| Revision as of 07:46, 29 December 2020 edit64.44.80.252 (talk) →Strange matter that is only stable at high pressure: Add a paragraph explaining how strange matter can be energetically favourable. The article needs it somewhere, but not sure if the place I picked is correct.← Previous edit | Revision as of 07:10, 30 December 2020 edit undoRobH103 (talk | contribs)225 edits Changed "The nuclear matter" to "Nuclear matter" because having "The" implies a reference to the atomic nucleus previously mentioned, which is an incorrect reference.Next edit → | ||
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| '''Strange matter''', or '''strange quark matter''', is ] containing ]s. In nature, strange matter is hypothesized to occur in the core of ]s, or, more speculatively, as isolated droplets that may vary in size from ]s (]s) to kilometers, as in the hypothetical ]. At high enough density, strange matter is expected to be ].{{citation needed|date=February 2019}} | '''Strange matter''', or '''strange quark matter''', is ] containing ]s. In nature, strange matter is hypothesized to occur in the core of ]s, or, more speculatively, as isolated droplets that may vary in size from ]s (]s) to kilometers, as in the hypothetical ]. At high enough density, strange matter is expected to be ].{{citation needed|date=February 2019}} | ||
| Ordinary ], also referred to as atomic matter, is composed of atoms, with nearly all matter concentrated in the atomic nuclei. |
Ordinary ], also referred to as atomic matter, is composed of atoms, with nearly all matter concentrated in the atomic nuclei. ] is a liquid composed of ]s and ]s, and they are themselves composed of ] and ]. Quark matter is a ] composed entirely of ]s. If quark matter contains ], it is often called strange matter (or strange quark matter), and when quark matter does not contain strange quarks, it is sometimes referred to as non-strange quark matter. | ||
| == Definition == | == Definition == | ||
Revision as of 07:10, 30 December 2020
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Strange matter, or strange quark matter, is quark matter containing strange quarks. In nature, strange matter is hypothesized to occur in the core of neutron stars, or, more speculatively, as isolated droplets that may vary in size from femtometers (strangelets) to kilometers, as in the hypothetical strange stars. At high enough density, strange matter is expected to be color superconducting.
Ordinary matter, also referred to as atomic matter, is composed of atoms, with nearly all matter concentrated in the atomic nuclei. Nuclear matter is a liquid composed of neutrons and protons, and they are themselves composed of up and down quarks. Quark matter is a condensed form of matter composed entirely of quarks. If quark matter contains strange quarks, it is often called strange matter (or strange quark matter), and when quark matter does not contain strange quarks, it is sometimes referred to as non-strange quark matter.
Definition
In particle physics and astrophysics, the term is used in two ways, one broader and the other more specific
- The broader meaning is simply quark matter that contains three types of quarks: up, down, and strange. In this definition, there is a critical pressure and an associated critical density, and when nuclear matter (made of protons and neutrons) is compressed beyond this density, the protons and neutrons dissociate into quarks, yielding quark matter (probably strange matter).
- The narrower meaning is that quark matter is more stable than nuclear matter, i.e. that the true ground state of matter is quark matter. The idea that this could happen is the "strange matter hypothesis" of Bodmer and Witten. In this definition, the critical pressure is zero. The nuclei that we see in the matter around us, which are droplets of nuclear matter, are actually metastable, and given enough time (or the right external stimulus) would decay into droplets of strange matter, i.e. strangelets.
Strange matter that is only stable at high pressure
Under the broader definition, strange matter might occur inside neutron stars, if the pressure at their core is high enough (i.e. above the critical pressure). At the sort of densities and high pressures we expect in the center of a neutron star, the quark matter would probably be strange matter. It could conceivably be non-strange quark matter, if the effective mass of the strange quark were too high. Charm quarks and heavier quarks would only occur at much higher densities.
Strange matter comes about as a way to relieve degeneracy pressure. The Pauli exclusion principle forbids fermions such as quarks from occupying the same position and energy level. When the particle density is high enough that all energy levels below the available thermal energy are already occupied, increasing the density further requires raising some to higher, unoccupied energy levels. This need for energy to cause compression manifests as a pressure. Normally, matter consists of twice as many down quarks (charge −1/3 e) as up quarks (charge +2/3 e), so the degeneracy pressure of down quarks dominates electrically neutral quark matter. However, when the required energy level is high enough, an alternative becomes available: half of the down quarks can be transmuted to strange quarks (charge −1/3 e). The higher rest mass of the strange quark costs some energy, but by opening up an additional set of energy levels, the average energy per particle can be lower, making strange matter more stable than non-strange quark matter.
A neutron star with a quark matter core is often called a hybrid star. However, it is hard to know whether hybrid stars really exist in nature because physicists currently have little idea of the likely value of the critical pressure or density. It seems plausible that the transition to quark matter will already have occurred when the separation between the nucleons becomes much smaller than their size, so the critical density must be less than about 100 times nuclear saturation density. But a more precise estimate is not yet available, because the strong interaction that governs the behavior of quarks is mathematically intractable, and numerical calculations using lattice QCD are currently blocked by the fermion sign problem.
One major area of activity in neutron star physics is the attempt to find observable signatures by which we could tell, from earth based observations of neutron stars, whether they have quark matter (probably strange matter) in their core.
Strange matter that is stable at zero pressure
If the "strange matter hypothesis" is true then nuclear matter is metastable against decaying into strange matter. The lifetime for spontaneous decay is very long, so we do not see this decay process happening around us. However, under this hypothesis there should be strange matter in the universe:
- Quark stars (often called "strange stars") consist of quark matter from their core to their surface. They would be several kilometers across, and may have a very thin crust of nuclear matter.
- Strangelets are small pieces of strange matter, perhaps as small as nuclei. They would be produced when strange stars are formed or collide, or when a nucleus decays.
See also
- Exotic matter – Physics term for multiple concepts
- Negative matter – Physics term for multiple conceptsPages displaying short descriptions of redirect targets
- Quark matter – Hypothetical phases of matterPages displaying short descriptions of redirect targets
- Quark star – Compact exotic star which forms matter consisting mostly of quarks
- Strangeness and quark-gluon plasma – Subatomic signaturePages displaying short descriptions of redirect targets
- Strangelet – Type of hypothetical particle
- Quark – Elementary particle, main constituent of matter
- QCD matter – Hypothetical phases of matter
References
- ^ Madsen, Jes (1999). "Physics and astrophysics of strange quark matter". Hadrons in Dense Matter and Hadrosynthesis. Lecture Notes in Physics. Vol. 516. pp. 162–203. arXiv:astro-ph/9809032. doi:10.1007/BFb0107314. ISBN 978-3-540-65209-0.
- ^ Weber, F. (2005). "Strange quark matter and compact stars". Progress in Particle and Nuclear Physics. 54 (1): 193–288. arXiv:astro-ph/0407155. Bibcode:2005PrPNP..54..193W. doi:10.1016/j.ppnp.2004.07.001..
- Bodmer, A. R. (1971). "Collapsed Nuclei". Physical Review D. 4 (6): 1601–1606. Bibcode:1971PhRvD...4.1601B. doi:10.1103/PhysRevD.4.1601.
- ^ Witten, Edward (1984). "Cosmic separation of phases". Physical Review D. 30 (2): 272–285. Bibcode:1984PhRvD..30..272W. doi:10.1103/PhysRevD.30.272.
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