2002
DOI: 10.1023/a:1015934027224
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Dark Matter as a Cosmic Bose-Einstein Condensate and Possible Superfluid

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Cited by 106 publications
(119 citation statements)
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“…1. If we solve the differential equation (31) with A 2 > ðA 2 Þ Ã (full lines), the density profile reaches a minimum f min at X ¼ X c before increasing indefinitely. As A 2 approaches ðA 2 Þ Ã from above, the point X c is pushed further and further away while f min decreases.…”
Section: Numerical Solutionmentioning
confidence: 99%
See 1 more Smart Citation
“…1. If we solve the differential equation (31) with A 2 > ðA 2 Þ Ã (full lines), the density profile reaches a minimum f min at X ¼ X c before increasing indefinitely. As A 2 approaches ðA 2 Þ Ã from above, the point X c is pushed further and further away while f min decreases.…”
Section: Numerical Solutionmentioning
confidence: 99%
“…On the other hand, some authors [21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36] have proposed that dark matter halos themselves could be in the form of gigantic self-gravitating Bose-Einstein condensates (with or without self-interaction [37]) described by a single wave function c ðr; tÞ. In the Newtonian limit, which is relevant at the galactic scale, the evolution of this wave function is governed by the Gross-Pitaevskii-Poisson (GPP) system [33].…”
Section: Introductionmentioning
confidence: 99%
“…This has lead some to general consideration of Bose-Einstein-Condensate (BEC) dark matter (see, for example, [47][48][49], and in the case of axions [50,51]). Indeed, the numerical simulation of [52] showed that the presence of such an ultra-light scalar condensate indeed reduces the number of dwarf galaxies, but in fact does very little to the cuspy density profile.…”
mentioning
confidence: 99%
“…(1) derives from the relation U K = mc 2 1+(p/mc) 2 −1 in which p = /ξ is the fermion linear momentum and ξ = N −1/3 r is the coherence length of the fermion wave function. 5 The second term derives from the magnetic dipole interaction U M = εN µ 2 /ξ 3 simplified to pertain to nearest-neighbor interactions in the two cases in which contiguous moments are either aligned (ε = +1) for minimum entropy or antiparallel (ε = −1) for minimum energy. It will be seen shortly that in a degenerate star, for which the fermions are effectively at 0 K, stable equilibrium results from the parallel alignment of magnetic moments.…”
mentioning
confidence: 99%