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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Main Authors: Alexander A. Potapov, Guzel M. Garipova, Kamal K. Nandi
Format: Article
Language:English
Published: Elsevier 2016-02-01
Series:Physics Letters B
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S0370269315009132
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spelling 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
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