QCD in Neutron Stars and Strange Stars
- Department of Physics, San Diego State University, 5500 Campanile Drive, San Diego, CA 92182-1233 (United States)
- FIAS, Goethe University, Ruth Moufang Str 1, 60438 Frankfurt (Germany)
This paper provides an overview of the possible role of Quantum Chromo Dynamics (QCD) for neutron stars and strange stars. The fundamental degrees of freedom of QCD are quarks, which may exist as unconfined (color superconducting) particles in the cores of neutron stars. There is also the theoretical possibility that a significantly large number of up, down, and strange quarks may settle down in a new state of matter known as strange quark matter, which, by hypothesis, could be more stable than even the most stable atomic nucleus, {sup 56}Fe. In the latter case new classes of self-bound, color superconducting objects, ranging from strange quark nuggets to strange quark stars, should exist. The properties of such objects will be reviewed along with the possible existence of deconfined quarks in neutron stars. Implications for observational astrophysics are pointed out.
- OSTI ID:
- 21516860
- Journal Information:
- AIP Conference Proceedings, Vol. 1354, Issue 1; Conference: Tropical QCD II workshop, Cairns (Australia), 26 Sep - 1 Oct 2010; Other Information: DOI: 10.1063/1.3587579; (c) 2011 American Institute of Physics; ISSN 0094-243X
- Country of Publication:
- United States
- Language:
- English
Similar Records
Sequential deconfinement of quark flavors in neutron stars
Single-flavor CSL phase in compact stars
Related Subjects
ASTROPHYSICS
COLOR MODEL
DEGREES OF FREEDOM
HYPERONS
HYPOTHESIS
IRON 56
NEUTRON STARS
NUCLEONS
QUANTUM CHROMODYNAMICS
S QUARKS
SUPERCONDUCTIVITY
BARYONS
COMPOSITE MODELS
ELECTRIC CONDUCTIVITY
ELECTRICAL PROPERTIES
ELEMENTARY PARTICLES
EVEN-EVEN NUCLEI
FERMIONS
FIELD THEORIES
HADRONS
INTERMEDIATE MASS NUCLEI
IRON ISOTOPES
ISOTOPES
MATHEMATICAL MODELS
NUCLEI
PARTICLE MODELS
PHYSICAL PROPERTIES
PHYSICS
QUANTUM FIELD THEORY
QUARK MODEL
QUARKS
STABLE ISOTOPES
STARS
STRANGE PARTICLES