DETERMINING THE HUBBLE CONSTANT FROM HUBBLE PARAMETER MEASUREMENTS

We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts to determine the present-day Hubble constant H0 in four cosmological models. We measure , and Mpc−1 (1 errors) in the ΛCDM (spatially flat and non-flat), CDM, and φCDM models, respectively. These measured H0 values are m...

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Veröffentlicht in:The Astrophysical journal Jg. 835; H. 1; S. 86 - 89
Hauptverfasser: Chen, Yun, Kumar, Suresh, Ratra, Bharat
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Sprache:Englisch
Veröffentlicht: Philadelphia The American Astronomical Society 20.01.2017
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Abstract We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts to determine the present-day Hubble constant H0 in four cosmological models. We measure , and Mpc−1 (1 errors) in the ΛCDM (spatially flat and non-flat), CDM, and φCDM models, respectively. These measured H0 values are more consistent with the lower values determined from recent data on the cosmic microwave background and baryon acoustic oscillations, as well as with the value found from a median statistical analysis of Huchra's compilation of H0 measurements, but include the higher local measurements of H0 within the 2 confidence limits.
AbstractList We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts to determine the present-day Hubble constant H0 in four cosmological models. We measure , and Mpc−1 (1 errors) in the ΛCDM (spatially flat and non-flat), CDM, and φCDM models, respectively. These measured H0 values are more consistent with the lower values determined from recent data on the cosmic microwave background and baryon acoustic oscillations, as well as with the value found from a median statistical analysis of Huchra's compilation of H0 measurements, but include the higher local measurements of H0 within the 2 confidence limits.
We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts \(0.07\leqslant z\leqslant 2.3\) to determine the present-day Hubble constant H0 in four cosmological models. We measure \({H}_{0}={68.3}_{-2.6}^{+2.7},{68.4}_{-3.3}^{+2.9},{65.0}_{-6.6}^{+6.5}\), and \({67.9}_{-2.4}^{+2.4}\,\mathrm{km}\ {{\rm{s}}}^{-1}\) Mpc−1 (1σ errors) in the ΛCDM (spatially flat and non-flat), ωCDM, and ϕCDM models, respectively. These measured H0 values are more consistent with the lower values determined from recent data on the cosmic microwave background and baryon acoustic oscillations, as well as with the value found from a median statistical analysis of Huchra’s compilation of H0 measurements, but include the higher local measurements of H0 within the 2σ confidence limits.
We use 28 measurements of the Hubble parameter, H ( z ), at intermediate redshifts to determine the present-day Hubble constant H 0 in four cosmological models. We measure , and Mpc −1 (1 σ errors) in the ΛCDM (spatially flat and non-flat), ω CDM, and ϕ CDM models, respectively. These measured H 0 values are more consistent with the lower values determined from recent data on the cosmic microwave background and baryon acoustic oscillations, as well as with the value found from a median statistical analysis of Huchra’s compilation of H 0 measurements, but include the higher local measurements of H 0 within the 2 σ confidence limits.
We use 28 Hubble parameter, H($z$), measurements at intermediate redshifts 0.07 $\leqslant z \leqslant$ 2.3 to determine the present-day Hubble constant H0 in four cosmological models. We measure H0 = 68:3$^{+2.7}_{-2.6}$, 68.4$^{+2.9}_{-3.3}$, 65.0$^{+6.5}_{-6:6}$ and 67.9$^{+2.4}_{-2.4}$ km s-1 Mpc-1 ( σ errors) in the ΛCDM (spatially flat and non-flat), ωCDM and ΦCDM models, respectively. These measured H0 values are more consistent with the lower values determined from recent cosmic microwave background and baryon acoustic oscillation data, as well as with that found from a median statistics analysis of Huchra’s compilation of H0 measurements, but include the higher local measurements of H0 within the 2σ confidence limits.
Author Chen, Yun
Kumar, Suresh
Ratra, Bharat
Author_xml – sequence: 1
  givenname: Yun
  orcidid: 0000-0001-8919-7409
  surname: Chen
  fullname: Chen, Yun
  email: chenyun@bao.ac.cn
  organization: Chinese Academy of Sciences Key Laboratory for Computational Astrophysics, National Astronomical Observatories, Beijing, 100012, China
– sequence: 2
  givenname: Suresh
  orcidid: 0000-0002-1638-2264
  surname: Kumar
  fullname: Kumar, Suresh
  email: suresh.kumar@pilani.bits-pilani.ac.in
  organization: Department of Mathematics, BITS Pilani, Pilani Campus, Rajasthan-333031, India
– sequence: 3
  givenname: Bharat
  surname: Ratra
  fullname: Ratra, Bharat
  email: ratra@phys.ksu.edu
  organization: Kansas State University Department of Physics, 116 Cardwell Hall, Manhattan, KS 66506, USA
BackLink https://www.osti.gov/servlets/purl/1532969$$D View this record in Osti.gov
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DocumentTitleAlternate DETERMINING THE HUBBLE CONSTANT FROM HUBBLE PARAMETER MEASUREMENTS
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Snippet We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts to determine the present-day Hubble constant H0 in four cosmological models. We...
We use 28 measurements of the Hubble parameter, H ( z ), at intermediate redshifts to determine the present-day Hubble constant H 0 in four cosmological...
We use 28 measurements of the Hubble parameter, H(z), at intermediate redshifts \(0.07\leqslant z\leqslant 2.3\) to determine the present-day Hubble constant...
We use 28 Hubble parameter, H($z$), measurements at intermediate redshifts 0.07 $\leqslant z \leqslant$ 2.3 to determine the present-day Hubble constant H0 in...
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StartPage 86
SubjectTerms Astronomical models
astronomy & astrophysics
ASTRONOMY AND ASTROPHYSICS
Astrophysics
Big Bang theory
Confidence limits
Cosmic microwave background
Cosmological models
cosmological parameters
Cosmology
dark energy
Hubble constant
Parameters
Statistical analysis
Title DETERMINING THE HUBBLE CONSTANT FROM HUBBLE PARAMETER MEASUREMENTS
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Volume 835
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