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6 - Cosmology from the top down

Published online by Cambridge University Press:  05 July 2014

Stephen Hawking
Affiliation:
Cambridge University
Bernard Carr
Affiliation:
Queen Mary University of London
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Summary

Problems with bottom-up approach

The usual approach in physics could be described as building from the bottom up. That is, one assumes some initial state for a system and then evolves it forward in time with the Hamiltonian and the Schrödinger equation. This approach is appropriate for laboratory experiments like particle scattering, where one can prepare the initial state and measure the final state. The bottom-up approach is more problematic in cosmology, however, because we do not know what the initial state of the Universe was, and we certainly cannot try out different initial states and see what kinds of universe they produce.

Different physicists react to this difficulty in different ways. Some — generally those brought up in the particle physics tradition — just ignore the problem. They feel the task of physics is to predict what happens in the laboratory, and they are convinced that string theory or M-theory can do this. All they think remains to be done is to identify a solution of M-theory, a Calabi—Yau or G2 manifold that will give the Standard Model as an effective theory in four dimensions. But they have no idea why the Universe should be 4-dimensional and have the Standard Model, with the values of the forty or so parameters that we observe. How can anyone believe that something so messy is the unique prediction of string theory?

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Publisher: Cambridge University Press
Print publication year: 2007

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References

[1] A. H., Guth. Phys. Rev. D 23 (1981), 347.
[2] A., Vilenkin. Phys. Lett. D 27 (1983), 2848.
[3] A. D., Linde. Phys. Lett. B 175 (1986), 395.
[4] J., Khoury, B. A., Ovrut, P. J., Steinhardt and N., Turok. Phys. Rev. D 61 (2001), 123522.
[5] P. J., Steinhardt and N., Turok. Phys. Rev. D 65 (2002), 126003.
[6] M., Gasperini, M., Maggiore and G., Veneziano. Nucl. Phys. B 494 (1997), 315.
[7] S. W., Hawking and R., Penrose. Proc. Roy. Soc. Lond. A 314 (1970), 529.
[8] J., Hartle and S. W., Hawking. Phys. Rev. D 28 (1983), 2960.
[9] D. N., Spergel, L., Verde, H. V., Peiriset al.Astrophys. J. Suppl. 148 (2003), 175.
[10] S. W., Hawking, T., Hertog and H. S., Reall. Phys. Rev. D 63 (2001), 083504.
[11] S. W., Hawking and N., Turok. Phys. Lett. B 425 (1998), 25.
[12] L., Susskind. This volume (2007) [hep-th/0302219].

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