Abstract
The exclusive production of pion pairs in the process \(pp\rightarrow pp\pi ^+\pi ^-\) has been measured at \(\sqrt{s}={7}\,\text {TeV}\) with the ATLAS detector at the LHC, using \({80}\,{\upmu \textrm{b}}^{-1}\) of low-luminosity data. The pion pairs were detected in the ATLAS central detector while outgoing protons were measured in the forward ATLAS ALFA detector system. This represents the first use of proton tagging to measure an exclusive hadronic final state at the LHC. A cross-section measurement is performed in two kinematic regions defined by the proton momenta, the pion rapidities and transverse momenta, and the pion–pion invariant mass. Cross-section values of \(4.8 \pm 1.0 \mathrm {\ (stat)} {~}^{+0.3}_{-0.2} \mathrm {\ (syst)}\ {\upmu \textrm{b}}\) and \(9 \pm 6 \mathrm {\ (stat)} {~}^{+2}_{-2} \mathrm {\ (syst)}\ {\upmu \textrm{b}} \) are obtained in the two regions; they are compared with theoretical models and provide a demonstration of the feasibility of measurements of this type.
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1 Introduction
A significant fraction of LHC proton–proton (\(pp\)) collisions are either elastic (\(\approx {25}{\%}\)) or diffractive (\(\approx {20}{\%}\) of the remaining inelastic collisions [1]). In many of these collisions the momentum transferred from the beam protons is too small (\(< 1\ {\text {GeV}} \)) for perturbative quantum chromodynamics (QCD) to be applicable, and instead Regge theory [2, 3] is used. This involves the exchange of a non-perturbative Pomeron, a soft colour-singlet object originally introduced to keep the universality of the \(s\)-dependence of high energy total cross sections by Gribov [4], Chew and Frautschi [5] and later providing an explanation of the rise of hadronic collision cross-sections with increasing beam energy energy [6]. Since QCD is assumed to be universally valid, there should nevertheless be a ‘mapping’ between Regge theory and QCD in which the exchanged Pomeron is equivalent to the exchange of quarks and gluons, the fundamental quanta of QCD. In certain kinematic regions, the Pomeron can be treated approximately as a two-gluon colour-singlet state. Exclusive diffractive processes provide a clean environment to study the interactions of Pomerons, via the observation of final states involving only several hadrons and no beam-remnants except the outgoing protons.
This paper presents first measurements of the exclusive double-diffractive production of charged-pion pairs in the process \(pp\rightarrow pp\pi ^+\pi ^-\), schematically shown in Fig. 1, using the ATLAS detector at the LHC.
The charged pions are measured with the ATLAS inner detector [7], while the outgoing protons are measured by the ALFA detector [8], comprising two tracking stations situated in the forward regions on either side of ATLAS at distances of approximately 240 m from the ATLAS interaction point (IP). The ALFA detector system was designed in the first place to determine the total pp cross section at LHC energies, as well as to measure the LHC luminosity via small-angle proton-scattering processes [9]. The use of the ALFA detectors is a distinctive feature of the present study, since the outgoing protons are directly measured, suppressing contamination from the remnants of excited scattered protons. The analysis benefits from procedures developed previously in the ALFA total cross section measurement [9].
The present results can be compared with existing measurements of the exclusive production of pion pairs using data from the ISR [10, 11], SPS [12], RHIC [13] and LHC [14, 15], where the CMS results [14, 15] are not based on purely exclusive events but on a mixture of exclusive and semi-exclusive processes. Some recent theory predictions for the process considered here may be found in Refs. [16,17,18,19,20,21,22,23,24,25,26]. In addition to revealing general properties of Pomerons, these channels provide a rich potential harvest for a variety of final states, including the production of resonances and the possible production of the long-sought glueball states.
2 Experimental apparatus
ATLAS is a multipurpose apparatus covering almost the entire solid angle around its LHC interaction point (IP) [7].Footnote 1 The present analysis combines information from the ATLAS inner detector, the minimum-bias trigger scintillators, and the ALFA detector system.
The ATLAS inner detector (ID) [7, 27] immediately surrounds the ATLAS IP and is composed of three tracker subsystems that provide high-precision track reconstruction: a silicon pixel detector (innermost), a silicon semiconductor tracker (SCT), and a transition-radiation tracker (outermost), which also helps to discriminate electrons from hadrons. The ID covers a range of \(|\eta |<2.5\). It is surrounded by a superconducting solenoid, which produces a 2 T axial field within the ID volume.
The minimum-bias trigger scintillators (MBTS) [28] are located on either side of ATLAS between the ID and the liquid-argon calorimeter at \(\pm 3.6~\text {m}\) from the IP. Each of the two MBTS detectors is oriented perpendicularly to the beam direction and consists of 16 panels assembled in two concentric rings, the outer ring covering the range \(2.1<|\eta |<2.8\) and the inner ring covering the range \(2.8<|\eta |<3.8\).
The ALFA detector system [8], located at \(z \approx ~\pm {240}\,\text {m}\), consists of four Roman pot stations, containing vertically movable detectors that can approach the outgoing beams to within one millimetre. A schematic diagram of the detector arrangement relative to the ATLAS IP is shown in Fig. 2.
Each station is equipped with two Roman pots, each of which hosts a nearly edgeless tracking detector composed of scintillating fibres, as depicted in Fig. 3.
The ALFA detector system has a limited radiation tolerance and takes data under conditions with low numbers (\(\mu \)) of simultaneous proton–proton collisions interactions per beam crossing (pile-up).
An extensive software suite [29] is used in the reconstruction and analysis of real and simulated data, in detector operations, and in the trigger and data acquisition systems of the experiment.
3 Monte Carlo generators
The analysis makes use of two Monte Carlo (MC) signal generators: GenEx [30] and Dime [25].Footnote 2 The models are similar, but not identical, and provide different predictions. The GenEx generator is used for the baseline calculations of detection and reconstruction efficiency for the events, and for corrections to the data, while Dime is used for comparison and to estimate model uncertainties.
The generator GenEx (version May 2015) is based on a theoretical model from Lebiedowicz et al. [24] and calculates the exclusive continuum production of \(\pi ^{+}\pi ^{-}\) and \(K^{+}K^{-}\) pairs. It is based on a Regge-exchange description. The parameter determining the meson form factor (in its exponential parameterization) is the only free parameter. The implemented model describes non-resonant production without an absorption correction and does not include a rapidity gap survival factor (see e.g. Ref. [33]). In the present analysis, pions were generated within a region of pseudorapidity \(|\eta |<2.7\), and with the off-shell-pion form-factor parameter set to \(\Lambda _{\textrm{off}} = {1}\,\text {GeV}\). Otherwise, default program settings were used.
The generator Dime (version 1.06) similarly generates exclusive continuum production of \(\pi ^{+}\pi ^{-}\) and \(K^{+}K^{-}\) pairs, although other channels are also implemented, e.g. exclusive \(\rho \rho \) or \(\phi \phi \) production. Unlike GenEx, Dime includes wider possibilities for modelling absorption effects: four different models (parameter \(iin\), 1 – the default value used in our analysis; see Table 12 in Ref. [34]) for absorption are available with three different parameterizations of the meson form factor (exponential, ‘Orear-like’ – used in the present analysis, and power-like) [25].
The central diffractive background processes were generated by Pythia8 [35] (version 8.183), using the ATLAS A2 set of tuned parameters [36] and the MSTW2008lo PDF set [37]. Pythia8 employs a parton structure function approach and calculates the processes of central diffraction via double Pomeron exchange (DPE). The exclusive pion-pair process is removed from the dataset.
The Geant4 [38] toolkit is implemented to simulate the response of the ATLAS central and forward detectors [39]. The leading outgoing protons are transported to the ALFA locations using the beam parameter values and ALFA detector positions corresponding to the data-taking period [9] in which a special high-beta* optics, referred to here as the nominal optics, was employed. The MC events were reconstructed using the same ATLAS software chain as used for the data.
4 Data taking
The data were recorded in October 2011 during a special four-hour run with high \(\beta ^{\star }= {90}\,\,\text {m}\) and very low pile-up given by \(\mu = 0.035\). Each beam of the LHC was filled with one circulating proton bunch containing \(7\cdot 10^{10}\) protons. The integrated delivered luminosity and its uncertainty were determined to be \(L_{\text {int}} = 78.7 \pm 0.1 {(\text {stat})} \pm 1.9 {\text { (syst)}} \,\upmu \text {b}^{-1}\) [9].
Two event topological configurations are used in this analysis, covering four regions of phase space. They are referred to as elastic and anti-elastic and are based on signals in different combinations of four ALFA detectors, as shown in Fig. 2. Each detector combination is designated as an arm (following the existing ALFA notation [9]), and includes detectors on side A and side C in order to measure forward protons on each side of ATLAS. The elastic configuration makes use of two arm combinations: Arm1 = arm\(_{1368}\) = A1+A3+A6+A8 (elastic arm 0) and Arm2 = arm\(_{2457}\) = A2+A4+A5+A7 (elastic arm 1), while the anti-elastic configuration uses Arm3 = arm\(_{1357}\) = A1+A3+A5+A7 (anti-elastic arm 0) and Arm4 = arm\(_{2468}\) = A2+A4+A6+A8 (anti-elastic arm 1). Each arm comprises two armlets, consisting of two ALFA stations on either the A side or C side of ATLAS. The two configurations measure different ranges of momentum transfer to the pion system and their events were recorded by different combinations of triggers during data taking. They correspond physically to different kinematic phase-space regions, and theoretical models can differ in their estimates of cross-sections.
5 Data analysis
5.1 Event selection
The event topology for exclusive pion-pair production consists of two oppositely charged pions detected by the ATLAS ID, accompanied by a leading outgoing proton entering each of the ATLAS forward regions and detected by the ALFA detector system. There should be no other activity in the ATLAS ID and in the inner cells of the MBTS, and the total three-momentum of the measured protons and pions must be consistent with zero.Footnote 3 The data selections are summarized in Table 1. The order in which the selections were applied to the data is given in Table 2.
5.1.1 Description of selections
The description of the conditions that are applied to select a clean sample of \(pp\pi ^+\pi ^-\) event candidates, as summarized in Table 1, is as follows.
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Bunch system and good lumi blocks. The data come from single colliding proton bunches in the LHC. The data-recording intervals that were used (‘lumi blocks’) are required to be longer than 60 s in duration and the dead time must be smaller than 5%.
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Trigger. For the elastic configuration, a coincidence in the upper A-side and lower C-side detectors or the lower A-side and upper C-side detectors was required [9] (see Fig. 2). The trigger efficiency within the geometrical acceptance of the detectors is measured to be \((99.96 \pm 0.10)\%\) [9]. For the anti-elastic configuration the relevant trigger (a signal in any of the eight ALFA detectors) was prescaled by a factor of 15, which resulted in a low numbers of recorded anti-elastic events. The trigger efficiency for each of the anti-elastic configurations is determined as the product of the measured single-diffractive trigger efficiencies on each side, leading to the value \((99.02 \pm 0.25)\%\) before prescaling.
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Pion system.
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Charged tracks. Tracks in the ATLAS ID were reconstructed using a low-\(p_{\textrm{T}}\) tracking algorithm (\(p_{\textrm{T}} > {100}\,\text {MeV}\)) as in Ref. [40], where \(p_{\textrm{T}}\) denotes the transverse momentum component. Each track must pass the following quality conditions:
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Pixel detector: at least one hit is required,
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Semiconductor tracker: a minimum number of hits in the SCT is required, depending on the track \(p_{\mathrm T}\): at least two hits for \(p_{\mathrm T} > {100}\,\text {MeV}\), four hits for \(p_{\mathrm T} > {200}\,\text {MeV}\) and six hits for \(p_{\mathrm T} > {300}\,\text {MeV}\).
Events with at least two tracks are required. A primary vertex is required and must have exactly two accepted tracks with opposite-sign charges and small impact parameters relative to the beam axis. For the purposes of this analysis, all charged tracks are treated as pion tracks, since the numbers of electron, kaon and proton pairs are estimated to be small. The pions’ transverse momenta are reconstructed [40] with an uncertainty of about 10 MeV independent of their charge.
-
-
-
MBTS. To select events with no additional visible activity in the ATLAS ID, taking into consideration its limited \(\eta \) coverage, a MBTS veto criterion is applied: the total number of MBTS inner cells on the two ATLAS sides with a signal is required to be at most one, ignoring the outer cells. This criterion was chosen since it was robust against electronic noise in the MBTS detector.
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Proton system.
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ALFA track reconstruction. The proton reconstruction criteria used in a previous analysis [9] – bunch group, data quality, selections on the reconstructed track and geometrical deflection, beam-screen and edge conditions (see Table 2 of Ref. [9]) – together with the detector alignment, are adopted for the current study.
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ALFA uv-condition. This requirement is introduced to remove contributions from beam halo and showers (caused by interactions with material between the IP and the ALFA detectors). These contributions are absent in MC simulations. The purpose of the ALFA uv-condition is to differentiate between events with single particles and those with multi-particle showers entering the detectors, so as to filter out multi-particle signals, and in this way to allow good correspondence between MC simulations and real data samples.
The uv-condition is based on the fibre multiplicities associated with a candidate proton. The first four u and first four v detector layers [8], closest to the IP, must satisfy the following:
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at least two of these u layers, and at least two of these v layers, must have at least one hit, and
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at most one u layer and one v layer may have more than three hits.
The first condition identifies a well-measured track and is based on the estimate of the single-fibre efficiency and a requirement on the uv-condition efficiency. The second, allowing at most two cross-talk hits surrounding that of the signal, is based on observations made during beam tests of the ALFA detectors. It also rejects tracks that give rise to showers.
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ALFA clean track. Due to e.g. beam halo, pile-up or showers, more than one track may be reconstructed in a given ALFA detector [9], and it may not be possible to decide which of the tracks is the correct one. Therefore, only events with exactly one reconstructed track in each of the detectors that comprise an arm are considered in the present analysis, and a correction is evaluated for each of the configuration arms to compensate for the consequent loss of signal.
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ALFA geometric condition. In measuring leading protons, the ALFA detector system operates as a spectrometer in which a proton having a larger energy loss undergoes a larger deflection, corresponding to a larger \(x\) value of its track position measured in the horizontal direction in the coordinates of the ALFA station. In the case of exclusive pion-pair production, the energy loss of a leading proton is low and the expected distribution in the scatter plot of the reconstructed \(x\)-positions of the protons and corresponding local angles \(\theta _x\) (see Fig. 3) should have a shape similar to that of elastically scattered protons. This is illustrated in Fig. 4 and allows a geometrical selection to be used to remove many protons not originating from the process of interest. Data and MC events were selected within the ellipse indicated in Fig. 4b, whose size is slightly larger than that from the elastically scattered protons shown in Fig. 4a. This covers the larger kinematic phase space occupied by the protons after losing energy to the pion system.
-
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Overall momentum balance. Because of the limited reconstruction of the proton kinematics, a selection criterion for overall four-momentum conservation is not possible; instead the momentum balance in the x and y projections is used.
The methods used for the reconstruction of the proton kinematics from the tracks measured by the ALFA detector are based on knowledge of the accelerator optics. As the mass of the centrally produced pion-pair system is low, the ‘lattice’ method [9], originally used for elastically scattered protons, can be applied. Proton momentum projections \(p_x\) and \(p_y\) are used in the analysis, and are reconstructed with a resolution of about 40 MeV and 1 MeV respectively.
The transverse momentum components of the full \(pp\pi ^+\pi ^-\) system are determined with a resolution of approximately 60 \(\text {MeV}\) in \(p_x\) and 20 \(\text {MeV}\) in \(p_y\), denoted by \(\sigma _x\) and \(\sigma _y\) respectively. The signal region is defined by \(3.5\sigma _{x,y}\) intervals about zero in \(p_x\) and \(p_y\).
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Fiducial condition. The exclusive production of pion pairs is studied within a fiducial region which is defined to be close to that which is allowed by the sub-detector acceptances. The data and Monte Carlo analyses use the same fiducial region, which is given in terms of the pseudorapidities \(\eta (\pi )\) and transverse momenta \(p_{\textrm{T}}(\pi )\) of the individual pions, and the mass of the central pion system \(m_{\pi \pi }\):
$$\begin{aligned}{} & {} |\eta (\pi )|< 2.5, \; p_{\textrm{T}}(\pi ) > 0.1\ \text {GeV},\\{} & {} \quad \; 2m_{\pi }< m_{\pi \pi } < 2.0\ \text {GeV}. \end{aligned}$$Additional conditions are applied to the y-components of the proton momenta \(p_{\textrm{y}}(\textrm{A})\) and \(p_{\textrm{y}}(\textrm{C})\), in both the elastic and anti-elastic configurations:
$$\begin{aligned}{} & {} \textrm{armlet}_{ij}^\mathrm {low\_cut}< p_{\textrm{y}}(\textrm{A})< \textrm{armlet}_{ij}^\mathrm {up\_cut} \ \mathrm {\ \ \ and \ \ \ }\\{} & {} \textrm{armlet}_{kl}^\mathrm {low\_cut}< p_{\textrm{y}}(\textrm{C}) < \textrm{armlet}_{kl}^\mathrm {up\_cut}, \end{aligned}$$where \(ijkl \in \) {1368, 2457, 1357, 2468} and
$$\begin{aligned} \begin{aligned} \textrm{armlet}_{13}^{\text {up}\_\text {cut}}&= \ \ 0.267\ \text {GeV},&\textrm{armlet}_{57}^{\text {up}\_\text {cut}}&= \ \ 0.246\ \text {GeV},&\\ \textrm{armlet}_{13}^{\text {low}\_\text {cut}}&= \ \ 0.080\ \text {GeV},&\textrm{armlet}_{57}^{\text {low}\_\text {cut}}&= \ \ 0.080\ \text {GeV},&\\ \textrm{armlet}_{24}^{\text {up}\_\text {cut}}&= -0.079\ \text {GeV},&\textrm{armlet}_{68}^{\text {up}\_\text {cut}}&= -0.082\ \text {GeV},&\\ \textrm{armlet}_{24}^{\text {low}\_\text {cut}}&= -0.250\ \text {GeV},&\textrm{armlet}_{68}^{\text {low}\_\text {cut}}&= -0.269\ \text {GeV}.&\end{aligned} \end{aligned}$$These selections are evaluated in terms of the reconstructed ALFA proton kinematic parameters, calculated using the nominal beam optics and ALFA detector positions. The experimental uncertainties of these values translate into a systematic uncertainty that is common to the corrected data and the MC predictions.
5.1.2 Data selection statistics
The numbers of events after the successive selection conditions are shown in Table 2.
5.2 Background estimation
One source of background consists of centrally produced pion pairs that are accidentally accompanied by one or more beam-halo protons which are detected in ALFA. This background is suppressed by the event selections to a low level. This can be seen in Fig. 5, which shows (a) the total multiplicity distribution of the MBTS inner rings for events that satisfy the selection criteria listed in Table 1, except for those on MBTS and momentum balance, and (b) after all the selections in Table 1 are applied. A fit to the data is performed in terms of a model comprising generated signal events (GenEx) and backgrounds from (i) generated diffractive events (Pythia8) and (ii) an ‘accidentals’ event sample formed from data events with a pion pair that are combined with unrelated data events randomly found to have ALFA signals. For exclusive pion events, the MBTS multiplicity is at most one, while for other diffractive events it can be higher. Events with accidental coincidences can give both higher and lower MBTS multiplicities. Such events are contained in the event sample, but Fig. 5b shows that they contribute no contamination to the signal region \(|p_a| < 3.5\sigma _a\), where \(a = x, y\) (see Sect. 5.1.1), after all conditions listed in Table 1 are applied.
The very strong effect of the MBTS veto on background suppression is demonstrated also in Fig. 6, which shows that the summed vertical (y-axis) track momenta exhibit a clear signal peak in the total \(p_y\) of the event only after this veto is applied. Figure 6a includes events with selections up to those on the ID and ALFA tracks listed in Table 2, while Fig. 6b shows the same data and backgrounds but with the MBTS veto also applied. The background was fitted outside the signal region, which approximately covers the central three plotted intervals. The signal peak is now prominent.
Since the data were taken during the special run with very low pile-up, the remaining backgrounds, after applying the event selections of Sect. 5.1, presumably originate from other central diffraction processes. For both the elastic and anti-elastic event configurations, the backgrounds due to these diffraction processes are estimated using events satisfying the complete set of selections listed in Table 1 except for the requirement on the momentum balance in the x and y projections. They are evaluated from a fit to the \(p_y\) distribution of the data outside the signal region, using a model consisting of a background generated by Pythia8 and accidentals. This is shown in Fig. 7a, while Fig. 7b shows the distribution with all the selections applied.
5.3 Beam and ALFA modelling inefficiencies, correction procedure
The implementation of the ALFA detector in the ATLAS simulation framework has some limitations. The response can differ from that of the real detector, mainly due to imperfect implementation of signal and noise production mechanisms and the omission of electronic cross-talk between channels.
Since the simulation does not include the production of particle showers that are due to the interaction of forward-going particles with parts of the LHC (accelerator beam pipe, collimators, shielding of magnets, etc.), the uv-condition is introduced, effectively removing these showers from the data. This affects the signal, and the corresponding correction depends on the elastic or anti-elastic configuration (‘conf’) and the arm. A further correction is required for the clean track selection (Sect. 5.1).
If the MC description were perfect, the detector efficiency \(\varepsilon \), for a given arm and configuration, would be written as
where \(N_{\text {trk}}\) is the number of generated MC signal events with at least one track reconstructed in each of the detectors in a given configuration and \({N_{\text {acc}}}\) is the number of MC signal events within the acceptance of that configuration.
Since the MC simulation does not contain all relevant effects, the uv-condition and the clean track selection are introduced and Eq. (1) is now rewritten as
where \({N_{\text {uv}}}\) is the number of events which pass the uv-condition. The first factor in Eq. (2) is given by physics that can be mismodelled by generators, and the second factor takes account of the clean track selection.
Denoting \(R_{\text {arm}}^{\textrm{conf}} = \left( o^{\text {MC}}/o^{\text {data}}\right) _{\text {arm}}^{\textrm{conf}}\), where the ratio \(o^{\text {X}} = N^{\text {X, clean}}/N^{\text {X, any}}\) gives the ratio of the number of events with clean tracks to all events in a given track sample X (MC or data), the combined correction factor \(f^{\mathrm {s+} uv \textrm{, conf}}_{\text {arm}}\), where \(\mathrm {s+} uv \) denotes the combination of single tracks and uv-conditions, is written as
which, using Eq. (2), can be re-written as
Its values are given in Table 3.
The effects arising from detector efficiency and due to migrations across the fiducial phase-space boundary at particle and detector level are corrected for with a single factor for each configuration. This is adequate in view of the limited statistical precision of the data, given that the MC model describes the data well. The correction factor, \(f^{\textrm{corr, conf}}_{\textrm{arm}}\), is based on the GenEx MC simulation, and for a given configuration it is defined as the ratio of the number of events, \(N_{\mathrm {detector\_level}}^{\textrm{passed}}\), that pass the event selection criteria at the detector level, to the number of events \(N_{\mathrm {particle\_level}}^{\textrm{passed}}\) that pass the fiducial region selection at the particle level, i.e. \(f^{\textrm{corr, conf}}_{\textrm{arm}} = \left( {N_{\mathrm {detector\_level}}^{\textrm{passed}}}/{N_{\mathrm {particle\_level}} ^{\textrm{passed}}}\right) ^{\textrm{conf}}_{\textrm{arm}}\). The geometrical acceptance of each ALFA detector is \(\approx \) 0.25, giving rise to the calculated combined values stated in Table 3.
The visible cross-section for a given elastic or anti-elastic configuration is then determined as
where L represents the integrated luminosity used; \(N^{\textrm{conf}}_{\textrm{arm}}\) and \(B^{\textrm{conf}}_{\textrm{arm}}\) are the numbers of selected signal candidate events and calculated background events in each arm; \( C^{\textrm{conf}}_{\text {arm}} = f^{\mathrm {s+} uv \textrm{, conf}}_{\text {arm}}/f^{\textrm{corr, conf}}_{\textrm{arm}}\); \(\epsilon _{\textrm{trig}}^{\textrm{conf}}\) is the trigger efficiency for the given configuration; \(\epsilon _{\textrm{DAQ}}\) is the dead-time correction factor, as defined and determined in Ref. [9].
5.4 Kinematic distributions
Taking into account the precision of the reconstruction, the kinematic distributions of the pions and protons are well modelled by the MC simulations. Figures 8, 9 and 10 show comparisons of the distributions of the momentum components of the reconstructed pions and protons, and the pion-pair rapidity, acoplanarity, transverse momentum and invariant mass, for the data and the GenEx MC and Dime MC simulations. The distributions are presented after applying all the event selections, but without applying a background subtraction (\(\approx 10\%\)) to the data. In view of the low number of events for the anti-elastic configuration, only distributions for the elastic configuration are shown.
5.5 Systematic uncertainties
The overall systematic uncertainty on the exclusive pion-pair cross-section measurement is estimated as \({~}^{+6.4}_{-4.2} \) \(\%\) for the elastic configuration and \({~}^{+6.0}_{-4.4} \) \(\%\) for the anti-elastic configuration. Table 4 summarizes the main sources of systematic uncertainty. The difference between the relative uncertainties of the two configurations comes mainly from data-driven systematic uncertainties. Some of the MC studies made use of slightly enlarged fiducial region criteria to estimate systematic uncertainties.
Background determination. The systematic uncertainty is determined as half of the difference between the background estimates for the standard signal region, \(3.5\sigma _{x,y}\) around zero in \(p_x\) and \(p_y\), and for the case when the signal region is increased to \(5\sigma _{x,y}\). It is symmetrized.
LHC beam energy. The systematic uncertainty due to that of the nominal beam energy is based on a beam energy variation of about \(\pm 0.1\%\) [41].
Thicknesses of material. An uncertainty in the amount of material in the ID is calculated by changing this by \(+5\%\) and \(+10\%\) in the whole ID and by \(+10\%\) in the pixel detector to determine the difference between the lowest and the highest value of the corrected exclusive pion-pair cross-section [40].
MBTS Veto. The MBTS veto uncertainty determination is based on the corresponding procedure used in the measurement of the inelastic proton–proton cross-section at \(\sqrt{s}\) = 7 TeV [42].
Selection criteria. The uncertainty in the efficiency due to the selection criteria is determined from the fraction of lost signal. The overall uncertainty in the ALFA reconstruction efficiency is determined by varying the event selection criteria and summing the corresponding individual uncertainties in quadrature.
Correction factors. An uncertainty in the values of \(f^{\mathrm {s+} uv \textrm{, conf}}_{\text {arm}}\) arises from the restricted selection of data that is used to evaluate this factor in each arm. Although of statistical origin, this is treated as a systematic uncertainty.
Beam optics. This analysis uses data at a collision energy of 7 TeV and with high \(\beta ^{\star }= {90}\,\text {m}\) beam optics, referred to as the nominal optics. Based on data measurements, an adjustment is made to the current-to-field calibration offset between the Q1Q3 and Q2 quadrupole magnets to derive the so-called effective optics [9]. Studies related to both optics are performed: the effective and the nominal optics are used in MC simulation to calculate all the corrections applied in reconstructing the data. The nominal optics is used as the baseline; the difference in the cross-section values is used to determine the systematic uncertainties.
Modelling. The analysis of the data uses the generator GenEx as the baseline for modelling the signal sample. The full analysis is repeated using the generator Dime, and the difference between the resulting cross-sections is taken as an uncertainty due to the modelling and is applied symmetrically.
6 Results and discussion
The cross-section for exclusive pion pair production is measured for two non-overlapping configurations, elastic and anti-elastic. The fiducial region is defined in Sect. 5.1.1 and the results are presented in Table 5.
There are 28 candidate signal events in the elastic configuration and 3 in the anti-elastic configuration (see Table 2). These include an estimated 2.9 background events in the elastic configuration (\(\approx \) 10%) and 0.2 background events (\(\approx \) 6%) in the anti-elastic configuration.
The results may be compared with cross-sections provided by MC generators using the same fiducial region definition: \({1.5}\,{\upmu \textrm{b}}\) (elastic configuration) and \({2}\,{\upmu \textrm{b}}\) (anti-elastic configuration) in the case of GenEx (these have been multiplied by an absorptive correction, abs. corr.), and \({1.6}\,{\upmu \textrm{b}}\) (elastic configuration) and \({3}\,{\upmu \textrm{b}}\) (anti-elastic configuration) in the case of Dime. The absorptive correction [25] applied here to GenEx covers possible rescatterings of the particles entering the process and complicates the simple picture in Fig. 1. The value used of 0.22 was communicated by its author; the correction is not included in GenEx itself and is, in general, kinematics and model dependent. It is not used in the experimental analysis, since the MC distributions are normalized to data, but only in the present comparison with the results. The measured anti-elastic cross-section has a large statistical uncertainty, and is not statistically different from zero, which prevents strong conclusions from being drawn.
7 Conclusion
A first measurement of the purely exclusive pion-pair cross-section at the LHC is presented, using \({80}\,{\upmu \textrm{b}}^{-1}\) of \(\sqrt{s}={7}\,\text {TeV}\) low-luminosity pp collision data collected by the ATLAS detector. The limited statistical precision obtained excludes the present possibility of tuning or excluding any of the existing physical models for the process, but the two models that are employed here, GenEx and Dime, evaluated with the parameters provided by their authors, provide preliminary theoretical estimates. The use of the forward ALFA detectors distinguishes the present measurement from others performed at comparable energies, since both outgoing protons have been measured directly, and used to suppress contamination from beam remnants. This measurement demonstrates the potential to measure exclusive diffractive hadronic processes using forward sub-detectors in combination with the ATLAS central detector.
Data Availability Statement
This manuscript has no associated data or the data will not be deposited. [Authors’ comment: “All ATLAS scientific output is published in journals, and preliminary results are made available in Conference Notes. All are openly available, without restriction on use by external parties beyond copyright law and the standard conditions agreed by CERN. Data associated with journal publications are also made available: tables and data from plots (e.g. cross section values, likelihood profiles, selection efficiencies, cross section limits, ...) are stored in appropriate repositories such as HEPDATA (https://www.hepdata.net/). ATLAS also strives to make additional material related to the paper available that allows a reinterpretation of the data in the context of new theoretical models. For example, an extended encapsulation of the analysis is often provided for measurements in the framework of RIVET (http://rivet.hepforge.org/).” This information is taken from the ATLAS Data Access Policy, which is a public document that can be downloaded from http://opendata.cern.ch/record/413 [opendata.cern.ch]. The data for this publication will be available at: https://doi.org/10.17182/hepdata.131222].
Notes
ATLAS uses a right-handed coordinate system with its origin at the nominal interaction point in the centre of the detector and the z-axis along the beam-pipe. The x-axis points from the interaction point to the centre of the LHC ring, and the y-axis points upwards. Cylindrical coordinates \((r,\phi )\) are used in the transverse plane, \(\phi \) being the azimuthal angle around the z-axis. The pseudorapidity is defined in terms of the polar angle \(\theta \) as \(\eta = -\ln \tan (\theta /2)\). Angular distance is measured in units of \(\Delta R \equiv \sqrt{(\Delta \eta )^{2} + (\Delta \phi )^{2}}\).
The precise expectation value depends on the beam-crossing angle, which varied during the data taking and was at most \({10}\,{\upmu }\,\text {rad}\) in the y projection and smaller in x. The full effect is safely ignored since its impact is less than those of the ALFA detector resolution.
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Acknowledgements
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; ANID, Chile; CAS, MOST and NSFC, China; Minciencias, Colombia; MEYS CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS and CEA-DRF/IRFU, France; SRNSFG, Georgia; BMBF, HGF and MPG, Germany; GSRI, Greece; RGC and Hong Kong SAR, China; ISF and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; NWO, Netherlands; RCN, Norway; MEiN, Poland; FCT, Portugal; MNE/IFA, Romania; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DSI/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TENMAK, Turkey; STFC, United Kingdom; DOE and NSF, USA. In addition, individual groups and members have received support from BCKDF, CANARIE, Compute Canada and CRC, Canada; PRIMUS 21/SCI/017 and UNCE SCI/013, Czech Republic; COST, ERC, ERDF, Horizon 2020 and Marie Skłodowska-Curie Actions, European Union; Investissements d’Avenir Labex, Investissements d’Avenir Idex and ANR, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF, Greece; BSF-NSF and MINERVA, Israel; Norwegian Financial Mechanism 2014–2021, Norway; NCN and NAWA, Poland; La Caixa Banking Foundation, CERCA Programme Generalitat de Catalunya and PROMETEO and GenT Programmes Generalitat Valenciana, Spain; Göran Gustafssons Stiftelse, Sweden; The Royal Society and Leverhulme Trust, UK. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [43].
Author information
D. Bruncko, I. A. Budagov, E. F. Torregrosa, V. Gratchev, J. Olszowska, L. Perini, S. Y. Sivoklokov:Deceased.
Authors and Affiliations
Department of Physics, University of Adelaide, Adelaide, Australia
M. Amerl, E. K. Filmer, P. Jackson, A. X. Y. Kong, H. Potti, T. A. Ruggeri, E. X. L. Ting & M. J. White
Department of Physics, University of Alberta, Edmonton, AB, Canada
D. M. Gingrich, J. H. Lindon, N. Nishu & J. L. Pinfold
Department of Physics, Ankara University, Ankara, Türkiye
O. Cakir, H. Duran Yildiz, S. Kuday & I. Turk Cakir
Division of Physics, TOBB University of Economics and Technology, Ankara, Türkiye
S. Sultansoy
LAPP, Univ. Savoie Mont Blanc, CNRS/IN2P3, Annecy, France
C. Adam Bourdarios, N. Berger, F. Costanza, M. Delmastro, L. Di Ciaccio, C. Goy, T. Guillemin, T. Hryn’ova, S. Jézéquel, I. Koletsou, J. Levêque, D. J. Lewis, J. D. Little, N. Lorenzo Martinez, G. Poddar, E. Rossi, A. Sanchez Pineda, E. Sauvan & L. Selem
APC, Université Paris Cité, CNRS/IN2P3, Paris, France
G. Bernardi, M. Bomben, R. Bouquet, G. Marchiori, Q. Shen & Y. Zhang
High Energy Physics Division, Argonne National Laboratory, Argonne, IL, USA
S. Chekanov, S. Darmora, W. H. Hopkins, J. Hoya, E. Kourlitis, T. LeCompte, J. Love, J. Metcalfe, A. S. Mete, A. Paramonov, J. Proudfoot, P. Van Gemmeren, R. Wang & J. Zhang
Department of Physics, University of Arizona, Tucson, AZ, USA
S. Berlendis, E. Cheu, Z. Cui, A. Ghosh, K. A. Johns, W. Lampl, R. E. Lindley, P. Loch, J. P. Rutherfoord, J. Sardain, E. W. Varnes, H. Zhou & Y. Zhou
Department of Physics, University of Texas at Arlington, Arlington, TX, USA
D. Bakshi Gupta, B. Burghgrave, J. C. J. Cardenas, K. De, A. Farbin, H. K. Hadavand, A. J. Myers, N. Ozturk, G. Usai & A. White
Physics Department, National and Kapodistrian University of Athens, Athens, Greece
S. Angelidakis, D. Fassouliotis, L. Fountas, I. Gkialas & C. Kourkoumelis
Physics Department, National Technical University of Athens, Zografou, Greece
T. Alexopoulos, C. Bakalis, I. Drivas-koulouris, E. N. Gazis, C. Kitsaki, S. Maltezos, C. Paraskevopoulos, M. Perganti & P. Tzanis
Department of Physics, University of Texas at Austin, Austin, TX, USA
T. Andeen, C. D. Burton, K. Choi, P. U. E. Onyisi, D. K. Panchal, M. Unal & A. F. Webb
Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan
N. Huseynov
Institut de Física d’Altes Energies (IFAE), Barcelona Institute of Science and Technology, Barcelona, Spain
M. N. Agaras, M. Bosman, J. I. Carlotto, M. P. Casado, L. Castillo Garcia, S. Epari, V. Gautam, S. Gonzalez Fernandez, C. Grieco, S. Grinstein, A. Juste Rozas, S. Kazakos, I. Korolkov, J. Mamuzic, M. Martinez, P. Martinez Suarez, L. M. Mir, J. L. Munoz Martinez, N. Orlando, A. Pacheco Pages, C. Padilla Aranda, I. Riu, A. Salvador Salas, A. Sonay & S. Terzo
Institute of High Energy Physics, Chinese Academy of Sciences, Beijing, China
J. Barreiro Guimarães da Costa, Y. Cai, X. Chu, H. Cui, Y. Fan, Y. Fang, J. A. García Pascual, F. Guo, Y. F. Hu, Y. Huang, X. Jia, M. Li, Z. Li, Z. Liang, B. Liu, P. Liu, X. Lou, G. Lu, F. Lyu, A. F. Mohammed, L. Y. Shan, J. Wu, S. Xin, D. Xu, Z. Xu, X. Yang, K. Zhang, P. Zhang, C. Zhu, H. Zhu & X. Zhuang
Physics Department, Tsinghua University, Beijing, China
X. Chen, W. Ding, M. Feng, B. Li, H. Pang, M. Xia, Y. Xu & G. Zhang
Department of Physics, Nanjing University, Nanjing, China
M. K. Ayoub, H. Chen, S. J. Chen, A. De Maria, A. D’Onofrio, L. Han, X. Huang, Z. Jia, S. Jin, H. Li, Y. Liu, F. L. Lucio Alves, T. Min, X. Wang, Y. Wang, L. Xia, H. Ye, B. Zhang & L. Zhang
University of Chinese Academy of Science (UCAS), Beijing, China
Y. Cai, X. Chu, H. Cui, Y. Fang, F. Guo, Y. F. Hu, X. Jia, M. Li, Z. Li, Y. Liu, X. Lou, G. Lu, A. F. Mohammed, K. Ran, J. Wu, S. Xin, K. Zhang, P. Zhang & C. Zhu
Institute of Physics, University of Belgrade, Belgrade, Serbia
E. Bakos, L. J. Beemster, J. Jovicevic, V. Maksimovic, Dj. Sijacki, N. Vranjes, M. Vranjes Milosavljevic & L. Živković
Department for Physics and Technology, University of Bergen, Bergen, Norway
T. Buanes, J. I. Djuvsland, G. Eigen, N. Fomin, S. K. Huiberts, G. R. Lee, A. Lipniacka, B. Martin dit Latour, B. Stugu & A. Traeet
Physics Division, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
D. J. A. Antrim, R. M. Barnett, J. Beringer, P. Calafiura, F. Cerutti, A. Ciocio, A. Dimitrievska, G. I. Dyckes, K. Einsweiler, I. Ene, M. G. Foti, L. G. Gagnon, M. Garcia-Sciveres, C. Gonzalez Renteria, H. M. Gray, C. Haber, S. Han, T. Heim, I. Hinchliffe, X. Ju, K. Krizka, C. Leggett, Z. Marshall, W. P. McCormack, M. Muškinja, B. P. Nachman, G. J. Ottino, S. Pagan Griso, V. R. Pascuzzi, M. Pettee, E. Pianori, E. D. Resseguie, E. Reynolds, B. R. Roberts, S. N. Santpur, M. Shapiro, B. Stanislaus, V. Tsulaia, C. Varni, H. Wang, J. Xiong, T. Yamazaki, H. T. Yang, W-M. Yao, B. K. Yeo & Z. Zhang
Institut für Physik, Humboldt Universität zu Berlin, Berlin, Germany
C. Appelt, N. B. Atlay, M. Bahmani, D. Battulga, D. Berge, A. Cortes-Gonzalez, S. Grancagnolo, C. Issever, T. J. Khoo, K. Kreul, H. Lacker, T. Lohse, M. Michetti, A. Nayaz, Y. S. Ng, V. H. Ruelas Rivera, C. Scharf, F. Schenck, P. Seema & T. Theveneaux-Pelzer
Albert Einstein Center for Fundamental Physics and Laboratory for High Energy Physics, University of Bern, Bern, Switzerland
J. K. Anders, H. P. Beck, M. Chatterjee, A. Ereditato, L. Franconi, L. Halser, S. Haug, A. Ilg, R. Müller, A. P. O’Neill, M. M. Schefer & M. S. Weber
School of Physics and Astronomy, University of Birmingham, Birmingham, UK
P. P. Allport, A. D. Auriol, P. Bellos, G. A. Bird, J. Bracinik, D. G. Charlton, A. S. Chisholm, H. G. Cooke, T. Fitschen, P. M. Freeman, W. F. George, L. Gonella, F. Gonnella, N. A. Gorasia, C. M. Hawkes, S. J. Hillier, J. J. Kempster, M. Marinescu, A. M. Mendes Jacques Da Costa, T. J. Neep, P. R. Newman, K. Nikolopoulos, J. M. Silva, A. Stampekis, J. P. Thomas, P. D. Thompson, G. S. Virdee, R. J. Ward, A. T. Watson & M. F. Watson
Department of Physics, Bogazici University, Istanbul, Türkiye
A. Bayirli, E. Celebi, S. Istin, K. Y. Oyulmaz & V. E. Ozcan
Department of Physics Engineering, Gaziantep University, Gaziantep, Türkiye
A. Bingul & Z. Uysal
Department of Physics, Istanbul University, Istanbul, Türkiye
A. Adiguzel
Istinye University, Sariyer, Istanbul, Türkiye
A. J. Beddall, S. A. Cetin, S. Ozturk & S. Simsek
Facultad de Ciencias y Centro de Investigaciónes, Universidad Antonio Nariño, Bogotá, Colombia
G. Navarro & Y. Rodriguez Garcia
Departamento de Física, Universidad Nacional de Colombia, Bogotá, Colombia
C. Sandoval
Dipartimento di Fisica e Astronomia A. Righi, Università di Bologna, Bologna, Italy
S. Biondi, G. Carratta, N. Cavalli, L. Clissa, S. De Castro, F. Del Corso, L. Fabbri, M. Franchini, A. Gabrielli, L. Rinaldi, A. Sbrizzi, N. Semprini-Cesari, M. Sioli, K. Todome, S. Valentinetti, M. Villa, C. Vittori & A. Zoccoli
INFN Sezione di Bologna, Bologna, Italy
G. L. Alberghi, F. Alfonsi, L. Bellagamba, S. Biondi, D. Boscherini, A. Bruni, G. Bruni, M. Bruschi, G. Cabras, G. Carratta, N. Cavalli, A. Cervelli, L. Clissa, S. De Castro, F. Del Corso, L. Fabbri, M. Franchini, A. Gabrielli, B. Giacobbe, F. Lasagni Manghi, L. Massa, M. Negrini, A. Polini, L. Rinaldi, M. Romano, C. Sbarra, A. Sbrizzi, N. Semprini-Cesari, A. Sidoti, M. Sioli, K. Todome, S. Valentinetti, M. Villa, C. Vittori & A. Zoccoli
Physikalisches Institut, Universität Bonn, Bonn, Germany
A. Bandyopadhyay, S. Bansal, P. Bauer, P. Bechtle, F. Beisiegel, F. U. Bernlochner, I. Brock, K. Desch, C. Deutsch, F. G. Diaz Capriles, C. Dimitriadi, J. Dingfelder, P. J. Falke, C. Grefe, S. Gurbuz, M. Hamer, F. Hinterkeuser, T. Holm, M. Huebner, F. Huegging, C. Kirfel, O. Kivernyk, T. Klingl, P. T. Koenig, H. Krüger, K. Lantzsch, T. Lenz, C. Nass, D. Pohl, M. Standke, C. Vergis, E. Von Toerne & N. Wermes
Department of Physics, Boston University, Boston, MA, USA
J. M. Butler & Z. Yan
Department of Physics, Brandeis University, Waltham, MA, USA
S. V. Addepalli, J. R. Bensinger, P. Bhattarai, C. Blocker, D. Camarero Munoz, F. Capocasa, J. Chen, G. Frattari, M. Goblirsch-Kolb, Z. M. Schillaci, G. Sciolla, D. A. Trischuk & D. T. Zenger Jr
Transilvania University of Brasov, Brasov, Romania
S. Popa
Horia Hulubei National Institute of Physics and Nuclear Engineering, Bucharest, Romania
C. Alexa, A. Chitan, D. A. Ciubotaru, I-M. Dinu, O. A. Ducu, A. E. Dumitriu, A. A. Geanta, A. Jinaru, V. S. Martoiu, J. Maurer, A. Olariu, D. Pietreanu, M. Renda, M. Rotaru, G. Stoicea, G. Tarna, I. S. Trandafir, A. Tudorache, V. Tudorache & M. E. Vasile
Department of Physics, Alexandru Ioan Cuza University of Iasi, Iasi, Romania
C. Agheorghiesei & P. Postolache
Physics Department, National Institute for Research and Development of Isotopic and Molecular Technologies, Cluj-Napoca, Romania
G. A. Popeneciu
University Politehnica Bucharest, Bucharest, Romania
A. A. Geanta & R. Hobincu
West University in Timisoara, Timisoara, Romania
P. M. Gravila
Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovak Republic
R. Astalos, D. Babal, P. Bartos, M. Dubovsky, B. Eckerova, S. Hyrych, L. Keszeghova, O. Majersky, I. Sykora, S. Tokár & T. Ženiš
Department of Subnuclear Physics, Institute of Experimental Physics of the Slovak Academy of Sciences, Kosice, Slovak Republic
D. Bruncko, F. Sopkova, P. Strizenec & J. Urban
Physics Department, Brookhaven National Laboratory, Upton, NY, USA
S. H. Abidi, K. Assamagan, G. Barone, M. Begel, D. P. Benjamin, M. Benoit, R. Bi, D. Boye, E. Brost, V. Cavaliere, H. Chen, G. D’amen, S. J. Das, J. Elmsheuser, B. Garcia, V. Garonne, Y. Go, G. Iakovidis, C. W. Kalderon, A. Klimentov, E. Lançon, D. Lynn, H. Ma, T. Maeno, C. Mc Ginn, C. Mwewa, J. L. Nagle, P. Nilsson, M. A. Nomura, D. Oliveira Damazio, J. Ouellette, D. V. Perepelitsa, M. -A. Pleier, V. Polychronakos, S. Protopopescu, S. Rajagopalan, G. Redlinger, T. T. Rinn, J. Roloff, S. Snyder, P. Steinberg, S. A. Stucci, A. Tricoli, A. Undrus, C. Weber, T. Wenaus & S. Ye
Departamento de Física, y CONICET, Facultad de Ciencias Exactas y Naturales, Instituto de Física de Buenos Aires (IFIBA), Universidad de Buenos Aires, Buenos Aires, Argentina
M. F. Daneri, G. Otero y Garzon, R. Piegaia & M. Toscani
California State University, Long Beach, CA, USA
K. Grimm, J. Moss & J. Veatch
Cavendish Laboratory, University of Cambridge, Cambridge, UK
W. K. Balunas, J. R. Batley, O. Brandt, J. T. P. Burr, J. D. Chapman, J. W. Cowley, W. J. Fawcett, L. Henkelmann, B. H. Hodkinson, L. B. A. H. Hommels, D. M. Jones, P. Jones, C. G. Lester, J. K. K. Liu, C. Malone, D. L. Noel, H. A. Pacey, M. A. Parker, C. J. Potter, D. Robinson, D. Rousso, R. Tombs & S. Williams
Department of Physics, University of Cape Town, Cape Town, South Africa
R. J. Atkin, K. N. Barends, J. M. Keaveney & S. Yacoob
Department of Mechanical Engineering Science, University of Johannesburg, Johannesburg, South Africa
M. Bhamjee, M. P. Connell, S. H. Connell, N. Govender, L. L. Leeuw & L. Truong
National Institute of Physics, University of the Philippines Diliman (Philippines), Quezon City, South Africa
M. Flores
School of Physics, University of the Witwatersrand, Johannesburg, South Africa
F. Carrio Argos, T. Chowdhury, L. D. Christopher, S. Dahbi, M. G. D. Gololo, D. Kar, M. Kumar, R. P. Mckenzie, B. R. Mellado Garcia, G. Mokgatitswane, E. K. Nkadimeng, N. P. Rapheeha, X. Ruan, E. M. Shrif, E. Sideras Haddad, S. Sinha & S. H. Tlou
Department of Physics, Carleton University, Ottawa, ON, Canada
A. Bachiu, A. Bellerive, B. Davis-Purcell, D. Gillberg, K. Graham, J. Heilman, C. E. Jessiman, S. Kaur, J. S. Keller, C. Klein, T. Koffas, A. Laurier, L. S. Miller, M. Naseri, B. J. Norman, F. G. Oakham, D. A. Pizzi, E. J. Staats, M. G. Vincter & N. Zakharchuk
Faculté des Sciences Ain Chock, Réseau Universitaire de Physique des Hautes Energies-Université Hassan II, Casablanca, Morocco
D. Benchekroun, F. Bendebba, K. Bouaouda, Z. Chadi, A. El Moussaouy, S. Ezzarqtouni, H. Imam & S. Zerradi
Faculté des Sciences, Université Ibn-Tofail, Kenitra, Morocco
Y. El Ghazali & M. Gouighri
LPMR, Faculté des Sciences, Université Mohamed Premier, Oujda, Morocco
J. Assahsah & M. Ouchrif
Faculté des sciences, Université Mohammed V, Rabat, Morocco
A. Aboulhorma, S. Batlamous, R. Cherkaoui El Moursli, H. El Jarrari, F. Fassi, H. Hamdaoui, B. Ngair, Z. Soumaimi, Y. Tayalati & M. Zaazoua
CERN, Geneva, Switzerland
Y. Afik, A. Ahmad, M. Aleksa, C. Amelung, N. Aranzabal, A. J. Armbruster, G. Avolio, M-S. Barisits, T. A. Beermann, C. Beirao Da Cruz E Silva, J. F. Beirer, L. Beresford, T. Bisanz, D. Bogavac, J. D. Bossio Sola, J. Boyd, V. M. M. Cairo, N. Calace, S. Camarda, T. Carli, A. Catinaccio, L. D. Corpe, A. Cueto, P. Czodrowski, V. Dao, A. Dell’Acqua, P. O. Deviveiros, A. Di Girolamo, F. Dittus, A. Dudarev, M. Dührssen, N. Ellis, M. Elsing, S. Falke, D. Francis, D. Froidevaux, P. Gessinger-Befurt, F. Giuli, L. Goossens, B. Gorini, C. A. Gottardo, S. Guindon, G. Gustavino, R. J. Hawkings, C. Helsens, A. M. Henriques Correia, L. Hervas, A. Hoecker, M. Huhtinen, J. J. Junggeburth, M. Kiehn, P. Klimek, T. Klioutchnikova, N. M. Köhler, A. Koulouris, A. Krasznahorkay, S. Kuehn, F. Lanni, M. Lassnig, M. LeBlanc, G. Lehmann Miotto, I. Lopez Paz, S. Manzoni, A. Marzin, M. Mentink, A. Milic, M. Mlynarikova, J. Montejo Berlingen, A. K. Morley, L. Morvaj, P. Moschovakos, B. Moser, A. M. Nairz, M. Nessi, N. Nikiforou, S. Palestini, T. Pauly, O. Penc, H. Pernegger, S. Perrella, B. A. Petersen, N. E. Pettersson, L. Pezzotti, L. Pontecorvo, M. E. Pozo Astigarraga, M. Raymond, C. Rembser, S. Rettie, P. Riedler, S. Roe, A. Rummler, D. Salamani, A. Salzburger, S. Schlenker, J. Schovancova, A. Sharma, M. V. Silva Oliveira, R. Simoniello, I. Siral, J. Smiesko, C. A. Solans Sanchez, P. Sommer, G. Spigo, G. A. Stewart, M. C. Stockton, A. N. Tuna, G. Unal, T. Vafeiadis, M. Van Rijnbach, W. Vandelli, T. Vazquez Schroeder, B. Vormwald, R. Vuillermet, T. Wengler, H. G. Wilkens & L. Zwalinski
Affiliated with an institute covered by a cooperation agreement with CERN, Geneva, Switzerland
A. V. Akimov, M. Aliev, A. V. Anisenkov, E. M. Baldin, S. Barsov, K. Beloborodov, K. Belotskiy, N. L. Belyaev, V. S. Bobrovnikov, A. G. Bogdanchikov, O. Bulekov, A. R. Buzykaev, S. P. Denisov, F. Dubinin, A. Ezhilov, R. M. Fakhrutdinov, O. L. Fedin, G. Fedotov, A. B. Fenyuk, I. L. Gavrilenko, A. Gavrilyuk, L. K. Gladilin, D. Golubkov, P. A. Gorbounov, V. Gratchev, S. Harkusha, A. N. Karyukhin, V. F. Kazanin, A. G. Kharlamov, T. Kharlamova, N. Korotkova, A. S. Kozhin, V. A. Kramarenko, O. Kuchinskaia, Y. Kulchitsky, A. Kupich, Y. A. Kurochkin, A. Kurova, M. Levchenko, V. P. Maleev, A. L. Maslennikov, D. A. Maximov, O. Meshkov, A. A. Minaenko, A. G. Myagkov, I. Naryshkin, P. Y. Nechaeva, V. Nikolaenko, S. V. Peleganchuk, M. Penzin, A. Petukhov, D. Ponomarenko, D. Pudzha, D. Pyatiizbyantseva, E. Ramakoti, O. L. Rezanova, A. Romaniouk, A. Ryzhov, V. A. Schegelsky, P. B. Shatalov, V. Sinetckii, S. Yu. Sivoklokov, S. Yu. Smirnov, Y. Smirnov, L. N. Smirnova, A. A. Snesarev, E. Yu. Soldatov, A. A. Solodkov, O. V. Solovyanov, V. Solovyev, E. A. Starchenko, V. V. Sulin, L. Sultanaliyeva, A. A. Talyshev, V. Tikhomirov, Yu. A. Tikhonov, S. Timoshenko, P. V. Tsiareshka, I. I. Tsukerman, K. Vorobev, O. Zenin, K. Zhukov & V. Zhulanov
Affiliated with an international laboratory covered by a cooperation agreement with CERN, Geneva, Switzerland
F. Ahmadov, I. N. Aleksandrov, V. A. Bednyakov, I. R. Boyko, I. A. Budagov, G. A. Chelkov, A. Cheplakov, M. V. Chizhov, D. V. Dedovich, M. Demichev, A. Gongadze, M. I. Gostkin, S. N. Karpov, Z. M. Karpova, U. Kruchonak, V. Kukhtin, E. Ladygin, V. Lyubushkin, T. Lyubushkina, S. Malyukov, M. Mineev, E. Plotnikova, I. N. Potrap, N. A. Rusakovich, M. Shiyakova, A. Soloshenko, S. Turchikhin, T. Turtuvshin, I. Yeletskikh, A. Zhemchugov & N. I. Zimine
Enrico Fermi Institute, University of Chicago, Chicago, IL, USA
R. W. Gardner, M. D. Hank, Y. K. Kim, D. W. Miller, M. J. Oreglia, J. L. Rainbolt, B. J. Rosser, D. Schaefer, T. Seiss, M. J. Shochet, E. A. Smith, C. Tosciri & I. Vukotic
LPC, Université Clermont Auvergne, CNRS/IN2P3, Clermont-Ferrand, France
D. Boumediene, A. M. Burger, D. Calvet, S. Calvet, J. Donini, R. Madar, T. Megy, O. Perrin, C. Santoni, A. Tnourji, L. Vaslin & F. Vazeille
Nevis Laboratory, Columbia University, Irvington, NY, USA
K. Al Khoury, A. Angerami, G. Brooijmans, E. L. Busch, B. Cole, A. Emerman, B. J. Gilbert, J. L. Gonski, D. A. Hangal, Q. Hu, A. Kahn, K. E. Kennedy, D. J. Mahon, S. Mohapatra, J. A. Parsons, B. D. Seidlitz, A. C. Smith, P. M. Tuts, D. M. Williams, P. Yin & W. Zou
Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
A. Camplani, M. Dam, J. B. Hansen, J. D. Hansen, P. H. Hansen, T. C. Petersen, C. Wiglesworth & S. Xella
Dipartimento di Fisica, Università della Calabria, Rende, Italy
E. Bisceglie, M. Capua, G. Crosetti, F. Curcio, D. Malito, A. Mastroberardino, E. Meoni, D. Salvatore, M. Schioppa & E. Tassi
INFN Gruppo Collegato di Cosenza, Laboratori Nazionali di Frascati, Frascati, Italy
E. Bisceglie, M. Capua, G. Crosetti, F. Curcio, I. Gnesi, D. Malito, A. Mastroberardino, E. Meoni, D. Salvatore, M. Schioppa & E. Tassi
Physics Department, Southern Methodist University, Dallas, TX, USA
A. M. Deiana, K. J. C. Leney, C. D. Milke, R. Narayan, S. Parajuli, S. J. Sekula, R. Stroynowski, P. Wang, Y. Yang & J. Ye
Physics Department, University of Texas at Dallas, Richardson, TX, USA
S. W. Ferguson, J. M. Izen, B. Meirose & K. Reeves
National Centre for Scientific Research “Demokritos”, Agia Paraskevi, Greece
G. Fanourakis, T. Geralis, M. M. Prapa, G. Stavropoulos & O. Zormpa
Department of Physics, Stockholm University, Stockholm, Sweden
S. Y. Andrean, F. Backman, L. Barranco Navarro, C. Bohm, C. Clement, K. Dunne, S. Hellman, T. Ingebretsen Carlson, D. W. Kim, S. Lee, X. Lou, D. A. Milstead, T. Moa, P. Pasuwan, L. Pereira Sanchez, S. Richter, N. W. Shaikh, S. B. Silverstein, J. Sjölin, S. Strandberg, A. Strubig & E. Valdes Santurio
Oskar Klein Centre, Stockholm, Sweden
S. Y. Andrean, F. Backman, L. Barranco Navarro, C. Clement, K. Dunne, S. Hellman, T. Ingebretsen Carlson, D. W. Kim, S. Lee, X. Lou, D. A. Milstead, T. Moa, P. Pasuwan, L. Pereira Sanchez, S. Richter, N. W. Shaikh, J. Sjölin, S. Strandberg, A. Strubig & E. Valdes Santurio
Deutsches Elektronen-Synchrotron DESY, Hamburg and Zeuthen, Germany
X. Ai, S. Amoroso, L. Aperio Bella, J.-H. Arling, A. Basalaev, J. K. Behr, I. Bloch, P. Bokan, F. Braren, K. Brendlinger, B. Brüers, C. D. Burgard, E. Cheremushkina, J. M. Clavijo Columbie, J. Clercx, N. De Biase, S. Díez Cornell, L. Ferencz, J. Ferrando, P. Gadow, G. Gaycken, N. E. K. Gillwald, V. Goumarre, I. M. Gregor, A. Guida, R. Gupta, M. Habedank, S. Heim, L. Helary, J. Hofer, A. Hrynevich, C. Issever, R. M. Jacobs, J. Katzy, D. Kuechler, J. T. Kuechler, T. Kuhl, C. E. Leitgeb, M. Liberatore, A. Linss, Y. Liu, E. M. Lobodzinska, A. Lopez Solis, T. C. Mclachlan, F. Meloni, P. Moder, K. Mönig, F. Nechansky, J. Neundorf, Y. W. Y. Ng, T. Novak, M. L. Ojeda, P. Pani, K. Peters, T. Poulsen, K. Ran, A. Renardi, F. Renner, M. Rimoldi, P. Rivadeneira, M. Robin, L. Rossini, C. O. Sander, S. Schmitt, C. Seitz, S. Sharma, S. Sinha, D. South, M. M. Stanitzki, B. Stapf, L. R. Strom, N. A. Styles, K. Tackmann, E. A. Thompson, J. Von Ahnen, C. J. Wells, A. F. Wongel, S. D. Worm & Y. C. Yap
Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany
M. Baselga, T. Dado, C. M. Delitzsch, S. Dungs, J. Erdmann, K. Kroeninger, T. Kupfer, O. Nackenhorst, K. Sedlaczek, J. Weingarten, B. Wendland & S. V. Zeißner
Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
A. Berthold, N. Fritzsche, T. Herrmann, D. Kirchmeier, T. Kresse, W. F. Mader, M. Maerker, J. Manjarres Ramos, A. Nag, J-E. Nitschke, O. Novgorodova, F. Siegert, M. V. Stange, A. Straessner, S. Todt, H. Torres & C. Wiel
Department of Physics, Duke University, Durham, NC, USA
A. T. H. Arce, J. B. Beacham, D. R. Davis, M. G. Eggleston, A. T. Goshaw, A. Kotwal, M. C. Kruse, K. Pachal, S. Sen, Z. Wang & P. Zhao
SUPA-School of Physics and Astronomy, University of Edinburgh, Edinburgh, UK
S. Alderweireldt, T. M. Carter, P. J. Clark, S. M. Farrington, Y. Gao, R. Y. González Andana, G. N. Hamity, A. Hasib, M. P. Heath, S. Jiggins, C. Leonidopoulos, V. J. Martin, L. Mijović, S. Palazzo, V. A. Parrish, E. A. Pender, E. P. Takeva, N. Themistokleous, E. M. Villhauer, A. Vishwakarma, B. M. Wynne & E. Zaid
INFN e Laboratori Nazionali di Frascati, Frascati, Italy
P. Albicocco, M. Antonelli, C. Arcangeletti, M. Beretta, V. Chiarella, G. Maccarrone, G. Mancini, A. Sansoni, M. Testa & E. Vilucchi
Physikalisches Institut, Albert-Ludwigs-Universität Freiburg, Freiburg, Germany
S. Argyropoulos, F. Becherer, M. Boehler, L. Diehl, A. Froch, S. Gargiulo, S. S. Gurdasani, C. Heidegger, K. K. Heidegger, G. Herten, D. Hohn, J. C. Honig, K. Jakobs, P. Jenni, E. Karentzos, A. Knue, K. Köneke, O. Kuprash, U. Landgraf, V. S. Lang, A. Lösle, V. Magerl, T. Moskalets, Ö. O. Öncel, U. Parzefall, V. Plesanovs, J. Pretel, D. Rafanoharana, A. Rodriguez Rodriguez, B. Roland, B. Rottler, F. Rühr, Z. Rurikova, D. Sammel, F. Sauerburger, K. E. Schleicher, P. G. Scholer, M. Schumacher, S. Solomon, K. Solovieva, D. Sperlich, C. Weiser, L. A. M. Wiik-Fuchs, B. T. Winter, C. J. S. Young & D. Zanzi
II. Physikalisches Institut, Georg-August-Universität Göttingen, Göttingen, Germany
K. Abeling, B. Achkar, W. Alkakhi, J. F. Beirer, M. Bindi, L. O. Gerlach, R. Goncalves Gama, J. Grosse-Knetter, Y. Hong, G. Kawamura, A. Kirchhoff, S. Korn, S. Lai, A. H. Melo, S. Mobius, M. Niemeyer, I. Pokharel, A. Quadt, B. Ravina, C. Scheulen, E. Shabalina, S. Sindhu, A. Skaf, Y. Tian & H. Ye
Département de Physique Nucléaire et Corpusculaire, Université de Genève, Geneve, Switzerland
S. Adorni, C. Antel, K. Axiotis, A. Clark, D. Della Volpe, M. Drozdova, L. F. Ehrke, D. Ferrere, T. Golling, S. Gonzalez-Sevilla, M. Guth, D. Harada, G. Iacobucci, T. Iizawa, S. B. Klein, M. Leigh, C. Moreno Martinez, H. R. Nindhito, L. Paolozzi, G. Quetant, J. A. Raine, C. Rizzi, J. A. Sabater Iglesias, S. Schramm, D. Sengupta, A. Sfyrla, O. Theiner, X. Wu, S. Zambito & K. Zoch
Dipartimento di Fisica, Università di Genova, Genoa, Italy
D. Barberis, G. Gagliardi, A. Lapertosa, F. Parodi, M. Ressegotti, C. Schiavi, F. Sforza, M. Tanasini & L. Vannoli
INFN Sezione di Genova, Genoa, Italy
D. Barberis, A. Coccaro, G. Darbo, G. Gagliardi, C. Gemme, A. Lapertosa, P. Morettini, F. Parodi, S. Passaggio, M. Ressegotti, L. P. Rossi, C. Schiavi, F. Sforza, M. Tanasini & L. Vannoli
II. Physikalisches Institut, Justus-Liebig-Universität Giessen, Giessen, Germany
D. Caforio, M. Düren & H. Stenzel
SUPA-School of Physics and Astronomy, University of Glasgow, Glasgow, UK
R. L. Bates, A. Blue, A. G. Borbély, D. Britton, A. G. Buckley, P. J. Bussey, C. M. Buttar, G. Callea, I. A. Connelly, W. R. Cunningham, A. T. Doyle, F. Fabbri, J. Howarth, J. Jamieson, L. Mince, V. O’Shea, M. Owen, A. G. Rennie, A. Robson, E. L. Simpson, D. P. Spiteri, N. Warrack & K. Wraight
LPSC, Université Grenoble Alpes, CNRS/IN2P3, Grenoble INP, Grenoble, France
J. Collot, S. Crépé-Renaudin, J. B. De Vivie De Regie, P. A. Delsart, M. H. Genest, N. Lalloue, F. Ledroit-Guillon, A. Lucotte, F. Malek, A. P. Pereira Peixoto, S. Shirabe & B. Trocmé
Laboratory for Particle Physics and Cosmology, Harvard University, Cambridge, MA, USA
N. A. Asbah, A. Badea, B. A. Bullard, A. W. Fortman, S. Francescato, M. Franklin, J. Huth, X. Jia, G. V. Kehris, L. Lee, M. Morii, G. Rabanal Bolanos, A. M. Wang, R. Wang & A. S. White
Department of Modern Physics and State Key Laboratory of Particle Detection and Electronics, University of Science and Technology of China, Hefei, China
A. Baroncelli, C. Chen, Y. Chen, M. J. Da Cunha Sargedas De Sousa, D. Du, Y. Fu, J. Gao, A. Giannini, K. Han, L. Han, F. He, Y. Huang, Y. Jiang, C. Li, H. Li, Q. Y. Li, J. B. Liu, M. Liu, M. Y. Liu, X. Liu, Y. W. Liu, R. Ospanov, H. Peng, S. Su, X. Su, C. Wang, T. Wang, W. X. Wang, C. Wei, Y. Wu, Z. Wu, M. Xie, X. Xie, H. Xu, H. Xu, L. Xu, S. Yang, X. Yang, Z. Yang, X. Ye, Z. Zhao, X. Zheng, H. L. Zhu & Y. Zhu
Institute of Frontier and Interdisciplinary Science and Key Laboratory of Particle Physics and Particle Irradiation (MOE), Shandong University, Qingdao, China
H. Atmani, C. Feng, J. Han, B. Li, H. Li, H. Li, T. Li, Z. Li, L. L. Ma, K. Tariq, S. Wang, Z. Xu, R. Yuan, J. Zhang, X. Zhang, T. Zhao & C. G. Zhu
School of Physics and Astronomy, Shanghai Jiao Tong University, Key Laboratory for Particle Astrophysics and Cosmology (MOE), SKLPPC, Shanghai, China
J. Chen, X. Chen, B. Dong, J. Guo, J. Hong, C-Q. Li, J. Li, L. Li, S. Li, D. Liu, K. Liu, Q. Liu, D. Sampsonidou, Q. Shen, W. Su, J. Tang, C. Wang, X. Wang, Z. Wang, J. Yan, H. J. Yang, X. Zhang, Y. Zhang, N. Zhou & Y. Zhu
Tsung-Dao Lee Institute, Shanghai, China
N. Brahimi, C. Kato, S. Li, D. Liu, K. Liu, Q. Liu, D. Sampsonidou, W. Su, Y. Wang, Z. Wang & H. J. Yang
Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L. M. Baltes, F. Bartels, F. L. Castillo, F. Del Rio, M. Dunford, S. Franchino, M. Klassen, T. Mkrtchyan, P. S. Ott, D. F. Rassloff, S. Rodriguez Bosca, H-C. Schultz-Coulon, V. Sothilingam, R. Stamen, P. Starovoitov, S. M. Weber, M. Wessels & X. Yue
Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. M. Czurylo, S. J. Dittmeier, A. Krishnan, C. Sauer, A. Schoening, L. Vigani & J. Zinsser
Department of Physics, Chinese University of Hong Kong, Shatin N.T., Hong Kong, China
H. C. Cheng, K. L. Chu, M. C. Chu, L. R. Flores Castillo, J. M. Iturbe Ponce, K. W. Kwok, T. S. Lau, T. Pan, J. Wang & M. Wu
Department of Physics, University of Hong Kong, Hong Kong, China
S. Huang, D. Paredes Hernandez, C. Peng, K. C. Tam & Y. Tu
Department of Physics and Institute for Advanced Study, Hong Kong University of Science and Technology, Clear Water Bay, Kowloon, Hong Kong, China
K. Lie, K. Prokofiev, J. Xiang & T. Yang
Department of Physics, National Tsing Hua University, Hsinchu, Taiwan
K. Cheung, P. J. Hsu & Y. J. Lu
IJCLab, Université Paris-Saclay, CNRS/IN2P3, 91405, Orsay, France
C. Allaire, A. Bassalat, L. Duflot, M. Escalier, L. Fayard, D. Fournier, J. -F. Grivaz, L. Guo, L. Iconomidou-Fayard, S. Keshri, Y. A. R. Khwaira, A. Lounis, O. Lukianchuk, N. Makovec, N. Morange, P. Puzo, D. Rousseau, A. C. Schaffer, L. Serin, S. Simion, X. Su, J. S. Tafoya Vargas, R. Tanaka, A. Trofymov, D. Varouchas, D. Zerwas & Z. Zhang
Department of Physics, Indiana University, Bloomington, IN, USA
P. Calfayan, H. Evans, B. C. Forland, R. Kopeliansky, S. Lammers, R. A. Linck, F. Luehring, C. Meyer, G. Myers, G. Palacino & C. P. A. Roland
INFN Gruppo Collegato di Udine, Sezione di Trieste, Udine, Italy
B. S. Acharya, M. Cobal, M. Faraj, M. P. Giordani, G. Giugliarelli, G. Guerrieri, J. Magro, G. Panizzo, M. Pinamonti & L. Serkin
ICTP, Trieste, Italy
B. S. Acharya, M. Faraj, G. Guerrieri & L. Serkin
Dipartimento Politecnico di Ingegneria e Architettura, Università di Udine, Udine, Italy
M. Cobal, M. P. Giordani, G. Giugliarelli, J. Magro, G. Panizzo & M. Pinamonti
INFN Sezione di Lecce, Lecce, Italy
M. S. Centonze, G. Chiodini, E. Gorini, F. G. Gravili, M. Greco, L. Longo, A. Palazzo, M. Primavera, E. J. Schioppa, S. Spagnolo & A. Ventura
Dipartimento di Matematica e Fisica, Università del Salento, Lecce, Italy
M. S. Centonze, E. Gorini, F. G. Gravili, M. Greco, L. Longo, A. Palazzo, E. J. Schioppa, S. Spagnolo & A. Ventura
INFN Sezione di Milano, Milan, Italy
G. Alimonti, A. Andreazza, E. Ballabene, A. Carbone, L. Carminati, S. Carrá, M. Citterio, S. Coelli, A. E. C. Coimbra, S. D’Auria, L. Dell’Asta, M. Fanti, D. Giugni, T. Lari, M. Lazzaroni, C. Marcon, C. Meroni, A. Murrone, L. Perini, F. Piazza, F. Ragusa, S. Resconi, A. Stabile, G. F. Tartarelli, C. Troncon & R. Turra
Dipartimento di Fisica, Università di Milano, Milan, Italy
A. Andreazza, E. Ballabene, A. Carbone, L. Carminati, S. Carrá, A. E. C. Coimbra, S. D’Auria, L. Dell’Asta, M. Fanti, M. Lazzaroni, C. Marcon, A. Murrone, L. Perini, F. Piazza, F. Ragusa & A. Stabile
INFN Sezione di Napoli, Naples, Italy
A. Aloisio, M. G. Alviggi, S. Auricchio, V. Canale, G. Carlino, F. Cirotto, F. Conventi, R. De Asmundis, M. Della Pietra, C. Di Donato, A. Doria, P. Iengo, V. Izzo, P. Massarotti, L. Merola, E. Rossi & G. Sekhniaidze
Dipartimento di Fisica, Università di Napoli, Naples, Italy
A. Aloisio, M. G. Alviggi, S. Auricchio, V. Canale, F. Cirotto, M. Della Pietra, C. Di Donato, P. Iengo, P. Massarotti, L. Merola & E. Rossi
INFN Sezione di Pavia, Pavia, Italy
J. Agarwala, R. Ferrari, G. Gaudio, G. Introzzi, A. Kourkoumeli-Charalampidi, A. Lanza, M. Livan, G. Manco, A. Negri, G. Polesello, D. M. Rebuzzi, A. Rimoldi, E. Romano, G. Rovelli & S. Sottocornola
Dipartimento di Fisica, Università di Pavia, Pavia, Italy
J. Agarwala, G. Introzzi, A. Kourkoumeli-Charalampidi, M. Livan, G. Manco, A. Negri, D. M. Rebuzzi, A. Rimoldi, E. Romano, G. Rovelli & S. Sottocornola
INFN Sezione di Pisa, Pisa, Italy
A. Annovi, M. Calvetti, V. Cavasinni, G. Chiarelli, G. Di Gregorio, P. Francavilla, P. Giannetti, S. Leone, P. Mastrandrea, C. Roda, F. Scuri & M. Verducci
Dipartimento di Fisica E. Fermi, Università di Pisa, Pisa, Italy
M. Calvetti, V. Cavasinni, G. Di Gregorio, P. Francavilla, P. Mastrandrea, C. Roda & M. Verducci
INFN Sezione di Roma, Rome, Italy
F. Anulli, G. Artoni, P. Bagnaia, M. Bauce, A. Betti, C. Bini, N. Bruscino, M. Carnesale, A. R. Chomont, M. Corradi, A. De Salvo, F. A. Di Bello, A. Di Domenico, S. Falciano, P. Gauzzi, S. Gentile, S. Giagu, V. Ippolito, M. Kado, F. Lacava, I. Longarini, C. Luci, L. Martinelli, F. Morodei, A. Nisati, G. Padovano, E. Pasqualucci, E. Pompa Pacchi, S. Rosati, L. Sabetta, F. Safai Tehrani, L. Santi, R. Vari & S. Veneziano
Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
G. Artoni, P. Bagnaia, M. Bauce, A. Betti, C. Bini, N. Bruscino, M. Carnesale, A. R. Chomont, M. Corradi, F. A. Di Bello, A. Di Domenico, P. Gauzzi, S. Gentile, S. Giagu, V. Ippolito, M. Kado, F. Lacava, I. Longarini, C. Luci, L. Martinelli, F. Morodei, G. Padovano, E. Pompa Pacchi, L. Sabetta & L. Santi
INFN Sezione di Roma Tor Vergata, Rome, Italy
G. Aielli, E. Alunno Camelia, P. Camarri, R. Cardarelli, L. Cerrito, U. De Sanctis, A. Di Ciaccio, M. Faucci Giannelli, B. Liberti, S. Loffredo, L. Marcoccia, L. Pizzimento, G. Proto, A. Rocchi & M. Vanadia
Dipartimento di Fisica, Università di Roma Tor Vergata, Rome, Italy
G. Aielli, E. Alunno Camelia, P. Camarri, L. Cerrito, U. De Sanctis, A. Di Ciaccio, M. Faucci Giannelli, S. Loffredo, L. Marcoccia, L. Pizzimento, G. Proto, A. Rocchi & M. Vanadia
INFN Sezione di Roma Tre, Rome, Italy
I. Bashta, M. Biglietti, M. T. Camerlingo, B. Di Micco, R. Di Nardo, A. Farilla, M. Iodice, D. Orestano, G. Salamanna & M. Sessa
Dipartimento di Matematica e Fisica, Università Roma Tre, Rome, Italy
I. Bashta, M. T. Camerlingo, B. Di Micco, R. Di Nardo, D. Orestano, G. Salamanna & M. Sessa
INFN-TIFPA, Trento, Italy
M. Cristoforetti, A. Di Luca, F. M. Follega, R. Iuppa, E. Ricci & D. M. S. Sultan
Università degli Studi di Trento, Trento, Italy
M. Cristoforetti, A. Di Luca, F. M. Follega, R. Iuppa, E. Ricci & D. M. S. Sultan
Department of Astro and Particle Physics, Universität Innsbruck, Innsbruck, Austria
E. Kneringer & A. Thaler
University of Iowa, Iowa City, IA, USA
M. Cano Bret, D. Garg, M. Lu, U. Mallik, P. Sharma & W. T. Wang
Department of Physics and Astronomy, Iowa State University, Ames, IA, USA
W. D. Heidorn, N. Krumnack, A. Lebedev & S. Tapia Araya
Departamento de Engenharia Elétrica, Universidade Federal de Juiz de Fora (UFJF), Juiz de Fora, Brazil
V. Araujo Ferraz, A. S. Cerqueira, L. Manhaes de Andrade Filho & D. Oliveira Goncalves
Universidade Federal do Rio De Janeiro COPPE/EE/IF, Rio de Janeiro, Brazil
Y. Amaral Coutinho, L. P. Caloba, J. V. Da Fonseca Pinto, E. Egidio Purcino De Souza, W. S. Freund, P. Gaspar, J. Lieber Marin, C. Maidantchik, N. M. J. Nunes De Moura Junior, J. M. Seixas & M. Verissimo De Araujo
Instituto de Física, Universidade de São Paulo, São Paulo, Brazil
M. Donadelli & M. A. L. Leite
Rio de Janeiro State University, Rio de Janeiro, Brazil
M. Begalli & B. S. Peralva
KEK, High Energy Accelerator Research Organization, Tsukuba, Japan
M. Aoki, K. Hanagaki, Y. Ikegami, A. Mizukami, K. Nagano, Y. Nakahama, K. Nakamura, O. Sasaki, Y. Takubo, M. Togawa, K. Tokushuku, M. Tomoto & S. Tsuno
Graduate School of Science, Kobe University, Kobe, Japan
H. Hibi, H. Kurashige, J. Maeda, A. Ochi, K. Takeda & Y. Yamazaki
AGH University of Science and Technology, Faculty of Physics and Applied Computer Science, Kraków, Poland
L. Adamczyk, T. Bold, K. M. Ciesla, W. Dabrowski, M. Dyndal, A. K. Gilbert, I. Grabowska-Bold, K. W. Janas, S. Koperny, I. K. Lakomiec, K. Maj, B. Mindur, A. Ogrodnik, M. Przybycien & R. Sikora
Marian Smoluchowski Institute of Physics, Jagiellonian University, Kraków, Poland
D. T. Gil, M. Palka, E. Richter-Was & K. W. Topolnicki
Institute of Nuclear Physics Polish Academy of Sciences, Kraków, Poland
E. Banas, P. A. Bruckman de Renstrom, J. J. Chwastowski, D. Derendarz, B. S. Dziedzic, P. A. Erland, A. Kaczmarska, K. Korcyl, J. A. Krzysiak, M. P. Lewicki, Pa. Malecki, A. Olszewski, J. Olszowska, P. Patel, M. Slawinska, A. Smykiewicz, E. Stanecka, R. Staszewski, M. Trzebinski, A. Trzupek, M. W. Wolter, B. K. Wosiek, K. W. Woźniak & B. Zabinski
Faculty of Science, Kyoto University, Kyoto, Japan
R. Kobayashi, Y. Mino, Y. Noguchi, Y. Okazaki, T. Sumida & Y. Tsujikawa
Kyoto University of Education, Kyoto, Japan
R. Takashima
Research Center for Advanced Particle Physics and Department of Physics, Kyushu University, Fukuoka, Japan
K. Kawagoe, D. Kobayashi, Y. Miyazaki, H. Otono, J. Tojo & N. Yamaguchi
Instituto de Física La Plata, Universidad Nacional de La Plata and CONICET, La Plata, Argentina
F. Alonso, M. T. Dova, F. Monticelli, S. J. Noacco Rosende, G. E. Orellana, F. Sili & H. Wahlberg
Physics Department, Lancaster University, Lancaster, UK
A. E. Barton, I. A. Bertram, G. Borissov, E. V. Bouhova-Thacker, H. Fox, R. C. W. Henderson, R. W. L. Jones, V. Kartvelishvili, P. A. Love, L. Meng, D. Muenstermann, K. Rybacki, M. Smizanska, S. Spinali, A. M. Wharton & M. R. Yexley
Oliver Lodge Laboratory, University of Liverpool, Liverpool, UK
E. Arena, A. Biondini, S. Burdin, P. Dervan, M. D’Onofrio, R. Gonzalez Lopez, C. B. Gwilliam, H. S. Hayward, A. E. Jaspan, T. J. Jones, M. Klein, U. Klein, J. Kretzschmar, T. F. Lee, Z. Li, H. Lyons, C. M. Mcpartland, A. Mehta, M. W. O’Keefe, J. Patton, N. Rompotis, A. J. Ruby, C. D. Sebastiani, J. L. Smith, M. J. Sullivan, H. Teagle & J. H. Vossebeld
Department of Experimental Particle Physics, Jožef Stefan Institute and Department of Physics, University of Ljubljana, Ljubljana, Slovenia
V. Cindro, A. Filipčič, A. Gorišek, B. Hiti, A. S. Howard, B. P. Kerševan, G. Kramberger, B. Leban, I. Mandić, B. Maček, M. Mikuž & J. Novak
School of Physics and Astronomy, Queen Mary University of London, London, UK
A. J. Bevan, U. Blumenschein, M. Bona, T. P. Charman, I. Dawson, A. A. Elliot, A. C. Freegard, R. Gamboa Goni, K. Ghorbanian, J. M. Hays, N. D. Hehir, M. P. J. Landon, S. L. Lloyd, J. P. Mandalia, P. S. Miyagawa, T. Qiu, E. Rizvi, E. J. Thorpe, L. Vozdecky & S. Zenz
Department of Physics, Royal Holloway University of London, Egham, UK
S. Ahuja, T. Berry, V. Boisvert, C. D. Booth, G. Cowan, S. George, S. M. Gibson, S. D. Lawlor, H. P. Lefebvre, J. G. Panduro Vazquez, F. Pastore, J. D. Shinner, F. Spanò, P. Teixeira-Dias, D. W. Thomas & P. J. Verschuuren
Department of Physics and Astronomy, University College London, London, UK
G. Barbour, L. S. Borgna, J. M. Butterworth, M. Campanelli, G. Facini, C. Gutschow, E. H. Haines, D. P. Huang, A. S. Kelly, N. Kimura, N. Konstantinidis, A. Korn, N. N. Lad, A. C. A. Lee, Y. Ma, A. C. Martyniuk, D. J. Mclaughlin, T. Mlinarevic, R. R. B. Norisam, E. Nurse, C. Pitman Donaldson, T. Scanlon, P. Sherwood, L. Shi, A. L. Sopio, S. Van Stroud, B. M. Waugh, Y. Yeh & L. Yue
Louisiana Tech University, Ruston, LA, USA
L. Sawyer & M. Wobisch
Fysiska Institutionen, Lunds Universitet, Lund, Sweden
T. P. A. Åkesson, E. E. Corrigan, C. Doglioni, P. A. Ekman, J. Geisen, V. Hedberg, H. Herde, G. Jarlskog, B. Konya, E. Lytken, J. U. Mjörnmark, G. A. Mullier, R. Poettgen, N. D. Simpson, E. Skorda & O. Smirnova
Departamento de Física Teorica C-15 and CIAFF, Universidad Autónoma de Madrid, Madrid, Spain
M. Alvarez Estevez, F. Barreiro, J. Del Peso, C. Glasman, M. A. Principe Martin & J. Terron
Institut für Physik, Universität Mainz, Mainz, Germany
A. Aggarwal, M. Akbiyik, J. Balz, A. Basan, J. Blumenthal, B. Brickwedde, V. Büscher, J. Damp, F. Fiedler, M. Geisen, R. Gugel, A. Hadef, C. Kahra, P. D. Kennedy, P. Kramer, J. A. Kremer, A. Laudrain, L. Masetti, F. Neuhaus, S. Rave, A. Reiss, M. Robles Manzano, U. Schäfer, B. Schlag, K. Schmieden, C. Schmitt, M. Schott, D. Ta, S. Tapprogge, E. Tzovara, O. Vujinovic, R. -J. Wang, M. Weirich & N. Wieseotte
School of Physics and Astronomy, University of Manchester, Manchester, UK
M. Aly, D. A. Baron Moreno, C. R. Basson, C. J. Birch-sykes, A. Bitadze, S. E. Clawson, C. Da Via, C. Doglioni, M. D’uffizi, S. Dysch, A. C. Forti, R. Hankache, T. G. Hitchings, B. P. Honan, Z. Huang, Z. Lawrence, B. Le, J. Masik, F. J. Munoz Sanchez, M. Murin, A. Oh, J. R. Pater, R. F. Y. Peters, A. D. Pilkington, D. Price, D. Qichen, Y. Qin, M. Queitsch-Maitland, S. M. Shaw, V. Vecchio, J. K. Winter & T. R. Wyatt
CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France
G. Aad, M. Barbero, T. P. Calvet, N. Chiedde, Y. Coadou, C. Diaconu, F. Djama, A. Duperrin, L. Feligioni, E. Fortin, G. D. Hallewell, N. Kumari, L. A. O. Laatu, E. Monnier, S. Muanza, E. Nagy, E. Petit, A. Rozanov, J. Stark, T. Strebler, M. Talby, G. Tarna, S. Tisserant & A. Vallier
Department of Physics, University of Massachusetts, Amherst, MA, USA
D. C. Abbott, B. Brau, Y. Chou, R. Coelho Lopes De Sa, C. Dallapiccola, M. Javurkova, S. Krishnamurthy, A. K. Kvam, R. J. Langenberg, W. A. Leight, V. I. Martinez Outschoorn, E. J. W. Moyse, J. A. Sandesara, P. Tornambe, M. J. Veen, M. Vessella, C. Wagner & S. Willocq
Department of Physics, McGill University, Montreal, QC, Canada
W. S. Ahmed, A. Ambler, A. Canesse, F. Corriveau, R. Hulsken, T. Kwan, X. Li, Z. Li, J. P. Mc Gowan, C. Nelson, S. H. Robertson, S. Saha, S. Stärz, B. Vachon & A. Warburton
School of Physics, University of Melbourne, Melbourne, VIC, Australia
E. L. Barberio, S. Goldfarb, E. F. McDonald, P. C. McNamara, T. Pham, F. Scutti, J. Shojaii, G. N. Taylor & P. Urquijo
Department of Physics, University of Michigan, Ann Arbor, MI, USA
D. Amidei, P. A. Atmasiddha, A. Chen, T. Dai, E. B. Diehl, C. Ferretti, P. Fleischmann, C. Grud, L. Guan, J. A. M. Guhit, Y. Guo, C. Hayes, M. H. Klein, N. G. Kyriacou, D. Levin, Y. L. Liu, S. P. Mc Kee, G. Merz, K. Nelson, J. Qian, T. A. Schwarz, S. Sun, M. Tsai, Z. Wang, Z. Wang, X. Xiao, T. Xu, W. Xu, Z. Yang, M. Yuan, S. Zhang, B. Zhou & J. Zhu
Department of Physics and Astronomy, Michigan State University, East Lansing, MI, USA
C. J. Buxo Vazquez, H. De la Torre, T. Farooque, W. C. Fisher, J. P. Gombas, R. Hauser, D. Hayden, J. Huston, K. S. Krowpman, R. Les, K. Lin, M. Mazza, I. Pogrebnyak, R. Schwienhorst & A. Tarek Abouelfadl Mohamed
Group of Particle Physics, University of Montreal, Montreal, QC, Canada
J-F. Arguin, G. Azuelos, H. M. Borecka-Bielska, D. Godin, C. Leroy, K. Mochizuki, H. D. N. Nguyen, C. Papadatos, B. Pascual Dias & M. Usman
Fakultät für Physik, Ludwig-Maximilians-Universität München, Munich, Germany
C. G. Ames, Z. P. Arrubarrena Tame, O. Biebel, V. D’Amico, G. Duckeck, N. M. Hartmann, M. G. Herrmann, R. Hertenberger, C. S. Jagfeld, F. F. Klitzner, F. Krieter, J. Lorenz, A. M. Lory, A. Mann, S. Mehlhase, P. Mogg, K. E. Penski, M. P. Rinnagel, D. Schaile, E. Schanet, C. Valderanis, F. Vogel & R. Walker
Max-Planck-Institut für Physik (Werner-Heisenberg-Institut), Munich, Germany
T. Barillari, S. Bethke, D. Britzger, D. Cieri, D. Duda, F. Guescini, S. Hadzic, L. Heinrich, M. Holzbock, A. Hönle, J. Jimenez Pena, A. E. Kiryunin, F. Klimpel, S. Kluth, O. Kortner, S. Kortner, H. Kroha, S. R. Maschek, S. Menke, R. Nisius, M. B. Rendel, R. Richter, M. Sahinsoy, P. Schacht, M. Spalla, S. Stonjek, A. Verbytskyi, E. Voevodina, V. M. Walbrecht & N. S. Wenke
Graduate School of Science and Kobayashi-Maskawa Institute, Nagoya University, Nagoya, Japan
H. Asada, S. Hayashida, Y. Horii, Y. Kano, M. Tomoto & M. Wakida
Department of Physics and Astronomy, University of New Mexico, Albuquerque, NM, USA
A. Grummer, E. A. Narayanan, R. Novotny & S. C. Seidel
Institute for Mathematics, Astrophysics and Particle Physics, Radboud University/Nikhef, Nijmegen, The Netherlands
S. Caron, N. De Groot, P. Ferrari, F. Filthaut, L. Franco, M. C. Missio, P. Moskvitina, C. Nellist, A. Perrevoort & M. Wu
Nikhef National Institute for Subatomic Physics and University of Amsterdam, Amsterdam, The Netherlands
A. Alfonsi, H. Arnold, P. J. Bakker, R. Balasubramanian, S. Bentvelsen, G. J. Bobbink, L. Brenner, E. Cherepanova, E. Y. S. Chow, M. De Beurs, P. de Jong, J. Degens, F. A. Dias, T. A. du Pree, Z. Feng, P. Ferrari, G. Gilles, P. Kluit, B. Kortman, A. E. McDougall, C. E. Pandini, F. Pasquali, A. Pizzini, H. L. Snoek, M. Stamenkovic, I. Van Vulpen, W. Verkerke, J. C. Vermeulen, M. Vozak & M. Vreeswijk
Department of Physics, Northern Illinois University, DeKalb, IL, USA
J. Adelman, D. Chakraborty, L. D’Eramo, B. L. Dwyer, W. H. Kostecka, A. N. Lancaster & E. W. Parrish
University of Sharjah, Sharjah, United Arab Emirates
R. Soualah
Department of Physics, New York University, New York, NY, USA
Y. Abulaiti, K. Cranmer, A. Haas, A. I. Mincer & P. Rieck
Ochanomizu University, Otsuka, Bunkyo-ku, Tokyo, Japan
K. Asai, M. Fujimoto & T. Kono
Ohio State University, Columbus, OH, USA
A. Boveia, B. M. Cote, K. K. Gan, N. M. Harrison, R. Joshi, H. Kagan, M. Montella, Z. B. Pollock, B. Reynolds, R. Rosten & S. Shrestha
Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK, USA
B. Abbott, M. Alhroob, P. Gutierrez, J. E. Lambert, M. Marjanovic, J. M. Muse, A. R. Roepe-Gier, H. Severini, P. Skubic, M. Strauss, J. Stupak & D. J. Wilbern
Department of Physics, Oklahoma State University, Stillwater, OK, USA
E. Antipov, V. S. Bhopatkar, J. Haley, A. Khanov, F. Rizatdinova & E. R. Vandewall
Palacký University, Joint Laboratory of Optics, Olomouc, Czech Republic
P. Baron, K. Cerny, P. Hamal, M. Hrabovsky, T. Komarek, J. Kvita, L. Nozka, J. Pacalt & R. Privara
Institute for Fundamental Science, University of Oregon, Eugene, OR, USA
R. Bielski, J. E. Brau, D. E. Fellers, G. R. Gledhill, M. Glisic, G. Gonella, J. J. Heinrich, L. Jeanty, A. Kilgallon, N. A. Luongo, S. Majewski, A. L. Steinhebel, D. M. Strom, E. Torrence, K. Whalen & F. Winklmeier
Graduate School of Science, Osaka University, Osaka, Japan
M. Hirose, H. Nanjo & L. Wickremasinghe
Department of Physics, University of Oslo, Oslo, Norway
V. Ananiev, K. Bjørke, M. K. Bugge, D. Cameron, J. R. Catmore, E. Gramstad, E. S. Haaland, A. L. Heggelund, S. Hellesund, V. Morisbak, F. Ould-Saada, M. Pedersen, A. L. Read, O. Røhne, E. B. Rye, H. Sandaker, D. R. Shope, K. O. H. Vadla & M. Van Rijnbach
Department of Physics, Oxford University, Oxford, UK
A. J. Barr, D. Bortoletto, T. L. Bruckler, F. Celli, E. I. Conroy, A. M. Cooper-Sarkar, M. A. Draguet, J. A. Frost, G. E. Gallardo, E. J. Gallas, J. C. Grundy, C. Gwenlan, Y. T. Harris, C. P. Hays, T. B. Huffman, K. Karava, Z. Li, C. Merlassino, M. Mironova, K. Nagai, L. Nedic, R. B. Nickerson, C. S. Pollard, K. Potamianos, E. Schopf, I. P. J. Shipsey, H. A. Smith, M. Stankaityte, I. Veliscek, G. H. A. Viehhauser, Y. Wei, A. R. Weidberg, P. J. Windischhofer, R. Wölker, J. Wuerzinger & S. Yan
LPNHE, Sorbonne Université, Université Paris Cité, CNRS/IN2P3, Paris, France
T. Beau, G. Calderini, R. Camacho Toro, F. Crescioli, F. Derue, L. Ginabat, Y. He, M. Khandoga, M. W. Krasny, D. Lacour, B. Laforge, B. Malaescu, I. Nikolic-Audit, J. Ocariz, L. Poggioli, V. Raskina, M. Ridel, L. Roos, R. H. M. Taibah & S. Trincaz-Duvoid
Department of Physics, University of Pennsylvania, Philadelphia, PA, USA
J. R. Dandoy, L. Flores, L. F. Gutierrez Zagazeta, J. G. Heinlein, A. Kahn, J. Kroll, E. Lipeles, S. Lu, J. J. Mullin, N. Proklova, J. D. Shahinian, E. Thomson, H. H. Williams & R. Xu
Department of Physics and Astronomy, University of Pittsburgh, Pittsburgh, PA, USA
M. Bandieramonte, R. M. Bianchi, J. Boudreau, H. Cai, B. T. Carlson, T. M. Hong, J. Mueller, A. A. Myers, C. W. Ng & H. J. Stelzer
Laboratório de Instrumentação e Física Experimental de Partículas-LIP, Lisbon, Portugal
S. P. Amor Dos Santos, M. G. Barros Teixeira, N. F. Castro, R. F. Coelho Barrue, P. Conde Muiño, G. Evans, M. C. N. Fiolhais, A. Gomes, R. Gonçalo, A. Maio, E. D. Mendes Gouveia, A. L. Moreira De Carvalho, I. Ochoa, L. F. Oleiro Seabra, A. Onofre, R. Pedro, B. C. Pinheiro Pereira, H. Santos, J. G. Saraiva, M. Stolarski, F. Veloso & H. Wolters
Departamento de Física, Faculdade de Ciências, Universidade de Lisboa, Lisbon, Portugal
A. Gomes, A. Maio & H. Santos
Departamento de Física, Universidade de Coimbra, Coimbra, Portugal
M. C. N. Fiolhais, R. Gonçalo, F. Veloso & H. Wolters
Centro de Física Nuclear da Universidade de Lisboa, Lisbon, Portugal
A. Maio & J. G. Saraiva
Departamento de Física, Universidade do Minho, Braga, Portugal
N. F. Castro & A. Onofre
Departamento de Física Teórica y del Cosmos, Universidad de Granada, Granada, Spain
J. A. Aguilar-Saavedra & M. Chala
Departamento de Física, Instituto Superior Técnico, Universidade de Lisboa, Lisbon, Portugal
P. Conde Muiño
Institute of Physics of the Czech Academy of Sciences, Prague, Czech Republic
J. Chudoba, P. Federicova, J. Hejbal, P. Jacka, O. Kepka, J. Kroll, A. Kupco, V. Latonova, M. Lokajicek, R. Lysak, M. Marcisovsky, M. Mikestikova, S. Nemecek, P. Sicho, P. Staroba, M. Svatos & M. Tasevsky
Czech Technical University in Prague, Prague, Czech Republic
B. Ali, K. Augsten, B. Bergmann, T. R. V. Billoud, M. Havranek, Z. Hubacek, P. Jacka, S. Mondal, M. Myska, L. Novotny, V. Petousis, R. Polifka, S. Pospisil, K. Smolek, A. Sopczak, V. Vacek, P. Vokac & O. Zaplatilek
Faculty of Mathematics and Physics, Charles University, Prague, Czech Republic
P. Balek, P. Berta, T. Davidek, J. Dolejsi, Z. Dolezal, J. Faltova, P. Kodyš, M. Krivos, R. Leitner, K. Petukhova, V. Pleskot, S. Polacek, P. Reznicek, M. Rybar, D. Scheirich, M. Spousta, M. Sykora, T. Sykora, P. Tas, S. Todorova-Nova & V. Vorobel
Particle Physics Department, Rutherford Appleton Laboratory, Didcot, UK
T. Adye, J. T. Baines, G. A. Bird, W. Buttinger, J. Dopke, D. Emeliyanov, B. J. Gallop, E. Guilloton, J. Kirk, S. Martin-Haugh, S. J. McMahon, R. P. Middleton, W. J. Murray, R. E. Owen, P. W. Phillips, D. P. C. Sankey, C. Sawyer, B. H. Smart, J. Walder & M. Wielers
IRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France
H. Bachacou, F. Balli, M. Boonekamp, L. Chevalier, F. Deliot, A. Formica, P. F. Giraud, C. Guyot, F. Jeanneau, T. Kawamoto, M. Kolb, A. Kotsokechagia, W. Kozanecki, J. F. Laporte, M. Manisha, B. Mansoulie, J-P. Meyer, R. Nicolaidou, A. Peyaud, M. Saimpert, L. Schoeffel, Ph. Schune, Ph. Schwemling, M. Vandenbroucke & Z. Wu
Santa Cruz Institute for Particle Physics, University of California Santa Cruz, Santa Cruz, CA, USA
A. A. Affolder, M. Battaglia, V. Fadeyev, C. M. Gee, M. Gignac, A. A. Grillo, M. Hance, N. J. Kang, S. M. Mazza, J. Nielsen, H. F-W. Sadrozinski, B. A. Schumm, A. Sciandra, A. Seiden, G. H. Stark & Y. Zhao
Departamento de Física, Pontificia Universidad Católica de Chile, Santiago, Chile
A. C. Abusleme Hoffman, M. A. Diaz & F. M. Garay Walls
Millennium Institute for Subatomic physics at high energy frontier (SAPHIR), Santiago, Chile
M. A. Diaz, F. M. Garay Walls & S. Kuleshov
Instituto de Investigación Multidisciplinario en Ciencia y Tecnología, y Departamento de Física, Universidad de La Serena, Chile
P. A. Ulloa Poblete
Universidad Andres Bello, Department of Physics, Santiago, Chile
S. Kuleshov & J. A. Zamora Saa
Instituto de Alta Investigación, Universidad de Tarapacá, Arica, Chile
S. Kabana, T. Lagouri & S. A. Olivares Pino
Departamento de Física, Universidad Técnica Federico Santa María, Valparaiso, Chile
W. K. Brooks, E. Carquin, R. Pezoa, C. M. Robles Gajardo & N. Viaux Maira
Department of Physics, University of Washington, Seattle, WA, USA
C. Alpigiani, Q. Buat, S. J. Gasiorowski, A. G. Goussiou, S. -C. Hsu, E. E. Khoda, K. Li, Q. Liu, H. J. Lubatti, M. L. Proffitt, J. Schaarschmidt, W. Su, T. R. Van Daalen, G. Watts & H. Zhao
Department of Physics and Astronomy, University of Sheffield, Sheffield, UK
C. Anastopoulos, M. T. Anthony, D. Costanzo, A. Fell, J. J. Hall, M. C. Hodgkinson, P. Johansson, K. Lohwasser, J. C. MacDonald, H. Maguire, H. Mildner, M. B. Norfolk, J. E. Puddefoot, N. P. Readioff, K. A. Saoucha, D. R. Tovey, T. Vickey, O. E. Vickey Boeriu, D. F. Zhang & T. G. Zorbas
Department of Physics, Shinshu University, Nagano, Japan
Y. Hasegawa & K. Kawade
Department Physik, Universität Siegen, Siegen, Germany
B. Batool, P. Buchholz, M. Cristinziani, C. Diez Pardos, F. Fischer, I. Fleck, M. Ghneimat, A. Ghosal, G. Gomes Da Silva, I. Ibragimov, V. V. Kostyukhin, J. K. R. Meshreki, B. Mondal, A. Petrukhin, A. Rej, W. Walkowiak & M. Ziolkowski
Department of Physics, Simon Fraser University, Burnaby, BC, Canada
J. C. Burzynski, M. Danninger, T. Dias Do Vale, E. Drechsler, H. Hanif, B. P. Jaeger, K. Lehmann, B. X. Liu, J. Llorente Merino, D. C. O’Neil, A. Poley, S. Singh, B. Stelzer & M. C. Vetterli
SLAC National Accelerator Laboratory, Stanford, CA, USA
T. Barklow, R. Bartoldus, C. Bernius, L. Bryngemark, S. Cheong, A. R. Cukierman, R. B. Garg, P. Grenier, N. M. Hartman, R. Hyneman, M. Kagan, M. Kocian, J. Pearkes, M. Safdari, A. Salnikov, A. Schwartzman, S. Sevova, R. Smith, D. Su, R. Teixeira De Lima, L. Tompkins, C. Vernieri, M. Wittgen, C. Young & Z. Zheng
Department of Physics, Royal Institute of Technology, Stockholm, Sweden
A. Leopold, O. Lundberg, B. Lund-Jensen, C. C. Ohm, G. Ripellino, R. Shaheen & J. Strandberg
Departments of Physics and Astronomy, Stony Brook University, Stony Brook, NY, USA
C. P. Bee, A. Behera, S. Bhatta, Y. Hernández Jiménez, J. Hobbs, J. Jia, Y. Ke, I. Luise, G. Piacquadio, M. Rijssenbeek, R. D. Schamberger, F. Tsai, V. Tsiskaridze & D. Tsybychev
Department of Physics and Astronomy, University of Sussex, Brighton, UK
B. M. M. Allbrooke, M. A. Aparo, A. Cerri, A. De Santo, Z. O. Earnshaw, M. O. Evans, M. Grandi, D. Kelsey, D. M. Koeck, O. Kovanda, J. A. Mcfayden, B. Safarzadeh Samani, F. Salvatore, K. Shaw, M. Spina, T. J. Stevenson, M. R. Sutton, I. Vivarelli & I. Xiotidis
School of Physics, University of Sydney, Sydney, Australia
S. Balaji, T. Nommensen, K. E. Varvell & B. Yabsley
Institute of Physics, Academia Sinica, Taipei, Taiwan
S. Ali, H. El Jarrari, S. Hou, S. C. Lee, R. Mazini, T. Varol & S. M. Wang
E. Andronikashvili Institute of Physics, Iv. Javakhishvili Tbilisi State University, Tbilisi, Georgia
J. Jejelava & E. G. Tskhadadze
High Energy Physics Institute, Tbilisi State University, Tbilisi, Georgia
B. Chargeishvili, T. Djobava, A. Durglishvili, J. Khubua, G. Mchedlidze, I. A. Minashvili, M. Mosidze & T. Zakareishvili
Department of Physics, Technion, Israel Institute of Technology, Haifa, Israel
H. Abreu, G. Avner, E. Kajomovitz, D. Melini, Y. Rozen, S. Tarem & O. Tsur
Raymond and Beverly Sackler School of Physics and Astronomy, Tel Aviv University, Tel Aviv, Israel
H. Abramowicz, L. Barak, U. Barron, G. Bella, Y. Benhammou, B. Chen, H. Cohen, E. Etzion, G. Koren, M. S. Lutz, R. Nayak, L. Pascual Dominguez, D. Reikher, A. Soffer, N. M. Tamir & D. Vannicola
Department of Physics, Aristotle University of Thessaloniki, Thessaloniki, Greece
K. Bachas, I. Karkanias, E. Kasimi, K. Kordas, C. Lampoudis, A. Leisos, I. M. Maniatis, A. Marantis, I. Maznas, C. Petridou, D. Sampsonidis, A. Tsiamis, A. Tsirigotis, M. Tsopoulou, S. Tzamarias & A. Vgenopoulos
International Center for Elementary Particle Physics and Department of Physics, University of Tokyo, Tokyo, Japan
T. Aoki, S. Asai, W. Y. Chan, S. Chen, Y. Enari, S. Ganguly, R. Iguchi, M. Ishino, T. Kishimoto, T. Mashimo, T. Masubuchi, N. Matsuzawa, M. Morinaga, T. Nobe, R. Oishi, Y. Okumura, M. Saito, T. Saito, R. Sawada, K. Sugizaki, A. Tanaka, J. Tanaka, G. Tateno, K. Terashi, K. Uchida, J. Zang & T. Zhang
Department of Physics, Tokyo Institute of Technology, Tokyo, Japan
Y. He, O. Jinnouchi, S. Kanayama, E. Kim, A. Kubota, M. Kuze, H. Oide, R. Ushioda & Y. Yamaguchi
Department of Physics, University of Toronto, Toronto, ON, Canada
L. Adamek, O. Arnaez, M. J. Basso, J. W. S. Carter, A. F. Casha, B. M. Ciungu, K. Dette, J. H. Foo, A. Gabrielli, C. A. Garner, N. Giangiacomi, Y. F. Han, N. Ilic, A. Kamenshchikov, S. Ketabchi Haghighat, D. P. Kisliuk, T. M. Knight, P. Krieger, H. Y. Meng, O. Miu, D. P. Mungo, R. S. Orr, T. H. Park, P. Savard, P. Sinervo, S. Singh, J. J. Teoh, R. J. Teuscher & L. M. Veloce
TRIUMF, Vancouver, BC, Canada
E. M. Carlson, S. V. Chekulaev, N. P. Hessey, L. L. Kurchaninov, E. Perez Codina, A. Poley, D. M. Portillo Quintero, B. Stelzer, O. Stelzer-Chilton, M. Swiatlowski, R. Tafirout, I. M. Trigger, S. Tsigaridas & M. Valente
Department of Physics and Astronomy, York University, Toronto, ON, Canada
C. David, M. J. Kareem, A. M. Rodríguez Vera, W. Y. Song, D. M. Starko & W. Taylor
Division of Physics and Tomonaga Center for the History of the Universe, Faculty of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Japan
K. Hara, S. Hirose, K. Sato, F. Ukegawa, S. Wada, R. Wakasa & H. Yamauchi
Department of Physics and Astronomy, Tufts University, Medford, MA, USA
P. H. Beauchemin, V. Croft, A. S. Drobac & F. I. Kaya
United Arab Emirates University, Al Ain, United Arab Emirates
M. Belfkir
Department of Physics and Astronomy, University of California Irvine, Irvine, CA, USA
T. Cuhadar Donszelmann, M. J. Fenton, A. Ghosh, A. J. Lankford, K. Ntekas, J. L. Oliver, M. J. R. Olsson, J. T. Roemer, M. Schernau, A. Taffard, G. Unel, D. Whiteson & J. Wollrath
Department of Physics and Astronomy, University of Uppsala, Uppsala, Sweden
E. Bergeaas Kuutmann, R. Brenner, C. Dimitriadi, T. Ekelof, V. Ellajosyula, M. Ellert, A. Ferrari, R. Gonzalez Suarez, T. Mathisen, S. Oerdek, J. Steentoft & O. Sunneborn Gudnadottir
Department of Physics, University of Illinois, Urbana, IL, USA
M. Atkinson, V. R. Bailey, Y. Cao, M. Feickert, B. H. Hooberman, J. D. Long, R. Longo, M. S. Neubauer, M. W. Phipps, A. C. Romero Hernandez, A. Roy, A. M. Sickles, A. C. Tate, X. Wang, J. C. Zeng & D. Zhong
Instituto de Física Corpuscular (IFIC), Centro Mixto Universidad de Valencia-CSIC, Valencia, Spain
K. R. Amos, J. A. Aparisi Pozo, A. J. Bailey, N. Bouchhar, S. Cabrera Urbán, J. Cantero, F. Cardillo, V. Castillo Gimenez, M. Chitishvili, M. J. Costa, M. Didenko, C. Escobar, L. Fiorini, E. Fullana Torregrosa, J. Fuster, C. García, J. E. García Navarro, A. J. Gomez Delegido, S. González de la Hoz, G. R. Gonzalvo Rodriguez, J. G. R. Guerrero Rojas, E. Higón-Rodriguez, C. Lacasta, J. J. Lozano Bahilo, S. Marti-Garcia, P. Martinez Agullo, M. Miralles Lopez, V. A. Mitsou, L. Monsonis Romero, M. Moreno Llácer, D. Munoz Perez, J. Navarro-Gonzalez, J. Poveda, A. Prades Ibanez, A. Rubio Jimenez, A. Ruiz-Martinez, P. Sabatini, J. Salt, J. Sánchez, V. Sanchez Sebastian, I. Sayago Galvan, V. Senthilkumar, U. Soldevila, E. Torró Pastor, A. Valero, J. A. Valls Ferrer, L. Varriale, M. Villaplana Perez & M. Vos
Department of Physics, University of British Columbia, Vancouver, BC, Canada
F. Cormier, C. Gay, C. Gubbels, R. L. Hayes, C. M. Helling, A. Lister, R. Newhouse, A. S. Sharma, Z. Tao & V. W. S. Wong
Department of Physics and Astronomy, University of Victoria, Victoria, BC, Canada
J. Albert, C. Camincher, E. M. Carlson, B. Chen, Y. H. Chiu, M. Ghasemi Bostanabad, K. Hamano, E. F. Kay, R. Keeler, R. Kowalewski, M. Lefebvre, D. M. Mac Donell, K. D. McLean, R. A. McPherson, J. C. Rivera Vergara, R. A. Rojas, H. L. Russell, M. J. Shroff, R. Sobie & G. A. Vasquez
Fakultät für Physik und Astronomie, Julius-Maximilians-Universität Würzburg, Würzburg, Germany
D. S. Bhattacharya, M. Haleem, G. Khoriauli, L. Klein, R. Ströhmer, T. Swirski & T. Trefzger
Department of Physics, University of Warwick, Coventry, UK
K. Becker, E. Guilloton, P. F. Harrison, E. Jones, B. P. Kerridge, T. A. Martin, A. Mitra, S. Morgenstern, W. J. Murray, B. A. Roberts & V. Vladimirov
Waseda University, Tokyo, Japan
H. Ito, T. Kaji, T. Mitani, Y. Shimogama & K. Yorita
Department of Particle Physics and Astrophysics, Weizmann Institute of Science, Rehovot, Israel
I. Aizenberg, M. Birman, R. Brener, S. Bressler, Z. H. Citron, E. Dreyer, E. Duchovni, E. Gross, N. Hod, A. Ivina, T. Jakoubek, N. Kakati, L. J. Levinson, D. C. Mankad, G. Mikenberg, A. Milov, I. Ravinovich, A. Santra, D. Shaked Renous, J. Shlomi & V. Smakhtin
Department of Physics, University of Wisconsin, Madison, WI, USA
D. Biswas, J. Chan, C. L. Cheng, W. Guan, A. Held, W. Islam, T. M. Pham, S. Sun, A. S. Tee, A. Z. Wang, W. Wiedenmann, S. L. Wu, R. Zhang & C. Zhou
Fakultät für Mathematik und Naturwissenschaften, Fachgruppe Physik, Bergische Universität Wuppertal, Wuppertal, Germany
V. A. Austrup, G. Brandt, C. Dülsen, F. Ellinghaus, M. Errenst, T. Flick, T. Harenberg, D. Hirschbuehl, G. Jäkel, S. Kersten, J. A. Reidelsturz, M. Rezaei Estabragh, J. Roggel, M. Sandhoff, M. A. Schmidt, F. Schroeder, O. Thielmann, W. Wagner, S. Wahdan & C. Zeitnitz
Department of Physics, Yale University, New Haven, CT, USA
O. K. Baker, E. G. Castiglia, S. Demers, J. Pan, G. Pezzullo, C. O. Shimmin & P. Tipton
Affiliated with an institute covered by a cooperation agreement with CERN, Geneva, Switzerland
G. A. Chelkov, O. L. Fedin, N. Huseynov, Y. Kulchitsky, A. G. Myagkov, V. Nikolaenko, L. N. Smirnova & V. Tikhomirov
An-Najah National University, Nablus, Palestine
A. Bassalat
Borough of Manhattan Community College, City University of New York, New York, NY, USA
M. C. N. Fiolhais
Bruno Kessler Foundation, Trento, Italy
M. Cristoforetti
Center for High Energy Physics, Peking University, Beijing, China
S. Li
Centro Studi e Ricerche Enrico Fermi, Rome, Italy
I. Gnesi
CERN, Geneva, Switzerland
P. Jenni
Département de Physique Nucléaire et Corpusculaire, Université de Genève, Geneve, Switzerland
M. Nessi
Departament de Fisica de la Universitat Autonoma de Barcelona, Barcelona, Spain
M. P. Casado
Department of Financial and Management Engineering, University of the Aegean, Chios, Greece
I. Gkialas
Department of Physics and Astronomy, Michigan State University, East Lansing, MI, USA
R. Yuan
Department of Physics and Astronomy, University of Louisville, Louisville, KY, USA
D. Biswas
Department of Physics, Ben Gurion University of the Negev, Beer Sheva, Israel
Z. H. Citron
Department of Physics, California State University, East Bay, Long Beach, USA
K. Grimm
Department of Physics, California State University, Sacramento, USA
J. Moss
Department of Physics, King’s College London, London, UK
B. S. Acharya
Department of Physics, University of Fribourg, Fribourg, Switzerland
H. P. Beck
Department of Physics, University of Thessaly, Greece
K. Bachas
Department of Physics, Westmont College, Santa Barbara, USA
B. T. Carlson
Hellenic Open University, Patras, Greece
A. Leisos & A. Tsirigotis
Institucio Catalana de Recerca i Estudis Avancats, ICREA, Barcelona, Spain
S. Grinstein, A. Juste Rozas & M. Martinez
Institut für Experimentalphysik, Universität Hamburg, Hamburg, Germany
K. Tackmann
Institute of Particle Physics (IPP), Montreal, Canada
F. Corriveau, R. A. McPherson, S. H. Robertson, R. Sobie & R. J. Teuscher
Institute of Physics, Azerbaijan Academy of Sciences, Baku, Azerbaijan
F. Ahmadov
Institute of Theoretical Physics, Ilia State University, Tbilisi, Georgia
J. Jejelava
Lawrence Livermore National Laboratory, Livermore, USA
A. Angerami, D. A. Hangal & Q. Hu
III. Physikalisches Institut A, RWTH Aachen University, Aachen, Germany
J. Erdmann
The Collaborative Innovation Center of Quantum Matter (CICQM), Beijing, China
X. Chen
TRIUMF, Vancouver, BC, Canada
G. Azuelos, D. M. Gingrich, F. G. Oakham, P. Savard & M. C. Vetterli
Università di Napoli Parthenope, Naples, Italy
F. Conventi
University of Chinese Academy of Sciences (UCAS), Beijing, China
Y. F. Hu
Department of Physics, University of Colorado Boulder, Colorado, USA
R. Bi, B. Garcia, Y. Go, C. Mc Ginn, J. L. Nagle, J. Ouellette & D. V. Perepelitsa
Washington College, Chestertown, MD, USA
S. Shrestha
Physics Department, Yeditepe University, Istanbul, Türkiye
S. Istin
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Aad, G., Abbott, B., Abbott, D.C. et al. Measurement of exclusive pion pair production in proton–proton collisions at \(\sqrt{s}={7}\,\text {TeV}\) with the ATLAS detector. Eur. Phys. J. C 83, 627 (2023). https://doi.org/10.1140/epjc/s10052-023-11700-x
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DOI: https://doi.org/10.1140/epjc/s10052-023-11700-x
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