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2004/10/13 | 宇宙常数[Cosmological Constant]
类别(Ω〖物理〗)
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发表于 13:21
A constant
introduced by
Einstein
(1917) into the equations of
general relativity
to allow a steady state cosmological solution to the
Einstein field equations
. The constant was introduced before the concept of the
Big Bang
had been conceived, so an expanding or contracting
universe
was regarded as physically implausible, leading Einstein to add
as a "fudge factor." In theory, the constant can be derived from quantum field theory, but the derivation has not yet been performed. Einstein's cosmological constant is equivalent to a vacuum energy density, which means it can be put on the left hand side of Einstein's equations with the geometry (as Einstein did), or on the right hand side with the stress-energy, both forms being mathematically equivalent.
Generally,
does not play a significant role in the early
universe
.
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