# Azimuthal Correlations within Exclusive Dijets with Large Momentum Transfer in Photon-Lead Collisions

A. Tumasyan et al.*

(CMS Collaboration)

<figure><img src="image_1.png" /></figure>

(Received 29 April 2022; revised 11 November 2022; accepted 15 February 2023; published 1 August 2023)

The structure of nucleons is multidimensional and depends on the transverse momenta, spatial geometry, and polarization of the constituent partons. Such a structure can be studied using high-energy photons produced in ultraperipheral heavy-ion collisions. The first measurement of the azimuthal angular correlations of exclusively produced events with two jets in photon-lead interactions at large momentum transfer is presented, a process that is considered to be sensitive to the underlying nuclear gluon polarization. This study uses a data sample of ultraperipheral lead-lead collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, corresponding to an integrated luminosity of 0.38 nb$^{-1}$, collected with the CMS experiment at the LHC. The measured second harmonic of the correlation between the sum and difference of the two jet transverse momentum vectors is found to be positive, and rising, as the dijet transverse momentum increases. A well-tuned model that has been successful at describing a wide range of proton scattering data from the HERA experiments fails to describe the observed correlations, suggesting the presence of gluon polarization effects.

DOI: 10.1103/PhysRevLett.131.051901

Considerable experimental and theoretical effort is being devoted to the study of the momentum distribution of gluons in nuclei [1,2]. The aim of such studies is to determine whether the distribution of low momentum gluons saturates, constituting a new state of matter. Accumulating evidence since early studies at BNL RHIC [3–6] points to a reduction of the density of low momentum gluons in heavy nuclei, as compared to the density in individual protons, at high energies. While experimental work has so far focused on one-dimensional studies, the gluon distribution is intrinsically multidimensional, depending on radial distance to the nucleus center, transverse momentum, and polarization [7].

Recent theoretical studies relate the polarization of gluons within nuclei to angular correlations of final-state jets produced in photon-hadron interactions [8–19]. The cross section for diffractive dijet production depends on the orientation of the quark-antiquark color dipole with respect to the radial distance. This orientation dependence results in an azimuthal decorrelation of the nominally back-to-back jets that comprise the dijet. The nature of gluon polarization in nuclei is of great interest, yet remains almost completely unexplored. While the gluon polarization density matrices have been theoretically classified,

estimates of the magnitude of gluon polarization effects vary widely [8–16]. Theory predicts that the distribution of elliptically polarized gluons [12] can be probed with the second Fourier moment $\langle\cos(2\Phi)\rangle$ of the distribution of the azimuthal angle $\Phi$ between the sum and the difference of the two jet transverse momentum vectors of a dijet [9]. In this approach, the observed moment measures a fundamental correlation of gluon polarizations with their transverse momenta.

After a preliminary version of the current results was shown, a calculation based on final-state radiation was found to result in a nonzero value for this harmonic, giving an alternative explanation for any observed correlations [20]. Initial-state radiation from parton showers could also lead to a decorrelation. Experimental measurements are essential to resolve the possible effects and to gain insight into the magnitude of gluon polarization within nuclei.

Photon-nucleus interactions can be produced using ultra-relativistic heavy-ion beams. At the CERN Large Hadron Collider, high-energy lead (Pb) beams produce a large flux of virtual photons that can interact with an oncoming lead nucleus [21–23], in so-called ultraperipheral heavy-ion collisions (UPCs). The CMS Collaboration has recently studied UPC exclusive vector meson photoproduction and photon-photon scattering [24–27]. The ALICE, ATLAS, and LHCb Collaborations have also recently reported on UPC measurements [28–30]. The CDF and ZEUS Collaborations have studied exclusive dijet production in proton-antiproton [31] and diffractive electron-proton collisions [32], respectively. While there are no published results on dijet production in photon-nucleus interactions, this

<footnote>*Full author list given at the end of the Letter.</footnote>

<footnote>Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.</footnote>
process has generated considerable interest in the context of
the future Electron-Ion Collider [2].

This Letter reports on the first measurement of
$\langle \cos(2\Phi) \rangle$ for exclusive dijet events produced at large
momentum transfer and with a large rapidity gap in photon-
lead collisions. In such events, the dijet and the incoming
photon are typically moving in the same direction and are
produced when the incoming photon fluctuates into a small
color dipole, in comparison to the size of the nucleus. This
dipole can then probe the interior of the Pb nucleus.
Tabulated results are provided in the HEPData record for
this analysis [33].

The central feature of the CMS apparatus is a super-
conducting solenoid of 6m internal diameter, providing a
magnetic field of 3.8 T. Within the solenoid volume are a
silicon pixel and strip tracker, a lead tungstate crystal
electromagnetic calorimeter (ECAL), and a brass and
scintillator hadron calorimeter (HCAL). ECAL provides
coverage in pseudorapidity $|\eta| < 1.48$ in a barrel region and
$1.48 < |\eta| < 3.0$ in two end cap (EE) regions, while HCAL
covers $|\eta| < 1.3$ for the barrel and $1.3 < |\eta| < 3.0$ for the
two end cap (HE) sections, respectively. Detector elements
in ECAL and HCAL are grouped into “towers.” Hadron
forward (HF) calorimeters extend the $\eta$ coverage provided
by the barrel and end cap detectors to $3.0 < |\eta| < 5.2$. The
data sample is collected with a two-level trigger system
[34]: at the hardware level, events are selected by custom
hardware processors, while a subsequent software trigger
uses fast versions of the off-line reconstruction code. 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. [35].

The analysis uses a data sample of lead-lead collisions at
$\sqrt{s_{NN}} = 5.02$ TeV corresponding to an integrated lumi-
nosity of $0.38 \text{ nb}^{-1}$ collected in fall 2015. The average
number of inelastic PbPb collisions per bunch crossing is
about 0.01. Events are selected with a dedicated trigger
designed to record a wide variety of photon-lead processes.
The hardware trigger requires a transverse energy of at least
5 GeV in any of the ECAL towers, and at least one of the
two HF calorimeters is required to not have a signal above
the noise threshold. The software-based trigger requires at
least one reconstructed track in the pixel detector. Since the
charged particle multiplicities are low, events are recon-
structed in the same way as if they were pp collisions [36].
The primary vertex is required to be within 20 cm of the
nominal center of the detector along the beam direction.

By combining information from all subdetectors, a
particle-flow (PF) algorithm [37] attempts to identify all
stable particles in an event, classifying them as electrons,
muons, photons, and charged or neutral hadrons. Jets are
reconstructed from these PF candidates using the anti-$k_T$
algorithm [38] with a distance parameter of 0.4, as
implemented in the FASTJET package [39]. The jet energy
is calibrated by applying a multiplicative factor to relate, on

average, the energy of the detector jet to that of the
corresponding generator-level particle jet (energy scale
correction). The leading (subleading) jet is required to
have a $p_T > 30(20)$ GeV.

The symmetry of the PbPb system leads to dijet events
where the jets can travel in either direction through CMS.
For the events of interest, the dijet is expected to be
predominantly in the photon direction. This is taken as
the “forward” direction. Events that have any additional jets
with $p_T > 20$ GeV in either the forward or backward
direction are rejected. While the expected yield for three
jet events is negligible, dijet events with a nonjet-related PF
candidate of more than 6 GeV in the forward hemisphere
are rejected. Events are discarded if they have an energy
deposit in any of the calorimeter towers in the forward and
backward rapidity hemispheres above the noise threshold
(3.9, 3.0 and 3.2 GeV in HF, HE and EE, respectively) [27].

Diffractive dijets are characterized by events with a
large rapidity gap. A pseudorapidity gap is defined with
$\Delta\eta^F = 2.4 - \eta_{\text{max}}$, where 2.4 is the upper limit of the
tracker and $\eta_{\text{max}}$ is the maximum pseudorapidity of any
high-purity charged track as defined in Ref. [40] and having
$p_T > 0.2$ GeV. A similar backward pseudorapidity gap
$\Delta\eta^B$ is defined for the opposite $\eta$ hemisphere. It is required
that $\Delta\eta^B > \Delta\eta^F$ and that $\Delta\eta^B$ is greater than 1.2, effectively
selecting dijet events that are located in the forward
direction with a large rapidity gap as measured using the
tracker. Finally, one of the jets must be within one unit of
pseudorapidity of the track defining the backward rapidity
gap. Event samples with the dijet detected in either hemi-
sphere of CMS are statistically independent and consistent
with each other within 1% for the $\langle \cos(2\Phi) \rangle$ value. The
samples are combined using the convention for defining the
forward direction as described above. This means that we
invert the rapidity sign for the sample having a backward
going dijet. A total of 6785 dijet events remain after
applying the above requirements.

In this analysis, the RAPGAP (version 3.303) [41]
Monte Carlo (MC) generator, which was developed to
explore electron-proton (ep) collisions, is used for com-
parisons with the experimental results, for detector accep-
tance and resolution corrections, and for studying sources
of systematic uncertainties. The exclusive dijet production
model used in RAPGAP is based on the boson-gluon fusion
process for diffractive electron-proton collisions, supple-
mented with initial and final-state parton showers. The
diffractive parton distribution functions are set to the “H1
2006 fit-A” model. Finally, the generated photon energy
spectrum has been reweighted to follow that of the
Weizsacker-Williams photon flux distribution in lead nuclei
described in Ref. [42]. The simulated events are processed
and reconstructed in the same way as the collision data.
GEANT4 [43] is used to account for the detector response.
For the simulated events, 94% have the interacting photon
and the dijet in the same hemisphere and, of these, 99%
pass the selection criteria described above.
<figure><img src="image_2.png" /><figcaption>FIG. 1. Magnitudes of the vector sum ($Q_T$) and vector difference ($P_T$) of the two jets (left). The dashed blue line illustrates the $Q_T < 25$ GeV requirement. Invariant mass (center) and rapidity (right) of the dijet candidates after all selection requirements. The lines show the RAPGAP MC generated events including detector resolution effects. The statistical uncertainties are covered by the symbol size.</figcaption></figure>

Based on the transverse momenta of the two jets relative to the beam axis, $\vec{p}_{T,1}$ and $\vec{p}_{T,2}$, the vector sum $\vec{Q}_T$ and vector difference $\vec{P}_T$ are defined, with $\vec{Q}_T = \vec{p}_{T,1} + \vec{p}_{T,2}$ and $\vec{P}_T = \frac{1}{2}(\vec{p}_{T,1} - \vec{p}_{T,2})$ [8]. Theoretical calculations have focused on the “back-to-back” regime, i.e., $P_T > Q_T$ [44]. This requirement results in the rejection of 47 events (0.7% of the sample). Figure 1 shows the distributions of dijet $Q_T$, $P_T$, invariant mass, and rapidity for both data and reconstructed MC events. The good agreement between data and MC for the invariant mass and rapidity distributions suggests that the rescaling of the photon flux from ep to PbPb is reasonable. The measured $Q_T$ distribution has its maximum at 9 GeV, which is well within the large momentum transfer regime.

To calculate the second moment of the azimuthal angle anisotropy $\langle \cos(2\Phi) \rangle$, the angle $\Phi$ is obtained from the relation $\vec{P}_T \cdot \vec{Q}_T = |\vec{p}_T||\vec{Q}_T|\cos(\Phi)$. For the angular correlation measurements, the $\vec{p}_{T,1}$ and $\vec{p}_{T,2}$ vectors used to calculate $\vec{Q}_T$ and $\vec{P}_T$ are assigned randomly to the leading and subleading jets on an event-by-event basis. The dijet angular correlations are distorted compared to the underlying distributions by the acceptance and finite resolution of the detector. To correct for these effects, an unfolding procedure is used to estimate the parton-level distributions. The TUNFOLD [45] software package with the Tikhonov regularization method is used, where the strength of the regularization parameter is determined with the L-curve scan method by minimizing the average global correlation coefficient. The response matrix is evaluated by using simulated dijet events that pass all of the analysis requirements. The unfolding of the $dN/d\Phi$ distribution is performed for five equal intervals in $0 < Q_T < 25$ GeV. The $\langle \cos(2\Phi) \rangle$ value is then calculated as a function of $Q_T$.

The following sources of systematic uncertainties on $\langle \cos(2\Phi) \rangle$ are considered: jet energy scale (JES) correction, JES nonclosure (JESNC), jet energy resolution (JER), jet $\eta$ resolution (JPR), jet azimuthal angular resolution (JAR), trigger efficiency (TR), and the purity estimation (PUR). The uncertainty in the JES is 2% for jets with $p_T$ of 20 GeV, as reported in Refs. [36,46]. After the nominal correction factors are applied, a small nonclosure remains between the generator-level JES and that of the reconstructed jets. The systematic uncertainty from this effect is estimated by applying first a residual correction to the JES in simulation and then the dedicated selection requirements. The deviation from the nominal result is taken as an estimate of the systematic uncertainty. The simulation provides a JER of 14% for 20 GeV jets, decreasing slightly as a function of jet $p_T$, consistent with Refs. [36,46]. The JAR and JPR are found to be $0.025 \pm 0.005(\text{stat})$ and $0.015 \pm 0.005(\text{stat})$, respectively, and are almost independent of $p_T$ and $\eta$ in the phase space relevant to this measurement. The uncertainties related to JER and JAR are estimated from the differences between the resolution in data and MC as done in Ref. [46]. For this estimate, the detector-level jets in the simulation are broadened in order to account for the observed resolution in data. The $\langle \cos(2\Phi) \rangle$ uncertainty related to the JPR is found to be negligible.

The uncertainty related to the purity of the signal (PUR) is estimated by varying the nominal pseudorapidity gap requirement between 0 and 2, and by varying the requirement for the minimal distance in pseudorapidity between the track defining the backward pseudorapidity gap and the nearest jet, which has a nominal value of 1.0, from 0.8 to 1.2. Increasing the threshold on the total energy of the PF candidates outside the jet cones from 6.0 to 6.6 GeV has a
<table><caption>TABLE I. Table of $\langle\cos(2\Phi)\rangle$ systematic uncertainties (abso-lute values). The individual components are discussed in the text.</caption><thead><tr><th>$Q_T$ (GeV)</th><th>JES</th><th>JESNC</th><th>JER</th><th>JAR</th><th>PUR</th><th>TR</th><th>Total</th></tr></thead><tbody><tr><td>0–5</td><td>0.018</td><td>0.004</td><td>0.002</td><td>0.004</td><td>0.002</td><td>0.004</td><td>0.019</td></tr><tr><td>5–10</td><td>0.012</td><td>0.006</td><td>0.005</td><td>0.003</td><td>0.002</td><td>0.003</td><td>0.015</td></tr><tr><td>10–15</td><td>0.010</td><td>0.008</td><td>0.007</td><td>0.002</td><td>0.002</td><td>0.001</td><td>0.014</td></tr><tr><td>15–20</td><td>0.009</td><td>0.008</td><td>0.014</td><td>0.002</td><td>0.002</td><td>0.001</td><td>0.018</td></tr><tr><td>20–25</td><td>0.005</td><td>0.018</td><td>0.056</td><td>0.001</td><td>0.002</td><td>0.002</td><td>0.059</td></tr></tbody></table>

negligible effect on the purity uncertainty. The uncertainty associated with the trigger efficiency is related to the component that requires the transverse energy in one of the ECAL towers to be larger than 5 GeV. This requirement tends to slightly increase the fraction of electromagnetic energy in the jets. To account for this effect, simulated events are weighted by the trigger efficiency as a function of jet $p_T$ on an event-by-event basis. This weighting reproduces the effect of the trigger efficiency on the measured $\langle\cos(2\Phi)\rangle$ values. The other elements forming the trigger, discussed above, are fully efficient. The uncertainties related to the calorimeter exclusivity selections and to the unfolding procedure are negligible. The various components of the $\langle\cos(2\Phi)\rangle$ distribution systematic uncertainties are summarized in Table I.

Figure 2 (left) shows the unfolded angular distribution $dN/d\Phi$ for $Q_T < 25$ GeV. The $dN/d\Phi$ distribution peaks at 0 and $\pi$, implying a positive value of $\langle\cos(2\Phi)\rangle$. This phenomenon is not a trivial acceptance effect as demonstrated by performing the analysis upon pairs of jets from different events, yielding the expected negative value of $\langle\cos(2\Phi)\rangle$ [13]. Figure 2 (right) shows that $\langle\cos(2\Phi)\rangle$ rises steadily with $Q_T$. The data have been compared to two different calculations that ignore the effect of elliptically polarized gluons. A calculation by Hatta et al. [20], which assumes soft gluon radiation from final-state jets as the dominant effect of the azimuthal anisotropy, has $\langle\cos(2\Phi)\rangle$ initially rising, but then plateauing for $Q_T > 1$ GeV. A calculation based on the RAPGAP model [41], which is tuned to HERA results, predicts that $\langle\cos(2\Phi)\rangle$ rises with $Q_T$, but overshoots the data by a factor of 3–5. The Dokshitzer-Gribov-Lipatov-Altarelli-Parisi-based initial-state parton shower in RAPGAP produces a finite transverse momentum of the incoming parton, and this leads to a decorrelation of the resulting dijet constituents. Such decorrelations are also observed in data for the azimuthal angular difference between two jets in proton-proton collisions [19] and are qualitatively described by parton shower production. The decorrelation observed here can also be driven by parton showers, but since heavy ions are involved, there could be further decorrelation effects at small Bjorken $x$, which are not simulated in RAPGAP. Such broadening of the azimuthal distribution for dijet events has been linked to gluon saturation effects when comparing

<figure><img src="image_3.png" /></figure>

<figure><img src="image_4.png" /><figcaption>FIG. 2. The unfolded $1/N_{events}dN/d\Phi$ distribution (upper) and the unfolded $\langle\cos(2\Phi)\rangle$ values as a function of $Q_T$ (lower). The corresponding distributions from the RAPGAP simulation at the generator level (blue lines) and theoretical calculation by Hatta et al. [20] for $\langle\cos(2\Phi)\rangle$ (red dashed lines) are also shown for $Q_T < 15$ GeV, consistent with the back-to-back limit in their calculation. The dijet events are found predominantly in the forward direction, with $0 < \eta_{jet} < 2.4$. Both the statistical (error bars) and systematic (green boxes) uncertainties are shown.</figcaption></figure>

proton-lead to proton-proton events [47]. The broadening claimed in this analysis corresponds to the comparison between photon-lead (data) and photon-proton (RAPGAP) interactions.

In summary, the exclusive production of two jets in photon-lead interactions with a large rapidity gap has been studied for the first time. The dijet events are characterized
by a large momentum transfer. The second harmonic of the angular correlation between the sum and difference of the two jet transverse momenta is found to be positive and rising, with dijet transverse momentum in the measured range 0–25 GeV. An *a posteriori* calculation that includes the effect of soft gluons from final-state radiation describes the average magnitude of the correlations, but does not rise with the magnitude of the dijet total momentum $Q_T$ to the extent found with the CMS data. A model [41] that has been successful at describing a wide range of proton scattering data from the HERA experiments overestimates the strength of the correlations, suggesting the presence of gluon polarization effects. This experiment calls for new theoretical calculations to quantify the theoretical implications and opens a new direction for probing the high-energy limit of strong interactions.

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 centers and personnel of the Worldwide LHC Computing Grid and other centers 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, the CMS detector, and the supporting computing infrastructure provided by the following funding agencies: BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MoST, and NSFC (China); MINCIENCIAS (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (U.S.).

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A. Tumasyan,¹ W. Adam,² T. Bergauer,² M. Dragicevic,² A. Escalante Del Valle,² R. Frühwirth,²,ᵇ M. Jeitler,²,ᵇ

N. Krammer,² L. Lechner,² D. Liko,² I. Mikulec,² F. M. Pitters,² N. Rad,² J. Schieck,²,ᵇ R. Schöfbeck,²

M. Spanring,² S. Templ,² W. Waltenberger,² C.-E. Wulz,²,ᵇ M. Zarucki,² M. R. Darwish,³,ᶜ E. A. De Wolf,³

D. Di Croce,³ T. Janssen,³ T. Kello,³,ᵈ A. Lelek,³ M. Pieters,³ H. Rejeb Sfar,³ H. Van Haevermaet,³

P. Van Mechelen,³ S. Van Putte,³ N. Van Remortel,³ F. Blekman,⁴ E. S. Bols,⁴ S. S. Chhibra,⁴ J. D'Hondt,⁴

J. De Clercq,⁴ D. Lontkovskyi,⁴ S. Lowette,⁴ I. Marchesini,⁴ S. Moortgat,⁴ A. Morton,⁴ D. Müller,⁴ Q. Python,⁴

S. Tavernier,⁴ W. Van Doninck,⁴ P. Van Mulders,⁴ D. Beghin,⁵ B. Bilin,⁵ B. Clerbaux,⁵ G. De Lentdecker,⁵

B. Dorney,⁵ L. Favart,⁵ A. Grebenyuk,⁵ A. K. Kalsi,⁵ I. Makarenko,⁵ L. Moureaux,⁵ L. Pétré,⁵ A. Popov,⁵

N. Postiau,⁵ E. Starling,⁵ L. Thomas,⁵ C. Vander Velde,⁵ P. Vanlaer,⁵ D. Vannerom,⁵ L. Wezenbeek,⁵

T. Cornelis,⁶ D. Dobur,⁶ M. Gruchala,⁶ I. Khvastunov,⁶,ᵉ M. Niedziela,⁶ C. Roskas,⁶ K. Skovpen,⁶ M. Tytgat,⁶

W. Verbeke,⁶ B. Vermassen,⁶ M. Vit,⁶ G. Bruno,⁷ F. Bury,⁷ C. Caputo,⁷ P. David,⁷ C. Delaere,⁷ M. Delcourt,⁷

I. S. Donertas,⁷ A. Giammanco,⁷ V. Lemaitre,⁷ K. Mondal,⁷ J. Prisciandaro,⁷ A. Taliercio,⁷ M. Teklishyn,⁷
P. Vischia,⁷ S. Wertz,⁷ S. Wuyckens,⁷ G. A. Alves,⁸ C. Hensel,⁸ A. Moraes,⁸ W. L. Aldá Júnior,⁹

E. Belchior Batista Das Chagas,⁹ H. Brandao Malbouisson,⁹ W. Carvalho,⁹ J. Chinellato,⁹,f E. Coelho,⁹

E. M. Da Costa,⁹ G. G. Da Silveira,⁹g D. De Jesus Damiao,⁹ S. Fonseca De Souza,⁹ J. Martins,⁹h

D. Matos Figueiredo,⁹ M. Medina Jaime,⁹,i C. Mora Herrera,⁹ L. Mundim,⁹ H. Nogima,⁹ P. Rebello Teles,⁹

L. J. Sanchez Rosas,⁹ A. Santoro,⁹ S. M. Silva Do Amaral,⁹ A. Sznajder,⁹ M. Thiel,⁹ F. Torres Da Silva De Araujo,⁹

A. Vilela Pereira,⁹ C. A. Bernardes,¹⁰ L. Calligaris,¹⁰ T. R. Fernandez Perez Tomei,¹⁰ E. M. Gregores,¹⁰

D. S. Lemos,¹⁰ P. G. Mercadante,¹⁰ S. F. Novaes,¹⁰ Sandra S. Padula,¹⁰ A. Aleksandrov,¹¹ G. Antchev,¹¹

I. Atanassov,¹¹ R. Hadjiiska,¹¹ P. Iaydjiev,¹¹ M. Misheva,¹¹ M. Rodozov,¹¹ M. Shopova,¹¹ G. Sultanov,¹¹

A. Dimitrov,¹² T. Ivanov,¹² L. Litov,¹² B. Pavlov,¹² P. Petkov,¹² A. Petrov,¹² T. Cheng,¹³ W. Fang,¹³,d Q. Guo,¹³

H. Wang,¹³ L. Yuan,¹³ M. Ahmad,¹⁴ G. Bauer,¹⁴ Z. Hu,¹⁴ Y. Wang,¹⁴ K. Yi,¹⁴,j,k E. Chapon,¹⁵ G. M. Chen,¹⁵,l

H. S. Chen,¹⁵,l M. Chen,¹⁵ T. Javaid,¹⁵,l A. Kapoor,¹⁵ D. Leggat,¹⁵ H. Liao,¹⁵ Z.-A. Liu,¹⁵,m R. Sharma,¹⁵

A. Spiezia,¹⁵ J. Tao,¹⁵ J. Thomas-Wilsker,¹⁵ J. Wang,¹⁵ H. Zhang,¹⁵ S. Zhang,¹⁵,l J. Zhao,¹⁵ A. Agapitos,¹⁶

Y. Ban,¹⁶ C. Chen,¹⁶ Q. Huang,¹⁶ A. Levin,¹⁶ Q. Li,¹⁶ M. Lu,¹⁶ X. Lyu,¹⁶ Y. Mao,¹⁶ S. J. Qian,¹⁶ D. Wang,¹⁶

Q. Wang,¹⁶ J. Xiao,¹⁶ Z. You,¹⁷ X. Gao,¹⁸,d M. Xiao,¹⁹ C. Avila,²⁰ A. Cabrera,²⁰ C. Florez,²⁰ J. Fraga,²⁰

A. Sarkar,²⁰ M. A. Segura Delgado,²⁰ J. Jaramillo,²¹ J. Mejia Guisao,²¹ F. Ramirez,²¹ J. D. Ruiz Alvarez,²¹

C. A. Salazar González,²¹ N. Vanegas Arbelaez,²¹ D. Giljanovic,²² N. Godinovic,²² D. Lelas,²² I. Puljak,²²

Z. Antunovic,²³ M. Kovac,²³ T. Sculac,²³ V. Brigljevic,²⁴ D. Ferencek,²⁴ D. Majumder,²⁴ M. Roguljic,²⁴

A. Starodumov,²⁴,n T. Susa,²⁴ M. W. Ather,²⁵ A. Attikis,²⁵ E. Erodotou,²⁵ A. Ioannou,²⁵ G. Kole,²⁵ M. Kolosova,²⁵

S. Konstantinou,²⁵ J. Mousa,²⁵ C. Nicolaou,²⁵ F. Ptochos,²⁵ P. A. Razis,²⁵ H. Rykaczewski,²⁵ H. Saka,²⁵

D. Tsiakkouri,²⁵ M. Finger,²⁶,n M. Finger Jr.,²⁶,n A. Kveton,²⁶ J. Tomsa,²⁶ E. Ayala,²⁷ E. Carrera Jarrin,²⁸

H. Abdalla,²⁹,o A. A. Abdelalim,²⁹,p,q Y. Assran,²⁹,r,s A. Lotfy,³⁰ M. A. Mahmoud,³⁰ S. Bhowmik,³¹

A. Carvalho Antunes De Oliveira,³¹ R. K. Dewanjee,³¹ K. Ehataht,³¹ M. Kadastik,³¹ M. Raidal,³¹ C. Veelken,³¹

P. Eerola,³² L. Forthomme,³² H. Kirschenmann,³² K. Osterberg,³² M. Voutilainen,³² E. Brücken,³³ F. Garcia,³³

J. Havukainen,³³ V. Karimäki,³³ M. S. Kim,³³ R. Kinnunen,³³ T. Lampén,³³ K. Lassila-Perini,³³ S. Lehti,³³

T. Lindén,³³ H. Siikonen,³³ E. Tuominen,³³ J. Tuominiemi,³³ P. Luukka,³⁴ T. Tuuva,³⁴ C. Amendola,³⁵

M. Besancon,³⁵ F. Couderc,³⁵ M. Dejardin,³⁵ D. Denegri,³⁵ J. L. Faure,³⁵ F. Ferri,³⁵ S. Ganjour,³⁵ A. Givernaud,³⁵

P. Gras,³⁵ G. Hamel de Monchenault,³⁵ P. Jarry,³⁵ B. Lenzi,³⁵ E. Locci,³⁵ J. Malcles,³⁵ J. Rander,³⁵

A. Rosowsky,³⁵ M. Ö. Sahin,³⁵ A. Savoy-Navarro,³⁵,t M. Titov,³⁵ G. B. Yu,³⁵ S. Ahuja,³⁶ F. Beaudette,³⁶

M. Bonanomi,³⁶ A. Buchot Perraguin,³⁶ P. Busson,³⁶ C. Charlot,³⁶ O. Davignon,³⁶ B. Diab,³⁶ G. Falmagne,³⁶

R. Granier de Cassagnac,³⁶ A. Hakimi,³⁶ I. Kucher,³⁶ A. Lobanov,³⁶ C. Martin Perez,³⁶ M. Nguyen,³⁶

C. Ochando,³⁶ P. Paganini,³⁶ J. Rembser,³⁶ R. Salerno,³⁶ J. B. Sauvan,³⁶ Y. Sirois,³⁶ A. Zabi,³⁶ A. Zghiche,³⁶

J.-L. Agram,³⁷,u J. Andrea,³⁷ D. Bloch,³⁷ G. Bourgatte,³⁷ J.-M. Brom,³⁷ E. C. Chabert,³⁷ C. Collard,³⁷

J.-C. Fontaine,³⁷,u D. Gelé,³⁷ U. Goerlach,³⁷ C. Grimault,³⁷ A.-C. Le Bihan,³⁷ P. Van Hove,³⁷ E. Asilar,³⁸

S. Beauceron,³⁸ C. Bernet,³⁸ G. Boudoul,³⁸ C. Camen,³⁸ A. Carle,³⁸ N. Chanon,³⁸ D. Contardo,³⁸ P. Depasse,³⁸

H. El Mamouni,³⁸ J. Fay,³⁸ S. Gascon,³⁸ M. Gouzevitch,³⁸ B. Ille,³⁸ Sa. Jain,³⁸ I. B. Laktineh,³⁸ H. Lattaud,³⁸

A. Lesauvage,³⁸ M. Lethuillier,³⁸ L. Mirabito,³⁸ K. Shchablo,³⁸ L. Torterotot,³⁸ G. Touquet,³⁸ M. Vander Donckt,³⁸

S. Viret,³⁸ I. Bagaturia,³⁹,v Z. Tsamalaidze,³⁹,n L. Feld,⁴⁰ K. Klein,⁴⁰ M. Lipinski,⁴⁰ D. Meuser,⁴⁰ A. Pauls,⁴⁰

M. P. Rauch,⁴⁰ J. Schulz,⁴⁰ M. Teroerde,⁴⁰ D. Eliseev,⁴¹ M. Erdmann,⁴¹ P. Fackeldey,⁴¹ B. Fischer,⁴¹ S. Ghosh,⁴¹

T. Hebbeker,⁴¹ K. Hoepfner,⁴¹ H. Keller,⁴¹ L. Mastrolorenzo,⁴¹ M. Merschmeyer,⁴¹ A. Meyer,⁴¹ G. Mocellin,⁴¹

S. Mondal,⁴¹ S. Mukherjee,⁴¹ D. Noll,⁴¹ A. Novak,⁴¹ T. Pook,⁴¹ A. Pozdnyakov,⁴¹ Y. Rath,⁴¹ H. Reithler,⁴¹

J. Roemer,⁴¹ A. Schmidt,⁴¹ S. C. Schuler,⁴¹ A. Sharma,⁴¹ S. Wiedenbeck,⁴¹ S. Zaleski,⁴¹ C. Dziwok,⁴² G. Flügge,⁴²

W. Haj Ahmad,⁴²,w O. Hlushchenko,⁴² T. Kress,⁴² A. Nowack,⁴² C. Pistone,⁴² O. Pooth,⁴² D. Roy,⁴² H. Sert,⁴²

A. Stahl,⁴²,x T. Ziemons,⁴² H. Aarup Petersen,⁴³ M. Aldaya Martin,⁴³ P. Asmuss,⁴³ I. Babounikau,⁴³ S. Baxter,⁴³

O. Behnke,⁴³ A. Bermúdez Martínez,⁴³ A. A. Bin Anuar,⁴³ K. Borras,⁴³,y V. Botta,⁴³ D. Brunner,⁴³

A. Campbell,⁴³ A. Cardini,⁴³ P. Connor,⁴³ S. Consuegra Rodríguez,⁴³ V. Danilov,⁴³ A. De Wit,⁴³

M. M. Deffranchis,⁴³ L. Didukh,⁴³ D. Domínguez Damiani,⁴³ G. Eckerlin,⁴³ D. Eckstein,⁴³ L. I. Estevez Banos,⁴³

E. Gallo,⁴³,z A. Geiser,⁴³ A. Giraldi,⁴³ A. Grohsjean,⁴³ M. Guthoff,⁴³ A. Harb,⁴³ A. Jafari,⁴³,aa N. Z. Jomhari,⁴³

A. Kasem,⁴³,y M. Kasemann,⁴³ H. Kaveh,⁴³ C. Kleinwort,⁴³ J. Knolle,⁴³ D. Krücker,⁴³ W. Lange,⁴³ T. Lenz,⁴³

J. Lidrych,⁴³ K. Lipka,⁴³ W. Lohmann,⁴³,bb T. Madlener,⁴³ R. Mankel,⁴³ I.-A. Melzer-Pellmann,⁴³ J. Metwally,⁴³
A. B. Meyer, 43 M. Meyer, 43 M. Missiroli, 43 J. Mnich, 43 A. Mussgiller, 43 V. Myronenko, 43 Y. Otarid, 43

D. Pérez Adán, 43 S. K. Pflitsch, 43 D. Pitzl, 43 A. Raspereza, 43 A. Saggio, 43 A. Saibel, 43 M. Savitskyi, 43 V. Scheurer, 43
C. Schwanenberger, 43 A. Singh, 43 R. E. Sosa Ricardo, 43 N. Tonon, 43 O. Turkot, 43 A. Vagnerini, 43

M. Van De Klundert, 43 R. Walsh, 43 D. Walter, 43 Y. Wen, 43 K. Wichmann, 43 C. Wissing, 43 S. Wuchterl, 43

O. Zenaiev, 43 R. Zlebcik, 43 R. Aggleton, 44 S. Bein, 44 L. Benato, 44 A. Benecke, 44 K. De Leo, 44 T. Dreyer, 44

A. Ebrahimi, 44 M. Eich, 44 F. Feindt, 44 A. Fröhlich, 44 C. Garbers, 44 E. Garutti, 44 P. Gunnellini, 44 J. Haller, 44

A. Hinzmann, 44 A. Karavdina, 44 G. Kasieczka, 44 R. Klanner, 44 R. Kogler, 44 V. Kutzner, 44 J. Lange, 44

T. Lange, 44 A. Malara, 44 C. E. N. Niemeyer, 44 A. Nigamova, 44 K. J. Pena Rodriguez, 44 O. Rieger, 44 P. Schleper, 44

S. Schumann, 44 J. Schwandt, 44 D. Schwarz, 44 J. Sonneveld, 44 H. Stadie, 44 G. Steinbrück, 44 B. Vormwald, 44

I. Zoi, 44 J. Bechtel, 45 T. Berger, 45 E. Butz, 45 R. Caspart, 45 T. Chwalek, 45 W. De Boer, 45 A. Dierlamm, 45 A. Droll, 45
K. El Morabit, 45 N. Faltermann, 45 K. Flöh, 45 M. Giffels, 45 A. Gottmann, 45 F. Hartmann, 45,x C. Heidecker, 45

U. Husemann, 45 I. Katkov, 45,n P. Keicher, 45 R. Koppenhöfer, 45 S. Maier, 45 M. Metzler, 45 S. Mitra, 45 Th. Müller, 45

M. Musich, 45 G. Quast, 45 K. Rabbertz, 45 J. Rauser, 45 D. Savoiu, 45 D. Schäfer, 45 M. Schnepf, 45 M. Schröder, 45

D. Seith, 45 I. Shvetsov, 45 H. J. Simonis, 45 R. Ulrich, 45 M. Wassmer, 45 M. Weber, 45 R. Wolf, 45 S. Wozniewski, 45
G. Anagnostou, 46 P. Asenov, 46 G. Daskalakis, 46 T. Geralis, 46 A. Kyriakis, 46 G. Paspalaki, 46 A. Stakia, 46

M. Diamantopoulou, 47 D. Karasavvas, 47 G. Karathanasis, 47 P. Kontaxakis, 47 C. K. Koraka, 47

A. Manousakis-Katsikakis, 47 A. Panagiotou, 47 I. Papavergou, 47 N. Saoulidou, 47 K. Theofilatos, 47 E. Tziaferi, 47

K. Vellidis, 47 E. Vourliotis, 47 G. Bakas, 48 K. Kousouris, 48 I. Papakrivopoulos, 48 G. Tsipolitis, 48

A. Zacharopoulou, 48 I. Evangelou, 49 C. Foudas, 49 P. Gianneios, 49 P. Katsoulis, 49 P. Kokkas, 49 K. Manitara, 49

N. Manthos, 49 I. Papadopoulos, 49 J. Strologas, 49 M. Bartók, 50,cc M. Csanád, 50 M. M. A. Gadallah, 50,dd

S. Lökös, 50,ee P. Major, 50 K. Mandal, 50 A. Mehta, 50 G. Pásztor, 50 O. Surányi, 50 G. I. Veres, 50 G. Bencze, 51

C. Hajdu, 51 D. Horvath, 51,ff F. Sikler, 51 V. Veszpremi, 51 G. Vesztergombi, 51,a,gg S. Czellar, 52 J. Karancsi, 52,cc

J. Molnar, 52 Z. Szillasi, 52 D. Teyssier, 52 P. Raics, 53 Z. L. Trocsanyi, 53 B. Ujvari, 53 T. Csorgo, 54,hh F. Nemes, 54,hh

T. Novak, 54 S. Choudhury, 55 J. R. Komaragiri, 55 D. Kumar, 55 L. Panwar, 55 P. C. Tiwari, 55 S. Bansal, 56

S. B. Beri, 56 V. Bhatnagar, 56 G. Chaudhary, 56 S. Chauhan, 56 N. Dhingra, 56,ii R. Gupta, 56 A. Kaur, 56 S. Kaur, 56
P. Kumari, 56 M. Meena, 56 K. Sandeep, 56 S. Sharma, 56 J. B. Singh, 56 A. K. Virdi, 56 A. Ahmed, 57

A. Bhardwaj, 57 B. C. Choudhary, 57 R. B. Garg, 57 M. Gola, 57 S. Keshri, 57 A. Kumar, 57 M. Naimuddin, 57

P. Priyanka, 57 K. Ranjan, 57 A. Shah, 57 M. Bharti, 58,ji R. Bhattacharya, 58 S. Bhattacharya, 58 D. Bhowmik, 58

S. Dutta, 58 S. Ghosh, 58 B. Gomber, 58,kk M. Maity, 58,ll S. Nandan, 58 P. Palit, 58 P. K. Rout, 58 G. Saha, 58 B. Sahu, 58

S. Sarkar, 58 M. Sharan, 58 B. Singh, 58,ji S. Thakur, 58,ji P. K. Behera, 59 S. C. Behera, 59 P. Kalbhor, 59 A. Muhammad, 59
R. Pradhan, 59 P. R. Pujahari, 59 A. Sharma, 59 A. K. Sikdar, 59 D. Dutta, 60 V. Kumar, 60 K. Naskar, 60,mm

P. K. Netrakanti, 60 L. M. Pant, 60 P. Shukla, 60 T. Aziz, 61 M. A. Bhat, 61 S. Dugad, 61 R. Kumar Verma, 61 G. B. Mohanty, 61

U. Sarkar, 61 S. Banerjee, 62 S. Bhattacharya, 62 S. Chatterjee, 62 R. Chudasama, 62 M. Guchait, 62 S. Karmakar, 62

S. Kumar, 62 G. Majumder, 62 K. Mazumdar, 62 S. Mukherjee, 62 D. Roy, 62 S. Bahinipati, 63,nn D. Dash, 63

C. Kar, 63 P. Mal, 63 T. Mishra, 63 V. K. Muraleedharan Nair Bindhu, 63 A. Nayak, 63,oo N. Sur, 63 S. K. Swain, 63
S. Dube, 64 B. Kansal, 64 S. Pandey, 64 A. Rane, 64 A. Rastogi, 64 S. Sharma, 64 H. Bakhshiansohi, 65,pp

M. Zeinali, 65,qq S. Chenarani, 66,rr S. M. Etesami, 66 M. Khakzad, 66 M. Mohammadi Najafabadi, 66 M. Felcini, 67
M. Grunewald, 67 M. Abbrescia, 68a,68b R. Aly, 68a,68c,p C. Aruta, 68a,68b A. Colaleo, 68a D. Creanza, 68a,68c

N. De Filippis, 68a,68c M. De Palma, 68a,68b A. Di Florio, 68a,68b A. Di Pilato, 68a,68b W. Elmetenawee, 68a,68b L. Fiore, 68a

A. Gelmi, 68a,68b M. Gul, 68a G. Iaselli, 68a,68c M. Ince, 68a,68b S. Lezki, 68a,68b G. Maggi, 68a,68c M. Maggi, 68a

I. Margjeka, 68a,68b V. Mastrapasqua, 68a,68b J. A. Merlin, 68a S. My, 68a,68b S. Nuzzo, 68a,68b A. Pompili, 68a,68b

G. Pugliese, 68a,68c A. Ranieri, 68a G. Selvaggi, 68a,68b L. Silvestris, 68a F. M. Simone, 68a,68b R. Venditti, 68a

P. Verwilligen, 68a G. Abbiendi, 69a C. Battilana, 69a,69b D. Bonacorsi, 69a,69b L. Borgonovi, 69a

S. Braibant-Giacomelli, 69a,69b R. Campanini, 69a,69b P. Capiluppi, 69a,69b A. Castro, 69a,69b F. R. Cavallo, 69a

C. Ciocca, 69a M. Cuffiani, 69a,69b G. M. Dallavalle, 69a T. Diotalevi, 69a,69b F. Fabbri, 69a A. Fanfani, 69a,69b

E. Fontanesi, 69a,69b P. Giacomelli, 69a L. Giommi, 69a,69b C. Grandi, 69a L. Guiducci, 69a,69b F. Iemmi, 69a,69b

S. Lo Meo, 69a,ss S. Marcellini, 69a G. Masetti, 69a F. L. Navarria, 69a,69b A. Perrotta, 69a F. Primavera, 69a,69b

A. M. Rossi, 69a,69b T. Rovelli, 69a,69b G. P. Siroli, 69a,69b N. Tosi, 69a S. Albergo, 70a,70b,tt S. Costa, 70a,70b,tt

A. Di Mattia, 70a R. Potenza, 70a,70b A. Tricomi, 70a,70b,tt C. Tuve, 70a,70b G. Barbagli, 71a A. Cassese, 71a
R. Ceccarelli, 71a,71b V. Ciulli, 71a,71b C. Civinini, 71a R. D'Alessandro, 71a,71b F. Fiori, 71a E. Focardi, 71a,71b

G. Latino, 71a,71b P. Lenzi, 71a,71b M. Lizzo, 71a,71b M. Meschini, 71a S. Paoletti, 71a R. Seidita, 71a,71b G. Sguazzoni, 71a

L. Viliani, 71a L. Benussi, 72 S. Bianco, 72 D. Piccolo, 72 M. Bozzo, 73a,73b F. Ferro, 73a R. Mulargia, 73a,73b

E. Robutti, 73a S. Tosi, 73a,73b A. Benaglia, 74a A. Beschi, 74a,74b F. Brivio, 74a,74b F. Cetorelli, 74a,74b V. Ciriolo, 74a,74b,x

F. De Guio, 74a,74b M. E. Dinardo, 74a,74b P. Dini, 74a S. Gennai, 74a A. Ghezzi, 74a,74b P. Govoni, 74a,74b L. Guzzi, 74a,74b

M. Malberti, 74a S. Malvezzi, 74a A. Massironi, 74a D. Menasce, 74a F. Monti, 74a,74b L. Moroni, 74a

M. Paganoni, 74a,74b D. Pedrini, 74a S. Ragazzi, 74a,74b T. Tabarelli de Fatis, 74a,74b D. Valsecchi, 74a,74b,x

D. Zuolo, 74a,74b S. Buontempo, 75a N. Cavallo, 75a,75c A. De Iorio, 75a,75b F. Fabozzi, 75a,75c F. Fienga, 75a

A. O. M. Iorio, 75a,75b L. Lista, 75a,75b S. Meola, 75a,75d,x P. Paolucci, 75a,x B. Rossi, 75a C. Sciacca, 75a,75b P. Azzi, 76a

N. Bacchetta, 76a D. Bisello, 76a,76b P. Bortignon, 76a A. Bragagnolo, 76a,76b R. Carlin, 76a,76b P. Checchia, 76a

P. De Castro Manzano, 76a T. Dorigo, 76a F. Gasparini, 76a,76b U. Gasparini, 76a,76b S. Y. Hoh, 76a,76b L. Layer, 76a,uu

M. Margoni, 76a,76b A. T. Meneguzzo, 76a,76b M. Presilla, 76a,76b P. Ronchese, 76a,76b R. Rossin, 76a,76b

F. Simonetto, 76a,76b G. Strong, 76a M. Tosi, 76a,76b H. YARAR, 76a,76b M. Zanetti, 76a,76b P. Zotto, 76a,76b

A. Zucchetta, 76a,76b G. Zumerle, 76a,76b C. Aime, 77a,77b A. Braghieri, 77a S. Calzaferri, 77a,77b D. Fiorina, 77a,77b

P. Montagna, 77a,77b S. P. Ratti, 77a,77b V. Re, 77a M. Ressegotti, 77a,77b C. Riccardi, 77a,77b P. Salvini, 77a I. Vai, 77a

P. Vitulo, 77a,77b M. Biasini, 78a,78b G. M. Bilei, 78a D. Ciangottini, 78a,78b L. Fanò, 78a,78b P. Lariccia, 78a,78b

G. Mantovani, 78a,78b V. Mariani, 78a,78b M. Menichelli, 78a F. Moscatelli, 78a A. Piccinelli, 78a,78b A. Rossi, 78a,78b

A. Santocchia, 78a,78b D. Spiga, 78a T. Tedeschi, 78a,78b K. Androsov, 79a P. Azzurri, 79a G. Bagliesi, 79a

V. Bertacchi, 79a,79c L. Bianchini, 79a T. Boccali, 79a R. Castaldi, 79a M. A. Ciocci, 79a,79b R. Dell'Orso, 79a

M. R. Di Domenico, 79a,79d S. Donato, 79a L. Giannini, 79a,79c A. Giassi, 79a M. T. Grippo, 79a F. Ligabue, 79a,79c

E. Manca, 79a,79c G. Mandorli, 79a,79c A. Messineo, 79a,79b F. Palla, 79a G. Ramirez-Sanchez, 79a,79c A. Rizzi, 79a,79b

G. Rolandi, 79a,79c S. Roy Chowdhury, 79a,79c A. Scribano, 79a N. Shafiei, 79a,79b P. Spagnolo, 79a R. Tenchini, 79a

G. Tonelli, 79a,79b N. Turini, 79a,79d A. Venturi, 79a P. G. Verdini, 79a F. Cavallari, 80a M. Cipriani, 80a,80b

D. Del Re, 80a,80b E. Di Marco, 80a M. Diemoz, 80a E. Longo, 80a,80b P. Meridiani, 80a G. Organtini, 80a,80b

F. Pandolfi, 80a R. Paramatti, 80a,80b C. Quaranta, 80a,80b S. Rahatlou, 80a,80b C. Rovelli, 80a F. Santanastasio, 80a,80b

L. Soffi, 80a,80b R. Tramontano, 80a,80b N. Amapane, 81a,81b R. Arcidiacono, 81a,81c S. Argiro, 81a,81b M. Arneodo, 81a,81c

N. Bartosik, 81a R. Bellan, 81a,81b A. Bellora, 81a,81b J. Berenguer Antequera, 81a,81b C. Biino, 81a A. Cappati, 81a,81b

N. Cartiglia, 81a S. Cometti, 81a M. Costa, 81a,81b R. Covarelli, 81a,81b N. Demaria, 81a B. Kiani, 81a,81b F. Legger, 81a

C. Mariotti, 81a S. Maselli, 81a E. Migliore, 81a,81b V. Monaco, 81a,81b E. Monteil, 81a,81b M. Monteno, 81a

M. M. Obertino, 81a,81b G. Ortona, 81a L. Pacher, 81a,81b N. Pastrone, 81a M. Pelliccioni, 81a G. L. Pinna Angioni, 81a,81b

M. Ruspa, 81a,81c R. Salvatico, 81a,81b F. Siviero, 81a,81b V. Sola, 81a A. Solano, 81a,81b D. Soldi, 81a,81b A. Staiano, 81a

M. Tornago, 81a,81b D. Trocino, 81a,81b S. Belforte, 82a V. Candelise, 82a,82b M. Casarsa, 82a F. Cossutti, 82a

A. Da Rold, 82a,82b G. Della Ricca, 82a,82b F. Vazzoler, 82a,82b S. Dogra, 83 C. Huh, 83 B. Kim, 83 D. H. Kim, 83

G. N. Kim, 83 J. Lee, 83 S. W. Lee, 83 C. S. Moon, 83 Y. D. Oh, 83 S. I. Pak, 83 B. C. Radburn-Smith, 83

S. Sekmen, 83 Y. C. Yang, 83 H. Kim, 84 D. H. Moon, 84 B. Francois, 85 T. J. Kim, 85 J. Park, 85 S. Cho, 86 S. Choi, 86

Y. Go, 86 S. Ha, 86 B. Hong, 86 B. Kim, 86 K. Lee, 86 K. S. Lee, 86 J. Lim, 86 J. Park, 86 S. K. Park, 86 J. Yoo, 86 J. Goh, 87

A. Gurtu, 87 H. S. Kim, 88 Y. Kim, 88 J. Almond, 89 J. H. Bhyun, 89 J. Choi, 89 S. Jeon, 89 J. Kim, 89 J. S. Kim, 89 S. Ko, 89

H. Kwon, 89 H. Lee, 89 K. Lee, 89 S. Lee, 89 K. Nam, 89 B. H. Oh, 89 M. Oh, 89 S. B. Oh, 89 H. Seo, 89 U. K. Yang, 89

I. Yoon, 89 D. Jeon, 90 J. H. Kim, 90 B. Ko, 90 J. S. H. Lee, 90 I. C. Park, 90 Y. Roh, 90 D. Song, 90 I. J. Watson, 90

H. D. Yoo, 91 Y. Choi, 92 C. Hwang, 92 Y. Jeong, 92 H. Lee, 92 Y. Lee, 92 I. Yu, 92 Y. Maghrbi, 93 V. Veckalns, 94

A. Juodagalvis, 95 A. Rinkevicius, 95 G. Tamulaitis, 95 A. Vaitkevicius, 95 W. A. T. Wan Abdullah, 96 M. N. Yusli, 96

Z. Zolkapli, 96 J. F. Benitez, 97 A. Castaneda Hernandez, 97 J. A. Murillo Quijada, 97 L. Valencia Palomo, 97

G. Ayala, 98 H. Castilla-Valdez, 98 E. De La Cruz-Burelo, 98 I. Heredia-De La Cruz, 98,yy R. Lopez-Fernandez, 98

C. A. Mondragon Herrera, 98 D. A. Perez Navarro, 98 A. Sánchez Hernández, 98 S. Carrillo Moreno, 99

C. Oropeza Barrera, 99 M. Ramírez García, 99 F. Vazquez Valencia, 99 J. Eysermans, 100 I. Pedraza, 100

H. A. Salazar Ibarguen, 100 C. Uribe Estrada, 100 A. Morelos Pineda, 101 J. Mijuskovic, 102,e N. Raicevic, 102

D. Krofcheck, 103 S. Bheesette, 104 P. H. Butler, 104 A. Ahmad, 105 M. I. Asghar, 105 A. Awais, 105 M. I. M. Awan, 105

H. R. Hoorani, 105 W. A. Khan, 105 M. A. Shah, 105 M. Shoaib, 105 M. Waqas, 105 V. Avati, 106 L. Grzanka, 106

M. Malawski, 106 H. Bialkowska, 107 M. Bluj, 107 B. Boimska, 107 T. Frueboes, 107 M. Górski, 107 M. Kazana, 107
M. Szleper,¹⁰⁷ P. Traczyk,¹⁰⁷ P. Zalewski,¹⁰⁷ K. Bunkowski,¹⁰⁸ K. Doroba,¹⁰⁸ A. Kalinowski,¹⁰⁸ M. Konecki,¹⁰⁸

J. Krolikowski,¹⁰⁸ M. Walczak,¹⁰⁸ M. Araujo,¹⁰⁹ P. Bargassa,¹⁰⁹ D. Bastos,¹⁰⁹ A. Boletti,¹⁰⁹ P. Faccioli,¹⁰⁹

M. Gallinaro,¹⁰⁹ J. Hollar,¹⁰⁹ N. Leonardo,¹⁰⁹ T. Niknejad,¹⁰⁹ J. Seixas,¹⁰⁹ K. Shchelina,¹⁰⁹ O. Toldaiev,¹⁰⁹

J. Varela,¹⁰⁹ P. Adzic,¹¹⁰,ww M. Dordevic,¹¹⁰ P. Milenovic,¹¹⁰ J. Milosevic,¹¹⁰ M. Aguilar-Benitez,¹¹¹

J. Alcaraz Maestre,¹¹¹ A. Álvarez Fernández,¹¹¹ I. Bachiller,¹¹¹ M. Barrio Luna,¹¹¹ C. F. Bedoya,¹¹¹

C. A. Carrillo Montoya,¹¹¹ M. Cepeda,¹¹¹ M. Cerrada,¹¹¹ N. Colino,¹¹¹ B. De La Cruz,¹¹¹ A. Delgado Peris,¹¹¹

J. P. Fernández Ramos,¹¹¹ J. Flix,¹¹¹ M. C. Fouz,¹¹¹ O. Gonzalez Lopez,¹¹¹ S. Goy Lopez,¹¹¹ J. M. Hernandez,¹¹¹

M. I. Josa,¹¹¹ J. León Holgado,¹¹¹ D. Moran,¹¹¹ Á. Navarro Tobar,¹¹¹ A. Pérez-Calero Yzquierdo,¹¹¹

J. Puerta Pelayo,¹¹¹ I. Redondo,¹¹¹ L. Romero,¹¹¹ S. Sánchez Navas,¹¹¹ M. S. Soares,¹¹¹ L. Urda Gómez,¹¹¹

C. Willmott,¹¹¹ C. Albajar,¹¹² J. F. de Trocóniz,¹¹² R. Reyes-Almanza,¹¹² B. Alvarez Gonzalez,¹¹³ J. Cuevas,¹¹³

C. Erice,¹¹³ J. Fernandez Menendez,¹¹³ S. Folgueras,¹¹³ I. Gonzalez Caballero,¹¹³ E. Palencia Cortezon,¹¹³

C. Ramón Álvarez,¹¹³ J. Ripoll Sau,¹¹³ V. Rodríguez Bouza,¹¹³ S. Sanchez Cruz,¹¹³ A. Trapote,¹¹³

J. A. Brochero Cifuentes,¹¹⁴ I. J. Cabrillo,¹¹⁴ A. Calderon,¹¹⁴ B. Chazin Quero,¹¹⁴ J. Duarte Campderros,¹¹⁴

M. Fernandez,¹¹⁴ P. J. Fernández Manteca,¹¹⁴ A. García Alonso,¹¹⁴ G. Gomez,¹¹⁴ C. Martinez Rivero,¹¹⁴

P. Martinez Ruiz del Arbol,¹¹⁴ F. Matorras,¹¹⁴ J. Piedra Gomez,¹¹⁴ C. Prieels,¹¹⁴ F. Ricci-Tam,¹¹⁴ T. Rodrigo,¹¹⁴

A. Ruiz-Jimeno,¹¹⁴ L. Scodellaro,¹¹⁴ I. Vila,¹¹⁴ J. M. Vizan Garcia,¹¹⁴ M. K. Jayananda,¹¹⁵ B. Kailasapathy,¹¹⁵,xx

D. U. J. Sonnadara,¹¹⁵ D. D. C. Wickramarathna,¹¹⁵ W. G. D. Dharmaratna,¹¹⁶ K. Liyanage,¹¹⁶ N. Perera,¹¹⁶

N. Wickramage,¹¹⁶ T. K. Aarrestad,¹¹⁷ D. Abbaneo,¹¹⁷ E. Auffray,¹¹⁷ G. Auzinger,¹¹⁷ J. Baechler,¹¹⁷ P. Baillon,¹¹⁷

A. H. Ball,¹¹⁷ D. Barney,¹¹⁷ J. Bendavid,¹¹⁷ N. Beni,¹¹⁷ M. Bianco,¹¹⁷ A. Bocci,¹¹⁷ E. Bossini,¹¹⁷

E. Brondolin,¹¹⁷ T. Camporesi,¹¹⁷ M. Capeans Garrido,¹¹⁷ G. Cerminara,¹¹⁷ L. Cristella,¹¹⁷ D. d'Enterria,¹¹⁷

A. Dabrowski,¹¹⁷ N. Daci,¹¹⁷ A. David,¹¹⁷ A. De Roeck,¹¹⁷ M. Deile,¹¹⁷ R. Di Maria,¹¹⁷ M. Dobson,¹¹⁷

M. Dünser,¹¹⁷ N. Dupont,¹¹⁷ A. Elliott-Peisert,¹¹⁷ N. Emriskova,¹¹⁷ F. Fallavollita,¹¹⁷,yy D. Fasanella,¹¹⁷ S. Fiorendi,¹¹⁷

A. Florent,¹¹⁷ G. Franzoni,¹¹⁷ J. Fulcher,¹¹⁷ W. Funk,¹¹⁷ S. Giani,¹¹⁷ D. Gigi,¹¹⁷ K. Gill,¹¹⁷ F. Glege,¹¹⁷

L. Gouskos,¹¹⁷ M. Guilbaud,¹¹⁷ M. Haranko,¹¹⁷ J. Hegeman,¹¹⁷ Y. Iiyama,¹¹⁷ V. Innocente,¹¹⁷ T. James,¹¹⁷

P. Janot,¹¹⁷ J. Kaspar,¹¹⁷ J. Kieseler,¹¹⁷ M. Komm,¹¹⁷ N. Kratochwil,¹¹⁷ C. Lange,¹¹⁷ S. Laurila,¹¹⁷

P. Lecoq,¹¹⁷ K. Long,¹¹⁷ C. Lourenço,¹¹⁷ L. Malgeri,¹¹⁷ S. Mallios,¹¹⁷ M. Mannelli,¹¹⁷ F. Meijers,¹¹⁷

S. Mersi,¹¹⁷ E. Meschi,¹¹⁷ F. Moortgat,¹¹⁷ M. Mulders,¹¹⁷ S. Orfanelli,¹¹⁷ L. Orsini,¹¹⁷ F. Pantaleo,¹¹⁷ L. Pape,¹¹⁷

E. Perez,¹¹⁷ M. Peruzzi,¹¹⁷ A. Petrilli,¹¹⁷ G. Petrucciani,¹¹⁷ A. Pfeiffer,¹¹⁷ M. Pierini,¹¹⁷ T. Quast,¹¹⁷ D. Rabady,¹¹⁷

A. Racz,¹¹⁷ M. Rieger,¹¹⁷ M. Rovere,¹¹⁷ H. Sakulin,¹¹⁷ J. Salfeld-Nebgen,¹¹⁷ S. Scarfi,¹¹⁷ C. Schäfer,¹¹⁷

M. Selvaggi,¹¹⁷ A. Sharma,¹¹⁷ P. Silva,¹¹⁷ W. Snoeys,¹¹⁷ P. Sphicas,¹¹⁷,zz S. Summers,¹¹⁷ V. R. Tavolaro,¹¹⁷

D. Treille,¹¹⁷ A. Tsirou,¹¹⁷ G. P. Van Onsem,¹¹⁷ A. Vartak,¹¹⁷ M. Verzetti,¹¹⁷ K. A. Wozniak,¹¹⁷ W. D. Zeuner,¹¹⁷

L. Caminada,¹¹⁸,aaa W. Erdmann,¹¹⁸ R. Horisberger,¹¹⁸ Q. Ingram,¹¹⁸ H. C. Kaestli,¹¹⁸ D. Kotlinski,¹¹⁸

T. Rohe,¹¹⁸ M. Backhaus,¹¹⁹ P. Berger,¹¹⁹ A. Calandri,¹¹⁹ N. Chernyavskaya,¹¹⁹ A. De Cosa,¹¹⁹ G. Dissertori,¹¹⁹

M. Dittmar,¹¹⁹ M. Donegà,¹¹⁹ C. Dorfer,¹¹⁹ T. Gadek,¹¹⁹ T. A. Gómez Espinosa,¹¹⁹ C. Grab,¹¹⁹ D. Hits,¹¹⁹

W. Lustermann,¹¹⁹ A.-M. Lyon,¹¹⁹ R. A. Manzoni,¹¹⁹ M. T. Meinhard,¹¹⁹ F. Micheli,¹¹⁹ F. Nessi-Tedaldi,¹¹⁹

J. Niedziela,¹¹⁹ F. Pauss,¹¹⁹ V. Perovic,¹¹⁹ G. Perrin,¹¹⁹ S. Pigazzini,¹¹⁹ M. G. Ratti,¹¹⁹ M. Reichmann,¹¹⁹

C. Reissel,¹¹⁹ T. Reitenspiess,¹¹⁹ B. Ristic,¹¹⁹ D. Ruini,¹¹⁹ D. A. Sanz Becerra,¹¹⁹ M. Schönenberger,¹¹⁹

V. Stampf,¹¹⁹ J. Steggemann,¹¹⁹,bbb R. Wallny,¹¹⁹ D. H. Zhu,¹¹⁹ C. Amsler,¹²⁰,ccc C. Botta,¹²⁰ D. Brzhechko,¹²⁰

M. F. Canelli,¹²⁰ R. Del Burgo,¹²⁰ J. K. Heikkilä,¹²⁰ M. Huwiler,¹²⁰ A. Jofrehei,¹²⁰ B. Kilminster,¹²⁰

S. Leontsinis,¹²⁰ A. Macchiolo,¹²⁰ P. Meiring,¹²⁰ V. M. Mikuni,¹²⁰ U. Molinatti,¹²⁰ I. Neutelings,¹²⁰ G. Rauco,¹²⁰

A. Reimers,¹²⁰ P. Robmann,¹²⁰ K. Schweiger,¹²⁰ Y. Takahashi,¹²⁰ C. Adloff,¹²¹,ddd C. M. Kuo,¹²¹ W. Lin,¹²¹

A. Roy,¹²¹ T. Sarkar,¹²¹,ll S. S. Yu,¹²¹ L. Ceard,¹²² P. Chang,¹²² Y. Chao,¹²² K. F. Chen,¹²² P. H. Chen,¹²²

W.-S. Hou,¹²² Y. y. Li,¹²² R.-S. Lu,¹²² E. Paganis,¹²² A. Psallidas,¹²² A. Steen,¹²² E. Yazgan,¹²²

B. Asavapibhop,¹²³ C. Asawatangtrakuldee,¹²³ N. Srimanobhas,¹²³ F. Boran,¹²⁴ S. Damarseckin,¹²⁴,eee

Z. S. Demiroglu,¹²⁴ F. Dolek,¹²⁴ C. Dozen,¹²⁴,fff I. Dumanoglu,¹²⁴,ggg E. Eskut,¹²⁴ G. Gokbulut,¹²⁴ Y. Guler,¹²⁴

E. Gurpinar Guler,¹²⁴,hhh I. Hos,¹²⁴,iii C. Isik,¹²⁴ E. E. Kangal,¹²⁴,iii O. Kara,¹²⁴ A. Kayis Topaksu,¹²⁴ U. Kiminsu,¹²⁴

G. Onengut,¹²⁴ K. Ozdemir,¹²⁴,kkk A. Polatoz,¹²⁴ A. E. Simsek,¹²⁴ B. Tali,¹²⁴,lll U. G. Tok,¹²⁴ S. Turkcapar,¹²⁴

I. S. Zorbakir,¹²⁴ C. Zorbilmez,¹²⁴ B. Isildak,¹²⁵,mmm G. Karapinar,¹²⁵,nnn K. Ocalan,¹²⁵,ooo M. Yalvac,¹²⁵,ppp

B. Akgun,¹²⁶ I. O. Atakisi,¹²⁶ E. Gülmez,¹²⁶ M. Kaya,¹²⁶,qqq O. Kaya,¹²⁶,rrr Ö. Özçelik,¹²⁶ S. Tekten,¹²⁶,sss
E. A. Yetkin,¹²⁶,ttt A. Cakir,¹²⁷ K. Cankocak,¹²⁷,ggg Y. Komurcu,¹²⁷ S. Sen,¹²⁷,uuu F. Aydogmus Sen,¹²⁸

S. Cerci,¹²⁸,lll B. Kaynak,¹²⁸ S. Ozkorucuklu,¹²⁸ D. Sunar Cerci,¹²⁸,lll B. Grynyov,¹²⁹ L. Levchuk,¹³⁰ E. Bhal,¹³¹

S. Bologna,¹³¹ J. J. Brooke,¹³¹ E. Clement,¹³¹ D. Cussans,¹³¹ H. Flacher,¹³¹ J. Goldstein,¹³¹ G. P. Heath,¹³¹

H. F. Heath,¹³¹ L. Kreczko,¹³¹ B. Krikler,¹³¹ S. Paramesvaran,¹³¹ T. Sakuma,¹³¹ S. Seif El Nasr-Storey,¹³¹

V. J. Smith,¹³¹ N. Stylianou,¹³¹,vvv J. Taylor,¹³¹ A. Titterton,¹³¹ K. W. Bell,¹³² A. Belyaev,¹³²,www C. Brew,¹³²

R. M. Brown,¹³² D. J. A. Cockerill,¹³² K. V. Ellis,¹³² K. Harder,¹³² S. Harper,¹³² J. Linacre,¹³² K. Manolopoulos,¹³²

D. M. Newbold,¹³² E. Olaiya,¹³² D. Petyt,¹³² T. Reis,¹³² T. Schuh,¹³² C. H. Shepherd-Themistocleous,¹³²

A. Thea,¹³² I. R. Tomalin,¹³² T. Williams,¹³² R. Bainbridge,¹³³ P. Bloch,¹³³ S. Bonomally,¹³³ J. Borg,¹³³

S. Breeze,¹³³ O. Buchmuller,¹³³ A. Bundock,¹³³ V. Cepaitis,¹³³ G. S. Chahal,¹³³,xxx D. Colling,¹³³ P. Dauncey,¹³³

G. Davies,¹³³ M. Della Negra,¹³³ G. Fedi,¹³³ G. Hall,¹³³ G. Iles,¹³³ J. Langford,¹³³ L. Lyons,¹³³

A.-M. Magnan,¹³³ S. Malik,¹³³ A. Martelli,¹³³ V. Milosevic,¹³³ J. Nash,¹³³,yyy V. Palladino,¹³³ M. Pesaresi,¹³³

D. M. Raymond,¹³³ A. Richards,¹³³ A. Rose,¹³³ E. Scott,¹³³ C. Seez,¹³³ A. Shtipliyski,¹³³ M. Stoye,¹³³ A. Tapper,¹³³

K. Uchida,¹³³ T. Virdee,¹³³,x N. Wardle,¹³³ S. N. Webb,¹³³ D. Winterbottom,¹³³ A. G. Zecchinelli,¹³³ J. E. Cole,¹³⁴

P. R. Hobson,¹³⁴ A. Khan,¹³⁴ P. Kyberd,¹³⁴ C. K. Mackay,¹³⁴ I. D. Reid,¹³⁴ L. Teodorescu,¹³⁴ S. Zahid,¹³⁴

S. Abdullin,¹³⁵ A. Brinkerhoff,¹³⁵ K. Call,¹³⁵ B. Caraway,¹³⁵ J. Dittmann,¹³⁵ K. Hatakeyama,¹³⁵

A. R. Kanuganti,¹³⁵ C. Madrid,¹³⁵ B. McMaster,¹³⁵ N. Pastika,¹³⁵ S. Sawant,¹³⁵ C. Smith,¹³⁵ J. Wilson,¹³⁵

R. Bartek,¹³⁶ A. Dominguez,¹³⁶ R. Uniyal,¹³⁶ A. M. Vargas Hernandez,¹³⁶ A. Buccilli,¹³⁷ O. Charaf,¹³⁷

S. I. Cooper,¹³⁷ S. V. Gleyzer,¹³⁷ C. Henderson,¹³⁷ C. U. Perez,¹³⁷ P. Rumerio,¹³⁷ C. West,¹³⁷ A. Akpinar,¹³⁸

A. Albert,¹³⁸ D. Arcaro,¹³⁸ C. Cosby,¹³⁸ Z. Demiragli,¹³⁸ D. Gastler,¹³⁸ J. Rohlf,¹³⁸ K. Salyer,¹³⁸ D. Sperka,¹³⁸

D. Spitzbart,¹³⁸ I. Suarez,¹³⁸ S. Yuan,¹³⁸ D. Zou,¹³⁸ G. Benelli,¹³⁹ B. Burkle,¹³⁹ X. Coubez,¹³⁹,y D. Cutts,¹³⁹

Y. t. Duh,¹³⁹ M. Hadley,¹³⁹ U. Heintz,¹³⁹ J. M. Hogan,¹³⁹,zzz K. H. M. Kwok,¹³⁹ E. Laird,¹³⁹ G. Landsberg,¹³⁹

K. T. Lau,¹³⁹ J. Lee,¹³⁹ M. Narain,¹³⁹ S. Sagir,¹³⁹,aaaa R. Syarif,¹³⁹ E. Usai,¹³⁹ W. Y. Wong,¹³⁹ D. Yu,¹³⁹

W. Zhang,¹³⁹ R. Band,¹⁴⁰ C. Brainerd,¹⁴⁰ R. Breedon,¹⁴⁰ M. Calderon De La Barca Sanchez,¹⁴⁰ M. Chertok,¹⁴⁰

J. Conway,¹⁴⁰ R. Conway,¹⁴⁰ P. T. Cox,¹⁴⁰ R. Erbacher,¹⁴⁰ C. Flores,¹⁴⁰ G. Funk,¹⁴⁰ F. Jensen,¹⁴⁰ W. Ko,¹⁴⁰,a

O. Kukral,¹⁴⁰ R. Lander,¹⁴⁰ M. Mulhearn,¹⁴⁰ D. Pellett,¹⁴⁰ J. Pilot,¹⁴⁰ M. Shi,¹⁴⁰ D. Taylor,¹⁴⁰ K. Tos,¹⁴⁰

M. Tripathi,¹⁴⁰ Y. Yao,¹⁴⁰ F. Zhang,¹⁴⁰ M. Bachtis,¹⁴¹ R. Cousins,¹⁴¹ A. Dasgupta,¹⁴¹ D. Hamilton,¹⁴¹

J. Hauser,¹⁴¹ M. Ignatenko,¹⁴¹ M. A. Iqbal,¹⁴¹ T. Lam,¹⁴¹ N. Mccoll,¹⁴¹ W. A. Nash,¹⁴¹ S. Regnard,¹⁴¹

D. Saltzberg,¹⁴¹ C. Schnaible,¹⁴¹ B. Stone,¹⁴¹ V. Valuev,¹⁴¹ K. Burt,¹⁴² Y. Chen,¹⁴² R. Clare,¹⁴² J. W. Gary,¹⁴²

G. Hanson,¹⁴² G. Karapostoli,¹⁴² O. R. Long,¹⁴² N. Manganelli,¹⁴² M. Olmedo Negrete,¹⁴² W. Si,¹⁴²

S. Wimpenny,¹⁴² Y. Zhang,¹⁴² J. G. Branson,¹⁴³ P. Chang,¹⁴³ S. Cittolin,¹⁴³ S. Cooperstein,¹⁴³ N. Deelen,¹⁴³

J. Duarte,¹⁴³ R. Gerosa,¹⁴³ D. Gilbert,¹⁴³ V. Krutelyov,¹⁴³ J. Letts,¹⁴³ M. Masciovecchio,¹⁴³ S. May,¹⁴³

S. Padhi,¹⁴³ M. Pieri,¹⁴³ V. Sharma,¹⁴³ M. Tadel,¹⁴³ F. Würthwein,¹⁴³ A. Yagil,¹⁴³ N. Amin,¹⁴⁴ C. Campagnari,¹⁴⁴

M. Citron,¹⁴⁴ A. Dorsett,¹⁴⁴ V. Dutta,¹⁴⁴ J. Incandela,¹⁴⁴ B. Marsh,¹⁴⁴ H. Mei,¹⁴⁴ A. Ovcharova,¹⁴⁴ H. Qu,¹⁴⁴

M. Quinnan,¹⁴⁴ J. Richman,¹⁴⁴ U. Sarica,¹⁴⁴ D. Stuart,¹⁴⁴ S. Wang,¹⁴⁴ A. Bornheim,¹⁴⁵ O. Cerri,¹⁴⁵ I. Dutta,¹⁴⁵

J. M. Lawhorn,¹⁴⁵ N. Lu,¹⁴⁵ J. Mao,¹⁴⁵ H. B. Newman,¹⁴⁵ J. Ngadiuba,¹⁴⁵ T. Q. Nguyen,¹⁴⁵ J. Pata,¹⁴⁵

M. Spiropulu,¹⁴⁵ J. R. Vlimant,¹⁴⁵ C. Wang,¹⁴⁵ S. Xie,¹⁴⁵ Z. Zhang,¹⁴⁵ R. Y. Zhu,¹⁴⁵ J. Alison,¹⁴⁶

M. B. Andrews,¹⁴⁶ T. Ferguson,¹⁴⁶ T. Mudholkar,¹⁴⁶ M. Paulini,¹⁴⁶ I. Vorobiev,¹⁴⁶ J. P. Cumalat,¹⁴⁷ W. T. Ford,¹⁴⁷

E. MacDonald,¹⁴⁷ R. Patel,¹⁴⁷ A. Perloff,¹⁴⁷ K. Stenson,¹⁴⁷ K. A. Ulmer,¹⁴⁷ S. R. Wagner,¹⁴⁷ J. Alexander,¹⁴⁸

Y. Cheng,¹⁴⁸ J. Chu,¹⁴⁸ D. J. Cranshaw,¹⁴⁸ A. Datta,¹⁴⁸ A. Frankenthal,¹⁴⁸ K. Mcdermott,¹⁴⁸ J. Monroy,¹⁴⁸

J. R. Patterson,¹⁴⁸ D. Quach,¹⁴⁸ A. Ryd,¹⁴⁸ W. Sun,¹⁴⁸ S. M. Tan,¹⁴⁸ Z. Tao,¹⁴⁸ J. Thom,¹⁴⁸ P. Wittich,¹⁴⁸

M. Zientek,¹⁴⁸ M. Albrow,¹⁴⁹ M. Alyari,¹⁴⁹ G. Apollinari,¹⁴⁹ A. Apresyan,¹⁴⁹ A. Apyan,¹⁴⁹ S. Banerjee,¹⁴⁹

L. A. T. Bauerdick,¹⁴⁹ A. Beretvas,¹⁴⁹ D. Berry,¹⁴⁹ J. Berryhill,¹⁴⁹ P. C. Bhat,¹⁴⁹ K. Burkett,¹⁴⁹ J. N. Butler,¹⁴⁹

A. Canepa,¹⁴⁹ G. B. Cerati,¹⁴⁹ H. W. K. Cheung,¹⁴⁹ F. Chlebana,¹⁴⁹ M. Cremonesi,¹⁴⁹ V. D. Elvira,¹⁴⁹

J. Freeman,¹⁴⁹ Z. Gecse,¹⁴⁹ L. Gray,¹⁴⁹ D. Green,¹⁴⁹ S. Grünendahl,¹⁴⁹ O. Gutsche,¹⁴⁹ R. M. Harris,¹⁴⁹

S. Hasegawa,¹⁴⁹ R. Heller,¹⁴⁹ T. C. Herwig,¹⁴⁹ J. Hirschauer,¹⁴⁹ B. Jayatilaka,¹⁴⁹ S. Jindariani,¹⁴⁹ M. Johnson,¹⁴⁹

U. Joshi,¹⁴⁹ P. Klabbers,¹⁴⁹ T. Klijnsma,¹⁴⁹ B. Klima,¹⁴⁹ M. J. Kortelainen,¹⁴⁹ S. Lammel,¹⁴⁹ D. Lincoln,¹⁴⁹

R. Lipton,¹⁴⁹ M. Liu,¹⁴⁹ T. Liu,¹⁴⁹ J. Lykken,¹⁴⁹ K. Maeshima,¹⁴⁹ D. Mason,¹⁴⁹ P. McBride,¹⁴⁹ P. Merkel,¹⁴⁹

S. Mrenna,¹⁴⁹ S. Nahn,¹⁴⁹ V. O'Dell,¹⁴⁹ V. Papadimitriou,¹⁴⁹ K. Pedro,¹⁴⁹ C. Pena,¹⁴⁹,bbbb O. Prokofyev,¹⁴⁹

F. Ravera,¹⁴⁹ A. Reinsvold Hall,¹⁴⁹ L. Ristori,¹⁴⁹ B. Schneider,¹⁴⁹ E. Sexton-Kennedy,¹⁴⁹ N. Smith,¹⁴⁹
A. Soha,¹⁴⁹ W. J. Spalding,¹⁴⁹ L. Spiegel,¹⁴⁹ J. Strait,¹⁴⁹ L. Taylor,¹⁴⁹ S. Tkaczyk,¹⁴⁹ N. V. Tran,¹⁴⁹

L. Uplegger,¹⁴⁹ E. W. Vaandering,¹⁴⁹ H. A. Weber,¹⁴⁹ A. Woodard,¹⁴⁹ D. Acosta,¹⁵⁰ P. Avery,¹⁵⁰

D. Bourilkov,¹⁵⁰ L. Cadamuro,¹⁵⁰ V. Cherepanov,¹⁵⁰ F. Errico,¹⁵⁰ R. D. Field,¹⁵⁰ D. Guerrero,¹⁵⁰ B. M. Joshi,¹⁵⁰

M. Kim,¹⁵⁰ J. Konigsberg,¹⁵⁰ A. Korytov,¹⁵⁰ K. H. Lo,¹⁵⁰ K. Matchev,¹⁵⁰ N. Menendez,¹⁵⁰ G. Mitselmakher,¹⁵⁰

D. Rosenzweig,¹⁵⁰ K. Shi,¹⁵⁰ J. Sturdy,¹⁵⁰ J. Wang,¹⁵⁰ X. Zuo,¹⁵⁰ T. Adams,¹⁵¹ A. Askew,¹⁵¹ D. Diaz,¹⁵¹

R. Habibullah,¹⁵¹ S. Hagopian,¹⁵¹ V. Hagopian,¹⁵¹ K. F. Johnson,¹⁵¹ R. Khurana,¹⁵¹ T. Kolberg,¹⁵¹ G. Martinez,¹⁵¹

H. Prosper,¹⁵¹ C. Schiber,¹⁵¹ R. Yohay,¹⁵¹ J. Zhang,¹⁵¹ M. M. Baarmand,¹⁵² S. Butalla,¹⁵² T. Elkafrawy,¹⁵², cccccc
M. Hohlmann,¹⁵² D. Noonan,¹⁵² M. Rahmani,¹⁵² M. Saunders,¹⁵² F. Yumiceva,¹⁵² M. R. Adams,¹⁵³

L. Apanasevich,¹⁵³ H. Becerril Gonzalez,¹⁵³ R. Cavanaugh,¹⁵³ X. Chen,¹⁵³ S. Dittmer,¹⁵³ O. Evdokimov,¹⁵³

C. E. Gerber,¹⁵³ D. A. Hangal,¹⁵³ D. J. Hofman,¹⁵³ C. Mills,¹⁵³ G. Oh,¹⁵³ T. Roy,¹⁵³ M. B. Tonjes,¹⁵³

N. Varelas,¹⁵³ J. Viinikainen,¹⁵³ X. Wang,¹⁵³ Z. Wu,¹⁵³ Z. Ye,¹⁵³ M. Alhusseini,¹⁵⁴ K. Dilsiz,¹⁵⁴,dddd

S. Durgut,¹⁵⁴ R. P. Gandrajula,¹⁵⁴ M. Haytmyradov,¹⁵⁴ V. Khristenko,¹⁵⁴ O. K. Köseyan,¹⁵⁴ J.-P. Merlo,¹⁵⁴

A. Mestvirishvili,¹⁵⁴, eeee A. Moeller,¹⁵⁴ J. Nachtman,¹⁵⁴ H. Ogul,¹⁵⁴, ffff Y. Onel,¹⁵⁴ F. Ozok,¹⁵⁴, gggg A. Penzo,¹⁵⁴

C. Snyder,¹⁵⁴ E. Tiras,¹⁵⁴, hhhh J. Wetzel,¹⁵⁴ O. Amram,¹⁵⁵ B. Blumenfeld,¹⁵⁵ L. Corcodilos,¹⁵⁵ M. Eminizer,¹⁵⁵

A. V. Gritsan,¹⁵⁵ S. Kyriacou,¹⁵⁵ P. Maksimovic,¹⁵⁵ C. Mantilla,¹⁵⁵ J. Roskes,¹⁵⁵ M. Swartz,¹⁵⁵ T. Á. Vámi,¹⁵⁵

C. Baldenegro Barrera,¹⁵⁶ P. Baringer,¹⁵⁶ A. Bean,¹⁵⁶ S. Boren,¹⁵⁶ J. Bowen,¹⁵⁶ A. Bylinkin,¹⁵⁶ T. Isidori,¹⁵⁶

S. Khalil,¹⁵⁶ J. King,¹⁵⁶ G. Krintiras,¹⁵⁶ A. Kropivnitskaya,¹⁵⁶ C. Lindsey,¹⁵⁶ N. Minafra,¹⁵⁶ M. Murray,¹⁵⁶

J. Ralston,¹⁵⁶ C. Rogan,¹⁵⁶ C. Royon,¹⁵⁶ S. Sanders,¹⁵⁶ E. Schmitz,¹⁵⁶ J. D. Tapia Takaki,¹⁵⁶ Q. Wang,¹⁵⁶

J. Williams,¹⁵⁶ G. Wilson,¹⁵⁶ S. Duric,¹⁵⁷ A. Ivanov,¹⁵⁷ K. Kaadze,¹⁵⁷ D. Kim,¹⁵⁷ Y. Maravin,¹⁵⁷ T. Mitchell,¹⁵⁷

A. Modak,¹⁵⁷ A. Mohammadi,¹⁵⁷ F. Rebassoo,¹⁵⁸ D. Wright,¹⁵⁸ E. Adams,¹⁵⁹ A. Baden,¹⁵⁹ O. Baron,¹⁵⁹

A. Belloni,¹⁵⁹ S. C. Eno,¹⁵⁹ Y. Feng,¹⁵⁹ N. J. Hadley,¹⁵⁹ S. Jabeen,¹⁵⁹ G. Y. Jeng,¹⁵⁹ R. G. Kellogg,¹⁵⁹

T. Koeth,¹⁵⁹ A. C. Mignerey,¹⁵⁹ S. Nabili,¹⁵⁹ M. Seidel,¹⁵⁹ A. Skuja,¹⁵⁹ S. C. Tonwar,¹⁵⁹ L. Wang,¹⁵⁹

K. Wong,¹⁵⁹ D. Abercrombie,¹⁶⁰ B. Allen,¹⁶⁰ R. Bi,¹⁶⁰ S. Brandt,¹⁶⁰ W. Busza,¹⁶⁰ I. A. Cali,¹⁶⁰ Y. Chen,¹⁶⁰

M. D'Alfonso,¹⁶⁰ G. Gomez-Ceballos,¹⁶⁰ M. Goncharov,¹⁶⁰ P. Harris,¹⁶⁰ D. Hsu,¹⁶⁰ M. Hu,¹⁶⁰ M. Klute,¹⁶⁰

D. Kovalskyi,¹⁶⁰ J. Krupa,¹⁶⁰ Y.-J. Lee,¹⁶⁰ P. D. Luckey,¹⁶⁰ B. Maier,¹⁶⁰ A. C. Marini,¹⁶⁰ C. Mironov,¹⁶⁰

S. Narayanan,¹⁶⁰ X. Niu,¹⁶⁰ C. Paus,¹⁶⁰ D. Rankin,¹⁶⁰ C. Roland,¹⁶⁰ G. Roland,¹⁶⁰ Z. Shi,¹⁶⁰

G. S. F. Stephans,¹⁶⁰ K. Sumorok,¹⁶⁰ K. Tatar,¹⁶⁰ D. Velicanu,¹⁶⁰ J. Wang,¹⁶⁰ T. W. Wang,¹⁶⁰ Z. Wang,¹⁶⁰

B. Wyslouch,¹⁶⁰ R. M. Chatterjee,¹⁶¹ A. Evans,¹⁶¹ P. Hansen,¹⁶¹ J. Hiltbrand,¹⁶¹ Sh. Jain,¹⁶¹ M. Krohn,¹⁶¹

Y. Kubota,¹⁶¹ Z. Lesko,¹⁶¹ J. Mans,¹⁶¹ M. Revering,¹⁶¹ R. Rusack,¹⁶¹ R. Saradhy,¹⁶¹ N. Schroeder,¹⁶¹

N. Strobbe,¹⁶¹ M. A. Wadud,¹⁶¹ J. G. Acosta,¹⁶² S. Oliveros,¹⁶² K. Bloom,¹⁶³ S. Chauhan,¹⁶³ D. R. Claes,¹⁶³

C. Fangmeier,¹⁶³ L. Finco,¹⁶³ F. Golf,¹⁶³ J. R. González Fernández,¹⁶³ C. Joo,¹⁶³ I. Kravchenko,¹⁶³

J. E. Siado,¹⁶³ G. R. Snow,¹⁶³, a W. Tabb,¹⁶³ F. Yan,¹⁶³ G. Agarwal,¹⁶⁴ H. Bandyopadhyay,¹⁶⁴ L. Hay,¹⁶⁴

I. Iashvili,¹⁶⁴ A. Kharchilava,¹⁶⁴ C. McLean,¹⁶⁴ D. Nguyen,¹⁶⁴ J. Pekkanen,¹⁶⁴ S. Rappoccio,¹⁶⁴ G. Alverson,¹⁶⁵

E. Barberis,¹⁶⁵ C. Freer,¹⁶⁵ Y. Haddad,¹⁶⁵ A. Hortiangtham,¹⁶⁵ J. Li,¹⁶⁵ G. Madigan,¹⁶⁵ B. Marzocchi,¹⁶⁵

D. M. Morse,¹⁶⁵ V. Nguyen,¹⁶⁵ T. Orimoto,¹⁶⁵ A. Parker,¹⁶⁵ L. Skinnari,¹⁶⁵ A. Tishelman-Charny,¹⁶⁵

T. Wamorkar,¹⁶⁵ B. Wang,¹⁶⁵ A. Wisecarver,¹⁶⁵ D. Wood,¹⁶⁵ S. Bhattacharya,¹⁶⁶ J. Bueghly,¹⁶⁶ Z. Chen,¹⁶⁶

A. Gilbert,¹⁶⁶ T. Gunter,¹⁶⁶ K. A. Hahn,¹⁶⁶ N. Odell,¹⁶⁶ M. H. Schmitt,¹⁶⁶ K. Sung,¹⁶⁶ M. Velasco,¹⁶⁶ R. Bucci,¹⁶⁷

N. Dev,¹⁶⁷ R. Goldouzian,¹⁶⁷ M. Hildreth,¹⁶⁷ K. Hurtado Anampa,¹⁶⁷ C. Jessop,¹⁶⁷ K. Lannon,¹⁶⁷ N. Loukas,¹⁶⁷

N. Marinelli,¹⁶⁷ I. Mcalister,¹⁶⁷ F. Meng,¹⁶⁷ K. Mohrman,¹⁶⁷ Y. Musienko,¹⁶⁷, n R. Ruchti,¹⁶⁷ P. Siddireddy,¹⁶⁷

M. Wayne,¹⁶⁷ A. Wightman,¹⁶⁷ M. Wolf,¹⁶⁷ L. Zygala,¹⁶⁷ J. Alimena,¹⁶⁸ B. Bylsma,¹⁶⁸ B. Cardwell,¹⁶⁸

L. S. Durkin,¹⁶⁸ B. Francis,¹⁶⁸ C. Hill,¹⁶⁸ A. Lefeld,¹⁶⁸ B. L. Winer,¹⁶⁸ B. R. Yates,¹⁶⁸ B. Bonham,¹⁶⁹ P. Das,¹⁶⁹

G. Dezoort,¹⁶⁹ P. Elmer,¹⁶⁹ B. Greenberg,¹⁶⁹ N. Haubrich,¹⁶⁹ S. Higginbotham,¹⁶⁹ A. Kalogeropoulos,¹⁶⁹

G. Kopp,¹⁶⁹ S. Kwan,¹⁶⁹ D. Lange,¹⁶⁹ M. T. Lucchini,¹⁶⁹ J. Luo,¹⁶⁹ D. Marlow,¹⁶⁹ K. Mei,¹⁶⁹ I. Ojalvo,¹⁶⁹

J. Olsen,¹⁶⁹ C. Palmer,¹⁶⁹ P. Piroué,¹⁶⁹ D. Stickland,¹⁶⁹ C. Tully,¹⁶⁹ S. Malik,¹⁷⁰ S. Norberg,¹⁷⁰ V. E. Barnes,¹⁷¹

R. Chawla,¹⁷¹ S. Das,¹⁷¹ L. Gutay,¹⁷¹ M. Jones,¹⁷¹ A. W. Jung,¹⁷¹ G. Negro,¹⁷¹ N. Neumeister,¹⁷¹ C. C. Peng,¹⁷¹

S. Piperov,¹⁷¹ A. Purohit,¹⁷¹ J. F. Schulte,¹⁷¹ M. Stojanovic,¹⁷¹ N. Trevisani,¹⁷¹ F. Wang,¹⁷¹ A. Wildridge,¹⁷¹

R. Xiao,¹⁷¹ W. Xie,¹⁷¹ J. Dolen,¹⁷² N. Parashar,¹⁷² A. Baty,¹⁷³ S. Dildick,¹⁷³ K. M. Ecklund,¹⁷³ S. Freed,¹⁷³

F. J. M. Geurts,¹⁷³ M. Kilpatrick,¹⁷³ A. Kumar,¹⁷³ W. Li,¹⁷³ B. P. Padley,¹⁷³ R. Redjimi,¹⁷³ J. Roberts,¹⁷³, a

J. Rorie,¹⁷³ W. Shi,¹⁷³ A. G. Stahl Leiton,¹⁷³ A. Bodek,¹⁷⁴ P. de Barbaro,¹⁷⁴ R. Demina,¹⁷⁴ J. L. Dulemba,¹⁷⁴
C. Fallon,¹⁷⁴ T. Ferbel,¹⁷⁴ M. Galanti,¹⁷⁴ A. Garcia-Bellido,¹⁷⁴ O. Hindrichs,¹⁷⁴ A. Khukhunaishvili,¹⁷⁴

E. Ranken,¹⁷⁴ R. Taus,¹⁷⁴ B. Chiarito,¹⁷⁵ J. P. Chou,¹⁷⁵ A. Gandrakota,¹⁷⁵ Y. Gershtein,¹⁷⁵ E. Halkiadakis,¹⁷⁵

A. Hart,¹⁷⁵ M. Heindl,¹⁷⁵ E. Hughes,¹⁷⁵ S. Kaplan,¹⁷⁵ O. Karacheban,¹⁷⁵,bb I. Laflotte,¹⁷⁵ A. Lath,¹⁷⁵

R. Montalvo,¹⁷⁵ K. Nash,¹⁷⁵ M. Osherson,¹⁷⁵ S. Salur,¹⁷⁵ S. Schnetzer,¹⁷⁵ S. Somalwar,¹⁷⁵ R. Stone,¹⁷⁵

S. A. Thayil,¹⁷⁵ S. Thomas,¹⁷⁵ H. Wang,¹⁷⁵ H. Acharya,¹⁷⁶ A. G. Delannoy,¹⁷⁶ S. Spanier,¹⁷⁶ O. Bouhali,¹⁷⁷,iiii

M. Dalchenko,¹⁷⁷ A. Delgado,¹⁷⁷ R. Eusebi,¹⁷⁷ J. Gilmore,¹⁷⁷ T. Huang,¹⁷⁷ T. Kamon,¹⁷⁷,iiii H. Kim,¹⁷⁷

S. Luo,¹⁷⁷ S. Malhotra,¹⁷⁷ R. Mueller,¹⁷⁷ D. Overton,¹⁷⁷ L. Perniè,¹⁷⁷ D. Rathjens,¹⁷⁷ A. Safonov,¹⁷⁷

N. Akchurin,¹⁷⁸ J. Damgov,¹⁷⁸ V. Hegde,¹⁷⁸ S. Kunori,¹⁷⁸ K. Lamichhane,¹⁷⁸ S. W. Lee,¹⁷⁸ T. Mengke,¹⁷⁸

S. Muthumuni,¹⁷⁸ T. Peltola,¹⁷⁸ S. Undleeb,¹⁷⁸ I. Volobouev,¹⁷⁸ Z. Wang,¹⁷⁸ A. Whitbeck,¹⁷⁸ E. Appelt,¹⁷⁹

S. Greene,¹⁷⁹ A. Gurrola,¹⁷⁹ R. Janjam,¹⁷⁹ W. Johns,¹⁷⁹ C. Maguire,¹⁷⁹ A. Melo,¹⁷⁹ H. Ni,¹⁷⁹ K. Padeken,¹⁷⁹

F. Romeo,¹⁷⁹ P. Sheldon,¹⁷⁹ S. Tuo,¹⁷⁹ J. Velkovska,¹⁷⁹ M. W. Arenton,¹⁸⁰ B. Cox,¹⁸⁰ G. Cummings,¹⁸⁰

J. Hakala,¹⁸⁰ R. Hirosky,¹⁸⁰ M. Joyce,¹⁸⁰ A. Ledovskoy,¹⁸⁰ A. Li,¹⁸⁰ C. Neu,¹⁸⁰ B. Tannenwald,¹⁸⁰

E. Wolfe,¹⁸⁰ P. E. Karchin,¹⁸¹ N. Poudyal,¹⁸¹ P. Thapa,¹⁸¹ K. Black,¹⁸² T. Bose,¹⁸² J. Buchanan,¹⁸² C. Caillol,¹⁸²

S. Dasu,¹⁸² I. De Bruyn,¹⁸² P. Everaerts,¹⁸² C. Galloni,¹⁸² H. He,¹⁸² M. Herndon,¹⁸² A. Hervé,¹⁸² U. Hussain,¹⁸²

A. Lanaro,¹⁸² A. Loeliger,¹⁸² R. Loveless,¹⁸² J. Madhusudanan Sreekala,¹⁸² A. Mallampalli,¹⁸² D. Pinna,¹⁸²

A. Savin,¹⁸² V. Shang,¹⁸² V. Sharma,¹⁸² W. H. Smith,¹⁸² D. Teague,¹⁸² S. Trembath-Reichert,¹⁸² W. Vetens,¹⁸²

S. Afanasiev,¹⁸³ V. Andreev,¹⁸³ Yu. Andreev,¹⁸³ T. Aushev,¹⁸³ M. Azarkin,¹⁸³ A. Babaev,¹⁸³ A. Belyaev,¹⁸³

V. Blinov,¹⁸³,n E. Boos,¹⁸³ V. Borchsh,¹⁸³ P. Bunin,¹⁸³ V. Chekhovsky,¹⁸³ R. Chistov,¹⁸³,n M. Danilov,¹⁸³,n

A. Demiyanov,¹⁸³ A. Dermenev,¹⁸³ T. Dimova,¹⁸³,n I. Dremin,¹⁸³ V. Epshteyn,¹⁸³,kkkk A. Ershov,¹⁸³

M. Gavrilenko,¹⁸³ G. Gavrilov,¹⁸³ V. Gavrilov,¹⁸³ S. Gninenko,¹⁸³ V. Golovtcov,¹⁸³ N. Golubev,¹⁸³ I. Golutvin,¹⁸³

I. Gorbunov,¹⁸³ A. Iuzhakov,¹⁸³ V. Ivanchenko,¹⁸³ Y. Ivanov,¹⁸³ V. Kachanov,¹⁸³ A. Kalinin,¹⁸³ A. Kamenev,¹⁸³

L. Kardapoltsev,¹⁸³,n V. Karjavine,¹⁸³ A. Karneyeu,¹⁸³ V. Kim,¹⁸³,n M. Kirakosyan,¹⁸³ M. Kirsanov,¹⁸³

O. Kodolova,¹⁸³,llll D. Konstantinov,¹⁸³ V. Korotkikh,¹⁸³ N. Krasnikov,¹⁸³ E. Kuznetsova,¹⁸³,mmmm A. Lanev,¹⁸³

A. Litomin,¹⁸³ O. Lukina,¹⁸³ N. Lychkovskaya,¹⁸³ V. Makarenko,¹⁸³ A. Malakhov,¹⁸³ V. Matveev,¹⁸³,n

V. Murzin,¹⁸³ A. Nikitenko,¹⁸³,nnnn S. Obraztsov,¹⁸³ V. Okhotnikov,¹⁸³ V. Oreshkin,¹⁸³ A. Oskin,¹⁸³ I. Ovtin,¹⁸³,n

V. Palichik,¹⁸³ P. Parygin,¹⁸³,oooo A. Pashenkov,¹⁸³ V. Perelygin,¹⁸³ S. Petrushanko,¹⁸³ G. Pivovarov,¹⁸³

S. Polikarpov,¹⁸³,n V. Popov,¹⁸³ G. Safronov,¹⁸³ M. Savina,¹⁸³ V. Savrin,¹⁸³ V. Shalaev,¹⁸³ S. Shmatov,¹⁸³

S. Shulha,¹⁸³ Y. Skovpen,¹⁸³,n I. Smirnov,¹⁸³ V. Smirnov,¹⁸³ A. Snigirev,¹⁸³ D. Sosnov,¹⁸³ A. Spiridonov,¹⁸³

A. Stepennov,¹⁸³ J. Suarez Gonzalez,¹⁸³ L. Sukhikh,¹⁸³ V. Sulimov,¹⁸³ E. Tcherniaev,¹⁸³ A. Terkulov,¹⁸³

O. Teryaev,¹⁸³ D. Tlisov,¹⁸³,a M. Toms,¹⁸³,pppp A. Toropin,¹⁸³ L. Uvarov,¹⁸³ A. Uzunian,¹⁸³ I. Vardanyan,¹⁸³

E. Vlasov,¹⁸³,qqqq S. Volkov,¹⁸³ A. Vorobyev,¹⁸³ N. Voytishin,¹⁸³ B. S. Yuldashev,¹⁸³,rrrr A. Zarubin,¹⁸³

I. Zhizhin,¹⁸³ and A. Zhokin¹⁸³

(CMS Collaboration)

<footnote n="1">¹Yerevan Physics Institute, Yerevan, Armenia</footnote>

<footnote n="2">²Institut für Hochenergiephysik, Vienna, Austria</footnote>

<footnote n="3">³Universiteit Antwerpen, Antwerpen, Belgium</footnote>

<footnote n="4">⁴Vrije Universiteit Brussel, Brussel, Belgium</footnote>

<footnote n="5">⁵Université Libre de Bruxelles, Bruxelles, Belgium</footnote>

<footnote n="6">⁶Ghent University, Ghent, Belgium</footnote>

<footnote n="7">⁷Université Catholique de Louvain, Louvain-la-Neuve, Belgium</footnote>

<footnote n="8">⁸Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, Brazil</footnote>

<footnote n="9">⁹Universidade do Estado do Rio de Janeiro, Rio de Janeiro, Brazil</footnote>

<footnote n="10">¹⁰Universidade Estadual Paulista, Universidade Federal do ABC, São Paulo, Brazil</footnote>

<footnote n="11">¹¹Institute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Sofia, Bulgaria</footnote>

<footnote n="12">¹²University of Sofia, Sofia, Bulgaria</footnote>

<footnote n="13">¹³Beihang University, Beijing, China</footnote>

<footnote n="14">¹⁴Department of Physics, Tsinghua University, Beijing, China</footnote>

<footnote n="15">¹⁵Institute of High Energy Physics, Beijing, China</footnote>

<footnote n="16">¹⁶State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing, China</footnote>
<sup>17</sup>Sun Yat-Sen University, Guangzhou, China

<sup>18</sup>Institute of Modern Physics and Key Laboratory of Nuclear Physics and Ion-beam Application (MOE) - Fudan University, Shanghai, China

<sup>19</sup>Zhejiang University, Hangzhou, Zhejiang, China

<sup>20</sup>Universidad de Los Andes, Bogota, Colombia

<sup>21</sup>Universidad de Antioquia, Medellín, Colombia

<sup>22</sup>University of Split, Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, Split, Croatia

<sup>23</sup>University of Split, Faculty of Science, Split, Croatia

<sup>24</sup>Institute Rudjer Bosković, Zagreb, Croatia

<sup>25</sup>University of Cyprus, Nicosia, Cyprus

<sup>26</sup>Charles University, Prague, Czech Republic

<sup>27</sup>Escuela Politécnica Nacional, Quito, Ecuador

<sup>28</sup>Universidad San Francisco de Quito, Quito, Ecuador

<sup>29</sup>Academy of Scientific Research and Technology of the Arab Republic of Egypt, Egyptian Network of High Energy Physics, Cairo, Egypt

<sup>30</sup>Center for High Energy Physics (CHEP-FU), Fayoum University, El-Fayoum, Egypt

<sup>31</sup>National Institute of Chemical Physics and Biophysics, Tallinn, Estonia

<sup>32</sup>Department of Physics, University of Helsinki, Helsinki, Finland

<sup>33</sup>Helsinki Institute of Physics, Helsinki, Finland

<sup>34</sup>Lappeenranta-Lahti University of Technology, Lappeenranta, Finland

<sup>35</sup>IRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France

<sup>36</sup>Laboratoire Leprince-Ringuet, CNRS/IN2P3, Ecole Polytechnique, Institut Polytechnique de Paris, Palaiseau, France

<sup>37</sup>Université de Strasbourg, CNRS, IPHC UMR 7178, Strasbourg, France

<sup>38</sup>Institut de Physique des 2 Infinis de Lyon (IP2I), Villeurbanne, France

<sup>39</sup>Georgian Technical University, Tbilisi, Georgia

<sup>40</sup>RWTH Aachen University, I. Physikalisches Institut, Aachen, Germany

<sup>41</sup>RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany

<sup>42</sup>RWTH Aachen University, III. Physikalisches Institut B, Aachen, Germany

<sup>43</sup>Deutsches Elektronen-Synchrotron, Hamburg, Germany

<sup>44</sup>University of Hamburg, Hamburg, Germany

<sup>45</sup>Karlsruher Institut fuer Technologie, Karlsruhe, Germany

<sup>46</sup>Institute of Nuclear and Particle Physics (INPP), NCSR Demokritos, Aghia Paraskevi, Greece

<sup>47</sup>National and Kapodistrian University of Athens, Athens, Greece

<sup>48</sup>National Technical University of Athens, Athens, Greece

<sup>49</sup>University of Ioánnina, Ioánnina, Greece

<sup>50</sup>MTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, Hungary

<sup>51</sup>Wigner Research Centre for Physics, Budapest, Hungary

<sup>52</sup>Institute of Nuclear Research ATOMKI, Debrecen, Hungary

<sup>53</sup>Institute of Physics, University of Debrecen, Debrecen, Hungary

<sup>54</sup>Karoly Robert Campus, MATE Institute of Technology, Gyongyos, Hungary

<sup>55</sup>Indian Institute of Science (IISc), Bangalore, India

<sup>56</sup>Panjab University, Chandigarh, India

<sup>57</sup>University of Delhi, Delhi, India

<sup>58</sup>Saha Institute of Nuclear Physics, HBNI, Kolkata, India

<sup>59</sup>Indian Institute of Technology Madras, Madras, India

<sup>60</sup>Bhabha Atomic Research Centre, Mumbai, India

<sup>61</sup>Tata Institute of Fundamental Research-A, Mumbai, India

<sup>62</sup>Tata Institute of Fundamental Research-B, Mumbai, India

<sup>63</sup>National Institute of Science Education and Research, An OCC of Homi Bhabha National Institute, Bhubaneswar, Odisha, India

<sup>64</sup>Indian Institute of Science Education and Research (IISER), Pune, India

<sup>65</sup>Isfahan University of Technology, Isfahan, Iran

<sup>66</sup>Institute for Research in Fundamental Sciences (IPM), Tehran, Iran

<sup>67</sup>University College Dublin, Dublin, Ireland

<sup>68a</sup>INFN Sezione di Bari, Bari, Italy

<sup>68b</sup>Università di Bari, Bari, Italy

<sup>68c</sup>Politécnico di Bari, Bari, Italy

<sup>69a</sup>INFN Sezione di Bologna, Bologna, Italy

<sup>69b</sup>Università di Bologna, Bologna, Italy

<sup>70a</sup>INFN Sezione di Catania, Catania, Italy
70b Università di Catania, Catania, Italy

71a INFN Sezione di Firenze, Firenze, Italy

71b Università di Firenze, Firenze, Italy

72INFN Laboratori Nazionali di Frascati, Frascati, Italy

73a INFN Sezione di Genova, Genova, Italy

73b Università di Genova, Genova, Italy

74a INFN Sezione di Milano-Bicocca, Milano, Italy

74b Università di Milano-Bicocca, Milano, Italy

75a INFN Sezione di Napoli, Napoli, Italy

75b Università di Napoli 'Federico II', Napoli, Italy

75c Università della Basilicata, Potenza, Italy

75d Università G. Marconi, Roma, Italy

76a INFN Sezione di Padova, Padova, Italy

76b Università di Padova, Padova, Italy

76c Università di Trento, Trento, Italy

77a INFN Sezione di Pavia, Pavia, Italy

77b Università di Pavia, Pavia, Italy

78a INFN Sezione di Perugia, Perugia, Italy

78b Università di Perugia, Perugia, Italy

79a INFN Sezione di Pisa, Pisa, Italy

79b Università di Pisa, Pisa, Italy

79c Scuola Normale Superiore di Pisa, Pisa, Italy

79d Università di Siena, Siena, Italy

80a INFN Sezione di Roma, Roma, Italy

80b Sapienza Università di Roma, Roma, Italy

81a INFN Sezione di Torino, Torino, Italy

81b Università di Torino, Torino, Italy

81c Università del Piemonte Orientale, Novara, Italy

82a INFN Sezione di Trieste, Trieste, Italy

82b Università di Trieste, Trieste, Italy

83 Kyungpook National University, Daegu, Korea

84 Chonnam National University, Institute for Universe and Elementary Particles, Kwangju, Korea

85 Hanyang University, Seoul, Korea

86 Korea University, Seoul, Korea

87 Kyung Hee University, Department of Physics, Seoul, Korea

88 Sejong University, Seoul, Korea

89 Seoul National University, Seoul, Korea

90 University of Seoul, Seoul, Korea

91 Yonsei University, Department of Physics, Seoul, Korea

92 Sungkyunkwan University, Suwon, Korea

93 College of Engineering and Technology, American University of the Middle East (AUM), Dasman, Kuwait

94 Riga Technical University, Riga, Latvia

95 Vilnius University, Vilnius, Lithuania

96 National Centre for Particle Physics, Universiti Malaya, Kuala Lumpur, Malaysia

97 Universidad de Sonora (UNISON), Hermosillo, Mexico

98 Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, Mexico

99 Universidad Iberoamericana, Mexico City, Mexico

100 Benemerita Universidad Autonoma de Puebla, Puebla, Mexico

101 Universidad Autónoma de San Luis Potosí, San Luis Potosí, Mexico

102 University of Montenegro, Podgorica, Montenegro

103 University of Auckland, Auckland, New Zealand

104 University of Canterbury, Christchurch, New Zealand

105 National Centre for Physics, Quaid-I-Azam University, Islamabad, Pakistan

106 AGH University of Science and Technology Faculty of Computer Science, Electronics and Telecommunications, Krakow, Poland

107 National Centre for Nuclear Research, Swierk, Poland

108 Institute of Experimental Physics, Faculty of Physics, University of Warsaw, Warsaw, Poland

109 Laboratório de Instrumentação e Física Experimental de Partículas, Lisboa, Portugal

110 VINCA Institute of Nuclear Sciences, University of Belgrade, Belgrade, Serbia

111 Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain

112 Universidad Autónoma de Madrid, Madrid, Spain
¹¹³Universidad de Oviedo, Instituto Universitario de Ciencias y Tecnologías Espaciales de Asturias (ICTEA), Oviedo, Spain

¹¹⁴Instituto de Física de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, Spain

¹¹⁵University of Colombo, Colombo, Sri Lanka

¹¹⁶University of Ruhuna, Department of Physics, Matara, Sri Lanka

¹¹⁷CERN, European Organization for Nuclear Research, Geneva, Switzerland

¹¹⁸Paul Scherrer Institut, Villigen, Switzerland

¹¹⁹ETH Zurich - Institute for Particle Physics and Astrophysics (IPA), Zurich, Switzerland

¹²⁰Universität Zürich, Zürich, Switzerland

¹²¹National Central University, Chung-Li, Taiwan

¹²²National Taiwan University (NTU), Taipei, Taiwan

¹²³Chulalongkorn University, Faculty of Science, Department of Physics, Bangkok, Thailand

¹²⁴Çukurova University, Physics Department, Science and Art Faculty, Adana, Turkey

¹²⁵Middle East Technical University, Physics Department, Ankara, Turkey

¹²⁶Bogazici University, Istanbul, Turkey

¹²⁷Istanbul Technical University, Istanbul, Turkey

¹²⁸Istanbul University, Istanbul, Turkey

¹²⁹Institute for Scintillation Materials of National Academy of Science of Ukraine, Kharkiv, Ukraine

¹³⁰National Science Centre, Kharkiv Institute of Physics and Technology, Kharkiv, Ukraine

¹³¹University of Bristol, Bristol, United Kingdom

¹³²Rutherford Appleton Laboratory, Didcot, United Kingdom

¹³³Imperial College, London, United Kingdom

¹³⁴Brunel University, Uxbridge, United Kingdom

¹³⁵Baylor University, Waco, Texas, USA

¹³⁶Catholic University of America, Washington, DC, USA

¹³⁷The University of Alabama, Tuscaloosa, Alabama, USA

¹³⁸Boston University, Boston, Massachusetts, USA

¹³⁹Brown University, Providence, Rhode Island, USA

¹⁴⁰University of California, Davis, Davis, California, USA

¹⁴¹University of California, Los Angeles, California, USA

¹⁴²University of California, Riverside, Riverside, California, USA

¹⁴³University of California, San Diego, La Jolla, California, USA

¹⁴⁴University of California, Santa Barbara - Department of Physics, Santa Barbara, California, USA

¹⁴⁵California Institute of Technology, Pasadena, California, USA

¹⁴⁶Carnegie Mellon University, Pittsburgh, Pennsylvania, USA

¹⁴⁷University of Colorado Boulder, Boulder, Colorado, USA

¹⁴⁸Cornell University, Ithaca, New York, USA

¹⁴⁹Fermi National Accelerator Laboratory, Batavia, Illinois, USA

¹⁵⁰University of Florida, Gainesville, Florida, USA

¹⁵¹Florida State University, Tallahassee, Florida, USA

¹⁵²Florida Institute of Technology, Melbourne, Florida, USA

¹⁵³University of Illinois at Chicago (UIC), Chicago, Illinois, USA

¹⁵⁴The University of Iowa, Iowa City, Iowa, USA

¹⁵⁵Johns Hopkins University, Baltimore, Maryland, USA

¹⁵⁶The University of Kansas, Lawrence, Kansas, USA

¹⁵⁷Kansas State University, Manhattan, Kansas, USA

¹⁵⁸Lawrence Livermore National Laboratory, Livermore, California, USA

¹⁵⁹University of Maryland, College Park, Maryland, USA

¹⁶⁰Massachusetts Institute of Technology, Cambridge, Massachusetts, USA

¹⁶¹University of Minnesota, Minneapolis, Minnesota, USA

¹⁶²University of Mississippi, Oxford, Mississippi, USA

¹⁶³University of Nebraska-Lincoln, Lincoln, Nebraska, USA

¹⁶⁴State University of New York at Buffalo, Buffalo, New York, USA

¹⁶⁵Northeastern University, Boston, Massachusetts, USA

¹⁶⁶Northwestern University, Evanston, Illinois, USA

¹⁶⁷University of Notre Dame, Notre Dame, Indiana, USA

¹⁶⁸The Ohio State University, Columbus, Ohio, USA

¹⁶⁹Princeton University, Princeton, New Jersey, USA

¹⁷⁰University of Puerto Rico, Mayaguez, Puerto Rico, USA

¹⁷¹Purdue University, West Lafayette, Indiana, USA

¹⁷²Purdue University Northwest, Hammond, Indiana, USA
<sup>173</sup>Rice University, Houston, Texas, USA

<sup>174</sup>University of Rochester, Rochester, New York, USA

<sup>175</sup>Rutgers, The State University of New Jersey, Piscataway, New Jersey, USA

<sup>176</sup>University of Tennessee, Knoxville, Tennessee, USA

<sup>177</sup>Texas A&M University, College Station, Texas, USA

<sup>178</sup>Texas Tech University, Lubbock, Texas, USA

<sup>179</sup>Vanderbilt University, Nashville, Tennessee, USA

<sup>180</sup>University of Virginia, Charlottesville, Virginia, USA

<sup>181</sup>Wayne State University, Detroit, Michigan, USA

<sup>182</sup>University of Wisconsin - Madison, Madison, Wisconsin, USA

<sup>183</sup>An institute or international laboratory covered by a cooperation agreement with CERN

<sup>a</sup>Deceased.

<sup>b</sup>Also at TU Wien, Vienna, Austria.

<sup>c</sup>Also at Institute of Basic and Applied Sciences, Faculty of Engineering, Arab Academy for Science, Technology and Maritime Transport, Alexandria, Egypt.

<sup>d</sup>Also at Université Libre de Bruxelles, Bruxelles, Belgium.

<sup>e</sup>Also at IRFU, CEA, Université Paris-Saclay, Gif-sur-Yvette, France.

<sup>f</sup>Also at Universidade Estadual de Campinas, Campinas, Brazil.

<sup>g</sup>Also at Federal University of Rio Grande do Sul, Porto Alegre, Brazil.

<sup>h</sup>Also at UFMS, Nova Andradina, Brazil.

<sup>i</sup>Also at Universidade Federal de Pelotas, Pelotas, Brazil.

<sup>j</sup>Also at Nanjing Normal University Department of Physics, Nanjing, China.

<sup>k</sup>Also at The University of Iowa, Iowa City, Iowa, USA.

<sup>l</sup>Also at University of Chinese Academy of Sciences, Beijing, China.

<sup>m</sup>Also at University of Chinese Academy of Sciences, Beijing, China.

<sup>n</sup>Also at Another institute or international laboratory covered by a cooperation agreement with CERN.

<sup>o</sup>Also at Cairo University, Cairo, Egypt.

<sup>p</sup>Also at Helwan University, Cairo, Egypt.

<sup>q</sup>Also at Zewail City of Science and Technology, Zewail, Egypt.

<sup>r</sup>Also at Suez University, Suez, Egypt.

<sup>s</sup>Also at British University in Egypt, Cairo, Egypt.

<sup>t</sup>Also at Purdue University, West Lafayette, Indiana, USA.

<sup>u</sup>Also at Université de Haute Alsace, Mulhouse, France.

<sup>v</sup>Also at Ilia State University, Tbilisi, Georgia.

<sup>w</sup>Also at Erzincan Binali Yildirim University, Erzincan, Turkey.

<sup>x</sup>Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland.

<sup>y</sup>Also at RWTH Aachen University, III. Physikalisches Institut A, Aachen, Germany.

<sup>z</sup>Also at University of Hamburg, Hamburg, Germany.

<sup>aa</sup>Also at Isfahan University of Technology, Isfahan, Iran.

<sup>bb</sup>Also at Brandenburg University of Technology, Cottbus, Germany.

<sup>cc</sup>Also at Institute of Physics, University of Debrecen, Debrecen, Hungary.

<sup>dd</sup>Also at Physics Department, Faculty of Science, Assiut University, Assiut, Egypt.

<sup>ee</sup>Also at Karoly Robert Campus, MATE Institute of Technology, Gyongyos, Hungary.

<sup>ff</sup>Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary.

<sup>gg</sup>Also at MTA-ELTE Lendület CMS Particle and Nuclear Physics Group, Eötvös Loránd University, Budapest, Hungary.

<sup>hh</sup>Also at Wigner Research Centre for Physics, Budapest, Hungary.

<sup>i</sup>Also at G.H.G. Khalsa College, Punjab, India.

<sup>j</sup>Also at Shoolini University, Solan, India.

<sup>kk</sup>Also at University of Hyderabad, Hyderabad, India.

<sup>l</sup>Also at University of Visva-Bharati, Santiniketan, India.

<sup>mm</sup>Also at Indian Institute of Technology (IIT), Mumbai, India.

<sup>nn</sup>Also at IIT Bhubaneswar, Bhubaneswar, India.

<sup>oo</sup>Also at Institute of Physics, Bhubaneswar, India.

<sup>pp</sup>Also at Deutsches Elektronen-Synchrotron, Hamburg, Germany.

<sup>qq</sup>Also at Sharif University of Technology, Tehran, Iran.

<sup>r</sup>Also at Department of Physics, University of Science and Technology of Mazandaran, Behshahr, Iran.

<sup>ss</sup>Also at Italian National Agency for New Technologies, Energy and Sustainable Economic Development, Bologna, Italy.

<sup>t</sup>Also at Centro Siciliano di Fisica Nucleare e di Struttura Della Materia, Catania, Italy.

<sup>uu</sup>Also at Università di Napoli 'Federico II', Napoli, Italy.
vv Also at Consejo Nacional de Ciencia y Tecnología, Mexico City, Mexico.

ww Also at Faculty of Physics, University of Belgrade, Belgrade, Serbia.

xx Also at Trincomalee Campus, Eastern University, Sri Lanka, Nilaveli, Sri Lanka.

yy Also at INFN Sezione di Pavia, Università di Pavia, Pavia, Italy.

zz Also at National and Kapodistrian University of Athens, Athens, Greece.

aaa Also at Universität Zürich, Zurich, Switzerland.

bbb Also at Ecole Polytechnique Fédérale Lausanne, Lausanne, Switzerland.

ccc Also at Stefan Meyer Institute for Subatomic Physics, Vienna, Austria.

ddd Also at Laboratoire d'Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux, France.

eee Also at Şırnak University, Şırnak, Turkey.

fff Also at Department of Physics, Tsinghua University, Beijing, China.

ggg Also at Near East University, Research Center of Experimental Health Science, Mersin, Turkey.

hhh Also at Beykent University, Istanbul, Turkey.

iii Also at Istanbul Aydin University, Application and Research Center for Advanced Studies, Istanbul, Turkey.

iii Also at Mersin University, Mersin, Turkey.

kkk Also at Izmir Bakircay University, Izmir, Turkey.

ll Also at Adiyaman University, Adiyaman, Turkey.

mmmm Also at Ozyegin University, Istanbul, Turkey.

nn Also at Izmir Institute of Technology, Izmir, Turkey.

ooo Also at Necmettin Erbakan University, Konya, Turkey.

ppp Also at Bozok Universitesesi Rektörlüğü, Yozgat, Turkey.

qqq Also at Marmara University, Istanbul, Turkey.

rr Also at Milli Savunma University, Istanbul, Turkey.

ss Also at Kafkas University, Kars, Turkey.

tt Also at Istanbul Bilgi University, Istanbul, Turkey.

uuu Also at Hacettepe University, Ankara, Turkey.

vvv Also at Vrije Universiteit Brussel, Brussel, Belgium.

www Also at School of Physics and Astronomy, University of Southampton, Southampton, United Kingdom.

xxx Also at IPPP Durham University, Durham, United Kingdom.

yyy Also at Monash University, Faculty of Science, Clayton, Australia.

zzz Also at Bethel University, St. Paul, Minnesota, USA.

aaaa Also at Karamanoğlu Mehmetbey University, Karaman, Turkey.

bbbb Also at California Institute of Technology, Pasadena, California, USA.

cccc Also at Ain Shams University, Cairo, Egypt.

dddd Also at Bingol University, Bingol, Turkey.

eeee Also at Georgian Technical University, Tbilisi, Georgia.

ffff Also at Sinop University, Sinop, Turkey.

gggg Also at Mimar Sinan University, Istanbul, Istanbul, Turkey.

hhhh Also at Erciyes University, Kayseri, Turkey.

iii Also at Texas A&M University at Qatar, Doha, Qatar.

jji Also at Kyungpook National University, Daegu, Korea.

kkkk Also at Istanbul University, Istanbul, Turkey.

lll Also at Yerevan Physics Institute, Yerevan, Armenia.

mmmm Also at University of Florida, Gainesville, Florida, USA.

nnnn Also at Imperial College, London, United Kingdom.

oooo Also at University of Rochester, Rochester, New York, USA.

pppp Also at Baylor University, Waco, Texas, USA.

qqqq Also at INFN Sezione di Torino, Università di Torino, Torino, Italy, Università del Piemonte Orientale, Novara, Italy.

rrr Also at Institute of Nuclear Physics of the Uzbekistan Academy of Sciences, Tashkent, Uzbekistan.