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Since the concept of an expanding universe was first introduced, there have been many estimates of the age of the universe that have evolved with scientific discoveries and developments. Many early estimates used the recessional velocities of distant galaxies to calculate the age of the universe, often getting results of about 2 Gyr (2 billion years) or less. Because this was less than calculations of Earth's age at the time, which were considered more accurate, doubt was cast upon the theory of expansion. This problem was resolved in 1952 when Walter Baade discovered that distances to neighboring galaxies, which were being used in the calculation of the age of the universe, were larger than previously thought; this brought the estimated age of the universe to about 4 Gyr.[1]
As time went on and observations improved, estimates for the age of the universe rose, with most estimates in the 1970s through 1990s in the range of 8–20 Gyr. Many of the higher estimates were due to the age of the oldest globular clusters, which had been estimated to be as high as 16 Gyr; these ages were later revised lower after new data revealed that they were further than previously thought.[2]
The launch of the Wilkinson Microwave Anisotropy Probe (WMAP) in 2001 and the Planck spacecraft in 2009, both measuring anisotropies in the cosmic microwave background, allowed astronomers to make more precise measurements of the age of the universe. The first year of WMAP data resulted in an estimated age of 13.7 ± 0.2 Gyr by two independent research groups.[3][4] As of 2026, the accepted age of the universe is 13.787 ± 0.020 Gyr, based on data from the Planck spacecraft analyzed in 2018.[5]
List
| Estimate | Year | Method | Authors | References |
|---|---|---|---|---|
| 10 Gyr | 1922 | Mathematical derivation of the Friedmann equations | Alexander Friedmann | [6][7] |
| 1.8 Gyr | 1929 | Recessional velocity, Cepheid variables | Edwin Hubble | [8][9][10] |
| >2×105 Gyr | 1930 | Gravitational collapse of nebulae | James Jeans | [11][12] |
| <2 Gyr | 1931 | Mathematical derivation from relativity | Arthur Eddington | [13][1] |
| 1–10 Gyr | 1935 | Recessional velocity | Edwin Hubble, Richard Tolman | [14][1] |
| 5–10×103 Gyr | 1936 | Orbits of binary stars | James Jeans | [15] |
| 0.75–1.5 Gyr | 1937 | Recessional velocity, positive cosmological constant | Edwin Hubble | [1][16] |
| 0.7 Gyr | 1938 | Recessional velocity | Paul Dirac | [17][1] |
| <1 Gyr | 1942 | Recessional velocity | Edwin Hubble | [10][1] |
| 3.64 Gyr | 1949 | Recessional velocity, nonhomogenous cosmology | Guy Omer | [18] |
| 3.5 Gyr | 1952 | Revised distance calculations, recessional velocity | Walter Baade | [1][19] |
| 4.1 Gyr | 1956 | Dirac large numbers hypothesis | C. Gilbert | [20] |
| 13.0 ± 4.3 Gyr | 1958 | Redshift–magnitude relation | Allan Sandage | [21][22] |
| 17.7 Gyr | 1972 | Cepheid variables | Allan Sandage | [23] |
| 8–18 Gyr | 1974 | Oldest globular clusters | Icko Iben Jr. | [24][25] |
| 13-20 Gyr | 1974 | Deuterium-limited density, oldest globular clusters, nucleochronology, galactic evolution | J. Richard Gott, James Gunn, David Schramm, Beatrice Tinsley | [24][26] |
| 6–20 Gyr | 1977 | Nucleochronology, galactic evolution | Kem Hainebach, David Schramm | [24][27] |
| 13.5–15.5 Gyr | 1978 | Oldest globular clusters, nuclear chronology | Demosthenes Kazanas, David Schramm, Kem Hainebach | [24] |
| 12+3 −2 Gyr |
1980–1981 | Nuclear chronology | William Alfred Fowler, David Schramm, Sidney van den Bergh | [28] |
| 10.3 ± 2.2 Gyr | 1987 | White dwarf luminosity distribution | Don Winget et. al | [29] |
| 13–18 Gyr | 1992 | Nucleochronology, oldest globular clusters | Sidney van den Bergh | [30] |
| >16 Gyr | 1992 | RR Lyrae stars, oldest globular clusters | Young-Wook Lee | [31] |
| >13 Gyr | 1994 | Cosmic microwave background anisotropies | Marc Kamionkowski, David Spergel, Naoshi Sugiyama | [32] |
| ≥12.07 Gyr | 1996 | Oldest globular clusters | Brian Chaboyer, Pierre Demarque, Peter Kernan, Lawrence Krauss | [33] |
| 9.7–15 Gyr | 1998 | Oldest globular clusters | Lawrence Krauss | [34] |
| ≥9.5 Gyr | 1998 | Oldest globular clusters | Brian Chaboyer | [35] |
| 13.4 ± 1.6 Gyr | 1999 | Literature review | Charles Lineweaver | [36] |
| <14 ± 2 Gyr | 2000 | Literature review | Wendy Freedman | [37] |
| 14.0 ± 0.5 Gyr | 2001 | Cosmic microwave background anisotropies | Lloyd Knox, Nelson Christensen, Constantinos Skordis | [38] |
| 13.2+1.2 −0.8 Gyr |
2001 | Cluster ellipticals, cosmic microwave background, type Ia supernovae | Ignacio Ferreras, Alessandro Melchiorri, Joseph Silk | [39] |
| 13.7 ± 0.2 Gyr | 2003 | Wilkinson Microwave Anisotropy Probe data | David Spergel et. al | [4] |
| 13.7 ± 0.2 Gyr | 2003 | Wilkinson Microwave Anisotropy Probe data | Charles Bennett et. al | [3] |
| 13.73+0.16 −0.15 Gyr |
2007 | Wilkinson Microwave Anisotropy Probe data | David Spergel et. al | [40] |
| 13.1+0.96 −0.87 Gyr |
2008 | Data from Wilkinson Microwave Anisotropy Probe, Sloan Digital Sky Survey, Hubble Space Telescope | Francesco De Bernardis, Alessandro Melchiorri, Licia Verde, Raul Jimenez | [41] |
| 13.31+1.0 −0.91 Gyr |
2008 | Data from Wilkinson Microwave Asinotropy Probe, Sloan Digital Sky Survey, Hubble Space Telescope, high-resolution CMB experiments, two degree field galaxy redshift survey, type 1a supernovae | Francesco De Bernardis, Alessandro Melchori, Licia Verde, Raul Jimenez | [41] |
| 13.772 ± 0.059 Gyr | 2013 | Wilkinson Microwave Anisotropy Probe data | Charles Bennett et. al | [42] |
| 13.817 ± 0.048 Gyr | 2014 | Planck data, WMAP polarization low-multipole likelihood | Planck collaboration | [43] |
| 13.798 ± 0.037 Gyr | 2014 | Planck data, WMAP polarization low-multipole likelihood, high-resolution CMB experiments, baryon acoustic oscillation | Planck collaboration | [43] |
| 13.813 ± 0.038 Gyr | 2016 | Planck data | Planck collaboration | [44] |
| 13.787 ± 0.020 Gyr | 2020 | Planck data | Planck collaboration | [5] |
See also
References
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