The restoration of chiral symmetry and its subsequent breaking through a phase transition has been predicted to create regions of Disoriented Chiral Condensates (DCC). This phenomenon has been predicted to cause anomalous fluctuations in the relative produ
determinationofthecentralityofeachcollision,weusethetransverseenergy(ET)measuredintheMidrapidityCalorimeter(MIRAC[13]).Forremovalofbackgroundevents,wealsousetheZero-DegreeCalorimeter(ZDC)andthePlasticBalldetector[14].
2.1Chargedparticlemultiplicity
WecountchargedparticlesusingacircularSiliconPadMultiplicityDetector(SPMD)[15]located32.8cmfromthetargetcovering2.35<η<3.75,thecentralrapidityregionatSPSenergies(whereηCMS=2.9),andfullazimuth.Thedetectorconsistsoffouroverlappingquadrants,eachfabricatedfromasingle300µmthicksiliconwafer.Theactiveareaofeachquadrantisdividedinto1012padsforming46azimuthalwedgesand22radialbinswithapadsizeincreasingwithradiustoprovideuniformpseudorapiditycoverage.Thee ciencyofdetectingachargedparticleintheactiveareahasbeendeterminedinatestbeamtobebetterthan99%.Conversely,thedetectoristransparenttohighenergyphotons,sinceonlyabout0.2%areexpectedtointeractinthesilicon.Duringthedatataking,95%ofthepadsworkedproperlyandareusedinthisanalysis.
Inacentralion-ioncollision,theoccupancycanbeashighas20%,imply-ingthat≈20%ofthepadscontaintwoormorehits.Anunbiasedwaytoestimatethetotalnumberofchargedparticlesinagiveneventundersuchconditionsistousethesumoftheenergydepositedinpadsexceeding1/2ofthemostprobableenergylossdividedbythemeanenergylossperparticleasdeterminedinlow-multiplicityevents:
Nch= dE/dxi
i=hits
N.For
typicalcentraleventswithamultiplicityof≈600,thisgivesanuncertaintyofabout2%.Tochecktheoverallscale,wecomparetheresultswiththemul-tiplicityobtainedbyassumingthattheparticlesaredistributeduniformlysothemulti-hitprobabilityisgivenbyPoissonstatistics.Asimplecalculation
′givesNch= Npadslog(1 Nhits/Npads),whereNpadsisthetotalnumberofpads,ingthisasacheck,weestimatethesystematicerroronNch,duetouncertaintiesinthegainsandbackgrounds,tobeabout4%.