Solar Constraints on Asymmetric Dark Matter

dc.contributor.authorLopes, I
dc.contributor.authorSilk, J
dc.date.accessioned2012-11-16T17:28:25Z
dc.date.available2012-11-16T17:28:25Z
dc.date.issued2012-10-01
dc.description.abstractThe dark matter content of the universe is likely to be a mixture of matter and antimatter, perhaps comparable to the measured asymmetric mixture of baryons and antibaryons. During the early stages of the universe, the dark matter particles are produced in a process similar to baryogenesis, and dark matter freezeout depends on the dark matter asymmetry and the annihilation cross section (s-wave and p-wave annihilation channels) of particles and antiparticles. In these η-parameterized asymmetric dark matter (ηADM) models, the dark matter particles have an annihilation cross section close to the weak interaction cross section, and a value of dark matter asymmetry η close to the baryon asymmetry η B . Furthermore, we assume that dark matter scattering of baryons, namely, the spin-independent scattering cross section, is of the same order as the range of values suggested by several theoretical particle physics models used to explain the current unexplained events reported in the DAMA/LIBRA, CoGeNT, and CRESST experiments. Here, we constrain ηADM by investigating the impact of such a type of dark matter on the evolution of the Sun, namely, the flux of solar neutrinos and helioseismology. We find that dark matter particles with a mass smaller than 15 GeV, a spin-independent scattering cross section on baryons of the order of a picobarn, and an η-asymmetry with a value in the interval 10-12-10-10, would induce a change in solar neutrino fluxes in disagreement with current neutrino flux measurements. This result is also confirmed by helioseismology data. A natural consequence of this model is suppressed annihilation, thereby reducing the tension between indirect and direct dark matter detection experiments, but the model also allows a greatly enhanced annihilation cross section. All the cosmological ηADM scenarios that we discuss have a relic dark matter density Ωh 2 and baryon asymmetry η B in agreement with the current WMAP measured values, ΩDM h 2 = 0.1109 ± 0.0056 and η B = 0.88 × 10-10.por
dc.identifier.authoremaililopes@uevora.pt
dc.identifier.authoremailnd
dc.identifier.doi10.1088/0004-637X/757/2/130
dc.identifier.scientificarea343por
dc.identifier.urihttp://hdl.handle.net/10174/5700
dc.language.isoengpor
dc.peerreviewedyespor
dc.publisherThe Astrophysical Journalpor
dc.rightsrestrictedAccesspor
dc.subjectAstrophysicspor
dc.subjectSunpor
dc.subjectdark matterpor
dc.titleSolar Constraints on Asymmetric Dark Matterpor
dc.typearticlepor

Files

Original bundle

Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
LopesSilkadm.pdf
Size:
229.27 KB
Format:
Adobe Portable Document Format

License bundle

Now showing 1 - 1 of 1
Loading...
Thumbnail Image
Name:
license.txt
Size:
3.89 KB
Format:
Item-specific license agreed upon to submission
Description: