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Subtracting combinatorial background in μ + μ - spectra

Subtracting combinatorial background in μ + μ - spectra. Using μ + μ + and μ - μ - pairs or a recombination method (mixing event) Hypothesizes, advantages, disadvantages… Real data and simulation (first attempt)

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Subtracting combinatorial background in μ + μ - spectra

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  1. Subtracting combinatorial background in μ+μ- spectra Using μ+μ+ and μ-μ- pairs or a recombination method (mixing event) Hypothesizes, advantages, disadvantages… Real data and simulation (first attempt) What must be done to check that we can use the method using μ+μ+ and μ-μ- pairs.

  2. Using μ+μ+ and μ-μ- pairs • Hypothesizes: H1: Muons from a pair are not physically correlated H2: No correlation between meson + and – multiplicities H3: Multiplicities follow a Poisson distribution • Experimental constraint: Accμ+μ-(M0) = Accμ+μ+(M0) = Accμ-μ-(M0)  Nμ+μ+ / Nμ-μ- • Nμ+μ-(Bgr) = 2 (Nμ+μ+ Nμ-μ-)½ ≈ Nμ+μ+ + Nμ-μ- Nμ+μ-(Sgl) = Nμ+μ- - Nμ+μ-(Bgr) for A-A

  3. Using μ+μ+ and μ-μ- pairs in p-p, p-A… Small multiplicities H2 (no correlation between mesons + and mesons -) not right: Nμ+μ-(Bgr) = 2 R (Nμ+μ+ Nμ-μ-)½, R>1 R estimated using MC simulation

  4. Recombination method • Hypothesis:muon kinematical distributions from pairs identical with distributions if measure muons individually • Condition:combination between muons from same Δzvertex and Δb class of events • Advantages: - high statistics - do not need Accμ+ = Accμ- • Difficulties: - Bias introduced by cuts - Uncertainty calculation

  5. Au-Au mass spectra no ghost Real Data (runs 28284+28286+ 28302 Sept 17th-18th) Simulation: Central + J/ψ (MDC) (49300 evts) ZDCNS*BBCLL1≥2

  6. Au-Au mass spectra no ghost Real Data (runs 28284+28286+ 28302 Sept 17th-18th) Simulation: Central + J/ψ (MDC) (49300 evts) ZDCNS*BBCLL1≥2

  7. Au-Au pT and y spectra Real Data (runs 28284+28286+ 28302 Sept 17th-18th) ZDCNS*BBCLL1≥2

  8. What must be done • Check if Accμ+μ-(X) = Accμ+μ+(X) = Accμ-μ-(X), (X=M, pT, y…) and/or Accμ+= Accμ+ ▪ simulations: - with a perfect detector - introducing dead channels: 1) FEM 2) HV ▪ real data: - study Nμ+μ+/Nμ-μ- versus M, pT, y • See which cuts applying • Understand why 2*(Nμ+μ+ Nμ-μ-)½ > Nμ+μ- at low masses • Check if the value of Nμ+μ+/Nμ-μ- is reproduced by the simulation

  9. References Recombination methods in PHENIX central arms – e’s: • Y. Akiba: https://www.phenix.bnl.gov:8080/phenix/WWW/p/draft/akiba/01.01/ AN_PART2.pdf • F. Matathias: http://www.phenix.bnl.gov/phenix/WWW/p/lists/phenix-heavy-l/recent/msg00240.html Recombination method and R calculation in NA38/NA50: • “Etude de la production du J/ψ dans les réactions p-Cu, p-U, O-U et S-U à 200 GeV par nucléon” PhD thesis S. Papillon, Paris-7 university (March 1991), IPNO-T.91.03 • “Estimation of the combinatorial background in dimuon spectra using recombination of muons, and associated error” S. Constantinescu, S. Dita, D. Jouan (1996), IPNO-DRE-96-01 • “Intermediate mass dimuons in ultrarelativistic proton-nucleus and nucleus-nucleus collisions at the CERN-SPS” PhD thesis Cristina Soave, Tesi di Dottorato di Ricerca, Università Degli Studi Di Torino, April 1998. (see chapter 5) http://na50.web.cern.ch/NA50/theses.html Limit of the methods estimating the combinatorial background: • M. Gaździcki and M. I. Gorenstein hep-ph/0003319 Combinatorial background in ALICE: • P. Crochet and P. Braun-Munzinger nucl-ex/0106008

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