Abstract
A measurement of the decorrelation of azimuthal angles between the two jets with the largest transverse momenta is presented for seven regions of leading jet transverse momentum up to 2.2\(\,\mathrm{TeV}\). The analysis is based on the proton-proton collision data collected with the CMS experiment at a centre-of-mass energy of 8\(\,\mathrm{TeV}\) corresponding to an integrated luminosity of 19.7\(\,\text {fb}^{-1}\). The dijet azimuthal decorrelation is caused by the radiation of additional jets and probes the dynamics of multijet production. The results are compared to fixed-order predictions of perturbative quantum chromodynamics (QCD), and to simulations using Monte Carlo event generators that include parton showers, hadronization, and multiparton interactions. Event generators with only two outgoing high transverse momentum partons fail to describe the measurement, even when supplemented with next-to-leading-order QCD corrections and parton showers. Much better agreement is achieved when at least three outgoing partons are complemented through either next-to-leading-order predictions or parton showers. This observation emphasizes the need to improve predictions for multijet production.
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1 Introduction
Hadronic jets with large transverse momenta \({p}_{\mathrm {T}}\) are produced in high-energy proton-proton collisions when two partons interact with high momentum transfer via the strong force. At leading order (LO) in perturbative quantum chromodynamics (pQCD), two final-state partons are produced back-to-back in the transverse plane. For this case, the azimuthal angular separation between the two leading \({p}_{\mathrm {T}}\) jets in the transverse plane, \(\Delta \phi _\text {dijet} =|\phi _\text {jet1}-\phi _\text {jet2} |\), equals \(\pi \). The nonperturbative effects of multiparton interactions or hadronization disturb this correlation only mildly, and \(\Delta \phi _\text {dijet} \approx \pi \) still holds. However, the production of a third high-\({p}_{\mathrm {T}}\) jet leads to a decorrelation in azimuthal angle. The smallest achievable value of \(\Delta \phi _\text {dijet} =2\pi /3\) occurs in a symmetric star-shaped 3-jet configuration. Fixed-order calculations in pQCD for 3-jet production with up to four outgoing partons provide next-to-leading-order (NLO) predictions for the region of \(2\pi /3 \le \Delta \phi _\text {dijet} < \pi \). If more than three jets are produced, the azimuthal angle between the two leading jets can approach zero, although very small angular separations are suppressed because of the finite jet sizes for a particular jet algorithm. The measurement of the dijet azimuthal angular decorrelation is an interesting tool to gain insight into multijet production processes without measuring jets beyond the leading two.
This paper reports the measurement of the normalized dijet differential cross section as a function of the dijet azimuthal angular separation,
for seven regions of the leading jet \({p}_{\mathrm {T}}\), \({p}_{\mathrm {T}} ^{\text {max}}\), within a rapidity region of \(|y |<2.5\). Experimental and theoretical uncertainties are reduced by normalizing the \(\Delta \phi _\text {dijet}\) distribution to the total dijet cross section \(\sigma _\text {dijet}\) within each region of \({p}_{\mathrm {T}} ^{\text {max}}\). For the first time, azimuthal angular separations \(\Delta \phi _\text {dijet}\) over the full phase space from 0 to \(\pi \) are covered. Comparisons are made to fixed-order predictions up to NLO for 3-jet production, and to NLO and LO dijet as well as to tree-level multijet production, each matched with parton showers and complemented with multiparton interactions and hadronization.
The measurement is performed using data collected during 2012 with the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of 19.7\(\,\text {fb}^{-1}\) of proton-proton collisions at \(\sqrt{s}=8\,\mathrm{TeV} \). Previous measurements of dijet azimuthal decorrelation were reported by the D0 Collaboration in \(\mathrm {p}\overline{{\mathrm{p}}} \) collisions at \(\sqrt{s}=1.96\,\mathrm{TeV} \) at the Tevatron [1, 2], and by the CMS and ATLAS Collaborations in \(\mathrm {p}\mathrm {p}\) collisions at \(\sqrt{s}=7\,\mathrm{TeV} \) at the LHC [3, 4].
2 The CMS detector
A detailed description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, can be found in Ref. [5]. The central feature of the CMS detector is a superconducting solenoid, 13 m in length and 6 m in inner diameter, providing an axial magnetic field of 3.8 T. Within the field volume are a silicon pixel and strip tracker, a lead tungstate crystal electromagnetic calorimeter (ECAL) and a brass and scintillator hadron calorimeter (HCAL), each composed of a barrel and two endcap sections. Charged particle trajectories are measured by the tracker with full azimuthal coverage within pseudorapidities \(|\eta |< 2.5\). The ECAL, which is equipped with a preshower detector in the endcaps, and the HCAL cover the region \(|\eta |< 3\). In addition to the barrel and endcap detectors, CMS has extensive forward calorimetry, which extends the coverage up to \(|\eta |< 5\). Finally, muons are measured up to \(|\eta |< 2.4\) by gas-ionization detectors embedded in the steel flux-return yoke outside the solenoid.
3 Event reconstruction and selection
This measurement uses data samples that were collected with single-jet high-level triggers (HLT) [6]. Four such single-jet HLTs were considered that require at least one jet in the event to have \({p}_{\mathrm {T}} > 140\), 200, 260, and \(320 \,\mathrm{GeV} \), respectively. All triggers were prescaled during the 2012 run except the highest-threshold trigger. The integrated luminosity \(\mathcal {L}\) for the four trigger samples is shown in Table 1. The trigger efficiency is estimated using triggers with lower \({p}_{\mathrm {T}}\) thresholds. Using these four jet-energy thresholds gives 100 % trigger efficiencies in the corresponding four momentum regions \(200<{p}_{\mathrm {T}} ^{\text {max}} <300\,\mathrm{GeV} \), \(300<{p}_{\mathrm {T}} ^{\text {max}} <400\,\mathrm{GeV} \), \(400<{p}_{\mathrm {T}} ^{\text {max}} <500\,\mathrm{GeV} \), and \({p}_{\mathrm {T}} ^{\text {max}} >500\,\mathrm{GeV} \).
Particles are reconstructed and identified using a particle-flow (PF) algorithm, which combines the information from the individual subdetectors [7, 8]. The four-vectors of particle candidates, reconstructed by the above technique, are used as input to the jet-clustering algorithm. Jets are reconstructed using the infrared- and collinear-safe anti-\({k}_{\mathrm {T}}\) clustering algorithm with a distance parameter \(R=0.7\) [9]. The clustering is performed with the FastJet package [10] using four-momentum summation.
The reconstructed jets require small additional energy corrections to account for various reconstruction inefficiencies in tracks and clusters in the PF algorithm. These jet energy corrections [11] are derived using (1) simulated events, generated with pythia 6.4.22 [12] with tune Z2* [13, 14] and processed through the CMS detector simulation based on Geant4 [15], and (2) measurements containing dijet, photon+jet, and Z+jet events. The jet energy corrections, which depend on the \(\eta \) and \({p}_{\mathrm {T}}\) of the jet, are applied to the jet four-momentum vectors as multiplicative factors [16]. The overall factor is typically 1.2 or smaller, approximately uniform in \(\eta \), and is 1.05 or smaller for jets having \({p}_{\mathrm {T}} > 100\,\mathrm{GeV} \). An offset correction is applied to take into account the extra energy clustered into jets from additional proton-proton interactions within the same or neighbouring bunch crossings (in-time and out-of-time pileup) [11]. Pileup effects are important only for jets with low \({p}_{\mathrm {T}}\) and become negligible for jets with \({p}_{\mathrm {T}} > 200 \,\mathrm{GeV} \). The current measurement is, therefore, insensitive to pileup effects on jet energy calibration.
Each event is required to have at least one vertex reconstructed offline [17] with a position along the beam line that is within 24 cm of the nominal interaction point. To suppress nonphysical jets, i.e. jets resulting from noise in the ECAL and/or HCAL calorimeters, stringent criteria [18] are applied for identifying jets: each jet should contain at least two particles, one of which is a charged hadron, and the jet energy fraction carried by neutral hadrons and photons should be less than 90 %. The efficiency for identifying physical jets using these criteria is greater than 99 %.
The two leading jets, which define \(\Delta \phi _\text {dijet}\), are selected by considering all jets in the event with \({p}_{\mathrm {T}} > 100 \,\mathrm{GeV} \) and an absolute rapidity \(|y |<5\). Events are selected in which the leading jet \({p}_{\mathrm {T}}\) exceeds 200\(\,\mathrm{GeV}\) and the rapidities \(y_1\) and \(y_2\) of the two leading jets lie within the tracker coverage of \(|y |<2.5\).
To reduce the background from \({\mathrm{t}}\overline{{\mathrm{t}}}\) and heavy vector boson production, the variable \(E_{\mathrm{T}}//\sum {{E}_{\mathrm {T}}} \) is used. The sum of the transverse energies is \(\sum {{E}_{\mathrm {T}}} = \sum _{i}E_{i}\sin \theta _{i}\), and the missing transverse energy \(E_{\mathrm{T}}/ = \sqrt{ \left[ \sum _{i}\left( E_{i}\sin \theta _{i}\cos \phi _{i}\right) \right] ^2 + \left[ \sum _{i}\left( E_{i}\sin \theta _{i}\sin \phi _{i}\right) \right] ^2 }\), where \(\theta \) is the polar angle and the sum runs over all PF candidates in the event. A noticeable fraction of high-\({p}_{\mathrm {T}}\) jet events with large \(E_{\mathrm{T}}/\) emerges from \({\mathrm{t}}\overline{{\mathrm{t}}}\) production with semileptonically decaying b quarks. In addition, Z/W+jet(s) events with Z decays to neutrinos and W decays into charged leptons with neutrinos have high \(E_{\mathrm{T}}/\) values. The distributions of the variable \(E_{\mathrm{T}}//\sum {{E}_{\mathrm {T}}} \) are shown in Fig. 1 for the two regions \(\Delta \phi _\text {dijet} < \pi /2\) (top) and \(\pi /2< \Delta \phi _\text {dijet} < \pi \) (bottom). The data (points) are compared to simulated events (stacked), using MadGraph 5.1.3.30 [19] matched to pythia6 [12] for event generation. Although some deviations of the simulation with respect to the data are visible in Fig. 1 (cf. Ref. [20]), the distributions allow a selection criterion to be optimized with respect to the ratio of signal over background. Events with \(E_{\mathrm{T}}//\sum {{E}_{\mathrm {T}}} >0.1\) are rejected in both regions of \(\Delta \phi _\text {dijet}\) considered in Fig. 1, which corresponds to about 0.7 % of the data sample. Negligible background fractions of \(\approx \)1 % and \(\approx \)0.1 % remain for the two regions \(\Delta \phi _\text {dijet} < \pi /2\) and \(\pi /2< \Delta \phi _\text {dijet} < \pi \), respectively.
4 Measurement of the dijet cross section differential in \(\Delta \phi _\text {dijet}\)
The normalized dijet cross section differential in \(\Delta \phi _\text {dijet}\) (Eq. 1) is corrected for detector smearing effects and unfolded to the level of stable (decay length \(c\tau > 1~\mathrm{cm}\)) final-state particles. In this way, a direct comparison of the measurement with corresponding results from other experiments and with QCD predictions can be made.
The unfolding method is based on the matrix inversion algorithm implemented in the software package RooUnfold [21]. Unfolding uses a response matrix that maps the distribution at particle-level onto the measured one. The response matrix is derived from a simulation that uses the true dijet cross section distribution from pythia6 with tune Z2* [13] as input, and introduces the smearing effects by taking into account the \(\Delta \phi _\text {dijet}\) resolution. As a cross-check, the response matrix was filled from event samples that have been passed through a detector simulation. No significant difference was observed. The unfolded distributions differ from the raw distributions by 3–4 % for \(\Delta \phi _\text {dijet} < \pi /2\) and by less than 3 % for \(\pi /2< \Delta \phi _\text {dijet} < \pi \). A two-dimensional unfolding based on the iterative D’Agostini algorithm [22], which corrects for the smearing effects by taking into account both \(\Delta \phi _\text {dijet}\) and \({p}_{\mathrm {T}}\) resolutions, gives almost identical results.
The main systematic uncertainties arise from the estimation of the jet energy scale (JES) calibration, the jet \({p}_{\mathrm {T}}\) resolution, and the unfolding correction. The JES uncertainty is estimated to be 1.0–2.5 % for PF jets, depending on the jet \({p}_{\mathrm {T}}\) and \(\eta \) [11, 16, 23]. The resulting uncertainties in the normalized \(\Delta \phi _\text {dijet}\) distributions range from 7 % at \(\Delta \phi _\text {dijet} \approx 0\) via 3 % at \(\pi /2\) to 1 % at \(\pi \).
The jet \({p}_{\mathrm {T}}\) resolution is determined from a full detector simulation using events generated by pythia6 with tune Z2*, and is scaled by factors derived from data [11]. The effect of the jet \({p}_{\mathrm {T}}\) resolution uncertainty is estimated by varying it by one standard deviation up and down, and comparing the \(\Delta \phi _\text {dijet}\) distributions before and after the changes. This results in a variation in the normalized \(\Delta \phi _\text {dijet}\) distributions ranging from 5 % at \(\Delta \phi _\text {dijet} \approx 0\) via 3 % at \(\pi /2\) to 0.5 % at \(\pi \).
The uncertainty in the unfolding correction factors is estimated by checking the dependence of the response matrix on the choice of the Monte Carlo (MC) generator. An alternative response matrix is built using the herwig++ 2.5.0 [24] event generator with the default tune of version 2.3. The observed effect is less than 1 %. An additional systematic uncertainty obtained by varying the \(\Delta \phi _\text {dijet}\) resolution by ±10 % to determine the unfolding correction factors is estimated to be of the order of 1 %. This variation of the \(\Delta \phi _\text {dijet}\) resolution by ±10 % is motivated by the observed difference between data and simulation in the \(\Delta \phi _\text {dijet}\) resolution. A total systematic unfolding uncertainty of 1 % accounts for the choice of the MC generator in building the response matrix and the \(\Delta \phi _\text {dijet}\) resolution.
The unfolded dijet cross section differential in \(\Delta \phi _\text {dijet}\) and normalized by the dijet cross section integrated over the entire phase space is shown in Fig. 2 for seven \({p}_{\mathrm {T}} ^{\text {max}}\) regions. Each region is scaled by a multiplicative factor for presentation purposes. The \(\Delta \phi _\text {dijet}\) distributions are strongly peaked at \(\pi \) and become steeper with increasing \({p}_{\mathrm {T}} ^{\text {max}}\). Overlaid on the data for \(\Delta \phi _\text {dijet} > \pi /2\) are predictions from pQCD, presented in more detail in the next section, using parton distribution functions (PDF) of the CT10 PDF set.
5 Comparison to theoretical predictions
5.1 Predictions from fixed-order calculations in pQCD
The theoretical predictions for the normalized dijet cross section differential in \(\Delta \phi _\text {dijet}\) are based on a 3-jet calculation at NLO. The correction of nonperturbative (NP) effects, which account for multiparton interactions (MPI) and hadronization, is studied using event samples simulated with the pythia6 (tune Z2*) and herwig++ (tune 2.3) event generators. Small NP effects are expected, since this measurement deals with a normalized distribution. These corrections are found to be of the order of 1 %, roughly at the limit of the accuracy of the MC simulations. Therefore NP corrections are considered to be negligible and are not applied.
The fixed-order calculations are performed using the NLOJet++ program version 4.1.3 [25, 26] within the framework of the fastNLO package version 2.3.1 [27]. The differential cross section is calculated for 3-jet production at NLO, i.e. up to terms of order \(\alpha _S ^{4}\), with three or four partons in the final state. This calculation has LO precision in the region \(\pi /2 \le \Delta \phi _\text {dijet} < 2\pi /3\) and NLO precision for \(2\pi /3 \le \Delta \phi _\text {dijet} < \pi \). The bin including \(\Delta \phi _\text {dijet} = \pi \) is computed from the NLO dijet cross section within this bin. For each region in \({p}_{\mathrm {T}} ^{\text {max}}\), the differential cross section is normalized to the dijet cross section calculated at LO for \(\pi /2 \le \Delta \phi _\text {dijet} < 2\pi /3\) and at NLO, i.e. up to terms proportional to \(\alpha _S ^{3}\), for \(2\pi /3 \le \Delta \phi _\text {dijet} \le \pi \). The use of the LO dijet cross section for the normalization in the region \(\pi /2 \le \Delta \phi _\text {dijet} < 2\pi /3\) leads to an improved description of the data and avoids artificially increased scale uncertainties as described in Refs. [28, 29]. Of course, this difference in normalization leads to a discontinuity proportional to \(\sigma _\text {dijet}^\text {NLO}/\sigma _\text {dijet}^\text {LO}\) at \(\Delta \phi _\text {dijet} = 2\pi /3\).
The number of quark flavours that are assumed to be massless is set to five, and the renormalization and factorization scales, \(\mu _r\) and \(\mu _f\), are chosen to be equal to \({p}_{\mathrm {T}} ^{\text {max}}\). The PDF sets with NLO evolutions used in the calculations are tabulated in Table 2. The ABM11 PDF set utilizes a fixed flavour number scheme, whereas the rest of the PDF sets use a variable flavour number scheme. The maximum number of flavours is denoted by \(N_f\).
The uncertainties due to the renormalization and factorization scales are evaluated by varying the default choice of \(\mu _r = \mu _f = {p}_{\mathrm {T}} ^{\text {max}} \) between \({p}_{\mathrm {T}} ^{\text {max}}\)/2 and 2\({p}_{\mathrm {T}} ^{\text {max}}\), simultaneously in the differential cross section and in the total cross section, in the following six combinations: \((\mu _r/{p}_{\mathrm {T}} ^{\text {max}}, \mu _f/{p}_{\mathrm {T}} ^{\text {max}}) = (1/2,1/2)\), (1 / 2, 1), (1, 1 / 2), (1, 2), (2, 1), and (2, 2). The PDF uncertainties are evaluated according to the prescriptions for the CT10 PDF set in Ref. [35]. The CT10 PDF set employs the eigenvector method with upward and downward variations for each eigenvector. To evaluate the uncertainty due to the value of the strong coupling constant at 68 % confidence level, \(\alpha _S(M_{{\mathrm{Z}}})\) is varied by ±0.001 as recommended in Ref. [36].
The results of fixed-order calculations with the CT10 PDF set are overlaid on the data for \(\Delta \phi _\text {dijet} > \pi /2\) in Fig. 2. Figure 3 shows the ratio of the normalized dijet cross section differential in \(\Delta \phi _\text {dijet}\) to theory calculated using the CT10 PDF set, together with the combined PDF and \(\alpha _S\) uncertainty (inner band), and the scale uncertainty (outer band). Also shown are the ratios of theory derived with the alternative PDF sets ABM11 (dashed line), HERAPDF1.5 (dashed–three-dotted line), MSTW2008 (dashed-dotted line), and NNPDF2.1 (dotted line) compared to the prediction with the CT10 PDFs.
The fixed-order calculations agree with the data for azimuthal angular separations larger than \(5\pi /6\) except for the highest \({p}_{\mathrm {T}} ^{\text {max}}\) region, where they exceed the data. For smaller \(\Delta \phi _\text {dijet}\) values between \(2\pi /3\) and \(5\pi /6\), in particular where the estimate of the theoretical uncertainties becomes small, systematic discrepancies are exhibited that diminish with increasing \({p}_{\mathrm {T}} ^{\text {max}}\). In the 4-jet LO region with \(\Delta \phi _\text {dijet} < 2\pi /3\), the pattern of increasing deviations towards smaller \(\Delta \phi _\text {dijet}\) and decreasing deviations towards larger \({p}_{\mathrm {T}} ^{\text {max}}\) is repeated, but with less significance because of the larger scale uncertainty. Similar observations were made in the previous CMS measurement [3], which exhibited larger discrepancies in the 4-jet region due to the normalization to the NLO dijet cross section instead of a LO one.
5.2 Predictions from fixed-order calculations matched to parton shower simulations
The pythia6 [12], pythia8 [37], and herwig++ [24] event generators complement LO dijet matrix elements with parton showers to simulate higher-order processes. Both pythia versions, pythia6 with the Z2* tune [13] and pythia8 with the CUETM1 tune [14], employ \({p}_{\mathrm {T}}\)-ordered parton showers [38, 39], while herwig++ with the default tune of version 2.3 uses a coherent-branching algorithm with angular ordering of the showers [40].
The MadGraph program version 5.1.5.7 [19] supplies the results of LO matrix element calculations with two to four outgoing partons that can be matched to the implementations of parton showers, hadronization, and MPI of the event generators. In this analysis, it is interfaced with pythia6 with tune Z2* using the MLM matching procedure [41] to avoid any double counting between tree-level and parton shower generated parton configurations.
The powheg framework [42–44] provides an NLO dijet calculation [45] that can also be matched via the parton showers to event generators. Here, powheg is used with the CT10NLO PDF set and is interfaced to pythia8 with the CUET [14] tune, which employs the LO CTEQ6L1 [35] PDF set. Predictions with parton showers matched to a NLO 3-jet calculation using powheg [46] or MadGraph5_aMC@NLO [47] would be even more relevant for a multijet topology. They could not, however, be included within the timescale of this analysis. Approaching azimuthal angular separations close to \(\pi \), it might also be interesting to compare to predictions employing the technique of \({p}_{\mathrm {T}}\) resummation [48].
In Fig. 4 the normalized dijet cross section differential in \(\Delta \phi _\text {dijet}\) is compared to the predictions from fixed-order calculations supplemented with parton showers, hadronization, and MPI. The error bars on the data points represent the total experimental uncertainty, which is the quadratic sum of the statistical and systematic uncertainties. Figure 5 shows the ratios of these predictions to the normalized dijet cross section differential in \(\Delta \phi _\text {dijet}\), for the seven \({p}_{\mathrm {T}} ^{\text {max}}\) regions. The solid band indicates the total experimental uncertainty and the error bars on the MC points represent the statistical uncertainties in the simulated data.
Among the LO dijet event generators pythia6, pythia8, and herwig++, pythia8 exhibits the smallest deviations from the measurements. pythia6 and herwig++ systematically overshoot the data, particular around \(\Delta \phi _\text {dijet} = 5\pi /6\). The best description of the measurement is given by the tree-level multiparton event generator MadGraph interfaced with pythia6 for showering, hadronization, and MPI. The powheg generator (here used only in the NLO dijet mode) matched to pythia8 shows deviations from the data similar to the LO dijet event generators.
6 Summary
A measurement is presented of the normalized dijet cross section differential in the azimuthal angular separation \(\Delta \phi _\text {dijet}\) of the two jets leading in \({p}_{\mathrm {T}}\) for seven regions in the leading-jet transverse momentum \({p}_{\mathrm {T}} ^{\text {max}}\). The data set of pp collisions at 8\(\,\mathrm{TeV}\) centre-of-mass energy collected in 2012 by the CMS experiment and corresponding to an integrated luminosity of 19.7\(\,\text {fb}^{-1}\) is analysed.
The measured distributions in \(\Delta \phi _\text {dijet}\) are compared to calculations in perturbative QCD for 3-jet production with up to four outgoing partons that provide NLO predictions for the range of \(2\pi /3 \le \Delta \phi _\text {dijet} < \pi \) and LO predictions for \(\pi /2 \le \Delta \phi _\text {dijet} < 2\pi /3\). The NLO predictions describe the data down to values of \(\Delta \phi _\text {dijet} \approx 5\pi /6\), but deviate increasingly when approaching the 4-jet region, starting at \(\Delta \phi _\text {dijet} = 2\pi /3\), particularly at low \({p}_{\mathrm {T}} ^{\text {max}}\). The pattern of increasing deviations towards smaller \(\Delta \phi _\text {dijet}\) and decreasing deviations towards larger \({p}_{\mathrm {T}} ^{\text {max}}\) is repeated in the 4-jet LO region with \(\Delta \phi _\text {dijet} < 2\pi /3\), but with less significance because of the larger scale uncertainty.
In a comparison of the normalized \(\Delta \phi _\text {dijet}\) distributions to the LO dijet event generators pythia6, pythia8, and herwig++, pythia8 gives the best agreement. pythia6 and herwig++ systematically overshoot the data, particularly for \(\Delta \phi _\text {dijet} \approx 5\pi /6\). A good overall description of the measurement is provided by the tree-level multijet event generator MadGraph in combination with pythia6 for showering, hadronization, and multiparton interactions. The dijet NLO calculations from powheg matched to pythia8 exhibit deviations similar to the LO dijet event generators. Improved multijet predictions can be expected from 3-jet NLO calculations matched to parton showers like from powheg or MadGraph5_aMC@NLO.
Similar observations were reported previously by CMS [3] and ATLAS [4], but with less significance because of the smaller data sets. The extension to \(\Delta \phi _\text {dijet}\) values below \(\pi /2\), the improved LO description in the 4-jet region \(\pi /2 \le \Delta \phi _\text {dijet} < 2\pi /3\), and the comparison to dijet NLO calculations matched to parton showers are new results of the present analysis.
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Acknowledgments
We acknowledge discussions and comparisons with P. Sun, C. P. Yuan, and F. Yuan following the approach of [48]. We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their contributions to the success of the CMS effort. In addition, we gratefully acknowledge the computing centres and personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC and the CMS detector provided by the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES and CSF (Croatia); RPF (Cyprus); MoER, ERC IUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); LAS (Lithuania); MOE and UM (Malaysia); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Dubna); MON, RosAtom, RAS and RFBR (Russia); MESTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK and TAEK (Turkey); NASU and SFFR (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and EPLANET (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial Research, India; the HOMING PLUS programme of the Foundation for Polish Science, cofinanced from European Union, Regional Development Fund; the OPUS programme of the National Science Center (Poland); the Compagnia di San Paolo (Torino); MIUR project 20108T4XTM (Italy); the Thalis and Aristeia programmes cofinanced by EU-ESF and the Greek NSRF; the National Priorities Research Program by Qatar National Research Fund; the Rachadapisek Sompot Fund for Postdoctoral Fellowship, Chulalongkorn University (Thailand); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project (Thailand); and the Welch Foundation, contract C-1845.
Author information
Authors and Affiliations
Yerevan Physics Institute, Yerevan, Armenia
V. Khachatryan, A. M. Sirunyan & A. Tumasyan
Institut für Hochenergiephysik der OeAW, Vienna, Austria
W. Adam, E. Asilar, T. Bergauer, J. Brandstetter, E. Brondolin, M. Dragicevic, J. Erö, M. Flechl, M. Friedl, R. Frühwirth, V. M. Ghete, C. Hartl, N. Hörmann, J. Hrubec, M. Jeitler, V. Knünz, A. König, M. Krammer, I. Krätschmer, D. Liko, T. Matsushita, I. Mikulec, D. Rabady, N. Rad, B. Rahbaran, H. Rohringer, J. Schieck, R. Schöfbeck, J. Strauss, W. Treberer-Treberspurg, W. Waltenberger & C.-E. Wulz
National Centre for Particle and High Energy Physics, Minsk, Belarus
V. Mossolov, N. Shumeiko & J. Suarez Gonzalez
Universiteit Antwerpen, Antwerp, Belgium
S. Alderweireldt, T. Cornelis, E. A. De Wolf, X. Janssen, A. Knutsson, J. Lauwers, S. Luyckx, M. Van De Klundert, H. Van Haevermaet, P. Van Mechelen, N. Van Remortel & A. Van Spilbeeck
Vrije Universiteit Brussel, Brussels, Belgium
S. Abu Zeid, F. Blekman, J. D’Hondt, N. Daci, I. De Bruyn, K. Deroover, N. Heracleous, J. Keaveney, S. Lowette, L. Moreels, A. Olbrechts, Q. Python, D. Strom, S. Tavernier, W. Van Doninck, P. Van Mulders, G. P. Van Onsem & I. Van Parijs
Université Libre de Bruxelles, Brussels, Belgium
P. Barria, H. Brun, C. Caillol, B. Clerbaux, G. De Lentdecker, G. Fasanella, L. Favart, R. Goldouzian, A. Grebenyuk, G. Karapostoli, T. Lenzi, A. Léonard, T. Maerschalk, A. Marinov, L. Perniè, A. Randle-conde, T. Seva, C. Vander Velde, P. Vanlaer, R. Yonamine, F. Zenoni & F. Zhang
Ghent University, Ghent, Belgium
K. Beernaert, L. Benucci, A. Cimmino, S. Crucy, D. Dobur, A. Fagot, G. Garcia, M. Gul, J. Mccartin, A. A. Ocampo Rios, D. Poyraz, D. Ryckbosch, S. Salva, M. Sigamani, M. Tytgat, W. Van Driessche, E. Yazgan & N. Zaganidis
Université Catholique de Louvain, Louvain-la-Neuve, Belgium
S. Basegmez, C. Beluffi, O. Bondu, S. Brochet, G. Bruno, A. Caudron, L. Ceard, C. Delaere, D. Favart, L. Forthomme, A. Giammanco, A. Jafari, P. Jez, M. Komm, V. Lemaitre, A. Mertens, M. Musich, C. Nuttens, L. Perrini, K. Piotrzkowski, A. Popov, L. Quertenmont, M. Selvaggi & M. Vidal Marono
Université de Mons, Mons, Belgium
N. Beliy & G. H. Hammad
Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, Brazil
W. L. Aldá Júnior, F. L. Alves, G. A. Alves, L. Brito, M. Correa Martins Junior, M. Hamer, C. Hensel, A. Moraes, M. E. Pol & P. Rebello Teles
Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil
E. Belchior Batista Das Chagas, W. Carvalho, J. Chinellato, A. Custódio, E. M. Da Costa, D. De Jesus Damiao, C. De Oliveira Martins, S. Fonseca De Souza, L. M. Huertas Guativa, H. Malbouisson, D. Matos Figueiredo, C. Mora Herrera, L. Mundim, H. Nogima, W. L. Prado Da Silva, A. Santoro, A. Sznajder, E. J. Tonelli Manganote & A. Vilela Pereira
Universidade Estadual Paulista, Universidade Federal do ABC, São Paulo, Brazil
S. Ahuja, C. A. Bernardes, A. De Souza Santos, S. Dogra, T. R. Fernandez Perez Tomei, E. M. Gregores, P. G. Mercadante, C. S. Moon, S. F. Novaes, Sandra S. Padula, D. Romero Abad & J. C. Ruiz Vargas
Institute for Nuclear Research and Nuclear Energy, Sofia, Bulgaria
A. Aleksandrov, R. Hadjiiska, P. Iaydjiev, M. Rodozov, S. Stoykova, G. Sultanov & M. Vutova
University of Sofia, Sofia, Bulgaria
A. Dimitrov, I. Glushkov, L. Litov, B. Pavlov & P. Petkov
Institute of High Energy Physics, Beijing, China
M. Ahmad, J. G. Bian, G. M. Chen, H. S. Chen, M. Chen, T. Cheng, R. Du, C. H. Jiang, D. Leggat, R. Plestina, F. Romeo, S. M. Shaheen, A. Spiezia, J. Tao, C. Wang, Z. Wang & H. Zhang
State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
C. Asawatangtrakuldee, Y. Ban, Q. Li, S. Liu, Y. Mao, S. J. Qian, D. Wang & Z. Xu
Universidad de Los Andes, Bogotá, Colombia
C. Avila, A. Cabrera, L. F. Chaparro Sierra, C. Florez, J. P. Gomez, B. Gomez Moreno & J. C. Sanabria
Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, Split, Croatia
N. Godinovic, D. Lelas, I. Puljak & P. M. Ribeiro Cipriano
Faculty of Science, University of Split, Split, Croatia
Z. Antunovic & M. Kovac
Institute Rudjer Boskovic, Zagreb, Croatia
V. Brigljevic, K. Kadija, J. Luetic, S. Micanovic & L. Sudic
University of Cyprus, Nicosia, Cyprus
A. Attikis, G. Mavromanolakis, J. Mousa, C. Nicolaou, F. Ptochos, P. A. Razis & H. Rykaczewski
Charles University, Prague, Czech Republic
M. Bodlak, M. Finger & M. Finger Jr.
Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt
E. El-khateeb, T. Elkafrawy, A. Mohamed & E. Salama
National Institute of Chemical Physics and Biophysics, Tallinn, Estonia
B. Calpas, M. Kadastik, M. Murumaa, M. Raidal, A. Tiko & C. Veelken
Department of Physics, University of Helsinki, Helsinki, Finland
P. Eerola, J. Pekkanen & M. Voutilainen
Helsinki Institute of Physics, Helsinki, Finland
J. Härkönen, V. Karimäki, R. Kinnunen, T. Lampén, K. Lassila-Perini, S. Lehti, T. Lindén, P. Luukka, T. Peltola, J. Tuominiemi, E. Tuovinen & L. Wendland
Lappeenranta University of Technology, Lappeenranta, Finland
J. Talvitie & T. Tuuva
DSM/IRFU, CEA/Saclay, Gif-sur-Yvette, France
M. Besancon, F. Couderc, M. Dejardin, D. Denegri, B. Fabbro, J. L. Faure, C. Favaro, F. Ferri, S. Ganjour, A. Givernaud, P. Gras, G. Hamel de Monchenault, P. Jarry, E. Locci, M. Machet, J. Malcles, J. Rander, A. Rosowsky, M. Titov & A. Zghiche
Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France
I. Antropov, S. Baffioni, F. Beaudette, P. Busson, L. Cadamuro, E. Chapon, C. Charlot, O. Davignon, N. Filipovic, R. Granier de Cassagnac, M. Jo, S. Lisniak, L. Mastrolorenzo, P. Miné, I. N. Naranjo, M. Nguyen, C. Ochando, G. Ortona, P. Paganini, P. Pigard, S. Regnard, R. Salerno, J. B. Sauvan, Y. Sirois, T. Strebler, Y. Yilmaz & A. Zabi
Institut Pluridisciplinaire Hubert Curien, Université de Strasbourg, Université de Haute Alsace Mulhouse, CNRS/IN2P3, Strasbourg, France
J.-L. Agram, J. Andrea, A. Aubin, D. Bloch, J.-M. Brom, M. Buttignol, E. C. Chabert, N. Chanon, C. Collard, E. Conte, X. Coubez, J.-C. Fontaine, D. Gelé, U. Goerlach, C. Goetzmann, A.-C. Le Bihan, J. A. Merlin, K. Skovpen & P. Van Hove
Centre de Calcul de l’Institut National de Physique Nucleaire et de Physique des Particules CNRS/IN2P3, Villeurbanne, France
S. Gadrat
Institut de Physique Nucléaire de Lyon, Université de Lyon, Université Claude Bernard Lyon 1, CNRS-IN2P3, Villeurbanne, France
S. Beauceron, C. Bernet, G. Boudoul, E. Bouvier, C. A. Carrillo Montoya, R. Chierici, D. Contardo, B. Courbon, P. Depasse, H. El Mamouni, J. Fan, J. Fay, S. Gascon, M. Gouzevitch, B. Ille, F. Lagarde, I. B. Laktineh, M. Lethuillier, L. Mirabito, A. L. Pequegnot, S. Perries, J. D. Ruiz Alvarez, D. Sabes, L. Sgandurra, V. Sordini, M. Vander Donckt, P. Verdier & S. Viret
Georgian Technical University, Tbilisi, Georgia
T. Toriashvili
Tbilisi State University, Tbilisi, Georgia
I. Bagaturia
RWTH Aachen University, I. Physikalisches Institut, Aachen, Germany
C. Autermann, S. Beranek, L. Feld, A. Heister, M. K. Kiesel, K. Klein, M. Lipinski, A. Ostapchuk, M. Preuten, F. Raupach, S. Schael, J. F. Schulte, T. Verlage, H. Weber & V. Zhukov
RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany
M. Ata, M. Brodski, E. Dietz-Laursonn, D. Duchardt, M. Endres, M. Erdmann, S. Erdweg, T. Esch, R. Fischer, A. Güth, T. Hebbeker, C. Heidemann, K. Hoepfner, S. Knutzen, P. Kreuzer, M. Merschmeyer, A. Meyer, P. Millet, S. Mukherjee, M. Olschewski, K. Padeken, P. Papacz, T. Pook, M. Radziej, H. Reithler, M. Rieger, F. Scheuch, L. Sonnenschein, D. Teyssier & S. Thüer
RWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany
V. Cherepanov, Y. Erdogan, G. Flügge, H. Geenen, M. Geisler, F. Hoehle, B. Kargoll, T. Kress, A. Künsken, J. Lingemann, A. Nehrkorn, A. Nowack, I. M. Nugent, C. Pistone, O. Pooth & A. Stahl
Deutsches Elektronen-Synchrotron, Hamburg, Germany
M. Aldaya Martin, I. Asin, N. Bartosik, O. Behnke, U. Behrens, K. Borras, A. Burgmeier, A. Campbell, C. Contreras-Campana, F. Costanza, C. Diez Pardos, G. Dolinska, S. Dooling, T. Dorland, G. Eckerlin, D. Eckstein, T. Eichhorn, G. Flucke, E. Gallo, J. Garay Garcia, A. Geiser, A. Gizhko, P. Gunnellini, J. Hauk, M. Hempel, H. Jung, A. Kalogeropoulos, O. Karacheban, M. Kasemann, P. Katsas, J. Kieseler, C. Kleinwort, I. Korol, W. Lange, J. Leonard, K. Lipka, A. Lobanov, W. Lohmann, R. Mankel, I.-A. Melzer-Pellmann, A. B. Meyer, G. Mittag, J. Mnich, A. Mussgiller, S. Naumann-Emme, A. Nayak, E. Ntomari, H. Perrey, D. Pitzl, R. Placakyte, A. Raspereza, B. Roland, M. Ö. Sahin, P. Saxena, T. Schoerner-Sadenius, C. Seitz, S. Spannagel, N. Stefaniuk, K. D. Trippkewitz, R. Walsh & C. Wissing
University of Hamburg, Hamburg, Germany
V. Blobel, M. Centis Vignali, A. R. Draeger, J. Erfle, E. Garutti, K. Goebel, D. Gonzalez, M. Görner, J. Haller, M. Hoffmann, R. S. Höing, A. Junkes, R. Klanner, R. Kogler, N. Kovalchuk, T. Lapsien, T. Lenz, I. Marchesini, D. Marconi, M. Meyer, D. Nowatschin, J. Ott, F. Pantaleo, T. Peiffer, A. Perieanu, N. Pietsch, J. Poehlsen, D. Rathjens, C. Sander, C. Scharf, P. Schleper, E. Schlieckau, A. Schmidt, S. Schumann, J. Schwandt, V. Sola, H. Stadie, G. Steinbrück, F. M. Stober, H. Tholen, D. Troendle, E. Usai, L. Vanelderen, A. Vanhoefer & B. Vormwald
Institut für Experimentelle Kernphysik, Karlsruhe, Germany
C. Barth, C. Baus, J. Berger, C. Böser, E. Butz, T. Chwalek, F. Colombo, W. De Boer, A. Descroix, A. Dierlamm, S. Fink, F. Frensch, R. Friese, M. Giffels, A. Gilbert, D. Haitz, F. Hartmann, S. M. Heindl, U. Husemann, I. Katkov, A. Kornmayer, P. Lobelle Pardo, B. Maier, H. Mildner, M. U. Mozer, T. Müller, Th. Müller, M. Plagge, G. Quast, K. Rabbertz, S. Röcker, F. Roscher, M. Schröder, G. Sieber, H. J. Simonis, R. Ulrich, J. Wagner-Kuhr, S. Wayand, M. Weber, T. Weiler, S. Williamson, C. Wöhrmann & R. Wolf
Institute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, Greece
G. Anagnostou, G. Daskalakis, T. Geralis, V. A. Giakoumopoulou, A. Kyriakis, D. Loukas, A. Psallidas & I. Topsis-Giotis
National and Kapodistrian University of Athens, Athens, Greece
A. Agapitos, S. Kesisoglou, A. Panagiotou, N. Saoulidou & E. Tziaferi
University of Ioánnina, Ioannina, Greece
I. Evangelou, G. Flouris, C. Foudas, P. Kokkas, N. Loukas, N. Manthos, I. Papadopoulos, E. Paradas & J. Strologas
Wigner Research Centre for Physics, Budapest, Hungary
G. Bencze, C. Hajdu, A. Hazi, P. Hidas, D. Horvath, F. Sikler, V. Veszpremi, G. Vesztergombi & A. J. Zsigmond
Institute of Nuclear Research ATOMKI, Debrecen, Hungary
N. Beni, S. Czellar, J. Karancsi, J. Molnar & Z. Szillasi
University of Debrecen, Debrecen, Hungary
M. Bartók, A. Makovec, P. Raics, Z. L. Trocsanyi & B. Ujvari
National Institute of Science Education and Research, Bhubaneswar, India
S. Choudhury, P. Mal, K. Mandal, D. K. Sahoo, N. Sahoo & S. K. Swain
Panjab University, Chandigarh, India
S. Bansal, S. B. Beri, V. Bhatnagar, R. Chawla, R. Gupta, U. Bhawandeep, A. K. Kalsi, A. Kaur, M. Kaur, R. Kumar, A. Mehta, M. Mittal, J. B. Singh & G. Walia
University of Delhi, Delhi, India
Ashok Kumar, A. Bhardwaj, B. C. Choudhary, R. B. Garg, S. Malhotra, M. Naimuddin, N. Nishu, K. Ranjan, R. Sharma & V. Sharma
Saha Institute of Nuclear Physics, Kolkata, India
S. Bhattacharya, K. Chatterjee, S. Dey, S. Dutta, N. Majumdar, A. Modak, K. Mondal, S. Mukhopadhyay, A. Roy, D. Roy, S. Roy Chowdhury, S. Sarkar & M. Sharan
Bhabha Atomic Research Centre, Mumbai, India
A. Abdulsalam, R. Chudasama, D. Dutta, V. Jha, V. Kumar, A. K. Mohanty, L. M. Pant, P. Shukla & A. Topkar
Tata Institute of Fundamental Research, Mumbai, India
T. Aziz, S. Banerjee, S. Bhowmik, R. M. Chatterjee, R. K. Dewanjee, S. Dugad, S. Ganguly, S. Ghosh, M. Guchait, A. Gurtu, Sa. Jain, G. Kole, S. Kumar, B. Mahakud, M. Maity, G. Majumder, K. Mazumdar, S. Mitra, G. B. Mohanty, B. Parida, T. Sarkar, N. Sur, B. Sutar & N. Wickramage
Indian Institute of Science Education and Research (IISER), Pune, India
S. Chauhan, S. Dube, A. Kapoor, K. Kothekar & S. Sharma
Institute for Research in Fundamental Sciences (IPM), Tehran, Iran
H. Bakhshiansohi, H. Behnamian, S. M. Etesami, A. Fahim, M. Khakzad, M. Mohammadi Najafabadi, M. Naseri, S. Paktinat Mehdiabadi, F. Rezaei Hosseinabadi, B. Safarzadeh & M. Zeinali
University College Dublin, Dublin, Ireland
M. Felcini & M. Grunewald
INFN Sezione di Bari, Università di Bari, Politecnico di Bari, Bari, Italy
M. Abbrescia, C. Calabria, C. Caputo, A. Colaleo, D. Creanza, L. Cristella, N. De Filippis, M. De Palma, L. Fiore, G. Iaselli, G. Maggi, M. Maggi, G. Miniello, S. My, S. Nuzzo, A. Pompili, G. Pugliese, R. Radogna, A. Ranieri, G. Selvaggi, L. Silvestris & R. Venditti
INFN Sezione di Bologna, Università di Bologna, Bologna, Italy
G. Abbiendi, C. Battilana, D. Bonacorsi, S. Braibant-Giacomelli, L. Brigliadori, R. Campanini, P. Capiluppi, A. Castro, F. R. Cavallo, S. S. Chhibra, G. Codispoti, M. Cuffiani, G. M. Dallavalle, F. Fabbri, A. Fanfani, D. Fasanella, P. Giacomelli, C. Grandi, L. Guiducci, S. Marcellini, G. Masetti, A. Montanari, F. L. Navarria, A. Perrotta, A. M. Rossi, T. Rovelli, G. P. Siroli & N. Tosi
INFN Sezione di Catania, Università di Catania, Catania, Italy
G. Cappello, M. Chiorboli, S. Costa, A. Di Mattia, F. Giordano, R. Potenza, A. Tricomi & C. Tuve
INFN Sezione di Firenze, Università di Firenze, Florence, Italy
G. Barbagli, V. Ciulli, C. Civinini, R. D’Alessandro, E. Focardi, V. Gori, P. Lenzi, M. Meschini, S. Paoletti, G. Sguazzoni & L. Viliani
INFN Laboratori Nazionali di Frascati, Frascati, Italy
L. Benussi, S. Bianco, F. Fabbri, D. Piccolo & F. Primavera
INFN Sezione di Genova, Università di Genova, Genoa, Italy
V. Calvelli, F. Ferro, M. Lo Vetere, M. R. Monge, E. Robutti & S. Tosi
INFN Sezione di Milano-Bicocca, Università di Milano-Bicocca, Milan, Italy
L. Brianza, M. E. Dinardo, S. Fiorendi, S. Gennai, R. Gerosa, A. Ghezzi, P. Govoni, S. Malvezzi, R. A. Manzoni, B. Marzocchi, D. Menasce, L. Moroni, M. Paganoni, D. Pedrini, S. Ragazzi, N. Redaelli & T. Tabarelli de Fatis
INFN Sezione di Napoli, Università di Napoli ‘Federico II’, Napoli, Italy, Università della Basilicata, Potenza, Italy, Università G. Marconi, Rome, Italy
S. Buontempo, N. Cavallo, S. Di Guida, M. Esposito, F. Fabozzi, A. O. M. Iorio, G. Lanza, L. Lista, S. Meola, M. Merola, P. Paolucci, C. Sciacca & F. Thyssen
INFN Sezione di Padova, Università di Padova, Padova, Italy, Università di Trento, Trento, Italy
P. Azzi, N. Bacchetta, L. Benato, D. Bisello, A. Boletti, A. Branca, R. Carlin, P. Checchia, M. Dall’Osso, T. Dorigo, U. Dosselli, F. Gasparini, U. Gasparini, A. Gozzelino, K. Kanishchev, S. Lacaprara, M. Margoni, A. T. Meneguzzo, M. Passaseo, J. Pazzini, M. Pegoraro, N. Pozzobon, P. Ronchese, F. Simonetto, E. Torassa, M. Tosi, M. Zanetti, P. Zotto & A. Zucchetta
INFN Sezione di Pavia, Università di Pavia, Pavia, Italy
A. Braghieri, A. Magnani, P. Montagna, S. P. Ratti, V. Re, C. Riccardi, P. Salvini, I. Vai & P. Vitulo
INFN Sezione di Perugia, Università di Perugia, Perugia, Italy
L. Alunni Solestizi, G. M. Bilei, D. Ciangottini, L. Fanò, P. Lariccia, G. Mantovani, M. Menichelli, A. Saha & A. Santocchia
INFN Sezione di Pisa, Università di Pisa, Scuola Normale Superiore di Pisa, Pisa, Italy
K. Androsov, P. Azzurri, G. Bagliesi, J. Bernardini, T. Boccali, R. Castaldi, M. A. Ciocci, R. Dell’Orso, S. Donato, G. Fedi, L. Foà, A. Giassi, M. T. Grippo, F. Ligabue, T. Lomtadze, L. Martini, A. Messineo, F. Palla, A. Rizzi, A. Savoy-Navarro, A. T. Serban, P. Spagnolo, R. Tenchini, G. Tonelli, A. Venturi & P. G. Verdini
INFN Sezione di Roma, Università di Roma, Rome, Italy
L. Barone, F. Cavallari, G. D’imperio, D. Del Re, M. Diemoz, S. Gelli, C. Jorda, E. Longo, F. Margaroli, P. Meridiani, G. Organtini, R. Paramatti, F. Preiato, S. Rahatlou, C. Rovelli, F. Santanastasio & P. Traczyk
INFN Sezione di Torino, Università di Torino, Torino, Italy, Università del Piemonte Orientale, Novara, Italy
N. Amapane, R. Arcidiacono, S. Argiro, M. Arneodo, R. Bellan, C. Biino, N. Cartiglia, M. Costa, R. Covarelli, A. Degano, N. Demaria, L. Finco, B. Kiani, C. Mariotti, S. Maselli, E. Migliore, V. Monaco, E. Monteil, M. M. Obertino, L. Pacher, N. Pastrone, M. Pelliccioni, G. L. Pinna Angioni, F. Ravera, A. Romero, M. Ruspa, R. Sacchi, A. Solano & A. Staiano
INFN Sezione di Trieste, Università di Trieste, Trieste, Italy
S. Belforte, V. Candelise, M. Casarsa, F. Cossutti, G. Della Ricca, B. Gobbo, C. La Licata, M. Marone, A. Schizzi & A. Zanetti
Kangwon National University, Chunchon, Korea
A. Kropivnitskaya & S. K. Nam
Kyungpook National University, Daegu, Korea
D. H. Kim, G. N. Kim, M. S. Kim, D. J. Kong, S. Lee, Y. D. Oh, A. Sakharov & D. C. Son
Chonbuk National University, Jeonju, Korea
J. A. Brochero Cifuentes, H. Kim & T. J. Kim
Chonnam National University, Institute for Universe and Elementary Particles, Kwangju, Korea
S. Song
Korea University, Seoul, Korea
S. Cho, S. Choi, Y. Go, D. Gyun, B. Hong, H. Kim, Y. Kim, B. Lee, K. Lee, K. S. Lee, S. Lee, J. Lim, S. K. Park & Y. Roh
Seoul National University, Seoul, Korea
H. D. Yoo
University of Seoul, Seoul, Korea
M. Choi, H. Kim, J. H. Kim, J. S. H. Lee, I. C. Park, G. Ryu & M. S. Ryu
Sungkyunkwan University, Suwon, Korea
Y. Choi, J. Goh, D. Kim, E. Kwon, J. Lee & I. Yu
Vilnius University, Vilnius, Lithuania
V. Dudenas, A. Juodagalvis & J. Vaitkus
National Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia
I. Ahmed, Z. A. Ibrahim, J. R. Komaragiri, M. A. B. Md Ali, F. Mohamad Idris, W. A. T. Wan Abdullah, M. N. Yusli & Z. Zolkapli
Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico
E. Casimiro Linares, H. Castilla-Valdez, E. De La Cruz-Burelo, I. Heredia-De La Cruz, A. Hernandez-Almada, R. Lopez-Fernandez & A. Sanchez-Hernandez
Universidad Iberoamericana, Mexico City, Mexico
S. Carrillo Moreno & F. Vazquez Valencia
Benemerita Universidad Autonoma de Puebla, Puebla, Mexico
I. Pedraza & H. A. Salazar Ibarguen
Universidad Autónoma de San Luis Potosí, San Luis Potosí, Mexico
A. Morelos Pineda
University of Auckland, Auckland, New Zealand
D. Krofcheck
University of Canterbury, Christchurch, New Zealand
P. H. Butler
National Centre for Physics, Quaid-I-Azam University, Islamabad, Pakistan
A. Ahmad, M. Ahmad, Q. Hassan, H. R. Hoorani, W. A. Khan, T. Khurshid & M. Shoaib
National Centre for Nuclear Research, Swierk, Poland
H. Bialkowska, M. Bluj, B. Boimska, T. Frueboes, M. Górski, M. Kazana, K. Nawrocki, K. Romanowska-Rybinska, M. Szleper & P. Zalewski
Institute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, Poland
G. Brona, K. Bunkowski, A. Byszuk, K. Doroba, A. Kalinowski, M. Konecki, J. Krolikowski, M. Misiura, M. Olszewski & M. Walczak
Laboratório de Instrumentação e Física Experimental de Partículas, Lisboa, Portugal
P. Bargassa, C. Beirão Da Cruz Silva, A. Di Francesco, P. Faccioli, P. G. Ferreira Parracho, M. Gallinaro, J. Hollar, N. Leonardo, L. Lloret Iglesias, F. Nguyen, J. Rodrigues Antunes, J. Seixas, O. Toldaiev, D. Vadruccio, J. Varela & P. Vischia
Joint Institute for Nuclear Research, Dubna, Russia
S. Afanasiev, P. Bunin, M. Gavrilenko, I. Golutvin, I. Gorbunov, A. Kamenev, V. Karjavin, A. Lanev, A. Malakhov, V. Matveev, P. Moisenz, V. Palichik, V. Perelygin, S. Shmatov, S. Shulha, N. Skatchkov, V. Smirnov & A. Zarubin
Petersburg Nuclear Physics Institute, Gatchina, St. Petersburg, Russia
V. Golovtsov, Y. Ivanov, V. Kim, E. Kuznetsova, P. Levchenko, V. Murzin, V. Oreshkin, I. Smirnov, V. Sulimov, L. Uvarov, S. Vavilov & A. Vorobyev
Institute for Nuclear Research, Moscow, Russia
Yu. Andreev, A. Dermenev, S. Gninenko, N. Golubev, A. Karneyeu, M. Kirsanov, N. Krasnikov, A. Pashenkov, D. Tlisov & A. Toropin
Institute for Theoretical and Experimental Physics, Moscow, Russia
V. Epshteyn, V. Gavrilov, N. Lychkovskaya, V. Popov, I. Pozdnyakov, G. Safronov, A. Spiridonov, E. Vlasov & A. Zhokin
National Research Nuclear University ‘Moscow Engineering Physics Institute’ (MEPhI), Moscow, Russia
A. Bylinkin, M. Chadeeva, R. Chistov, M. Danilov & V. Rusinov
P.N. Lebedev Physical Institute, Moscow, Russia
V. Andreev, M. Azarkin, I. Dremin, M. Kirakosyan, A. Leonidov, G. Mesyats & S. V. Rusakov
Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow, Russia
A. Baskakov, A. Belyaev, E. Boos, M. Dubinin, L. Dudko, A. Ershov, A. Gribushin, V. Klyukhin, O. Kodolova, I. Lokhtin, I. Miagkov, S. Obraztsov, S. Petrushanko, V. Savrin & A. Snigirev
State Research Center of Russian Federation, Institute for High Energy Physics, Protvino, Russia
I. Azhgirey, I. Bayshev, S. Bitioukov, V. Kachanov, A. Kalinin, D. Konstantinov, V. Krychkine, V. Petrov, R. Ryutin, A. Sobol, L. Tourtchanovitch, S. Troshin, N. Tyurin, A. Uzunian & A. Volkov
Faculty of Physics and Vinca Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia
P. Adzic, P. Cirkovic, J. Milosevic & V. Rekovic
Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
J. Alcaraz Maestre, E. Calvo, M. Cerrada, M. Chamizo Llatas, N. Colino, B. De La Cruz, A. Delgado Peris, A. Escalante Del Valle, C. Fernandez Bedoya, J. P. Fernández Ramos, J. Flix, M. C. Fouz, P. Garcia-Abia, O. Gonzalez Lopez, S. Goy Lopez, J. M. Hernandez, M. I. Josa, E. Navarro De Martino, A. Pérez-Calero Yzquierdo, J. Puerta Pelayo, A. Quintario Olmeda, I. Redondo, L. Romero, J. Santaolalla & M. S. Soares
Universidad Autónoma de Madrid, Madrid, Spain
C. Albajar, J. F. de Trocóniz, M. Missiroli & D. Moran
Universidad de Oviedo, Oviedo, Spain
J. Cuevas, J. Fernandez Menendez, S. Folgueras, I. Gonzalez Caballero, E. Palencia Cortezon & J. M. Vizan Garcia
Instituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, Spain
I. J. Cabrillo, A. Calderon, J. R. Castiñeiras De Saa, P. De Castro Manzano, M. Fernandez, J. Garcia-Ferrero, G. Gomez, A. Lopez Virto, J. Marco, R. Marco, C. Martinez Rivero, F. Matorras, J. Piedra Gomez, T. Rodrigo, A. Y. Rodríguez-Marrero, A. Ruiz-Jimeno, L. Scodellaro, N. Trevisani, I. Vila & R. Vilar Cortabitarte
CERN, European Organization for Nuclear Research, Geneva, Switzerland
D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A. H. Ball, D. Barney, A. Benaglia, J. Bendavid, L. Benhabib, G. M. Berruti, P. Bloch, A. Bocci, A. Bonato, C. Botta, H. Breuker, T. Camporesi, R. Castello, G. Cerminara, M. D’Alfonso, D. d’Enterria, A. Dabrowski, V. Daponte, A. David, M. De Gruttola, F. De Guio, A. De Roeck, S. De Visscher, E. Di Marco, M. Dobson, M. Dordevic, B. Dorney, T. du Pree, D. Duggan, M. Dünser, N. Dupont, A. Elliott-Peisert, G. Franzoni, J. Fulcher, W. Funk, D. Gigi, K. Gill, D. Giordano, M. Girone, F. Glege, R. Guida, S. Gundacker, M. Guthoff, J. Hammer, P. Harris, J. Hegeman, V. Innocente, P. Janot, H. Kirschenmann, M. J. Kortelainen, K. Kousouris, K. Krajczar, P. Lecoq, C. Lourenço, M. T. Lucchini, N. Magini, L. Malgeri, M. Mannelli, A. Martelli, L. Masetti, F. Meijers, S. Mersi, E. Meschi, F. Moortgat, S. Morovic, M. Mulders, M. V. Nemallapudi, H. Neugebauer, S. Orfanelli, L. Orsini, L. Pape, E. Perez, M. Peruzzi, A. Petrilli, G. Petrucciani, A. Pfeiffer, M. Pierini, D. Piparo, A. Racz, T. Reis, G. Rolandi, M. Rovere, M. Ruan, H. Sakulin, C. Schäfer, C. Schwick, M. Seidel, A. Sharma, P. Silva, M. Simon, P. Sphicas, J. Steggemann, B. Stieger, M. Stoye, Y. Takahashi, D. Treille, A. Triossi, A. Tsirou, G. I. Veres, N. Wardle, H. K. Wöhri, A. Zagozdzinska & W. D. Zeuner
Paul Scherrer Institut, Villigen, Switzerland
W. Bertl, K. Deiters, W. Erdmann, R. Horisberger, Q. Ingram, H. C. Kaestli, D. Kotlinski, U. Langenegger & T. Rohe
Institute for Particle Physics ETH Zurich, Zurich, Switzerland
F. Bachmair, L. Bäni, L. Bianchini, B. Casal, G. Dissertori, M. Dittmar, M. Donegà, P. Eller, C. Grab, C. Heidegger, D. Hits, J. Hoss, G. Kasieczka, P. Lecomte, W. Lustermann, B. Mangano, M. Marionneau, P. Martinez Ruiz del Arbol, M. Masciovecchio, M. T. Meinhard, D. Meister, F. Micheli, P. Musella, F. Nessi-Tedaldi, F. Pandolfi, J. Pata, F. Pauss, L. Perrozzi, M. Quittnat, M. Rossini, M. Schönenberger, A. Starodumov, M. Takahashi, V. R. Tavolaro, K. Theofilatos & R. Wallny
Universität Zürich, Zurich, Switzerland
T. K. Aarrestad, C. Amsler, L. Caminada, M. F. Canelli, V. Chiochia, A. De Cosa, C. Galloni, A. Hinzmann, T. Hreus, B. Kilminster, C. Lange, J. Ngadiuba, D. Pinna, G. Rauco, P. Robmann, D. Salerno & Y. Yang
National Central University, Chung-Li, Taiwan
M. Cardaci, K. H. Chen, T. H. Doan, Sh. Jain, R. Khurana, M. Konyushikhin, C. M. Kuo, W. Lin, Y. J. Lu, A. Pozdnyakov & S. S. Yu
National Taiwan University (NTU), Taipei, Taiwan
Arun Kumar, P. Chang, Y. H. Chang, Y. W. Chang, Y. Chao, K. F. Chen, P. H. Chen, C. Dietz, F. Fiori, U. Grundler, W.-S. Hou, Y. Hsiung, Y. F. Liu, R.-S. Lu, M. Miñano Moya, E. Petrakou, J. f. Tsai & Y. M. Tzeng
Faculty of Science, Department of Physics, Chulalongkorn University, Bangkok, Thailand
B. Asavapibhop, K. Kovitanggoon, G. Singh, N. Srimanobhas & N. Suwonjandee
Cukurova University, Adana, Turkey
A. Adiguzel, S. Cerci, S. Damarseckin, Z. S. Demiroglu, C. Dozen, I. Dumanoglu, E. Eskut, F. H. Gecit, S. Girgis, G. Gokbulut, Y. Guler, E. Gurpinar, I. Hos, E. E. Kangal, A. Kayis Topaksu, G. Onengut, M. Ozcan, K. Ozdemir, S. Ozturk, A. Polatoz & C. Zorbilmez
Physics Department, Middle East Technical University, Ankara, Turkey
B. Bilin, S. Bilmis, B. Isildak, G. Karapinar, M. Yalvac & M. Zeyrek
Bogazici University, Istanbul, Turkey
E. Gülmez, M. Kaya, O. Kaya, E. A. Yetkin & T. Yetkin
Istanbul Technical University, Istanbul, Turkey
A. Cakir, K. Cankocak, S. Sen & F. I. Vardarlı
Institute for Scintillation Materials of National Academy of Science of Ukraine, Kharkov, Ukraine
B. Grynyov
National Scientific Center, Kharkov Institute of Physics and Technology, Kharkov, Ukraine
L. Levchuk & P. Sorokin
University of Bristol, Bristol, UK
R. Aggleton, F. Ball, L. Beck, J. J. Brooke, E. Clement, D. Cussans, H. Flacher, J. Goldstein, M. Grimes, G. P. Heath, H. F. Heath, J. Jacob, L. Kreczko, C. Lucas, Z. Meng, D. M. Newbold, S. Paramesvaran, A. Poll, T. Sakuma, S. Seif El Nasr-storey, S. Senkin, D. Smith & V. J. Smith
Rutherford Appleton Laboratory, Didcot, UK
K. W. Bell, A. Belyaev, C. Brew, R. M. Brown, L. Calligaris, D. Cieri, D. J. A. Cockerill, J. A. Coughlan, K. Harder, S. Harper, E. Olaiya, D. Petyt, C. H. Shepherd-Themistocleous, A. Thea, I. R. Tomalin, T. Williams & S. D. Worm
Imperial College, London, UK
M. Baber, R. Bainbridge, O. Buchmuller, A. Bundock, D. Burton, S. Casasso, M. Citron, D. Colling, L. Corpe, P. Dauncey, G. Davies, A. De Wit, M. Della Negra, P. Dunne, A. Elwood, D. Futyan, G. Hall, G. Iles, R. Lane, R. Lucas, L. Lyons, A.-M. Magnan, S. Malik, J. Nash, A. Nikitenko, J. Pela, M. Pesaresi, D. M. Raymond, A. Richards, A. Rose, C. Seez, A. Tapper, K. Uchida, M. Vazquez Acosta, T. Virdee & S. C. Zenz
Brunel University, Uxbridge, UK
J. E. Cole, P. R. Hobson, A. Khan, P. Kyberd, D. Leslie, I. D. Reid, P. Symonds, L. Teodorescu & M. Turner
Baylor University, Waco, USA
A. Borzou, K. Call, J. Dittmann, K. Hatakeyama, H. Liu & N. Pastika
The University of Alabama, Tuscaloosa, USA
O. Charaf, S. I. Cooper, C. Henderson & P. Rumerio
Boston University, Boston, USA
D. Arcaro, A. Avetisyan, T. Bose, D. Gastler, D. Rankin, C. Richardson, J. Rohlf, L. Sulak & D. Zou
Brown University, Providence, USA
J. Alimena, E. Berry, D. Cutts, A. Ferapontov, A. Garabedian, J. Hakala, U. Heintz, O. Jesus, E. Laird, G. Landsberg, Z. Mao, M. Narain, S. Piperov, S. Sagir & R. Syarif
University of California, Davis, Davis, USA
R. Breedon, G. Breto, M. Calderon De La Barca Sanchez, S. Chauhan, M. Chertok, J. Conway, R. Conway, P. T. Cox, R. Erbacher, G. Funk, M. Gardner, W. Ko, R. Lander, C. Mclean, M. Mulhearn, D. Pellett, J. Pilot, F. Ricci-Tam, S. Shalhout, J. Smith, M. Squires, D. Stolp, M. Tripathi, S. Wilbur & R. Yohay
University of California, Los Angeles, USA
R. Cousins, P. Everaerts, A. Florent, J. Hauser, M. Ignatenko, D. Saltzberg, E. Takasugi, V. Valuev & M. Weber
University of California, Riverside, Riverside, USA
K. Burt, R. Clare, J. Ellison, J. W. Gary, G. Hanson, J. Heilman, M. Ivova Paneva, P. Jandir, E. Kennedy, F. Lacroix, O. R. Long, M. Malberti, M. Olmedo Negrete, A. Shrinivas, H. Wei, S. Wimpenny & B. R. Yates
University of California, San Diego, La Jolla, USA
J. G. Branson, G. B. Cerati, S. Cittolin, R. T. D’Agnolo, M. Derdzinski, A. Holzner, R. Kelley, D. Klein, J. Letts, I. Macneill, D. Olivito, S. Padhi, M. Pieri, M. Sani, V. Sharma, S. Simon, M. Tadel, A. Vartak, S. Wasserbaech, C. Welke, F. Würthwein, A. Yagil & G. Zevi Della Porta
University of California, Santa Barbara, Santa Barbara, USA
J. Bradmiller-Feld, C. Campagnari, A. Dishaw, V. Dutta, K. Flowers, M. Franco Sevilla, P. Geffert, C. George, F. Golf, L. Gouskos, J. Gran, J. Incandela, N. Mccoll, S. D. Mullin, J. Richman, D. Stuart, I. Suarez, C. West & J. Yoo
California Institute of Technology, Pasadena, USA
D. Anderson, A. Apresyan, A. Bornheim, J. Bunn, Y. Chen, J. Duarte, A. Mott, H. B. Newman, C. Pena, M. Spiropulu, J. R. Vlimant, S. Xie & R. Y. Zhu
Carnegie Mellon University, Pittsburgh, USA
M. B. Andrews, V. Azzolini, A. Calamba, B. Carlson, T. Ferguson, M. Paulini, J. Russ, M. Sun, H. Vogel & I. Vorobiev
University of Colorado Boulder, Boulder, USA
J. P. Cumalat, W. T. Ford, A. Gaz, F. Jensen, A. Johnson, M. Krohn, T. Mulholland, U. Nauenberg, K. Stenson & S. R. Wagner
Cornell University, Ithaca, USA
J. Alexander, A. Chatterjee, J. Chaves, J. Chu, S. Dittmer, N. Eggert, N. Mirman, G. Nicolas Kaufman, J. R. Patterson, A. Rinkevicius, A. Ryd, L. Skinnari, L. Soffi, W. Sun, S. M. Tan, W. D. Teo, J. Thom, J. Thompson, J. Tucker, Y. Weng & P. Wittich
Fermi National Accelerator Laboratory, Batavia, USA
S. Abdullin, M. Albrow, G. Apollinari, S. Banerjee, L. A. T. Bauerdick, A. Beretvas, J. Berryhill, P. C. Bhat, G. Bolla, K. Burkett, J. N. Butler, H. W. K. Cheung, F. Chlebana, S. Cihangir, V. D. Elvira, I. Fisk, J. Freeman, E. Gottschalk, L. Gray, D. Green, S. Grünendahl, O. Gutsche, J. Hanlon, D. Hare, R. M. Harris, S. Hasegawa, J. Hirschauer, Z. Hu, B. Jayatilaka, S. Jindariani, M. Johnson, U. Joshi, B. Klima, B. Kreis, S. Lammel, J. Linacre, D. Lincoln, R. Lipton, T. Liu, R. Lopes De Sá, J. Lykken, K. Maeshima, J. M. Marraffino, S. Maruyama, D. Mason, P. McBride, P. Merkel, S. Mrenna, S. Nahn, C. Newman-Holmes, V. O’Dell, K. Pedro, O. Prokofyev, G. Rakness, E. Sexton-Kennedy, A. Soha, W. J. Spalding, L. Spiegel, S. Stoynev, N. Strobbe, L. Taylor, S. Tkaczyk, N. V. Tran, L. Uplegger, E. W. Vaandering, C. Vernieri, M. Verzocchi, R. Vidal, M. Wang, H. A. Weber & A. Whitbeck
University of Florida, Gainesville, USA
D. Acosta, P. Avery, P. Bortignon, D. Bourilkov, A. Brinkerhoff, A. Carnes, M. Carver, D. Curry, S. Das, R. D. Field, I. K. Furic, S. V. Gleyzer, J. Konigsberg, A. Korytov, K. Kotov, P. Ma, K. Matchev, H. Mei, P. Milenovic, G. Mitselmakher, D. Rank, R. Rossin, L. Shchutska, M. Snowball, D. Sperka, N. Terentyev, L. Thomas, J. Wang, S. Wang & J. Yelton
Florida International University, Miami, USA
S. Hewamanage, S. Linn, P. Markowitz, G. Martinez & J. L. Rodriguez
Florida State University, Tallahassee, USA
A. Ackert, J. R. Adams, T. Adams, A. Askew, S. Bein, J. Bochenek, B. Diamond, J. Haas, S. Hagopian, V. Hagopian, K. F. Johnson, A. Khatiwada, H. Prosper & M. Weinberg
Florida Institute of Technology, Melbourne, USA
M. M. Baarmand, V. Bhopatkar, S. Colafranceschi, M. Hohlmann, H. Kalakhety, D. Noonan, T. Roy & F. Yumiceva
University of Illinois at Chicago (UIC), Chicago, USA
M. R. Adams, L. Apanasevich, D. Berry, R. R. Betts, I. Bucinskaite, R. Cavanaugh, O. Evdokimov, L. Gauthier, C. E. Gerber, D. J. Hofman, P. Kurt, C. O’Brien, I. D. Sandoval Gonzalez, P. Turner, N. Varelas, Z. Wu, M. Zakaria & J. Zhang
The University of Iowa, Iowa City, USA
B. Bilki, W. Clarida, K. Dilsiz, S. Durgut, R. P. Gandrajula, M. Haytmyradov, V. Khristenko, J.-P. Merlo, H. Mermerkaya, A. Mestvirishvili, A. Moeller, J. Nachtman, H. Ogul, Y. Onel, F. Ozok, A. Penzo, C. Snyder, E. Tiras, J. Wetzel & K. Yi
Johns Hopkins University, Baltimore, USA
I. Anderson, B. A. Barnett, B. Blumenfeld, N. Eminizer, D. Fehling, L. Feng, A. V. Gritsan, P. Maksimovic, M. Osherson, J. Roskes, A. Sady, U. Sarica, M. Swartz, M. Xiao, Y. Xin & C. You
The University of Kansas, Lawrence, USA
P. Baringer, A. Bean, G. Benelli, C. Bruner, R. P. Kenny III, D. Majumder, M. Malek, W. Mcbrayer, M. Murray, S. Sanders, R. Stringer & Q. Wang
Kansas State University, Manhattan, USA
A. Ivanov, K. Kaadze, S. Khalil, M. Makouski, Y. Maravin, A. Mohammadi, L. K. Saini, N. Skhirtladze & S. Toda
Lawrence Livermore National Laboratory, Livermore, USA
D. Lange, F. Rebassoo & D. Wright
University of Maryland, College Park, USA
C. Anelli, A. Baden, O. Baron, A. Belloni, B. Calvert, S. C. Eno, C. Ferraioli, J. A. Gomez, N. J. Hadley, S. Jabeen, R. G. Kellogg, T. Kolberg, J. Kunkle, Y. Lu, A. C. Mignerey, Y. H. Shin, A. Skuja, M. B. Tonjes & S. C. Tonwar
Massachusetts Institute of Technology, Cambridge, USA
A. Apyan, R. Barbieri, A. Baty, K. Bierwagen, S. Brandt, W. Busza, I. A. Cali, Z. Demiragli, L. Di Matteo, G. Gomez Ceballos, M. Goncharov, D. Gulhan, Y. Iiyama, G. M. Innocenti, M. Klute, D. Kovalskyi, Y. S. Lai, Y.-J. Lee, A. Levin, P. D. Luckey, A. C. Marini, C. Mcginn, C. Mironov, S. Narayanan, X. Niu, C. Paus, C. Roland, G. Roland, J. Salfeld-Nebgen, G. S. F. Stephans, K. Sumorok, M. Varma, D. Velicanu, J. Veverka, J. Wang, T. W. Wang, B. Wyslouch, M. Yang & V. Zhukova
University of Minnesota, Minneapolis, USA
A. C. Benvenuti, B. Dahmes, A. Evans, A. Finkel, A. Gude, P. Hansen, S. Kalafut, S. C. Kao, K. Klapoetke, Y. Kubota, Z. Lesko, J. Mans, S. Nourbakhsh, N. Ruckstuhl, R. Rusack, N. Tambe & J. Turkewitz
University of Mississippi, Oxford, USA
J. G. Acosta & S. Oliveros
University of Nebraska-Lincoln, Lincoln, USA
E. Avdeeva, R. Bartek, K. Bloom, S. Bose, D. R. Claes, A. Dominguez, C. Fangmeier, R. Gonzalez Suarez, R. Kamalieddin, D. Knowlton, I. Kravchenko, F. Meier, J. Monroy, F. Ratnikov, J. E. Siado & G. R. Snow
State University of New York at Buffalo, Buffalo, USA
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Northeastern University, Boston, USA
G. Alverson, E. Barberis, D. Baumgartel, M. Chasco, A. Hortiangtham, A. Massironi, D. M. Morse, D. Nash, T. Orimoto, R. Teixeira De Lima, D. Trocino, R.-J. Wang, D. Wood & J. Zhang
Northwestern University, Evanston, USA
S. Bhattacharya, K. A. Hahn, A. Kubik, J. F. Low, N. Mucia, N. Odell, B. Pollack, M. Schmitt, K. Sung, M. Trovato & M. Velasco
University of Notre Dame, Notre Dame, USA
N. Dev, M. Hildreth, C. Jessop, D. J. Karmgard, N. Kellams, K. Lannon, N. Marinelli, F. Meng, C. Mueller, Y. Musienko, M. Planer, A. Reinsvold, R. Ruchti, G. Smith, S. Taroni, N. Valls, M. Wayne, M. Wolf & A. Woodard
The Ohio State University, Columbus, USA
L. Antonelli, J. Brinson, B. Bylsma, L. S. Durkin, S. Flowers, A. Hart, C. Hill, R. Hughes, W. Ji, T. Y. Ling, B. Liu, W. Luo, D. Puigh, M. Rodenburg, B. L. Winer & H. W. Wulsin
Princeton University, Princeton, USA
O. Driga, P. Elmer, J. Hardenbrook, P. Hebda, S. A. Koay, P. Lujan, D. Marlow, T. Medvedeva, M. Mooney, J. Olsen, C. Palmer, P. Piroué, D. Stickland, C. Tully & A. Zuranski
University of Puerto Rico, Mayagüez, USA
S. Malik
Purdue University, West Lafayette, USA
A. Barker, V. E. Barnes, D. Benedetti, D. Bortoletto, L. Gutay, M. K. Jha, M. Jones, A. W. Jung, K. Jung, A. Kumar, D. H. Miller, N. Neumeister, B. C. Radburn-Smith, X. Shi, I. Shipsey, D. Silvers, J. Sun, A. Svyatkovskiy, F. Wang, W. Xie & L. Xu
Purdue University Calumet, Hammond, USA
N. Parashar & J. Stupak
Rice University, Houston, USA
A. Adair, B. Akgun, Z. Chen, K. M. Ecklund, F. J. M. Geurts, M. Guilbaud, W. Li, B. Michlin, M. Northup, B. P. Padley, R. Redjimi, J. Roberts, J. Rorie, Z. Tu & J. Zabel
University of Rochester, Rochester, USA
B. Betchart, A. Bodek, P. de Barbaro, R. Demina, Y. Eshaq, T. Ferbel, M. Galanti, A. Garcia-Bellido, J. Han, A. Harel, O. Hindrichs, A. Khukhunaishvili, K. H. Lo, G. Petrillo, P. Tan & M. Verzetti
Rutgers, The State University of New Jersey, Piscataway, USA
J. P. Chou, E. Contreras-Campana, D. Ferencek, Y. Gershtein, E. Halkiadakis, M. Heindl, D. Hidas, E. Hughes, S. Kaplan, R. Kunnawalkam Elayavalli, A. Lath, K. Nash, H. Saka, S. Salur, S. Schnetzer, D. Sheffield, S. Somalwar, R. Stone, S. Thomas, P. Thomassen & M. Walker
University of Tennessee, Knoxville, USA
M. Foerster, G. Riley, K. Rose, S. Spanier & K. Thapa
Texas A&M University, College Station, USA
O. Bouhali, A. Castaneda Hernandez, A. Celik, M. Dalchenko, M. De Mattia, A. Delgado, S. Dildick, R. Eusebi, J. Gilmore, T. Huang, T. Kamon, V. Krutelyov, R. Mueller, I. Osipenkov, Y. Pakhotin, R. Patel, A. Perloff, A. Rose, A. Safonov, A. Tatarinov & K. A. Ulmer
Texas Tech University, Lubbock, USA
N. Akchurin, C. Cowden, J. Damgov, C. Dragoiu, P. R. Dudero, J. Faulkner, S. Kunori, K. Lamichhane, S. W. Lee, T. Libeiro, S. Undleeb & I. Volobouev
Vanderbilt University, Nashville, USA
E. Appelt, A. G. Delannoy, S. Greene, A. Gurrola, R. Janjam, W. Johns, C. Maguire, Y. Mao, A. Melo, H. Ni, P. Sheldon, S. Tuo, J. Velkovska & Q. Xu
University of Virginia, Charlottesville, USA
M. W. Arenton, B. Cox, B. Francis, J. Goodell, R. Hirosky, A. Ledovskoy, H. Li, C. Lin, C. Neu, T. Sinthuprasith, X. Sun, Y. Wang, E. Wolfe, J. Wood & F. Xia
Wayne State University, Detroit, USA
C. Clarke, R. Harr, P. E. Karchin, C. Kottachchi Kankanamge Don, P. Lamichhane & J. Sturdy
University of Wisconsin-Madison, Madison, WI, USA
D. A. Belknap, D. Carlsmith, M. Cepeda, S. Dasu, L. Dodd, S. Duric, B. Gomber, M. Grothe, M. Herndon, A. Hervé, P. Klabbers, A. Lanaro, A. Levine, K. Long, R. Loveless, A. Mohapatra, I. Ojalvo, T. Perry, G. A. Pierro, G. Polese, T. Ruggles, T. Sarangi, A. Savin, A. Sharma, N. Smith, W. H. Smith, D. Taylor, P. Verwilligen & N. Woods
CERN, Geneva, Switzerland
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Khachatryan, V., Sirunyan, A.M., Tumasyan, A. et al. Measurement of dijet azimuthal decorrelation in pp collisions at \(\sqrt{s}=8\,\mathrm{TeV} \) . Eur. Phys. J. C 76, 536 (2016). https://doi.org/10.1140/epjc/s10052-016-4346-8
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DOI: https://doi.org/10.1140/epjc/s10052-016-4346-8
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