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A quantum singularity is a term used in Star Trek to
refer to a point or region in the space-time continuum where normal
physical models do not apply and extraordinary amounts of gravitational
forces are typically present. Singularities can be both natural and
artificial: wormholes, quantum matrices of planets, and black holes all
can contain singularities, as do certain reactors (e.g. those found in
Romulan starships).
There are relationships between singularities and time.
Singularities in general, and quantum singularities in particular, are
known by 24th century science even when stable to send out waves of
temporal displacement that affects, among other things, delta-series
radioisotopes. The USS Enterprise encountered temporal effects from a
singularity in a black star in 2267. (TOS: "Tomorrow is Yesterday")
Also, energy emitted by an exploding microscopic singularity can shift
chroniton particles into a high state of temporal polarization and/or
create "bubbles" in subspace. This latter result can cause temporal
anomalies and was directly observed by the USS Defiant in 2371. (DS9:
"Past Tense, Part I"). In 2371, the USS Voyager, while traveling in the
Delta Quadrant, became trapped in a type-4 singularity. (VOY:
"Parallax").
Singularities can be detected by the effect they have on
local gravimetric field signatures nearby (although they can be buried
so far down in subspace layers that they cannot be detected in that
way), and/or by using tetryon emissions as a guide.One example of the
use of a singularity was demonstrated in 2373. The Borg, Species 8472,
and the USS Voyager were all able to travel between the fluidic space
dimension and our dimension via artificially created quantum
singularities. (VOY: "Scorpion", "Scorpion, Part II").
The term quantum singularity used in Star Trek actually
resembles what the real scientific calls a gravitational singularity -
massive, localized distortions of space and time. A gravitational
singularity (sometimes spacetime singularity) is, approximately, a
place where quantities which are used to measure the gravitational
field become infinite. Such quantities include the curvature of
spacetime or the density of matter. More accurately, a spacetime with a
singularity contains geodesics ("straight lines" to curved spacetime)
which cannot be completed in a smooth manner. The limit of such a
geodesic is the singularity.
The two most important types of spacetime singularities
are curvature singularities and conical singularities. Singularities
can also be divided according to whether they are covered by an event
horizon or not (naked singularities). According to general relativity,
the initial state of the universe, at the beginning of the Big Bang,
was a singularity. Another type of singularity predicted by general
relativity is inside a black hole: any star collapsing beyond a certain
point would form a black hole, inside which a singularity (covered by
an event horizon) would be formed, as all the matter would flow into a
certain point (or a circular line, if the black hole is rotating).
These singularities are also known as curvature singularities.
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