CMS PAPER CFT-09-005

CMS Paper

2010/02/16

Measurement of the Muon Stopping Power in LeadTungstate

The CMS Collaboration∗

Abstract

A large sample of cosmic ray events collected by the CMS detector is exploited tomeasure the specific energy loss of muons in the lead tungstate (PbWO4) of the elec-tromagnetic calorimeter. The measurement spans a momentum range from 5 GeV/cto 1 TeV/c. The results are consistent with the expectations over the entire range. Thecalorimeter energy scale, set with 120 GeV/c electrons, is validated down to the sub-GeV region using energy deposits, of order 100 MeV, associated with low-momentummuons. The muon critical energy in PbWO4 is measured to be 160+5

−6± 8 GeV, in agree-ment with expectations. This is the first experimental determination of muon criticalenergy.

∗See Appendix A for the list of collaboration members

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1 IntroductionThe electromagnetic calorimeter (ECAL) of the Compact Muon Solenoid (CMS) experiment [1]has been designed with a stringent performance goal on energy resolution, driven by the capa-bility to detect a Higgs boson decaying into two photons. While waiting to record events frombeam collisions at the LHC, its outstanding characteristics have been exploited to measure themuon stopping power in lead tungstate (PbWO4) for cosmic ray muon momenta between 5and 1000 GeV/c.

The stopping power for muons in the energy range considered can be conveniently written as

f (E) =⟨−dE

dx

⟩= a(E) + b(E)E , (1)

where E is the total muon energy, x is the thickness of the traversed material, commonly mea-sured in mass per unit surface, a(E) is the stopping power due to collisions with atomic elec-trons, and b(E) is due to radiative processes: bremsstrahlung, direct pair production, and pho-tonuclear interactions; a(E) and b(E) are slowly varying functions of E at energies where ra-diative contributions are important [2, 3].

Numerical values of stopping power and related quantities quoted throughout this paper aretaken from tables in [4]. The tables [see 2] are obtained from calculations following [3] includ-ing post-Born corrections from [5], which result in an increase of the critical energy by 6 GeV.The theoretical uncertainties are everywhere smaller than the statistical precision of the resultsreported in this paper. The definition of critical energy as the energy at which the average ratesof energy loss through collision and radiation are equal [2, 3] is adopted in this paper.

The lowest and highest momenta considered in the analysis reported here correspond to re-gions dominated by collision and radiative processes, respectively. Comparison of the experi-mental values of the stopping power with predictions, extends the validity of the ECAL energyscale, set with 120 GeV/c electron beams, down to energy deposits below 1 GeV. Analysis ofdata in the full momentum range permits a comparison of collision losses with radiative losses,thus leading to the first experimental determination of muon critical energy.

The experimental setup and the characteristics of the data sample are described in Section 2.Event selection and measurement of relevant physical quantities are discussed in Section 3.Possible limitations in the measurement of the muon stopping power are addressed in Sec-tion 4. In Section 5, corrections for systematic effects and statistical issues are addressed, andresults are reported.

2 Experimental setup and data sampleThe data set consists of cosmic ray muons traversing the CMS detector located 100 m under-ground, collected during the detector commissioning phase.

The central feature of the CMS apparatus is a superconducting solenoid of 6 m internal diam-eter. Within the field volume are the silicon pixel and strip tracker, the crystal electromagneticcalorimeter and the brass-scintillator hadron calorimeter (HCAL). Muons are measured in gas-ionization chambers embedded in the steel return yoke. In addition to the barrel and endcapdetectors, CMS has an extensive forward calorimetry. The silicon pixel and strip detectors pro-vide excellent momentum reconstruction, with a 10 % resolution for 1 TeV/c muons passingclose to the nominal interaction vertex.

2 3 Event measurement and selection

The electromagnetic calorimeter is a hermetic homogeneous scintillator detector made ofPbWO4 crystals. Lead tungstate has a high density (8.3 g cm−3), a short radiation length,(X0 = 0.89 cm) and a small Moliere radius (RM = 2.0 cm). Crystals are organized in a centralbarrel of 61 200 crystals closed by two end-caps of 7324 crystals each. The light is read out byavalanche photodiodes (APD) in the barrel and by vacuum phototriodes (VPT) in theend-caps. In the barrel, relevant to the analysis presented in this paper, the individual crystalshave a truncated-pyramid shape with a mean lateral size in the front section of 2.2 cm and alength of 23 cm, which corresponds to 25.8 radiation lengths. The barrel crystals are organizedin a quasi-projective geometry, where their principal axis is tilted by 3◦ with respect to thenominal interaction vertex, in both the azimuthal and polar angle projections.

The CMS collaboration conducted a month-long data-taking exercise, known as the CosmicRun At Four Tesla (CRAFT), during October-November 2008 with the goal of commissioningthe experiment for extended operation [6]. With all installed detector systems participating,CMS recorded 270 million cosmic ray triggered events with the solenoid at its nominal axialfield strength of 3.8 T. An event display of a cosmic ray muon crossing CMS is shown in Fig. 1.

During data taking at the LHC, the APDs will be operated at a gain of 50. In order to increasethe sensitivity to low-energy deposits and to reduce the impact of the electronic noise, the APDgain was raised to 200 for several of the commissioning runs. In this condition the noise perreadout channel amounts to about 1 ADC count, which corresponds on average to 9.3 MeV [7].

The signal from the APDs, after being amplified and shaped, is digitized at 40 MHz and tenpulse samples are recorded for each calorimeter channel. In order to reduce the bandwidthrequired for data acquisition, a reduction procedure is applied. A summary of data reductionalgorithms is reported in Section 3; for more details the reader is referred to [8].

Because of the angular distribution of the cosmic ray muon flux and the lower sensitivity of theECAL end-caps to the energy released by a minimum ionizing particle, only the barrel part ofECAL is used in the present analysis.

3 Event measurement and selectionThe physical variables to be measured for each muon are the momentum, the path length inECAL, and the energy lost in ECAL.

The muon momentum is measured from the track fit performed in the inner tracking system [9].

The path length in ECAL is estimated by propagating the measured muon track inside thecalorimeter taking into account bending due to the magnetic field and expected energy loss.The average path length in ECAL for the selected muon sample is 22.0 cm, with an rms spreadof 2.6 cm.

A dedicated algorithm has been developed to reconstruct the energy deposited by cosmic raymuons in ECAL. The main differences with respect to the standard reconstruction algorithm forevents collected during LHC operation are driven by the requirement of good reconstructionand association efficiency down to low energy and for energy deposits associated with muonsnot pointing to the nominal interaction vertex. Online data reduction is based on zero suppres-sion (ZS), that is, a readout of channels above the ZS threshold, and on a full readout of selectedregions (SR) of high interest, as identified by a Selective Readout Processor (SRP), based on theinformation of the Level-1 trigger system of ECAL [8]. For CRAFT runs with APD gain set to200, the ZS threshold corresponds to about 20 MeV and the SR threshold to about 170 MeV.

3

Run 66748, Event 8894786, LS 160, Orbit 167263116, BX 19

x

y

(a)

(b)

Figure 1: An event display of a cosmic ray muon crossing CMS: (a) the full detector and (b) adetail of the central region. ECAL hits are in magenta, HCAL hits in blue, tracker and muon hitsin green. The views represent a section of CMS in a plane perpendicular to the beam direction,the x axis pointing to the centre of the LHC ring and the y axis pointing vertically upwards.

4 3 Event measurement and selection

When the condition for SR is met, a matrix of 3×3 trigger towers is read out. Each tower iscomprised of 5×5 crystals, the matrix is centered around the tower with energy deposit abovethe SR threshold. The energy reconstruction algorithm identifies clusters starting from a centralcrystal (seed) with an energy deposit of at least 15 ADC counts (139.5 MeV), or from the mostenergetic of a pair of adjacent crystals with at least 5 ADC counts (46.5 MeV) each, the clusterenergy is determined as the sum of all channels above 2 ADC counts (18.5 MeV) belonging toa 5×5 matrix of crystals.

Contiguous clusters are merged and the size of the resulting cluster depends on the impactangle of the muon at the calorimeter surface. Clusters in ECAL are then associated with muontracks according to a geometrical match between the track extrapolation to the calorimeter sur-face and the centre of gravity of the energy deposit. The energy in the cluster is obtained afterapplication of relative calibration constants to individual channels and of an absolute energyscale factor. The intercalibration constants are defined to equalize the response of the individ-ual channels to the same energy deposits in the corresponding crystals. The absolute energyscale was determined from data taken with a 120 GeV/c electron beam [10]. It is defined as theresponse to 120 GeV/c electrons striking the centre of a 5× 5 matrix of crystals in a referenceregion of ECAL. With these definitions, the same energy scale is obtained over the entire ECALup to local containment effects. According to Monte Carlo simulation, this containment factorcorresponds to 97 % of the electron energy for an impact at the point of maximum response ofthe reference crystal matrix. Energy deposits due to non-radiating relativistic particles are fullycontained in a 5× 5 crystal matrix, thus the energy scale defined at the test beam is scaled by0.97 to measure the ECAL response to muons. Additional corrections, related to containmenteffects due to leakage from the crystals of muon induced secondary particles, are addressed inSection 5.

Only runs in which the APD gain was set to 200 are considered in the present analysis. Theuseful sample of CMS triggers is thus reduced to 8.8× 107. Furthermore, muons are requiredto cross both the upper and the lower half of ECAL barrel (see Section 5). The initial sampleof events considered in the present analysis was thus defined by the combined requirementsof a muon at the trigger level [11], of a single muon track reconstructed by the tracker [9], andof an energy deposit associated with the track in both the upper and the lower half of ECALbarrel. Moreover, analysis is limited to muons with momentum ranging from 5 to 1000 GeV/c.This interval, which is mainly determined by the size of the event sample, is further dividedfor analysis purposes into 20 equal bins in log(p). For the present analysis, the muon momen-tum has to be measured upstream of the energy release in the calorimeter. Thus only energydeposits in the bottom half of ECAL are used. The following selections are then applied to theinitial sample: the uncertainty on muon momentum must be smaller than the bin width; theratio of the energy deposit in the calorimeter to muon momentum must be less than 1 withinthe experimental accuracy; the angle between the muon track at the ECAL surface and the cor-responding crystal axis must be smaller than 0.5 radians. These criteria reduce the sample by afactor 1.7, the largest reduction coming from the angle selection. Moreover, as will be clarifiedin Section 5, events with energy deposits above 500 MeV in the upper part of the ECAL barrelare vetoed. This last selection further reduces the sample by a factor 1.15. The final sampleconsists of 2.5× 105 muons.

The measured muon spectrum, after the selections, is shown in Fig. 2(a). The spectrum ofenergy deposited in crystals is shown in Fig. 2(b).

Figure 3 displays the distributions of ∆E/∆x, the measured cluster energy divided by the pathlength in ECAL, for muons with momentum below 10 GeV/c, where collision losses domi-

5

(GeV/c)muon

p1 10 210 310

even

ts

10

210

310

CMS 2008

(a)

(GeV)clusterE-210 -110 1 10 210 310

even

ts1

10

210

310

410 CMS 2008

(b)

Figure 2: (a) Momentum spectrum of the muons passing the selections; (b) spectrum of thereconstructed energy in the lower ECAL hemisphere. A logarithmic binning is used.

nate (a), and for muons with momentum above 300 GeV/c, where sizable radiation losses areexpected (b).

4 Measurement of the stopping powerIn making a calorimetric measurement of stopping power, the choice of optimal thickness of thesampling material must be the result of a compromise. On the one hand, the thickness shouldbe small enough for the variation of primary particle energy to be negligible; on the other,the thickness should be large enough to allow a precise measurement of the energy released.Furthermore, the correction arising from energy leaking from the measurement volume shouldbe kept small. The extent to which the CMS ECAL crystals meet these requirements is discussedin 4.1 and 4.2.

4.1 dE/dx approximation

The stopping power is experimentally determined by the measurement of the energy ∆E lostby a muon when traversing a known thickness ∆x, which must be small in order that theapproximation f (E) = −dE/dx = ∆E/∆x holds. Quantitatively ∆ f / f , where ∆ f = f (E)−f (E−∆E), has to be smaller than the desired relative precision on the measurement of f . Since

∆ f ∼ d fdE

dEdx

∆x (2)

then

∆ ff∼ d f

dE∆x . (3)

6 4 Measurement of the stopping power

)2 cm-1x (MeV g∆E/∆0 2 4 6 8 10

even

ts

0

200

400

600

800

1000

1200

1400

1600

1800

2000

2200CMS 2008

(a)

)2 cm-1x (MeV g∆E/∆0 2 4 6 8 10

even

ts0

10

20

30

40

50

60

70

80

CMS 2008

(b)

Figure 3: Measured distributions of ∆E/∆x in ECAL; (a) for muon momenta below 10 GeV/c;(b) for muon momenta above 300 GeV/c; the fraction of events with ∆E/∆x > 10 MeV g−1 cm2

is 1.3× 10−3 and 8× 10−2 in (a) and (b) respectively.

In the present case, ∆x is typically 180 g/cm2 (about 25 X0 in PbWO4). The derivative of thestopping power with respect to E can be written as a sum of the contributions of collision andradiation processes, namely

∆ ff

=

[(d fdE

)coll

+

(d fdE

)rad

]∆x . (4)

For the scope of this analysis, b(E) in Eq. 1 can be assumed to be constant, with a value equalto that at 1 TeV. Then (d f /dE)rad = b = 1.4× 10−5 cm2/g [4].

This corresponds to a muon radiating 1/400 of the energy when traversing ∆x = 180 g/cm2. Itsaverage contribution to ∆ f / f is then 1/400, which is negligible when compared to the precisionof the measurement.

The component of the derivative due to collisions is a monotonically decreasing function of Ein the energy range of the present measurement; its expected value at the lowest momentum(5 GeV/c) is 2.6× 10−5 cm2/g [4]. Thus ∆ f / f is everywhere small when compared with othersources of uncertainty.

The above arguments apply not only to muons losing an energy equal to the expectation value,but also to the case of large fluctuations occurring in radiative processes. In fact f (E) is essen-tially a linear function of E in this energy range.

4.2 Containment effects

Energy lost by a muon is transferred to energy of secondaries. Since secondaries and theirdaughters may travel a significant distance, the energy lost by a muon traversing a given vol-ume is in general different from the energy deposited in that same volume. The energy ∆Econsidered in the previous section is the energy lost by a muon along a given path, while the

7

first output of the measurement procedure is the energy deposited in a given volume of thecalorimeter. Taking as a reference volume a cylinder with its axis along the muon direction,energy flow across the lateral surface can be made negligible by choosing a sufficiently largeradius. On the other hand there is always a non-negligible flow of energy carried by secon-daries entering and leaving the two ends of the cylinder, since secondaries are produced alongthe entire muon path. In a homogeneous material an equilibrium between the energy flowingin through the front surface and the energy flowing out of the rear surface is approximatelyreached when the front surface is preceded by at least an amount of material correspondingto the energy-weighted average range of secondaries. In fact, considering a muon entering adense homogeneous material from vacuum, the average energy deposition per unit thickness isgiven by the convolution product of a step function equal to the muon stopping power (muonpassing from vacuum to homogeneous material) with the function S(t) describing the averagefractional energy deposition density as a function of depth t for secondaries (i.e. the showerdepth-profile for high-energy electrons and photons). This convolution product at depth x inthe material is equal to the muon stopping power times the definite integral from 0 to x of S(t).Considering, as an illustration, the non-physical case of a muon whose only interaction withmatter is photon radiation, at a depth in the dense material at which an electromagnetic showerwould have deposited 90 % of its energy, the ratio between the average energy deposition den-sity and the stopping power would be 0.9. Therefore, considering the spectra of secondariesproduced by muons, it is found that the equilibrium condition is approached for δ-electronsafter the muon has traversed a thickness of about 10 g/cm2, while for radiated photons it isapproached after about 20 radiation lengths.

In the present case, the situation is well described as a homogeneous region of PbWO4 precededby order of 10 g/cm2 of nearby material. Because of the presence of a strong magnetic field,material separated by more than a few tens of centimeters from the crystals is less effective inproducing secondaries flowing into the measurement volume. Thus the crystals diametricallyopposite to those under study (corresponding to a separation of approximately 2.6 m) havelittle effect on the measured energy loss. Therefore, net containment corrections are expectedto be small or negligible for collision losses, but sizable for radiative losses. A quantitativeestimate of these corrections has been obtained by means of a dedicated simulation based onthe Geant4 package [12], as detailed in Section 5.

5 Data analysis and experimental resultsThis section first addresses corrections to systematic effects; instrumental effects are consideredin 5.1; the physics effects identified in Section 4 are considered in 5.2. Statistical analysis of dataand experimental results are then discussed in 5.3.

5.1 Instrumental effects

The relevant instrumental effects are related to the online data reduction and to the energyreconstruction procedure described in Section 3.

The presence of thresholds introduces a bias in energy reconstruction: noise fluctuations abovethreshold contribute a positive bias, while energy deposits below threshold contribute a nega-tive bias.

When the muon direction is close to the crystal axis, the energy deposited in ECAL is in mostcases above the SR threshold (90 % of events with the angle between muon and crystal axissmaller than 0.1 radians). When this condition is met, the bias arises mainly from effects asso-

8 5 Data analysis and experimental results

ciated with the clustering threshold and the noise spectrum, signals below threshold makinga negligible contribution. The probability of noise fluctuation above threshold is measured ina dedicated analysis of the noise spectrum. A 14.7 MeV bias is estimated for muons at anglessmaller than 0.1 radians. At larger muon angles to the crystal axis, the average energy de-posit per crystal decreases. Therefore conditions for ZS read-out occur more frequently, withthe higher ZS threshold reducing the noise bias. Moreover, the probability that the energy de-posited in a single crystal is below clustering threshold increases, thus contributing a negativebias. Bias is then expected to decrease with increasing angles, but its estimate depends on sev-eral contributions, and is less reliable than the estimate at small angles. Both a Monte Carlosimulation and the analysis of crystal multiplicity versus angle in experimental data indicatea constant positive bias (plateau) at small angles, followed by a monotonic decrease at largerangles.

(radians)α0 0.1 0.2 0.3 0.4 0.5

)2 c

m-1

<dE

/dx>

(M

eV g

1.65

1.7

1.75

1.8

1.85 CMS 2008

Figure 4: Dependence of the raw 〈dE/dx〉 on the angle α between the muon direction and thecrystal axis, for muon momentum between 5 and 10 GeV/c. Vertical bars represent statisticalerrors.

Bias dependence on angle for non-radiating muons has been further studied by analyzing thedependence of the raw dE/dx on angle for muons below 10 GeV/c in experimental data. Theresult, shown in Fig. 4, is consistent with expectations, although it is not inconsistent with awider plateau, extending up to 0.2 radians, or with a linear dependence of bias on angle withno plateau. A bias correction, dependent on angle, is thus applied to the estimated collisioncomponent of the stopping power, by applying the following procedure. At small angles, thebias to be subtracted is 14.7 MeV. At larger angles, the bias to be subtracted is estimated froma fit to the data shown in Fig. 4, assuming a plateau followed by a linear decrease with angle.The central value of the bias estimate is obtained assuming that the plateau extends up to0.1 radians, the hypotheses of no plateau and of a plateau up to 0.2 radians are taken as extremecases in the evaluation of the systematic uncertainty of bias subtraction. The uncertainty in theevaluation of the 14.7 MeV bias and the statistical uncertainty of the fit also contribute to thesystematic uncertainty of the bias correction. The overall systematic uncertainty is estimatedto be 3.5 MeV, which corresponds to about 1.2 % of the average energy deposited by a low-momentum muon.

The bias is estimated to be negligible in the presence of the larger energy deposits associated

5.2 Containment corrections 9

with radiative processes; it is in any case negligibly small compared to the systematic effectsdiscussed in Section 5.2. Therefore, no bias correction is applied to the expected contributionto dE/dx from radiative processes over the entire muon momentum spectrum.

5.2 Containment corrections

Energy leakage and the effects of upstream and downstream materials are quantitatively dif-ferent for collisions and radiative processes. Therefore, in order to make an experimental de-termination of the muon critical energy, losses and compensation for radiative and collisionprocesses are treated separately.

To estimate the difference between energy lost and energy deposited in ECAL, a model basedon the Geant4 simulation toolkit, with a simplified description of the detector and materialssurrounding it, was developed. The use of a simplified simulation instead of the full simula-tion available in CMS was driven by the high statistics needed for these studies and for thosereported in Section 5.3. The results of the simulations were also compared with dedicated ana-lytical calculations.

Because of the effect of the intense magnetic field on the trajectories of charged particles, ma-terial lying more than a few tens of centimeters away from the crystals under study may beneglected. In particular, the upper half of the ECAL has been ignored in the simulation. Thevalidity of this approximation has been reinforced by selecting muons that produce a signalof less than 500 MeV in the upper part of the ECAL, thus removing most of those emitting ahard photon. As a further check, the energy deposited in the lower half of ECAL by muonsreleasing less than 500 MeV in the upper ECAL hemisphere (the selected sample) has beencompared with the complementary sample and agreement was found within the precision ofthe comparison. In fact, in the muon momentum region between 145 and 1000 GeV/c, whereradiative losses are relevant, the weighted average of the ratio of the dE/dx measured in thetwo samples in seven momentum bins is 0.95± 0.09. This result gives no indication of an ef-fect of the upper part of ECAL on the energy deposited in the lower part, thus supporting thehypothesis that far material can be neglected. However, due to the modest statistical precisionof this test, it was conservatively decided to activate the veto in the event selection.

The low-momentum region is of major interest for the present analysis, since the large sam-ple size and the small energy loss fluctuations allow precise results to be obtained. Accordingto the simulation, the energy carried by secondaries flowing out of the rear detector surfaceis, on average, 3 % of the energy lost in the crystals for a muon with momentum 15 GeV/c.This represents an upper limit to containment corrections in the low-momentum region, wherecollision losses dominate. In fact, as already discussed in Sect. 4.2, the rear leakage can be com-pensated by secondaries produced in upstream material entering the front detector surface. Acomparison of the deposits in the upper and lower hemispheres of the ECAL barrel, for muonswith momentum between 5 and 10 GeV/c, shows no difference in dE/dx, with a sensitivitybetter than 1 % [7]. Given the similarity of the results, in spite of the asymmetric distributionof the outer and inner material around ECAL, the net correction has been neglected, and 1 %systematic uncertainty on the null correction for collision losses has been assumed.

Estimated corrections for energy containment in radiative processes have been derived fromdedicated simulations of two extreme cases: with no material in front of ECAL and with thewhole material budget of the tracker concentrated just in front of ECAL. The former case rep-resents the upper limit to the containment correction, where only rear losses are considered;the latter case gives a lower limit to the correction, as it maximally overestimates the energyflow through the front face due to upstream material. In both cases the effects of the upper

10 5 Data analysis and experimental results

ECAL hemisphere, used as a veto in the analysis, were ignored. The mean value and half ofthe difference between the results of the two simulations are the estimate of the correctionsfor the energy containment in radiative processes and of the associated systematic error. Thecorrection for energy leakage in radiative processes is maximal at 1 TeV/c: at this muon mo-mentum it corresponds to (28± 5)% of the average energy lost, while at 170 GeV/c it reducesto (14.5± 2.5)%, where the error arises from the systematic uncertainty mentioned above. Theuncertainty is small compared to the statistical uncertainty in the measurement of the stoppingpower in the corresponding region. Given the size of statistical uncertainty and the contribu-tion from other sources of systematic errors, the precision of the correction obtained with thesimplified simulation is sufficient over the entire momentum range. The correction for non-containment of radiated secondaries is applied over the whole momentum spectrum to theexpected contribution of radiative processes to stopping power.

5.3 Critical energy, energy scale, Cherenkov contribution

Several possible sources of systematic error have been taken into account in making a compar-ison between the energy scale of the ECAL set with a 120 GeV/c electron beam and the scaleresulting from the measurement of muon stopping power.

Four out of 36 supermodules were calibrated with 120 GeV/c electrons. The energy scale wastransferred to all supermodules by means of the cosmic ray intercalibration discussed in [10].This procedure resulted in a typical single-channel uncertainty of 1.5%, which is dominatedby statistics, and an overall scale uncertainty whose contribution to the final precision of thepresent measurement is negligible.

The precise variation in the gain of each APD, when going from a nominal gain of 50 to anominal gain of 200, has been measured by means of the laser monitoring system describedin [1]. The resulting uncertainty on the average energy scale is negligible.

The overall variation of the response to incident electrons with temperature has been measuredin test beam to be −(3.8± 0.4)%◦C−1. In CMS, the temperature is monitored with a 0.01◦Cprecision, and the cooling system has been demonstrated to maintain the temperature stable to18± 0.1◦C [1, 7], thus uncertainties on temperature corrections are negligible.

A test of reproducibility of calibration constants was performed by exposing the same moduleto test-beam electrons on two occasions, separated by 30 days. This resulted in no measurableoffset on the energy scale [10].

A different pulse height reconstruction procedure is required for cosmic-ray data, which areasynchronous with respect to detector clock, compared to collision data, which aresynchronous, or to test-beam data, which are also asynchronous but were recorded togetherwith accurate timing information from trigger. This has been estimated to introduce asystematic uncertainty of 1% in the energy scale of cosmic ray data with respect to test beam.

In Fig. 5(a), the specific muon energy loss resulting after corrections is compared to expectationsas a function of the muon momentum [4]. Fig. 5(b) shows the ratio of experimental measure-ments to expected values. Two regions are indicated in Fig. 5: the expected 68 % probabilitycentral interval (grey shaded area), and the minimum interval corresponding to 68 % probabil-ity (region delimited by continuous curves). The reasons for considering both intervals and theprocedure adopted for their estimate are summarized below.

The characteristics of radiative losses, which correspond to rare processes with high energyreleases, generate probability distribution functions (pdf) of energy loss for single events with

5.3 Critical energy, energy scale, Cherenkov contribution 11

p (GeV/c)1 10 210

)2 c

m-1

<dE

/dx>

(M

eV g

1

10

CMS 2008

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p (GeV/c)1 10 210

expe

ct.

/ <

dE/d

x>m

eas.

<dE

/dx>

0.5

0.6

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0.8

0.9

1

1.1

1.2

1.3

1.4

CMS 2008

(b)

Figure 5: (a) Muon stopping power measured in PbWO4 (dots) as a function of muon momen-tum compared to expectations [4] (continuous black line). The expected contributions fromcollision and radiative processes are plotted as well (red dotted line and blue dashed line re-spectively). (b) Ratio of the measured and the expected values of the muon stopping power,as a function of muon momentum. As discussed in the text, in both figures, the shaded greyarea indicates the expected 68 % probability central interval, while the continuous cyan curvesdelimit the minimum interval containing 68 % of the expected results. “Experimental errors”are not shown for reasons discussed in the text.

12 5 Data analysis and experimental results

long tails at high energy, that is: highly positively skewed distributions. In this condition, con-vergence to a normal distribution for the average dE/dx of a sample of N events is slow. Theskewness of the single event distribution increases with increasing muon momentum, owingto the increasing contribution of radiative losses with momentum. The number of events perbin in the selected data sample rapidly decreases with momentum for p > 50 GeV/c (Fig. 2(a)).It is thus expected that, due to the combined effect of increasing skewness of single event dis-tribution and decreasing event statistics with increasing momentum, in the higher momentumbins the pdf of the sample mean of dE/dx cannot be approximated by a Gaussian. Moreover,when this condition occurs, sample mean and sample variance are highly correlated. It fol-lows that the widely used “experimental error”, namely the sample rms divided by the squareroot of the sample population, is not a good measure for the consistency of the sample meanwith the expected value. Therefore the uncertainty of the result has been estimated, consis-tently over the entire momentum range covered by the measurement, by means of a numericaltechnique based on the simulation of the expected results with Geant4. Ten thousand identi-cal experiments, each with the same statistics per momentum bin as the actual data sample,were simulated. The expected pdf of the mean is then obtained for each bin as the distributionof the mean values of the stopping power from the different experiments. For each pdf two68 % probability intervals for the expected result were derived: the central interval, obtainedby discarding 16 % of the results on each tail of the pdf, and the interval of minimum widthcontaining 68 % of the results; this last interval always contains the most probable value. ForGaussian distributions these intervals coincide. In Fig. 5, for the event samples correspondingto the bins above 100 GeV/c, the differences between the two intervals become increasinglysignificant. At lower momenta, where the two intervals tend to coincide, they also correspondto the conventional estimate of the experimental error.

For the high momentum bins, the increasing probability of large fluctuations in radiative en-ergy losses, combined with the decreasing size of the event samples, cause the most probablevalues to be systematically lower than the expectation values. This trend is particularly markedin the highest momentum bin of Fig. 5, where the expectation value lies outside the 68% prob-ability interval.

The curve

(dE/dx)meas = α

[(dEdx

)coll

+ β×(

dEdx

)rad

],

where coll and rad label the predicted energy losses in PbWO4 due to collisions with atomicelectrons and radiative processes respectively [4], is fitted to experimental stopping power datausing a binned maximum likelihood and the pdf described above. The parameters α and βaccount for the overall normalization of the energy scale and for the relative normalization ofradiation and collision losses. With the adopted parameterization the β parameter, from whichthe critical energy is measured, is independent of the overall energy scale. The fit results in:

α = 1.004+0.002−0.003 (stat.)± 0.019 (syst.)

β = 1.07+0.05−0.04 (stat.)± 0.6 (syst.).

Adding statistical and systematic contributions in quadrature, it may be concluded from theabove results that the energy scale is consistent with expectations within a systematic uncer-tainty of 1.6 %, with a 1.2 % contribution from the uncertainty on the energy scale dependence

13

on the angle and on the clustering, and a 1.0 % contribution from uncertainty in containmentcorrections. This result is mainly determined by the precision of the measurements in the mo-mentum region below 20 GeV/c, where radiation losses are marginal. The typical energy re-leased in this region is about 300 MeV. Thus the energy scale set with 120 GeV/c electrons stillholds in the sub-GeV region. This, assuming a linear response of the detector to the collectedlight, implies that the relative contribution to collected photons of Cherenkov light and scintil-lation are the same for 120 GeV/c electrons and for muons in the 5-20 GeV/c region, within the1.6 % precision of this measurement (this last statement strictly holds only for muons at smallangle with respect to the crystal axis).

From the fit results, a muon critical energy of 160+5−6 (stat.)± 8 (syst.) GeV is obtained, in agree-

ment with the computed value of 169.5 GeV for PbWO4 [4]. The systematic uncertainty in-cludes a contribution of 4.5 GeV from the uncertainty of the containment corrections, domi-nated by the limited knowledge of the correction for radiation losses, and a contribution of6 GeV due to the stability of the result against bias subtraction and event selection. For thelatter, sizable contributions come from the variation of the acceptance of the muon angle withrespect to the crystal axis, and, to a lesser extent, from the requirement that E/p be lower than1. The contributions from these sources were estimated by varying the muon acceptance anglebetween 0.3 and 0.7 radians, and by removing the requirement that E/p be lower than 1.

It might be argued that the use of pdf, calculated a priori in anticipation of a particular outcome,would be inappropriate when the fitted parameters differ from the expected values. In orderto investigate the possible importance of this, fits were performed with alternative pdf sets,parametrized as functions of α and β, with α controlling the pdf energy scale, and β controllingthe relative contributions of radiation and collisions. The changes in the results were found tobe negligible compared to the quoted error.

6 ConclusionsThe muon stopping power in PbWO4 has been measured over the momentum range from5 GeV/c to 1000 GeV/c, yielding the first experimental determination of the muon criticalenergy. The value obtained: 160+5

−6 (stat.)± 8.0 (syst.) GeV, agrees with the value calculated forthis material.

In the region corresponding to muon momenta less than 20 GeV/c, where collision losses dom-inate, the average energy deposited in the crystals is of order 300 MeV. Thus the agreement(to within 1-2 %) between the measured stopping power and the calculated values confirmsthat the energy calibration of the detector, previously determined with 120 GeV/c electrons,remains valid down to the sub-GeV scale. Alternatively, the observed linearity in energy re-sponse may be interpreted as demonstrating that the relative contributions of Cherenkov andscintillation light to the measured signal are the same for muons of ∼10 GeV/c as for electronsof 120 GeV/c (in the specific case of muons traversing the crystals at small angles with respectto the axis, and of electrons striking the crystals at normal incidence). The confirmation ofthe detector energy calibration and linearity of response relies on the validity of the calculatedstopping power in lead tungstate, in the region dominated by collision losses. On the otherhand, the value extracted for the critical energy does not depend on the energy calibration,although it would be sensitive to a deviation from linearity of the response.

14 6 Conclusions

AcknowledgementsWe thank the technical and administrative staff at CERN and other CMS Institutes, and ac-knowledge support from: FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ,and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIEN-CIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia);Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG,and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India);IPM (Iran); SFI (Ireland); INFN (Italy); NRF (Korea); LAS (Lithuania); CINVESTAV, CONA-CYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR(Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTDS (Serbia);MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAKand TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA). Individuals have receivedsupport from the Marie-Curie IEF program (European Union); the Leventis Foundation; the A.P. Sloan Foundation; and the Alexander von Humboldt Foundation.

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15

A The CMS CollaborationYerevan Physics Institute, Yerevan, ArmeniaS. Chatrchyan, V. Khachatryan, A.M. Sirunyan

Institut fur Hochenergiephysik der OeAW, Wien, AustriaW. Adam, B. Arnold, H. Bergauer, T. Bergauer, M. Dragicevic, M. Eichberger, J. Ero, M. Friedl,R. Fruhwirth, V.M. Ghete, J. Hammer1, S. Hansel, M. Hoch, N. Hormann, J. Hrubec, M. Jeitler,G. Kasieczka, K. Kastner, M. Krammer, D. Liko, I. Magrans de Abril, I. Mikulec, F. Mittermayr,B. Neuherz, M. Oberegger, M. Padrta, M. Pernicka, H. Rohringer, S. Schmid, R. Schofbeck,T. Schreiner, R. Stark, H. Steininger, J. Strauss, A. Taurok, F. Teischinger, T. Themel, D. Uhl,P. Wagner, W. Waltenberger, G. Walzel, E. Widl, C.-E. Wulz

National Centre for Particle and High Energy Physics, Minsk, BelarusV. Chekhovsky, O. Dvornikov, I. Emeliantchik, A. Litomin, V. Makarenko, I. Marfin,V. Mossolov, N. Shumeiko, A. Solin, R. Stefanovitch, J. Suarez Gonzalez, A. Tikhonov

Research Institute for Nuclear Problems, Minsk, BelarusA. Fedorov, A. Karneyeu, M. Korzhik, V. Panov, R. Zuyeuski

Research Institute of Applied Physical Problems, Minsk, BelarusP. Kuchinsky

Universiteit Antwerpen, Antwerpen, BelgiumW. Beaumont, L. Benucci, M. Cardaci, E.A. De Wolf, E. Delmeire, D. Druzhkin, M. Hashemi,X. Janssen, T. Maes, L. Mucibello, S. Ochesanu, R. Rougny, M. Selvaggi, H. Van Haevermaet,P. Van Mechelen, N. Van Remortel

Vrije Universiteit Brussel, Brussel, BelgiumV. Adler, S. Beauceron, S. Blyweert, J. D’Hondt, S. De Weirdt, O. Devroede, J. Heyninck, A. Ka-logeropoulos, J. Maes, M. Maes, M.U. Mozer, S. Tavernier, W. Van Doninck1, P. Van Mulders,I. Villella

Universite Libre de Bruxelles, Bruxelles, BelgiumO. Bouhali, E.C. Chabert, O. Charaf, B. Clerbaux, G. De Lentdecker, V. Dero, S. Elgammal,A.P.R. Gay, G.H. Hammad, P.E. Marage, S. Rugovac, C. Vander Velde, P. Vanlaer, J. Wickens

Ghent University, Ghent, BelgiumM. Grunewald, B. Klein, A. Marinov, D. Ryckbosch, F. Thyssen, M. Tytgat, L. Vanelderen,P. Verwilligen

Universite Catholique de Louvain, Louvain-la-Neuve, BelgiumS. Basegmez, G. Bruno, J. Caudron, C. Delaere, P. Demin, D. Favart, A. Giammanco,G. Gregoire, V. Lemaitre, O. Militaru, S. Ovyn, K. Piotrzkowski1, L. Quertenmont, N. Schul

Universite de Mons, Mons, BelgiumN. Beliy, E. Daubie

Centro Brasileiro de Pesquisas Fisicas, Rio de Janeiro, BrazilG.A. Alves, M.E. Pol, M.H.G. Souza

Universidade do Estado do Rio de Janeiro, Rio de Janeiro, BrazilW. Carvalho, D. De Jesus Damiao, C. De Oliveira Martins, S. Fonseca De Souza, L. Mundim,V. Oguri, A. Santoro, S.M. Silva Do Amaral, A. Sznajder

Instituto de Fisica Teorica, Universidade Estadual Paulista, Sao Paulo, Brazil

16 A The CMS Collaboration

T.R. Fernandez Perez Tomei, M.A. Ferreira Dias, E. M. Gregores2, S.F. Novaes

Institute for Nuclear Research and Nuclear Energy, Sofia, BulgariaK. Abadjiev1, T. Anguelov, J. Damgov, N. Darmenov1, L. Dimitrov, V. Genchev1, P. Iaydjiev,S. Piperov, S. Stoykova, G. Sultanov, R. Trayanov, I. Vankov

University of Sofia, Sofia, BulgariaA. Dimitrov, M. Dyulendarova, V. Kozhuharov, L. Litov, E. Marinova, M. Mateev, B. Pavlov,P. Petkov, Z. Toteva1

Institute of High Energy Physics, Beijing, ChinaG.M. Chen, H.S. Chen, W. Guan, C.H. Jiang, D. Liang, B. Liu, X. Meng, J. Tao, J. Wang, Z. Wang,Z. Xue, Z. Zhang

State Key Lab. of Nucl. Phys. and Tech., Peking University, Beijing, ChinaY. Ban, J. Cai, Y. Ge, S. Guo, Z. Hu, Y. Mao, S.J. Qian, H. Teng, B. Zhu

Universidad de Los Andes, Bogota, ColombiaC. Avila, M. Baquero Ruiz, C.A. Carrillo Montoya, A. Gomez, B. Gomez Moreno, A.A. OcampoRios, A.F. Osorio Oliveros, D. Reyes Romero, J.C. Sanabria

Technical University of Split, Split, CroatiaN. Godinovic, K. Lelas, R. Plestina, D. Polic, I. Puljak

University of Split, Split, CroatiaZ. Antunovic, M. Dzelalija

Institute Rudjer Boskovic, Zagreb, CroatiaV. Brigljevic, S. Duric, K. Kadija, S. Morovic

University of Cyprus, Nicosia, CyprusR. Fereos, M. Galanti, J. Mousa, A. Papadakis, F. Ptochos, P.A. Razis, D. Tsiakkouri, Z. Zinonos

National Institute of Chemical Physics and Biophysics, Tallinn, EstoniaA. Hektor, M. Kadastik, K. Kannike, M. Muntel, M. Raidal, L. Rebane

Helsinki Institute of Physics, Helsinki, FinlandE. Anttila, S. Czellar, J. Harkonen, A. Heikkinen, V. Karimaki, R. Kinnunen, J. Klem,M.J. Kortelainen, T. Lampen, K. Lassila-Perini, S. Lehti, T. Linden, P. Luukka, T. Maenpaa,J. Nysten, E. Tuominen, J. Tuominiemi, D. Ungaro, L. Wendland

Lappeenranta University of Technology, Lappeenranta, FinlandK. Banzuzi, A. Korpela, T. Tuuva

Laboratoire d’Annecy-le-Vieux de Physique des Particules, IN2P3-CNRS, Annecy-le-Vieux,FranceP. Nedelec, D. Sillou

DSM/IRFU, CEA/Saclay, Gif-sur-Yvette, FranceM. Besancon, R. Chipaux, M. Dejardin, D. Denegri, J. Descamps, B. Fabbro, J.L. Faure, F. Ferri,S. Ganjour, F.X. Gentit, A. Givernaud, P. Gras, G. Hamel de Monchenault, P. Jarry, M.C. Lemaire,E. Locci, J. Malcles, M. Marionneau, L. Millischer, J. Rander, A. Rosowsky, D. Rousseau,M. Titov, P. Verrecchia

Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, FranceS. Baffioni, L. Bianchini, M. Bluj3, P. Busson, C. Charlot, L. Dobrzynski, R. Granier deCassagnac, M. Haguenauer, P. Mine, P. Paganini, Y. Sirois, C. Thiebaux, A. Zabi

17

Institut Pluridisciplinaire Hubert Curien, Universite de Strasbourg, Universite de HauteAlsace Mulhouse, CNRS/IN2P3, Strasbourg, FranceJ.-L. Agram4, A. Besson, D. Bloch, D. Bodin, J.-M. Brom, E. Conte4, F. Drouhin4, J.-C. Fontaine4,D. Gele, U. Goerlach, L. Gross, P. Juillot, A.-C. Le Bihan, Y. Patois, J. Speck, P. Van Hove

Universite de Lyon, Universite Claude Bernard Lyon 1, CNRS-IN2P3, Institut de PhysiqueNucleaire de Lyon, Villeurbanne, FranceC. Baty, M. Bedjidian, J. Blaha, G. Boudoul, H. Brun, N. Chanon, R. Chierici, D. Contardo,P. Depasse, T. Dupasquier, H. El Mamouni, F. Fassi5, J. Fay, S. Gascon, B. Ille, T. Kurca, T. LeGrand, M. Lethuillier, N. Lumb, L. Mirabito, S. Perries, M. Vander Donckt, P. Verdier

E. Andronikashvili Institute of Physics, Academy of Science, Tbilisi, GeorgiaN. Djaoshvili, N. Roinishvili, V. Roinishvili

Institute of High Energy Physics and Informatization, Tbilisi State University, Tbilisi,GeorgiaN. Amaglobeli

RWTH Aachen University, I. Physikalisches Institut, Aachen, GermanyR. Adolphi, G. Anagnostou, R. Brauer, W. Braunschweig, M. Edelhoff, H. Esser, L. Feld,W. Karpinski, A. Khomich, K. Klein, N. Mohr, A. Ostaptchouk, D. Pandoulas, G. Pierschel,F. Raupach, S. Schael, A. Schultz von Dratzig, G. Schwering, D. Sprenger, M. Thomas, M. Weber,B. Wittmer, M. Wlochal

RWTH Aachen University, III. Physikalisches Institut A, Aachen, GermanyO. Actis, G. Altenhofer, W. Bender, P. Biallass, M. Erdmann, G. Fetchenhauer1, J. Frangenheim,T. Hebbeker, G. Hilgers, A. Hinzmann, K. Hoepfner, C. Hof, M. Kirsch, T. Klimkovich,P. Kreuzer1, D. Lanske†, M. Merschmeyer, A. Meyer, B. Philipps, H. Pieta, H. Reithler,S.A. Schmitz, L. Sonnenschein, M. Sowa, J. Steggemann, H. Szczesny, D. Teyssier, C. Zeidler

RWTH Aachen University, III. Physikalisches Institut B, Aachen, GermanyM. Bontenackels, M. Davids, M. Duda, G. Flugge, H. Geenen, M. Giffels, W. Haj Ahmad,T. Hermanns, D. Heydhausen, S. Kalinin, T. Kress, A. Linn, A. Nowack, L. Perchalla,M. Poettgens, O. Pooth, P. Sauerland, A. Stahl, D. Tornier, M.H. Zoeller

Deutsches Elektronen-Synchrotron, Hamburg, GermanyM. Aldaya Martin, U. Behrens, K. Borras, A. Campbell, E. Castro, D. Dammann, G. Eckerlin,A. Flossdorf, G. Flucke, A. Geiser, D. Hatton, J. Hauk, H. Jung, M. Kasemann, I. Katkov,C. Kleinwort, H. Kluge, A. Knutsson, E. Kuznetsova, W. Lange, W. Lohmann, R. Mankel1,M. Marienfeld, A.B. Meyer, S. Miglioranzi, J. Mnich, M. Ohlerich, J. Olzem, A. Parenti,C. Rosemann, R. Schmidt, T. Schoerner-Sadenius, D. Volyanskyy, C. Wissing, W.D. Zeuner1

University of Hamburg, Hamburg, GermanyC. Autermann, F. Bechtel, J. Draeger, D. Eckstein, U. Gebbert, K. Kaschube, G. Kaussen,R. Klanner, B. Mura, S. Naumann-Emme, F. Nowak, U. Pein, C. Sander, P. Schleper, T. Schum,H. Stadie, G. Steinbruck, J. Thomsen, R. Wolf

Institut fur Experimentelle Kernphysik, Karlsruhe, GermanyJ. Bauer, P. Blum, V. Buege, A. Cakir, T. Chwalek, W. De Boer, A. Dierlamm, G. Dirkes,M. Feindt, U. Felzmann, M. Frey, A. Furgeri, J. Gruschke, C. Hackstein, F. Hartmann1,S. Heier, M. Heinrich, H. Held, D. Hirschbuehl, K.H. Hoffmann, S. Honc, C. Jung, T. Kuhr,T. Liamsuwan, D. Martschei, S. Mueller, Th. Muller, M.B. Neuland, M. Niegel, O. Oberst,A. Oehler, J. Ott, T. Peiffer, D. Piparo, G. Quast, K. Rabbertz, F. Ratnikov, N. Ratnikova, M. Renz,C. Saout1, G. Sartisohn, A. Scheurer, P. Schieferdecker, F.-P. Schilling, G. Schott, H.J. Simonis,

18 A The CMS Collaboration

F.M. Stober, P. Sturm, D. Troendle, A. Trunov, W. Wagner, J. Wagner-Kuhr, M. Zeise, V. Zhukov6,E.B. Ziebarth

Institute of Nuclear Physics ”Demokritos”, Aghia Paraskevi, GreeceG. Daskalakis, T. Geralis, K. Karafasoulis, A. Kyriakis, D. Loukas, A. Markou, C. Markou,C. Mavrommatis, E. Petrakou, A. Zachariadou

University of Athens, Athens, GreeceL. Gouskos, P. Katsas, A. Panagiotou1

University of Ioannina, Ioannina, GreeceI. Evangelou, P. Kokkas, N. Manthos, I. Papadopoulos, V. Patras, F.A. Triantis

KFKI Research Institute for Particle and Nuclear Physics, Budapest, HungaryG. Bencze1, L. Boldizsar, G. Debreczeni, C. Hajdu1, S. Hernath, P. Hidas, D. Horvath7,K. Krajczar, A. Laszlo, G. Patay, F. Sikler, N. Toth, G. Vesztergombi

Institute of Nuclear Research ATOMKI, Debrecen, HungaryN. Beni, G. Christian, J. Imrek, J. Molnar, D. Novak, J. Palinkas, G. Szekely, Z. Szillasi1,K. Tokesi, V. Veszpremi

University of Debrecen, Debrecen, HungaryA. Kapusi, G. Marian, P. Raics, Z. Szabo, Z.L. Trocsanyi, B. Ujvari, G. Zilizi

Panjab University, Chandigarh, IndiaS. Bansal, H.S. Bawa, S.B. Beri, V. Bhatnagar, M. Jindal, M. Kaur, R. Kaur, J.M. Kohli,M.Z. Mehta, N. Nishu, L.K. Saini, A. Sharma, A. Singh, J.B. Singh, S.P. Singh

University of Delhi, Delhi, IndiaS. Ahuja, S. Arora, S. Bhattacharya8, S. Chauhan, B.C. Choudhary, P. Gupta, S. Jain, S. Jain,M. Jha, A. Kumar, K. Ranjan, R.K. Shivpuri, A.K. Srivastava

Bhabha Atomic Research Centre, Mumbai, IndiaR.K. Choudhury, D. Dutta, S. Kailas, S.K. Kataria, A.K. Mohanty, L.M. Pant, P. Shukla,A. Topkar

Tata Institute of Fundamental Research - EHEP, Mumbai, IndiaT. Aziz, M. Guchait9, A. Gurtu, M. Maity10, D. Majumder, G. Majumder, K. Mazumdar,A. Nayak, A. Saha, K. Sudhakar

Tata Institute of Fundamental Research - HECR, Mumbai, IndiaS. Banerjee, S. Dugad, N.K. Mondal

Institute for Studies in Theoretical Physics & Mathematics (IPM), Tehran, IranH. Arfaei, H. Bakhshiansohi, A. Fahim, A. Jafari, M. Mohammadi Najafabadi, A. Moshaii,S. Paktinat Mehdiabadi, S. Rouhani, B. Safarzadeh, M. Zeinali

University College Dublin, Dublin, IrelandM. Felcini

INFN Sezione di Bari a, Universita di Bari b, Politecnico di Bari c, Bari, ItalyM. Abbresciaa ,b, L. Barbonea, F. Chiumaruloa, A. Clementea, A. Colaleoa, D. Creanzaa,c,G. Cuscelaa, N. De Filippisa, M. De Palmaa,b, G. De Robertisa, G. Donvitoa, F. Fedelea, L. Fiorea,M. Francoa, G. Iasellia,c, N. Lacalamitaa, F. Loddoa, L. Lusitoa,b, G. Maggia,c, M. Maggia,N. Mannaa,b, B. Marangellia ,b, S. Mya ,c, S. Natalia ,b, S. Nuzzoa,b, G. Papagnia, S. Piccolomoa,G.A. Pierroa, C. Pintoa, A. Pompilia ,b, G. Pugliesea ,c, R. Rajana, A. Ranieria, F. Romanoa,c,

19

G. Rosellia,b, G. Selvaggia ,b, Y. Shindea, L. Silvestrisa, S. Tupputia ,b, G. Zitoa

INFN Sezione di Bologna a, Universita di Bologna b, Bologna, ItalyG. Abbiendia, W. Bacchia ,b, A.C. Benvenutia, M. Boldinia, D. Bonacorsia, S. Braibant-Giacomellia,b, V.D. Cafaroa, S.S. Caiazzaa, P. Capiluppia,b, A. Castroa ,b, F.R. Cavalloa,G. Codispotia,b, M. Cuffiania,b, I. D’Antonea, G.M. Dallavallea,1, F. Fabbria, A. Fanfania ,b,D. Fasanellaa, P. Giacomellia, V. Giordanoa, M. Giuntaa ,1, C. Grandia, M. Guerzonia,S. Marcellinia, G. Masettia,b, A. Montanaria, F.L. Navarriaa,b, F. Odoricia, G. Pellegrinia,A. Perrottaa, A.M. Rossia,b, T. Rovellia ,b, G. Sirolia ,b, G. Torromeoa, R. Travaglinia ,b

INFN Sezione di Catania a, Universita di Catania b, Catania, ItalyS. Albergoa,b, S. Costaa,b, R. Potenzaa,b, A. Tricomia,b, C. Tuvea

INFN Sezione di Firenze a, Universita di Firenze b, Firenze, ItalyG. Barbaglia, G. Broccoloa,b, V. Ciullia ,b, C. Civininia, R. D’Alessandroa ,b, E. Focardia ,b,S. Frosalia,b, E. Galloa, C. Gentaa,b, G. Landia ,b, P. Lenzia,b ,1, M. Meschinia, S. Paolettia,G. Sguazzonia, A. Tropianoa

INFN Laboratori Nazionali di Frascati, Frascati, ItalyL. Benussi, M. Bertani, S. Bianco, S. Colafranceschi11, D. Colonna11, F. Fabbri, M. Giardoni,L. Passamonti, D. Piccolo, D. Pierluigi, B. Ponzio, A. Russo

INFN Sezione di Genova, Genova, ItalyP. Fabbricatore, R. Musenich

INFN Sezione di Milano-Biccoca a, Universita di Milano-Bicocca b, Milano, ItalyA. Benagliaa, M. Callonia, G.B. Ceratia ,b ,1, P. D’Angeloa, F. De Guioa, F.M. Farinaa, A. Ghezzia,P. Govonia,b, M. Malbertia,b ,1, S. Malvezzia, A. Martellia, D. Menascea, V. Miccioa,b, L. Moronia,P. Negria,b, M. Paganonia ,b, D. Pedrinia, A. Pulliaa ,b, S. Ragazzia ,b, N. Redaellia, S. Salaa,R. Salernoa,b, T. Tabarelli de Fatisa ,b, V. Tancinia,b, S. Taronia ,b

INFN Sezione di Napoli a, Universita di Napoli ”Federico II” b, Napoli, ItalyS. Buontempoa, N. Cavalloa, A. Cimminoa ,b ,1, M. De Gruttolaa,b ,1, F. Fabozzia,12, A.O.M. Iorioa,L. Listaa, D. Lomidzea, P. Nolia ,b, P. Paoluccia, C. Sciaccaa,b

INFN Sezione di Padova a, Universita di Padova b, Padova, ItalyP. Azzia,1, N. Bacchettaa, L. Barcellana, P. Bellana ,b ,1, M. Bellatoa, M. Benettonia, M. Biasottoa ,13,D. Biselloa,b, E. Borsatoa ,b, A. Brancaa, R. Carlina ,b, L. Castellania, P. Checchiaa, E. Contia,F. Dal Corsoa, M. De Mattiaa,b, T. Dorigoa, U. Dossellia, F. Fanzagoa, F. Gasparinia ,b,U. Gasparinia,b, P. Giubilatoa,b, F. Gonellaa, A. Greselea,14, M. Gulminia ,13, A. Kaminskiya ,b,S. Lacapraraa ,13, I. Lazzizzeraa ,14, M. Margonia ,b, G. Marona ,13, S. Mattiazzoa,b, M. Mazzucatoa,M. Meneghellia, A.T. Meneguzzoa,b, M. Michelottoa, F. Montecassianoa, M. Nespoloa,M. Passaseoa, M. Pegoraroa, L. Perrozzia, N. Pozzobona ,b, P. Ronchesea,b, F. Simonettoa,b,N. Tonioloa, E. Torassaa, M. Tosia ,b, A. Triossia, S. Vaninia ,b, S. Venturaa, P. Zottoa,b,G. Zumerlea,b

INFN Sezione di Pavia a, Universita di Pavia b, Pavia, ItalyP. Baessoa,b, U. Berzanoa, S. Bricolaa, M.M. Necchia ,b, D. Paganoa,b, S.P. Rattia,b, C. Riccardia,b,P. Torrea ,b, A. Vicinia, P. Vituloa,b, C. Viviania,b

INFN Sezione di Perugia a, Universita di Perugia b, Perugia, ItalyD. Aisaa, S. Aisaa, E. Babuccia, M. Biasinia,b, G.M. Bileia, B. Caponeria,b, B. Checcuccia, N. Dinua,L. Fanoa, L. Farnesinia, P. Laricciaa,b, A. Lucaronia,b, G. Mantovania ,b, A. Nappia,b, A. Pilusoa,V. Postolachea, A. Santocchiaa,b, L. Servolia, D. Tonoiua, A. Vedaeea, R. Volpea ,b

20 A The CMS Collaboration

INFN Sezione di Pisa a, Universita di Pisa b, Scuola Normale Superiore di Pisa c, Pisa, ItalyP. Azzurria ,c, G. Bagliesia, J. Bernardinia,b, L. Berrettaa, T. Boccalia, A. Boccia ,c, L. Borrelloa,c,F. Bosia, F. Calzolaria, R. Castaldia, R. Dell’Orsoa, F. Fioria,b, L. Foaa ,c, S. Gennaia,c, A. Giassia,A. Kraana, F. Ligabuea ,c, T. Lomtadzea, F. Mariania, L. Martinia, M. Massaa, A. Messineoa ,b,A. Moggia, F. Pallaa, F. Palmonaria, G. Petragnania, G. Petrucciania ,c, F. Raffaellia, S. Sarkara,G. Segneria, A.T. Serbana, P. Spagnoloa ,1, R. Tenchinia ,1, S. Tolainia, G. Tonellia,b ,1, A. Venturia,P.G. Verdinia

INFN Sezione di Roma a, Universita di Roma ”La Sapienza” b, Roma, ItalyS. Baccaroa ,15, L. Baronea,b, A. Bartolonia, F. Cavallaria ,1, I. Dafineia, D. Del Rea ,b, E. DiMarcoa ,b, M. Diemoza, D. Francia,b, E. Longoa,b, G. Organtinia ,b, A. Palmaa ,b, F. Pandolfia ,b,R. Paramattia,1, F. Pellegrinoa, S. Rahatloua ,b, C. Rovellia

INFN Sezione di Torino a, Universita di Torino b, Universita del Piemonte Orientale (No-vara) c, Torino, ItalyG. Alampia, N. Amapanea ,b, R. Arcidiaconoa,b, S. Argiroa,b, M. Arneodoa ,c, C. Biinoa,M.A. Borgiaa,b, C. Bottaa,b, N. Cartigliaa, R. Castelloa ,b, G. Cerminaraa,b, M. Costaa ,b,D. Dattolaa, G. Dellacasaa, N. Demariaa, G. Dugheraa, F. Dumitrachea, A. Grazianoa ,b,C. Mariottia, M. Maronea,b, S. Masellia, E. Migliorea,b, G. Milaa ,b, V. Monacoa ,b, M. Musicha ,b,M. Nervoa ,b, M.M. Obertinoa ,c, S. Oggeroa,b, R. Paneroa, N. Pastronea, M. Pelliccionia ,b,A. Romeroa,b, M. Ruspaa,c, R. Sacchia,b, A. Solanoa,b, A. Staianoa, P.P. Trapania ,b ,1, D. Trocinoa ,b,A. Vilela Pereiraa,b, L. Viscaa,b, A. Zampieria

INFN Sezione di Trieste a, Universita di Trieste b, Trieste, ItalyF. Ambroglinia ,b, S. Belfortea, F. Cossuttia, G. Della Riccaa,b, B. Gobboa, A. Penzoa

Kyungpook National University, Daegu, KoreaS. Chang, J. Chung, D.H. Kim, G.N. Kim, D.J. Kong, H. Park, D.C. Son

Wonkwang University, Iksan, KoreaS.Y. Bahk

Chonnam National University, Kwangju, KoreaS. Song

Konkuk University, Seoul, KoreaS.Y. Jung

Korea University, Seoul, KoreaB. Hong, H. Kim, J.H. Kim, K.S. Lee, D.H. Moon, S.K. Park, H.B. Rhee, K.S. Sim

Seoul National University, Seoul, KoreaJ. Kim

University of Seoul, Seoul, KoreaM. Choi, G. Hahn, I.C. Park

Sungkyunkwan University, Suwon, KoreaS. Choi, Y. Choi, J. Goh, H. Jeong, T.J. Kim, J. Lee, S. Lee

Vilnius University, Vilnius, LithuaniaM. Janulis, D. Martisiute, P. Petrov, T. Sabonis

Centro de Investigacion y de Estudios Avanzados del IPN, Mexico City, MexicoH. Castilla Valdez1, A. Sanchez Hernandez

21

Universidad Iberoamericana, Mexico City, MexicoS. Carrillo Moreno

Universidad Autonoma de San Luis Potosı, San Luis Potosı, MexicoA. Morelos Pineda

University of Auckland, Auckland, New ZealandP. Allfrey, R.N.C. Gray, D. Krofcheck

University of Canterbury, Christchurch, New ZealandN. Bernardino Rodrigues, P.H. Butler, T. Signal, J.C. Williams

National Centre for Physics, Quaid-I-Azam University, Islamabad, PakistanM. Ahmad, I. Ahmed, W. Ahmed, M.I. Asghar, M.I.M. Awan, H.R. Hoorani, I. Hussain,W.A. Khan, T. Khurshid, S. Muhammad, S. Qazi, H. Shahzad

Institute of Experimental Physics, Warsaw, PolandM. Cwiok, R. Dabrowski, W. Dominik, K. Doroba, M. Konecki, J. Krolikowski, K. Pozniak16,R. Romaniuk, W. Zabolotny16, P. Zych

Soltan Institute for Nuclear Studies, Warsaw, PolandT. Frueboes, R. Gokieli, L. Goscilo, M. Gorski, M. Kazana, K. Nawrocki, M. Szleper, G. Wrochna,P. Zalewski

Laboratorio de Instrumentacao e Fısica Experimental de Partıculas, Lisboa, PortugalN. Almeida, L. Antunes Pedro, P. Bargassa, A. David, P. Faccioli, P.G. Ferreira Parracho,M. Freitas Ferreira, M. Gallinaro, M. Guerra Jordao, P. Martins, G. Mini, P. Musella, J. Pela,L. Raposo, P.Q. Ribeiro, S. Sampaio, J. Seixas, J. Silva, P. Silva, D. Soares, M. Sousa, J. Varela,H.K. Wohri

Joint Institute for Nuclear Research, Dubna, RussiaI. Altsybeev, I. Belotelov, P. Bunin, Y. Ershov, I. Filozova, M. Finger, M. Finger Jr.,A. Golunov, I. Golutvin, N. Gorbounov, V. Kalagin, A. Kamenev, V. Karjavin, V. Konoplyanikov,V. Korenkov, G. Kozlov, A. Kurenkov, A. Lanev, A. Makankin, V.V. Mitsyn, P. Moisenz,E. Nikonov, D. Oleynik, V. Palichik, V. Perelygin, A. Petrosyan, R. Semenov, S. Shmatov,V. Smirnov, D. Smolin, E. Tikhonenko, S. Vasil’ev, A. Vishnevskiy, A. Volodko, A. Zarubin,V. Zhiltsov

Petersburg Nuclear Physics Institute, Gatchina (St Petersburg), RussiaN. Bondar, L. Chtchipounov, A. Denisov, Y. Gavrikov, G. Gavrilov, V. Golovtsov, Y. Ivanov,V. Kim, V. Kozlov, P. Levchenko, G. Obrant, E. Orishchin, A. Petrunin, Y. Shcheglov, A. Shchet-kovskiy, V. Sknar, I. Smirnov, V. Sulimov, V. Tarakanov, L. Uvarov, S. Vavilov, G. Velichko,S. Volkov, A. Vorobyev

Institute for Nuclear Research, Moscow, RussiaYu. Andreev, A. Anisimov, P. Antipov, A. Dermenev, S. Gninenko, N. Golubev, M. Kirsanov,N. Krasnikov, V. Matveev, A. Pashenkov, V.E. Postoev, A. Solovey, A. Solovey, A. Toropin,S. Troitsky

Institute for Theoretical and Experimental Physics, Moscow, RussiaA. Baud, V. Epshteyn, V. Gavrilov, N. Ilina, V. Kaftanov†, V. Kolosov, M. Kossov1, A. Krokhotin,S. Kuleshov, A. Oulianov, G. Safronov, S. Semenov, I. Shreyber, V. Stolin, E. Vlasov, A. Zhokin

Moscow State University, Moscow, RussiaE. Boos, M. Dubinin17, L. Dudko, A. Ershov, A. Gribushin, V. Klyukhin, O. Kodolova, I. Lokhtin,

22 A The CMS Collaboration

S. Petrushanko, L. Sarycheva, V. Savrin, A. Snigirev, I. Vardanyan

P.N. Lebedev Physical Institute, Moscow, RussiaI. Dremin, M. Kirakosyan, N. Konovalova, S.V. Rusakov, A. Vinogradov

State Research Center of Russian Federation, Institute for High Energy Physics, Protvino,RussiaS. Akimenko, A. Artamonov, I. Azhgirey, S. Bitioukov, V. Burtovoy, V. Grishin1, V. Kachanov,D. Konstantinov, V. Krychkine, A. Levine, I. Lobov, V. Lukanin, Y. Mel’nik, V. Petrov, R. Ryutin,S. Slabospitsky, A. Sobol, A. Sytine, L. Tourtchanovitch, S. Troshin, N. Tyurin, A. Uzunian,A. Volkov

Vinca Institute of Nuclear Sciences, Belgrade, SerbiaP. Adzic, M. Djordjevic, D. Jovanovic18, D. Krpic18, D. Maletic, J. Puzovic18, N. Smiljkovic

Centro de Investigaciones Energeticas Medioambientales y Tecnologicas (CIEMAT),Madrid, SpainM. Aguilar-Benitez, J. Alberdi, J. Alcaraz Maestre, P. Arce, J.M. Barcala, C. Battilana, C. BurgosLazaro, J. Caballero Bejar, E. Calvo, M. Cardenas Montes, M. Cepeda, M. Cerrada, M. ChamizoLlatas, F. Clemente, N. Colino, M. Daniel, B. De La Cruz, A. Delgado Peris, C. Diez Pardos,C. Fernandez Bedoya, J.P. Fernandez Ramos, A. Ferrando, J. Flix, M.C. Fouz, P. Garcia-Abia,A.C. Garcia-Bonilla, O. Gonzalez Lopez, S. Goy Lopez, J.M. Hernandez, M.I. Josa, J. Marin,G. Merino, J. Molina, A. Molinero, J.J. Navarrete, J.C. Oller, J. Puerta Pelayo, L. Romero,J. Santaolalla, C. Villanueva Munoz, C. Willmott, C. Yuste

Universidad Autonoma de Madrid, Madrid, SpainC. Albajar, M. Blanco Otano, J.F. de Troconiz, A. Garcia Raboso, J.O. Lopez Berengueres

Universidad de Oviedo, Oviedo, SpainJ. Cuevas, J. Fernandez Menendez, I. Gonzalez Caballero, L. Lloret Iglesias, H. Naves Sordo,J.M. Vizan Garcia

Instituto de Fısica de Cantabria (IFCA), CSIC-Universidad de Cantabria, Santander, SpainI.J. Cabrillo, A. Calderon, S.H. Chuang, I. Diaz Merino, C. Diez Gonzalez, J. DuarteCampderros, M. Fernandez, G. Gomez, J. Gonzalez Sanchez, R. Gonzalez Suarez, C. Jorda,P. Lobelle Pardo, A. Lopez Virto, J. Marco, R. Marco, C. Martinez Rivero, P. Martinez Ruiz delArbol, F. Matorras, T. Rodrigo, A. Ruiz Jimeno, L. Scodellaro, M. Sobron Sanudo, I. Vila, R. VilarCortabitarte

CERN, European Organization for Nuclear Research, Geneva, SwitzerlandD. Abbaneo, E. Albert, M. Alidra, S. Ashby, E. Auffray, J. Baechler, P. Baillon, A.H. Ball,S.L. Bally, D. Barney, F. Beaudette19, R. Bellan, D. Benedetti, G. Benelli, C. Bernet, P. Bloch,S. Bolognesi, M. Bona, J. Bos, N. Bourgeois, T. Bourrel, H. Breuker, K. Bunkowski, D. Campi,T. Camporesi, E. Cano, A. Cattai, J.P. Chatelain, M. Chauvey, T. Christiansen, J.A. CoarasaPerez, A. Conde Garcia, R. Covarelli, B. Cure, A. De Roeck, V. Delachenal, D. Deyrail, S. DiVincenzo20, S. Dos Santos, T. Dupont, L.M. Edera, A. Elliott-Peisert, M. Eppard, M. Favre,N. Frank, W. Funk, A. Gaddi, M. Gastal, M. Gateau, H. Gerwig, D. Gigi, K. Gill, D. Giordano,J.P. Girod, F. Glege, R. Gomez-Reino Garrido, R. Goudard, S. Gowdy, R. Guida, L. Guiducci,J. Gutleber, M. Hansen, C. Hartl, J. Harvey, B. Hegner, H.F. Hoffmann, A. Holzner, A. Honma,M. Huhtinen, V. Innocente, P. Janot, G. Le Godec, P. Lecoq, C. Leonidopoulos, R. Loos,C. Lourenco, A. Lyonnet, A. Macpherson, N. Magini, J.D. Maillefaud, G. Maire, T. Maki,L. Malgeri, M. Mannelli, L. Masetti, F. Meijers, P. Meridiani, S. Mersi, E. Meschi, A. MeynetCordonnier, R. Moser, M. Mulders, J. Mulon, M. Noy, A. Oh, G. Olesen, A. Onnela, T. Orimoto,

23

L. Orsini, E. Perez, G. Perinic, J.F. Pernot, P. Petagna, P. Petiot, A. Petrilli, A. Pfeiffer, M. Pierini,M. Pimia, R. Pintus, B. Pirollet, H. Postema, A. Racz, S. Ravat, S.B. Rew, J. Rodrigues Antunes,G. Rolandi21, M. Rovere, V. Ryjov, H. Sakulin, D. Samyn, H. Sauce, C. Schafer, W.D. Schlatter,M. Schroder, C. Schwick, A. Sciaba, I. Segoni, A. Sharma, N. Siegrist, P. Siegrist, N. Sinanis,T. Sobrier, P. Sphicas22, D. Spiga, M. Spiropulu17, F. Stockli, P. Traczyk, P. Tropea, J. Troska,A. Tsirou, L. Veillet, G.I. Veres, M. Voutilainen, P. Wertelaers, M. Zanetti

Paul Scherrer Institut, Villigen, SwitzerlandW. Bertl, K. Deiters, W. Erdmann, K. Gabathuler, R. Horisberger, Q. Ingram, H.C. Kaestli,S. Konig, D. Kotlinski, U. Langenegger, F. Meier, D. Renker, T. Rohe, J. Sibille23,A. Starodumov24

Institute for Particle Physics, ETH Zurich, Zurich, SwitzerlandB. Betev, L. Caminada25, Z. Chen, S. Cittolin, D.R. Da Silva Di Calafiori, S. Dambach25,G. Dissertori, M. Dittmar, C. Eggel25, J. Eugster, G. Faber, K. Freudenreich, C. Grab, A. Herve,W. Hintz, P. Lecomte, P.D. Luckey, W. Lustermann, C. Marchica25, P. Milenovic26, F. Moortgat,A. Nardulli, F. Nessi-Tedaldi, L. Pape, F. Pauss, T. Punz, A. Rizzi, F.J. Ronga, L. Sala,A.K. Sanchez, M.-C. Sawley, V. Sordini, B. Stieger, L. Tauscher†, A. Thea, K. Theofilatos,D. Treille, P. Trub25, M. Weber, L. Wehrli, J. Weng, S. Zelepoukine27

Universitat Zurich, Zurich, SwitzerlandC. Amsler, V. Chiochia, S. De Visscher, C. Regenfus, P. Robmann, T. Rommerskirchen,A. Schmidt, D. Tsirigkas, L. Wilke

National Central University, Chung-Li, TaiwanY.H. Chang, E.A. Chen, W.T. Chen, A. Go, C.M. Kuo, S.W. Li, W. Lin

National Taiwan University (NTU), Taipei, TaiwanP. Bartalini, P. Chang, Y. Chao, K.F. Chen, W.-S. Hou, Y. Hsiung, Y.J. Lei, S.W. Lin, R.-S. Lu,J. Schumann, J.G. Shiu, Y.M. Tzeng, K. Ueno, Y. Velikzhanin, C.C. Wang, M. Wang

Cukurova University, Adana, TurkeyA. Adiguzel, A. Ayhan, A. Azman Gokce, M.N. Bakirci, S. Cerci, I. Dumanoglu, E. Eskut,S. Girgis, E. Gurpinar, I. Hos, T. Karaman, T. Karaman, A. Kayis Topaksu, P. Kurt, G. Onengut,G. Onengut Gokbulut, K. Ozdemir, S. Ozturk, A. Polatoz, K. Sogut28, B. Tali, H. Topakli,D. Uzun, L.N. Vergili, M. Vergili

Middle East Technical University, Physics Department, Ankara, TurkeyI.V. Akin, T. Aliev, S. Bilmis, M. Deniz, H. Gamsizkan, A.M. Guler, K. Ocalan, M. Serin, R. Sever,U.E. Surat, M. Zeyrek

Bogazici University, Department of Physics, Istanbul, TurkeyM. Deliomeroglu, D. Demir29, E. Gulmez, A. Halu, B. Isildak, M. Kaya30, O. Kaya30, S. Ozkoru-cuklu31, N. Sonmez32

National Scientific Center, Kharkov Institute of Physics and Technology, Kharkov, UkraineL. Levchuk, S. Lukyanenko, D. Soroka, S. Zub

University of Bristol, Bristol, United KingdomF. Bostock, J.J. Brooke, T.L. Cheng, D. Cussans, R. Frazier, J. Goldstein, N. Grant,M. Hansen, G.P. Heath, H.F. Heath, C. Hill, B. Huckvale, J. Jackson, C.K. Mackay, S. Metson,D.M. Newbold33, K. Nirunpong, V.J. Smith, J. Velthuis, R. Walton

Rutherford Appleton Laboratory, Didcot, United KingdomK.W. Bell, C. Brew, R.M. Brown, B. Camanzi, D.J.A. Cockerill, J.A. Coughlan, N.I. Geddes,

24 A The CMS Collaboration

K. Harder, S. Harper, B.W. Kennedy, P. Murray, C.H. Shepherd-Themistocleous, I.R. Tomalin,J.H. Williams†, W.J. Womersley, S.D. Worm

Imperial College, University of London, London, United KingdomR. Bainbridge, G. Ball, J. Ballin, R. Beuselinck, O. Buchmuller, D. Colling, N. Cripps, G. Davies,M. Della Negra, C. Foudas, J. Fulcher, D. Futyan, G. Hall, J. Hays, G. Iles, G. Karapostoli,B.C. MacEvoy, A.-M. Magnan, J. Marrouche, J. Nash, A. Nikitenko24, A. Papageorgiou,M. Pesaresi, K. Petridis, M. Pioppi34, D.M. Raymond, N. Rompotis, A. Rose, M.J. Ryan,C. Seez, P. Sharp, G. Sidiropoulos1, M. Stettler, M. Stoye, M. Takahashi, A. Tapper, C. Timlin,S. Tourneur, M. Vazquez Acosta, T. Virdee1, S. Wakefield, D. Wardrope, T. Whyntie,M. Wingham

Brunel University, Uxbridge, United KingdomJ.E. Cole, I. Goitom, P.R. Hobson, A. Khan, P. Kyberd, D. Leslie, C. Munro, I.D. Reid,C. Siamitros, R. Taylor, L. Teodorescu, I. Yaselli

Boston University, Boston, USAT. Bose, M. Carleton, E. Hazen, A.H. Heering, A. Heister, J. St. John, P. Lawson, D. Lazic,D. Osborne, J. Rohlf, L. Sulak, S. Wu

Brown University, Providence, USAJ. Andrea, A. Avetisyan, S. Bhattacharya, J.P. Chou, D. Cutts, S. Esen, G. Kukartsev,G. Landsberg, M. Narain, D. Nguyen, T. Speer, K.V. Tsang

University of California, Davis, Davis, USAR. Breedon, M. Calderon De La Barca Sanchez, M. Case, D. Cebra, M. Chertok, J. Conway,P.T. Cox, J. Dolen, R. Erbacher, E. Friis, W. Ko, A. Kopecky, R. Lander, A. Lister, H. Liu,S. Maruyama, T. Miceli, M. Nikolic, D. Pellett, J. Robles, M. Searle, J. Smith, M. Squires, J. Stilley,M. Tripathi, R. Vasquez Sierra, C. Veelken

University of California, Los Angeles, Los Angeles, USAV. Andreev, K. Arisaka, D. Cline, R. Cousins, S. Erhan1, J. Hauser, M. Ignatenko, C. Jarvis,J. Mumford, C. Plager, G. Rakness, P. Schlein†, J. Tucker, V. Valuev, R. Wallny, X. Yang

University of California, Riverside, Riverside, USAJ. Babb, M. Bose, A. Chandra, R. Clare, J.A. Ellison, J.W. Gary, G. Hanson, G.Y. Jeng, S.C. Kao,F. Liu, H. Liu, A. Luthra, H. Nguyen, G. Pasztor35, A. Satpathy, B.C. Shen†, R. Stringer, J. Sturdy,V. Sytnik, R. Wilken, S. Wimpenny

University of California, San Diego, La Jolla, USAJ.G. Branson, E. Dusinberre, D. Evans, F. Golf, R. Kelley, M. Lebourgeois, J. Letts, E. Lipeles,B. Mangano, J. Muelmenstaedt, M. Norman, S. Padhi, A. Petrucci, H. Pi, M. Pieri, R. Ranieri,M. Sani, V. Sharma, S. Simon, F. Wurthwein, A. Yagil

University of California, Santa Barbara, Santa Barbara, USAC. Campagnari, M. D’Alfonso, T. Danielson, J. Garberson, J. Incandela, C. Justus, P. Kalavase,S.A. Koay, D. Kovalskyi, V. Krutelyov, J. Lamb, S. Lowette, V. Pavlunin, F. Rebassoo, J. Ribnik,J. Richman, R. Rossin, D. Stuart, W. To, J.R. Vlimant, M. Witherell

California Institute of Technology, Pasadena, USAA. Apresyan, A. Bornheim, J. Bunn, M. Chiorboli, M. Gataullin, D. Kcira, V. Litvine, Y. Ma,H.B. Newman, C. Rogan, V. Timciuc, J. Veverka, R. Wilkinson, Y. Yang, L. Zhang, K. Zhu,R.Y. Zhu

Carnegie Mellon University, Pittsburgh, USA

25

B. Akgun, R. Carroll, T. Ferguson, D.W. Jang, S.Y. Jun, M. Paulini, J. Russ, N. Terentyev,H. Vogel, I. Vorobiev

University of Colorado at Boulder, Boulder, USAJ.P. Cumalat, M.E. Dinardo, B.R. Drell, W.T. Ford, B. Heyburn, E. Luiggi Lopez, U. Nauenberg,K. Stenson, K. Ulmer, S.R. Wagner, S.L. Zang

Cornell University, Ithaca, USAL. Agostino, J. Alexander, F. Blekman, D. Cassel, A. Chatterjee, S. Das, L.K. Gibbons, B. Heltsley,W. Hopkins, A. Khukhunaishvili, B. Kreis, V. Kuznetsov, J.R. Patterson, D. Puigh, A. Ryd, X. Shi,S. Stroiney, W. Sun, W.D. Teo, J. Thom, J. Vaughan, Y. Weng, P. Wittich

Fairfield University, Fairfield, USAC.P. Beetz, G. Cirino, C. Sanzeni, D. Winn

Fermi National Accelerator Laboratory, Batavia, USAS. Abdullin, M.A. Afaq1, M. Albrow, B. Ananthan, G. Apollinari, M. Atac, W. Badgett, L. Bagby,J.A. Bakken, B. Baldin, S. Banerjee, K. Banicz, L.A.T. Bauerdick, A. Beretvas, J. Berryhill,P.C. Bhat, K. Biery, M. Binkley, I. Bloch, F. Borcherding, A.M. Brett, K. Burkett, J.N. Butler,V. Chetluru, H.W.K. Cheung, F. Chlebana, I. Churin, S. Cihangir, M. Crawford, W. Dagenhart,M. Demarteau, G. Derylo, D. Dykstra, D.P. Eartly, J.E. Elias, V.D. Elvira, D. Evans, L. Feng,M. Fischler, I. Fisk, S. Foulkes, J. Freeman, P. Gartung, E. Gottschalk, T. Grassi, D. Green,Y. Guo, O. Gutsche, A. Hahn, J. Hanlon, R.M. Harris, B. Holzman, J. Howell, D. Hufnagel,E. James, H. Jensen, M. Johnson, C.D. Jones, U. Joshi, E. Juska, J. Kaiser, B. Klima, S. Kossiakov,K. Kousouris, S. Kwan, C.M. Lei, P. Limon, J.A. Lopez Perez, S. Los, L. Lueking, G. Lukhanin,S. Lusin1, J. Lykken, K. Maeshima, J.M. Marraffino, D. Mason, P. McBride, T. Miao, K. Mishra,S. Moccia, R. Mommsen, S. Mrenna, A.S. Muhammad, C. Newman-Holmes, C. Noeding,V. O’Dell, O. Prokofyev, R. Rivera, C.H. Rivetta, A. Ronzhin, P. Rossman, S. Ryu, V. Sekhri,E. Sexton-Kennedy, I. Sfiligoi, S. Sharma, T.M. Shaw, D. Shpakov, E. Skup, R.P. Smith†,A. Soha, W.J. Spalding, L. Spiegel, I. Suzuki, P. Tan, W. Tanenbaum, S. Tkaczyk1, R. Trentadue1,L. Uplegger, E.W. Vaandering, R. Vidal, J. Whitmore, E. Wicklund, W. Wu, J. Yarba, F. Yumiceva,J.C. Yun

University of Florida, Gainesville, USAD. Acosta, P. Avery, V. Barashko, D. Bourilkov, M. Chen, G.P. Di Giovanni, D. Dobur,A. Drozdetskiy, R.D. Field, Y. Fu, I.K. Furic, J. Gartner, D. Holmes, B. Kim, S. Klimenko,J. Konigsberg, A. Korytov, K. Kotov, A. Kropivnitskaya, T. Kypreos, A. Madorsky, K. Matchev,G. Mitselmakher, Y. Pakhotin, J. Piedra Gomez, C. Prescott, V. Rapsevicius, R. Remington,M. Schmitt, B. Scurlock, D. Wang, J. Yelton

Florida International University, Miami, USAC. Ceron, V. Gaultney, L. Kramer, L.M. Lebolo, S. Linn, P. Markowitz, G. Martinez,J.L. Rodriguez

Florida State University, Tallahassee, USAT. Adams, A. Askew, H. Baer, M. Bertoldi, J. Chen, W.G.D. Dharmaratna, S.V. Gleyzer, J. Haas,S. Hagopian, V. Hagopian, M. Jenkins, K.F. Johnson, E. Prettner, H. Prosper, S. Sekmen

Florida Institute of Technology, Melbourne, USAM.M. Baarmand, S. Guragain, M. Hohlmann, H. Kalakhety, H. Mermerkaya, R. Ralich, I. Vo-dopiyanov

University of Illinois at Chicago (UIC), Chicago, USAB. Abelev, M.R. Adams, I.M. Anghel, L. Apanasevich, V.E. Bazterra, R.R. Betts, J. Callner,

26 A The CMS Collaboration

M.A. Castro, R. Cavanaugh, C. Dragoiu, E.J. Garcia-Solis, C.E. Gerber, D.J. Hofman,S. Khalatian, C. Mironov, E. Shabalina, A. Smoron, N. Varelas

The University of Iowa, Iowa City, USAU. Akgun, E.A. Albayrak, A.S. Ayan, B. Bilki, R. Briggs, K. Cankocak36, K. Chung, W. Clarida,P. Debbins, F. Duru, F.D. Ingram, C.K. Lae, E. McCliment, J.-P. Merlo, A. Mestvirishvili,M.J. Miller, A. Moeller, J. Nachtman, C.R. Newsom, E. Norbeck, J. Olson, Y. Onel, F. Ozok,J. Parsons, I. Schmidt, S. Sen, J. Wetzel, T. Yetkin, K. Yi

Johns Hopkins University, Baltimore, USAB.A. Barnett, B. Blumenfeld, A. Bonato, C.Y. Chien, D. Fehling, G. Giurgiu, A.V. Gritsan,Z.J. Guo, P. Maksimovic, S. Rappoccio, M. Swartz, N.V. Tran, Y. Zhang

The University of Kansas, Lawrence, USAP. Baringer, A. Bean, O. Grachov, M. Murray, V. Radicci, S. Sanders, J.S. Wood, V. Zhukova

Kansas State University, Manhattan, USAD. Bandurin, T. Bolton, K. Kaadze, A. Liu, Y. Maravin, D. Onoprienko, I. Svintradze, Z. Wan

Lawrence Livermore National Laboratory, Livermore, USAJ. Gronberg, J. Hollar, D. Lange, D. Wright

University of Maryland, College Park, USAD. Baden, R. Bard, M. Boutemeur, S.C. Eno, D. Ferencek, N.J. Hadley, R.G. Kellogg, M. Kirn,S. Kunori, K. Rossato, P. Rumerio, F. Santanastasio, A. Skuja, J. Temple, M.B. Tonjes,S.C. Tonwar, T. Toole, E. Twedt

Massachusetts Institute of Technology, Cambridge, USAB. Alver, G. Bauer, J. Bendavid, W. Busza, E. Butz, I.A. Cali, M. Chan, D. D’Enterria, P. Everaerts,G. Gomez Ceballos, K.A. Hahn, P. Harris, S. Jaditz, Y. Kim, M. Klute, Y.-J. Lee, W. Li, C. Loizides,T. Ma, M. Miller, S. Nahn, C. Paus, C. Roland, G. Roland, M. Rudolph, G. Stephans, K. Sumorok,K. Sung, S. Vaurynovich, E.A. Wenger, B. Wyslouch, S. Xie, Y. Yilmaz, A.S. Yoon

University of Minnesota, Minneapolis, USAD. Bailleux, S.I. Cooper, P. Cushman, B. Dahmes, A. De Benedetti, A. Dolgopolov, P.R. Dudero,R. Egeland, G. Franzoni, J. Haupt, A. Inyakin37, K. Klapoetke, Y. Kubota, J. Mans, N. Mirman,D. Petyt, V. Rekovic, R. Rusack, M. Schroeder, A. Singovsky, J. Zhang

University of Mississippi, University, USAL.M. Cremaldi, R. Godang, R. Kroeger, L. Perera, R. Rahmat, D.A. Sanders, P. Sonnek,D. Summers

University of Nebraska-Lincoln, Lincoln, USAK. Bloom, B. Bockelman, S. Bose, J. Butt, D.R. Claes, A. Dominguez, M. Eads, J. Keller, T. Kelly,I. Kravchenko, J. Lazo-Flores, C. Lundstedt, H. Malbouisson, S. Malik, G.R. Snow

State University of New York at Buffalo, Buffalo, USAU. Baur, I. Iashvili, A. Kharchilava, A. Kumar, K. Smith, M. Strang

Northeastern University, Boston, USAG. Alverson, E. Barberis, O. Boeriu, G. Eulisse, G. Govi, T. McCauley, Y. Musienko38,S. Muzaffar, I. Osborne, T. Paul, S. Reucroft, J. Swain, L. Taylor, L. Tuura

Northwestern University, Evanston, USAA. Anastassov, B. Gobbi, A. Kubik, R.A. Ofierzynski, A. Pozdnyakov, M. Schmitt, S. Stoynev,M. Velasco, S. Won

27

University of Notre Dame, Notre Dame, USAL. Antonelli, D. Berry, M. Hildreth, C. Jessop, D.J. Karmgard, T. Kolberg, K. Lannon, S. Lynch,N. Marinelli, D.M. Morse, R. Ruchti, J. Slaunwhite, J. Warchol, M. Wayne

The Ohio State University, Columbus, USAB. Bylsma, L.S. Durkin, J. Gilmore39, J. Gu, P. Killewald, T.Y. Ling, G. Williams

Princeton University, Princeton, USAN. Adam, E. Berry, P. Elmer, A. Garmash, D. Gerbaudo, V. Halyo, A. Hunt, J. Jones, E. Laird,D. Marlow, T. Medvedeva, M. Mooney, J. Olsen, P. Piroue, D. Stickland, C. Tully, J.S. Werner,T. Wildish, Z. Xie, A. Zuranski

University of Puerto Rico, Mayaguez, USAJ.G. Acosta, M. Bonnett Del Alamo, X.T. Huang, A. Lopez, H. Mendez, S. Oliveros, J.E. RamirezVargas, N. Santacruz, A. Zatzerklyany

Purdue University, West Lafayette, USAE. Alagoz, E. Antillon, V.E. Barnes, G. Bolla, D. Bortoletto, A. Everett, A.F. Garfinkel, Z. Gecse,L. Gutay, N. Ippolito, M. Jones, O. Koybasi, A.T. Laasanen, N. Leonardo, C. Liu, V. Maroussov,P. Merkel, D.H. Miller, N. Neumeister, A. Sedov, I. Shipsey, H.D. Yoo, Y. Zheng

Purdue University Calumet, Hammond, USAP. Jindal, N. Parashar

Rice University, Houston, USAV. Cuplov, K.M. Ecklund, F.J.M. Geurts, J.H. Liu, D. Maronde, M. Matveev, B.P. Padley,R. Redjimi, J. Roberts, L. Sabbatini, A. Tumanov

University of Rochester, Rochester, USAB. Betchart, A. Bodek, H. Budd, Y.S. Chung, P. de Barbaro, R. Demina, H. Flacher, Y. Gotra,A. Harel, S. Korjenevski, D.C. Miner, D. Orbaker, G. Petrillo, D. Vishnevskiy, M. Zielinski

The Rockefeller University, New York, USAA. Bhatti, L. Demortier, K. Goulianos, K. Hatakeyama, G. Lungu, C. Mesropian, M. Yan

Rutgers, the State University of New Jersey, Piscataway, USAO. Atramentov, E. Bartz, Y. Gershtein, E. Halkiadakis, D. Hits, A. Lath, K. Rose, S. Schnetzer,S. Somalwar, R. Stone, S. Thomas, T.L. Watts

University of Tennessee, Knoxville, USAG. Cerizza, M. Hollingsworth, S. Spanier, Z.C. Yang, A. York

Texas A&M University, College Station, USAJ. Asaadi, A. Aurisano, R. Eusebi, A. Golyash, A. Gurrola, T. Kamon, C.N. Nguyen, J. Pivarski,A. Safonov, S. Sengupta, D. Toback, M. Weinberger

Texas Tech University, Lubbock, USAN. Akchurin, L. Berntzon, K. Gumus, C. Jeong, H. Kim, S.W. Lee, S. Popescu, Y. Roh, A. Sill,I. Volobouev, E. Washington, R. Wigmans, E. Yazgan

Vanderbilt University, Nashville, USAD. Engh, C. Florez, W. Johns, S. Pathak, P. Sheldon

University of Virginia, Charlottesville, USAD. Andelin, M.W. Arenton, M. Balazs, S. Boutle, M. Buehler, S. Conetti, B. Cox, R. Hirosky,A. Ledovskoy, C. Neu, D. Phillips II, M. Ronquest, R. Yohay

28 A The CMS Collaboration

Wayne State University, Detroit, USAS. Gollapinni, K. Gunthoti, R. Harr, P.E. Karchin, M. Mattson, A. Sakharov

University of Wisconsin, Madison, USAM. Anderson, M. Bachtis, J.N. Bellinger, D. Carlsmith, I. Crotty1, S. Dasu, S. Dutta, J. Efron,F. Feyzi, K. Flood, L. Gray, K.S. Grogg, M. Grothe, R. Hall-Wilton1, M. Jaworski, P. Klabbers,J. Klukas, A. Lanaro, C. Lazaridis, J. Leonard, R. Loveless, M. Magrans de Abril, A. Mohapatra,G. Ott, G. Polese, D. Reeder, A. Savin, W.H. Smith, A. Sourkov40, J. Swanson, M. Weinberg,D. Wenman, M. Wensveen, A. White

†: Deceased1: Also at CERN, European Organization for Nuclear Research, Geneva, Switzerland2: Also at Universidade Federal do ABC, Santo Andre, Brazil3: Also at Soltan Institute for Nuclear Studies, Warsaw, Poland4: Also at Universite de Haute-Alsace, Mulhouse, France5: Also at Centre de Calcul de l’Institut National de Physique Nucleaire et de Physique desParticules (IN2P3), Villeurbanne, France6: Also at Moscow State University, Moscow, Russia7: Also at Institute of Nuclear Research ATOMKI, Debrecen, Hungary8: Also at University of California, San Diego, La Jolla, USA9: Also at Tata Institute of Fundamental Research - HECR, Mumbai, India10: Also at University of Visva-Bharati, Santiniketan, India11: Also at Facolta’ Ingegneria Universita’ di Roma ”La Sapienza”, Roma, Italy12: Also at Universita della Basilicata, Potenza, Italy13: Also at Laboratori Nazionali di Legnaro dell’ INFN, Legnaro, Italy14: Also at Universita di Trento, Trento, Italy15: Also at ENEA - Casaccia Research Center, S. Maria di Galeria, Italy16: Also at Warsaw University of Technology, Institute of Electronic Systems, Warsaw, Poland17: Also at California Institute of Technology, Pasadena, USA18: Also at Faculty of Physics of University of Belgrade, Belgrade, Serbia19: Also at Laboratoire Leprince-Ringuet, Ecole Polytechnique, IN2P3-CNRS, Palaiseau, France20: Also at Alstom Contracting, Geneve, Switzerland21: Also at Scuola Normale e Sezione dell’ INFN, Pisa, Italy22: Also at University of Athens, Athens, Greece23: Also at The University of Kansas, Lawrence, USA24: Also at Institute for Theoretical and Experimental Physics, Moscow, Russia25: Also at Paul Scherrer Institut, Villigen, Switzerland26: Also at Vinca Institute of Nuclear Sciences, Belgrade, Serbia27: Also at University of Wisconsin, Madison, USA28: Also at Mersin University, Mersin, Turkey29: Also at Izmir Institute of Technology, Izmir, Turkey30: Also at Kafkas University, Kars, Turkey31: Also at Suleyman Demirel University, Isparta, Turkey32: Also at Ege University, Izmir, Turkey33: Also at Rutherford Appleton Laboratory, Didcot, United Kingdom34: Also at INFN Sezione di Perugia; Universita di Perugia, Perugia, Italy35: Also at KFKI Research Institute for Particle and Nuclear Physics, Budapest, Hungary36: Also at Istanbul Technical University, Istanbul, Turkey37: Also at University of Minnesota, Minneapolis, USA38: Also at Institute for Nuclear Research, Moscow, Russia

29

39: Also at Texas A&M University, College Station, USA40: Also at State Research Center of Russian Federation, Institute for High Energy Physics,Protvino, Russia