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Magnetic fields within color superconducting neutron star cores
High Energy Physics - Phenomenology · Submitted 6 Oct 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our results demonstrate that such cores admit magnetic fields without restricting them to quantized flux tubes.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We discuss the Meissner effect for a color superconductor formed by cold dense quark matter. Though color and ordinary electromagnetism are broken in a color superconductor, there is a linear combination of the photon and a gluon that remains massless. Consequently, a color superconducting region may be penetrated by an external magnetic field. We show that at most a small fraction of the magnetic field is expelled, and if the screening distance is the smallest length scale in the problem there is no expulsion at all. We calculate the behavior of the magnetic field for a spherical geometry relevant for compact stars. If a neutron star contains a quark matter core, this core is a color superconductor. Our results demonstrate that such cores admit magnetic fields without restricting them to quantized flux tubes. Such magnetic fields within color superconducting neutron star cores are stable on time scales longer than the age of the universe, even if the spin period of the neutron star is changing.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the Meissner effect for a color superconductor formed by cold dense quark matter. | contribution 0.73 | 0.61 | 0.03 | unclear 0.75 |
| s1 | Though color and ordinary electromagnetism are broken in a color superconductor, there is a linear combination of the photon and a gluon that remains massless. | background 0.84 | 0.21 | 0.06 | asserted 1.00 |
| s2 | Consequently, a color superconducting region may be penetrated by an external magnetic field. | result 0.60 | 0.29 | 0.14 | hedged possibility 1.00 |
| s3 | We show that at most a small fraction of the magnetic field is expelled, and if the screening distance is the smallest length scale in the problem there is no expulsion at all. | result 1.00 | 0.92 | 0.33 | asserted 0.99 |
| s4 | We calculate the behavior of the magnetic field for a spherical geometry relevant for compact stars. | method 0.55 | 0.94 | 0.05 | asserted 0.98 |
| s5 | If a neutron star contains a quark matter core, this core is a color superconductor. | background 0.81 | 0.18 | 0.07 | asserted 0.99 |
| s6 | Our results demonstrate that such cores admit magnetic fields without restricting them to quantized flux tubes. | result 0.60 | 0.90 | 0.41 | asserted 1.00 |
| s7 | Such magnetic fields within color superconducting neutron star cores are stable on time scales longer than the age of the universe, even if the spin period of the neutron star is changing. | result 0.94 | 0.84 | 0.45 | asserted 1.00 |
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The paper
Original abstract
We discuss the Meissner effect for a color superconductor formed by cold dense quark matter. Though color and ordinary electromagnetism are broken in a color superconductor, there is a linear combination of the photon and a gluon that remains massless. Consequently, a color superconducting region may be penetrated by an external magnetic field. We show that at most a small fraction of the magnetic field is expelled, and if the screening distance is the smallest length scale in the problem there is no expulsion at all. We calculate the behavior of the magnetic field for a spherical geometry relevant for compact stars. If a neutron star contains a quark matter core, this core is a color superconductor. Our results demonstrate that such cores admit magnetic fields without restricting them to quantized flux tubes. Such magnetic fields within color superconducting neutron star cores are stable on time scales longer than the age of the universe, even if the spin period of the neutron star is changing.
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References
How the literature uses it
18 arXiv papers cite this in 27 sentences
Papers citing it · 19 sentences without a confident label
Uses its method or tool 1 paper
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The organization of this paper is as follows: In Sec. II, starting from an extended Lagrangian density of a gauged NJL model containing two flavors, and following the method presented in [ref] , we introduce the rotated magnetic field $ẽB$ and determine the Lagrangian density containing the $χ$SB and CSC mass gaps, $σ_B$ and $Δ_B$, respectively.
Color neutral 2SC phase of cold and dense quark matter in the presence of constant magnetic fields · Introduction · 1.00
Uses its data or values 1 paper
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The mixing coefficients have been determined in [ref] (see also [ref] ) and are given by cosθ= √(3) g/√(3 g^2 + e^2) sinθ= e/√(3 g^2 + e^2) .
Crystalline color superconductors · Meissner masses of gluons in the g2SC phase · 0.90
Compares with it 1 paper
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For comparison, the critical magnetic field needed to destroy superconductivity is at least of order $μΔ/e$ [ref] .
Axial anomaly and magnetism of nuclear and quark matter · 2SC phase in a magnetic field · 0.95
Cites it as background 5 papers
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The $(3)$ color symmetries and the global $(3)_L$ and $(3)_R$ flavor symmetries are broken by the condensate to a global subgroup consisting of simultaneous color and flavor transformations, [equation] A diagonal subgroup of the $(3)_L×(3)_R$ is weakly gauged by the electric charge $Qe$, where $Qe$ is a diagonal matrix in the flavor space with entries equalling the electric charges of the $u$, $d$ and $s$ quarks, and a linear combination of the $t^8$ and $Q$ (known as $Q̃$) is unbroken [ref] .
The shear viscosity of two-flavor crystalline color superconducting quark matter · Review · 0.95
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Possible effects caused by strong magnetic fields include magnetic catalysis [ref] , modification of the nature of electroweak phase transition [ref] , spontaneous creation of axial currents [ref] , formation of $π_0$ domain walls [ref] and chiral density waves [ref] , chiral magnetic effect [ref] , and last but not least the influence on possible color-superconducting phases [ref] .
Phase diagram of hot magnetized two-flavor color superconducting quark matter · Introduction · 0.99
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The response of color-superconducting quark matter to a strong magnetic field has also been studied [ref] .
Axial anomaly and magnetism of nuclear and quark matter · Introduction · 1.00
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