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

Chemical freeze-out study in proton-proton collisions at RHIC and LHC energies

17 Feb 2016, 15:00
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 8

Speaker

SABITA DAS (NISER, Bhubaneswar, India)

Description

Particle multiplicities measured at Relativistic Heavy Ion Collider (RHIC) and Large Hadron Collider (LHC) facilities can be used to understand the chemical freeze-out dynamics. At chemical freeze-out (CFO), inelastic collisions cease and the freeze-out parameters can be determined using measured particle multiplicities within the framework of a statistical model.The statistical model has proven to be quite successful in describing the particle production from elementary $p-p$ and $e^{+}e^{-}$ collisions up to heavy-ion collisions [1,2]. It helps to do a systematic study of the centrality and energy dependence of freeze-out parameters in heavy-ion collisions from lower SPS to higher LHC energies [3]. The new data at LHC along with the RHIC data can be used to do such a systematic study in proton-proton collisions. Here, we will present the particle production in proton-proton collisions within a statistical model at RHIC center-of-mass energy $\sqrt{s}$ = 200 GeV and at LHC center-of-mass energy $\sqrt{s}$ = 900 GeV and 7 TeV. In this model, particle production is described by a set of thermal parameters like the temperature, the volume and the set of chemical potentials corresponding to different conserved quantities such as baryon number, strangeness and charge. Two different freeze-out schemes have been used for this study. One is single freeze-out (1CFO) [4] where all hadrons freeze-out together. Other one is double freeze-out (2CFO) [5] where strange and non-strange hadrons freeze-out separately giving two different sets of parameters. We will discuss the energy dependence of different chemical freeze-out parameters in 1CFO. The freeze-out parameters are also extracted in 2CFO and compared with 1CFO. The non-strange temperature is found to be lower than that of strange temperature in 2CFO for all energies studied here which can be interpreted as the early freeze-out of strange hadrons. The freeze-out parameters from 1CFO found to lie intermediate to the corresponding strange and non-strange values of 2CFO. **References** 1. J. Cleymans et al. Phys. Rev. C 79, 014901 (2009). 2. J. Cleymans and K. Redlich, Phys. Rev. C 60, 054908 (1999). 3. S. Chatterjee et al., Adv. in High Eng. Phys., Vol. 2015, Review Article ID: 349013. 4. S. Wheaton and J. Cleymans, Comput. Phys. Commun. 180, 84 (2009). 5. S. Chatterjee, R. Godbole, and S. Gupta, Phys. Lett. B 727, 554(2013).

Primary author

SABITA DAS (NISER, Bhubaneswar, India)

Co-authors

Bedangadas Mohanty (NISER, Bhubaneshwar, India) DEBADEEPTI MISHRA (NISER, Bhubaneshwar, India) Sandeep Chatterjee (Variable Energy Cyclotron Centre)

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