1771 |
Messier |
Before 20th century |
Cataloged about 100 non-stellar objects |
1864 |
Herschel |
Before 20th century |
General Catalogue of Galaxies: 5079 objects |
1888 |
Dreyer |
Before 20th century |
New General Catalogue of Nebulae and Clusters of Stars: about 15000 objects |
1902 |
Jeans |
Structure Formation |
Structures can form via gravitational instability |
1916 |
Einstein |
Cosmology |
General Relativity |
1920 |
Shapley Curtis |
Cosmology |
Great debate on whether the Nebula are separate islands or not |
1922 |
Friedmann |
Cosmology |
Solved Einstein's equations for a homogeneous universe |
1925 |
Hubble |
Cosmology |
Galaxies are very far objects; Galaxies are separate islands |
1929 |
Hubble |
Cosmology |
Speed of more distant galaxies is more |
1933 |
Zwicky |
ΛCDM |
Velocity in clusters needed 400times more mass than visible |
1936 |
Hubble |
Galaxy Formation |
Classification of galaxies in the Hubble Sequence |
1937 |
Zwicky |
ΛCDM |
Large invisible cluster mass should produce lensing |
1939 |
Gamow Teller |
Structure Formation |
Application of Jeans criterion to an expanding universe; with the result that perturbation growth is power-law in time, rather than exponential as for a static back ground |
1948 |
Gamow Alpher |
Cosmology |
Initial model for Primordial Nucleosynthesis |
1949 |
Hoyle |
Structure Formation |
Purturbations might gain angluar momentum from their neighbors |
1957 |
Hoyle Fowler |
Cosmology |
Heavy elements can only be made in stars |
1959 |
Schmidt |
Galaxy Formation |
Star formation efficiency appears to scale as the squared of density |
1962 |
Eggen
| Galaxy Formation |
Galaxies form from the collapse of gas clouds; Difference in elliptical and spiral reflects the rapidity of star formation |
1964 |
Hoyle Taylor |
Cosmology |
Explanation of Helium abundance from Big Bang |
1965 |
Penzias Wilson |
Cosmology |
Discovery of the Cosmic Microwave Background |
1965 |
Peebles |
Structure Formation |
Isothermal initial conditions: Structure forms Bottom-up |
1966 |
Gershtein Zel'dovich |
ΛCDM |
Exotic elementary particles like massive neutrinos (HDM) constitute the dark matter |
1967 |
Wagoner |
Cosmology |
Detailed calculation of a complete network of nuclear reactions; Helium 3, Deuterium and Lithium |
1968 |
Misner |
Cosmology |
Problem of horizons: different parts of the universe we see today were never in casual contact |
1968 |
Silk |
Structure Formation |
Adiabatic initial conditions: Structure forms Top-down |
1970 |
Harrison |
Structure Formation |
Harrison-Zel'dovich initial function spectrum: Structure on every scale has the same dimensionless amplitude |
1970 |
Doroshkehvich |
Structure Formation |
A linear perturbation analysis of the hoyle process carried out in full generality |
1970 |
Zel'dovich |
Structure Formation |
He describes the initial non-linear collapse of a coherent purturbation of the cosmic density field; 2D pancake |
1971 |
Peebles |
Structure Formation |
Numerical simulations of the hoyle-doroshkevech processes |
1972 |
Gunn Gott |
Structure Formation |
Simple spherically symmetric model to describle the growth, turn around (from the general expansion), collapse and virialization of a purturbation |
1972 |
Toomre Toomre |
Galaxy Formation |
Using simple numerical simulations they demonstrated convincingly that some of the extraordinary structures seen in peculiar galaxies could be produced by tidal interactionds between two normal spirals. Based on their frequency and interaction signitures, they argued that elliptical galaxies could be merger remnants |
1973 |
Roberts Rots |
ΛCDM |
Using 21cm and optical observations, they showed that the velocity towards the outer galaxy radius does not fall off |
1974 |
Press Schechter |
Structure Formation |
Applied the Gun & Gutt perturbation growth to a gaussian initial density field |
1974 |
Ostriker Einasto |
ΛCDM |
A halo is needed to understand the motion of satellites around the milky way |
1975 |
Bertola Capaccioli |
Galaxy Formation |
Showed the absence of highly flattened ellipticals in the Larson model |
1976 |
Gutt Thuan |
Galaxy Formation |
Protogalaxies associated with the highest initial density perturbations would complete star formation earlier and become ellipticals |
1976 |
Larson |
Galaxy Formation |
That it is indeed the ratio of the star-formation time to the dissipation/cooling time which determines whether the system turns into an elliptical or a spiral. Also emphasised the importance of feedback processes |
1977 |
Silk |
Galaxy Formation |
Galaxies can form effectively only in systems where the cooling time is comparable to or shorter than the collapse time, which leads to a characteristic scale of ~10^(12) Solar masses. |
1977 |
Illingworth |
Galaxy Formation |
Many bright ellipticals show little or no rotation in contrast to the Larson model |
1978 |
White Rees |
ΛCDM |
Two stage theory for galaxy formation: Dark halos form first through hierarchical clustering; the luminous content of galaxies then results from cooling and condensation of gas within thre Press & Schechter model for the growth of non-linear structure. They used Larson's model for feedback processes |
1978 |
White Rees |
Galaxy Formation |
Showed the absence of highly flattened ellipticals in the Larson model |
1978 |
White |
Galaxy Formation |
Simulations showed that mergers of two spheroids produces remnants with density profiles that agree with observed ellipticals |
1979 |
Dicke Peebles |
Cosmology |
Problem of flatness: Why the universe as stayed so flat |
1979 |
Efstathiou Jones |
Structure Formation |
Clumps formed through gravitational collapse in a cosmological context typically acquire about 15% of the angluar momentum needed for full rotational support |
1979 |
Tremain Gunn |
ΛCDM |
Based on the Pauli exclusion principle they showed that galaxy halos cannot be made of neutrinos with masses as small as 30eV |
1980 |
Lyubimov Reines |
ΛCDM |
Announced the detection of mass for the electron neutrino at a level of cosmological interest (about 30eV); Not conclusive |
1980 |
Bond Sato |
ΛCDM |
detailed study of structure formation with massive neutrinos as dark matter |
1980 |
Fall & Efstathiou |
Galaxy Formation |
Developed a model of disk formation in dark matter halos incorporating the angular momentum expected from tidal torques and showed that many properties of observed galaxies can be understood in this way. |
1980 |
Ostriker |
Galaxy Formation |
Observed giant ellipticals which are dense and can have velocity dispersions as high as 300km/s cannot be formed through mergers |
1981 |
Guth |
Cosmology |
Introduced inflation: Early period of exponential expansion, to solve the flatness and curvature problems |
1981 |
Gerhard |
Galaxy Formation |
Simulations on mergers of disk galaxies that create ellipticals |
1982 |
Linde Steinhardt |
Cosmology |
Revised inflation |
1982 |
Howking |
Structure Formation |
Quantum fluctuations in the inflation scalar field could be the source of the Harrison - Zel'dovich spectrum: in the simplest form perturbations are adiabatic and the initial density field is Gaussian. |
1982 |
Peebles |
ΛCDM |
Consideration of a variety of Warm and Cold Dark Matter models |
1983 |
Kaiser |
ΛCDM |
Galaxies form at the deepest dark matter potential wells |
1983 |
Efstathiou & Silk |
Galaxy Formation |
In the two stage theory, they argued that cool gas can settle in a rotationally supported disk in a fraction of the hubble time, whereas with out the dark matter halo it would take too long. |
1984 |
White |
ΛCDM |
Simulations of structure formation in a neutrino dominted universe showed that they cannot make galaxies with out making highly dense clusters at the same time. |
1984 |
Blumenthal |
Galaxy Formation |
Biased galaxy formation: suggesting that disk galaxies may be associated with density peaks of typical heights in the CDM density field, while giant ellipticals may be associated with higher density peaks. |
1985 |
Davis |
ΛCDM |
Simulations of the CDM model and how the can create a good match to the observed clustering of galaxies |
1990 |
Maddox Efstathiou |
ΛCDM |
APM galaxy survey, showed that the standard CDM model predicts less clustering on large scales |
1991 |
Katz Gunn |
Galaxy Formation |
Three-dimensional, hydrodynamical simulations of galaxy formation: They focused on the collapse of a homogeneous, uniformly rotating sphere. |
1991 |
White Frenk |
Galaxy Formation |
Semi-analytical models of galaxy formation: uses knowledge about the structure and assembly history of CDM halos to model the gravitational potential wells within which galaxies form and evolve , treating all the relevant physical processes (cooling, star formation, feedback, dynamical friction , etc.) |
1992 |
Smooth |
Structure Formation |
Anisotropy in the CMB was detected with COBE |
1992 |
Davis |
ΛCDM |
MDM: Mixed Dark Matter: 30%HDM, 70%CDM; Ultimately too slow galaxy formation |
1992 |
Warren |
Galaxy Formation |
CDM halo angular-momentum distributions |
1993 |
Lacey Cole |
Galaxy Formation |
Merger Histories in the CDM halos |
1994 |
Ratra |
ΛCDM |
OCDM: Open CDM: CDM only 30% of critical density; Ultimately problems showed in matching perturbation amplitudes with COBE |
1994 |
Dodelson |
ΛCDM |
τCDM: Enhanced Radiation background was proposed for more clustering, but ultimately too slow galaxy formation |
1996 |
Mo White |
Galaxy Formation |
Spatial Clustering in CDM halos |
1997 |
Navarro |
Galaxy Formation |
CDM halos density profiles |
1998 |
Granavich |
ΛCDM |
Measurement of cosmic acceleration in expansion with Type Ia supernovae |
1998 |
Moore |
Galaxy Formation |
Substructure in the CDM halos |
1999 |
Perlmutter |
ΛCDM |
Measurement of cosmic constants Ω and Λ, using Type Ia supernovae |
2000 |
Brinchmann & Ellis |
Observational |
New method of photometric redshift through fitting a modeled Spectral Enegery Distribution with discrete photmetric observations in different wavelengths. |
2000 |
de Bernardis |
ΛCDM |
The Universe is flat |
2002 |
Jing Sato |
Galaxy Formation |
CDM Halo Shapes |
2003 |
Bennett |
Galaxy Formation |
COBE results confirmed and dramatically refined by WMAP |
2003 |
Bruzual & Charlot |
Observational |
New software for stellar population synthesis of galaxies that enabled the easy fitting of observed galaxy spectra with those of a hypothetical galaxy. |
2003 |
Spregel |
ΛCDM |
Determination of cosmological parameters using WMAP |