Flat central density profile and constant dark matter surface density in galaxies from scalar field dark matter

被引:118
作者
Robles, Victor H. [1 ]
Matos, T. [1 ]
机构
[1] Inst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Fis, Mexico City 07000, DF, Mexico
关键词
galaxies: fundamental parameters; cosmology: observations; dark matter; BRIGHTNESS GALAXIES; ROTATION CURVES; HALO; MODELS;
D O I
10.1111/j.1365-2966.2012.20603.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Using the scalar field dark matter (SFDM) model, it is proposed that galaxies form by condensation of a scalar field (SF) very early in the Universe, forming Bose-Einstein condensate (BEC) drops (i.e. in this model, the haloes of galaxies are gigantic drops of SF). Here, as in the Lambda cold dark matter (LCDM) model, large structures form by hierarchy, and thus all the predictions of the LCDM model at large scales are reproduced by the SFDM model. This model predicts that all galaxies must be very similar and must exist for larger redshifts than in the LCDM model. In this paper, we show that BEC dark matter haloes fit the high-resolution rotation curves of a sample of 13 low-surface-brightness galaxies. We compare our fits to those obtained using Navarro-Frenk-White and pseudo-isothermal (PI) profiles. We have found better agreement with the SFDM and PI profiles. The mean value of the logarithmic inner density slopes is alpha = -0.27 +/- 0.18. As a second result, we find a natural way to define the core radius with the advantage of being model-independent. Using this new definition in the BEC density profile, we find that the recent observation of the constant dark matter central surface density can be reproduced. We conclude that, in light of the difficulties that the standard model is currently facing, the SFDM model could be a worthy alternative to enable us to continue exploring further.
引用
收藏
页码:282 / 289
页数:8
相关论文
共 51 条
[1]   Galactic collapse of scalar field dark matter [J].
Alcubierre, M ;
Guzmán, FS ;
Matos, T ;
Núñez, D ;
Ureña-López, LA ;
Wiederhold, P .
CLASSICAL AND QUANTUM GRAVITY, 2002, 19 (19) :5017-5024
[2]  
Athanassoula E., 1987, A A, V179, P2340
[3]   EXTENDED ROTATION CURVES OF SPIRAL GALAXIES - DARK HALOES AND MODIFIED DYNAMICS [J].
BEGEMAN, KG ;
BROEILS, AH ;
SANDERS, RH .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1991, 249 (03) :523-537
[4]  
Bernal A, 2008, REV MEX ASTRON ASTR, V44, P149
[5]   Can dark matter be a Bose-Einstein condensate? [J].
Bohmer, C. G. ;
Harko, T. .
JOURNAL OF COSMOLOGY AND ASTROPARTICLE PHYSICS, 2007, (06)
[6]   Universal Properties of Dark Matter Halos [J].
Boyarsky, A. ;
Neronov, A. ;
Ruchayskiy, O. ;
Tkachev, I. .
PHYSICAL REVIEW LETTERS, 2010, 104 (19)
[7]  
Boyarsky A., 2009, ARXIV09111774V1
[8]   THE STRUCTURE OF DARK-MATTER HALOS IN DWARF GALAXIES [J].
BURKERT, A .
ASTROPHYSICAL JOURNAL, 1995, 447 (01) :L25-L28
[9]   Mass-radius relation of Newtonian self-gravitating Bose-Einstein condensates with short-range interactions. II. Numerical results [J].
Chavanis, Pierre-Henri ;
Delfini, Luca .
PHYSICAL REVIEW D, 2011, 84 (04)
[10]   Mass-radius relation of Newtonian self-gravitating Bose-Einstein condensates with short-range interactions. I. Analytical results [J].
Chavanis, Pierre-Henri .
PHYSICAL REVIEW D, 2011, 84 (04)