Evidence of
b
-Jet Quenching in PbPb Collisions at
ffiffiffiffiffiffiffiffi
s
NN
p
¼
2
.
76
TeV
S. Chatrchyan et al.*(CMS Collaboration)
(Received 15 December 2013; published 22 September 2014)
The production of jets associated to bottom quarks is measured for the first time in PbPb collisions at a center-of-mass energy of 2.76 TeV per nucleon pair. Jet spectra are reported in the transverse momentum (pT) range of80–250GeV=c, and within pseudorapidityjηj<2. The nuclear modification factor (RAA)
calculated from these spectra shows a strong suppression in theb-jet yield in PbPb collisions relative to the yield observed inppcollisions at the same energy. The suppression persists to the largest values ofpT
studied, and is centrality dependent. TheRAAis about 0.4 in the most central events, similar to previous
observations for inclusive jets. This implies that jet quenching does not have a strong dependence on parton mass and flavor in the jetpT range studied.
DOI:10.1103/PhysRevLett.113.132301 PACS numbers: 25.75.Dw, 24.85.+p
By colliding heavy nuclei at the Large Hadron Collider (LHC), one expects to reach sufficiently large energy densities to form a strongly coupled quark-gluon plasma (QGP), a state which is characterized by effective decon-finement of the quarks and gluons [1–3]. Hard-scattered
partons are expected to suffer energy loss as they traverse the QGP via elastic and inelastic interactions[4,5]. This is commonly thought to be the mechanism responsible for the observed suppression of high transverse momentum (pT)
hadrons and jets, or “jet quenching,” in nuclear collisions
[6–16]. Measurements of parton energy loss are expected to reveal the fundamental thermodynamic and transport properties of this phase of matter (see Refs. [17,18] for recent reviews).
The quenching of jets in heavy-ion collisions is expected to depend upon the flavor of the fragmenting parton. Energy loss via gluon bremsstrahlung, which is thought to be the dominant mechanism for light partons, should be larger for gluon jets than quark jets, due to the larger color factor for gluon emission from the former. The mass of the leading parton may also play a role. Collisional energy loss could be an important effect for massive quarks and has been invoked to describe the nuclear modification factors for leptons from heavy-flavor decays at lowpT[19–21]. In
this regime, radiative energy loss from heavy quarks may be suppressed due to coherence effects[22,23], although the relevance of such effects in finite-size systems is a subject of debate[24]. The strongly coupled nature of the QGP may also introduce mass effects, according to a description of jet quenching based on the AdS-CFT correspondence[25,26]. Consequently, measurements of the flavor and mass
dependence of jet quenching are essential to obtain a sound theoretical description of this phenomenon.
Measurements of hadrons containing b quarks are
expected to be sensitive to the details ofb-quark energy loss. Recent data on single-particle production ofBmesons
(via nonprompt J=ψ) [27] show a smaller suppression
compared to D mesons [28] and nonidentified charged
particles[29,30]. Experimentally, the jet associated to ab
hadron is commonly referred to a“bjet,” although the b
quark is not guaranteed to be the leading parton of the jet. In relation to B mesons,b jets provide a complementary
approach to study b-quark energy loss, albeit typically
in a different range ofpT. Through comparisons with the
existing measurements of inclusive jet production [31],
b-jet measurements can be used to study the flavor
dependence of jet quenching, which in turn provides insight on the dynamics of parton energy loss.
The Compact Muon Solenoid (CMS) detector has excellent capabilities to perform b-jet identification
(b-tagging) measurements as demonstrated in Ref. [32]. Measurements of the b-jet cross section [33] and b-jet
angular correlations [34] have been performed in pp
collisions at 7 TeV. This Letter presents the first measure-ments ofb-jet production in heavy-ion collisions using a data set corresponding to an integrated luminosity of 150μb−1 of PbPb collisions at ffiffiffiffiffiffiffiffis
NN
p
¼2.76TeV deliv-ered by the LHC in 2011. The comparison measurements are performed with a data set consisting of pp data
recorded in 2013 and corresponding to an integrated luminosity of5.3pb−1at pffiffiffis¼2.76TeV.
The central feature of the CMS apparatus is a super-conducting solenoid providing a magnetic field of 3.8 T. Charged particle trajectories are measured with the silicon tracker, which provides an impact parameter resolution of∼15μm and apT resolution of∼1.5%for100GeV=c
particles. A PbWO4 crystal electromagnetic calorimeter and a brass-scintillator hadron calorimeter surround the * Full author list given at the end of the article.
Published by the American Physical Society under the terms of the Creative Commons Attribution 3.0 License. Further distri-bution of this work must maintain attridistri-bution to the author(s) and the published articles title, journal citation, and DOI.
tracking volume. The forward regions (2.9<jηj<5.2, whereη¼−ln½tanðθ=2Þandθis the polar angle measured
with respect to the counterclockwise beam direction) are instrumented with iron/quartz-fiber hadron forward calo-rimeters (HF). Collision centrality, defined as a percentile of the total inelastic nucleus-nucleus cross section, is calculated using the sum of the HF transverse energy
[35]. A set of scintillator tiles, used for triggering and beam-halo rejection, is mounted on the inner side of the HF calorimeters. A more detailed description of the CMS detector can be found in Ref.[36].
Jets are reconstructed from particle candidates obtained from a particle-flow algorithm [37]. This algorithm improves the resolution of jets, while reducing the parton flavor dependence of the detector response as compared to a purely calorimetric measurement. The anti-kTclustering
algorithm [38] is used, with a distance parameter of
R¼0.3. Details of the jet reconstruction, resolution and energy corrections may be found in Refs.[14,16,39]. The underlying background of bulk particle production in PbPb collisions is subtracted using the same method described in Ref. [40]. JetpT resolution effects are unfolded using an
iterative method[41], as implemented in the ROOUNFOLD
package [42].
The Monte Carlo simulations are performed using
PYTHIA 6.422 [43] with tune Z2 [44]. A parton flavor is
assigned to reconstructed jets by matching them inΔR¼ ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
Δη2
þΔϕ2
p
to generator-level partons (ϕis the azimuthal
angle measured in radians in the plane transverse to the beams). If a bottom quark is found within ΔR <0.3then the jet is considered to be abjet, irrespective of any other
partons in the cone. This definition includesbquarks from
gluon splitting (g→bb¯), even if the splitting occurs late in
the parton shower (i.e., at low virtuality), consistent with
the theoretical treatment of heavy-flavor production in Refs. [45,46]. We note that b jets from gluon splitting
comprise about 30–35% of the total b-jet cross section according to PYTHIAsimulations, although measurements
of b−b¯ angular correlations at 7 TeV indicate that the
contribution is somewhat larger[34]. Such jets are expected to interact differently with the QGP than those from primary b quarks [47]. To compare with PbPb data,
PYTHIA events are embedded into PbPb events produced
by theHYDJETgenerator (version 1.8)[48], which is tuned
to reproduce event properties, such as charged-hadron multiplicity, pT spectra, and elliptic flow. The rate of
bottom-quark production per nucleon-nucleon interaction in HYDJET was found to be consistent with theoretical
calculations forppcollisions based on Ref.[46]. Identification of b jets is based on kinematic variables related to the relatively long lifetime and large mass ofb
hadrons. Charged tracks ofpT>1GeV=cwithinR <0.3
from the jet axis are used to reconstruct secondary vertices (SV) from bhadrons and/or subsequent c-hadron decays from theb→ccascade, using an adaptive vertex fit[49].
The contribution ofbjets is enhanced by requiring that SVs
are far enough from the primary vertex, using a selection on the significance of the three-dimensional flight distance. This selection is chosen to give a misidentification rate of roughly 1% for light jets and 10% on charm-quark jets (cjets), based on simulation. The correspondingb-tagging
efficiency is about 65% for pp and 45% for PbPb
collisions. The compatibility of the simulation with data was verified by comparing basic distributions such as the
χ2 of the SV fit, the number of tracks per SV, and the number of SVs per jet. Figure1(left) shows an example comparison of the SV pT distribution. The shape of the
distribution is well described over the fullpT range.
(GeV/c)
T
Secondary vertex p
0 10 20 30 40 50 60 70 80 90 100
Number of jets / 10 GeV/c 5
10 15 20 25 30 35 3 10 × Data b jets c jets light jets < 90 GeV/c
T
80 < p |η| < 2
CMS -1 b μ PbPb, 150 0-100%
= 2.76 TeV
NN
s
0 20 40 60 80 100 10 2 10 3 10 4 10
0 10 20 30 40 50 60 70 80 90 100
0.5 1 1.5
)
2
Secondary vertex mass (GeV/c
0 1 2 3 4 5 6
0.5 1 1.5 2 2.5 3 3.5 4 4.5 3 10 × Data b jets c jets light jets < 90 GeV/c
T
80 < p |η| < 2
CMS -1 b μ PbPb, 150 0-100%
= 2.76 TeV
NN
s
0 1 2 3 4 5 6 10
2 10
3 10
0 1 2 3 4 5 6
0.5 1 1.5
Data/MC
(GeV/c) Secondary vertex mass (GeV/c )2
T
Secondary vertex p
2
Number of jets / 0.5 GeV/c
Data/MC
FIG. 1 (color online). Left: Comparison of SVpTdistribution between data and simulation for the same jet and event selections. The
simulation is normalized to the data. Right: Template fit to the SV invariant mass distribution in centrality-integrated (0–100%) PbPb
The SV invariant mass is calculated from the constituent tracks. An example SV mass distribution, for jets with 80< pT<90GeV=c, is shown in Fig.1(right). For each jetpTbin, theb-jet purity (fb), i.e., the ratio of the number
of bjets to that of inclusive jets in the tagged sample, is
extracted by means of a template fit. The shapes of the light-quark, c and b contributions are determined from simulation, while their normalizations are allowed to float. After tagging, the three contributions are of comparable magnitude, as shown in the figure, but the b-quark
contribution dominates above the c-quark mass threshold
near2GeV=c2, which allows for an accurate determination of theb-jet contribution. The quality of the SV mass fits was found to be good, with values of χ2 per degree of freedom typically in the range of 1–2. The proportion of tagged jets for which the SV corresponds to a b hadron
from a different nucleon-nucleon interaction than the one that produced the jet was estimated from simulation to be 2% for the 20% most central PbPb collisions.
For the systematic studies described below, an alternative b-tagging strategy is employed, which uses
the jet probability (JP) algorithm[32]. In contrast to direct reconstruction of SVs, the JP tagger is based on an estimate of the compatibility of tracks with the primary vertex, using their three-dimensional impact parameter significance. A probability density for this compatibility is obtained directly from data using tracks with negative impact parameter, which are unlikely to come from heavy-flavor decays. The impact parameter (IP) is defined to have the same sign as the scalar product of the vector pointing from the primary vertex to the point of closest approach with the jet direction. Tracks originating from the decay of particles traveling along the jet axis will tend to have positive IP values.
Using theb-jet purity (fb) derived from the template fit,
theb-jet yield in a givenpTbin is obtained asNb¼Nfb=ϵ,
where N is the number of all b-tagged jets and ϵ is the b-tagging efficiency. The efficiencyϵ is determined from
simulation and cross-checked using the so-called reference lifetime tagger method [32], which uses the JP tagger to determine the efficiency of the SV tagger directly from data, taking advantage of the calibration of the primary vertex compatibility used in this tagger which is obtained from data. The simulation reproduces the estimate ofϵfrom
data to within 5%.
The unfolded b-jet pT spectra in PbPb collisions are
shown in Fig.2for several centrality selections. The PbPb data are divided byTAA, computed from a Glauber model
(for a review, see Ref.[50]), to scale to the expectation for
ppcollisions in the absence of nuclear effects. The value of TAA is the number of nucleon-nucleon (NN) collisions
divided by the total inelasticNNcross section and may be interpreted as the NN equivalent luminosity per PbPb collision. Also shown is the measured b-jet cross section
inppcollisions. The cross section is compared toPYTHIA
simulations, which agree well with the data, as is the case at ffiffiffi
s
p
¼7TeV for the pT range covered by the present study[33].
The systematic uncertainties fall into two general cat-egories: b tagging and jet reconstruction. The b-tagging uncertainty onb-jet yields varies from about 12 to 18%, depending on jetpTand collision system. The uncertainty
is evaluated via the following systematic variations of the tagging procedure, which influence the extractedb-tagging
purity and efficiency values: (a) varying the SV flight distance selection such that ϵ differs by about 10%,
(b) using ϵ from the reference lifetime tagger method [32], rather than from simulation, (c) fixing the c jet to
light-quark jet normalization, rather than allowing them to float independently in the template fits, (d) using a non-b -jet template produced from -jets with small JP in data, and (e) varying the gluon-splitting contribution in theb-jet and c-jet templates by 50%.
The uncertainty on the spectra due to the jet reconstruction is 10–12% for pp and 15–17% for PbPb, and is comprised of the following sources: (1) a 10% uncertainty in the jet energy resolution [51], (2) a 2% uncertainty in the jet energy scale (JES) [51], (3) an
(GeV/c)
T
b-jet p
100 150 200 250
GeV/c pb T p Δ PbPb N Δ AA T evt N 1 , T p Δ pp σ Δ -1 10 1 10 2 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 -1 b μ PbPb, 150 Data, 0-100% 2 10 × 0-10% 3 10 × 10-30% 4 10 × 30-50% 5 10 × 50-100% -1
pp, 5.3 pb Data PYTHIA
| < 2
η |
CMS sNN = 2.76 TeV
FIG. 2 (color online). The b-jet yield as a function ofpT is
shown for various centrality classes of PbPb collisions as indicated in the legend. The yields are scaled by the equivalent number of minimum bias events sampled and by TAA. The
spectra are also scaled by powers of 10 for visibility. Theb-jet
additional, centrality-dependent, 1–2% uncertainty in the JES in PbPb collisions due to the underlying event, evaluated from random-cone and embedding studies, and (4) an uncertainty in the unfolding procedure evaluated by varying the number of iterations and the presumed prior spectrum.
Theppluminosity has an uncertainty of 3.6%, while the uncertainty inTAAvaries from about 4% for a centrality of
0–10% to 15% for 50–100%[16].
Figure 3 shows the centrality-integrated b-jet nuclear
modification factor (RAA), which is the ratio of the TAA
-normalized PbPb yield and the measuredppcross section
in Fig. 2, as a function of pT. The jet and b-tagging
systematic uncertainties in RAA are obtained by varying
the pp and PbPb data simultaneously. This results in
partial cancellation, giving a systematic uncertainty of 16–21%, which is dominated by theb-tagging uncertainty. A significant suppression of the yield with respect to the
pp expectation is observed in b jets, which is indicative
of the parton energy loss in the hot medium. No strong trend is observed as a function of pT, although the data
hint a modest rise at higher pT. The data are compared
to perturbative QCD (pQCD)-based calculations from Ref. [47]. The data are found to be consistent with a jet-medium coupling (gmed) in the range of 1.8–2, similar to the value found for inclusive jets.
Figure 4 shows RAA as a function of the number of
participating nucleons (Npart), which is derived from the
centrality (as measured by the energy in the forward
calorimeters) through a Glauber calculation. Data for 80< pT<90GeV=cand90< pT<110GeV=care shown. For both jet selections RAA shows a smooth decrease
with increasing centrality from about 0.70–0.75 to about 0.35–0.40.
The data presented in this study demonstrate the jet quenching phenomenon in the b-jet sector using fully
reconstructed b jets for the first time in heavy-ion
colli-sions. Integrating over all collision centralities, bjets are found to be suppressed over the80–250GeV=c pTrange explored in this study. For the 80–110GeV=c pT range,
RAAis found to decrease with collision centrality. At larger
pT, the trend is less evident due to the reduced statistical
precision. Theb-jet suppression is found to be qualitatively consistent with that of inclusive jets [31]. Although a sizable fraction ofb-tagged jets come from gluon splitting,
a large mass and/or flavor dependence for parton energy loss can be excluded. For example, a model based on strong coupling (via the AdS-CFT correspondence)[26], in which mass effects could persist to largepTwould be
incompat-ible with the current data, in contrast to a perturbative model in which mass effects are expected to be small at largepT[47]. A milder mass dependence, but one which
still persists to largepT, as predicted for light- and
heavy-flavor hadrons in Ref.[52], cannot be ruled out with the present uncertainties.
We congratulate our colleagues in the CERN accelerator departments for the excellent performance of the LHC and (GeV/c)
T
b-jet p
100 150 200 250
AA b-jet R 0 0.2 0.4 0.6 0.8 1 1.2
pQCD: PLB 726 (2013) 251-256 = 1.8 med g = 2.0 med g = 2.2 med g CMS -1 pp, 5.3 pb
-1 b
μ
PbPb, 150
= 2.76 TeV
NN
s
0-100% |η| < 2
FIG. 3 (color online). The centrality-integrated (0–100%)b-jet RAA as a function ofpT. Vertical and horizontal bars represent
statistical uncertainties and bin widths, respectively, while filled boxes represent systematics uncertainties. The normaliza-tion uncertainty from the integrated luminosity inppcollisions
and fromTAAis represented by the green band around unity. The
data are compared to pQCD-based calculations from Ref.[47].
part
N
0 50 100 150 200 250 300 350 400
AA b-Jet R 0 0.2 0.4 0.6 0.8 1 1.2
< 90 GeV/c T
80 < p
< 110 GeV/c T
90 < p CMS
-1 pp, 5.3 pb
-1 b
μ
PbPb, 150
= 2.76 TeV
NN
s
| < 2
η | 0-10% 10-30% 30-50% 50-100%
FIG. 4 (color online). Theb-jetRAA, as a function ofNpartfor
two jet pT selections as indicated in the legend. Statistical
uncertainties are shown as error bars. The filled boxes represent the systematics uncertainties, excluding the TAA uncertainties,
which are depicted as open boxes. The normalization uncertainty in the integrated luminosity inppcollisions is represented by the
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 centers 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: BMWF 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, SF0690030s09 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); NRF and WCU (Republic of Korea); LAS (Lithuania);
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); NSC (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA).
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S. Chatrchyan,1 V. Khachatryan,1 A. M. Sirunyan,1 A. Tumasyan,1 W. Adam,2 T. Bergauer,2 M. Dragicevic,2 J. Erö,2 C. Fabjan,2,bM. Friedl,2R. Frühwirth,2,bV. M. Ghete,2C. Hartl,2N. Hörmann,2J. Hrubec,2M. Jeitler,2,bW. Kiesenhofer,2
V. Knünz,2 M. Krammer,2,bI. Krätschmer,2 D. Liko,2 I. Mikulec,2D. Rabady,2,c B. Rahbaran,2H. Rohringer,2 R. Schöfbeck,2 J. Strauss,2 A. Taurok,2 W. Treberer-Treberspurg,2 W. Waltenberger,2 C.-E. Wulz,2,b V. Mossolov,3 N. Shumeiko,3J. Suarez Gonzalez,3S. Alderweireldt,4M. Bansal,4S. Bansal,4T. Cornelis,4E. A. De Wolf,4X. Janssen,4 A. Knutsson,4S. Luyckx,4L. Mucibello,4S. Ochesanu,4B. Roland,4R. Rougny,4H. Van Haevermaet,4P. Van Mechelen,4 N. Van Remortel,4 A. Van Spilbeeck,4 F. Blekman,5 S. Blyweert,5 J. D’Hondt,5 N. Heracleous,5 A. Kalogeropoulos,5
J. Keaveney,5 T. J. Kim,5S. Lowette,5 M. Maes,5 A. Olbrechts,5 D. Strom,5 S. Tavernier,5W. Van Doninck,5 P. Van Mulders,5G. P. Van Onsem,5I. Villella,5C. Caillol,6B. Clerbaux,6G. De Lentdecker,6L. Favart,6A. P. R. Gay,6 A. Léonard,6P. E. Marage,6A. Mohammadi,6L. Perniè,6 T. Reis,6 T. Seva,6 L. Thomas,6 C. Vander Velde,6P. Vanlaer,6
J. Wang,6 V. Adler,7 K. Beernaert,7 L. Benucci,7 A. Cimmino,7S. Costantini,7S. Dildick,7 G. Garcia,7 B. Klein,7 J. Lellouch,7J. Mccartin,7A. A. Ocampo Rios,7D. Ryckbosch,7S. Salva Diblen,7M. Sigamani,7N. Strobbe,7F. Thyssen,7
M. Tytgat,7 S. Walsh,7 E. Yazgan,7 N. Zaganidis,7 S. Basegmez,8 C. Beluffi,8,dG. Bruno,8 R. Castello,8A. Caudron,8 L. Ceard,8G. G. Da Silveira,8C. Delaere,8T. du Pree,8D. Favart,8L. Forthomme,8A. Giammanco,8,eJ. Hollar,8P. Jez,8
M. Komm,8 V. Lemaitre,8 J. Liao,8 O. Militaru,8 C. Nuttens,8 D. Pagano,8 A. Pin,8 K. Piotrzkowski,8 A. Popov,8,f
L. Quertenmont,8 M. Selvaggi,8M. Vidal Marono,8 J. M. Vizan Garcia,8 N. Beliy,9 T. Caebergs,9 E. Daubie,9 G. H. Hammad,9 G. A. Alves,10M. Correa Martins Junior,10T. Martins,10M. E. Pol,10M. H. G. Souza,10 W. L. Aldá Júnior,11W. Carvalho,11J. Chinellato,11,gA. Custódio,11E. M. Da Costa,11D. De Jesus Damiao,11 C. De Oliveira Martins,11S. Fonseca De Souza,11H. Malbouisson,11M. Malek,11D. Matos Figueiredo,11L. Mundim,11
H. Nogima,11 W. L. Prado Da Silva,11 J. Santaolalla,11A. Santoro,11A. Sznajder,11E. J. Tonelli Manganote,11,g A. Vilela Pereira,11C. A. Bernardes,12bF. A. Dias,12a,hT. R. Fernandez Perez Tomei,12aE. M. Gregores,12bC. Lagana,12a
P. G. Mercadante,12b S. F. Novaes,12a S. S. Padula,12a V. Genchev,13,cP. Iaydjiev,13,c A. Marinov,13S. Piperov,13 M. Rodozov,13G. Sultanov,13 M. Vutova,13A. Dimitrov,14I. Glushkov,14R. Hadjiiska,14V. Kozhuharov,14 L. Litov,14 B. Pavlov,14P. Petkov,14J. G. Bian,15G. M. Chen,15H. S. Chen,15M. Chen,15R. Du,15C. H. Jiang,15D. Liang,15S. Liang,15 X. Meng,15R. Plestina,15,iJ. Tao,15X. Wang,15Z. Wang,15C. Asawatangtrakuldee,16Y. Ban,16Y. Guo,16W. Li,16S. Liu,16
Y. Mao,16S. J. Qian,16H. Teng,16D. Wang,16L. Zhang,16W. Zou,16C. Avila,17C. A. Carrillo Montoya,17 L. F. Chaparro Sierra,17C. Florez,17J. P. Gomez,17B. Gomez Moreno,17J. C. Sanabria,17N. Godinovic,18D. Lelas,18 D. Polic,18I. Puljak,18Z. Antunovic,19M. Kovac,19V. Brigljevic,20K. Kadija,20J. Luetic,20D. Mekterovic,20S. Morovic,20 L. Tikvica,20 A. Attikis,21 G. Mavromanolakis,21J. Mousa,21C. Nicolaou,21F. Ptochos,21 P. A. Razis,21M. Finger,22 M. Finger Jr.,22Y. Assran,23,jS. Elgammal,23,kT. Elkafrawy,23,lA. Ellithi Kamel,23,mM. A. Mahmoud,23,n A. Radi,23,k,l M. Kadastik,24M. Müntel,24M. Murumaa,24M. Raidal,24L. Rebane,24A. Tiko,24P. Eerola,25G. Fedi,25M. Voutilainen,25 J. Härkönen,26V. Karimäki,26R. Kinnunen,26M. J. Kortelainen,26T. Lampén,26K. Lassila-Perini,26S. Lehti,26T. Lindén,26 P. Luukka,26T. Mäenpää,26T. Peltola,26E. Tuominen,26J. Tuominiemi,26E. Tuovinen,26L. Wendland,26T. Tuuva,27
M. Besancon,28F. Couderc,28M. Dejardin,28 D. Denegri,28B. Fabbro,28J. L. Faure,28F. Ferri,28S. Ganjour,28 A. Givernaud,28P. Gras,28G. Hamel de Monchenault,28P. Jarry,28E. Locci,28J. Malcles,28A. Nayak,28 J. Rander,28 A. Rosowsky,28M. Titov,28S. Baffioni,29F. Beaudette,29P. Busson,29C. Charlot,29N. Daci,29T. Dahms,29M. Dalchenko,29
L. Dobrzynski,29A. Florent,29R. Granier de Cassagnac,29P. Miné,29C. Mironov,29I. N. Naranjo,29M. Nguyen,29 C. Ochando,29P. Paganini,29D. Sabes,29R. Salerno,29Y. Sirois,29C. Veelken,29Y. Yilmaz,29A. Zabi,29J.-L. Agram,30,o
J. Andrea,30 D. Bloch,30J.-M. Brom,30E. C. Chabert,30C. Collard,30 E. Conte,30,o F. Drouhin,30,oJ.-C. Fontaine,30,o D. Gelé,30U. Goerlach,30C. Goetzmann,30 P. Juillot,30A.-C. Le Bihan,30P. Van Hove,30 S. Gadrat,31S. Beauceron,32 N. Beaupere,32G. Boudoul,32S. Brochet,32J. Chasserat,32R. Chierici,32D. Contardo,32P. Depasse,32H. El Mamouni,32
J. Fan,32J. Fay,32S. Gascon,32M. Gouzevitch,32B. Ille,32T. Kurca,32M. Lethuillier,32L. Mirabito,32 S. Perries,32 J. D. Ruiz Alvarez,32L. Sgandurra,32V. Sordini,32M. Vander Donckt,32P. Verdier,32S. Viret,32H. Xiao,32 Z. Tsamalaidze,33,pC. Autermann,34S. Beranek,34M. Bontenackels,34B. Calpas,34M. Edelhoff,34L. Feld,34O. Hindrichs,34 K. Klein,34A. Ostapchuk,34A. Perieanu,34F. Raupach,34J. Sammet,34S. Schael,34D. Sprenger,34H. Weber,34B. Wittmer,34
B. Kargoll,36T. Kress,36Y. Kuessel,36J. Lingemann,36,cA. Nowack,36I. M. Nugent,36L. Perchalla,36O. Pooth,36A. Stahl,36 I. Asin,37N. Bartosik,37J. Behr,37W. Behrenhoff,37U. Behrens,37A. J. Bell,37M. Bergholz,37,qA. Bethani,37K. Borras,37 A. Burgmeier,37A. Cakir,37L. Calligaris,37A. Campbell,37S. Choudhury,37F. Costanza,37C. Diez Pardos,37S. Dooling,37 T. Dorland,37G. Eckerlin,37D. Eckstein,37T. Eichhorn,37G. Flucke,37A. Geiser,37A. Grebenyuk,37P. Gunnellini,37 S. Habib,37J. Hauk,37G. Hellwig,37M. Hempel,37D. Horton,37H. Jung,37M. Kasemann,37 P. Katsas,37 J. Kieseler,37 C. Kleinwort,37M. Krämer,37D. Krücker,37W. Lange,37J. Leonard,37K. Lipka,37W. Lohmann,37,qB. Lutz,37R. Mankel,37 I. Marfin,37I.-A. Melzer-Pellmann,37A. B. Meyer,37J. Mnich,37A. Mussgiller,37S. Naumann-Emme,37O. Novgorodova,37 F. Nowak,37H. Perrey,37A. Petrukhin,37D. Pitzl,37R. Placakyte,37A. Raspereza,37P. M. Ribeiro Cipriano,37C. Riedl,37
E. Ron,37M. O. Sahin,37J. Salfeld-Nebgen,37 P. Saxena,37R. Schmidt,37,q T. Schoerner-Sadenius,37M. Schröder,37 M. Stein,37A. D. R. Vargas Trevino,37R. Walsh,37C. Wissing,37M. Aldaya Martin,38V. Blobel,38H. Enderle,38J. Erfle,38
E. Garutti,38K. Goebel,38M. Görner,38M. Gosselink,38J. Haller,38R. S. Höing,38H. Kirschenmann,38R. Klanner,38 R. Kogler,38J. Lange,38I. Marchesini,38J. Ott,38T. Peiffer,38N. Pietsch,38D. Rathjens,38C. Sander,38H. Schettler,38 P. Schleper,38E. Schlieckau,38A. Schmidt,38M. Seidel,38J. Sibille,38,rV. Sola,38H. Stadie,38G. Steinbrück,38D. Troendle,38
E. Usai,38L. Vanelderen,38 C. Barth,39C. Baus,39J. Berger,39 C. Böser,39E. Butz,39T. Chwalek,39W. De Boer,39 A. Descroix,39A. Dierlamm,39M. Feindt,39M. Guthoff,39,cF. Hartmann,39,c T. Hauth,39,c H. Held,39K. H. Hoffmann,39
U. Husemann,39I. Katkov,39,f A. Kornmayer,39,c E. Kuznetsova,39P. Lobelle Pardo,39D. Martschei,39 M. U. Mozer,39 T. Müller,39M. Niegel,39A. Nürnberg,39O. Oberst,39G. Quast,39K. Rabbertz,39F. Ratnikov,39S. Röcker,39F.-P. Schilling,39 G. Schott,39H. J. Simonis,39F. M. Stober,39R. Ulrich,39J. Wagner-Kuhr,39S. Wayand,39T. Weiler,39R. Wolf,39M. Zeise,39 G. Anagnostou,40G. Daskalakis,40T. Geralis,40S. Kesisoglou,40A. Kyriakis,40D. Loukas,40A. Markou,40C. Markou,40
E. Ntomari,40A. Psallidas,40I. Topsis-giotis,40 L. Gouskos,41A. Panagiotou,41N. Saoulidou,41E. Stiliaris,41 X. Aslanoglou,42I. Evangelou,42G. Flouris,42C. Foudas,42P. Kokkas,42N. Manthos,42I. Papadopoulos,42E. Paradas,42 G. Bencze,43 C. Hajdu,43P. Hidas,43D. Horvath,43,sF. Sikler,43 V. Veszpremi,43G. Vesztergombi,43,tA. J. Zsigmond,43 N. Beni,44 S. Czellar,44J. Molnar,44J. Palinkas,44Z. Szillasi,44 J. Karancsi,45P. Raics,45Z. L. Trocsanyi,45B. Ujvari,45 S. K. Swain,46S. B. Beri,47V. Bhatnagar,47N. Dhingra,47R. Gupta,47M. Kaur,47M. Z. Mehta,47M. Mittal,47N. Nishu,47
A. Sharma,47J. B. Singh,47A. Kumar,48A. Kumar,48 S. Ahuja,48A. Bhardwaj,48B. C. Choudhary,48A. Kumar,48 S. Malhotra,48M. Naimuddin,48K. Ranjan,48V. Sharma,48R. K. Shivpuri,48S. Banerjee,49 S. Bhattacharya,49 K. Chatterjee,49S. Dutta,49 B. Gomber,49S. Jain,49S. Jain,49R. Khurana,49A. Modak,49 S. Mukherjee,49D. Roy,49
S. Sarkar,49M. Sharan,49A. P. Singh,49 A. Abdulsalam,50D. Dutta,50S. Kailas,50V. Kumar,50A. K. Mohanty,50,c L. M. Pant,50P. Shukla,50A. Topkar,50T. Aziz,51R. M. Chatterjee,51S. Ganguly,51S. Ghosh,51M. Guchait,51,uA. Gurtu,51,v
G. Kole,51S. Kumar,51 M. Maity,51,w G. Majumder,51K. Mazumdar,51G. B. Mohanty,51B. Parida,51K. Sudhakar,51 N. Wickramage,51,x S. Banerjee,52S. Dugad,52H. Arfaei,53H. Bakhshiansohi,53H. Behnamian,53S. M. Etesami,53,y
A. Fahim,53,z A. Jafari,53M. Khakzad,53M. Mohammadi Najafabadi,53M. Naseri,53 S. Paktinat Mehdiabadi,53 B. Safarzadeh,53,aaM. Zeinali,53M. Grunewald,54M. Abbrescia,55a,55bL. Barbone,55a,55b C. Calabria,55a,55b S. S. Chhibra,55a,55bA. Colaleo,55aD. Creanza,55a,55cN. De Filippis,55a,55cM. De Palma,55a,55bL. Fiore,55aG. Iaselli,55a,55c
G. Maggi,55a,55c M. Maggi,55a B. Marangelli,55a,55bS. My,55a,55c S. Nuzzo,55a,55bN. Pacifico,55a A. Pompili,55a,55b G. Pugliese,55a,55cR. Radogna,55a,55bG. Selvaggi,55a,55bL. Silvestris,55aG. Singh,55a,55bR. Venditti,55a,55bP. Verwilligen,55a
G. Zito,55a G. Abbiendi,56aA. C. Benvenuti,56aD. Bonacorsi,56a,56b S. Braibant-Giacomelli,56a,56b L. Brigliadori,56a,56b R. Campanini,56a,56bP. Capiluppi,56a,56b A. Castro,56a,56bF. R. Cavallo,56a G. Codispoti,56a,56b M. Cuffiani,56a,56b G. M. Dallavalle,56a F. Fabbri,56a A. Fanfani,56a,56b D. Fasanella,56a,56bP. Giacomelli,56a C. Grandi,56a L. Guiducci,56a,56b S. Marcellini,56aG. Masetti,56aM. Meneghelli,56a,56b A. Montanari,56a F. L. Navarria,56a,56bF. Odorici,56a A. Perrotta,56a F. Primavera,56a,56bA. M. Rossi,56a,56bT. Rovelli,56a,56bG. P. Siroli,56a,56bN. Tosi,56a,56bR. Travaglini,56a,56bS. Albergo,57a,57b G. Cappello,57a M. Chiorboli,57a,57bS. Costa,57a,57bF. Giordano,57a,c R. Potenza,57a,57b A. Tricomi,57a,57bC. Tuve,57a,57b
G. Barbagli,58a V. Ciulli,58a,58b C. Civinini,58a R. D’Alessandro,58a,58b E. Focardi,58a,58b E. Gallo,58a S. Gonzi,58a,58b
V. Gori,58a,58bP. Lenzi,58a,58bM. Meschini,58aS. Paoletti,58aG. Sguazzoni,58aA. Tropiano,58a,58bL. Benussi,59S. Bianco,59 F. Fabbri,59D. Piccolo,59P. Fabbricatore,60aR. Ferretti,60a,60bF. Ferro,60aM. Lo Vetere,60a,60bR. Musenich,60aE. Robutti,60a S. Tosi,60a,60bA. Benaglia,61a M. E. Dinardo,61a,61b S. Fiorendi,61a,61b,c S. Gennai,61a A. Ghezzi,61a,61bP. Govoni,61a,61b
P. Azzi,63aN. Bacchetta,63aD. Bisello,63a,63bA. Branca,63a,63bR. Carlin,63a,63bP. Checchia,63aT. Dorigo,63aU. Dosselli,63a M. Galanti,63a,63b,c F. Gasparini,63a,63b P. Giubilato,63a,63bA. Gozzelino,63a K. Kanishchev,63a,63c S. Lacaprara,63a I. Lazzizzera,63a,63c M. Margoni,63a,63bA. T. Meneguzzo,63a,63b F. Montecassiano,63a M. Passaseo,63aJ. Pazzini,63a,63b M. Pegoraro,63a N. Pozzobon,63a,63bP. Ronchese,63a,63bF. Simonetto,63a,63bE. Torassa,63a M. Tosi,63a,63bP. Zotto,63a,63b A. Zucchetta,63a,63bG. Zumerle,63a,63bM. Gabusi,64a,64bS. P. Ratti,64a,64bC. Riccardi,64a,64bP. Vitulo,64a,64bM. Biasini,65a,65b
G. M. Bilei,65aL. Fanò,65a,65b P. Lariccia,65a,65bG. Mantovani,65a,65bM. Menichelli,65a F. Romeo,65a,65bA. Saha,65a A. Santocchia,65a,65b A. Spiezia,65a,65bK. Androsov,66a,bb P. Azzurri,66a G. Bagliesi,66a J. Bernardini,66aT. Boccali,66a
G. Broccolo,66a,66c R. Castaldi,66a M. A. Ciocci,66a,bbR. Dell’Orso,66a F. Fiori,66a,66c L. Foà,66a,66c A. Giassi,66a
M. T. Grippo,66a,bb A. Kraan,66a F. Ligabue,66a,66c T. Lomtadze,66aL. Martini,66a,66bA. Messineo,66a,66bC. S. Moon,66a,cc F. Palla,66a A. Rizzi,66a,66bA. Savoy-Navarro,66a,dd A. T. Serban,66a P. Spagnolo,66a P. Squillacioti,66a,bb R. Tenchini,66a
G. Tonelli,66a,66bA. Venturi,66a P. G. Verdini,66a C. Vernieri,66a,66c L. Barone,67a,67bF. Cavallari,67a D. Del Re,67a,67b M. Diemoz,67a M. Grassi,67a,67bC. Jorda,67a E. Longo,67a,67b F. Margaroli,67a,67bP. Meridiani,67aF. Micheli,67a,67b S. Nourbakhsh,67a,67bG. Organtini,67a,67bR. Paramatti,67aS. Rahatlou,67a,67bC. Rovelli,67a L. Soffi,67a,67bP. Traczyk,67a,67b N. Amapane,68a,68b R. Arcidiacono,68a,68c S. Argiro,68a,68bM. Arneodo,68a,68c R. Bellan,68a,68bC. Biino,68a N. Cartiglia,68a
S. Casasso,68a,68bM. Costa,68a,68bA. Degano,68a,68b N. Demaria,68a C. Mariotti,68a S. Maselli,68a E. Migliore,68a,68b V. Monaco,68a,68bM. Musich,68aM. M. Obertino,68a,68cG. Ortona,68a,68bL. Pacher,68a,68bN. Pastrone,68aM. Pelliccioni,68a,c
A. Potenza,68a,68bA. Romero,68a,68b M. Ruspa,68a,68c R. Sacchi,68a,68bA. Solano,68a,68bA. Staiano,68a U. Tamponi,68a S. Belforte,69aV. Candelise,69a,69b M. Casarsa,69a F. Cossutti,69a G. Della Ricca,69a,69b B. Gobbo,69a C. La Licata,69a,69b M. Marone,69a,69bD. Montanino,69a,69bA. Penzo,69aA. Schizzi,69a,69bT. Umer,69a,69bA. Zanetti,69aS. Chang,70T. Y. Kim,70 S. K. Nam,70D. H. Kim,71G. N. Kim,71J. E. Kim,71M. S. Kim,71D. J. Kong,71S. Lee,71Y. D. Oh,71H. Park,71D. C. Son,71 J. Y. Kim,72Z. J. Kim,72S. Song,72S. Choi,73D. Gyun,73B. Hong,73M. Jo,73H. Kim,73Y. Kim,73K. S. Lee,73S. K. Park,73 Y. Roh,73M. Choi,74J. H. Kim,74C. Park,74I. C. Park,74S. Park,74G. Ryu,74Y. Choi,75Y. K. Choi,75J. Goh,75E. Kwon,75
B. Lee,75J. Lee,75 S. Lee,75H. Seo,75I. Yu,75A. Juodagalvis,76J. R. Komaragiri,77H. Castilla-Valdez,78 E. De La Cruz-Burelo,78I. Heredia-de La Cruz,78,eeR. Lopez-Fernandez,78J. Martínez-Ortega,78A. Sanchez-Hernandez,78 L. M. Villasenor-Cendejas,78S. Carrillo Moreno,79F. Vazquez Valencia,79H. A. Salazar Ibarguen,80E. Casimiro Linares,81
A. Morelos Pineda,81 D. Krofcheck,82P. H. Butler,83 R. Doesburg,83S. Reucroft,83 H. Silverwood,83M. Ahmad,84 M. I. Asghar,84J. Butt,84H. R. Hoorani,84S. Khalid,84W. A. Khan,84T. Khurshid,84S. Qazi,84M. A. Shah,84M. Shoaib,84
H. Bialkowska,85M. Bluj,85,ffB. Boimska,85T. Frueboes,85M. Górski,85M. Kazana,85K. Nawrocki,85 K. Romanowska-Rybinska,85M. Szleper,85G. Wrochna,85P. Zalewski,85G. Brona,86K. Bunkowski,86M. Cwiok,86 W. Dominik,86K. Doroba,86A. Kalinowski,86M. Konecki,86J. Krolikowski,86M. Misiura,86W. Wolszczak,86P. Bargassa,87 C. Beirão Da Cruz E Silva,87P. Faccioli,87P. G. Ferreira Parracho,87M. Gallinaro,87F. Nguyen,87J. Rodrigues Antunes,87 J. Seixas,87,cJ. Varela,87P. Vischia,87S. Afanasiev,88P. Bunin,88I. Golutvin,88I. Gorbunov,88A. Kamenev,88V. Karjavin,88 V. Konoplyanikov,88G. Kozlov,88A. Lanev,88A. Malakhov,88V. Matveev,88,ggP. Moisenz,88V. Palichik,88V. Perelygin,88
S. Shmatov,88N. Skatchkov,88V. Smirnov,88A. Zarubin,88V. Golovtsov,89 Y. Ivanov,89V. Kim,89P. Levchenko,89 V. Murzin,89V. Oreshkin,89I. Smirnov,89V. Sulimov,89L. Uvarov,89S. Vavilov,89A. Vorobyev,89A. Vorobyev,89 Y. Andreev,90A. Dermenev,90S. Gninenko,90N. Golubev,90M. Kirsanov,90N. Krasnikov,90A. Pashenkov,90D. Tlisov,90 A. Toropin,90V. Epshteyn,91V. Gavrilov,91N. Lychkovskaya,91V. Popov,91G. Safronov,91S. Semenov,91A. Spiridonov,91
V. Stolin,91E. Vlasov,91A. Zhokin,91V. Andreev,92M. Azarkin,92I. Dremin,92M. Kirakosyan,92A. Leonidov,92 G. Mesyats,92S. V. Rusakov,92A. Vinogradov,92A. Belyaev,93E. Boos,93A. Ershov,93 A. Gribushin,93 V. Klyukhin,93 O. Kodolova,93V. Korotkikh,93I. Lokhtin,93S. Obraztsov,93S. Petrushanko,93V. Savrin,93A. Snigirev,93I. Vardanyan,93 I. Azhgirey,94I. Bayshev,94S. Bitioukov,94V. Kachanov,94A. Kalinin,94D. Konstantinov,94V. Krychkine,94V. Petrov,94
R. Ryutin,94A. Sobol,94 L. Tourtchanovitch,94S. Troshin,94N. Tyurin,94A. Uzunian,94A. Volkov,94P. Adzic,95,hh M. Djordjevic,95M. Ekmedzic,95J. Milosevic,95M. Aguilar-Benitez,96J. Alcaraz Maestre,96C. Battilana,96E. Calvo,96
M. Cerrada,96M. Chamizo Llatas,96,c N. Colino,96B. De La Cruz,96A. Delgado Peris,96D. Domínguez Vázquez,96 C. Fernandez Bedoya,96J. P. Fernández Ramos,96A. Ferrando,96J. Flix,96M. C. Fouz,96P. Garcia-Abia,96 O. Gonzalez Lopez,96S. Goy Lopez,96J. M. Hernandez,96M. I. Josa,96 G. Merino,96E. Navarro De Martino,96 J. Puerta Pelayo,96A. Quintario Olmeda,96I. Redondo,96L. Romero,96M. S. Soares,96C. Willmott,96C. Albajar,97
J. F. de Trocóniz,97 M. Missiroli,97H. Brun,98J. Cuevas,98J. Fernandez Menendez,98S. Folgueras,98
J. Duarte Campderros,99M. Fernandez,99G. Gomez,99J. Gonzalez Sanchez,99A. Graziano,99A. Lopez Virto,99J. Marco,99 R. Marco,99C. Martinez Rivero,99F. Matorras,99F. J. Munoz Sanchez,99J. Piedra Gomez,99T. Rodrigo,99 A. Y. Rodríguez-Marrero,99A. Ruiz-Jimeno,99L. Scodellaro,99I. Vila,99R. Vilar Cortabitarte,99D. Abbaneo,100 E. Auffray,100 G. Auzinger,100M. Bachtis,100 P. Baillon,100A. H. Ball,100D. Barney,100J. Bendavid,100 L. Benhabib,100 J. F. Benitez,100C. Bernet,100,iG. Bianchi,100P. Bloch,100A. Bocci,100A. Bonato,100O. Bondu,100C. Botta,100H. Breuker,100 T. Camporesi,100 G. Cerminara,100T. Christiansen,100J. A. Coarasa Perez,100S. Colafranceschi,100,ii M. D’Alfonso,100
D. d’Enterria,100A. Dabrowski,100A. David,100F. De Guio,100 A. De Roeck,100S. De Visscher,100 S. Di Guida,100
M. Dobson,100 N. Dupont-Sagorin,100A. Elliott-Peisert,100J. Eugster,100G. Franzoni,100 W. Funk,100M. Giffels,100 D. Gigi,100K. Gill,100M. Girone,100M. Giunta,100F. Glege,100 R. Gomez-Reino Garrido,100S. Gowdy,100 R. Guida,100 J. Hammer,100M. Hansen,100 P. Harris,100V. Innocente,100 P. Janot,100 E. Karavakis,100 K. Kousouris,100K. Krajczar,100
P. Lecoq,100 C. Lourenço,100 N. Magini,100L. Malgeri,100M. Mannelli,100L. Masetti,100F. Meijers,100 S. Mersi,100 E. Meschi,100F. Moortgat,100M. Mulders,100P. Musella,100L. Orsini,100E. Palencia Cortezon,100E. Perez,100L. Perrozzi,100
A. Petrilli,100 G. Petrucciani,100 A. Pfeiffer,100 M. Pierini,100 M. Pimiä,100 D. Piparo,100 M. Plagge,100 A. Racz,100 W. Reece,100G. Rolandi,100,jjM. Rovere,100H. Sakulin,100F. Santanastasio,100C. Schäfer,100C. Schwick,100S. Sekmen,100
A. Sharma,100P. Siegrist,100 P. Silva,100 M. Simon,100P. Sphicas,100,kk J. Steggemann,100 B. Stieger,100M. Stoye,100 A. Tsirou,100G. I. Veres,100,tJ. R. Vlimant,100H. K. Wöhri,100W. D. Zeuner,100W. Bertl,101K. Deiters,101W. Erdmann,101 R. Horisberger,101Q. Ingram,101H. C. Kaestli,101S. König,101D. Kotlinski,101U. Langenegger,101D. Renker,101T. Rohe,101 F. Bachmair,102L. Bäni,102L. Bianchini,102P. Bortignon,102M. A. Buchmann,102B. Casal,102N. Chanon,102A. Deisher,102
G. Dissertori,102 M. Dittmar,102M. Donegà,102M. Dünser,102 P. Eller,102C. Grab,102D. Hits,102W. Lustermann,102 B. Mangano,102A. C. Marini,102 P. Martinez Ruiz del Arbol,102 D. Meister,102 N. Mohr,102C. Nägeli,102,ll P. Nef,102 F. Nessi-Tedaldi,102 F. Pandolfi,102 L. Pape,102F. Pauss,102 M. Peruzzi,102M. Quittnat,102 F. J. Ronga,102 M. Rossini,102
A. Starodumov,102,mmM. Takahashi,102 L. Tauscher,102,a K. Theofilatos,102 D. Treille,102R. Wallny,102H. A. Weber,102 C. Amsler,103,nnV. Chiochia,103 A. De Cosa,103 C. Favaro,103 A. Hinzmann,103 T. Hreus,103M. Ivova Rikova,103 B. Kilminster,103B. Millan Mejias,103J. Ngadiuba,103P. Robmann,103H. Snoek,103S. Taroni,103M. Verzetti,103Y. Yang,103
M. Cardaci,104K. H. Chen,104C. Ferro,104C. M. Kuo,104 S. W. Li,104 W. Lin,104 Y. J. Lu,104 R. Volpe,104S. S. Yu,104 P. Bartalini,105 P. Chang,105Y. H. Chang,105Y. W. Chang,105Y. Chao,105K. F. Chen,105 P. H. Chen,105C. Dietz,105
U. Grundler,105W.-S. Hou,105Y. Hsiung,105K. Y. Kao,105Y. J. Lei,105 Y. F. Liu,105R.-S. Lu,105 D. Majumder,105 E. Petrakou,105X. Shi,105J. G. Shiu,105Y. M. Tzeng,105M. Wang,105R. Wilken,105B. Asavapibhop,106N. Suwonjandee,106 A. Adiguzel,107M. N. Bakirci,107,ooS. Cerci,107,ppC. Dozen,107I. Dumanoglu,107E. Eskut,107S. Girgis,107G. Gokbulut,107
E. Gurpinar,107I. Hos,107E. E. Kangal,107A. Kayis Topaksu,107G. Onengut,107,qqK. Ozdemir,107S. Ozturk,107,oo A. Polatoz,107 K. Sogut,107,rrD. Sunar Cerci,107,pp B. Tali,107,pp H. Topakli,107,oo M. Vergili,107 I. V. Akin,108T. Aliev,108 B. Bilin,108S. Bilmis,108M. Deniz,108H. Gamsizkan,108A. M. Guler,108G. Karapinar,108,ssK. Ocalan,108A. Ozpineci,108
M. Serin,108 R. Sever,108U. E. Surat,108M. Yalvac,108M. Zeyrek,108 E. Gülmez,109B. Isildak,109,ttM. Kaya,109,uu O. Kaya,109,uuS. Ozkorucuklu,109,vvH. Bahtiyar,110,wwE. Barlas,110K. Cankocak,110Y. O. Günaydin,110,xxF. I. Vardarl
ı,110 M. Yücel,110 L. Levchuk,111 P. Sorokin,111J. J. Brooke,112E. Clement,112D. Cussans,112 H. Flacher,112R. Frazier,112
J. Goldstein,112 M. Grimes,112G. P. Heath,112H. F. Heath,112J. Jacob,112 L. Kreczko,112 C. Lucas,112Z. Meng,112 D. M. Newbold,112,yyS. Paramesvaran,112 A. Poll,112 S. Senkin,112 V. J. Smith,112 T. Williams,112A. Belyaev,113,zz C. Brew,113R. M. Brown,113D. J. A. Cockerill,113J. A. Coughlan,113K. Harder,113S. Harper,113J. Ilic,113E. Olaiya,113
D. Petyt,113C. H. Shepherd-Themistocleous,113 A. Thea,113I. R. Tomalin,113W. J. Womersley,113 S. D. Worm,113 M. Baber,114R. Bainbridge,114O. Buchmuller,114D. Burton,114D. Colling,114N. Cripps,114M. Cutajar,114P. Dauncey,114
G. Davies,114M. Della Negra,114 W. Ferguson,114 J. Fulcher,114 D. Futyan,114A. Gilbert,114A. Guneratne Bryer,114 G. Hall,114Z. Hatherell,114J. Hays,114G. Iles,114M. Jarvis,114G. Karapostoli,114M. Kenzie,114R. Lane,114R. Lucas,114,yy
L. Lyons,114 A.-M. Magnan,114J. Marrouche,114B. Mathias,114 R. Nandi,114J. Nash,114A. Nikitenko,114,mm J. Pela,114 M. Pesaresi,114K. Petridis,114M. Pioppi,114,aaaD. M. Raymond,114S. Rogerson,114A. Rose,114C. Seez,114P. Sharp,114,a
D. Cutts,119Z. Demiragli,119A. Ferapontov,119A. Garabedian,119U. Heintz,119S. Jabeen,119G. Kukartsev,119E. Laird,119 G. Landsberg,119M. Luk,119M. Narain,119M. Segala,119T. Sinthuprasith,119T. Speer,119 J. Swanson,119 R. Breedon,120 G. Breto,120M. Calderon De La Barca Sanchez,120S. Chauhan,120M. Chertok,120J. Conway,120R. Conway,120P. T. Cox,120 R. Erbacher,120M. Gardner,120W. Ko,120A. Kopecky,120R. Lander,120T. Miceli,120D. Pellett,120J. Pilot,120F. Ricci-Tam,120 B. Rutherford,120M. Searle,120 S. Shalhout,120 J. Smith,120 M. Squires,120M. Tripathi,120S. Wilbur,120 R. Yohay,120
V. Andreev,121 D. Cline,121R. Cousins,121S. Erhan,121 P. Everaerts,121C. Farrell,121M. Felcini,121J. Hauser,121 M. Ignatenko,121C. Jarvis,121 G. Rakness,121 P. Schlein,121,a E. Takasugi,121 V. Valuev,121M. Weber,121 J. Babb,122 R. Clare,122J. Ellison,122J. W. Gary,122G. Hanson,122J. Heilman,122P. Jandir,122F. Lacroix,122H. Liu,122O. R. Long,122
A. Luthra,122M. Malberti,122H. Nguyen,122A. Shrinivas,122J. Sturdy,122S. Sumowidagdo,122 S. Wimpenny,122 W. Andrews,123J. G. Branson,123G. B. Cerati,123S. Cittolin,123R. T. D’Agnolo,123D. Evans,123A. Holzner,123R. Kelley,123
D. Kovalskyi,123 M. Lebourgeois,123J. Letts,123I. Macneill,123S. Padhi,123C. Palmer,123 M. Pieri,123 M. Sani,123 V. Sharma,123 S. Simon,123E. Sudano,123M. Tadel,123Y. Tu,123A. Vartak,123S. Wasserbaech,123,bbbF. Würthwein,123 A. Yagil,123J. Yoo,123D. Barge,124C. Campagnari,124T. Danielson,124K. Flowers,124P. Geffert,124C. George,124F. Golf,124 J. Incandela,124C. Justus,124R. Magaña Villalba,124N. Mccoll,124V. Pavlunin,124J. Richman,124R. Rossin,124D. Stuart,124 W. To,124C. West,124A. Apresyan,125A. Bornheim,125J. Bunn,125Y. Chen,125E. Di Marco,125J. Duarte,125D. Kcira,125
A. Mott,125H. B. Newman,125C. Pena,125 C. Rogan,125M. Spiropulu,125 V. Timciuc,125 R. Wilkinson,125 S. Xie,125 R. Y. Zhu,125 V. Azzolini,126 A. Calamba,126R. Carroll,126T. Ferguson,126Y. Iiyama,126 D. W. Jang,126M. Paulini,126 J. Russ,126H. Vogel,126 I. Vorobiev,126J. P. Cumalat,127 B. R. Drell,127 W. T. Ford,127 A. Gaz,127E. Luiggi Lopez,127 U. Nauenberg,127 J. G. Smith,127 K. Stenson,127K. A. Ulmer,127S. R. Wagner,127J. Alexander,128A. Chatterjee,128 N. Eggert,128L. K. Gibbons,128W. Hopkins,128A. Khukhunaishvili,128B. Kreis,128N. Mirman,128G. Nicolas Kaufman,128 J. R. Patterson,128A. Ryd,128E. Salvati,128W. Sun,128W. D. Teo,128J. Thom,128J. Thompson,128J. Tucker,128Y. Weng,128
L. Winstrom,128 P. Wittich,128 D. Winn,129S. Abdullin,130M. Albrow,130J. Anderson,130 G. Apollinari,130 L. A. T. Bauerdick,130A. Beretvas,130 J. Berryhill,130P. C. Bhat,130 K. Burkett,130J. N. Butler,130V. Chetluru,130 H. W. K. Cheung,130F. Chlebana,130S. Cihangir,130V. D. Elvira,130I. Fisk,130J. Freeman,130Y. Gao,130E. Gottschalk,130 L. Gray,130D. Green,130S. Grünendahl,130O. Gutsche,130D. Hare,130R. M. Harris,130J. Hirschauer,130B. Hooberman,130
S. Jindariani,130 M. Johnson,130 U. Joshi,130K. Kaadze,130 B. Klima,130S. Kwan,130 J. Linacre,130D. Lincoln,130 R. Lipton,130J. Lykken,130 K. Maeshima,130 J. M. Marraffino,130V. I. Martinez Outschoorn,130 S. Maruyama,130 D. Mason,130P. McBride,130 K. Mishra,130 S. Mrenna,130 Y. Musienko,130,gg S. Nahn,130C. Newman-Holmes,130 V. O’Dell,130O. Prokofyev,130 N. Ratnikova,130 E. Sexton-Kennedy,130 S. Sharma,130 W. J. Spalding,130 L. Spiegel,130
L. Taylor,130S. Tkaczyk,130N. V. Tran,130L. Uplegger,130E. W. Vaandering,130R. Vidal,130A. Whitbeck,130J. Whitmore,130 W. Wu,130F. Yang,130J. C. Yun,130D. Acosta,131P. Avery,131D. Bourilkov,131T. Cheng,131S. Das,131M. De Gruttola,131
G. P. Di Giovanni,131 D. Dobur,131R. D. Field,131M. Fisher,131Y. Fu,131I. K. Furic,131J. Hugon,131B. Kim,131 J. Konigsberg,131 A. Korytov,131A. Kropivnitskaya,131T. Kypreos,131 J. F. Low,131K. Matchev,131 P. Milenovic,131,ccc G. Mitselmakher,131 L. Muniz,131 A. Rinkevicius,131L. Shchutska,131 N. Skhirtladze,131 M. Snowball,131 J. Yelton,131 M. Zakaria,131 V. Gaultney,132S. Hewamanage,132S. Linn,132P. Markowitz,132 G. Martinez,132J. L. Rodriguez,132 T. Adams,133A. Askew,133 J. Bochenek,133J. Chen,133B. Diamond,133J. Haas,133S. Hagopian,133 V. Hagopian,133 K. F. Johnson,133H. Prosper,133V. Veeraraghavan,133M. Weinberg,133M. M. Baarmand,134B. Dorney,134M. Hohlmann,134 H. Kalakhety,134F. Yumiceva,134M. R. Adams,135L. Apanasevich,135V. E. Bazterra,135R. R. Betts,135I. Bucinskaite,135
R. Cavanaugh,135 O. Evdokimov,135 L. Gauthier,135 C. E. Gerber,135 D. J. Hofman,135S. Khalatyan,135 P. Kurt,135 D. H. Moon,135C. O’Brien,135C. Silkworth,135P. Turner,135N. Varelas,135 U. Akgun,136 E. A. Albayrak,136,ww B. Bilki,136,dddW. Clarida,136K. Dilsiz,136F. Duru,136 M. Haytmyradov,136J.-P. Merlo,136H. Mermerkaya,136,eee A. Mestvirishvili,136A. Moeller,136J. Nachtman,136H. Ogul,136Y. Onel,136F. Ozok,136,wwS. Sen,136P. Tan,136E. Tiras,136 J. Wetzel,136T. Yetkin,136,fffK. Yi,136B. A. Barnett,137B. Blumenfeld,137S. Bolognesi,137D. Fehling,137A. V. Gritsan,137 P. Maksimovic,137C. Martin,137M. Swartz,137P. Baringer,138A. Bean,138G. Benelli,138R. P. Kenny III,138M. Murray,138 D. Noonan,138S. Sanders,138J. Sekaric,138R. Stringer,138Q. Wang,138J. S. Wood,138A. F. Barfuss,139I. Chakaberia,139 A. Ivanov,139S. Khalil,139M. Makouski,139Y. Maravin,139L. K. Saini,139S. Shrestha,139I. Svintradze,139J. Gronberg,140 D. Lange,140F. Rebassoo,140 D. Wright,140 A. Baden,141 B. Calvert,141 S. C. Eno,141J. A. Gomez,141 N. J. Hadley,141 R. G. Kellogg,141T. Kolberg,141Y. Lu,141M. Marionneau,141A. C. Mignerey,141K. Pedro,141A. Skuja,141J. Temple,141
L. Di Matteo,142V. Dutta,142G. Gomez Ceballos,142M. Goncharov,142D. Gulhan,142M. Klute,142Y. S. Lai,142Y.-J. Lee,142 A. Levin,142P. D. Luckey,142T. Ma,142C. Paus,142 D. Ralph,142C. Roland,142 G. Roland,142G. S. F. Stephans,142 F. Stöckli,142 K. Sumorok,142D. Velicanu,142 J. Veverka,142B. Wyslouch,142 M. Yang,142A. S. Yoon,142 M. Zanetti,142 V. Zhukova,142B. Dahmes,143A. De Benedetti,143A. Gude,143 S. C. Kao,143 K. Klapoetke,143Y. Kubota,143J. Mans,143
N. Pastika,143 R. Rusack,143A. Singovsky,143N. Tambe,143J. Turkewitz,143J. G. Acosta,144L. M. Cremaldi,144 R. Kroeger,144S. Oliveros,144L. Perera,144R. Rahmat,144D. A. Sanders,144D. Summers,144E. Avdeeva,145K. Bloom,145
S. Bose,145 D. R. Claes,145 A. Dominguez,145R. Gonzalez Suarez,145J. Keller,145D. Knowlton,145I. Kravchenko,145 J. Lazo-Flores,145 S. Malik,145F. Meier,145G. R. Snow,145 J. Dolen,146 A. Godshalk,146 I. Iashvili,146S. Jain,146
A. Kharchilava,146A. Kumar,146S. Rappoccio,146Z. Wan,146G. Alverson,147E. Barberis,147D. Baumgartel,147 M. Chasco,147 J. Haley,147 A. Massironi,147D. Nash,147T. Orimoto,147D. Trocino,147D. Wood,147 J. Zhang,147 A. Anastassov,148K. A. Hahn,148A. Kubik,148L. Lusito,148N. Mucia,148N. Odell,148B. Pollack,148 A. Pozdnyakov,148
M. Schmitt,148S. Stoynev,148 K. Sung,148M. Velasco,148S. Won,148D. Berry,149 A. Brinkerhoff,149 K. M. Chan,149 A. Drozdetskiy,149M. Hildreth,149C. Jessop,149D. J. Karmgard,149 N. Kellams,149J. Kolb,149K. Lannon,149W. Luo,149
S. Lynch,149 N. Marinelli,149 D. M. Morse,149 T. Pearson,149M. Planer,149R. Ruchti,149J. Slaunwhite,149N. Valls,149 M. Wayne,149 M. Wolf,149A. Woodard,149L. Antonelli,150B. Bylsma,150L. S. Durkin,150S. Flowers,150C. Hill,150 R. Hughes,150 K. Kotov,150T. Y. Ling,150 D. Puigh,150M. Rodenburg,150G. Smith,150 C. Vuosalo,150 B. L. Winer,150 H. Wolfe,150H. W. Wulsin,150E. Berry,151P. Elmer,151V. Halyo,151P. Hebda,151J. Hegeman,151A. Hunt,151P. Jindal,151 S. A. Koay,151P. Lujan,151D. Marlow,151T. Medvedeva,151M. Mooney,151J. Olsen,151P. Piroué,151X. Quan,151A. Raval,151 H. Saka,151D. Stickland,151C. Tully,151J. S. Werner,151S. C. Zenz,151 A. Zuranski,151E. Brownson,152 A. Lopez,152 H. Mendez,152J. E. Ramirez Vargas,152 E. Alagoz,153 D. Benedetti,153 G. Bolla,153 D. Bortoletto,153 M. De Mattia,153 A. Everett,153 Z. Hu,153M. Jones,153 K. Jung,153M. Kress,153 N. Leonardo,153D. Lopes Pegna,153V. Maroussov,153 P. Merkel,153D. H. Miller,153N. Neumeister,153B. C. Radburn-Smith,153I. Shipsey,153D. Silvers,153A. Svyatkovskiy,153
F. Wang,153 W. Xie,153L. Xu,153 H. D. Yoo,153J. Zablocki,153Y. Zheng,153 N. Parashar,154A. Adair,155B. Akgun,155 K. M. Ecklund,155F. J. M. Geurts,155 W. Li,155 B. Michlin,155B. P. Padley,155R. Redjimi,155 J. Roberts,155 J. Zabel,155 B. Betchart,156A. Bodek,156R. Covarelli,156P. de Barbaro,156R. Demina,156Y. Eshaq,156T. Ferbel,156A. Garcia-Bellido,156 P. Goldenzweig,156J. Han,156A. Harel,156D. C. Miner,156G. Petrillo,156D. Vishnevskiy,156M. Zielinski,156A. Bhatti,157 R. Ciesielski,157L. Demortier,157K. Goulianos,157G. Lungu,157S. Malik,157C. Mesropian,157S. Arora,158A. Barker,158
J. P. Chou,158 C. Contreras-Campana,158E. Contreras-Campana,158D. Duggan,158 D. Ferencek,158 Y. Gershtein,158 R. Gray,158E. Halkiadakis,158D. Hidas,158A. Lath,158S. Panwalkar,158M. Park,158R. Patel,158V. Rekovic,158J. Robles,158
S. Salur,158S. Schnetzer,158 C. Seitz,158 S. Somalwar,158 R. Stone,158 S. Thomas,158P. Thomassen,158M. Walker,158 K. Rose,159 S. Spanier,159Z. C. Yang,159 A. York,159O. Bouhali,160,ggg R. Eusebi,160W. Flanagan,160 J. Gilmore,160 T. Kamon,160,hhhV. Khotilovich,160V. Krutelyov,160R. Montalvo,160I. Osipenkov,160Y. Pakhotin,160A. Perloff,160J. Roe,160
A. Safonov,160 T. Sakuma,160 I. Suarez,160A. Tatarinov,160D. Toback,160N. Akchurin,161C. Cowden,161J. Damgov,161 C. Dragoiu,161P. R. Dudero,161K. Kovitanggoon,161S. Kunori,161S. W. Lee,161T. Libeiro,161I. Volobouev,161E. Appelt,162
A. G. Delannoy,162 S. Greene,162A. Gurrola,162W. Johns,162C. Maguire,162Y. Mao,162A. Melo,162M. Sharma,162 P. Sheldon,162B. Snook,162S. Tuo,162J. Velkovska,162 M. W. Arenton,163 S. Boutle,163 B. Cox,163B. Francis,163
J. Goodell,163R. Hirosky,163A. Ledovskoy,163C. Lin,163C. Neu,163J. Wood,163S. Gollapinni,164 R. Harr,164 P. E. Karchin,164C. Kottachchi Kankanamge Don,164P. Lamichhane,164D. A. Belknap,165L. Borrello,165D. Carlsmith,165
M. Cepeda,165S. Dasu,165 S. Duric,165 E. Friis,165M. Grothe,165 R. Hall-Wilton,165M. Herndon,165 A. Hervé,165 P. Klabbers,165 J. Klukas,165 A. Lanaro,165A. Levine,165R. Loveless,165A. Mohapatra,165I. Ojalvo,165T. Perry,165
G. A. Pierro,165G. Polese,165I. Ross,165A. Sakharov,165T. Sarangi,165A. Savin165 and W. H. Smith165
(CMS Collaboration)
1
Yerevan Physics Institute, Yerevan, Armenia
2
Institut für Hochenergiephysik der OeAW, Wien, Austria
3
National Centre for Particle and High Energy Physics, Minsk, Belarus
4
Universiteit Antwerpen, Antwerpen, Belgium
5
Vrije Universiteit Brussel, Brussel, Belgium
7Ghent University, Ghent, Belgium 8
Université Catholique de Louvain, Louvain-la-Neuve, Belgium
9Université de Mons, Mons, Belgium 10
Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, Brazil
11Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil 12
Universidade Estadual Paulista, Universidade Federal do ABC, São Paulo, Brazil
12aUniversidade Estadual Paulista, Brazil 12b
Universidade Federal do ABC, Brazil
13Institute for Nuclear Research and Nuclear Energy, Sofia, Bulgaria 14
University of Sofia, Sofia, Bulgaria
15Institute of High Energy Physics, Beijing, China 16
State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China
17Universidad de Los Andes, Bogota, Colombia 18
Technical University of Split, Split, Croatia
19University of Split, Split, Croatia 20
Institute Rudjer Boskovic, Zagreb, Croatia
21University of Cyprus, Nicosia, Cyprus 22
Charles University, Prague, Czech Republic
23Academy of Scientific Research and Technology of the Arab Republic of Egypt,
Egyptian Network of High Energy Physics, Cairo, Egypt
24National Institute of Chemical Physics and Biophysics, Tallinn, Estonia 25
Department of Physics, University of Helsinki, Helsinki, Finland
26Helsinki Institute of Physics, Helsinki, Finland 27
Lappeenranta University of Technology, Lappeenranta, Finland
28DSM/IRFU, CEA/Saclay, Gif-sur-Yvette, France 29
Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France
30Institut Pluridisciplinaire Hubert Curien, Université de Strasbourg, Université de Haute Alsace Mulhouse,
CNRS/IN2P3, Strasbourg, France
31Centre de Calcul de l
’Institut National de Physique Nucleaire et de Physique des Particules, CNRS/IN2P3, Villeurbanne, France
32
Université de Lyon, Université Claude Bernard Lyon 1, CNRS-IN2P3, Institut de Physique Nucléaire de Lyon, Villeurbanne, France
33Institute of High Energy Physics and Informatization, Tbilisi State University, Tbilisi, Georgia 34
RWTH Aachen University, I. Physikalisches Institut, Aachen, Germany
35RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany 36
RWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany
37Deutsches Elektronen-Synchrotron, Hamburg, Germany 38
University of Hamburg, Hamburg, Germany
39Institut für Experimentelle Kernphysik, Karlsruhe, Germany 40
Institute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, Greece
41University of Athens, Athens, Greece 42
University of Ioánnina, Ioánnina, Greece
43Wigner Research Centre for Physics, Budapest, Hungary 44
Institute of Nuclear Research ATOMKI, Debrecen, Hungary
45University of Debrecen, Debrecen, Hungary 46
National Institute of Science Education and Research, Bhubaneswar, India
47Panjab University, Chandigarh, India 48
University of Delhi, Delhi, India
49Saha Institute of Nuclear Physics, Kolkata, India 50
Bhabha Atomic Research Centre, Mumbai, India
51Tata Institute of Fundamental Research - EHEP, Mumbai, India 52
Tata Institute of Fundamental Research - HECR, Mumbai, India
53Institute for Research in Fundamental Sciences (IPM), Tehran, Iran 54
University College Dublin, Dublin, Ireland
55INFN Sezione di Bari, Università di Bari, Politecnico di Bari, Bari, Italy 55a
INFN Sezione di Bari, Italy
55bUniversità di Bari, Italy 55c
Politecnico di Bari, Italy
56INFN Sezione di Bologna, Università di Bologna, Bologna, Italy 56a
INFN Sezione di Bologna, Italy
56bUniversità di Bologna, Italy 57
57aINFN Sezione di Catania, Italy 57b
Università di Catania, Italy
57cCSFNSM, Italy 58
INFN Sezione di Firenze, Università di Firenze, Firenze, Italy
58aINFN Sezione di Firenze, Italy 58b
Università di Firenze, Italy
59INFN Laboratori Nazionali di Frascati, Frascati, Italy 60
INFN Sezione di Genova, Università di Genova, Genova, Italy
60aINFN Sezione di Genova, Italy 60b
Università di Genova, Italy
61INFN Sezione di Milano-Bicocca, Università di Milano-Bicocca, Milano, Italy 61a
INFN Sezione di Milano-Bicocca, Italy
61bUniversità di Milano-Bicocca, Italy 62
INFN Sezione di Napoli, Università di Napoli’Federico II’, Università della Basilicata (Potenza), Università G. Marconi (Roma), Napoli, Italy
62a
INFN Sezione di Napoli, Italy
62bUniversità di Napoli
’Federico II’, Italy
62c
Università della Basilicata (Potenza), Italy
62dUniversità G. Marconi (Roma), Italy 63
INFN Sezione di Padova, Università di Padova, Università di Trento (Trento), Padova, Italy
63aINFN Sezione di Padova, Italy 63b
Università di Padova, Italy
63cUniversità di Trento (Trento), Italy 64
INFN Sezione di Pavia, Università di Pavia, Pavia, Italy
64aINFN Sezione di Pavia, Italy 64b
Università di Pavia, Italy
65aNFN Sezione di Perugia, Italy 65b
Università di Perugia, Italy
66INFN Sezione di Pisa, Università di Pisa, Scuola Normale Superiore di Pisa, Pisa, Italy 66a
INFN Sezione di Pisa, Italy
66bUniversità di Pisa, Italy 66c
Scuola Normale Superiore di Pisa, Italy
67INFN Sezione di Roma, Università di Roma, Roma, Italy 67a
INFN Sezione di Roma, Italy
67bUniversità di Roma, Italy 68
INFN Sezione di Torino, Università di Torino, Università del Piemonte Orientale (Novara), Torino, Italy
68aINFN Sezione di Torino, Italy 68b
Università di Torino, Italy
68cUniversità del Piemonte Orientale (Novara), Italy 69
INFN Sezione di Trieste, Università di Trieste, Trieste, Italy
69aINFN Sezione di Trieste, Italy 69b
Università di Trieste, Italy
70Kangwon National University, Chunchon, Korea 71
Kyungpook National University, Daegu, Korea
72Chonnam National University, Institute for Universe and Elementary Particles, Kwangju, Korea 73
Korea University, Seoul, Korea
74University of Seoul, Seoul, Korea 75
Sungkyunkwan University, Suwon, Korea
76Vilnius University, Vilnius, Lithuania 77
University of Malaya Jabatan Fizik, Kuala Lumpur, Malaysia
78Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico 79
Universidad Iberoamericana, Mexico City, Mexico
80Benemerita Universidad Autonoma de Puebla, Puebla, Mexico 81
Universidad Autónoma de San Luis Potosí, San Luis Potosí, Mexico
82University of Auckland, Auckland, New Zealand 83
University of Canterbury, Christchurch, New Zealand
84National Centre for Physics, Quaid-I-Azam University, Islamabad, Pakistan 85
National Centre for Nuclear Research, Swierk, Poland
86Institute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, Poland 87
88Joint Institute for Nuclear Research, Dubna, Russia 89
Petersburg Nuclear Physics Institute, Gatchina (St. Petersburg), Russia
90Institute for Nuclear Research, Moscow, Russia 91
Institute for Theoretical and Experimental Physics, Moscow, Russia
92P.N. Lebedev Physical Institute, Moscow, Russia 93
Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow, Russia
94State Research Center of Russian Federation, Institute for High Energy Physics, Protvino, Russia 95
University of Belgrade, Faculty of Physics and Vinca Institute of Nuclear Sciences, Belgrade, Serbia
96Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain 97
Universidad Autónoma de Madrid, Madrid, Spain
98Universidad de Oviedo, Oviedo, Spain 99
Instituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, Spain
100CERN, European Organization for Nuclear Research, Geneva, Switzerland 101
Paul Scherrer Institut, Villigen, Switzerland
102Institute for Particle Physics, ETH Zurich, Zurich, Switzerland 103
Universität Zürich, Zurich, Switzerland
104National Central University, Chung-Li, Taiwan 105
National Taiwan University (NTU), Taipei, Taiwan
106Chulalongkorn University, Bangkok, Thailand 107
Cukurova University, Adana, Turkey
108Physics Department, Middle East Technical University, Ankara, Turkey 109
Bogazici University, Istanbul, Turkey
110Istanbul Technical University, Istanbul, Turkey 111
National Scientific Center, Kharkov Institute of Physics and Technology, Kharkov, Ukraine
112University of Bristol, Bristol, United Kingdom 113
Rutherford Appleton Laboratory, Didcot, United Kingdom
114Imperial College, London, United Kingdom 115
Brunel University, Uxbridge, United Kingdom
116Baylor University, Waco, USA 117
The University of Alabama, Tuscaloosa, USA
118Boston University, Boston, USA 119
Brown University, Providence, USA
120University of California, Davis, Davis, USA 121
University of California, Los Angeles, USA
122University of California, Riverside, Riverside, USA 123
University of California, San Diego, La Jolla, USA
124University of California, Santa Barbara, Santa Barbara, USA 125
California Institute of Technology, Pasadena, USA
126Carnegie Mellon University, Pittsburgh, USA 127
University of Colorado at Boulder, Boulder, USA
128Cornell University, Ithaca, USA 129
Fairfield University, Fairfield, USA
130Fermi National Accelerator Laboratory, Batavia, USA 131
University of Florida, Gainesville, USA
132Florida International University, Miami, USA 133
Florida State University, Tallahassee, USA
134Florida Institute of Technology, Melbourne, USA 135
University of Illinois at Chicago (UIC), Chicago, USA
136The University of Iowa, Iowa City, USA 137
Johns Hopkins University, Baltimore, USA
138The University of Kansas, Lawrence, USA 139
Kansas State University, Manhattan, USA
140Lawrence Livermore National Laboratory, Livermore, USA 141
University of Maryland, College Park, USA
142Massachusetts Institute of Technology, Cambridge, USA 143
University of Minnesota, Minneapolis, USA
144University of Mississippi, Oxford, USA 145
University of Nebraska-Lincoln, Lincoln, USA
146State University of New York at Buffalo, Buffalo, USA 147
148Northwestern University, Evanston, USA 149
University of Notre Dame, Notre Dame, USA
150The Ohio State University, Columbus, USA 151
Princeton University, Princeton, USA
152University of Puerto Rico, Mayaguez, USA 153
Purdue University, West Lafayette, USA
154Purdue University Calumet, Hammond, USA 155
Rice University, Houston, USA
156University of Rochester, Rochester, USA 157
The Rockefeller University, New York, USA
158Rutgers, The State University of New Jersey, Piscataway, USA 159
University of Tennessee, Knoxville, USA
160Texas A&M University, College Station, USA 161
Texas Tech University, Lubbock, USA
162Vanderbilt University, Nashville, USA 163
University of Virginia, Charlottesville, USA
164Wayne State University, Detroit, USA 165
University of Wisconsin, Madison, USA
aDeceased.
bAlso at Vienna University of Technology, Vienna, Austria.
cAlso at CERN, European Organization for Nuclear Research, Geneva, Switzerland.
dAlso at Institut Pluridisciplinaire Hubert Curien, Université de Strasbourg, Université de Haute Alsace Mulhouse, CNRS/IN2P3,
Strasbourg, France.
eAlso at National Institute of Chemical Physics and Biophysics, Tallinn, Estonia.
fAlso at Skobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, Moscow, Russia. gAlso at Universidade Estadual de Campinas, Campinas, Brazil.
hAlso at California Institute of Technology, Pasadena, USA.
iAlso at Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France. jAlso at Suez Canal University, Suez, Egypt.
kAlso at British University in Egypt, Cairo, Egypt. lAlso at Ain Shams University, Cairo, Egypt. mAlso at Cairo University, Cairo, Egypt.
nAlso at Fayoum University, El-Fayoum, Egypt. oAlso at Université de Haute Alsace, Mulhouse, France. pAlso at Joint Institute for Nuclear Research, Dubna, Russia. qAlso at Brandenburg University of Technology, Cottbus, Germany.
rAlso at The University of Kansas, Lawrence, USA.
sAlso at Institute of Nuclear Research ATOMKI, Debrecen, Hungary. tAlso at Eötvös Loránd University, Budapest, Hungary.
uAlso at Tata Institute of Fundamental Research - HECR, Mumbai, India. vAlso at King Abdulaziz University, Jeddah, Saudi Arabia.
wAlso at University of Visva-Bharati, Santiniketan, India. xAlso at University of Ruhuna, Matara, Sri Lanka. yAlso at Isfahan University of Technology, Isfahan, Iran. zAlso at Sharif University of Technology, Tehran, Iran.
aaAlso at Plasma Physics Research Center, Science and Research Branch, Islamic Azad University, Tehran, Iran. bbAlso at Università degli Studi di Siena, Siena, Italy.
ccAlso at Centre National de la Recherche Scientifique (CNRS) - IN2P3, Paris, France. ddAlso at Purdue University, West Lafayette, USA.
eeAlso at Universidad Michoacana de San Nicolas de Hidalgo, Morelia, Mexico. ffAlso at National Centre for Nuclear Research, Swierk, Poland.
ggAlso at Institute for Nuclear Research, Moscow, Russia.
hhAlso at Faculty of Physics, University of Belgrade, Belgrade, Serbia. iiAlso at Facoltà Ingegneria, Università di Roma, Roma, Italy. jjAlso at Scuola Normale e Sezione dell
’INFN, Pisa, Italy.
kkAlso at University of Athens, Athens, Greece. llAlso at Paul Scherrer Institut, Villigen, Switzerland.
