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arXiv:1507.03013astro-ph.CO

A Dark Matter Superfluid

Justin Khoury

Abstract

In this talk we present a novel framework that unifies the stunning success of MOND on galactic scales with the triumph of the LambdaCDM model on cosmological scales. This is achieved through the rich and well-studied physics of superfluidity. The dark matter and MOND components have a common origin, representing different phases of a single underlying substance. In galaxies, dark matter thermalizes and condenses to form a superfluid phase. The superfluid phonons couple to baryonic matter particles and mediate a MOND-like force. Our framework naturally distinguishes between galaxies (where MOND is successful) and galaxy clusters (where MOND is not): dark matter has a higher temperature in clusters, and hence is in a mixture of superfluid and normal phase. The rich and well-studied physics of superfluidity leads to a number of striking observational signatures, which we briefly discuss. Remarkably the critical temperature and equation of state of the dark matter superfluid are similar to those of known cold atom systems. Identifying a precise cold atom analogue would give important insights on the microphysical interactions underlying DM superfluidity. Tantalizingly, it might open the possibility of simulating the properties and dynamics of galaxies in laboratory experiments.

arXiv comments
8 pages. To appear in the proceedings of the 2015 Rencontres de Moriond, "Gravitation: 100 years after GR"
Journal reference
DOI
Subjects
astro-ph.COCosmology and Nongalactic Astrophysics cond-mat.otherOther Condensed Matter gr-qcGeneral Relativity and Quantum Cosmology hep-thHigh Energy Physics, Theory

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    • The conclusion drawn in the article, but not mentioned by name, is a reference to Dark Matter Superfluid [1] [1] https://arxiv.org/abs/1507.03013

      TrispusAttucksView on HNParent context

    • Dark Matter Superfluid [1] [1] https://arxiv.org/abs/1507.03013

      TrispusAttucksView on HNParent context

    • " So what we need is a kind of phase transition that explains why and under which circumstances the behavior of these additional fields, or particles, changes, so that we need two different sets of equations. And once you look at it this way, it’s obvious why we have not made…

      amaiView on HNParent context

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