Bound for entropy and viscosity ratio for strange quark matter
| dc.creator | Bagchi, Manjari | |
| dc.creator | Dey, Jishnu | |
| dc.creator | Dey, Mira | |
| dc.creator | Gangopadhyay, Taparati | |
| dc.creator | Laha, Sibasish | |
| dc.creator | Ray, Subharthi | |
| dc.creator | Sinha, Monika | |
| dc.date | 2007-05-31 | |
| dc.date | 2008-07-03 | |
| dc.date.accessioned | 2026-07-07T11:56:53Z | |
| dc.date.available | 2026-07-07T11:56:53Z | |
| dc.description | High energy density ($\eps$) and temperature (T) links general relativity and hydrodynamics leading to a lower bound for the ratio of shear viscosity ($η$) and entropy density ($s$). We get the interesting result that the bound is saturated in the simple model for quark matter that we use for strange stars at the surface for $T \sim 80 MeV$. At this $T$ we have the possibility of cosmic separation of phases. At the surface of the star where the pressure is zero - the density $\eps$ has a fixed value for all stars of various masses with correspondingly varying central energy density $\eps_c$. Inside the star where this density is higher, the ratio of $η/s$ is larger and are like the known results found for perturbative QCD. This serves as a check of our calculation. The deconfined quarks at the surface of the strange star at $T = 80 MeV$ seem to constitute the most perfect interacting fluid permitted by nature. | |
| dc.description | 10 pages, 2 figures, 1 table; Accepted for publication in Phys. Lett. B | |
| dc.identifier | https://arxiv.org/abs/0705.4645 | |
| dc.identifier | http://arxiv.org/abs/0705.4645 | |
| dc.identifier | Phys.Lett.B666:145-149,2008 | |
| dc.identifier | doi:10.1016/j.physletb.2008.07.008 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/205692 | |
| dc.subject | Astrophysics | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Bound for entropy and viscosity ratio for strange quark matter | |
| dc.type | text |