27 September 2015 to 3 October 2015
Kobe, Fashion Mart, Japan
Japan timezone

Probing Pb+Pb collisions at $\sqrt{s{\rm NN}} = $ 2.76 TeV using spectator neutrons

29 Sept 2015, 16:30
2h
Exhibition space 3 & 4

Exhibition space 3 & 4

Board: 0304
Poster Initial State Physics and Approach to Equilibrium Poster Session

Speaker

Bedangadas Mohanty (National Institute of Science Education and Research (IN))

Description

The primary goal in heavy ion collision (HIC) experiments is to characterise the properties of the hot and dense strongly interacting matter produced after the collision. A precise comparison between theoretical predictions and experimental data helps to select one theoretical model over another. However, one of the significant challenges in such endeavors is the ignorance of the initial condition at the time of collision. The nuclei being extended objects, there are event by event geometric fluctuations in addition to quantum fluctuations of the nuclear wave function. The standard method of analyzing the collisions in bins of centrality is only able to select events with the initial condition averaged over many possible initial states. In this work, we perform an additional binning in terms of total spectator neutrons in an event. A Multi Phase Transport (AMPT) model has been used in our analysis. We have used the left ($L$) going and right ($R$) going spectator neutrons to form the observable $L+R$ that can be measured in experiments using Zero Degree Calorimeters (ZDC). The spectator binning helps us to analyse rarer events whose property usually get masked in the standard analysis with centrality bins. We find that in a given centrality bin, events with different ellipticity can be selected with $L+R$ binning. This serves as a complementary technique to $q_2$-binning to analyse intial event shape. The advantage in using spectators is that they are never part of the fireball produced and hence are pristine carriers of the initial state information. We find that the scaling relation between $v_2/\varepsilon_2$ and $\left(1/S\right)dN_{ch}/d\eta$ obeyed by different centrality bins is broken by the $L+R$ bins, instead the hydrodynamic response for both centrality as well as $L+R$ bins exhibit scaling with the initial transverse dimension.
On behalf of collaboration: NONE

Primary author

Sandeep Chatterjee (Variable Energy Cyclotron Centre)

Co-authors

Bedangadas Mohanty (National Institute of Science Education and Research (IN)) Md. Rihan Haque (V) Vipul Bairathi (National Institute of Science Education and Research)

Presentation materials

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