Part IV. Cosmology Chapter 13
General relativity and cosmology
Martin Bucherā ,ā” and Wei-Tou NiĀ§
ā Laboratoire APC, UniversitĆ© Paris 7/CNRS,
BĆ¢timent Condorcet, Case 7020,
75205 Paris Cedex 13, France
[email protected] ā”Astrophysics and Cosmology Research Unit and
School of Mathematics, Statistics and Computer Science,
University of KwaZulu-Natal, Durban 4041, South Africa
Ā§Center for Gravitation and Cosmology,
Department of Physics, National Tsing Hua University,
Hsinchu, Taiwan 30013, Republic of China
[email protected] This year marks the 100th anniversary of Einsteinās 1915 landmark paper āDie Feldgleichungen der Gravitationā in which the field equations of general relativity were correctly formulated for the first time, thus rendering general relativity a complete theory. Over the subsequent hundred years, physicists and astronomers have struggled with uncovering the consequences and applications of these equations. This paper, which was written as an introduction to six chapters dealing with the connection between general relativity and cosmology that will appear in the two-volume book One Hundred Years of General Relativity: From Genesis and Empirical Foundations to Gravitational Waves, Cosmology and Quantum Gravity, endeavors to provide a historical overview of the connection between general relativity and cosmology, two areas whose development has been closely intertwined.
Keywords: General relativity; cosmology; centennial connection.
PACS Number(s): 04, 98.80.āk
One hundred years ago, the best model of the universe summarizing the state of the observations at that time was the Kapteyn universe, which consists of a system of stars distributed more or less uniformly within a disk about 10 kpc in diameter and 2 kpc thick. In this model, the Sun is situated near the center of the disk. In 1917, Einstein1 proposed a static cosmological model based on the ācosmological principle,ā a generalization of the Copernican principle postulating that the homogeneity and isotropy of space in the large should be extended to include the time dimension as well. Using distance determinations to about 100 globular clusters, Shapley in 1918 pushed back the boundaries of the measured universe and concluded that the Sun lies near the edge of this distribution. As a result of rapid improvements in astronomical observations, the size of our observed universe soon grew to extend almost to our causal horizon.
This next group of chapters comprising Part IV of GR100 book deals with Cosmology, applying Einsteinās theory of general relativity to the universe as a whole. Cosmology considers the universe on very large scales and evolving over very long times, comparable to the age of the universe. Cosmology today is often described as being a āprecisionā science and the insistence on this term reflects that cosmology had not always been seen as such. When Einstein formulated his general theory of relativity, little was known about the universe beyond our own galaxy, and although distant galaxies had been observed as ānebulousā unresolved spiral blotches, it was not at all clear that these ānebulaeā consisted of numerous stars much like our own galaxy.
A glimpse of the state of affairs slightly after the formulation of general relativity may be gained by reading the written summaries2 of the āGreat Debateā held at the Smithsonian institution in 1920, where Harlow Shapley and Heber Curtis sparred over the question of the āscale of the universe.ā The former argued that the ānebulaeā were simply clouds lying on the periphery of our own galaxy, whereas the latter maintained that the observations at the time suggested that the ānebulaeā were distant āisland universesā much like our own galaxy. A key observation that helped settle this question in favor of the latter point of view was the discovery by Edwin Hubble of Cepheid variable stars in the Andromeda galaxy, which established that Andromeda lies far beyond the confines of our own galaxy.
On the observational side, as telescopes and other observational techniques greatly improved, our view of the universe progressively expanded to greater and greater distances. Once it had been established that the universe was populated by galaxies of different sizes, a recurrent question became whether the universe was homogeneous and isotropic on the largest observable scales, and it is only recently that galaxy surveys sufficiently deep and with sufficient statistics became available to settle this question definitively. An excellent historical account of these early debates and their role of the development of modern cosmology can be found in Peeblesā 1980 book3 (see also Ref. 4).
The theory underlying the hot big bang model as we know it today was developed before the observational issues mentioned above had been settled. The geometry and time evolution of the universe as predicted by Einsteinās theory are given by what is now known as the FriedmannāLemaĆ®treāRobertsonāWalker (FLRW) model, which describes the solutions to Einsteinās field equations for a spatially homogeneous and isotropic universe whose scale factor varies with time. This solution to the Einstein field equations was first put forward by Alexander Friedmann in 19225,6 and later independently by Georges LamaĆ®tre7 (see also Ref. 8). Robertson9 and Walker10 subsequently showed that this was the only solution to the field equations consistent with spatial homogeneity and isotropy. As discussed above, in 1917 Einstein1 had put forth a theory of a static universe ā a solution of the general relativity field equations that is not only homogeneous and isotropic in the three spatial dimensions but also homogeneo...