Skip to main content

The Theory of Cosmic Inflation

  • Chapter
  • First Online:
Cosmology for the Curious
  • 253k Accesses

Abstract

The horizon and flatness problems had been recognized since the 1960s, but were rarely discussed—simply because no one had any idea as to what to do about them.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 29.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 39.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 39.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    We show in the Appendix that the doubling time in an inflating spacetime is \(t_{D} = \frac{0.7}{H}\).

  2. 2.

    Despite the similarity between the tunneling of a ball and that of a scalar field, there is also an important difference. The ball tunnels between two different points in space, while the field tunnels between two different field values at the same location in space.

  3. 3.

    A ball rolling on a similarly curved surface would also oscillate about the lowest point, would gradually slow down due to friction, and would come to rest, with all its mechanical energy turned into heat. Similarly, analysis shows that an oscillating field loses its energy by particle production, creating a fireball.

  4. 4.

    Quantum fluctuations occur on smaller scales as well, but upward and downward kicks alternate in rapid succession, so their overall effect is nil. But once the fluctuation region is stretched to a size larger than \(d_{H}\), its different parts become causally disconnected, and coherent fluctuations in such a region are no longer possible. The surviving fluctuations are the ones produced in regions of size \(\sim d_{H}\). The region is then immediately stretched to a larger size, and the fluctuation “freezes”.

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing AG

About this chapter

Cite this chapter

Perlov, D., Vilenkin, A. (2017). The Theory of Cosmic Inflation. In: Cosmology for the Curious. Springer, Cham. https://doi.org/10.1007/978-3-319-57040-2_16

Download citation

Publish with us

Policies and ethics