Literature DB >> 36093314

Leptons lurking in semi-visible jets at the LHC.

Cesare Cazzaniga1, Annapaola de Cosa1.   

Abstract

This Letter proposes a new search for confining dark sectors at the Large Hadron Collider. As a result of the strong dynamics in the hidden sector, dark matter could manifest in proton-proton collisions at the Large Hadron Collider in form of hadronic jets containing stable invisible bound states. These semi-visible jets have been studied theoretically and experimentally in the fully hadronic signature where the unstable composite dark matter can only decay promptly back to Standard Model quarks. We present a simplified model based on two messenger fields separated by a large mass gap allowing dark bound states to decay into pairs of oppositely charged leptons. The resulting experimental signature is characterized by non-isolated lepton pairs inside semi-visible jets. We propose a search strategy independent from the underlying model assumptions targeting this new signature, and discuss the orthogonality with respect to the existing searches. Remaining agnostic on the shape of the di-lepton spectrum, we determine the sensitivity of a dedicated analysis to the target signal. The proposed search can claim the 3 σ evidence (exclusion) of the heavier mediator up to masses of 3.5 TeV (4.5 TeV) with the full Run 2 data of the LHC. Exploiting the resonant feature of the lepton pairs can enhance the sensitivity reach on a specific model. We estimate that an analysis using the di-lepton invariant mass information can reach 5 σ discovery up to masses of 3.5 TeV and improve the exclusion up to more than 5 TeV.
© The Author(s) 2022.

Entities:  

Year:  2022        PMID： 36093314      PMCID： PMC9448692          DOI： 10.1140/epjc/s10052-022-10775-2

Source DB:  PubMed          Journal:  Eur Phys J C Part Fields        ISSN： 1434-6044            Impact factor:   4.991


Introduction

The Standard Model (SM) has collected many successes, culminating with the discovery of the Higgs boson [1, 2]. However, there are still open questions such as the origin of dark matter (DM), the neutrino masses and the baryon asymmetry, that cannot be addressed within the SM framework. The astrophysical and cosmological measurements of DM gravitational effects at large scales [3, 4] strongly support the idea of a separate sector of particles whose spectrum has not been observed yet by the current searches [5-7]. The most common strategy adopted by the LHC collaborations to search for DM relies on the assumption that DM is composed of Weakly Interacting Massive Particles (WIMPs) [8, 9]. WIMPs produce in the detector an excess of missing transverse momentum () accompanied by other visible objects, e.g. jets, photons, leptons [10-17] or by a Higgs boson [18, 19] (X signatures). Hidden Valley models [20] propose alternative, well-motivated BSM scenarios to explain DM nature. These models arise in many top-down approaches, including String theory [21, 22] and they appear consistent with many UV-complete theories aiming to solve fundamental problems such as the electroweak hierarchy [23-25]. Hidden Valley models with strongly coupled hidden sectors can evade the phase-space probed by the collider searches mentioned above. In this scenario, novel experimental signatures emerge, characterized by sprays of particles resembling hadronic jets that include DM bound states and their decay products (dark jets). Dark jets can appear in the detector at different distances according to the lifetime of the hidden sector bound states. In case of long-lived DM bound states, displaced signatures arise, such as those characterizing emerging jets [26] and trackless/displaced jets [27]. For prompt decays of the dark sector bound states to SM particles, typical signatures are prompt dark jets [28, 29] or semi-visible jets (SVJ) [30-32]. In particular, semi-visible jets occur if a sizable fraction of the DM bound states within the dark jets remains stable, resulting in a multijet+ signature characterized by aligned with one of the jets. To evade the strong experimental constraints from high mass di-lepton searches [33, 34], available semi-visible jets simplified models assume a TeV-scale leptophobic boson as unique mediator between the dark sector and the SM. Under this hypothesis, leptons cannot be produced directly from the decays of the DM bound states mediated by the messenger boson. This assumption poses some limits in terms of possible experimental signatures and DM discovery perspectives. In this Letter, we present a simplified model developed on concepts proposed in [35] leading to semi-visible jets enriched in non-isolated leptons (SVJ), and propose a general search strategy to probe this novel signature at the LHC experiments.

Simplified model setup

Driven by our target experimental signature, characterized by prompt non-isolated leptons produced inside semi-visible jets, we introduce a simple Hidden Valley model that will enable us to estimate the LHC sensitivity to this class of signals. The model is built in the Simplified DM Models fashion [36] and it is presented for illustration purposes since the experimental signature we are targeting in this study is common to a large class of dark-sector theories. In the Hidden Valley scenario that we consider, the SM gauge group is supplemented by a non-abelian dark sector with gauge coupling . Here we choose the number of dark color charges for concreteness. Within this hidden sector, the only fermions in the fundamental representation of are the dark quarks , with , where is the number of dark flavors. Confinement of this Yang Mills theory at a scale is guaranteed only for [37]. In our study, we assume a minimal two dark flavors model () with mass degenerate states. The dark sector is assumed not to be completely secluded from the SM. Following the same approach as in [30, 31], we require a first TeV-scale leptophobic messenger field to couple directly with both the SM quarks axial-vector current and the dark quarks vector current [38]. The boson can acquire its mass via spontaneous symmetry breaking of the due to a dark Higgs field with non-zero vacuum expectation value [20]. The dark Higgs sector has been neglected as it is assumed to be out of the LHC reach and therefore irrelevant for the phenomenology discussed here. The energy scale of the event is set by . Requiring the coupling of to dark quarks () to be much larger than the coupling to SM quarks (), the boson is expected to decay predominantly into dark quarks . A QCD-like parton shower in the dark sector initiated by is considered [35, 39]. The soft and collinear splittings draw the energy scale of the process down to the dark confinement scale where dark hadrons of spin 0 (pseudo-scalar mesons ) and spin 1 (vector mesons ) are produced after hadronization. Some of these dark hadrons will be stable, and others will decay back to SM according to the conservation of global accidental symmetries of the dark sector, such as dark-isospin and dark-baryon number [20, 30, 31]. To allow DM bound states to decay to leptons, we follow a similar approach as in [35], and we introduce a light vector messenger field . The field mixes with the SM hypercharge field via a term governed by the parameter . After the diagonalization of the mixing term [40], the Lagrangian for the messenger sector is:The mass of the boson can be generated in the same way as the mass. However, we assume to couple much more weakly to the dark Higgs field compared to the boson, therefore leading to , with at the GeV-scale. This mass hierarchy favors the decay of the unstable dark vector mesons via the lighter messenger . Indeed, the decay width of these DM bound states scales with the mediator mass as , thus suppressing the off-shell -mediated decays. The dark pseudo-scalar mesons can decay promptly through the portal to heavy quarks via a mass insertion [30] due to helicity suppression. The partial widths of an unstable dark vector meson decaying to SM fermions via the boson can be calculated from a chiral EFT [35]. The parameter governing the mixing in the chiral EFT is given by incorporating the non-perturbative dark sector dynamics information together with the gauge mixing parameter , and an effective mass scale dependence . The immediate phenomenological consequence of the two messenger fields model is a factorization between the production of the dark quarks, which can be mediated by a heavy leptophobic boson, and the decays of the dark vector mesons, which are completely driven by the lighter . As sketched in Fig. 1, this model leads to semi-visible jets with inside pairs of opposite charge leptons produced by the unstable dark hadrons. A further production mechanism for dark quarks could be directly via the boson. However, this production channel contributes mainly to low mass SVJ, where current trigger selection strategies dramatically limit a search sensitivity. For this reason, we don’t investigate this contribution here and leave it to future studies. Lower bounds for the life-times of the unstable dark vector mesons have been calculated in [35]. For DM bound states with masses at least around the GeV-scale, can be so small that detectable displacements between the production and decay points of unstable dark hadrons cannot be resolved, resulting in a signature with prompt leptons.
Fig. 1

S-channel production of semi-visible jets with non-isolated prompt leptons produced from dark hadrons decays

Monte Carlo simulations

The signal and background processes are produced at  TeV with MadGraph5_aMC@NLO [41] event generator using the parton distribution functions NN23LO1 [42] from the Lhapdf [43] repository. The evolution of the parton-level events and hadronization are performed with Pythia8 [44]. The initial state partons are matched with the jets using the MLM scheme [45] implemented in MadGraph5. Initial and final-state radiation as well as underlying events are included in the simulation. To simulate the showering, hadronization and decays in the dark sector, we used the Hidden Valley module [46, 47] in Pythia8. The generated events are then interfaced with Delphes3 [48] to model the response of the CMS detector [49]. In our study, anti- jets [50, 51] with (AK8 jets) are reconstructed requiring a minimum for clustering of 200 GeV. We use AK8 jets since semi-visible jets are expected to be wider than typical SM jets because they arise from a multi-step process beginning with dark quarks produced via and ending up with SM hadrons after hadronization in the hidden sector and in the SM [52]. All the samples have been normalized to the LHC Run 2 integrated luminosity . S-channel production of semi-visible jets with non-isolated prompt leptons produced from dark hadrons decays For the SVJ s-channel signal process, events have been generated at LO for  TeV with 500 GeV steps. Following the most recent recommendations from the LHC DM Working Group [53], the coupling has been assumed to be flavour-universal and set to 0.25. Taking into account the number of flavours and colours in the dark sector as in [52], the coupling has been fixed to 0.4. For this set of couplings, the constraints from the di-jet searches are still weak [30, 52, 54]. The number of stable and unstable dark hadrons produced in the dark hadronization process can vary according to the details of the dark sector. To capture these variations, an effective invisible fraction can be defined as . This parameter can take any value between 0 and 1 [30, 31] depending on the details of the dark sector such as the number of dark flavours, the number of dark colors, dark quark masses, fragmentation and accidental global symmetries. To span a wide range of possible experimental signatures as a function of the model parameters Table 1, we consider three different benchmark scenarios for representing different possible regimes.
Table 1

Signal model parameterization

ParameterDescriptionBenchmark
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$M_{Z'}$$\end{document}MZ′\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$Z'$$\end{document}Z′ pole mass1.5–5 TeV
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\epsilon _{\text {eff,v}}$$\end{document}ϵeff,vEffective mixing0.03
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$r_{\text {inv}}$$\end{document}rinvInvisible fraction0.3, 0.5, 0.7
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\Lambda _v$$\end{document}ΛvDark confinement scale5 GeV
\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$m_{\pi _v}/\Lambda _v$$\end{document}mπv/ΛvPseudo-scalar mass ratio1.6
The effect of is simulated by requiring dark hadrons to decay to a pair of invisible particles with probability . The dark hadrons that decay invisibly are proxies for the stable dark hadrons, while the remaining dark hadrons are the unstable ones. Even for mass degenerate dark quarks, the dark pseudo-scalar and dark vector mesons masses can differ according to the hidden sector non-perturbative dynamics. Setting as overall mass scale for dark mesons, lattice QCD fits in [37] have been used to predict the masses of dark vector mesons from the input ratio . As a benchmark, the hadronization scale has been set to 5 GeV and the ratio , therefore fixing in the heavy quarkonium region at 8 GeV and 15 GeV. The effective mixing parameter has been set saturating the electroweak precision tests bound [35, 55] evading the existent constraints from searches for dilepton resonances [33, 34, 56]. With this choice of the input parameters, the predicted average fraction of unstable mesons decaying into leptons is per each flavour. The life-times of the unstable dark hadrons has been fixed such that no displacement can be resolved experimentally according to theoretical lower bounds for dark hadron masses at the GeV-scale. Table 1 summarizes the five most relevant parameters for signal modelling. Three are sensitive to the details of the dark sector: the confinement scale , the pseudo-scalar mass ratio and the invisible fraction . Moreover, there are two portal parameters: the mass of the boson , and the effective mixing . Signal model parameterization In this study, we have considered the same background processes as in the CMS semi-visible jets search [52]. All the background samples have been generated at LO. The QCD sample ( events) has been produced requiring a generator level cut on the leading parton jet  GeV. The QCD background is particularly relevant due to the large cross-section and the possibility of mis-reconstruction of the jet momentum leading to additional missing momentum aligned with the jet axis. The presence of b-flavored hadrons decaying into leptons inside the jets further mimics the signal signature. The inclusive sample ( events) has been generated with up to two additional partons. This background mainly becomes of relevance when the top quarks are boosted, and therefore the W boson decay and the b-initiated jet are merged into a larger jet. The electroweak inclusive backgrounds and (both events) have been produced with a generator level cut  GeV and including up to three additional partons in the matrix element.

Search strategy

The main feature of the SVJ signal is the presence of pairs of leptons from dark hadrons decays. The hadronic activity near a reconstructed object such as a lepton , is quantified by the isolation variable [48]. The isolation is defined as the sum of the momenta of all the particles reconstructed within a cone of given radius centred around the lepton itself, normalized to lepton . The isolated leptons () have a small probability to originate from a jet. Due to a large number of constituents within a jet cone, SVJ leptons pairs fail the standard isolation requirements applied in BSM searches [33, 34, 56–61]. a Multiplicity of mini-isolated muons. b Distribution of muons inter-isolation for . c Multiplicity of non inter-isolated muons. In all the histograms the last bin represents the overflow. The signal distributions are referred to a benchmark mass point  TeV and , while all the other parameters are fixed as in Table 1 Furthermore, in the fully hadronic SVJ search [52], the background from boosted top decays in semi-leptonic final states is reduced by applying a veto on mini-isolated leptons [62, 63]. However, this veto is highly inefficient to select SVJ events, because some leptons inside SVJ are expected to be mini-isolated as shown in Fig. 2a.
Fig. 2

a Multiplicity of mini-isolated muons. b Distribution of muons inter-isolation for . c Multiplicity of non inter-isolated muons. In all the histograms the last bin represents the overflow. The signal distributions are referred to a benchmark mass point  TeV and , while all the other parameters are fixed as in Table 1

To exploit the lepton-enriched content of SVJ signal and enhance background rejection, we define an inter-isolation variable quantifying how much each lepton is isolated with respect to all the other leptons within a cone of radius . As shown in Fig. 2b, inter-isolation provides an evident handle against all the backgrounds and it remains almost independent from . Furthermore, this variable captures the main feature of the SVJ leptons leading to a peak in the multiplicity for one pair of non inter-isolated leptons as evidenced in Fig. 2c. Due to its features, inter-isolation can be used as an additional requirement to select SVJ candidates. In this letter, we propose a cut-based search strategy for leptons-enriched semi-visible jets. We apply the selections used in the inclusive fully hadronic SVJ search [52]. For completeness, we explicit the selections in the following paragraphs. On top of it, we introduce a set of model-independent requirements exploiting the leptonic content of SVJ. We require each event to have at least two AK8 jets with  GeV and . Furthermore, the two leading jets are required to have a maximum pseudo-rapidity separation , removing the large t-channel QCD contribution [64, 65]. The features of the s-channel due to the high mass resonance is exploited by reconstructing the invariant mass of the di-jet system. To improve mass resolution, we included information from the missing momentum, computing the missing transverse mass, , as done in [30]. A realistic trigger selection is expected to sculpt . Therefore, we require  GeV. A minimal amount of is required by asking the transverse ratio to be larger than 0.15. This last requirement does not affect the distribution shape. Finally, we require the minimum azimuthal opening between either of the two AK8 jets and the to be less than 0.8. This selection allows to suppress backgrounds, and select events where the missing momentum is aligned to one of the jets as expected for SVJ events, unlike previous multijet+ searches [10, 11]. For selecting SVJ events, we add some requirements on the leptons. The selected electrons must have a transverse momentum well above the CMS ECAL noise and meet current trigger requirements, namely  GeV in the barrel () and in the end-caps (). We require muons with and  GeV such that they can be good seeds for the CMS outside-in global muon reconstruction [66]. Both electrons and muons are required to have a small transverse impact parameter, m, since SVJ leptons are produced by dark hadrons prompt decays. This requirement allows to further suppress background as well as the QCD events where leptons are produced by long-lived b-flavored hadrons decays. We use standard isolation to veto all events with more than one isolated lepton () since the signal is characterized by pairs of non-isolated opposite-charge leptons. Moreover, we require to have at least one pair of opposite-sign non-inter-isolated leptons (). This last requirement improves by more than QCD rejection and more than rejection compared to SVJ-tag selections. Also the electro-weak background contribution is heavily suppressed due to the charge and inter-isolation requirements. To estimate the sensitivity of a dedicated LHC search, we perform a bump hunt in the di-jet spectrum (Fig. 3a). In addition, the model predicts resonances appearing in the di-lepton spectrum at the GeV scale. However, the low mass di-lepton signal strongly depends on the details of the dark sector. This model-dependent feature can be exploited by applying a selection on the di-lepton invariant mass spectrum, thus enhancing the sensitivity reach of the search. Here we report the expected sensitivity reach of the LHC remaining agnostic on the di-lepton mass range, together with an estimate of the sensitivity improvement brought by an additional selection on non-inter-isolated leptons pairs with opposite charges requiring their invariant mass to be consistent with the mass ( GeV).
Fig. 3

a template for the signal (benchmark mass point  TeV and ) and background processes after applying the selections proposed in this Letter (without the requirement on ). The binning has been chosen according to an experimental resolution . b Expected limits on for the signal benchmark with and all the other parameters fixed as in Table 1. The fully hadronic SVJ analysis expected exclusion reach (dashed blue line) for the SVJ signature is compared with the proposed SVJ cut based analysis without exploiting the selection on (dashed gray line)

a template for the signal (benchmark mass point  TeV and ) and background processes after applying the selections proposed in this Letter (without the requirement on ). The binning has been chosen according to an experimental resolution . b Expected limits on for the signal benchmark with and all the other parameters fixed as in Table 1. The fully hadronic SVJ analysis expected exclusion reach (dashed blue line) for the SVJ signature is compared with the proposed SVJ cut based analysis without exploiting the selection on (dashed gray line)

Results

We have estimated the expected exclusion limit at 95% confidence level (CL) for for different masses using the modified frequentist approach in the asymptotic approximation [67-69]. Systematic uncertainties related to the trigger (2%) and luminosity measurement (1.6%) have been included in the binned likelihood template fit of the spectrum as nuisance parameters with a log-normal prior distribution [52]. No uncertainties related to the shape of the distribution have been included. As shown in Fig. 3b for a benchmark , the LHC with full Run 2 luminosity is expected to claim the evidence (exclusion) of a leptophobic boson with SVJ signature and SM couplings up to masses of  TeV (4.5 TeV). We estimate that adding the requirement on the di-lepton invariant mass allows to reach the discovery of the boson up to  TeV and improve the exclusion up to more than 5 TeV. The sensitivity to the signal diminishes with higher values of since the missing momentum tends to be less and less aligned with the jet axis. Moreover, as shown in Fig. 3b, the sensitivity of the hadronic SVJ search is from one up to two orders of magnitude worse with respect to a SVJ-dedicated search. We have verified that this loss in sensitivity of the hadronic analysis holds for all values of .

Discussion and conclusions

This Letter proposed a new search strategy for the discovery of confining hidden sectors giving rise to semi-visible jets with non-isolated prompt lepton pairs. We have introduced a simplified model based on two messenger bosons separated by a large mass gap to allow leptonic decays of the composite DM. The phase space of the SVJ signal is expected to be loosely constrained by the existing searches. We have shown that the fully hadronic SVJ s-channel search has poor sensitivity to the SVJ signature due to the mini-isolation lepton veto. Remaining agnostic on the shapes and number of di-lepton resonances produced by the dark hadrons decays, we provided expected exclusion limits performing a bump hunt in the di-jet transverse mass. The proposed search can claim the evidence (exclude) the heavier mediator up to masses of 3.5 TeV (4.5 TeV) with . We have estimated that selecting events in the mass range around the expected di-lepton resonance the analysis can achieve the discovery up to masses of 3.5 TeV and improve the exclusion up to more than 5 TeV. The sensitivity to higher values of can be significantly enhanced by exploiting the resonant shape of the di-lepton spectrum. Further extensions of the current study on SVJ can go in two main directions. On the one hand, from a phenomenological perspective, one can study signatures where dark pseudo-scalars can decay through the portal to leptons via a mass insertion. Or, it would be worth to investigate signatures where the dark hadrons have sizable lifetimes. In this last case, the main background is instrumental. If the displacement is larger than the tracker volume, no track parameterization is available to treat this case with the current fast simulation tools. On the other hand, for the prompt signature, one can develop dedicated taggers for SVJ exploiting the additional substructure information related to the leptons. In this direction, a classifier exploiting both standard jet substructure and other variables capturing mutual relations between the leptons, such as the inter-isolation variable proposed here, is expected to improve the signal-to-background discrimination and the sensitivity of the analysis drastically. Another possibility is to adopt signal agnostic strategies based on anomaly detection techniques [70] to identify leptons-enriched semi-visible jets. Finally, the model proposed in this Letter allows also for a low mass production mechanism of leptons-enriched semi-visible jets where dark quarks come directly from the boson. Current limitations imposed by the trigger selection strategy require the development of dedicated algorithms to probe this production channel. In addition, the boosted event topology, resulting from high momentum and low mass of , would lead the production of two collimated semi-visible jets, appearing as merged into a single large jet. This topology requires a dedicated reconstruction strategy that is not addressed in this Letter.
  7 in total

1.  Semivisible Jets: Dark Matter Undercover at the LHC.

Authors:  Timothy Cohen; Mariangela Lisanti; Hou Keong Lou
Journal:  Phys Rev Lett       Date:  2015-10-23       Impact factor: 9.161

2.  Natural electroweak breaking from a mirror symmetry.

Authors:  Z Chacko; Hock-Seng Goh; Roni Harnik
Journal:  Phys Rev Lett       Date:  2006-06-14       Impact factor: 9.161

3.  Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy.

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A Rinkevicius; P Sellers; N Skhirtladze; M Snowball; J Yelton; M Zakaria; V Gaultney; L M Lebolo; S Linn; P Markowitz; G Martinez; J L Rodriguez; J R Adams; T Adams; A Askew; J Bochenek; J Chen; B Diamond; S V Gleyzer; J Haas; S Hagopian; V Hagopian; M Jenkins; K F Johnson; H Prosper; V Veeraraghavan; M Weinberg; M M Baarmand; B Dorney; M Hohlmann; H Kalakhety; I Vodopiyanov; M R Adams; I M Anghel; L Apanasevich; Y Bai; V E Bazterra; R R Betts; I Bucinskaite; J Callner; R Cavanaugh; C Dragoiu; O Evdokimov; L Gauthier; C E Gerber; S Hamdan; D J Hofman; S Khalatyan; F Lacroix; M Malek; C O'Brien; C Silkworth; D Strom; N Varelas; U Akgun; E A Albayrak; B Bilki; W Clarida; F Duru; S Griffiths; J-P Merlo; H Mermerkaya; A Mestvirishvili; A Moeller; J Nachtman; C R Newsom; E Norbeck; Y Onel; F Ozok; S Sen; E Tiras; J Wetzel; T Yetkin; K Yi; B A Barnett; B Blumenfeld; S Bolognesi; D Fehling; G Giurgiu; A V Gritsan; Z J Guo; G Hu; P Maksimovic; S Rappoccio; M Swartz; A Whitbeck; P Baringer; A Bean; G Benelli; O Grachov; R P Kenny Iii; M Murray; D Noonan; S Sanders; R Stringer; G Tinti; J S Wood; V Zhukova; A F Barfuss; T Bolton; I Chakaberia; A Ivanov; S Khalil; M Makouski; Y Maravin; S Shrestha; I Svintradze; J Gronberg; D Lange; D Wright; A Baden; M Boutemeur; B Calvert; S C Eno; J A Gomez; N J Hadley; R G Kellogg; M Kirn; T Kolberg; Y Lu; M Marionneau; A C Mignerey; K Pedro; A Peterman; A Skuja; J Temple; M B Tonjes; S C Tonwar; E Twedt; G Bauer; J Bendavid; W Busza; E Butz; I A Cali; M Chan; V Dutta; G Gomez Ceballos; M Goncharov; K A Hahn; Y Kim; M Klute; W Li; P D Luckey; T Ma; S Nahn; C Paus; D Ralph; C Roland; G Roland; M Rudolph; G S F Stephans; F Stöckli; K Sumorok; K Sung; D Velicanu; E A Wenger; R Wolf; B Wyslouch; S Xie; M Yang; Y Yilmaz; A S Yoon; M Zanetti; S I Cooper; P Cushman; B Dahmes; A De Benedetti; G Franzoni; A Gude; J Haupt; S C Kao; K Klapoetke; Y Kubota; J Mans; N Pastika; R Rusack; M Sasseville; A Singovsky; N Tambe; J Turkewitz; L M Cremaldi; R Kroeger; L Perera; R Rahmat; D A Sanders; E Avdeeva; K Bloom; S Bose; J Butt; D R Claes; A Dominguez; M Eads; P Jindal; J Keller; I Kravchenko; J Lazo-Flores; H Malbouisson; S Malik; G R Snow; U Baur; A Godshalk; I Iashvili; S Jain; A Kharchilava; A Kumar; S P Shipkowski; K Smith; G Alverson; E Barberis; D Baumgartel; M Chasco; J Haley; D Nash; D Trocino; D Wood; J Zhang; A Anastassov; A Kubik; N Mucia; N Odell; R A Ofierzynski; B Pollack; A Pozdnyakov; M Schmitt; S Stoynev; M Velasco; S Won; L Antonelli; D Berry; A Brinkerhoff; M Hildreth; C Jessop; D J Karmgard; J Kolb; K Lannon; W Luo; S Lynch; N Marinelli; D M Morse; T Pearson; R Ruchti; J Slaunwhite; N Valls; M Wayne; M Wolf; B Bylsma; L S Durkin; A Hart; C Hill; R Hughes; K Kotov; T Y Ling; D Puigh; M Rodenburg; C Vuosalo; G Williams; B L Winer; N Adam; E Berry; P Elmer; D Gerbaudo; V Halyo; P Hebda; J Hegeman; A Hunt; D Lopes Pegna; P Lujan; D Marlow; T Medvedeva; M Mooney; J Olsen; P Piroué; X Quan; A Raval; H Saka; D Stickland; C Tully; J S Werner; A Zuranski; J G Acosta; E Brownson; X T Huang; A Lopez; H Mendez; S Oliveros; J E Ramirez Vargas; A Zatserklyaniy; E Alagoz; V E Barnes; D Benedetti; G Bolla; D Bortoletto; M De Mattia; A Everett; Z Hu; M Jones; O Koybasi; M Kress; A T Laasanen; N Leonardo; V Maroussov; P Merkel; D H Miller; N Neumeister; I Shipsey; D Silvers; A Svyatkovskiy; M Vidal Marono; H D Yoo; J Zablocki; Y Zheng; S Guragain; N Parashar; A Adair; C Boulahouache; V Cuplov; K M Ecklund; F J M Geurts; B P Padley; R Redjimi; J Roberts; J Zabel; B Betchart; A Bodek; Y S Chung; R Covarelli; P de Barbaro; R Demina; Y Eshaq; A Garcia-Bellido; P Goldenzweig; Y Gotra; J Han; A Harel; S Korjenevski; D C Miner; D Vishnevskiy; M Zielinski; A Bhatti; R Ciesielski; L Demortier; K Goulianos; G Lungu; S Malik; C Mesropian; S Arora; A Barker; J P Chou; C Contreras-Campana; E Contreras-Campana; D Duggan; D Ferencek; Y Gershtein; R Gray; E Halkiadakis; D Hidas; A Lath; S Panwalkar; M Park; R Patel; V Rekovic; A Richards; J Robles; K Rose; S Salur; S Schnetzer; C Seitz; S Somalwar; R Stone; S Thomas; G Cerizza; M Hollingsworth; S Spanier; Z C Yang; A York; R Eusebi; W Flanagan; J Gilmore; T Kamon; V Khotilovich; R Montalvo; I Osipenkov; Y Pakhotin; A Perloff; J Roe; A Safonov; T Sakuma; S Sengupta; I Suarez; A Tatarinov; D Toback; N Akchurin; J Damgov; P R Dudero; C Jeong; K Kovitanggoon; S W Lee; T Libeiro; Y Roh; I Volobouev; E Appelt; D Engh; C Florez; S Greene; A Gurrola; W Johns; C Johnston; P Kurt; C Maguire; A Melo; P Sheldon; B Snook; S Tuo; J Velkovska; M W Arenton; M Balazs; S Boutle; B Cox; B Francis; J Goodell; R Hirosky; A Ledovskoy; C Lin; C Neu; J Wood; R Yohay; S Gollapinni; R Harr; P E Karchin; C Kottachchi Kankanamge Don; P Lamichhane; A Sakharov; M Anderson; M Bachtis; D Belknap; L Borrello; D Carlsmith; M Cepeda; S Dasu; L Gray; K S Grogg; M Grothe; R Hall-Wilton; M Herndon; A Hervé; P Klabbers; J Klukas; A Lanaro; C Lazaridis; J Leonard; R Loveless; A Mohapatra; I Ojalvo; F Palmonari; G A Pierro; I Ross; A Savin; W H Smith; J Swanson
Journal:  Phys Rev Lett       Date:  2012-08-16       Impact factor: 9.161

4.  Search for A^{'}→μ^{+}μ^{-} Decays.

Authors:  R Aaij; C Abellán Beteta; T Ackernley; B Adeva; M Adinolfi; H Afsharnia; C A Aidala; S Aiola; Z Ajaltouni; S Akar; P Albicocco; J Albrecht; F Alessio; M Alexander; A Alfonso Albero; G Alkhazov; P Alvarez Cartelle; A A Alves; S Amato; Y Amhis; L An; L Anderlini; G Andreassi; M Andreotti; F Archilli; J Arnau Romeu; A Artamonov; M Artuso; K Arzymatov; E Aslanides; M Atzeni; B Audurier; S Bachmann; J J Back; S Baker; V Balagura; W Baldini; A Baranov; R J Barlow; S Barsuk; W Barter; M Bartolini; F Baryshnikov; G Bassi; V Batozskaya; B Batsukh; A Battig; V Battista; A Bay; M Becker; F Bedeschi; I Bediaga; A Beiter; L J Bel; V Belavin; S Belin; N Beliy; V Bellee; K Belous; I Belyaev; G Bencivenni; E Ben-Haim; S Benson; S Beranek; A Berezhnoy; R Bernet; D Berninghoff; H C Bernstein; E Bertholet; A Bertolin; C Betancourt; F Betti; M O Bettler; Ia Bezshyiko; S Bhasin; J Bhom; M S Bieker; S Bifani; P Billoir; A Bizzeti; M Bjørn; M P Blago; T Blake; F Blanc; S Blusk; D Bobulska; V Bocci; O Boente Garcia; T Boettcher; A Boldyrev; A Bondar; N Bondar; S Borghi; M Borisyak; M Borsato; J T Borsuk; T J V Bowcock; C Bozzi; S Braun; A Brea Rodriguez; M Brodski; J Brodzicka; A Brossa Gonzalo; D Brundu; E Buchanan; A Buonaura; C Burr; A Bursche; J S Butter; J Buytaert; W Byczynski; S Cadeddu; H Cai; R Calabrese; L Calero Diaz; S Cali; R Calladine; M Calvi; M Calvo Gomez; A Camboni; P Campana; D H Campora Perez; L Capriotti; A Carbone; G Carboni; R Cardinale; A Cardini; P Carniti; K Carvalho Akiba; A Casais Vidal; G Casse; M Cattaneo; G Cavallero; R Cenci; J Cerasoli; M G Chapman; M Charles; Ph Charpentier; G Chatzikonstantinidis; M Chefdeville; V Chekalina; C Chen; S Chen; A Chernov; S-G Chitic; V Chobanova; M Chrzaszcz; A Chubykin; P Ciambrone; M F Cicala; X Cid Vidal; G Ciezarek; F Cindolo; P E L Clarke; M Clemencic; H V Cliff; J Closier; J L Cobbledick; V Coco; J A B Coelho; J Cogan; E Cogneras; L Cojocariu; P Collins; T Colombo; A Comerma-Montells; A Contu; N Cooke; G Coombs; S Coquereau; G Corti; C M Costa Sobral; B Couturier; D C Craik; J Crkovska; A Crocombe; M Cruz Torres; R Currie; C L Da Silva; E Dall'Occo; J Dalseno; C D'Ambrosio; A Danilina; P d'Argent; A Davis; O De Aguiar Francisco; K De Bruyn; S De Capua; M De Cian; J M De Miranda; L De Paula; M De Serio; P De Simone; J A de Vries; C T Dean; W Dean; D Decamp; L Del Buono; B Delaney; H-P Dembinski; M Demmer; A Dendek; V Denysenko; D Derkach; O Deschamps; F Desse; F Dettori; B Dey; A Di Canto; P Di Nezza; S Didenko; H Dijkstra; F Dordei; M Dorigo; A C Dos Reis; L Douglas; A Dovbnya; K Dreimanis; M W Dudek; L Dufour; G Dujany; P Durante; J M Durham; D Dutta; R Dzhelyadin; M Dziewiecki; A Dziurda; A Dzyuba; S Easo; U Egede; V Egorychev; S Eidelman; S Eisenhardt; R Ekelhof; S Ek-In; L Eklund; S Ely; A Ene; S Escher; S Esen; T Evans; A Falabella; J Fan; N Farley; S Farry; D Fazzini; M Féo; P Fernandez Declara; A Fernandez Prieto; F Ferrari; L Ferreira Lopes; F Ferreira Rodrigues; S Ferreres Sole; M Ferrillo; M Ferro-Luzzi; S Filippov; R A Fini; M Fiorini; M Firlej; K M Fischer; C Fitzpatrick; T Fiutowski; F Fleuret; M Fontana; F Fontanelli; R Forty; V Franco Lima; M Franco Sevilla; M Frank; C Frei; D A Friday; J Fu; M Fuehring; W Funk; E Gabriel; A Gallas Torreira; D Galli; S Gallorini; S Gambetta; Y Gan; M Gandelman; P Gandini; Y Gao; L M Garcia Martin; J García Pardiñas; B Garcia Plana; F A Garcia Rosales; J Garra Tico; L Garrido; D Gascon; C Gaspar; D Gerick; E Gersabeck; M Gersabeck; T Gershon; D Gerstel; Ph Ghez; V Gibson; A Gioventù; O G Girard; P Gironella Gironell; L Giubega; C Giugliano; K Gizdov; V V Gligorov; C Göbel; D Golubkov; A Golutvin; A Gomes; P Gorbounov; I V Gorelov; C Gotti; E Govorkova; J P Grabowski; R Graciani Diaz; T Grammatico; L A Granado Cardoso; E Graugés; E Graverini; G Graziani; A Grecu; R Greim; P Griffith; L Grillo; L Gruber; B R Gruberg Cazon; C Gu; E Gushchin; A Guth; Yu Guz; T Gys; T Hadavizadeh; G Haefeli; C Haen; S C Haines; P M Hamilton; Q Han; X Han; T H Hancock; S Hansmann-Menzemer; N Harnew; T Harrison; R Hart; C Hasse; M Hatch; J He; M Hecker; K Heijhoff; K Heinicke; A Heister; A M Hennequin; K Hennessy; L Henry; J Heuel; A Hicheur; R Hidalgo Charman; D Hill; M Hilton; P H Hopchev; J Hu; W Hu; W Huang; W Hulsbergen; T Humair; R J Hunter; M Hushchyn; D Hutchcroft; D Hynds; P Ibis; M Idzik; P Ilten; A Inglessi; A Inyakin; K Ivshin; R Jacobsson; S Jakobsen; J Jalocha; E Jans; B K Jashal; A Jawahery; V Jevtic; F Jiang; M John; D Johnson; C R Jones; B Jost; N Jurik; S Kandybei; M Karacson; J M Kariuki; N Kazeev; M Kecke; F Keizer; M Kelsey; M Kenzie; T Ketel; B Khanji; A Kharisova; K E Kim; T Kirn; V S Kirsebom; S Klaver; K Klimaszewski; S Koliiev; A Kondybayeva; A Konoplyannikov; P Kopciewicz; R Kopecna; P Koppenburg; I Kostiuk; O Kot; S Kotriakhova; L Kravchuk; R D Krawczyk; M Kreps; F Kress; S Kretzschmar; P Krokovny; W Krupa; W Krzemien; W Kucewicz; M Kucharczyk; V Kudryavtsev; H S Kuindersma; G J Kunde; A K Kuonen; T Kvaratskheliya; D Lacarrere; G Lafferty; A Lai; D Lancierini; J J Lane; G Lanfranchi; C Langenbruch; T Latham; F Lazzari; C Lazzeroni; R Le Gac; R Lefèvre; A Leflat; F Lemaitre; O Leroy; T Lesiak; B Leverington; H Li; X Li; Y Li; Z Li; X Liang; R Lindner; F Lionetto; V Lisovskyi; G Liu; X Liu; D Loh; A Loi; J Lomba Castro; I Longstaff; J H Lopes; G Loustau; G H Lovell; Y Lu; D Lucchesi; M Lucio Martinez; Y Luo; A Lupato; E Luppi; O Lupton; A Lusiani; X Lyu; S Maccolini; F Machefert; F Maciuc; V Macko; P Mackowiak; S Maddrell-Mander; L R Madhan Mohan; O Maev; A Maevskiy; K Maguire; D Maisuzenko; M W Majewski; S Malde; B Malecki; A Malinin; T Maltsev; H Malygina; G Manca; G Mancinelli; R Manera Escalero; D Manuzzi; D Marangotto; J Maratas; J F Marchand; U Marconi; S Mariani; C Marin Benito; M Marinangeli; P Marino; J Marks; P J Marshall; G Martellotti; L Martinazzoli; M Martinelli; D Martinez Santos; F Martinez Vidal; A Massafferri; M Materok; R Matev; A Mathad; Z Mathe; V Matiunin; C Matteuzzi; K R Mattioli; A Mauri; E Maurice; M McCann; L Mcconnell; A McNab; R McNulty; J V Mead; B Meadows; C Meaux; G Meier; N Meinert; D Melnychuk; S Meloni; M Merk; A Merli; M Mikhasenko; D A Milanes; E Millard; M-N Minard; O Mineev; L Minzoni; S E Mitchell; B Mitreska; D S Mitzel; A Mödden; A Mogini; R D Moise; T Mombächer; I A Monroy; S Monteil; M Morandin; G Morello; M J Morello; J Moron; A B Morris; A G Morris; R Mountain; H Mu; F Muheim; M Mukherjee; M Mulder; D Müller; K Müller; V Müller; C H Murphy; D Murray; P Muzzetto; P Naik; T Nakada; R Nandakumar; A Nandi; T Nanut; I Nasteva; M Needham; N Neri; S Neubert; N Neufeld; R Newcombe; T D Nguyen; C Nguyen-Mau; E M Niel; S Nieswand; N Nikitin; N S Nolte; C Nunez; A Oblakowska-Mucha; V Obraztsov; S Ogilvy; D P O'Hanlon; R Oldeman; C J G Onderwater; J D Osborn; A Ossowska; J M Otalora Goicochea; T Ovsiannikova; P Owen; A Oyanguren; P R Pais; T Pajero; A Palano; M Palutan; G Panshin; A Papanestis; M Pappagallo; L L Pappalardo; C Pappenheimer; W Parker; C Parkes; G Passaleva; A Pastore; M Patel; C Patrignani; A Pearce; A Pellegrino; M Pepe Altarelli; S Perazzini; D Pereima; P Perret; L Pescatore; K Petridis; A Petrolini; A Petrov; S Petrucci; M Petruzzo; B Pietrzyk; G Pietrzyk; M Pikies; M Pili; D Pinci; J Pinzino; F Pisani; A Piucci; V Placinta; S Playfer; J Plews; M Plo Casasus; F Polci; M Poli Lener; M Poliakova; A Poluektov; N Polukhina; I Polyakov; E Polycarpo; G J Pomery; S Ponce; A Popov; D Popov; S Poslavskii; K Prasanth; L Promberger; C Prouve; V Pugatch; A Puig Navarro; H Pullen; G Punzi; W Qian; J Qin; R Quagliani; B Quintana; N V Raab; R I Rabadan Trejo; B Rachwal; J H Rademacker; M Rama; M Ramos Pernas; M S Rangel; F Ratnikov; G Raven; M Ravonel Salzgeber; M Reboud; F Redi; S Reichert; F Reiss; C Remon Alepuz; Z Ren; V Renaudin; S Ricciardi; S Richards; K Rinnert; P Robbe; A Robert; A B Rodrigues; E Rodrigues; J A Rodriguez Lopez; M Roehrken; S Roiser; A Rollings; V Romanovskiy; M Romero Lamas; A Romero Vidal; J D Roth; M Rotondo; M S Rudolph; T Ruf; J Ruiz Vidal; J Ryzka; J J Saborido Silva; N Sagidova; B Saitta; C Sanchez Gras; C Sanchez Mayordomo; B Sanmartin Sedes; R Santacesaria; C Santamarina Rios; M Santimaria; E Santovetti; G Sarpis; A Sarti; C Satriano; A Satta; M Saur; D Savrina; L G Scantlebury Smead; S Schael; M Schellenberg; M Schiller; H Schindler; M Schmelling; T Schmelzer; B Schmidt; O Schneider; A Schopper; H F Schreiner; M Schubiger; S Schulte; M H Schune; R Schwemmer; B Sciascia; A Sciubba; S Sellam; A Semennikov; A Sergi; N Serra; J Serrano; L Sestini; A Seuthe; P Seyfert; D M Shangase; M Shapkin; T Shears; L Shekhtman; V Shevchenko; E Shmanin; J D Shupperd; B G Siddi; R Silva Coutinho; L Silva de Oliveira; G Simi; S Simone; I Skiba; N Skidmore; T Skwarnicki; M W Slater; J G Smeaton; A Smetkina; E Smith; I T Smith; M Smith; A Snoch; M Soares; L Soares Lavra; M D Sokoloff; F J P Soler; B Souza De Paula; B Spaan; E Spadaro Norella; P Spradlin; F Stagni; M Stahl; S Stahl; P Stefko; S Stefkova; O Steinkamp; S Stemmle; O Stenyakin; M Stepanova; H Stevens; S Stone; S Stracka; M E Stramaglia; M Straticiuc; S Strokov; J Sun; L Sun; Y Sun; P Svihra; K Swientek; A Szabelski; T Szumlak; M Szymanski; S Taneja; Z Tang; T Tekampe; G Tellarini; F Teubert; E Thomas; K A Thomson; M J Tilley; V Tisserand; S T'Jampens; M Tobin; S Tolk; L Tomassetti; D Tonelli; D Y Tou; E Tournefier; M Traill; M T Tran; C Trippl; A Trisovic; A Tsaregorodtsev; G Tuci; A Tully; N Tuning; A Ukleja; A Usachov; A Ustyuzhanin; U Uwer; A Vagner; V Vagnoni; A Valassi; G Valenti; M van Beuzekom; H Van Hecke; E van Herwijnen; C B Van Hulse; J van Tilburg; M van Veghel; R Vazquez Gomez; P Vazquez Regueiro; C Vázquez Sierra; S Vecchi; J J Velthuis; M Veltri; A Venkateswaran; M Vernet; M Veronesi; M Vesterinen; J V Viana Barbosa; D Vieira; M Vieites Diaz; H Viemann; X Vilasis-Cardona; A Vitkovskiy; V Volkov; A Vollhardt; D Vom Bruch; A Vorobyev; V Vorobyev; N Voropaev; R Waldi; J Walsh; J Wang; J Wang; J Wang; M Wang; Y Wang; Z Wang; D R Ward; H M Wark; N K Watson; D Websdale; A Weiden; C Weisser; B D C Westhenry; D J White; M Whitehead; D Wiedner; G Wilkinson; M Wilkinson; I Williams; M Williams; M R J Williams; T Williams; F F Wilson; M Winn; W Wislicki; M Witek; G Wormser; S A Wotton; H Wu; K Wyllie; Z Xiang; D Xiao; Y Xie; H Xing; A Xu; L Xu; M Xu; Q Xu; Z Xu; Z Xu; Z Yang; Z Yang; Y Yao; L E Yeomans; H Yin; J Yu; X Yuan; O Yushchenko; K A Zarebski; M Zavertyaev; M Zdybal; M Zeng; D Zhang; L Zhang; S Zhang; W C Zhang; Y Zhang; A Zhelezov; Y Zheng; X Zhou; Y Zhou; X Zhu; V Zhukov; J B Zonneveld; S Zucchelli
Journal:  Phys Rev Lett       Date:  2020-01-31       Impact factor: 9.161

5.  Search for a Narrow Resonance Lighter than 200 GeV Decaying to a Pair of Muons in Proton-Proton Collisions at sqrt[s]=13  TeV.

Authors:  A M Sirunyan; A Tumasyan; W Adam; F Ambrogi; T Bergauer; M Dragicevic; J Erö; A Escalante Del Valle; M Flechl; R Frühwirth; M Jeitler; N Krammer; I Krätschmer; D Liko; T Madlener; I Mikulec; N Rad; J Schieck; R Schöfbeck; M Spanring; D Spitzbart; W Waltenberger; C-E Wulz; M Zarucki; V Drugakov; V Mossolov; J Suarez Gonzalez; M R Darwish; E A De Wolf; D Di Croce; X Janssen; A Lelek; M Pieters; H Rejeb Sfar; H Van Haevermaet; P Van Mechelen; S Van Putte; N Van Remortel; F Blekman; E S Bols; S S Chhibra; J D'Hondt; J De Clercq; D Lontkovskyi; S Lowette; I Marchesini; S Moortgat; Q Python; K Skovpen; S Tavernier; W Van Doninck; P Van Mulders; D Beghin; B Bilin; B Clerbaux; G De Lentdecker; H Delannoy; B Dorney; L Favart; A Grebenyuk; A K Kalsi; A Popov; N Postiau; E Starling; L Thomas; C Vander Velde; P Vanlaer; D Vannerom; T Cornelis; D Dobur; I Khvastunov; M Niedziela; C Roskas; M Tytgat; W Verbeke; B Vermassen; M Vit; O Bondu; G Bruno; C Caputo; P David; C Delaere; M Delcourt; A Giammanco; V Lemaitre; J Prisciandaro; A Saggio; M Vidal Marono; P Vischia; J Zobec; F L Alves; G A Alves; G Correia Silva; C Hensel; A Moraes; P Rebello Teles; E Belchior Batista Das Chagas; W Carvalho; J Chinellato; E Coelho; E M Da Costa; G G Da Silveira; D De Jesus Damiao; C De Oliveira Martins; S Fonseca De Souza; L M Huertas Guativa; H Malbouisson; J Martins; D Matos Figueiredo; M Medina Jaime; M Melo De Almeida; C Mora Herrera; L Mundim; H Nogima; W L Prado Da Silva; L J Sanchez Rosas; A Santoro; A Sznajder; M Thiel; E J Tonelli Manganote; F Torres Da Silva De Araujo; A Vilela Pereira; C A Bernardes; L Calligaris; T R Fernandez Perez Tomei; E M Gregores; D S Lemos; P G Mercadante; S F Novaes; Sandra S Padula; A Aleksandrov; G Antchev; R Hadjiiska; P Iaydjiev; M Misheva; M Rodozov; M Shopova; G Sultanov; M Bonchev; A Dimitrov; T Ivanov; L Litov; B Pavlov; P Petkov; W Fang; X Gao; L Yuan; M Ahmad; Z Hu; Y Wang; G M Chen; H S Chen; M Chen; C H Jiang; D Leggat; H Liao; Z Liu; A Spiezia; J Tao; E Yazgan; H Zhang; S Zhang; J Zhao; A Agapitos; Y Ban; G Chen; A Levin; J Li; L Li; Q Li; Y Mao; S J Qian; D Wang; Q Wang; M Xiao; C Avila; A Cabrera; C Florez; C F González Hernández; M A Segura Delgado; J Mejia Guisao; J D Ruiz Alvarez; C A Salazar González; N Vanegas Arbelaez; D Giljanović; N Godinovic; D Lelas; I Puljak; T Sculac; Z Antunovic; M Kovac; V Brigljevic; D Ferencek; K Kadija; B Mesic; M Roguljic; A Starodumov; T Susa; M W Ather; A Attikis; E Erodotou; A Ioannou; M Kolosova; S Konstantinou; G Mavromanolakis; J Mousa; C Nicolaou; F Ptochos; P A Razis; H Rykaczewski; D Tsiakkouri; M Finger; M Finger; A Kveton; J Tomsa; E Ayala; E Carrera Jarrin; Y Assran; S Elgammal; S Bhowmik; A Carvalho Antunes De Oliveira; R K Dewanjee; K Ehataht; M Kadastik; M Raidal; C Veelken; P Eerola; L Forthomme; H Kirschenmann; K Osterberg; M Voutilainen; F Garcia; J Havukainen; J K Heikkilä; V Karimäki; M S Kim; R Kinnunen; T Lampén; K Lassila-Perini; S Laurila; S Lehti; T Lindén; P Luukka; 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B Klima; M J Kortelainen; B Kreis; S Lammel; J Lewis; D Lincoln; R Lipton; M Liu; T Liu; J Lykken; K Maeshima; J M Marraffino; D Mason; P McBride; P Merkel; S Mrenna; S Nahn; V O'Dell; V Papadimitriou; K Pedro; C Pena; G Rakness; F Ravera; L Ristori; B Schneider; E Sexton-Kennedy; N Smith; A Soha; W J Spalding; L Spiegel; S Stoynev; J Strait; N Strobbe; L Taylor; S Tkaczyk; N V Tran; L Uplegger; E W Vaandering; C Vernieri; R Vidal; M Wang; H A Weber; D Acosta; P Avery; D Bourilkov; A Brinkerhoff; L Cadamuro; V Cherepanov; F Errico; R D Field; S V Gleyzer; D Guerrero; B M Joshi; M Kim; J Konigsberg; A Korytov; K H Lo; K Matchev; N Menendez; G Mitselmakher; D Rosenzweig; K Shi; J Wang; S Wang; X Zuo; Y R Joshi; T Adams; A Askew; S Hagopian; V Hagopian; K F Johnson; R Khurana; T Kolberg; G Martinez; T Perry; H Prosper; C Schiber; R Yohay; J Zhang; M M Baarmand; M Hohlmann; D Noonan; M Rahmani; M Saunders; F Yumiceva; M R Adams; L Apanasevich; R R Betts; R Cavanaugh; X Chen; S Dittmer; O Evdokimov; C E Gerber; D A Hangal; D J Hofman; C Mills; T Roy; M B Tonjes; N Varelas; J Viinikainen; H Wang; X Wang; Z Wu; M Alhusseini; B Bilki; K Dilsiz; S Durgut; R P Gandrajula; M Haytmyradov; V Khristenko; O K Köseyan; J-P Merlo; A Mestvirishvili; A Moeller; J Nachtman; H Ogul; Y Onel; F Ozok; A Penzo; C Snyder; E Tiras; J Wetzel; B Blumenfeld; A Cocoros; N Eminizer; A V Gritsan; W T Hung; S Kyriacou; P Maksimovic; J Roskes; M Swartz; C Baldenegro Barrera; P Baringer; A Bean; S Boren; J Bowen; A Bylinkin; T Isidori; S Khalil; J King; G Krintiras; A Kropivnitskaya; C Lindsey; D Majumder; W Mcbrayer; N Minafra; M Murray; C Rogan; C Royon; S Sanders; E Schmitz; J D Tapia Takaki; Q Wang; J Williams; G Wilson; S Duric; A Ivanov; K Kaadze; D Kim; Y Maravin; D R Mendis; T Mitchell; A Modak; A Mohammadi; F Rebassoo; D Wright; A Baden; O Baron; A Belloni; S C Eno; Y Feng; N J Hadley; S Jabeen; G Y Jeng; R G Kellogg; A C Mignerey; S Nabili; F Ricci-Tam; M Seidel; Y H Shin; A Skuja; S C Tonwar; K Wong; 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T Gunter; K A Hahn; N Odell; M H Schmitt; K Sung; M Trovato; M Velasco; R Bucci; N Dev; R Goldouzian; M Hildreth; K Hurtado Anampa; C Jessop; D J Karmgard; K Lannon; W Li; N Loukas; N Marinelli; I Mcalister; F Meng; Y Musienko; R Ruchti; P Siddireddy; G Smith; S Taroni; M Wayne; A Wightman; M Wolf; A Woodard; J Alimena; B Bylsma; L S Durkin; B Francis; C Hill; W Ji; A Lefeld; T Y Ling; B L Winer; G Dezoort; P Elmer; J Hardenbrook; N Haubrich; S Higginbotham; A Kalogeropoulos; S Kwan; D Lange; M T Lucchini; J Luo; D Marlow; K Mei; I Ojalvo; J Olsen; C Palmer; P Piroué; D Stickland; C Tully; S Malik; S Norberg; A Barker; V E Barnes; S Das; L Gutay; M Jones; A W Jung; A Khatiwada; B Mahakud; D H Miller; G Negro; N Neumeister; C C Peng; S Piperov; H Qiu; J F Schulte; N Trevisani; F Wang; R Xiao; W Xie; T Cheng; J Dolen; N Parashar; U Behrens; K M Ecklund; S Freed; F J M Geurts; M Kilpatrick; Arun Kumar; W Li; B P Padley; R Redjimi; J Roberts; J Rorie; W Shi; A G Stahl Leiton; Z Tu; A Zhang; A Bodek; P de Barbaro; R Demina; J L Dulemba; C Fallon; T Ferbel; M Galanti; A Garcia-Bellido; O Hindrichs; A Khukhunaishvili; E Ranken; R Taus; B Chiarito; J P Chou; A Gandrakota; Y Gershtein; E Halkiadakis; A Hart; M Heindl; E Hughes; S Kaplan; I Laflotte; A Lath; R Montalvo; K Nash; M Osherson; H Saka; S Salur; S Schnetzer; S Somalwar; R Stone; S Thomas; H Acharya; A G Delannoy; S Spanier; O Bouhali; M Dalchenko; M De Mattia; A Delgado; S Dildick; R Eusebi; J Gilmore; T Huang; T Kamon; H Kim; S Luo; S Malhotra; D Marley; R Mueller; D Overton; L Perniè; D Rathjens; A Safonov; N Akchurin; J Damgov; F De Guio; V Hegde; S Kunori; K Lamichhane; S W Lee; T Mengke; S Muthumuni; T Peltola; S Undleeb; I Volobouev; Z Wang; A Whitbeck; S Greene; A Gurrola; R Janjam; W Johns; C Maguire; A Melo; H Ni; K Padeken; F Romeo; P Sheldon; S Tuo; J Velkovska; M Verweij; M W Arenton; P Barria; B Cox; G Cummings; J Hakala; R Hirosky; M Joyce; A Ledovskoy; C Neu; B Tannenwald; Y Wang; E Wolfe; F Xia; R Harr; P E Karchin; N Poudyal; J Sturdy; P Thapa; T Bose; J Buchanan; C Caillol; D Carlsmith; S Dasu; I De Bruyn; L Dodd; C Galloni; H He; M Herndon; A Hervé; U Hussain; A Lanaro; A Loeliger; K Long; R Loveless; J Madhusudanan Sreekala; D Pinna; T Ruggles; A Savin; V Sharma; W H Smith; D Teague; S Trembath-Reichert
Journal:  Phys Rev Lett       Date:  2020-04-03       Impact factor: 9.161

6.  Higher-order QCD predictions for dark matter production at the LHC in simplified models with s-channel mediators.

Authors:  Mihailo Backović; Michael Krämer; Fabio Maltoni; Antony Martini; Kentarou Mawatari; Mathieu Pellen
Journal:  Eur Phys J C Part Fields       Date:  2015-10-07       Impact factor: 4.590

7.  Search for doubly charged scalar bosons decaying into same-sign W boson pairs with the ATLAS detector.

Authors:  M Aaboud; G Aad; B Abbott; O Abdinov; B Abeloos; D K Abhayasinghe; S H Abidi; O S AbouZeid; N L Abraham; H Abramowicz; H Abreu; Y Abulaiti; B S Acharya; S Adachi; L Adamczyk; J Adelman; M Adersberger; A Adiguzel; T Adye; A A Affolder; Y Afik; C Agheorghiesei; J A Aguilar-Saavedra; F Ahmadov; G Aielli; S Akatsuka; T P A Åkesson; E Akilli; A V Akimov; G L Alberghi; J Albert; P Albicocco; M J Alconada Verzini; S Alderweireldt; M Aleksa; I N Aleksandrov; C Alexa; T Alexopoulos; M Alhroob; B Ali; G Alimonti; J Alison; S P Alkire; C Allaire; B M M Allbrooke; B W Allen; P P Allport; A Aloisio; A Alonso; F Alonso; C Alpigiani; A A Alshehri; M I Alstaty; B Alvarez Gonzalez; D Álvarez Piqueras; M G Alviggi; B T Amadio; Y Amaral Coutinho; L Ambroz; C Amelung; D Amidei; S P Amor Dos Santos; S Amoroso; C S Amrouche; C Anastopoulos; L S Ancu; N Andari; T Andeen; C F Anders; J K Anders; K J Anderson; A Andreazza; V Andrei; C R Anelli; S Angelidakis; I Angelozzi; A Angerami; A V Anisenkov; A Annovi; C Antel; M T Anthony; M Antonelli; D J A Antrim; F Anulli; M Aoki; J A Aparisi Pozo; L Aperio Bella; G Arabidze; J P Araque; V Araujo Ferraz; R Araujo Pereira; A T H Arce; R E Ardell; F A Arduh; J-F Arguin; S Argyropoulos; A J Armbruster; L J Armitage; A Armstrong; O Arnaez; H Arnold; M Arratia; O Arslan; A Artamonov; G Artoni; S Artz; S Asai; N Asbah; A Ashkenazi; E M Asimakopoulou; L Asquith; K Assamagan; R Astalos; R J Atkin; M Atkinson; N B Atlay; K Augsten; G Avolio; R Avramidou; M K Ayoub; G Azuelos; A E Baas; M J Baca; H Bachacou; K Bachas; M Backes; P Bagnaia; M Bahmani; H Bahrasemani; A J Bailey; J T Baines; M Bajic; C Bakalis; O K Baker; P J Bakker; D Bakshi Gupta; E M Baldin; P Balek; F Balli; W K Balunas; J Balz; E Banas; A Bandyopadhyay; S Banerjee; A A E Bannoura; L Barak; W M Barbe; E L Barberio; D Barberis; M Barbero; T Barillari; M-S Barisits; J Barkeloo; T Barklow; N Barlow; R Barnea; S L Barnes; B M Barnett; R M Barnett; Z Barnovska-Blenessy; A Baroncelli; G Barone; A J Barr; L Barranco Navarro; F Barreiro; J Barreiro Guimarães da Costa; R Bartoldus; A E Barton; P Bartos; A Basalaev; A Bassalat; R L Bates; S J Batista; S Batlamous; J R Batley; M Battaglia; M Bauce; F Bauer; K T Bauer; H S Bawa; J B Beacham; M D Beattie; T Beau; P H Beauchemin; P Bechtle; H C Beck; H P Beck; K Becker; M Becker; C Becot; A Beddall; A J Beddall; V A Bednyakov; M Bedognetti; C P Bee; T A Beermann; M Begalli; M Begel; A Behera; J K Behr; A S Bell; G Bella; L Bellagamba; A Bellerive; M Bellomo; P Bellos; K Belotskiy; N L Belyaev; O Benary; D Benchekroun; M Bender; N Benekos; Y Benhammou; E Benhar Noccioli; J Benitez; D P Benjamin; M Benoit; J R Bensinger; S Bentvelsen; L Beresford; M Beretta; D Berge; E Bergeaas Kuutmann; N Berger; L J Bergsten; J Beringer; S Berlendis; N R Bernard; G Bernardi; C Bernius; F U Bernlochner; T Berry; P Berta; C Bertella; G Bertoli; I A Bertram; G J Besjes; O Bessidskaia Bylund; M Bessner; N Besson; A Bethani; S Bethke; A Betti; A J Bevan; J Beyer; R M Bianchi; O Biebel; D Biedermann; R Bielski; K Bierwagen; N V Biesuz; M Biglietti; T R V Billoud; M Bindi; A Bingul; C Bini; S Biondi; M Birman; T Bisanz; J P Biswal; C Bittrich; D M Bjergaard; J E Black; K M Black; T Blazek; I Bloch; C Blocker; A Blue; U Blumenschein; Dr Blunier; G J Bobbink; V S Bobrovnikov; S S Bocchetta; A Bocci; D Boerner; D Bogavac; A G Bogdanchikov; C Bohm; V Boisvert; P Bokan; T Bold; A S Boldyrev; A E Bolz; M Bomben; M Bona; J S Bonilla; M Boonekamp; A Borisov; G Borissov; J Bortfeldt; D Bortoletto; V Bortolotto; D Boscherini; M Bosman; J D Bossio Sola; K Bouaouda; J Boudreau; E V Bouhova-Thacker; D Boumediene; C Bourdarios; S K Boutle; A Boveia; J Boyd; I R Boyko; A J Bozson; J Bracinik; N Brahimi; A Brandt; G Brandt; O Brandt; F Braren; U Bratzler; B Brau; J E Brau; W D Breaden Madden; K Brendlinger; A J Brennan; L Brenner; R Brenner; S Bressler; B Brickwedde; D L Briglin; D Britton; D Britzger; I Brock; R Brock; G Brooijmans; T Brooks; W K Brooks; E Brost; J H Broughton; P A Bruckman de Renstrom; D Bruncko; A Bruni; G Bruni; L S Bruni; S Bruno; B H Brunt; M Bruschi; N Bruscino; P Bryant; L Bryngemark; T Buanes; Q Buat; P Buchholz; A G Buckley; I A Budagov; F Buehrer; M K Bugge; O Bulekov; D Bullock; T J Burch; S Burdin; C D Burgard; A M Burger; B Burghgrave; K Burka; S Burke; I Burmeister; J T P Burr; D Büscher; V Büscher; E Buschmann; P Bussey; J M Butler; C M Buttar; J M Butterworth; P Butti; W Buttinger; A Buzatu; A R Buzykaev; G Cabras; S Cabrera Urbán; D Caforio; H Cai; V M M Cairo; O Cakir; N Calace; P Calafiura; A Calandri; G Calderini; P Calfayan; G Callea; L P Caloba; S Calvente Lopez; D Calvet; S Calvet; T P Calvet; M Calvetti; R Camacho Toro; S Camarda; P Camarri; D Cameron; R Caminal Armadans; C Camincher; S Campana; M Campanelli; A Camplani; A Campoverde; V Canale; M Cano Bret; J Cantero; T Cao; Y Cao; M D M Capeans Garrido; I Caprini; M Caprini; M Capua; R M Carbone; R Cardarelli; F C Cardillo; I Carli; T Carli; G Carlino; B T Carlson; L Carminati; R M D Carney; S Caron; E Carquin; S Carrá; G D Carrillo-Montoya; D Casadei; M P Casado; A F Casha; M Casolino; D W Casper; R Castelijn; F L Castillo; V Castillo Gimenez; N F Castro; A Catinaccio; J R Catmore; A Cattai; J Caudron; V Cavaliere; E Cavallaro; D Cavalli; M Cavalli-Sforza; V Cavasinni; E Celebi; F Ceradini; L Cerda Alberich; A S Cerqueira; A Cerri; L Cerrito; F Cerutti; A Cervelli; S A Cetin; A Chafaq; D Chakraborty; S K Chan; W S Chan; Y L Chan; J D Chapman; D G Charlton; C C Chau; C A Chavez Barajas; S Che; A Chegwidden; S Chekanov; S V Chekulaev; G A Chelkov; M A Chelstowska; C Chen; C H Chen; H Chen; J Chen; J Chen; S Chen; S J Chen; X Chen; Y Chen; Y-H Chen; H C Cheng; H J Cheng; A Cheplakov; E Cheremushkina; R Cherkaoui El Moursli; E Cheu; K Cheung; L Chevalier; V Chiarella; G Chiarelli; G Chiodini; A S Chisholm; A Chitan; I Chiu; Y H Chiu; M V Chizhov; K Choi; A R Chomont; S Chouridou; Y S Chow; V Christodoulou; M C Chu; J Chudoba; A J Chuinard; 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K De; R De Asmundis; A De Benedetti; M De Beurs; S De Castro; S De Cecco; N De Groot; P de Jong; H De la Torre; F De Lorenzi; A De Maria; D De Pedis; A De Salvo; U De Sanctis; A De Santo; K De Vasconcelos Corga; J B De Vivie De Regie; C Debenedetti; D V Dedovich; N Dehghanian; M Del Gaudio; J Del Peso; Y Delabat Diaz; D Delgove; F Deliot; C M Delitzsch; M Della Pietra; D Della Volpe; A Dell'Acqua; L Dell'Asta; M Delmastro; C Delporte; P A Delsart; D A DeMarco; S Demers; M Demichev; S P Denisov; D Denysiuk; L D'Eramo; D Derendarz; J E Derkaoui; F Derue; P Dervan; K Desch; C Deterre; K Dette; M R Devesa; P O Deviveiros; A Dewhurst; S Dhaliwal; F A Di Bello; A Di Ciaccio; L Di Ciaccio; W K Di Clemente; C Di Donato; A Di Girolamo; B Di Micco; R Di Nardo; K F Di Petrillo; A Di Simone; R Di Sipio; D Di Valentino; C Diaconu; M Diamond; F A Dias; T Dias Do Vale; M A Diaz; J Dickinson; E B Diehl; J Dietrich; S Díez Cornell; A Dimitrievska; J Dingfelder; F Dittus; F Djama; T Djobava; J I Djuvsland; M A B Do Vale; M Dobre; D Dodsworth; C Doglioni; J Dolejsi; Z Dolezal; M Donadelli; J Donini; A D'onofrio; M D'Onofrio; J Dopke; A Doria; M T Dova; A T Doyle; E Drechsler; E Dreyer; T Dreyer; Y Du; J Duarte-Campderros; F Dubinin; M Dubovsky; A Dubreuil; E Duchovni; G Duckeck; A Ducourthial; O A Ducu; D Duda; A Dudarev; A C Dudder; E M Duffield; L Duflot; M Dührssen; C Dülsen; M Dumancic; A E Dumitriu; A K Duncan; M Dunford; A Duperrin; H Duran Yildiz; M Düren; A Durglishvili; D Duschinger; B Dutta; D Duvnjak; M Dyndal; S Dysch; B S Dziedzic; C Eckardt; K M Ecker; R C Edgar; T Eifert; G Eigen; K Einsweiler; T Ekelof; M El Kacimi; R El Kosseifi; V Ellajosyula; M Ellert; F Ellinghaus; A A Elliot; N Ellis; J Elmsheuser; M Elsing; D Emeliyanov; Y Enari; J S Ennis; M B Epland; J Erdmann; A Ereditato; S Errede; M Escalier; C Escobar; O Estrada Pastor; A I Etienvre; E Etzion; H Evans; A Ezhilov; M Ezzi; F Fabbri; L Fabbri; V Fabiani; G Facini; R M Faisca Rodrigues Pereira; R M Fakhrutdinov; S Falciano; P J Falke; S Falke; J Faltova; Y Fang; M Fanti; A Farbin; A Farilla; E M Farina; T Farooque; S Farrell; S M Farrington; P Farthouat; F Fassi; P Fassnacht; D Fassouliotis; M Faucci Giannelli; A Favareto; W J Fawcett; L Fayard; O L Fedin; W Fedorko; M Feickert; S Feigl; L Feligioni; C Feng; E J Feng; M Feng; M J Fenton; A B Fenyuk; L Feremenga; J Ferrando; A Ferrari; P Ferrari; R Ferrari; D E Ferreira de Lima; A Ferrer; D Ferrere; C Ferretti; F Fiedler; A Filipčič; F Filthaut; K D Finelli; M C N Fiolhais; L Fiorini; C Fischer; W C Fisher; N Flaschel; I Fleck; P Fleischmann; R R M Fletcher; T Flick; B M Flierl; L M Flores; L R Flores Castillo; N Fomin; G T Forcolin; A Formica; F A Förster; A C Forti; A G Foster; D Fournier; H Fox; S Fracchia; P Francavilla; M Franchini; S Franchino; D Francis; L Franconi; M Franklin; M Frate; M Fraternali; D Freeborn; S M Fressard-Batraneanu; B Freund; W S Freund; D Froidevaux; J A Frost; C Fukunaga; E Fullana Torregrosa; T Fusayasu; J Fuster; O Gabizon; 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C Kourkoumelis; E Kourlitis; V Kouskoura; A B Kowalewska; R Kowalewski; T Z Kowalski; C Kozakai; W Kozanecki; A S Kozhin; V A Kramarenko; G Kramberger; D Krasnopevtsev; M W Krasny; A Krasznahorkay; D Krauss; J A Kremer; J Kretzschmar; P Krieger; K Krizka; K Kroeninger; H Kroha; J Kroll; J Kroll; J Krstic; U Kruchonak; H Krüger; N Krumnack; M C Kruse; T Kubota; S Kuday; J T Kuechler; S Kuehn; A Kugel; F Kuger; T Kuhl; V Kukhtin; R Kukla; Y Kulchitsky; S Kuleshov; Y P Kulinich; M Kuna; T Kunigo; A Kupco; T Kupfer; O Kuprash; H Kurashige; L L Kurchaninov; Y A Kurochkin; M G Kurth; E S Kuwertz; M Kuze; J Kvita; T Kwan; A La Rosa; J L La Rosa Navarro; L La Rotonda; F La Ruffa; C Lacasta; F Lacava; J Lacey; D P J Lack; H Lacker; D Lacour; E Ladygin; R Lafaye; B Laforge; T Lagouri; S Lai; S Lammers; W Lampl; E Lançon; U Landgraf; M P J Landon; M C Lanfermann; V S Lang; J C Lange; R J Langenberg; A J Lankford; F Lanni; K Lantzsch; A Lanza; A Lapertosa; S Laplace; J F Laporte; T Lari; F Lasagni Manghi; M Lassnig; T S Lau; A Laudrain; M Lavorgna; A T Law; P Laycock; M Lazzaroni; B Le; O Le Dortz; E Le Guirriec; E P Le Quilleuc; M LeBlanc; T LeCompte; F Ledroit-Guillon; C A Lee; G R Lee; L Lee; S C Lee; B Lefebvre; M Lefebvre; F Legger; C Leggett; N Lehmann; G Lehmann Miotto; W A Leight; A Leisos; M A L Leite; R Leitner; D Lellouch; B Lemmer; K J C Leney; T Lenz; B Lenzi; R Leone; S Leone; C Leonidopoulos; G Lerner; C Leroy; R Les; A A J Lesage; C G Lester; M Levchenko; J Levêque; D Levin; L J Levinson; D Lewis; B Li; C-Q Li; H Li; L Li; Q Li; Q Y Li; S Li; X Li; Y Li; Z Liang; B Liberti; A Liblong; K Lie; S Liem; A Limosani; C Y Lin; K Lin; T H Lin; R A Linck; B E Lindquist; A L Lionti; E Lipeles; A Lipniacka; M Lisovyi; T M Liss; A Lister; A M Litke; J D Little; B Liu; B L Liu; H B Liu; H Liu; J B Liu; J K K Liu; K Liu; M Liu; P Liu; Y Liu; Y L Liu; Y W Liu; M Livan; A Lleres; J Llorente Merino; S L Lloyd; C Y Lo; F Lo Sterzo; E M Lobodzinska; P Loch; A Loesle; K M Loew; T Lohse; K Lohwasser; M Lokajicek; B A Long; J D Long; R E Long; L Longo; K A Looper; J A Lopez; I Lopez Paz; A Lopez Solis; J Lorenz; N Lorenzo Martinez; M Losada; P J Lösel; X Lou; X Lou; A Lounis; J Love; P A Love; J J Lozano Bahilo; H Lu; M Lu; N Lu; Y J Lu; H J Lubatti; C Luci; A Lucotte; C Luedtke; F Luehring; I Luise; W Lukas; L Luminari; B Lund-Jensen; M S Lutz; P M Luzi; D Lynn; R Lysak; E Lytken; F Lyu; V Lyubushkin; H Ma; L L Ma; Y Ma; G Maccarrone; A Macchiolo; C M Macdonald; J Machado Miguens; D Madaffari; R Madar; W F Mader; A Madsen; N Madysa; J Maeda; K Maekawa; S Maeland; T Maeno; A S Maevskiy; V Magerl; C Maidantchik; T Maier; A Maio; O Majersky; S Majewski; Y Makida; N Makovec; B Malaescu; Pa Malecki; V P Maleev; F Malek; U Mallik; D Malon; C Malone; S Maltezos; S Malyukov; J Mamuzic; G Mancini; I Mandić; J Maneira; L Manhaes de Andrade Filho; J Manjarres Ramos; K H Mankinen; A Mann; A Manousos; B Mansoulie; J D Mansour; M Mantoani; S Manzoni; G Marceca; L March; L Marchese; G Marchiori; M Marcisovsky; C A Marin Tobon; M Marjanovic; D E Marley; F Marroquim; Z Marshall; M U F Martensson; S Marti-Garcia; C B Martin; T A Martin; V J Martin; B Martin Dit Latour; M Martinez; V I Martinez Outschoorn; S Martin-Haugh; V S Martoiu; A C Martyniuk; A Marzin; L Masetti; T Mashimo; R Mashinistov; J Masik; A L Maslennikov; L H Mason; L Massa; P Massarotti; P Mastrandrea; A Mastroberardino; T Masubuchi; P Mättig; J Maurer; B Maček; S J Maxfield; D A Maximov; R Mazini; I Maznas; S M Mazza; N C Mc Fadden; G Mc Goldrick; S P Mc Kee; A McCarn; T G McCarthy; L I McClymont; E F McDonald; J A Mcfayden; G Mchedlidze; M A McKay; K D McLean; S J McMahon; P C McNamara; C J McNicol; R A McPherson; J E Mdhluli; Z A Meadows; S Meehan; T M Megy; S Mehlhase; A Mehta; T Meideck; B Meirose; D Melini; B R Mellado Garcia; J D Mellenthin; M Melo; F Meloni; A Melzer; S B Menary; E D Mendes Gouveia; L Meng; X T Meng; A Mengarelli; S Menke; E Meoni; S Mergelmeyer; C Merlassino; P Mermod; L Merola; C Meroni; 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P Mullen; G A Mullier; F J Munoz Sanchez; P Murin; W J Murray; A Murrone; M Muškinja; C Mwewa; A G Myagkov; J Myers; M Myska; B P Nachman; O Nackenhorst; K Nagai; K Nagano; Y Nagasaka; K Nagata; M Nagel; E Nagy; A M Nairz; Y Nakahama; K Nakamura; T Nakamura; I Nakano; H Nanjo; F Napolitano; R F Naranjo Garcia; R Narayan; D I Narrias Villar; I Naryshkin; T Naumann; G Navarro; R Nayyar; H A Neal; P Y Nechaeva; T J Neep; A Negri; M Negrini; S Nektarijevic; C Nellist; M E Nelson; S Nemecek; P Nemethy; M Nessi; M S Neubauer; M Neumann; P R Newman; T Y Ng; Y S Ng; H D N Nguyen; T Nguyen Manh; E Nibigira; R B Nickerson; R Nicolaidou; J Nielsen; N Nikiforou; V Nikolaenko; I Nikolic-Audit; K Nikolopoulos; P Nilsson; Y Ninomiya; A Nisati; N Nishu; R Nisius; I Nitsche; T Nitta; T Nobe; Y Noguchi; M Nomachi; I Nomidis; M A Nomura; T Nooney; M Nordberg; N Norjoharuddeen; T Novak; O Novgorodova; R Novotny; L Nozka; K Ntekas; E Nurse; F Nuti; F G Oakham; H Oberlack; T Obermann; J Ocariz; A Ochi; I Ochoa; J P Ochoa-Ricoux; K O'Connor; S Oda; S Odaka; S Oerdek; A Oh; S H Oh; C C Ohm; H Oide; H Okawa; Y Okazaki; Y Okumura; T Okuyama; A Olariu; L F Oleiro Seabra; S A Olivares Pino; D Oliveira Damazio; J L Oliver; M J R Olsson; A Olszewski; J Olszowska; D C O'Neil; A Onofre; K Onogi; P U E Onyisi; H Oppen; M J Oreglia; Y Oren; D Orestano; E C Orgill; N Orlando; A A O'Rourke; R S Orr; B Osculati; V O'Shea; R Ospanov; G Otero Y Garzon; H Otono; M Ouchrif; F Ould-Saada; A Ouraou; Q Ouyang; M Owen; R E Owen; V E Ozcan; N Ozturk; J Pacalt; H A Pacey; K Pachal; A Pacheco Pages; L Pacheco Rodriguez; C Padilla Aranda; S Pagan Griso; M Paganini; G Palacino; S Palazzo; S Palestini; M Palka; D Pallin; I Panagoulias; C E Pandini; J G Panduro Vazquez; P Pani; G Panizzo; L Paolozzi; T D Papadopoulou; K Papageorgiou; A Paramonov; D Paredes Hernandez; S R Paredes Saenz; B Parida; A J Parker; K A Parker; M A Parker; F Parodi; J A Parsons; U Parzefall; V R Pascuzzi; J M P Pasner; E Pasqualucci; S Passaggio; F Pastore; P Pasuwan; S Pataraia; J R Pater; A Pathak; T Pauly; B Pearson; M Pedersen; L Pedraza Diaz; R Pedro; S V Peleganchuk; O Penc; C Peng; H Peng; B S Peralva; M M Perego; A P Pereira Peixoto; D V Perepelitsa; F Peri; L Perini; H Pernegger; S Perrella; V D Peshekhonov; K Peters; R F Y Peters; B A Petersen; T C Petersen; E Petit; A Petridis; C Petridou; P Petroff; E Petrolo; M Petrov; F Petrucci; M Pettee; N E Pettersson; A Peyaud; R Pezoa; T Pham; F H Phillips; P W Phillips; G Piacquadio; E Pianori; A Picazio; M A Pickering; R Piegaia; J E Pilcher; A D Pilkington; M Pinamonti; J L Pinfold; M Pitt; M-A Pleier; V Pleskot; E Plotnikova; D Pluth; P Podberezko; R Poettgen; R Poggi; L Poggioli; I Pogrebnyak; D Pohl; I Pokharel; G Polesello; A Poley; A Policicchio; R Polifka; A Polini; C S Pollard; V Polychronakos; D Ponomarenko; L Pontecorvo; G A Popeneciu; D M Portillo Quintero; S Pospisil; K Potamianos; I N Potrap; C J Potter; H Potti; T Poulsen; J Poveda; T D Powell; M E Pozo Astigarraga; 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D Rodriguez Rodriguez; A M Rodríguez Vera; S Roe; C S Rogan; O Røhne; R Röhrig; C P A Roland; J Roloff; A Romaniouk; M Romano; N Rompotis; M Ronzani; L Roos; S Rosati; K Rosbach; P Rose; N-A Rosien; E Rossi; E Rossi; L P Rossi; L Rossini; J H N Rosten; R Rosten; M Rotaru; J Rothberg; D Rousseau; D Roy; A Rozanov; Y Rozen; X Ruan; F Rubbo; F Rühr; A Ruiz-Martinez; Z Rurikova; N A Rusakovich; H L Russell; J P Rutherfoord; E M Rüttinger; Y F Ryabov; M Rybar; G Rybkin; S Ryu; A Ryzhov; G F Rzehorz; P Sabatini; G Sabato; S Sacerdoti; H F-W Sadrozinski; R Sadykov; F Safai Tehrani; P Saha; M Sahinsoy; A Sahu; M Saimpert; M Saito; T Saito; H Sakamoto; A Sakharov; D Salamani; G Salamanna; J E Salazar Loyola; D Salek; P H Sales De Bruin; D Salihagic; A Salnikov; J Salt; D Salvatore; F Salvatore; A Salvucci; A Salzburger; J Samarati; D Sammel; D Sampsonidis; D Sampsonidou; J Sánchez; A Sanchez Pineda; H Sandaker; C O Sander; M Sandhoff; C Sandoval; D P C Sankey; M Sannino; Y Sano; A Sansoni; C Santoni; H Santos; I Santoyo Castillo; A Sapronov; J G Saraiva; O Sasaki; K Sato; E Sauvan; P Savard; N Savic; R Sawada; C Sawyer; L Sawyer; C Sbarra; A Sbrizzi; T Scanlon; J Schaarschmidt; P Schacht; B M Schachtner; D Schaefer; L Schaefer; J Schaeffer; S Schaepe; U Schäfer; A C Schaffer; D Schaile; R D Schamberger; N Scharmberg; V A Schegelsky; D Scheirich; F Schenck; M Schernau; C Schiavi; S Schier; L K Schildgen; Z M Schillaci; E J Schioppa; M Schioppa; K E Schleicher; S Schlenker; K R Schmidt-Sommerfeld; K Schmieden; C Schmitt; S Schmitt; S Schmitz; U Schnoor; L Schoeffel; A Schoening; E Schopf; M Schott; J F P Schouwenberg; J Schovancova; S Schramm; A Schulte; H-C Schultz-Coulon; M Schumacher; B A Schumm; Ph Schune; A Schwartzman; T A Schwarz; H Schweiger; Ph Schwemling; R Schwienhorst; A Sciandra; G Sciolla; M Scornajenghi; F Scuri; F Scutti; L M Scyboz; J Searcy; C D Sebastiani; P Seema; S C Seidel; A Seiden; T Seiss; J M Seixas; G Sekhniaidze; K Sekhon; S J Sekula; N Semprini-Cesari; S Sen; S Senkin; C Serfon; L Serin; L Serkin; M Sessa; H Severini; F Sforza; A Sfyrla; E Shabalina; J D Shahinian; N W Shaikh; L Y Shan; R Shang; J T Shank; M Shapiro; A S Sharma; A Sharma; P B Shatalov; K Shaw; S M Shaw; A Shcherbakova; Y Shen; N Sherafati; A D Sherman; P Sherwood; L Shi; S Shimizu; C O Shimmin; M Shimojima; I P J Shipsey; S Shirabe; M Shiyakova; J Shlomi; A Shmeleva; D Shoaleh Saadi; M J Shochet; S Shojaii; D R Shope; S Shrestha; E Shulga; P Sicho; A M Sickles; P E Sidebo; E Sideras Haddad; O Sidiropoulou; A Sidoti; F Siegert; Dj Sijacki; J Silva; M Silva; M V Silva Oliveira; S B Silverstein; L Simic; S Simion; E Simioni; M Simon; R Simoniello; P Sinervo; N B Sinev; M Sioli; G Siragusa; I Siral; S Yu Sivoklokov; J Sjölin; M B Skinner; P Skubic; M Slater; T Slavicek; M Slawinska; K Sliwa; R Slovak; V Smakhtin; B H Smart; J Smiesko; N Smirnov; S Yu Smirnov; Y Smirnov; L N Smirnova; O Smirnova; J W Smith; M N K Smith; R W Smith; M Smizanska; K Smolek; A A Snesarev; I M Snyder; S Snyder; R Sobie; A M Soffa; A Soffer; A Søgaard; D A Soh; G Sokhrannyi; C A Solans Sanchez; M Solar; E Yu Soldatov; U Soldevila; A A Solodkov; A Soloshenko; O V Solovyanov; V Solovyev; P Sommer; H Son; W Song; A Sopczak; F Sopkova; D Sosa; C L Sotiropoulou; S Sottocornola; R Soualah; A M Soukharev; D South; B C Sowden; S Spagnolo; M Spalla; M Spangenberg; F Spanò; D Sperlich; F Spettel; T M Spieker; R Spighi; G Spigo; L A Spiller; D P Spiteri; M Spousta; A Stabile; R Stamen; S Stamm; E Stanecka; R W Stanek; C Stanescu; B Stanislaus; M M Stanitzki; B Stapf; S Stapnes; E A Starchenko; G H Stark; J Stark; S H Stark; P Staroba; P Starovoitov; S Stärz; R Staszewski; M Stegler; P Steinberg; B Stelzer; H J Stelzer; O Stelzer-Chilton; H Stenzel; T J Stevenson; G A Stewart; M C Stockton; G Stoicea; P Stolte; S Stonjek; A Straessner; J Strandberg; S Strandberg; M Strauss; P Strizenec; R Ströhmer; D M Strom; R Stroynowski; A Strubig; S A Stucci; B Stugu; J Stupak; N A Styles; D Su; J Su; S Suchek; Y Sugaya; M Suk; V V Sulin; D M S Sultan; S Sultansoy; T Sumida; S Sun; X Sun; K Suruliz; C J E Suster; M R Sutton; S Suzuki; M Svatos; M Swiatlowski; S P Swift; A Sydorenko; I Sykora; T Sykora; D Ta; K Tackmann; J Taenzer; A Taffard; R Tafirout; E Tahirovic; N Taiblum; H Takai; R Takashima; E H Takasugi; K Takeda; T Takeshita; Y Takubo; M Talby; A A Talyshev; J Tanaka; M Tanaka; R Tanaka; R Tanioka; B B Tannenwald; S Tapia Araya; S Tapprogge; A Tarek Abouelfadl Mohamed; S Tarem; G Tarna; G F Tartarelli; P Tas; M Tasevsky; T Tashiro; E Tassi; A Tavares Delgado; Y Tayalati; A C Taylor; A J Taylor; G N Taylor; P T E Taylor; W Taylor; A S Tee; P Teixeira-Dias; H Ten Kate; P K Teng; J J Teoh; F Tepel; S Terada; K Terashi; J Terron; S Terzo; M Testa; R J Teuscher; S J Thais; T Theveneaux-Pelzer; F Thiele; J P Thomas; A S Thompson; P D Thompson; L A Thomsen; E Thomson; Y Tian; R E Ticse Torres; V O Tikhomirov; Yu A Tikhonov; S Timoshenko; P Tipton; S Tisserant; K Todome; S Todorova-Nova; S Todt; J Tojo; S Tokár; K Tokushuku; E Tolley; K G Tomiwa; M Tomoto; L Tompkins; K Toms; B Tong; P Tornambe; E Torrence; H Torres; E Torró Pastor; C Tosciri; J Toth; F Touchard; D R Tovey; C J Treado; T Trefzger; F Tresoldi; A Tricoli; I M Trigger; S Trincaz-Duvoid; M F Tripiana; W Trischuk; B Trocmé; A Trofymov; C Troncon; M Trovatelli; F Trovato; L Truong; M Trzebinski; A Trzupek; F Tsai; J C-L Tseng; P V Tsiareshka; N Tsirintanis; V Tsiskaridze; E G Tskhadadze; I I Tsukerman; V Tsulaia; S Tsuno; D Tsybychev; Y Tu; A Tudorache; V Tudorache; T T Tulbure; A N Tuna; S Turchikhin; D Turgeman; I Turk Cakir; R Turra; P M Tuts; E Tzovara; G Ucchielli; I Ueda; M Ughetto; F Ukegawa; G Unal; A Undrus; G Unel; F C Ungaro; Y Unno; K Uno; J Urban; P Urquijo; P Urrejola; G Usai; J Usui; L Vacavant; V Vacek; B Vachon; K O H Vadla; A Vaidya; C Valderanis; E Valdes Santurio; M Valente; S Valentinetti; A Valero; L Valéry; R A Vallance; A Vallier; J A Valls Ferrer; T R Van Daalen; W Van Den Wollenberg; H Van der Graaf; P Van Gemmeren; J Van Nieuwkoop; I Van Vulpen; M Vanadia; W Vandelli; A Vaniachine; P Vankov; R Vari; E W Varnes; C Varni; T Varol; D Varouchas; K E Varvell; G A Vasquez; J G Vasquez; F Vazeille; D Vazquez Furelos; T Vazquez Schroeder; J Veatch; V Vecchio; L M Veloce; F Veloso; S Veneziano; A Ventura; M Venturi; N Venturi; V Vercesi; M Verducci; C M Vergel Infante; W Verkerke; A T Vermeulen; J C Vermeulen; M C Vetterli; N Viaux Maira; M Vicente Barreto Pinto; I Vichou; T Vickey; O E Vickey Boeriu; G H A Viehhauser; S Viel; L Vigani; M Villa; M Villaplana Perez; E Vilucchi; M G Vincter; V B Vinogradov; A Vishwakarma; C Vittori; I Vivarelli; S Vlachos; M Vogel; P Vokac; G Volpi; S E von Buddenbrock; E Von Toerne; V Vorobel; K Vorobev; M Vos; J H Vossebeld; N Vranjes; M Vranjes Milosavljevic; V Vrba; M Vreeswijk; T Šfiligoj; R Vuillermet; I Vukotic; T Ženiš; L Živković; P Wagner; W Wagner; J Wagner-Kuhr; H Wahlberg; S Wahrmund; K Wakamiya; V M Walbrecht; J Walder; R Walker; S D Walker; W Walkowiak; V Wallangen; A M Wang; C Wang; F Wang; H Wang; H Wang; J Wang; J Wang; P Wang; Q Wang; R-J Wang; R Wang; R Wang; S M Wang; W T Wang; W Wang; W X Wang; Y Wang; Z Wang; C Wanotayaroj; A Warburton; C P Ward; D R Wardrope; A Washbrook; P M Watkins; A T Watson; M F Watson; G Watts; S Watts; B M Waugh; A F Webb; S Webb; C Weber; M S Weber; S A Weber; S M Weber; A R Weidberg; B Weinert; J Weingarten; M Weirich; C Weiser; P S Wells; T Wenaus; T Wengler; S Wenig; N Wermes; M D Werner; P Werner; M Wessels; T D Weston; K Whalen; N L Whallon; A M Wharton; A S White; A White; M J White; R White; D Whiteson; B W Whitmore; F J Wickens; W Wiedenmann; M Wielers; C Wiglesworth; L A M Wiik-Fuchs; A Wildauer; F Wilk; H G Wilkens; L J Wilkins; H H Williams; S Williams; C Willis; S Willocq; J A Wilson; I Wingerter-Seez; E Winkels; F Winklmeier; O J Winston; B T Winter; M Wittgen; M Wobisch; A Wolf; T M H Wolf; R Wolff; M W Wolter; H Wolters; V W S Wong; N L Woods; S D Worm; B K Wosiek; K W Woźniak; K Wraight; M Wu; S L Wu; X Wu; Y Wu; T R Wyatt; B M Wynne; S Xella; Z Xi; L Xia; D Xu; H Xu; L Xu; T Xu; W Xu; B Yabsley; S Yacoob; K Yajima; D P Yallup; D Yamaguchi; Y Yamaguchi; A Yamamoto; T Yamanaka; F Yamane; M Yamatani; T Yamazaki; Y Yamazaki; Z Yan; H J Yang; H T Yang; S Yang; Y Yang; Z Yang; W-M Yao; Y C Yap; Y Yasu; E Yatsenko; J Ye; S Ye; I Yeletskikh; E Yigitbasi; E Yildirim; K Yorita; K Yoshihara; C J S Young; C Young; J Yu; J Yu; X Yue; S P Y Yuen; B Zabinski; G Zacharis; E Zaffaroni; R Zaidan; A M Zaitsev; N Zakharchuk; J Zalieckas; S Zambito; D Zanzi; D R Zaripovas; S V Zeißner; C Zeitnitz; G Zemaityte; J C Zeng; Q Zeng; O Zenin; D Zerwas; M Zgubič; D F Zhang; D Zhang; F Zhang; G Zhang; H Zhang; J Zhang; L Zhang; L Zhang; M Zhang; P Zhang; R Zhang; R Zhang; X Zhang; Y Zhang; Z Zhang; P Zhao; X Zhao; Y Zhao; Z Zhao; A Zhemchugov; B Zhou; C Zhou; L Zhou; M S Zhou; M Zhou; N Zhou; Y Zhou; C G Zhu; H L Zhu; H Zhu; J Zhu; Y Zhu; X Zhuang; K Zhukov; V Zhulanov; A Zibell; D Zieminska; N I Zimine; S Zimmermann; Z Zinonos; M Zinser; M Ziolkowski; G Zobernig; A Zoccoli; K Zoch; T G Zorbas; R Zou; M Zur Nedden; L Zwalinski
Journal:  Eur Phys J C Part Fields       Date:  2019-01-23       Impact factor: 4.590
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