The Spacetime Metric

Historical research guide · 0631 · 2001

The Cosmological Constant

Sean M. Carroll

In one minute

Sean Carroll wrote this Living Review in 2001, at the moment the cosmological constant came back. He lays out what the constant is: a measure of the energy density of empty space, which general relativity treats as a perfect fluid whose pressure is the negative of its energy density, and which therefore pushes the universe apart instead of pulling it together. Then he does the arithmetic that has bothered physicists ever since. Add up what quantum field theory says should be sitting in the vacuum — the electroweak and QCD phase transitions, a grand-unification scale, zero-point fluctuations cut off at the Planck scale — and you get a number roughly 120 orders of magnitude larger than what the sky shows. On the observational side he walks through the two supernova teams, the microwave background, cluster masses and lensing, and finds them converging on a flat universe that is about seventy per cent vacuum energy and thirty per cent matter. His own verdict on that universe is the title of his last section: preposterous, and the best fit we have.

Connection

Chapter 2 turns on the identification Carroll spells out here — the cosmological constant and the energy of the vacuum are the same quantity — and this is the standard reference for it. Chapter 13 needs the honest ledger, and the gap between the vacuum energy the laboratory implies and the vacuum energy the sky measures is the largest open number in the whole picture.

From the source

  1. The cosmological constant is a measure of the energy density of the vacuum. Because the only Lorentz-invariant form the vacuum energy-momentum tensor can take is one proportional to the metric, the vacuum behaves as a perfect fluid whose pressure is minus its energy density, and adding such a fluid to the Einstein equations is exactly equivalent to adding a cosmological constant. Carroll uses ’vacuum energy’ and ’cosmological constant’ interchangeably from that point on, and notes that the vacuum fluctuations themselves are very real, as evidenced by the Casimir effect.Section 1.3, Vacuum energy

  2. The net vacuum energy is a sum of contributions that can each be estimated, and every estimate is enormous. The electroweak phase transition suggests a contribution set by a scale of about 200 giga-electronvolts, the breaking of chiral symmetry in the strong interactions a scale of about 0.3 giga-electronvolts, grand unification a scale near ten to the sixteenth giga-electronvolts, and zero-point fluctuations trusted up to the Planck scale a scale near ten to the eighteenth. Cosmological observation implies something far smaller, and the ratio is the famous discrepancy of 120 orders of magnitude. Carroll states plainly that no known symmetry enforces a vanishing vacuum energy, and calls this one of the most significant unsolved problems in fundamental physics.Section 1.3, Vacuum energy, closing paragraphs

  3. Two independent supernova searches reached the same answer. The High-Z Supernova Team and the Supernova Cosmology Project both favour a positive cosmological constant and strongly rule out the traditional flat matter-dominated universe. The method works because the peak brightness of a Type Ia supernova is tightly correlated with the shape of its light curve — dimmer events decline faster — which cuts the scatter in peak brightness from about 40 per cent to less than 15 per cent, enough to separate cosmological models.Section 3.1, Type Ia supernovae

  4. The concordance is a flat universe of roughly thirty per cent matter and seventy per cent vacuum energy. Big-bang nucleosynthesis fixes the baryon share at about four per cent, so most of the matter is in some unknown non-baryonic form, and the largest single component of the universe is the energy of empty space.Section 5, Conclusions: The Preposterous Universe, first paragraph

  5. The coincidence is the part Carroll finds hardest to swallow. Plot the vacuum fraction against the scale factor and it is negligible early and total late; we happen to observe from the brief cosmological era in which matter and vacuum are of comparable magnitude. He sets the challenge for the years after: work out whether these apparently distasteful features are surprising coincidences or a clue to a deeper structure not yet understood.Section 5, Conclusions: The Preposterous Universe, second and third paragraphs

  6. Dark energy need not be a constant. Any component that resists clustering on small scales and redshifts away only slowly will fit the data, and such a component is parameterised by an equation-of-state number running from zero for ordinary matter to minus one for a true cosmological constant. Supernovae, large-scale structure, lensing and the microwave background already favour a value near minus one, without closing off the others. The simplest dynamical alternative is quintessence, a single slowly rolling scalar field, and Carroll is careful that it brings its own naturalness problems: the field must be light enough to be rolling today, which by particle-physics standards is an incredibly small mass, and its couplings to ordinary matter must be suppressed by several orders of magnitude beyond what one would expect.Section 4.6, Other sources of dark energy

The way in

https://arxiv.org/abs/astro-ph/0004075

How to cite it

Sean M. Carroll (2001) The Cosmological Constant doi:10.12942/lrr-2001-1

Where it sits in the curriculum

Provenance: Retrieved 2026-09-08

Summary by: The Spacetime Metric editorial rail (AI draft from the source text, 2026-09-07)

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