15–19 Feb 2016
IIC, New Delhi
Asia/Calcutta timezone

Production of light nuclei and measurement of coalescence parameter in heavy$-$ion collisions at RHIC

17 Feb 2016, 17:10
20m
Multi Purpose Hall (IIC, New Delhi)

Multi Purpose Hall

IIC, New Delhi

India International Centre, 40 Max Muller Marg, New Delhi, India
Parallel Session 11

Speaker

Md. Rihan Haque (NISER, Bhubaneswar(IN))

Description

A strongly interacting medium, namely Quark Gluon Plasma (QGP), is formed in high-energy heavy-ion collisions at RHIC. Light nuclei (anti-nuclei) can be produced in such heavy-ion collisions by the recombination of produced nucleons (anti-nucleons) or stopped nucleons. This formation process is called final-state coalescence. The production of light nuclei is dependent on the baryon density and the correlation (freeze-out) volume. Therefore, by studying the yield and azimuthal anisotropy of light nuclei (anti-nuclei) and comparing them with that of proton (anti-proton) we can gain insight in the particle production mechanism via coalescence and physical properties of the expanding system at the thermal (kinetic) freeze-out. Unlike the quark coalescence phenomena of identified hadrons, nucleonic coalescence is directly measurable as both the light nuclei and nucleons (proton and anti-proton) are measured by the detectors in a given experiment. In this presentation, we will show the invariant yields of $d$ and $\overline{d}$ for Au+Au collisions at $\sqrt{s_{NN}}$ = 7.7, 11.5, 19.6, 27, 39, 62.4 and 200 GeV from the STAR experiment at RHIC. Light nuclei are identified using the Time Projection Chamber (TPC) and Time-of-Flight (TOF) detector of the STAR experiment. The TOF detector enhances the identification of the light nuclei and extends the $p_{T}$ reach of light nuclei beyond 1 GeV/c. The $p_{T}$ spectra of nuclei will be compared with p $(\overline{p})$ to obtain the nuclei to nucleon ratio and $B_{2}$ parameter to understand the light nucleus production mechanism in heavy-ion collisions. Light nucleus spectra will also be compared with the prediction from Blast-wave model, using the fit parameters obtained from Blast-wave fit of $\pi$, K, p spectra.

Authors

Md. Rihan Haque (NISER, Bhubaneswar(IN)) for the STAR Collaboration

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