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THE UNIVERSE WILL EXPAND FOREVER

WHT+ISIS, INT+PFC

New studies of supernovae in the farthest reaches of deep space indicate that the universe will expand forever because there isn't enough mass in the universe for its gravity to slow the expansion, which started with the Big Bang.

This result rests on analysis of 42 of the roughly 78 type Ia supernovae so far discovered by the Supernova Cosmology Project(1). By the time the light of the most distant supernova explosions so far discovered by the team reached telescopes on Earth, some seven billion years had passed since the stars exploded. After such a journey the starlight is feeble, and its wavelength has been stretched by the expansion of the universe, i.e. red-shifting its wavelength. By comparing the faint light of distant supernovae to that of bright nearby supernovae, one could tell how far the light had travelled. Distances combined with redshifts of the supernovae give the rate of expansion of the universe over its history, allowing a determination of how much the expansion rate is slowing. Although not all type Ia supernova have the same brightness, their intrinsic brightness can be determined by examining how quickly each supernova fades.

Since the most distant supernova explosions appear so faint from Earth, last for such a short time, and occur at unpredictable intervals, the Supernova Cosmology Project team had to develop a tightly choreographed sequence of observations to be performed at telescopes around the world, among them, the Isaac Newton and the William Herschel telescopes. While some team members are surveying distant galaxies using the largest telescopes in Chile and La Palma, others in Berkeley are retrieving that data over the Internet and analysing it to find supernovae. Once they detect a potential supernova they rush out to Hawaii to confirm its supernova status and measure the redshifts using the Keck telescope. Meanwhile, team members at telescopes outside Tucson and on La Palma are standing by to measure the supernovae as they fade away. The Hubble Space Telescope is called into action to study the most distant of the supernovae, since they are too hard to accurately measure from the ground.

Reaching out to these most distant supernovae teaches us about the cosmological constant. If the newly discovered supernovae confirm the story told by the previous 42, astrophysicists may have to invoke Einstein's cosmological constant to explain the observed accelerated expansion of the universe. This cosmological constant has nowadays an interpretation in terms of vacuum energy density which works against gravity to produce the observed accelerated rate of expansion.

(1)The Supernova Cosmology Project is a collaboration between the following institutions: Lawrence Berkeley National Laboratory (USA), Institute of Astrophysics, Cambridge and Royal Observatory of Edinburgh (UK), LPNHE, Paris and College de France, Paris (France), University of Barcelona (Spain), and Isaac Newton Group, La Palma (UK and The Netherlands), Stockholm University (Sweden), ESO (Chile), Yale University (USA) and STscI (USA).

References:
 

  • S Perlmutter et al, 1997, "Measurements of the Cosmological Parameters Omega and Lambda from the First Seven Supernovae at z >= 0.35", Astrophys J, 483, 565.
  • S Perlmutter et al, 1998, "Discovery of a supernova explosion at half the age of the universe", Nature, 391, 51.
  • S Perlmutter et al, 1999, "Measurements of Omega and Lambda from 42 High-Redshift Supernovae", Astrophys J, 517, 565.

 
Observing strategy[ JPEG | TIFF ]
INT image of a high z supernova [ JPEG | TIFF ]

Lambda non-equal to zero [ JPEG | TIFF ]

Ages of the Universe [ JPEG | TIFF ]
 
 

 

Top: The observing strategy allows the team to find sets of high-redshift supernovae on the rising part of their light curves and guarantees the date of discovery, thus allowing follow-up photometry and spectroscopy of the transient supernovae to be scheduled. The supernova light curves are then followed with scheduled R-, I- and some B-band photometry at the INT and other telescopes. 

Top left: INT image of a high-redshift type Ia supernova thousands of millions of light years away. When a star explodes as a type Ia supernova its brightness is similar to the host galaxy. This latter feature along with the possibility of calibrating their maximum brightness, make type Ia supernovae the best known standard candles to investigate the geometry and the dynamics of our universe. 

Middle left: Best-fit confidence regions in the OmegaMass – OmegaLambda  plane. The 68%, 90%, 95%, and 99% statistical confidence regions are shown. Note that the spatial curvature of the universe — open, flat, or closed — is not determinative of the future of the universe's expansion, indicated by the near-horizontal solid line. In cosmologies above this near-horizontal line the universe will expand forever, while below this line the expansion of the universe will eventually come to a halt and recollapse. The upper-left shaded region, labelled 'no big bang', represents 'bouncing universe' cosmologies with no big bang in the past. The lower right shaded region corresponds to a universe that is younger than the oldest heavy elements for any value of H0>=50 kms-1Mpc-1

Bottom left: Isochrones of constant H0t0, the age of the universe relative to the Hubble time, H0-1, with the best-fit 68% and 90% confidence regions in the OmegaMass – OmegaLambda  plane. The isochrones are labelled for the case of H0=63 kms-1Mpc-1. If H0 were taken to be 10% larger, the age labels would be 10% smaller. The diagonal line labelled accelerating/decelerating is drawn for q0=OmegaMass/2 – OmegaLambda =0 and divides the cosmological models with an accelerating or decelerating expansion at present time. A value of OmegaLambda non-equal to zero is favored from the data of all the observed supernovae.

Bottom: Hubble diagram (effective B-magnitude at maximum versus redshift) containing 42 high-redshift supernovae (red dots) that could be width-luminosity corrected, and 18 from the lower-redshift Calán/Tololo Supernova Survey. Magnitudes have been K-corrected, and also corrected for the width-luminosity relation. The inner error bar corresponds to the photometry error alone, while the outer error bar includes the intrinsic dispersion of type Ia supernovae after stretch correction. The solid curves indicate theoretical model predictions based on different cosmological parameters. 

Hubble diagram [ JPEG | TIFF ]


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