Title: Event By Event Fluctuation
1Event By Event Fluctuation in K/p ratio at RHIC
Supriya Das VECC, Kolkata (for STAR
Collaboration)
Present address GSI, Darmstadt
2Motivation
Statistical fluctuations Arise due
to the measurement process itself such as finite
number statistics
Dynamical fluctuations
Reflect the dynamics and responses of the
system (density fluctuations etc.)
- K/p ratio shows interesting
- behavior as function of
- collision energy.
- It would be interesting to
- see what happens to the
- fluctuation of the ratio.
Why K/p ?
3Search for QCD Phase Transition
The production of strangeness may be related to
the onset of deconfinement Excitation function
of ltKgt/lt?gt shows structure around sNN1/2 7
GeV The excitation function of ltK-gt/lt?-gt is
smooth
C. Blume (NA49), hep-ph/0505137
4Fluctuations in ltKgt/lt?gt
- Event-by-event fluctuations in ltKgt/lt?gt may give
insight into the production mechanism of Ks - NA49 measured dynamical fluctuation in K/p ratio
by comparing the width of distributions from data
and mixed events
PbPb at 158 A GeV (top 5 central)
S. V. Afanasiev et al. for NA 49 Collaboration
PRL 86 (2001)
5Fluctuations in ltKgt/lt?gt
NA49 has also measured thefluctuation of
ltKgt/lt??gtas a function of incidentenergy for
central PbPbcollisions from 6 to 17GeV using
the observable ?dyn
C. Roland QM 2004
6Relativistic Heavy Ion Collider
1 km
v 0.99995?c 186,000 miles/sec
7Solenoidal Tracker At RHIC
Tracking Detectors TPC, FTPC, SVT Calorimeters
BEMC, EEMC, ZDC Trigger Detectors CTB, BBC,
MWPC Photon Detector PMD
Others TOF, FPD
Goal to track all the hadrons (and photons) in
each collision
8Potential at STAR
- Large acceptance detector ( 2 units of h with
full f symmetry) - Good K to p separation (for a wide momentum
range) - from Time Projection Chamber
M. Anderson et al. for STAR Collaboration,
NIMA499 (2003)
9Dynamical fluctuation sdyn
- Kaons and Pions are counted event by event and
the - ratio is plotted for a large number of
events. - Same ratio is calculated from mixed events and
distribution - of that is obtained.
- Width of the distribution (s) is the measure of
fluctuation - Dynamical fluctuation, sdyn is calculated as
- sdyn ?(sdata2
smixed2)
10Phase space distributions of identified K and p
11Dynamical Fluctuation (contd)
Mixed Event
- To get the measure of the statistical
fluctuation from - Finite number statistics
- Experimental resolution
- Correlations if any
- Mixed track pool constructed by randomly picking
up one track - from each event.
- Same cuts applied on the mixed tracks before
applying the particle - identification.
12sdyn Kp for different center of mass energies
Data not corrected for efficiency
13Excitation Function for ?dyn
We extracted ?dyn for AuAu, 0 - 5 most central,
for 20, 62, 130, and 200 GeV and compared the
results with the NA49-SPS results
- Possibilities
- Related to K/? horn
- Increase of resonances decaying intoK ? with
increasing incident energy - Dilution of correlations as multiplicity
increases with energy
Statistical errors only
14Better Measure
- The use of ?dyn is problematic because it
involves event-by-event fluctuations of a ratio - A better measure is ?dyn,K?
- Insensitive to efficiency
- Properly deals with small multiplicities
- Centrality studies
- We will use ?dyn,K? for our systematic studies of
K/? fluctuations
First proposed by Pruneau, Gavin and Voloshin PRC
66 (2002) Used in STAR Net Charge fluctuation
paper PRC 68 (2003)
15Determination of collision centrality
Based on multiplicity of charged particles in the
STAR TPC (hlt0.5)
16Centrality dependence of dynamical fluctuation
for different collision energies
17Summary
- Excitation function of ?dyn remains flat at RHIC
energies. - Study of the excitation function and centrality
dependence of K/?? fluctuations requires a robust
variable like ?dyn,Kp . - ndyn,Kp is positive and it decreases with
increasing centrality of collisions for 62 and
200 GeV centre of mass energies. - We are looking into the detailed systematics of
20 and 130 GeV dataset to decrease the errors.
18STAR Collaboration