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Course: PHY 306, Fall 2009
School: East Los Angeles College
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1990s 1920s (from Friedmann to Freedman) theoretical technology available, but no data 20th century: birth of observational cosmology Hubble's law ~1930 Development of astrophysics 1940s 1950s Discovery of the CMB 1965 Inflation 1981 CMB anisotropies: COBE ~1990 1920s 1990s (from Friedmann to Freedman) theoretical technology available, but no data 20th century: birth of observational cosmology Hubble's law...

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1990s 1920s (from Friedmann to Freedman) theoretical technology available, but no data 20th century: birth of observational cosmology Hubble's law ~1930 Development of astrophysics 1940s 1950s Discovery of the CMB 1965 Inflation 1981 CMB anisotropies: COBE ~1990 1920s 1990s (from Friedmann to Freedman) theoretical technology available, but no data 20th century: birth of observational cosmology Hubble's law ~1930 from antiquity Universe had been assumed to be static relativity naturally expects universe to expand or contract, but very few people took this literally Alexander Friedmann Georges Lematre not Einstein! expansion eventually discovered by observation At z << 1 all cosmological models expect a linear behaviour, z d first evidence: Edwin Hubble 1929 "the possibility that the velocity-distance relation may represent the de Sitter effect" slope of graph 46550 km/s/Mpc or 51360 km/s/Mpc (individual vs grouped) assumption of linearity no centre to expansion established by 1931 (Hubble & Humason) 1 Timeline 1907: Bertram Boltwood dates rocks to 0.4 2.2 Gyr (U-Pb) 1915: Vesto Slipher demonstrates that most galaxies are redshifted 1925: Hubble identifies Cepheids in M31 and M33 1927: Arthur Holmes "age of Earth's crust is 1.6 3.0 Gyr" 1929: Hubble's constant value of 500 km/s/Mpc implies age of Universe ~2.0 Gyr Hubble's law systematics distances mostly depend on m M = 5 log(d/10) (luminosity distance) getting M wrong changes d by a factor of which does not affect linearity (just changes slope) typical systematic error: very difficult to spot Jan Oort expressed doubts very quickly (1931) no-one else till 1951! 10 ( M - M est ) 5 potential problem here... Hubble used Cepheid variables as calibrated by Shapley (1930) brightest stars in galaxies as calibrated by Cepheids total luminosities of galaxies calibrated by Cepheids and brightest stars Wrong by factor of 2! Wrong by factor of ~4! Wrong because calibration wrong Shapley (1930): calibration of extragalactic Cepheids based on assumption of consistency with RR Lyrae variables in globular clusters Baade (1952): Cepheids in Magellanic Clouds ( Cephei stars or classical Cepheids) are different from "Cepheids" in globular clusters (W Vir stars or Type II Cepheids) Typical classical Cepheid and W Vir light curves from the HIPPARCOS database 2 Period-luminosity relation RR Lyrae stars period < 1 day M ~ 0.7 (on horizontal branch) little evidence of dependence on period (does depend on metallicity) period > 10 days post-horizontal-branch low mass stars MB = -4.35 log P + 3.98 MB = -1.33 log P + 0.24 W Vir stars DH McNamara, AJ 109 (1995) 2134 Ngeow & Kanbur, MNRAS 349 (2004) 1130 MB = -2.59 log P - 0.67 classical Cepheids period > 1 day post-main-sequence stars of a few solar masses Distance error from +0.7 to -0.7: ~ factor 2 Idea: brightest in stars all galaxies are about the same absolute magnitude not unreasonable: tip of red giant branch is still used as distance indicator might worry about age and metallicity effects but first be sure you are looking at a star! Hubble wasn't: he was seeing H II regions (ionised gas around young massive stars) these are much brighter than individual stars difference ~2 mag M74/NOAO ! M100 spiral arm " " blue plate; star marked red plate; H II regions marked Allan Sandage, ApJ 127 (1958) 123 3 # 1200 1000 Compilation by John Huchra H 0 (km/s/Mpc) 800 600 400 200 Jan Oort Baade identifies Pop. I and II Cepheids "Brightest stars" identified as H II regions 0 1920 1930 1940 1950 1960 1970 1980 1990 2000 Date $ Distance indicators Stars, clusters, etc. classical Cepheids novae globular clusters planetary nebulae supernovae Ia and II Sources of uncertainty calibration zero point dependence on age, metallicity, galaxy type, etc. reddening corrections bias Malmquist bias at large distances, you tend to detect brighter than average objects Galaxies Tully-Fisher Fundamental plane Bigger things Sunyaev-Zeldovich effect gravitational lensing personal biases too! Allan Sandage: low Gerard de Vaucouleurs: high $ 140 120 general cosmology dependent Key project Sandage camp de Vaucouleurs cam p H 0 (km/s/Mpc) 100 80 60 40 20 0 1970 1980 Date 1990 2000 reasonable convergence only in last decade see later 4 % Does Hubble's law mean universe is expanding (i.e. a(t) in RW metric not constant)? Alternative hypotheses real explosion at some past time over time t galaxies travel distance d=vt, so build up Hubble law don't expect to be at centre of expansion, so don't expect isotropy "...

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