Revisiting perfect fluid dark matter: Observational constraints from our galaxy
We revisit certain features of an assumed spherically symmetric perfect fluid dark matter halo in the light of the observed data of our galaxy, the Milky Way (MW). The idea is to apply the Faber–Visser approach of combined observations of rotation curves and lensing to a first post-Newtonian approxi...
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doaj-e683f150355c4e1e9f27abb709379bf72020-11-24T22:37:38ZengElsevierPhysics Letters B0370-26931873-24452016-02-01753C14014610.1016/j.physletb.2015.11.057Revisiting perfect fluid dark matter: Observational constraints from our galaxyAlexander A. Potapov0Guzel M. Garipova1Kamal K. Nandi2Department of Physics & Astronomy, Bashkir State University, Sterlitamak Campus, Sterlitamak 453103, RB, RussiaDepartment of Physics & Astronomy, Bashkir State University, Sterlitamak Campus, Sterlitamak 453103, RB, RussiaDepartment of Physics & Astronomy, Bashkir State University, Sterlitamak Campus, Sterlitamak 453103, RB, RussiaWe revisit certain features of an assumed spherically symmetric perfect fluid dark matter halo in the light of the observed data of our galaxy, the Milky Way (MW). The idea is to apply the Faber–Visser approach of combined observations of rotation curves and lensing to a first post-Newtonian approximation to “measure” the equation of state ω(r) of the perfect fluid galactic halo. However, for the model considered here, no constraints from lensing are used as it will be sufficient to consider only the rotation curve observations. The lensing mass together with other masses will be just computed using recent data. Since the halo has attractive gravity, we shall impose the constraint that ω(r)≥0 for r≤RMW, where RMW∼200 kpc is the adopted halo radius of our galaxy. The observed circular velocity ℓ (=2vc2/c02) from the flat rotation curve and a crucial adjustable parameter D appearing in the perfect fluid solution then yield different numerical ranges of ω(r). It is demonstrated that the computed observables such as the rotation curve mass, the lens mass, the post-Newtonian mass of our galaxy compare well with the recent mass data. We also calculate the Faber–Visser χ-factor, which is a measure of pressure content in the dark matter. Our analysis indicates that a range 0≤ω(r)≤2.8×10−7 for the perfect fluid dark matter can reasonably describe the attractive galactic halo. This is a strong constraint indicating a dust-like CDM halo (ω∼0) supported also by CMB constraints.http://www.sciencedirect.com/science/article/pii/S0370269315009132Dark matterPerfect fluidEquation of stateGalactic masses |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Alexander A. Potapov Guzel M. Garipova Kamal K. Nandi |
spellingShingle |
Alexander A. Potapov Guzel M. Garipova Kamal K. Nandi Revisiting perfect fluid dark matter: Observational constraints from our galaxy Physics Letters B Dark matter Perfect fluid Equation of state Galactic masses |
author_facet |
Alexander A. Potapov Guzel M. Garipova Kamal K. Nandi |
author_sort |
Alexander A. Potapov |
title |
Revisiting perfect fluid dark matter: Observational constraints from our galaxy |
title_short |
Revisiting perfect fluid dark matter: Observational constraints from our galaxy |
title_full |
Revisiting perfect fluid dark matter: Observational constraints from our galaxy |
title_fullStr |
Revisiting perfect fluid dark matter: Observational constraints from our galaxy |
title_full_unstemmed |
Revisiting perfect fluid dark matter: Observational constraints from our galaxy |
title_sort |
revisiting perfect fluid dark matter: observational constraints from our galaxy |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 1873-2445 |
publishDate |
2016-02-01 |
description |
We revisit certain features of an assumed spherically symmetric perfect fluid dark matter halo in the light of the observed data of our galaxy, the Milky Way (MW). The idea is to apply the Faber–Visser approach of combined observations of rotation curves and lensing to a first post-Newtonian approximation to “measure” the equation of state ω(r) of the perfect fluid galactic halo. However, for the model considered here, no constraints from lensing are used as it will be sufficient to consider only the rotation curve observations. The lensing mass together with other masses will be just computed using recent data. Since the halo has attractive gravity, we shall impose the constraint that ω(r)≥0 for r≤RMW, where RMW∼200 kpc is the adopted halo radius of our galaxy. The observed circular velocity ℓ (=2vc2/c02) from the flat rotation curve and a crucial adjustable parameter D appearing in the perfect fluid solution then yield different numerical ranges of ω(r). It is demonstrated that the computed observables such as the rotation curve mass, the lens mass, the post-Newtonian mass of our galaxy compare well with the recent mass data. We also calculate the Faber–Visser χ-factor, which is a measure of pressure content in the dark matter. Our analysis indicates that a range 0≤ω(r)≤2.8×10−7 for the perfect fluid dark matter can reasonably describe the attractive galactic halo. This is a strong constraint indicating a dust-like CDM halo (ω∼0) supported also by CMB constraints. |
topic |
Dark matter Perfect fluid Equation of state Galactic masses |
url |
http://www.sciencedirect.com/science/article/pii/S0370269315009132 |
work_keys_str_mv |
AT alexanderapotapov revisitingperfectfluiddarkmatterobservationalconstraintsfromourgalaxy AT guzelmgaripova revisitingperfectfluiddarkmatterobservationalconstraintsfromourgalaxy AT kamalknandi revisitingperfectfluiddarkmatterobservationalconstraintsfromourgalaxy |
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