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The Amplitude of Mass Fluctuations and Mass Density of the Universe Constrained by Strong Gravitational Lensing

The Amplitude of Mass Fluctuations and Mass Density of the Universe Constrained by Strong Gravitational Lensing
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摘要 We investigate the linear amplitude of mass fluctuations in the universe, σ8, and the present mass density parameter of the Universe, Ωm, from statistical strong gravitational lensing. We use the two population model of lens halos with fixed cooling mass scale Mc = 3×1013h-1M⊙ to match the observed lensing probabilities, and leave σ8 orΩm as a free parameter to be constrained by the data. Another varying parameter, the equation of state of dark energy ω, and its typical values of -1, -2/3, -1/2 and -1/3 are investigated. We find that σ8 is degenerate with Ωm in a way similar to that suggested by present day cluster abundance as well as cosmic shear lensing measurements: σ8Ω0.6m≈0.33. However, both σ8≤0.7 and Ωm≤0.2 can be safely ruled out, the best fit is when σ8 = 1.0, Ωm = 0.3 and ω= - 1. This result is different from that obtained by Bahcall & Bode, who gave σ8 = 0.98±0.1 and Ωm = 0.17 ±0.05. For σ8 = 1.0, the higher value ofΩm = 0.35 requires ω = -2/3 and Ωm = 0.40 requires ω= -1/2. We investigate the linear amplitude of mass fluctuations in the universe, σ8, and the present mass density parameter of the Universe, Ωm, from statistical strong gravitational lensing. We use the two population model of lens halos with fixed cooling mass scale Mc = 3×1013h-1M⊙ to match the observed lensing probabilities, and leave σ8 orΩm as a free parameter to be constrained by the data. Another varying parameter, the equation of state of dark energy ω, and its typical values of -1, -2/3, -1/2 and -1/3 are investigated. We find that σ8 is degenerate with Ωm in a way similar to that suggested by present day cluster abundance as well as cosmic shear lensing measurements: σ8Ω0.6m≈0.33. However, both σ8≤0.7 and Ωm≤0.2 can be safely ruled out, the best fit is when σ8 = 1.0, Ωm = 0.3 and ω= - 1. This result is different from that obtained by Bahcall & Bode, who gave σ8 = 0.98±0.1 and Ωm = 0.17 ±0.05. For σ8 = 1.0, the higher value ofΩm = 0.35 requires ω = -2/3 and Ωm = 0.40 requires ω= -1/2.
出处 《Chinese Journal of Astronomy and Astrophysics》 CSCD 北大核心 2004年第2期118-124,共7页 中国天文和天体物理学报(英文版)
基金 Supported by the National Natural Science Foundation of China
关键词 cosmology: theory - cosmological parameters - gravitational lensing cosmology: theory - cosmological parameters - gravitational lensing
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参考文献34

  • 1[1]Bahcall N. A., Bode P., 2003, Ap J, 588, L1
  • 2[2]Bahcall N. A., Fan X., 1998, Ap J, 504, 1
  • 3[3]Bahcall N. A., Fan X., Cen R., 1997, Ap J, 485, L53
  • 4[4]Bartelmann M., 1996, A&A, 313, 697
  • 5[5]Bond J. R., Contaldi C. R., Pen U. -L. et al., 2002, Ap J, submitted (astro-ph/0205386)
  • 6[6]Browne I. W., Meyers S. T., 2000, in New Cosmological Data and the Values of the Fundamental Parameters, IAU Symposium, 201, 47
  • 7[7]Browne I. W. A., Wilkinson P. N., Jackson N. J. F. et al., 2003, MNRAS, 341, 13
  • 8[8]Bullock J. S., Kolatt T. S., Sigad Y. et al., 2001, MNRAS, 321, 559
  • 9[9]Carlberg R. G.,Morris S. L., Yee H. K. C., Ellingson E., 1997, ApJ, 479, L19
  • 10[10]Chen D. -M., 2003a, Ap J, 587, L55 (Paper Ⅰ)

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