fig. 3 and summarized in Table 4 and Fig. 4. The best sensitivity is obtained for a mass of about 50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and a lifetime of about 10 ps. The main improvements with respect to the previous result [9] are due to the enlarged data sample, the improved trigger selections, and the addition of the Rxy\documentclass[12pt]{minimal}
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\begin{document}$$R_{xy}$$\end{document} bin above 5 mm, which contributes to the increased sensitivity at larger lifetimes.
Observed upper limit versus lifetime for different πv\documentclass[12pt]{minimal}
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\begin{document}$$\pi _{\text {v}}$$\end{document} masses and decay modes. The decay πv→bb¯\documentclass[12pt]{minimal}
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\begin{document}$${\pi _{\text {v}}{}}\rightarrow {{b\bar{b}}{}}$$\end{document} is assumed, unless specified otherwise
Conclusion
Results have been presented from a search for long-lived particles with a mass in the range 25–50GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} and a lifetime between 2 and 500 ps. The particles are assumed to be pair-produced in the decay of a 125GeV/c2\documentclass[12pt]{minimal}
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\begin{document}$$\,\mathrm{GeV}/c^{2}$$\end{document} Standard-Model-like Higgs boson and to decay into two jets. Besides decays to bb¯\documentclass[12pt]{minimal}
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\begin{document}$$b\bar{b}$$\end{document}, which are the best motivated in the context of hidden-valley models [1, 2], also decays to cc¯\documentclass[12pt]{minimal}
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\begin{document}$$s\bar{s}$$\end{document} quark pairs are considered. No evidence for so far unknown long-lived particles is observed and limits are set as a function of mass and lifetime. These measurements complement other constraints on this production model at the LHC [13, 15] by placing stronger constraints at small masses and lifetimes.
Acknowledgements
We express our gratitude to our colleagues in the CERN accelerator departments for the excellent performance of the LHC. We thank the technical and administrative staff at the LHCb institutes. We acknowledge support from CERN and from the national agencies: CAPES, CNPq, FAPERJ and FINEP (Brazil); MOST and NSFC (China); CNRS/IN2P3 (France); BMBF, DFG and MPG (Germany); INFN (Italy); NWO (The Netherlands); MNiSW and NCN (Poland); MEN/IFA (Romania); MinES and FASO (Russia); MinECo (Spain); SNSF and SER (Switzerland); NASU (Ukraine); STFC (United Kingdom); NSF (USA). We acknowledge the computing resources that are provided by CERN, IN2P3 (France), KIT and DESY (Germany), INFN (Italy), SURF (The Netherlands), PIC (Spain), GridPP (United Kingdom), RRCKI and Yandex LLC (Russia), CSCS (Switzerland), IFIN-HH (Romania), CBPF (Brazil), PL-GRID (Poland) and OSC (USA). We are indebted to the communities behind the multiple open source software packages on which we depend. Individual groups or members have received support from AvH Foundation (Germany), EPLANET, Marie Skłodowska-Curie Actions and ERC (European Union), Conseil Général de Haute-Savoie, Labex ENIGMASS and OCEVU, Région Auvergne (France), RFBR and Yandex LLC (Russia), GVA, XuntaGal and GENCAT (Spain), Herchel Smith Fund, The Royal Society, Royal Commission for the Exhibition of 1851 and the Leverhulme Trust (United Kingdom).
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\begin{document}$$\sqrt{s}= 7$$\end{document} TeV in the forward region. JHEP 01, 064 (2015). arXiv:1411.1264LHC Higgs Cross Section Working Group, S. Heinemeyer et al., Handbook of LHC Higgs cross sections: 3. Higgs properties. CERN-2013-004. arXiv:1307.1347ReadALPresentation of search results: the CLs\documentclass[12pt]{minimal}
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\begin{document}$$CL_s$$\end{document} techniqueJ. Phys. G20022826932002JPhG...28.2693R10.1088/0954-3899/28/10/313