Physics with ALICE-PMD Basanta K. Nandi IIT Bombay For PMD collaboration Photon Multiplicity Detector (PMD) in ALICE PMD Distance from IP : 367 cm Approx. 9 sq.m. η Covergae : 2.3 to 3.9 2 Photon Multiplicity Detector Cell depth : 0.5 cm Cell cross-section : 0.23 cm2 Total no. of cells : 220 K Sensitive medium : Gas (Ar+CO2 in the ratio 70:30) Honeycomb chamber (48×96 cells) 3 Principle of Photon Multiplicity Detector Energy deposition in PMD Hadron Photon Edep (a.u.) 4 Particle CPV PRE Photon No Yes Ch Hadron Yes Yes Photon Multiplicity Detector PMD measures: - Event-by-event number of photons produced in heavy-ion collisions - Spatial distribution (x,y) or (,) of photons Physics Capabilities: - Pseudo-rapidity density - Limiting Fragmentation - Fluctuation in the ratio of N/Nch in the common coverage of PMD & FMD - Azimuthal anisotropy and event plane determination - Charged particle multiplicity - Jet ??? 5 Charged Particle pseudo-rapidity Density Au + Au at mid-rapidity Particle production mechanism Soft process : Nch/γ scales with Npart 200 GeV 130 GeV 19.6 GeV Hard process : Nch/γ scales with Ncoll dNch/d = A x Npart + B x Ncoll • Hard processes contribution increases with centrality from ~30% to 50% in the mid-rapidity Rapidity distribution of charged particles and photons gives the input to the theorist to validate their model Q. What happens at higher energy? 6 Charged Particle pseudo-rapidity Density Q. What happens in the forward rapidity for photons? 7 Pseudo-rapidity distributions of Photons 900 GeV p+p 7 TeV p+p ALICE PRELIMINARY 8 At 0.9 TeV Phojet explains the data where as Pythia6D6T and Pythia6ATLAS underpredict. At 7 TeV both Pythia and Phojet under-predict the data. Limiting Fragmentation Particle production is independent of beam energy near beam rapidity Q. Is the limiting fragmentation scenario valid for photons? 9 Limiting fragmentation (LF) behavior of photons Limiting fragmentation behavior of photons seems to be inline with the earlier measurement. 10 Elliptic Flow Flow is a phenomenon seen in nucleus-nucleus collisions, which correlates the momentum distributions of the produced particles with the spatial eccentricity of the overlap region. azimuthal dependence of the pressure gradient. y py x y x z Reaction plane: z-x plane 2 2 y x 2 2 y x p y 1 v cos 2 , tan ( ) 2 p x 3 d N 1 d N v cos 2 2 2 E 1 2 v cos n n RP 3 d p 2 p d d p y t t n 1 11 Event Plane Determination from PMD PMD event plane determination codes are in the repository for global use 12 Charged particle measurement FMD 1 FMD 2 FMD 3 Outer ing Inner ring PMD Similar Eta acceptance of FMD2I and CPV = 2.3 = 3.5 FMD2i IP FMD1 PRE 13 CPV FMD2 o Beam line FMD3i Z-axis FMD3o Method to determine primary Charged Particles I.P. @ z = 0 CPV FMD X-Y plane @ z = 0 Principle – Three point straight line tracking Necessity – Magnetic Field OFF data 14 Method to determine primary Charged Particles Y X R = √(x2 + y2) 15 Charged particle measurement using CPV 16 Jet Study using PMD ? p p TPC 17 PMD Physics studies other than PMD Fluctuation in mid-rapidity K* measurement Anti-Nuclei search 18 Centrality Dependence of νdyn 10% Centrality Bins 5% Centrality Bins Measurement of K* 20 Anti-Nuclei Search in ALICE pp @ 7 TeV Approximately 350 M events are analyzed Various nuclei are nicely identified in ALICE 21 Summary: 22