We consider quarkyonic matter to naturally explain the observed properties of neutron stars. We argue that such matter might exist at densities close to that of nuclear matter, and at the onset, the pressure and the sound velocity in quarkyonic matter increase rapidly. In the limit of large number of quark colors N_{c}, this transition is characterized by a discontinuous change in pressure as a function of baryon number density. We make a simple model of quarkyonic matter and show that generically the sound velocity is a nonmonotonic function of density-it reaches a maximum at relatively low density, decreases, and then increases again to its asymptotic value of 1/sqrt[3].
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http://dx.doi.org/10.1103/PhysRevLett.122.122701 | DOI Listing |
Phys Rev Lett
March 2024
Institute for Nuclear Theory, University of Washington, Box 351550, Seattle, Washington 98195, USA.
Phys Rev Lett
March 2019
Institute for Nuclear Theory and Department of Physics, University of Washington, Seattle, Washington 98195, USA.
We consider quarkyonic matter to naturally explain the observed properties of neutron stars. We argue that such matter might exist at densities close to that of nuclear matter, and at the onset, the pressure and the sound velocity in quarkyonic matter increase rapidly. In the limit of large number of quark colors N_{c}, this transition is characterized by a discontinuous change in pressure as a function of baryon number density.
View Article and Find Full Text PDFPhys Rev Lett
July 2013
FIAS, Goethe Universität, Ruth-Moufang-Strasse 1, 60438 Frankfurt am Main, Germany.
We calculate the bremsstrahlung photon spectrum emitted from dynamically evolving "quarkyonic" matter and compare this spectrum with that of a high chemical potential quark-gluon plasma as well as to a hadron gas. We find that the transverse momentum distribution and the harmonic coefficient is markedly different in the three cases. The transverse momentum distribution of quarkyonic matter can be fit with an exponential but is markedly steeper than the distribution expected for the quark-gluon plasma or a hadron gas, even at the lower temperatures expected in the critical point region.
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