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8/3/2019 Theo M. Nieuwenhuizen- Do non-relativistic neutrinos constitute the dark matter ?
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Do non-relativistic neutrinos
constitute the dark matter ?
Europhysics Letters 86 (2009) 59001
Theo M. NieuwenhuizenInstitute for Theoretical Physics
University of Amsterdam
CSNSM
Orsay 23-5-2009
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Outline
A modeling in virial equilibrium
Comparison to a galaxy supercluster
Mass, properties, name of DM particle
Introduction: What is dark matter DM
Nucleosynthesis
About virial equilibrium
Dark matter condensation on cluster; reionization
Conclusion
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Dark matter in the Universe
! Studied by Jan Hendrik Oort 1932 for our galaxy! Zwicky 1933: for rotation galaxy clusters! V. Rubin 1980: for rotation around galaxies! Needed to explain stability of galaxies
!Needed to explain cosmology
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Dark matter ringaround massive galaxy cluster
detected by Hubble Space Telescope HST
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Bullet clusterTwo galaxy clusters crossed each other.
And so didtheir dark matter.
! White: galaxies and foregrounds
!Red: X ray emitted by hot gas! Blue: dark matter inferred from lensing
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The two types of dark matter! MACHOs: Massive Astrophysical Compact Halo Objects
!Most baryons are dark (non-luminous).
! A fraction is in ionized hydrogen clouds.! A fraction is locked up in frozen H-He planets of earth weight.! These planets occur in clumps of 100,000 solar masses.! Some clumps developed into globular star clusters! These clumps act as ideal gas particles around galaxies.
!This explains galactic dark matter, its rotation curves.! Too small for detection in Eros II (Dapnia)
! WIMPs Weakly Interacting Massive Particles: this talk! The dark matter of galaxy clusters is non-baryonic.! Detected by lensing (galaxies have banana-shape)! About 20-25% of total mass of the Universe.! May or may not be detectable in sky searches (e.g. Edelweiss)! Not MACHOs or WIMPs but MACHOs and WIMPs !!
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! Abell 1689galaxy cluster
! Nearby z = 0.184! Total mass
! Luminous mass
!
Baryon poor
! Einstein ring
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Abell 1689
X-ray
emitting gas
T=10 keV =
1.16 10^8 K
Dark matter
GalaxiesGas
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! Against slavery! How to prevent despotism?! Trias politica! American, French, (Dutch,) constitution! woman can head a government,
but not be effective as the head of a family
1689: birth of Montesquieu
Charles Louis de Secondat,baron de La Brde et de Montesquieu
(1689-1755)
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Theory
! Assume that DM comes from quantum particlesin their common gravitational potential U(r)
! Mass m, degeneracy g = 2 (2s+1) #families! Mass density for fermions in equilibrium at T
! Gravitational potentialU(0)=0
! Poisson eqn (spherical symmetry)! Together they give closed problem for U(r)
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Dark matter (x), Galaxies (G) and gas (g)
! Hydrostatic equilibrium
!
Ideal gas laws
! Result! Virial equilibrium:
equal velocity dispersions
M(r) total mass inside r
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Dimensionless shape
radius, potential
thermal length, scale
Dark density
Poisson eqn
dark matter + Galaxies + gas
Virial equilibrium: Galaxies
gas (ionized H, He, 30% solar metallicity)
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Observed quantity in strong and weak lensing
Integrated mass
along line-of-sight
Average in (0, r)
Average in (r, r_m)
Contrast function
From the model
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Fit to A1689 lensing data of Tyson and Fischer ApJ 1995
Limousin et al, ApJ 2007
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The mass of the dark matter particle
reduced Hubble parameter
small error, 2.0%
Previous estimates: keV, MeV, GeV, TeV: excluded
Cosmic density of g occupied
modes that once were thermal
Cosmic matter fraction
= number ofavailable modes
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What is the dark matter particle?
The dark matter fraction
matches WMAP5 for g=12
(anti) neutrinos, left+right handed, 3 families 2*2*3=12 mass = 1.455 eV
Not: axions, gravitinos, neutralinos, X-inos (early decouplers have small occupation)
Typical speed is non-relativistic, v = 490 km/s
Local density can be enormous: in Abell center: one billion in a few cc
Thermal length visible to the eye
Temperature is low
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The biggest quantum structure
# neutrinos
per (thermal
wavelength)^3
per degree of freedom
N=1: quantum-to-classical crossover
at r = 505 kpc = 1.6 million light yeard = 2r = 3.2 million light year
That is pretty big
Baryons are poor tracers
of dark matterdensity,even though they do
trace the enclosed mass
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Temperature of gas: 10 keV=10^8 K
Log(Mass)
Log(r/kpc)
Cluster radiates like a star.
Radiated energy supplied by contraction.
Radiation helps to keep virial equilibrium.
Virial T of alpha-particles
Virial equilibrium assumed;
only amplitude adjusted
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Right handed neutrinos and nucleosynthesis
! Extra neutrino `families! Extra matter causes enhanced expansion
! Faster expansion: too few neutron decays, too much He-4! Neutrino asymmetry: more neutrinos than anti-neutrinos
! Thus more reactions for neutron decay
!These effects can compensate each other
! So nucleosynthesis can accommodate right-handed neutrinos
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Effect on data Steigman IJMP E, 2005
=0=
==0==
===0=====
Adjusting He-4 to WMAP
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Why virial equilibrium?
! Lynden Bell: violent relaxation.
!Relaxation in time-dependent potential exchangesenergy of a given particle with
the gravitational energy of the whole cluster
! Iff phase space density uniform, then Fermi-Diracdistribution
! Iff not, it is probably a good approximation.! X-ray radiation helps to maintain the virial state
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CDM or HDM?
! Cold Dark Matter: it is already clumped at decoupling z=1100
!But neutrinos are free streaming until trapped by galaxy cluster
! Crossover when Newton force matches Hubble force! Free streaming! At cluster center! They match at crossover: Voids loose neutrinos at z=28, T=77 L, age 120 Myr.! This heats the intracluster gas up to 10 keV, so it reionizes! Hot Dark Matter is the proper paradigm; Agrees with gravito-hydrodynamics
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What about galactic dark matter?
! Proto globolar clusters:Clumps of H-He planets, of weight 1 million M_sun each,
act as ideal gas particles
! In virial equilibrium due to mutual collisions! polylog linearizes! gets absorbed by a shift: unique shape of profile! Virial speed
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Galaxy rotation curves
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Psalm 118:22
The stone which the builders refused
is become the head stone of the corner
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KArlsruhe TRItium Neutrino Experiments
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