000322924 001__ 322924
000322924 003__ SzGeCERN
000322924 005__ 20211222041121.0
000322924 0247_ $$2DOI$$a10.1007/s002880050588
000322924 0248_ $$aoai:cds.cern.ch:322924$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
000322924 035__ $$9CERN annual report$$a98-1135
000322924 035__ $$a0246175CERCER
000322924 035__ $$9SPIRES$$a3529177
000322924 035__ $$9arXiv$$aoai:arXiv.org:hep-ph/9703396
000322924 035__ $$9Inspire$$a441492
000322924 037__ $$9arXiv$$ahep-ph/9703396$$chep-ph
000322924 037__ $$aHZPP-9701
000322924 041__ $$aeng
000322924 088__ $$aHZPP-97-001
000322924 100__ $$aAdamovich, M.I.
000322924 245__ $$aNuclear Effect in Higher-Dimensional Factorial Moment Analysis of the $^{16}O$-, $^{32}S$- and $^{197}Au$-$Em$ Interaction Data at 200, 60 and 11 AGeV/c
000322924 260__ $$c1997
000322924 269__ $$aWuhan$$bHua-Zhong Teacher's Coll. Inst. Part. Phys.$$c24 Mar 1997
000322924 300__ $$a10 p
000322924 340__ $$apaper
000322924 500__ $$9arXiv$$aLatex, 7 pages, 6 figures in 2 PS files, submitted to Z. Phys. C
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ^{16}O-, ^{32}S- and ^{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ~{16}O-, ~{32}S- and ~{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 520__ $$9arXiv$$aThe anomalous behavior of 2-dimensional factorial moment in nucleus-nucleus collisions is studied in some detail using both mini-bias and central collision data of ^{16}O-, ^{32}S- and ^{197}Au-Em interactions from EMU01 experiment. The correct value for the effective Hurst exponent in the analysis of higher-dimensional factorial moment is found to be greater than unity, showing clearly the existence of superposition effect in nucleus-nucleus collisions.
000322924 595__ $$aLANL EDS
000322924 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
000322924 690C_ $$aARTICLE
000322924 690C_ $$aCERN
000322924 693__ $$aCERN SPS$$eEMU01
000322924 695__ $$9LANL EDS$$ahep-ph
000322924 700__ $$aAggarwal, M.M.
000322924 700__ $$aAlexandrov, Y.A.
000322924 700__ $$aAmirikas, R.
000322924 700__ $$aAndreeva, N.P.
000322924 700__ $$aAvetian, F.A.
000322924 700__ $$aBadyal, S.K.
000322924 700__ $$aBakich, A.M.
000322924 700__ $$aBasova, E.S.
000322924 700__ $$aBhalla, K.B.
000322924 700__ $$aBhasin, A.
000322924 700__ $$aBhatia, V.S.
000322924 700__ $$aBogdanov, V.G.
000322924 700__ $$aBradnova, V.
000322924 700__ $$aBubnov, V.I.
000322924 700__ $$aCai, X.
000322924 700__ $$aChasnikov, I.Y.
000322924 700__ $$aChen, G.M.
000322924 700__ $$aChernova, L.P.
000322924 700__ $$aChernyavsky, M.M.
000322924 700__ $$aDeng, Y.
000322924 700__ $$aDhamija, S.
000322924 700__ $$aEl Chenawi, K.
000322924 700__ $$aFelea, D.
000322924 700__ $$aFeng, S.Q.
000322924 700__ $$aGaitinov, A.S.
000322924 700__ $$aGanssauge, E.R.
000322924 700__ $$aGarpman, S.
000322924 700__ $$aGerasimov, S.G.
000322924 700__ $$aGheata, A.
000322924 700__ $$aGheata, M.
000322924 700__ $$aGrote, J.
000322924 700__ $$aGulamov, K.G.
000322924 700__ $$aGupta, S.K.
000322924 700__ $$aGupta, V.K.
000322924 700__ $$aHaiduc, M.
000322924 700__ $$aHasegan, D.
000322924 700__ $$aHu, Z.R.
000322924 700__ $$aJakobsson, B.
000322924 700__ $$aJust, L.
000322924 700__ $$aKanygina, E.K.
000322924 700__ $$aKarabova, M.
000322924 700__ $$aKharlamov, S.P.
000322924 700__ $$aKim, Y.C.
000322924 700__ $$aKovalenko, A.D.
000322924 700__ $$aKrasnov, S.A.
000322924 700__ $$aKumar, V.
000322924 700__ $$aLarionova, V.G.
000322924 700__ $$aLee, C.G.
000322924 700__ $$aLepekhin, F.G.
000322924 700__ $$aLevitskaya, O.V.
000322924 700__ $$aLi, Y.X.
000322924 700__ $$aLiang, L.
000322924 700__ $$aLiu, L.S.
000322924 700__ $$aLiu, Z.G.
000322924 700__ $$aLokanathan, S.
000322924 700__ $$aLord, J.J.
000322924 700__ $$aLu, Y.
000322924 700__ $$aLukicheva, N.S.
000322924 700__ $$aLuo, S.B.
000322924 700__ $$aMangotra, L.K.
000322924 700__ $$aMarutian, N.A.
000322924 700__ $$aMittra, I.S.
000322924 700__ $$aMusaeva, A.K.
000322924 700__ $$aNasyrov, S.Z.
000322924 700__ $$aNavotny, V.S.
000322924 700__ $$aNilsson, P.
000322924 700__ $$aNystrand, J.
000322924 700__ $$aOrlova, G.I.
000322924 700__ $$aOtterlund, I.
000322924 700__ $$aPavukova, A.
000322924 700__ $$aPeak, L.S.
000322924 700__ $$aPeresadko, N.G.
000322924 700__ $$aPetrov, N.V.
000322924 700__ $$aPlyushchev, V.A.
000322924 700__ $$aQian, W.Y.
000322924 700__ $$aQin, Y.M.
000322924 700__ $$aRaniwala, R.
000322924 700__ $$aRao, N.K.
000322924 700__ $$aRhee, J.T.
000322924 700__ $$aRoeper, M.
000322924 700__ $$aRusakova, V.V.
000322924 700__ $$aSaidkhanov, N.
000322924 700__ $$aSalmanova, N.A.
000322924 700__ $$aSarkisova, L.G.
000322924 700__ $$aSarkisian, V.R.
000322924 700__ $$aSeitimbetov, A.M.
000322924 700__ $$aSeliverstov, D.M.
000322924 700__ $$aSethi, R.
000322924 700__ $$aShakhova, C.I.
000322924 700__ $$aSimonov, B.B.
000322924 700__ $$aSingh, B.
000322924 700__ $$aSkelding, D.
000322924 700__ $$aSkorobogatova, V.I.
000322924 700__ $$aSoderstrom, K.
000322924 700__ $$aStenlund, E.
000322924 700__ $$aSvechnikova, L.N.
000322924 700__ $$aTawfik, A.M.
000322924 700__ $$aTothova, M.
000322924 700__ $$aTretyakova, M.I.
000322924 700__ $$aTrofimova, T.P.
000322924 700__ $$aTuleeva, U.I.
000322924 700__ $$aVashisht, V.
000322924 700__ $$aVokal, S.
000322924 700__ $$aVrlakova, J.
000322924 700__ $$aWang, H.Q.
000322924 700__ $$aWang, S.H.
000322924 700__ $$aWang, X.R.
000322924 700__ $$aWeng, Z.Q.
000322924 700__ $$aWilkes, R.J.
000322924 700__ $$aYang, C.B.
000322924 700__ $$aYin, Z.B.
000322924 700__ $$aYu, L.Z.
000322924 700__ $$aYu, Y.L.
000322924 700__ $$aXu, G.F.
000322924 700__ $$aZhang, D.H.
000322924 700__ $$aZheng, P.Y.
000322924 700__ $$aZhokhova, S.I.
000322924 700__ $$aZhou, D.C.
000322924 710__ $$gEMU01 Collaboration
000322924 710__ $$5PPE
000322924 773__ $$c659-663$$pZ. Phys. C$$v76$$y1997
000322924 852__ $$cCERN Central Library$$hhep-ph/9703396
000322924 8564_ $$uhttp://arxiv.org/pdf/hep-ph/9703396$$yFulltext
000322924 8564_ $$82319021$$s222412$$uhttps://cds.cern.ch/record/322924/files/arXiv:hep-ph_9703396.pdf
000322924 916__ $$sn$$w199713$$ya1998
000322924 960__ $$a13
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