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NUCLEUS-NUCLEUS COLLISION Centrality Determination For NICA/MPD
ZDC RESOLUTION A.M. SEHONE Supervisor: A. Litvinenko 17 November 2018 Alfred Mogotsi Sehone
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Outline. Introduction Multiplicity ZDC Conclusions 17 November 2018
Alfred Mogotsi Sehone
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Nuclotron-based Ion Collider fAcility - NICA
Nuclei up to the gold Energy up to 4 – 4.5 GeV/(N) (each beam) 17 November 2018 Alfred Mogotsi Sehone
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Multi-Purpose Detector - MPD
Collision Region Detectors: Inner Tracker (IT) Barrel Tracker (BT) End Cap Tracker (ECT) Time of Flight (TOF) Electromagnetic Calorimeter (ECAL) Beam-Beam Counters (BBC) Zero Degree Calorimeter (ZDC) 17 November 2018 Alfred Mogotsi Sehone
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Why people study nucleus-nucleus collisions?
To describe particle formation with the application of statistical models. Information about the phase diagram (QCD phase diagram) Production of Hadrons that carry strange and charm quarks (exotic particles) with information about the QGP phase. To give some information on the early evolution of the universe. 17 November 2018 Alfred Mogotsi Sehone
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Can the impact parameter (b) measured?
b cannot be measured directly. Experimental results are presented in windows of energy deposited in a zero-degree calorimeter, number of participants, multiplicity, etc. b 17 November 2018 Alfred Mogotsi Sehone
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Centrality Classification:
Central collision --- b = 0 Small number of spectator particles Large number of participant particles Peripheral collision --- b ~ 2R (R = nuclei radii) Large number of spectator particles Small number of participant particles 2R 17 November 2018 Alfred Mogotsi Sehone
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How centrality is measured in other experiments:
Multiplicity Number of particles produced in a collision Needs more time to reach equilibrium after the interaction. Cannot get a reliable data in the hot QGP. γ emission 17 November 2018 Alfred Mogotsi Sehone
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ZDC A Hadron calorimeter or a Zero Degree Calorimeter is a detector that detects and measures the energy of neutrons, protons and light nuclei emitted along the direction of the beam. Event characterization and triggering purposes. A compensated/corrected Iron-Modular scintillators - to obtain equal signals produced by hadronic and electromagnetic showers. 17 November 2018 Alfred Mogotsi Sehone
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Results from the NA49 ( Pb+Pb Collision)
17 November 2018 Alfred Mogotsi Sehone
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Layout of the ZDC ZDC > 20 Fe + 5 Sc Interaction length = 5
Fe (20mm) Scintillator (5mm) 1 set 40 sets Spectators PMT Light fibers Beam 17 November 2018 Alfred Mogotsi Sehone
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ZDC CENTRAL COLLISION PERIPHERAL 17 November 2018
Alfred Mogotsi Sehone
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ZDC Evaporated nucleons Uniform 17 November 2018 Alfred Mogotsi Sehone
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Energy distribution for nucleons of different energies
ZDC No.1 17 November 2018 Alfred Mogotsi Sehone
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Monte-Carlo simulation results + Root package:
The kinetic, mean and dispersion energy of the detected particles were fitted in a linearity graph using a statistical model. Determines whether the difference between the observed and predicted values are significant. 17 November 2018 Alfred Mogotsi Sehone
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ZDC Resolution and Linearity
pN = 3GeV/c pN = 4GeV/c pN = 5GeV/c pN = 3GeV/c pN = 4GeV/c pN = 5GeV/c 17 November 2018 Alfred Mogotsi Sehone
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Conclusions The energy deposited by the spectator particles to the ZDC and the ZDC signal are linearly related. The resolution of the ZDC can be used in a Monte-Carlo simulation to specify the impact parameter for centrality purposes and event triggering. With the use of Root package and statistical models, a better fitting results for the resolution can be obtained. 17 November 2018 Alfred Mogotsi Sehone
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THANK YOU FOR YOUR ATTENTION...
17 November 2018 Alfred Mogotsi Sehone
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BACKUP SLIDES 17 November 2018 Alfred Mogotsi Sehone
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Number of participants
Number of collisions 17 November 2018 Alfred Mogotsi Sehone
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NA49 ZDC Only PHOBOS Paddle only PHENIX BBC & ZDC 17 November 2018
Alfred Mogotsi Sehone
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17 November 2018 Alfred Mogotsi Sehone
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17 November 2018 Alfred Mogotsi Sehone
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Magnetic Field 17 November 2018 Alfred Mogotsi Sehone
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