| dc.contributor.author | 
Mishra, Madhukar | 
 | 
| dc.date.accessioned | 
2024-02-13T07:18:14Z | 
 | 
| dc.date.available | 
2024-02-13T07:18:14Z | 
 | 
| dc.date.issued | 
2011-07 | 
 | 
| dc.identifier.uri | 
https://link.springer.com/article/10.1007/s12648-011-0088-5 | 
 | 
| dc.identifier.uri | 
http://dspace.bits-pilani.ac.in:8080/jspui/xmlui/handle/123456789/14251 | 
 | 
| dc.description.abstract | 
We extend our previous formalism [Phys. Lett. B 656 45 (2007)] on J/ψ suppression at midrapidity using the colour screening framework. Our formalism is more general as the complete rapidity, transverse momentum and centrality dependence including J/ψ suppression at forward as well as mid-rapidity can be computed directly from it. We have assumed that QGP fluid is expanding obeying Bjorken’s boost invariant scaling law and bag model EOS is used. Sequential melting of χ c (1P) as well as ψ′ (2S) higher resonances is incorporated. We find that our model shows a reasonable agreement with the mid and forward rapidity data. Furthermore, we observe a larger suppression at forward rapidity in our model which is again well supported by the PHENIX data. | 
en_US | 
| dc.language.iso | 
en | 
en_US | 
| dc.publisher | 
Springer | 
en_US | 
| dc.subject | 
Physics | 
en_US | 
| dc.subject | 
Relativistic Heavy Ion Collider (RHIC) | 
en_US | 
| dc.title | 
J/ψ suppression vs centrality at forward and mid-rapidity in Au+Au collisions at RHIC in colour screening mechanism | 
en_US | 
| dc.type | 
Article | 
en_US |