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Dark Matter and the Solar Neutrino Problem: Can Particle Physics Provide a Single Solution?
Author(s) -
WEST GEOFFREY B.
Publication year - 1989
Publication title -
annals of the new york academy of sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.712
H-Index - 248
eISSN - 1749-6632
pISSN - 0077-8923
DOI - 10.1111/j.1749-6632.1989.tb50643.x
Subject(s) - physics , neutrino , solar core , solar neutrino , observable , radius , dark matter , standard solar model , particle physics , astrophysics , luminosity , solar neutrino problem , neutrino oscillation , quantum mechanics , computer security , galaxy , computer science
It has been known for some time that weakly interacting massive particles (WIMPS or cosmions) can simultaneously solve both the dark matter and solar neutrino problem. 1 The idea is quite simple and elegant: such particles being the constituents of dark matter 2 would, if sufficiently massive, acrete in the core region of the sun. As they orbit in the sun's interior, they transfer heat from the inner to the outer regions thereby cooling the core. Lowering the core temperature ( T ) by only 10% is sufficient to reduce the predicted output of observable neutrinos by a factor of 3 to 4 leading to a resolution of the solar neutrino problem. 3 The crucial point is that almost 80% of the observable neutrinos (which represent only 10 −6 of the total neutrino output of the sun!) result from the decay 8 B ± 8 Be *+ e + v e and the rate for this is very sensitive to T ). On the other hand, solar models that accurately describe bulk properties of the sun such as its total luminosity, radius, mass, and surface abundance of elements are not very sensitive to T ). Indeed, changing T ) by 10% has only a negligible effect on these gross properties, including the total neutrino output of the sun. 3 Roughly speaking the necessary properties of the cosmion, such as its mass ( M c ) and cross‐section off of protons (σ) can be deduced by requiring that it lowers T ± by ±10% without appreciably affecting the temperature beyond a radius ±0.1 R , where most of the solar luminosity ( L ) originates.