Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb Collisions at sqrt(s(NN))= 2.76 TeV with the ATLAS detector

EUROPEAN ORGANISATION FOR NUCLEAR RESEARCH (CERN)

CERN-PH-EP-2013-081

Submitted to: PRL

Measurement of the Azimuthal Angle Dependence of Inclusive

Jet Yields in Pb+Pb Collisions at

√

s

NN

= 2.76 TeV

with the

ATLAS detector

The ATLAS Collaboration

Abstract

Measurements of the variation of inclusive jet suppression as a function of relative azimuthal

angle, ∆φ, with respect to the elliptic event plane provide insight into the path-length dependence of

jet quenching. ATLAS has measured the ∆φ dependence of jet yields in 0.14 nb

−1

of

√

s

NN

= 2.76 TeV

Pb+Pb collisions at the LHC for jet transverse momenta p

T

> 45 GeV

in different collision centrality

bins using an underlying event subtraction procedure that accounts for elliptic flow. The variation of

the jet yield with ∆φ was characterized by the parameter, v

₂jet

, and the ratio of out-of-plane (∆φ ∼ π/2)

to in-plane (∆φ ∼ 0) yields. Non-zero v

₂jet

values were measured in all centrality bins for p

T

< 160 GeV.

The jet yields are observed to vary by as much as 20% between in-plane and out-of-plane directions.

Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb

Collisions at

√

s

NN

= 2.76 TeV with the ATLAS detector

ATLAS Collaboration

Measurements of the variation of inclusive jet suppression as a function of relative azimuthal angle, ∆φ, with respect to the elliptic event plane provide insight into the path-length dependence of jet quenching. ATLAS has measured the ∆φ dependence of jet yields in 0.14 nb−1of√sNN= 2.76 TeV Pb+Pb collisions at the LHC for jet transverse momenta pT> 45 GeV in different collision centrality bins using an underlying event subtraction procedure that accounts for elliptic flow. The variation of the jet yield with ∆φ was characterized by the parameter, vjet₂ , and the ratio of out-of-plane (∆φ ∼ π/2) to in-plane (∆φ ∼ 0) yields. Non-zero vjet2 values were measured in all centrality bins for pT < 160 GeV. The jet yields are observed to vary by as much as 20% between in-plane and out-of-plane directions.

PACS numbers: 25.75.-q

Studies of jet production in Pb+Pb collisions at the LHC [1, 2] show behavior consistent with “jet quench-ing,” a general term for the modification of parton show-ers in the hot dense medium created in ultra-relativistic nuclear collisions. For example, the inclusive yield of jets was observed to be suppressed by a factor of ap-proximately two in central Pb+Pb collisions relative to peripheral collisions [3], consistent with a medium-induced reduction in the jet energies. Perturbative or weak-coupling calculations model jet energy loss, dE/dx, through a combination of collisional and radiative energy loss of the constituents of the parton shower. The radia-tive contributions are subject to coherence effects [4] that explicitly depend on the path length of the shower in the medium. Strong-coupling calculations suggest a different path-length dependence [5, 6]. Measurements of the jet yield as a function of quantities providing indirect con-trol over the jet path lengths may provide insight into the physical mechanisms responsible for jet quenching [7, 8]. Such quantities include the Pb+Pb collision centrality and the azimuthal angle of the jet with respect to the elliptic event plane.

Elliptic flow refers to a cos 2φ modulation of the az-imuthal angle (φ) distribution of particles produced in ultra-relativistic nuclear collisions [9]. This modulation is understood to arise from an approximately elliptic anisotropy of the initial-state transverse energy density profile that is imprinted on the azimuthal angle distribu-tion of final-state particles [10] by the strong collective evolution of the medium. The resulting azimuthal angle distribution is often parameterized by the form:

dN

dφ ∝ 1 + 2v2cos 2(φ − Ψ2), (1)

where the elliptic event plane angle, Ψ2, specifies the

ori-entation of the initial density profile in the transverse plane, and the parameter v2 quantifies the magnitude of

the modulation. Jets measured at different azimuthal angles relative to the event plane, ∆φ ≡ φjet− Ψ2,

re-sult from parton showers that traverse, on average,

dif-ferent path lengths and density profiles in the medium. Thus, a measurement of the variation of the jet yield as a function of ∆φ should provide a direct constraint on theoretical models of the path-length dependence of the energy loss. This measurement is not directly sensitive to the contribution to jet suppression from higher order flow harmonics, which may arise from the fluctuating initial geometry [11–13].

Variations in jet yield as a function of ∆φ have been ob-served indirectly through measurements of single hadrons with large transverse momentum (pT) at RHIC [14–16]

and the LHC [17–19]. The utility of such measurements is limited by the weak relationship between hadron pTand

the transverse momentum of the parent parton shower. This Letter presents results of measurements using fully reconstructed jets, which have kinematics properties that are more closely related to those of the parent partons. The ∆φ dependence of the inclusive jet yield was mea-sured in√sNN= 2.76 TeV Pb+Pb collisions as a function

of jet pT and Pb+Pb collision centrality. The

measure-ment was performed with the anti-ktalgorithm [20] with

distance parameter R = 0.2, chosen to limit the contri-bution of the underlying event (UE) to the measurement. The ∆φ dependence was characterized by the jet v2, v2jet,

and the ratios of the jet yields in different ∆φ intervals at fixed pT and centrality. Such dependence is expected to

be small in either the most central or most peripheral col-lisions, due to the lack of initial-state anisotropy and the lack of quenching, respectively. For intermediate central-ities, measurement of the ∆φ dependence of the jet yields probes the interplay between contributions to quenching from the overall system size and energy density, as well as from the initial state anisotropy.

The measurements presented here were performed with the ATLAS detector [21] using its calorimeter, inner detector, trigger, and data acquisition systems. The calorimeter system consists of a liquid argon (LAr) elec-tromagnetic (EM) calorimeter covering |η| < 3.2, a steel/scintillator sampling hadronic calorimeter covering

|η| < 1.7, a LAr hadronic calorimeter covering 1.5 < |η| < 3.2, and a forward calorimeter (FCal) covering 3.2 < |η| < 4.9. Charged-particle tracks were measured over the range |η| < 2.5 using the inner detector [22], which is composed of silicon pixel detectors in the in-nermost layers, followed by silicon microstrip detectors and a straw-tube transition-radiation tracker (|η| < 2.0), all immersed in a 2 T axial magnetic field. The zero-degree calorimeters (ZDCs) are located symmetrically at z = ±140 m and cover |η| > 8.3. In Pb+Pb collisions the ZDCs primarily measure non-interacting “spectator” neutrons from the incident nuclei. A ZDC coincidence trigger was defined by requiring a signal consistent with one or more neutrons in each of the calorimeters.

Pb+Pb collisions corresponding to a total integrated luminosity of 0.14 nb−1 were analyzed. The events were recorded using either a minimum-bias trigger, formed from the logical OR of triggers based on a ZDC co-incidence or total transverse energy in the event, or a jet trigger implemented using the Pb+Pb jet reconstruc-tion algorithm. The jet trigger selected events having at least one jet with transverse energy ET > 20 GeV.

Event selection and background rejection criteria were applied [17] yielding 52 million and 14 million events in the minimum-bias and jet-triggered samples, respec-tively. For each event, Ψ2 was computed from the

az-imuthal distribution of the transverse energy measured in the FCal [17, 23], and angles with respect to Ψ2 were

defined over 0 ≤ ∆φ ≤ π/2. The centrality of Pb+Pb collisions was characterized by ΣEFCal

T , the total

trans-verse energy measured in the FCal [17]. The results re-ported here were obtained using the following central-ity intervals defined according to successive percentiles of the ΣEFCal

T distribution ordered from the most

cen-tral (highest ΣE_TFCal) to the most peripheral collisions: 5–10%, 10–20%, 20–30%, 30–40%, 40–50%, and 50–60%. The centrality interval 5–60% coincides to the range over which the Ψ2 resolution is adequate for the

measure-ment. The percentiles were defined after correcting the ΣEFCal

T distribution for an estimated 2% minimum-bias

trigger inefficiency that is concentrated in the most pe-ripheral intervals, which are not included in this analysis. A Glauber model analysis [24, 25] of the ΣEFCal

T

distri-bution [17] was used to evaluate the average number of nucleons participating in the collision, hNparti, in each

centrality interval.

The jet reconstruction and underlying event subtrac-tion procedures are the same as those used in Ref. [3], which is summarized in the following. The anti-kt

algo-rithm was applied to calorimeter towers with segmenta-tion ∆η × ∆φ = 0.1 × 0.1. A two-step iterative proce-dure was used to obtain an event-by-event estimate of the average η-dependent UE energy density while excluding actual jets from that estimate. The jet kinematics were obtained by subtracting the UE energy from the towers within the jet. This subtraction accounts for elliptic flow

by modulating the average background density by the magnitude of the elliptic flow measured by the calorime-ter, vcalo

2 , over the interval |η| < 3.2 and excluding η

regions containing jets. Following reconstruction, the jet energies were corrected to account for the calorimeter en-ergy response using an η- and ET-dependent

multiplica-tive factor that was derived from the MC simulation [26]. Separate from the calorimeter jets, “track jets” were reconstructed by applying the anti-kt algorithm with

R = 0.4 to charged particles having pT > 4 GeV. The

pT of the track jets, ptrkjet_T , is largely unaffected by

the UE due to the pT > 4 GeV requirement. To

ex-clude the contribution to the jet yield from UE fluctu-ations of soft particles falsely identified as calorimeter jets, the jets used in this analysis were required to be within ∆R = p∆η2_{+ ∆φ}2 _{= 0.2 of a track jet with}

ptrkjet_T > 10 GeV or an EM cluster [27] with pT> 9 GeV

[28].

The performance of the jet reconstruction was eval-uated using the GEANT4-simulated detector response [29, 30] in a Monte Carlo (MC) sample of pp hard scat-tering events at √sNN = 2.76 TeV. The events were

produced with the PYTHIA event generator [31] ver-sion 6.423 using the AUET2B tune [32] and overlaid on minimum-bias Pb+Pb collisions recorded by ATLAS. Through this embedding procedure, the MC sample con-tains a UE contribution that is identical in all respects to the data, including azimuthal modulation of the UE due to harmonic flow. Jets reconstructed in the MC events using the same algorithms as applied to data were compared to generator-level jets reconstructed from final-state PYTHIA hadrons. Potential variations in the jet energy resolution (JER) and jet energy scale (JES) with ∆φ due to elliptic and higher-order modulation [11–13] of the UE were investigated in the MC sample; no signif-icant variation was found.

The dependence of the JES on ∆φ was further con-strained by comparing the calorimeter jets to matched track jets in the data. For different values of ∆φ, the mean pT of calorimeter jets was evaluated as a function

of the pT of the matched track jet, and no significant

variation with ∆φ was observed. This study provides an upper limit on the variation in the JES between jets at ∆φ = 0 and ∆φ = π/2 of 0.1% for pT> 45 GeV.

Double differential jet yields, d2Njet/dpTd∆φ, were

measured over |η| < 2.1 for each of the centrality ranges described above and in five pTintervals: 45–60 GeV, 60–

80 GeV, 80–110 GeV, 110–160 GeV, and 160–210 GeV. The measurement in each pTrange was performed using

events selected by the jet trigger except for the 45–60 GeV pTrange, in which minimum-bias events were used. The

∆φ dependence of the jet yields in the 60–80 GeV pT

interval is shown for each centrality range in Fig. 1. A significant ∆φ variation that is consistent with a cos 2∆φ modulation is seen for all centrality intervals.

0.028 0.03 0.032 0.034 5 - 10 % 0.002 ± = 0.016 meas | jet 2 v -1 = 0.14 nb t d L

∫

= 2.76 TeV NN s Pb+Pb 10 - 20 % 0.002 ± = 0.032 meas | jet 2 v ATLAS = 0.2 R t k < 80 GeV T p 60 < ] -1 [GeV meas φ∆ d T p d jet N 2 d jet N 1 0.028 0.03 0.032 0.034 20 - 30 % 0.002 ± = 0.042 meas | jet 2 v 30 - 40 % 0.002 ± = 0.041 meas | jet 2 v φ ∆ 0 0.5 1 1.5 0.028 0.03 0.032 0.034 40 - 50 % 0.003 ± = 0.034 meas | jet 2 v φ ∆ 0 0.5 1 1.5 50 - 60 % 0.004 ± = 0.027 meas | jet 2 v

FIG. 1. ∆φ dependence of measured d2_{Njet/dpTd∆φ in the} 60 < pT< 80 GeV interval for six ranges of collision centrality. The yields are normalized by the total number of jets in the pT interval. The solid curves indicate the results of fitting the data to the functional form of Eq. (1), with the resulting v2 values, v₂jet|meas, listed in each panel. The error bars and errors on v2jet|measindicate statistical uncertainties.

are distorted by the finite resolutions in Ψ2 and the jet

pT. The Ψ2 resolution was evaluated using a sub-event

technique [17, 23] in which Ψ2 was measured separately

in the positive and negative η halves of the FCal yielding values Ψ+₂ and Ψ−₂, respectively. The width of the Ψ+₂ − Ψ−₂ distribution was used [23] to estimate a factor, κ, that was used to correct each measured v2 value for the

finite Ψ2resolution according to

v2= v2|meas/κ . (2)

This factor was evaluated for events containing jets to account for the relevant distribution of events within each centrality interval.

The pTdependence, and possibly also the ∆φ

depen-dence, of the measured yields are affected by the JER, which arises from both fluctuations in the UE and the detector response. The MC study shows that for the R = 0.2 jets used in this analysis, the JER-induced mi-gration between jet pTintervals is sufficiently small that

a “bin-by-bin” unfolding method, utilizing multiplicative corrections to the jet yields, is appropriate. The bin-by-bin correction factors are defined to be the number of generator-level jets divided by the number of recon-structed jets in each pT, ∆φ, and centrality interval. The

MC studies show no significant ∆φ variation of the JER, JES, and the correction factors, and so these correction factors were taken to be ∆φ-independent. Since the mea-surements presented here depend only on the ratios of

jet yields between different ∆φ intervals for the same pT

range, the correction factors do not affect any of the final results; the potential for a ∆φ dependence of the correc-tion factors is included in the estimates of the systematic uncertainty.

Systematic uncertainties on the corrected v2 values

arise due to uncertainties on the two correction proce-dures described above. Uncertainties on κ were estimated by using the values obtained in previous studies[17] for slightly different centrality intervals and interpolating to obtain values appropriate for the centrality intervals used here. The uncertainties were found to vary between 1% and 4% from central to peripheral collisions. Potential distortions in the measurement of Ψ2due to the

produc-tion of jets in the FCal pseudorapidity range were studied in the MC sample and found to be negligible for the cen-trality intervals included in this analysis.

Uncertainties on the measurements arising from ∆φ-dependent systematic uncertainties on the bin-by-bin correction factors were estimated by determining the sen-sitivity of these correction factors to each systematic variation and then parameterizing that sensitivity with a cos 2∆φ dependence. The sensitivity to the ∆φ de-pendence of the spectrum was evaluated by varying the pT spectrum of the generator-level jets in each ∆φ

in-terval within a range consistent with the measured v₂jet values. The JES and JER contributions to the uncer-tainty were obtained by varying the relationship between generator-level and reconstructed jet pTin the

determi-nation of the correction factors. These procedures uti-lized the JES constraints obtained from track jets and direct measurements of the UE contribution to the JER [3]. Parameterizations of the measured vcalo

2 and the

av-erage background ET underlying a typical jet measured

in the data were used to provide the dependence of vari-ations on centrality. The systematic uncertainties on v₂jet are less than 0.002 except in the most central and low-est pT intervals where the JER contribution dominates,

resulting in uncertainties between 0.005 and 0.01. The azimuthal dependence of jet suppression can be characterized by v₂jet, which was obtained by correcting the vjet₂ |meas values using Eq.(2). Figure 2 shows the

re-sulting v₂jetvalues as a function of jet pTfor all

central-ity intervals. Significant, non-zero values are observed over the range 45 < pT < 160 GeV for all centrality

in-tervals. A direct comparison between the v2 of single

high-pTcharged particles and v2jetis generally not

possi-ble; however the fact that both quantities exhibit only a weak pT dependence leads to the expectation that they

should be of similar magnitude. In the charged parti-cle measurements, the v2values of charged particles with

28 < pT< 48 GeV were found to vary between 0.02 and

0.05 for the 10–50% centrality range [18], which are gen-erally in agreement with vjet₂ values reported here indicat-ing no obvious inconsistencies between the two results.

jet 2 v 0 0.02 0.04 0.06 5 - 10 % = 0.2 R t k anti- 10 - 20 % ATLAS jet 2 v 0 0.02 0.04 0.06 20 - 30 % = 2.76 TeV NN s Pb+Pb -1 = 0.14 nb t d L

∫

30 - 40 % [GeV] T p 50 100 150 200 jet 2 v 0 0.02 0.04 0.06 40 - 50 % [GeV] T p 50 100 150 200 50 - 60 %

FIG. 2. v2jetas a function of jet pTin each centrality interval. The error bars on the points indicate statistical uncertainties while the shaded boxes represent the systematic uncertainties (see text). The horizontal width of the systematic error band is chosen for presentation purposes only.

The centrality dependence of vjet₂ is shown in Fig. 3 as a function of hNparti for different ranges in pT. The

variation in jet yields with ∆φ can also be characterized by the ratio of jet yields between the most out-of-plane (3π/8 ≤ ∆φ ≤ π/2) and most in-plane (0 ≤ ∆φ < π/8) bins, R_∆φmax≡ d2Njet/dpTd∆φ  _out/ d 2 Njet/dpTd∆φ  _in. (3)

This quantity is more general than v₂jet as it does not assume a functional form for the ∆φ dependence of the jet yields. The nuclear modification factor, RAA, is a

measure of the effect of quenching on hard scattering rates, and Rmax

∆φ can be interpreted as the ratio of

∆φ-dependent RAA factors, Rmax∆φ = RAA|_out/ RAA|_in [16].

The yields were corrected for Ψ2resolution assuming that

the ∆φ variation is dominated by the cos 2∆φ modula-tion, d2Ncorr jet dpTd∆φ =d 2_Nmeas jet dpTd∆φ 1 + 2vjet₂ cos 2∆φ 1 + 2v₂jet|meascos 2∆φ

!

. (4)

The results, expressed in terms of the quantity f2 ≡

1 − Rmax

∆φ, show as much as a 20% variation between

the out-of-plane and in-plane jet yields, but they are re-duced slightly from the maximal difference, evaluated at ∆φ = π/2 and ∆φ = 0, by the finite bin size used in the measurement. That reduction was corrected by assuming a 1+2vjet₂ cos 2∆φ variation of the jet yields within the ∆φ

0 0.1 0.2 < 60 GeV T p 45 < 60 < p_T < 80 GeV ATLAS = 0.2 R t k 〉 part N 〈 0 100 200 300 0 0.1 0.2 < 110 GeV T p 80 < jet 2 v jet 2 v 1+2 jet 2 v 4 corr 2 f 〉 part N 〈 0 100 200 300 < 160 GeV T p 110 < = 2.76 TeV NN s Pb+Pb -1 = 0.14 nb t d L

∫

FIG. 3. The hNparti dependence of vjet 2 ( ◦ ), f

corr

2 ( ) and

4v2jet/(1 + 2v jet

2 ) ( • ). All quantities have statistical and sys-tematic uncertainties that are indicated by error bars and shaded bands, respectively. The uncertainties for all quanti-ties are strongly correlated. The horizontal positions of the points have been offset slightly for presentation purposes and the width of the error bands indicates the uncertainty on hNparti.

bins containing ∆φ = 0 and π/2, and calculating the cor-responding yields at those ∆φ values. From these yields, f₂corrwas calculated analogously to f2. The magnitude of

the correction is typically a few percent. The f2corrvalues

are shown in Fig. 3. For a pure cos 2∆φ modulation of the jet yields, fcorr

2 would be given by 4v jet 2 /(1+2v

jet 2 ). To

test for deviations of the ∆φ dependence of the jet yields from a pure cos 2∆φ variation, 4v₂jet/(1 + 2v₂jet) was cal-culated using the measured vjet₂ values and is shown for each pTand centrality interval in Fig. 3.

Similar variations of v₂jet, fcorr

2 and 4v

jet

2 /(1 + 2v jet

2 )

with hNparti are seen in the 60–80 GeV range, which has

the best statistical precision. A reduction in f₂corr and vjet₂ in both the most central and peripheral collisions is not surprising; for very central collisions, the anisotropy of the initial state is small and the possible ∆φ varia-tion of path lengths in the medium is limited. Although the anisotropy is greater in peripheral collisions, there is little suppression in the jet yields [3]. Therefore large variations in jet yield as a function of ∆φ would be un-expected. The fcorr

2 and 4v

jet

2 /(1 + 2v jet

2 ) values are

gen-erally in agreement within uncertainties, indicating an azimuthal dependence of relative suppression when mea-sured with respect to the elliptic event plane that is dom-inated by second-harmonic modulation.

measure-ments of the variation of R = 0.2 anti-kt jet yields in

√

sNN= 2.76 TeV Pb+Pb collisions as a function of ∆φ,

the relative azimuthal angle of the jet with respect to the elliptic event plane. A significant ∆φ variation in the jet yield is observed for all centrality intervals and in all pTranges except for the 160–210 GeV pTinterval where

the statistical uncertainties are large. The observed az-imuthal variation of jet yields amounts to a reduction of 10–20% in the jet yields between in-plane and out-of-plane directions. These results establish a relationship between jet suppression and the initial nuclear geometry that should constrain models of the path-length depen-dence of the quenching mechanism.

We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWF and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC

and NSRF, European Union; IN2P3-CNRS,

CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, DFG, HGF, MPG and AvH Foundation, Germany; GSRT and NSRF, Greece; ISF, MINERVA, GIF, DIP and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; FOM and NWO, Netherlands; BRF and RCN, Norway; MNiSW, Poland; GRICES and FCT, Portugal; MERYS (MECTS), Romania; MES of Rus-sia and ROSATOM, RusRus-sian Federation; JINR; MSTD, Serbia; MSSR, Slovakia; ARRS and MVZT, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SER, SNSF and Can-tons of Bern and Geneva, Switzerland; NSC, Taiwan; TAEK, Turkey; STFC, the Royal Society and Lever-hulme Trust, United Kingdom; DOE and NSF, United States of America.

The crucial computing support from all WLCG part-ners is acknowledged gratefully, in particular from CERN and the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Tai-wan), RAL (UK) and BNL (USA) and in the Tier-2 fa-cilities worldwide.

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THE ATLAS COLLABORATION

G. Aad48_{, T. Abajyan}21_{, B. Abbott}112_{, J. Abdallah}12_{, S. Abdel Khalek}116_{, O. Abdinov}11_{, R. Aben}106_{, B. Abi}113_,

M. Abolins89_{, O.S. AbouZeid}159_{, H. Abramowicz}154_{, H. Abreu}137_{, Y. Abulaiti}147a,147b_{, B.S. Acharya}165a,165b,a_,

L. Adamczyk38a_{, D.L. Adams}25_{, T.N. Addy}56_{, J. Adelman}177_{, S. Adomeit}99_{, T. Adye}130_{, S. Aefsky}23_,

J.A. Aguilar-Saavedra125b,b_{, M. Agustoni}17_{, S.P. Ahlen}22_{, A. Ahmad}149_{, M. Ahsan}41_{, G. Aielli}134a,134b_,

T.P.A. ˚Akesson80_{, G. Akimoto}156_{, A.V. Akimov}95_{, M.A. Alam}76_{, J. Albert}170_{, S. Albrand}55_,

M.J. Alconada Verzini70_{, M. Aleksa}30_{, I.N. Aleksandrov}64_{, F. Alessandria}90a_{, C. Alexa}26a_{, G. Alexander}154_,

G. Alexandre49_{, T. Alexopoulos}10_{, M. Alhroob}165a,165c_{, M. Aliev}16_{, G. Alimonti}90a_{, L. Alio}84_{, J. Alison}31_,

B.M.M. Allbrooke18_{, L.J. Allison}71_{, P.P. Allport}73_{, S.E. Allwood-Spiers}53_{, J. Almond}83_{, A. Aloisio}103a,103b_,

R. Alon173_{, A. Alonso}36_{, F. Alonso}70_{, A. Altheimer}35_{, B. Alvarez Gonzalez}89_{, M.G. Alviggi}103a,103b_{, K. Amako}65_,

Y. Amaral Coutinho24a, C. Amelung23, V.V. Ammosov129,∗, S.P. Amor Dos Santos125a, A. Amorim125a,c, S. Amoroso48, N. Amram154, C. Anastopoulos30, L.S. Ancu17, N. Andari30, T. Andeen35, C.F. Anders58b, G. Anders58a, K.J. Anderson31, A. Andreazza90a,90b, V. Andrei58a, X.S. Anduaga70, S. Angelidakis9, P. Anger44, A. Angerami35, F. Anghinolfi30, A.V. Anisenkov108, N. Anjos125a, A. Annovi47, A. Antonaki9, M. Antonelli47, A. Antonov97_{, J. Antos}145b_{, F. Anulli}133a_{, M. Aoki}102_{, L. Aperio Bella}18_{, R. Apolle}119,d_{, G. Arabidze}89_,

I. Aracena144_{, Y. Arai}65_{, A.T.H. Arce}45_{, S. Arfaoui}149_{, J-F. Arguin}94_{, S. Argyropoulos}42_{, E. Arik}19a,∗_{, M. Arik}19a_,

A.J. Armbruster88_{, O. Arnaez}82_{, V. Arnal}81_{, A. Artamonov}96_{, G. Artoni}133a,133b_{, D. Arutinov}21_{, S. Asai}156_,

N. Asbah94_{, S. Ask}28_{, B. ˚Asman}147a,147b_{, L. Asquith}6_{, K. Assamagan}25_{, R. Astalos}145a_{, A. Astbury}170_,

M. Atkinson166_{, N.B. Atlay}142_{, B. Auerbach}6_{, E. Auge}116_{, K. Augsten}127_{, M. Aurousseau}146b_{, G. Avolio}30_,

D. Axen169_{, G. Azuelos}94,e_{, Y. Azuma}156_{, M.A. Baak}30_{, C. Bacci}135a,135b_{, A.M. Bach}15_{, H. Bachacou}137_,

K. Bachas155_{, M. Backes}49_{, M. Backhaus}21_{, J. Backus Mayes}144_{, E. Badescu}26a_{, P. Bagiacchi}133a,133b_,

P. Bagnaia133a,133b_{, Y. Bai}33a_{, D.C. Bailey}159_{, T. Bain}35_{, J.T. Baines}130_{, O.K. Baker}177_{, S. Baker}77_{, P. Balek}128_,

F. Balli137_{, E. Banas}39_{, Sw. Banerjee}174_{, D. Banfi}30_{, A. Bangert}151_{, V. Bansal}170_{, H.S. Bansil}18_{, L. Barak}173_,

S.P. Baranov95_{, T. Barber}48_{, E.L. Barberio}87_{, D. Barberis}50a,50b_{, M. Barbero}84_{, D.Y. Bardin}64_{, T. Barillari}100_,

M. Barisonzi176_{, T. Barklow}144_{, N. Barlow}28_{, B.M. Barnett}130_{, R.M. Barnett}15_{, A. Baroncelli}135a_{, G. Barone}49_,

A.J. Barr119, F. Barreiro81, J. Barreiro Guimar˜aes da Costa57, R. Bartoldus144, A.E. Barton71, V. Bartsch150, A. Basye166, R.L. Bates53, L. Batkova145a, J.R. Batley28, M. Battistin30, F. Bauer137, H.S. Bawa144,f, S. Beale99, T. Beau79, P.H. Beauchemin162, R. Beccherle50a, P. Bechtle21, H.P. Beck17, K. Becker176, S. Becker99,

M. Beckingham139, K.H. Becks176, A.J. Beddall19c, A. Beddall19c, S. Bedikian177, V.A. Bednyakov64, C.P. Bee84, L.J. Beemster106_{, T.A. Beermann}176_{, M. Begel}25_{, C. Belanger-Champagne}86_{, P.J. Bell}49_{, W.H. Bell}49_{, G. Bella}154_,

L. Bellagamba20a_{, A. Bellerive}29_{, M. Bellomo}30_{, A. Belloni}57_{, O.L. Beloborodova}108,g_{, K. Belotskiy}97_,

O. Beltramello30_{, O. Benary}154_{, D. Benchekroun}136a_{, K. Bendtz}147a,147b_{, N. Benekos}166_{, Y. Benhammou}154_,

E. Benhar Noccioli49_{, J.A. Benitez Garcia}160b_{, D.P. Benjamin}45_{, J.R. Bensinger}23_{, K. Benslama}131_,

S. Bentvelsen106_{, D. Berge}30_{, E. Bergeaas Kuutmann}16_{, N. Berger}5_{, F. Berghaus}170_{, E. Berglund}106_{, J. Beringer}15_,

C. Bernard22_{, P. Bernat}77_{, R. Bernhard}48_{, C. Bernius}78_{, F.U. Bernlochner}170_{, T. Berry}76_{, C. Bertella}84_,

F. Bertolucci123a,123b_{, M.I. Besana}90a,90b_{, G.J. Besjes}105_{, O. Bessidskaia}147a,147b_{, N. Besson}137_{, S. Bethke}100_,

W. Bhimji46_{, R.M. Bianchi}124_{, L. Bianchini}23_{, M. Bianco}72a,72b_{, O. Biebel}99_{, S.P. Bieniek}77_{, K. Bierwagen}54_,

J. Biesiada15_{, M. Biglietti}135a_{, J. Bilbao De Mendizabal}49_{, H. Bilokon}47_{, M. Bindi}20a,20b_{, S. Binet}116_{, A. Bingul}19c_,

C. Bini133a,133b_{, B. Bittner}100_{, C.W. Black}151_{, J.E. Black}144_{, K.M. Black}22_{, D. Blackburn}139_{, R.E. Blair}6_,

J.-B. Blanchard137, T. Blazek145a, I. Bloch42, C. Blocker23, J. Blocki39, W. Blum82,∗, U. Blumenschein54, G.J. Bobbink106, V.S. Bobrovnikov108, S.S. Bocchetta80, A. Bocci45, C.R. Boddy119, M. Boehler48, J. Boek176, T.T. Boek176, N. Boelaert36, J.A. Bogaerts30, A.G. Bogdanchikov108, A. Bogouch91,∗, C. Bohm147a, J. Bohm126, V. Boisvert76, T. Bold38a, V. Boldea26a, N.M. Bolnet137, M. Bomben79, M. Bona75, M. Boonekamp137, S. Bordoni79, C. Borer17, A. Borisov129, G. Borissov71, M. Borri83, S. Borroni42, J. Bortfeldt99, V. Bortolotto135a,135b, K. Bos106, D. Boscherini20a_{, M. Bosman}12_{, H. Boterenbrood}106_{, J. Bouchami}94_{, J. Boudreau}124_{, E.V. Bouhova-Thacker}71_,

D. Boumediene34_{, C. Bourdarios}116_{, N. Bousson}84_{, S. Boutouil}136d_{, A. Boveia}31_{, J. Boyd}30_{, I.R. Boyko}64_,

I. Bozovic-Jelisavcic13b_{, J. Bracinik}18_{, P. Branchini}135a_{, A. Brandt}8_{, G. Brandt}15_{, O. Brandt}54_{, U. Bratzler}157_,

B. Brau85_{, J.E. Brau}115_{, H.M. Braun}176,∗_{, S.F. Brazzale}165a,165c_{, B. Brelier}159_{, J. Bremer}30_{, K. Brendlinger}121_,

R. Brenner167_{, S. Bressler}173_{, T.M. Bristow}146c_{, D. Britton}53_{, F.M. Brochu}28_{, I. Brock}21_{, R. Brock}89_{, F. Broggi}90a_,

C. Bromberg89_{, J. Bronner}100_{, G. Brooijmans}35_{, T. Brooks}76_{, W.K. Brooks}32b_{, E. Brost}115_{, G. Brown}83_,

J. Brown55_{, P.A. Bruckman de Renstrom}39_{, D. Bruncko}145b_{, R. Bruneliere}48_{, S. Brunet}60_{, A. Bruni}20a_{, G. Bruni}20a_,

M. Bruschi20a_{, L. Bryngemark}80_{, T. Buanes}14_{, Q. Buat}55_{, F. Bucci}49_{, J. Buchanan}119_{, P. Buchholz}142_,

R.M. Buckingham119_{, A.G. Buckley}46_{, S.I. Buda}26a_{, I.A. Budagov}64_{, B. Budick}109_{, L. Bugge}118_{, O. Bulekov}97_,

V. B¨uscher82, P. Bussey53, C.P. Buszello167, B. Butler57, J.M. Butler22, C.M. Buttar53, J.M. Butterworth77, W. Buttinger28, M. Byszewski10, S. Cabrera Urb´an168, D. Caforio20a,20b, O. Cakir4a, P. Calafiura15, G. Calderini79, P. Calfayan99_{, R. Calkins}107_{, L.P. Caloba}24a_{, R. Caloi}133a,133b_{, D. Calvet}34_{, S. Calvet}34_{, R. Camacho Toro}49_,

P. Camarri134a,134b_{, D. Cameron}118_{, L.M. Caminada}15_{, R. Caminal Armadans}12_{, S. Campana}30_{, M. Campanelli}77_,

V. Canale103a,103b_{, F. Canelli}31_{, A. Canepa}160a_{, J. Cantero}81_{, R. Cantrill}76_{, T. Cao}40_{, M.D.M. Capeans Garrido}30_,

I. Caprini26a_{, M. Caprini}26a_{, D. Capriotti}100_{, M. Capua}37a,37b_{, R. Caputo}82_{, R. Cardarelli}134a_{, T. Carli}30_,

G. Carlino103a_{, L. Carminati}90a,90b_{, S. Caron}105_{, E. Carquin}32b_{, G.D. Carrillo-Montoya}146c_{, A.A. Carter}75_,

J.R. Carter28_{, J. Carvalho}125a,h_{, D. Casadei}77_{, M.P. Casado}12_{, M. Cascella}123a,123b_{, C. Caso}50a,50b,∗_,

E. Castaneda-Miranda174_{, A. Castelli}106_{, V. Castillo Gimenez}168_{, N.F. Castro}125a_{, G. Cataldi}72a_{, P. Catastini}57_,

A. Catinaccio30_{, J.R. Catmore}30_{, A. Cattai}30_{, G. Cattani}134a,134b_{, S. Caughron}89_{, V. Cavaliere}166_{, D. Cavalli}90a_,

M. Cavalli-Sforza12_{, V. Cavasinni}123a,123b_{, F. Ceradini}135a,135b_{, B. Cerio}45_{, A.S. Cerqueira}24b_{, A. Cerri}15_,

L. Cerrito75_{, F. Cerutti}15_{, A. Cervelli}17_{, S.A. Cetin}19b_{, A. Chafaq}136a_{, D. Chakraborty}107_{, I. Chalupkova}128_,

K. Chan3, P. Chang166, B. Chapleau86, J.D. Chapman28, J.W. Chapman88, D.G. Charlton18, V. Chavda83, C.A. Chavez Barajas30, S. Cheatham86, S. Chekanov6, S.V. Chekulaev160a, G.A. Chelkov64, M.A. Chelstowska88, C. Chen63, H. Chen25, S. Chen33c, X. Chen174, Y. Chen35, Y. Cheng31, A. Cheplakov64,

R. Cherkaoui El Moursli136e, V. Chernyatin25,∗, E. Cheu7, L. Chevalier137, V. Chiarella47, G. Chiefari103a,103b, J.T. Childers30, A. Chilingarov71, G. Chiodini72a, A.S. Chisholm18, R.T. Chislett77, A. Chitan26a, M.V. Chizhov64, G. Choudalakis31_{, S. Chouridou}9_{, B.K.B. Chow}99_{, I.A. Christidi}77_{, A. Christov}48_{, D. Chromek-Burckhart}30_,

M.L. Chu152_{, J. Chudoba}126_{, G. Ciapetti}133a,133b_{, A.K. Ciftci}4a_{, R. Ciftci}4a_{, D. Cinca}62_{, V. Cindro}74_{, A. Ciocio}15_,

M. Cirilli88_{, P. Cirkovic}13b_{, Z.H. Citron}173_{, M. Citterio}90a_{, M. Ciubancan}26a_{, A. Clark}49_{, P.J. Clark}46_,

R.N. Clarke15_{, J.C. Clemens}84_{, B. Clement}55_{, C. Clement}147a,147b_{, Y. Coadou}84_{, M. Cobal}165a,165c_{, A. Coccaro}139_,

J. Cochran63_{, S. Coelli}90a_{, L. Coffey}23_{, J.G. Cogan}144_{, J. Coggeshall}166_{, J. Colas}5_{, B. Cole}35_{, S. Cole}107_,

A.P. Colijn106_{, C. Collins-Tooth}53_{, J. Collot}55_{, T. Colombo}120a,120b_{, G. Colon}85_{, G. Compostella}100_,

P. Conde Mui˜no125a_{, E. Coniavitis}167_{, M.C. Conidi}12_{, S.M. Consonni}90a,90b_{, V. Consorti}48_{, S. Constantinescu}26a_,

C. Conta120a,120b_{, G. Conti}57_{, F. Conventi}103a,i_{, M. Cooke}15_{, B.D. Cooper}77_{, A.M. Cooper-Sarkar}119_,

N.J. Cooper-Smith76_{, K. Copic}15_{, T. Cornelissen}176_{, M. Corradi}20a_{, F. Corriveau}86,j_{, A. Corso-Radu}164_,

A. Cortes-Gonzalez166_{, G. Cortiana}100_{, G. Costa}90a_{, M.J. Costa}168_{, D. Costanzo}140_{, D. Cˆot´e}8_{, G. Cottin}32a_,

L. Courneyea170, G. Cowan76, B.E. Cox83, K. Cranmer109, S. Cr´ep´e-Renaudin55, F. Crescioli79, M. Cristinziani21, G. Crosetti37a,37b, C.-M. Cuciuc26a, C. Cuenca Almenar177, T. Cuhadar Donszelmann140, J. Cummings177, M. Curatolo47, C. Cuthbert151, H. Czirr142, P. Czodrowski44, Z. Czyczula177, S. D’Auria53, M. D’Onofrio73, A. D’Orazio133a,133b, M.J. Da Cunha Sargedas De Sousa125a, C. Da Via83, W. Dabrowski38a, A. Dafinca119, T. Dai88_{, F. Dallaire}94_{, C. Dallapiccola}85_{, M. Dam}36_{, D.S. Damiani}138_{, A.C. Daniells}18_{, H.O. Danielsson}30_,

V. Dao105_{, G. Darbo}50a_{, G.L. Darlea}26c_{, S, Darmora}8_{, J.A. Dassoulas}42_{, W. Davey}21_{, C. David}170_{, T. Davidek}128_,

E. Davies119,d_{, M. Davies}94_{, O. Davignon}79_{, A.R. Davison}77_{, Y. Davygora}58a_{, E. Dawe}143_{, I. Dawson}140_,

R.K. Daya-Ishmukhametova23_{, K. De}8_{, R. de Asmundis}103a_{, S. De Castro}20a,20b_{, S. De Cecco}79_{, J. de Graat}99_,

N. De Groot105_{, P. de Jong}106_{, C. De La Taille}116_{, H. De la Torre}81_{, F. De Lorenzi}63_{, L. De Nooij}106_,

D. De Pedis133a_{, A. De Salvo}133a_{, U. De Sanctis}165a,165c_{, A. De Santo}150_{, J.B. De Vivie De Regie}116_,

G. De Zorzi133a,133b_{, W.J. Dearnaley}71_{, R. Debbe}25_{, C. Debenedetti}46_{, B. Dechenaux}55_{, D.V. Dedovich}64_,

J. Degenhardt121_{, J. Del Peso}81_{, T. Del Prete}123a,123b_{, T. Delemontex}55_{, M. Deliyergiyev}74_{, A. Dell’Acqua}30_,

L. Dell’Asta22_{, M. Della Pietra}103a,i_{, D. della Volpe}103a,103b_{, M. Delmastro}5_{, P.A. Delsart}55_{, C. Deluca}106_,

S. Demers177_{, M. Demichev}64_{, A. Demilly}79_{, B. Demirkoz}12,k_{, S.P. Denisov}129_{, D. Derendarz}39_{, J.E. Derkaoui}136d_,

F. Derue79_{, P. Dervan}73_{, K. Desch}21_{, P.O. Deviveiros}106_{, A. Dewhurst}130_{, B. DeWilde}149_{, S. Dhaliwal}106_,

R. Dhullipudi78,l, A. Di Ciaccio134a,134b, L. Di Ciaccio5, C. Di Donato103a,103b, A. Di Girolamo30, B. Di Girolamo30, S. Di Luise135a,135b, A. Di Mattia153, B. Di Micco135a,135b, R. Di Nardo47, A. Di Simone48, R. Di Sipio20a,20b, M.A. Diaz32a, E.B. Diehl88, J. Dietrich42, T.A. Dietzsch58a, S. Diglio87, K. Dindar Yagci40, J. Dingfelder21, F. Dinut26a, C. Dionisi133a,133b, P. Dita26a, S. Dita26a, F. Dittus30, F. Djama84, T. Djobava51b, M.A.B. do Vale24c, A. Do Valle Wemans125a,m_{, T.K.O. Doan}5_{, D. Dobos}30_{, E. Dobson}77_{, J. Dodd}35_{, C. Doglioni}49_{, T. Doherty}53_,

T. Dohmae156_{, Y. Doi}65,∗_{, J. Dolejsi}128_{, Z. Dolezal}128_{, B.A. Dolgoshein}97,∗_{, M. Donadelli}24d_{, J. Donini}34_,

J. Dopke30_{, A. Doria}103a_{, A. Dos Anjos}174_{, A. Dotti}123a,123b_{, M.T. Dova}70_{, A.T. Doyle}53_{, M. Dris}10_{, J. Dubbert}88_,

S. Dube15_{, E. Dubreuil}34_{, E. Duchovni}173_{, G. Duckeck}99_{, D. Duda}176_{, A. Dudarev}30_{, F. Dudziak}63_{, L. Duflot}116_,

M-A. Dufour86_{, L. Duguid}76_{, M. D¨uhrssen}30_{, M. Dunford}58a_{, H. Duran Yildiz}4a_{, M. D¨uren}52_{, M. Dwuznik}38a_,

J. Ebke99_{, W. Edson}2_{, C.A. Edwards}76_{, N.C. Edwards}53_{, W. Ehrenfeld}21_{, T. Eifert}144_{, G. Eigen}14_{, K. Einsweiler}15_,

E. Eisenhandler75_{, T. Ekelof}167_{, M. El Kacimi}136c_{, M. Ellert}167_{, S. Elles}5_{, F. Ellinghaus}82_{, K. Ellis}75_{, N. Ellis}30_,

J. Elmsheuser99_{, M. Elsing}30_{, D. Emeliyanov}130_{, Y. Enari}156_{, O.C. Endner}82_{, R. Engelmann}149_{, A. Engl}99_,

J. Erdmann177_{, A. Ereditato}17_{, D. Eriksson}147a_{, J. Ernst}2_{, M. Ernst}25_{, J. Ernwein}137_{, D. Errede}166_{, S. Errede}166_,

A.I. Etienvre137, E. Etzion154, D. Evangelakou54, H. Evans60, L. Fabbri20a,20b, C. Fabre30, G. Facini30, R.M. Fakhrutdinov129, S. Falciano133a, Y. Fang33a, M. Fanti90a,90b, A. Farbin8, A. Farilla135a, T. Farooque159, S. Farrell164_{, S.M. Farrington}171_{, P. Farthouat}30_{, F. Fassi}168_{, P. Fassnacht}30_{, D. Fassouliotis}9_{, B. Fatholahzadeh}159_,

A. Favareto90a,90b_{, L. Fayard}116_{, P. Federic}145a_{, O.L. Fedin}122_{, W. Fedorko}169_{, M. Fehling-Kaschek}48_{, L. Feligioni}84_,

C. Feng33d_{, E.J. Feng}6_{, H. Feng}88_{, A.B. Fenyuk}129_{, J. Ferencei}145b_{, W. Fernando}6_{, S. Ferrag}53_{, J. Ferrando}53_,

V. Ferrara42_{, A. Ferrari}167_{, P. Ferrari}106_{, R. Ferrari}120a_{, D.E. Ferreira de Lima}53_{, A. Ferrer}168_{, D. Ferrere}49_,

C. Ferretti88_{, A. Ferretto Parodi}50a,50b_{, M. Fiascaris}31_{, F. Fiedler}82_{, A. Filipˇciˇc}74_{, M. Filipuzzi}42_{, F. Filthaut}105_,

M. Fincke-Keeler170_{, K.D. Finelli}45_{, M.C.N. Fiolhais}125a,h_{, L. Fiorini}168_{, A. Firan}40_{, J. Fischer}176_{, M.J. Fisher}110_,

E.A. Fitzgerald23_{, M. Flechl}48_{, I. Fleck}142_{, P. Fleischmann}175_{, S. Fleischmann}176_{, G.T. Fletcher}140_{, G. Fletcher}75_,

T. Flick176_{, A. Floderus}80_{, L.R. Flores Castillo}174_{, A.C. Florez Bustos}160b_{, M.J. Flowerdew}100_{, T. Fonseca Martin}17_,

A. Formica137_{, A. Forti}83_{, D. Fortin}160a_{, D. Fournier}116_{, H. Fox}71_{, P. Francavilla}12_{, M. Franchini}20a,20b_,

S. Franchino30_{, D. Francis}30_{, M. Franklin}57_{, S. Franz}61_{, M. Fraternali}120a,120b_{, S. Fratina}121_{, S.T. French}28_,

C. Friedrich42, F. Friedrich44, D. Froidevaux30, J.A. Frost28, C. Fukunaga157, E. Fullana Torregrosa128, B.G. Fulsom144, J. Fuster168, C. Gabaldon30, O. Gabizon173, A. Gabrielli20a,20b, A. Gabrielli133a,133b,

S. Gadatsch106, T. Gadfort25, S. Gadomski49, G. Gagliardi50a,50b, P. Gagnon60, C. Galea99, B. Galhardo125a, E.J. Gallas119, V. Gallo17, B.J. Gallop130, P. Gallus127, G.A.G.K. Galster36, K.K. Gan110, R.P. Gandrajula62, Y.S. Gao144,f, A. Gaponenko15, F.M. Garay Walls46, F. Garberson177, C. Garc´ıa168, J.E. Garc´ıa Navarro168, M. Garcia-Sciveres15_{, R.W. Gardner}31_{, N. Garelli}144_{, V. Garonne}30_{, C. Gatti}47_{, G. Gaudio}120a_{, B. Gaur}142_,

L. Gauthier94_{, P. Gauzzi}133a,133b_{, I.L. Gavrilenko}95_{, C. Gay}169_{, G. Gaycken}21_{, E.N. Gazis}10_{, P. Ge}33d,n_{, Z. Gecse}169_,

C.N.P. Gee130_{, D.A.A. Geerts}106_{, Ch. Geich-Gimbel}21_{, K. Gellerstedt}147a,147b_{, C. Gemme}50a_{, A. Gemmell}53_,

M.H. Genest55_{, S. Gentile}133a,133b_{, M. George}54_{, S. George}76_{, D. Gerbaudo}164_{, A. Gershon}154_{, H. Ghazlane}136b_,

N. Ghodbane34_{, B. Giacobbe}20a_{, S. Giagu}133a,133b_{, V. Giangiobbe}12_{, P. Giannetti}123a,123b_{, F. Gianotti}30_,

B. Gibbard25_{, S.M. Gibson}76_{, M. Gilchriese}15_{, T.P.S. Gillam}28_{, D. Gillberg}30_{, A.R. Gillman}130_{, D.M. Gingrich}3,e_,

N. Giokaris9_{, M.P. Giordani}165c_{, R. Giordano}103a,103b_{, F.M. Giorgi}16_{, P. Giovannini}100_{, P.F. Giraud}137_,

D. Giugni90a_{, C. Giuliani}48_{, M. Giunta}94_{, B.K. Gjelsten}118_{, I. Gkialas}155,o_{, L.K. Gladilin}98_{, C. Glasman}81_,

J. Glatzer21_{, A. Glazov}42_{, G.L. Glonti}64_{, J.R. Goddard}75_{, J. Godfrey}143_{, J. Godlewski}30_{, M. Goebel}42_,

C. Goeringer82_{, S. Goldfarb}88_{, T. Golling}177_{, D. Golubkov}129_{, A. Gomes}125a,c_{, L.S. Gomez Fajardo}42_{, R. Gon¸calo}76_,

J. Goncalves Pinto Firmino Da Costa42, L. Gonella21, S. Gonz´alez de la Hoz168, G. Gonzalez Parra12,

M.L. Gonzalez Silva27, S. Gonzalez-Sevilla49, J.J. Goodson149, L. Goossens30, P.A. Gorbounov96, H.A. Gordon25, I. Gorelov104, G. Gorfine176, B. Gorini30, E. Gorini72a,72b, A. Goriˇsek74, E. Gornicki39, A.T. Goshaw6,

C. G¨ossling43, M.I. Gostkin64, I. Gough Eschrich164, M. Gouighri136a, D. Goujdami136c, M.P. Goulette49, A.G. Goussiou139_{, C. Goy}5_{, S. Gozpinar}23_{, H.M.X. Grabas}137_{, L. Graber}54_{, I. Grabowska-Bold}38a_,

P. Grafstr¨om20a,20b_{, K-J. Grahn}42_{, E. Gramstad}118_{, F. Grancagnolo}72a_{, S. Grancagnolo}16_{, V. Grassi}149_,

V. Gratchev122_{, H.M. Gray}30_{, J.A. Gray}149_{, E. Graziani}135a_{, O.G. Grebenyuk}122_{, T. Greenshaw}73_,

Z.D. Greenwood78,l_{, K. Gregersen}36_{, I.M. Gregor}42_{, P. Grenier}144_{, J. Griffiths}8_{, N. Grigalashvili}64_{, A.A. Grillo}138_,

K. Grimm71_{, S. Grinstein}12,p_{, Ph. Gris}34_{, Y.V. Grishkevich}98_{, J.-F. Grivaz}116_{, J.P. Grohs}44_{, A. Grohsjean}42_,

E. Gross173_{, J. Grosse-Knetter}54_{, J. Groth-Jensen}173_{, K. Grybel}142_{, F. Guescini}49_{, D. Guest}177_{, O. Gueta}154_,

C. Guicheney34_{, E. Guido}50a,50b_{, T. Guillemin}116_{, S. Guindon}2_{, U. Gul}53_{, J. Gunther}127_{, J. Guo}35_{, S. Gupta}119_,

P. Gutierrez112_{, N.G. Gutierrez Ortiz}53_{, N. Guttman}154_{, O. Gutzwiller}174_{, C. Guyot}137_{, C. Gwenlan}119_,

C.B. Gwilliam73_{, A. Haas}109_{, S. Haas}30_{, C. Haber}15_{, H.K. Hadavand}8_{, P. Haefner}21_{, Z. Hajduk}39_{, H. Hakobyan}178_,

D. Hall119_{, G. Halladjian}62_{, K. Hamacher}176_{, P. Hamal}114_{, K. Hamano}87_{, M. Hamer}54_{, A. Hamilton}146a,q_,

S. Hamilton162_{, L. Han}33b_{, K. Hanagaki}117_{, K. Hanawa}156_{, M. Hance}15_{, C. Handel}82_{, P. Hanke}58a_{, J.R. Hansen}36_,

J.B. Hansen36, J.D. Hansen36, P.H. Hansen36, P. Hansson144, K. Hara161, A.S. Hard174, T. Harenberg176, S. Harkusha91, D. Harper88, R.D. Harrington46, O.M. Harris139, J. Hartert48, F. Hartjes106, A. Harvey56, S. Hasegawa102, Y. Hasegawa141, S. Hassani137, S. Haug17, M. Hauschild30, R. Hauser89, M. Havranek21, C.M. Hawkes18, R.J. Hawkings30, A.D. Hawkins80, T. Hayashi161, D. Hayden89, C.P. Hays119, H.S. Hayward73, S.J. Haywood130_{, S.J. Head}18_{, T. Heck}82_{, V. Hedberg}80_{, L. Heelan}8_{, S. Heim}121_{, B. Heinemann}15_{, S. Heisterkamp}36_,

J. Hejbal126_{, L. Helary}22_{, C. Heller}99_{, M. Heller}30_{, S. Hellman}147a,147b_{, D. Hellmich}21_{, C. Helsens}30_{, J. Henderson}119_,

R.C.W. Henderson71_{, A. Henrichs}177_{, A.M. Henriques Correia}30_{, S. Henrot-Versille}116_{, C. Hensel}54_{, G.H. Herbert}16_,

C.M. Hernandez8_{, Y. Hern´andez Jim´enez}168_{, R. Herrberg-Schubert}16_{, G. Herten}48_{, R. Hertenberger}99_{, L. Hervas}30_,

G.G. Hesketh77_{, N.P. Hessey}106_{, R. Hickling}75_{, E. Hig´on-Rodriguez}168_{, J.C. Hill}28_{, K.H. Hiller}42_{, S. Hillert}21_,

S.J. Hillier18_{, I. Hinchliffe}15_{, E. Hines}121_{, M. Hirose}117_{, D. Hirschbuehl}176_{, J. Hobbs}149_{, N. Hod}106_,

M.C. Hodgkinson140_{, P. Hodgson}140_{, A. Hoecker}30_{, M.R. Hoeferkamp}104_{, J. Hoffman}40_{, D. Hoffmann}84_,

J.I. Hofmann58a_{, M. Hohlfeld}82_{, S.O. Holmgren}147a_{, J.L. Holzbauer}89_{, T.M. Hong}121_{, L. Hooft van Huysduynen}109_,

J-Y. Hostachy55_{, S. Hou}152_{, A. Hoummada}136a_{, J. Howard}119_{, J. Howarth}83_{, M. Hrabovsky}114_{, I. Hristova}16_,

A. Huettmann42, T.B. Huffman119, E.W. Hughes35, G. Hughes71, M. Huhtinen30, T.A. H¨ulsing82, M. Hurwitz15, N. Huseynov64,r, J. Huston89, J. Huth57, G. Iacobucci49, G. Iakovidis10, I. Ibragimov142, L. Iconomidou-Fayard116, J. Idarraga116_{, P. Iengo}103a_{, O. Igonkina}106_{, Y. Ikegami}65_{, K. Ikematsu}142_{, M. Ikeno}65_{, D. Iliadis}155_{, N. Ilic}159_,

T. Ince100_{, P. Ioannou}9_{, M. Iodice}135a_{, K. Iordanidou}9_{, V. Ippolito}133a,133b_{, A. Irles Quiles}168_{, C. Isaksson}167_,

M. Ishino67_{, M. Ishitsuka}158_{, R. Ishmukhametov}110_{, C. Issever}119_{, S. Istin}19a_{, A.V. Ivashin}129_{, W. Iwanski}39_,

H. Iwasaki65_{, J.M. Izen}41_{, V. Izzo}103a_{, B. Jackson}121_{, J.N. Jackson}73_{, P. Jackson}1_{, M.R. Jaekel}30_{, V. Jain}2_,

K. Jakobs48_{, S. Jakobsen}36_{, T. Jakoubek}126_{, J. Jakubek}127_{, D.O. Jamin}152_{, D.K. Jana}112_{, E. Jansen}77_{, H. Jansen}30_,

J. Janssen21_{, M. Janus}171_{, R.C. Jared}174_{, G. Jarlskog}80_{, L. Jeanty}57_{, G.-Y. Jeng}151_{, I. Jen-La Plante}31_,

D. Jennens87_{, P. Jenni}30_{, J. Jentzsch}43_{, C. Jeske}171_{, S. J´ez´equel}5_{, M.K. Jha}20a_{, H. Ji}174_{, W. Ji}82_{, J. Jia}149_,

Y. Jiang33b_{, M. Jimenez Belenguer}42_{, S. Jin}33a_{, O. Jinnouchi}158_{, M.D. Joergensen}36_{, D. Joffe}40_{, K.E. Johansson}147a_,

P. Johansson140_{, S. Johnert}42_{, K.A. Johns}7_{, K. Jon-And}147a,147b_{, G. Jones}171_{, R.W.L. Jones}71_{, T.J. Jones}73_,

P.M. Jorge125a_{, K.D. Joshi}83_{, J. Jovicevic}148_{, T. Jovin}13b_{, X. Ju}174_{, C.A. Jung}43_{, R.M. Jungst}30_{, P. Jussel}61_,

A. Juste Rozas12,p, M. Kaci168, A. Kaczmarska39, P. Kadlecik36, M. Kado116, H. Kagan110, M. Kagan57, E. Kajomovitz153, S. Kalinin176, S. Kama40, N. Kanaya156, M. Kaneda30, S. Kaneti28, T. Kanno158, V.A. Kantserov97, J. Kanzaki65, B. Kaplan109, A. Kapliy31, D. Kar53, K. Karakostas10, N Karastathis10, M. Karnevskiy82, S.N. Karpov64, V. Kartvelishvili71, A.N. Karyukhin129, L. Kashif174, G. Kasieczka58b,

R.D. Kass110, A. Kastanas14, Y. Kataoka156, A. Katre49, J. Katzy42, V. Kaushik7, K. Kawagoe69, T. Kawamoto156, G. Kawamura54_{, S. Kazama}156_{, V.F. Kazanin}108_{, M.Y. Kazarinov}64_{, R. Keeler}170_{, P.T. Keener}121_{, R. Kehoe}40_,

M. Keil54_{, J.S. Keller}139_{, H. Keoshkerian}5_{, O. Kepka}126_{, B.P. Kerˇsevan}74_{, S. Kersten}176_{, K. Kessoku}156_,

J. Keung159_{, F. Khalil-zada}11_{, H. Khandanyan}147a,147b_{, A. Khanov}113_{, D. Kharchenko}64_{, A. Khodinov}97_,

A. Khomich58a_{, T.J. Khoo}28_{, G. Khoriauli}21_{, A. Khoroshilov}176_{, V. Khovanskiy}96_{, E. Khramov}64_{, J. Khubua}51b_,

H. Kim147a,147b_{, S.H. Kim}161_{, N. Kimura}172_{, O. Kind}16_{, B.T. King}73_{, M. King}66_{, R.S.B. King}119_{, S.B. King}169_,

J. Kirk130_{, A.E. Kiryunin}100_{, T. Kishimoto}66_{, D. Kisielewska}38a_{, T. Kitamura}66_{, T. Kittelmann}124_{, K. Kiuchi}161_,

E. Kladiva145b_{, M. Klein}73_{, U. Klein}73_{, K. Kleinknecht}82_{, M. Klemetti}86_{, P. Klimek}147a,147b_{, A. Klimentov}25_,

R. Klingenberg43_{, J.A. Klinger}83_{, E.B. Klinkby}36_{, T. Klioutchnikova}30_{, P.F. Klok}105_{, E.-E. Kluge}58a_{, P. Kluit}106_,

S. Kluth100_{, E. Kneringer}61_{, E.B.F.G. Knoops}84_{, A. Knue}54_{, B.R. Ko}45_{, T. Kobayashi}156_{, M. Kobel}44_{, M. Kocian}144_,

P. Kodys128_{, S. Koenig}82_{, P. Koevesarki}21_{, T. Koffas}29_{, E. Koffeman}106_{, L.A. Kogan}119_{, S. Kohlmann}176_{, F. Kohn}54_,

Z. Kohout127, T. Kohriki65, T. Koi144, H. Kolanoski16, I. Koletsou90a, J. Koll89, A.A. Komar95, Y. Komori156, T. Kondo65, K. K¨oneke48, A.C. K¨onig105, T. Kono42,s, A.I. Kononov48, R. Konoplich109,t, N. Konstantinidis77, R. Kopeliansky153, S. Koperny38a, L. K¨opke82, A.K. Kopp48, K. Korcyl39, K. Kordas155, A. Korn46, A.A. Korol108, I. Korolkov12, E.V. Korolkova140, V.A. Korotkov129, O. Kortner100, S. Kortner100, V.V. Kostyukhin21, S. Kotov100, V.M. Kotov64_{, A. Kotwal}45_{, C. Kourkoumelis}9_{, V. Kouskoura}155_{, A. Koutsman}160a_{, R. Kowalewski}170_,

T.Z. Kowalski38a_{, W. Kozanecki}137_{, A.S. Kozhin}129_{, V. Kral}127_{, V.A. Kramarenko}98_{, G. Kramberger}74_,

M.W. Krasny79_{, A. Krasznahorkay}109_{, J.K. Kraus}21_{, A. Kravchenko}25_{, S. Kreiss}109_{, J. Kretzschmar}73_,

K. Kreutzfeldt52_{, N. Krieger}54_{, P. Krieger}159_{, K. Kroeninger}54_{, H. Kroha}100_{, J. Kroll}121_{, J. Kroseberg}21_{, J. Krstic}13a_,

U. Kruchonak64_{, H. Kr¨uger}21_{, T. Kruker}17_{, N. Krumnack}63_{, Z.V. Krumshteyn}64_{, A. Kruse}174_{, M.K. Kruse}45_,

M. Kruskal22_{, T. Kubota}87_{, S. Kuday}4a_{, S. Kuehn}48_{, A. Kugel}58c_{, T. Kuhl}42_{, V. Kukhtin}64_{, Y. Kulchitsky}91_,

S. Kuleshov32b_{, M. Kuna}79_{, J. Kunkle}121_{, A. Kupco}126_{, H. Kurashige}66_{, M. Kurata}161_{, Y.A. Kurochkin}91_,

V. Kus126_{, E.S. Kuwertz}148_{, M. Kuze}158_{, J. Kvita}143_{, R. Kwee}16_{, A. La Rosa}49_{, L. La Rotonda}37a,37b_{, L. Labarga}81_,

S. Lablak136a_{, C. Lacasta}168_{, F. Lacava}133a,133b_{, J. Lacey}29_{, H. Lacker}16_{, D. Lacour}79_{, V.R. Lacuesta}168_,

E. Ladygin64_{, R. Lafaye}5_{, B. Laforge}79_{, T. Lagouri}177_{, S. Lai}48_{, H. Laier}58a_{, E. Laisne}55_{, L. Lambourne}77_,

C.L. Lampen7_{, W. Lampl}7_{, E. Lan¸con}137_{, U. Landgraf}48_{, M.P.J. Landon}75_{, V.S. Lang}58a_{, C. Lange}42_,

A.J. Lankford164, F. Lanni25, K. Lantzsch30, A. Lanza120a, S. Laplace79, C. Lapoire21, J.F. Laporte137, T. Lari90a, A. Larner119, M. Lassnig30, P. Laurelli47, V. Lavorini37a,37b, W. Lavrijsen15, P. Laycock73, B.T. Le55, O. Le Dortz79, E. Le Guirriec84, E. Le Menedeu12, T. LeCompte6, F. Ledroit-Guillon55, C.A. Lee152, H. Lee106, J.S.H. Lee117, S.C. Lee152, L. Lee177, G. Lefebvre79, M. Lefebvre170, M. Legendre137, F. Legger99, C. Leggett15, A. Lehan73, M. Lehmacher21_{, G. Lehmann Miotto}30_{, A.G. Leister}177_{, M.A.L. Leite}24d_{, R. Leitner}128_{, D. Lellouch}173_,

B. Lemmer54_{, V. Lendermann}58a_{, K.J.C. Leney}146c_{, T. Lenz}106_{, G. Lenzen}176_{, B. Lenzi}30_{, K. Leonhardt}44_,

S. Leontsinis10_{, C. Leroy}94_{, J-R. Lessard}170_{, C.G. Lester}28_{, C.M. Lester}121_{, J. Levˆeque}5_{, D. Levin}88_,

L.J. Levinson173_{, A. Lewis}119_{, G.H. Lewis}109_{, A.M. Leyko}21_{, M. Leyton}16_{, B. Li}33b,u_{, B. Li}84_{, H. Li}149_{, H.L. Li}31_,

S. Li33b,v_{, X. Li}88_{, Z. Liang}119,w_{, H. Liao}34_{, B. Liberti}134a_{, P. Lichard}30_{, K. Lie}166_{, J. Liebal}21_{, W. Liebig}14_,

C. Limbach21_{, A. Limosani}87_{, M. Limper}62_{, S.C. Lin}152,x_{, F. Linde}106_{, B.E. Lindquist}149_{, J.T. Linnemann}89_,

E. Lipeles121_{, A. Lipniacka}14_{, M. Lisovyi}42_{, T.M. Liss}166_{, D. Lissauer}25_{, A. Lister}169_{, A.M. Litke}138_{, B. Liu}152_,

D. Liu152_{, J.B. Liu}33b_{, K. Liu}33b,y_{, L. Liu}88_{, M Liu}45_{, M. Liu}33b_{, Y. Liu}33b_{, M. Livan}120a,120b_{, S.S.A. Livermore}119_,

A. Lleres55_{, J. Llorente Merino}81_{, S.L. Lloyd}75_{, F. Lo Sterzo}133a,133b_{, E. Lobodzinska}42_{, P. Loch}7_{, W.S. Lockman}138_,

K. Lohwasser48, M. Lokajicek126, V.P. Lombardo5, R.E. Long71, L. Lopes125a, D. Lopez Mateos57,

B. Lopez Paredes140, J. Lorenz99, N. Lorenzo Martinez116, M. Losada163, P. Loscutoff15, M.J. Losty160a,∗, X. Lou41, A. Lounis116_{, K.F. Loureiro}163_{, J. Love}6_{, P.A. Love}71_{, A.J. Lowe}144,f_{, F. Lu}33a_{, H.J. Lubatti}139_{, C. Luci}133a,133b_,

A. Lucotte55_{, D. Ludwig}42_{, I. Ludwig}48_{, J. Ludwig}48_{, F. Luehring}60_{, W. Lukas}61_{, L. Luminari}133a_{, E. Lund}118_,

J. Lundberg147a,147b_{, O. Lundberg}147a,147b_{, B. Lund-Jensen}148_{, M. Lungwitz}82_{, D. Lynn}25_{, R. Lysak}126_,

E. Lytken80_{, H. Ma}25_{, L.L. Ma}33d_{, G. Maccarrone}47_{, A. Macchiolo}100_{, B. Maˇcek}74_{, J. Machado Miguens}125a_,

D. Macina30_{, R. Mackeprang}36_{, R. Madar}48_{, R.J. Madaras}15_{, H.J. Maddocks}71_{, W.F. Mader}44_{, A. Madsen}167_,

M. Maeno5_{, T. Maeno}25_{, L. Magnoni}164_{, E. Magradze}54_{, K. Mahboubi}48_{, J. Mahlstedt}106_{, S. Mahmoud}73_,

G. Mahout18_{, C. Maiani}137_{, C. Maidantchik}24a_{, A. Maio}125a,c_{, S. Majewski}115_{, Y. Makida}65_{, N. Makovec}116_,

P. Mal137,z_{, B. Malaescu}79_{, Pa. Malecki}39_{, P. Malecki}39_{, V.P. Maleev}122_{, F. Malek}55_{, U. Mallik}62_{, D. Malon}6_,

C. Malone144_{, S. Maltezos}10_{, V.M. Malyshev}108_{, S. Malyukov}30_{, J. Mamuzic}13b_{, L. Mandelli}90a_{, I. Mandi´c}74_,

R. Mandrysch62_{, J. Maneira}125a_{, A. Manfredini}100_{, L. Manhaes de Andrade Filho}24b_{, J.A. Manjarres Ramos}137_,

A. Mann99, P.M. Manning138, A. Manousakis-Katsikakis9, B. Mansoulie137, R. Mantifel86, L. Mapelli30, L. March168, J.F. Marchand29, F. Marchese134a,134b, G. Marchiori79, M. Marcisovsky126, C.P. Marino170,

C.N. Marques125a, F. Marroquim24a, Z. Marshall121, L.F. Marti17, S. Marti-Garcia168, B. Martin30, B. Martin89, J.P. Martin94, T.A. Martin171, V.J. Martin46, B. Martin dit Latour49, H. Martinez137, M. Martinez12,p,

S. Martin-Haugh150, A.C. Martyniuk170, M. Marx83, F. Marzano133a, A. Marzin112, L. Masetti82, T. Mashimo156, R. Mashinistov95_{, J. Masik}83_{, A.L. Maslennikov}108_{, I. Massa}20a,20b_{, N. Massol}5_{, P. Mastrandrea}149_,

A. Mastroberardino37a,37b_{, T. Masubuchi}156_{, H. Matsunaga}156_{, T. Matsushita}66_{, P. M¨attig}176_{, S. M¨attig}42_,

J. Mattmann82_{, C. Mattravers}119,d_{, J. Maurer}84_{, S.J. Maxfield}73_{, D.A. Maximov}108,g_{, R. Mazini}152_,

L. Mazzaferro134a,134b_{, M. Mazzanti}90a_{, S.P. Mc Kee}88_{, A. McCarn}166_{, R.L. McCarthy}149_{, T.G. McCarthy}29_,

N.A. McCubbin130_{, K.W. McFarlane}56,∗_{, J.A. Mcfayden}140_{, G. Mchedlidze}51b_{, T. Mclaughlan}18_{, S.J. McMahon}130_,

R.A. McPherson170,j_{, A. Meade}85_{, J. Mechnich}106_{, M. Mechtel}176_{, M. Medinnis}42_{, S. Meehan}31_,

R. Meera-Lebbai112_{, S. Mehlhase}36_{, A. Mehta}73_{, K. Meier}58a_{, C. Meineck}99_{, B. Meirose}80_{, C. Melachrinos}31_,

B.R. Mellado Garcia146c_{, F. Meloni}90a,90b_{, L. Mendoza Navas}163_{, A. Mengarelli}20a,20b_{, S. Menke}100_{, E. Meoni}162_,

K.M. Mercurio57_{, N. Meric}137_{, P. Mermod}49_{, L. Merola}103a,103b_{, C. Meroni}90a_{, F.S. Merritt}31_{, H. Merritt}110_,

A. Messina30,aa_{, J. Metcalfe}25_{, A.S. Mete}164_{, C. Meyer}82_{, C. Meyer}31_{, J-P. Meyer}137_{, J. Meyer}30_{, J. Meyer}54_,

S. Michal30, R.P. Middleton130, S. Migas73, L. Mijovi´c137, G. Mikenberg173, M. Mikestikova126, M. Mikuˇz74, D.W. Miller31, W.J. Mills169, C. Mills57, A. Milov173, D.A. Milstead147a,147b, D. Milstein173, A.A. Minaenko129, M. Mi˜nano Moya168, I.A. Minashvili64, A.I. Mincer109, B. Mindur38a, M. Mineev64, Y. Ming174, L.M. Mir12, G. Mirabelli133a, T. Mitani172, J. Mitrevski138, V.A. Mitsou168, S. Mitsui65, P.S. Miyagawa140, J.U. Mj¨ornmark80, T. Moa147a,147b_{, V. Moeller}28_{, S. Mohapatra}149_{, W. Mohr}48_{, R. Moles-Valls}168_{, A. Molfetas}30_{, K. M¨onig}42_,

C. Monini55_{, J. Monk}36_{, E. Monnier}84_{, J. Montejo Berlingen}12_{, F. Monticelli}70_{, S. Monzani}20a,20b_{, R.W. Moore}3_,

C. Mora Herrera49_{, A. Moraes}53_{, N. Morange}62_{, J. Morel}54_{, D. Moreno}82_{, M. Moreno Ll´acer}168_{, P. Morettini}50a_,

M. Morgenstern44_{, M. Morii}57_{, S. Moritz}82_{, A.K. Morley}148_{, G. Mornacchi}30_{, J.D. Morris}75_{, L. Morvaj}102_,

H.G. Moser100_{, M. Mosidze}51b_{, J. Moss}110_{, R. Mount}144_{, E. Mountricha}10,ab_{, S.V. Mouraviev}95,∗_{, E.J.W. Moyse}85_,

R.D. Mudd18_{, F. Mueller}58a_{, J. Mueller}124_{, K. Mueller}21_{, T. Mueller}28_{, T. Mueller}82_{, D. Muenstermann}49_,

Y. Munwes154_{, J.A. Murillo Quijada}18_{, W.J. Murray}130_{, I. Mussche}106_{, E. Musto}153_{, A.G. Myagkov}129,ac_,

M. Myska126_{, O. Nackenhorst}54_{, J. Nadal}12_{, K. Nagai}161_{, R. Nagai}158_{, Y. Nagai}84_{, K. Nagano}65_{, A. Nagarkar}110_,

Y. Nagasaka59_{, M. Nagel}100_{, A.M. Nairz}30_{, Y. Nakahama}30_{, K. Nakamura}65_{, T. Nakamura}156_{, I. Nakano}111_,

H. Namasivayam41_{, G. Nanava}21_{, A. Napier}162_{, R. Narayan}58b_{, M. Nash}77,d_{, T. Nattermann}21_{, T. Naumann}42_,

G. Navarro163_{, H.A. Neal}88_{, P.Yu. Nechaeva}95_{, T.J. Neep}83_{, A. Negri}120a,120b_{, G. Negri}30_{, M. Negrini}20a_,

S. Nektarijevic49, A. Nelson164, T.K. Nelson144, S. Nemecek126, P. Nemethy109, A.A. Nepomuceno24a, M. Nessi30,ad, M.S. Neubauer166, M. Neumann176, A. Neusiedl82, R.M. Neves109, P. Nevski25, F.M. Newcomer121, P.R. Newman18, D.H. Nguyen6, V. Nguyen Thi Hong137, R.B. Nickerson119, R. Nicolaidou137, B. Nicquevert30, J. Nielsen138,

N. Nikiforou35, A. Nikiforov16, V. Nikolaenko129,ac, I. Nikolic-Audit79, K. Nikolics49, K. Nikolopoulos18, P. Nilsson8, Y. Ninomiya156_{, A. Nisati}133a_{, R. Nisius}100_{, T. Nobe}158_{, L. Nodulman}6_{, M. Nomachi}117_{, I. Nomidis}155_,

S. Norberg112_{, M. Nordberg}30_{, J. Novakova}128_{, M. Nozaki}65_{, L. Nozka}114_{, K. Ntekas}10_{, A.-E. Nuncio-Quiroz}21_,

G. Nunes Hanninger87_{, T. Nunnemann}99_{, E. Nurse}77_{, B.J. O’Brien}46_{, D.C. O’Neil}143_{, V. O’Shea}53_{, L.B. Oakes}99_,

F.G. Oakham29,e_{, H. Oberlack}100_{, J. Ocariz}79_{, A. Ochi}66_{, M.I. Ochoa}77_{, S. Oda}69_{, S. Odaka}65_{, J. Odier}84_,

H. Ogren60_{, A. Oh}83_{, S.H. Oh}45_{, C.C. Ohm}30_{, T. Ohshima}102_{, W. Okamura}117_{, H. Okawa}25_{, Y. Okumura}31_,

T. Okuyama156_{, A. Olariu}26a_{, A.G. Olchevski}64_{, S.A. Olivares Pino}46_{, M. Oliveira}125a,h_{, D. Oliveira Damazio}25_,

E. Oliver Garcia168_{, D. Olivito}121_{, A. Olszewski}39_{, J. Olszowska}39_{, A. Onofre}125a,ae_{, P.U.E. Onyisi}31,af_,

C.J. Oram160a_{, M.J. Oreglia}31_{, Y. Oren}154_{, D. Orestano}135a,135b_{, N. Orlando}72a,72b_{, C. Oropeza Barrera}53_,

R.S. Orr159_{, B. Osculati}50a,50b_{, R. Ospanov}121_{, G. Otero y Garzon}27_{, H. Otono}69_{, J.P. Ottersbach}106_,