Have neutrinos to do with Dark Energy ?

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Presentation transcript:

Have neutrinos to do with Dark Energy ?

Why neutrinos may play a role Mass scales : Dark Energy density : ρ ~ ( 2×10 -3 eV )- 4. Neutrino mass : eV or below. Cosmological trigger : Neutrinos became non-relativistic only in the late Universe . Neutrino energy density not much smaller than Dark Energy density . Neutrinos can have substantial coupling to Dark Energy.

connection between dark energy and neutrino properties = 1.27 present dark energy density given by neutrino mass present equation of state given by neutrino mass !

What do we know about Dark Energy ?

Dark Energy dominates the Universe Energy - density in the Universe = Matter + Dark Energy 30 % + 70 %

Composition of the universe Atoms : Ωb = 0.045 Dark Matter : Ωdm= 0.25 Dark Energy : Ωh = 0.7

Energy density that does not clump Dark Energy : Energy density that does not clump Photons , gravitons : insignificant

Space between clumps is not empty : Dark Energy !

Dark Energy : Homogeneously distributed

Einstein’s equations : ( almost ) static Dark Energy predicts accelerated expansion of Universe

Dark Energy : observations fit together !

Observational bounds on Ωh G.Robbers , M.Doran ,…

Why now problem Why does fraction in Dark Energy increase in present cosmological epoch , and not much earlier or much later ?

What is Dark Energy ? Cosmological Constant or Quintessence ?

Cosmological Constant - Einstein - Constant λ compatible with all symmetries No time variation in contribution to energy density Why so small ? λ/M4 = 10-120 Why important just today ?

Cosmological mass scales Energy density ρ ~ ( 2.4×10 -3 eV )- 4 Reduced Planck mass M=2.44×10 27 eV Newton’s constant GN=(8πM²) Only ratios of mass scales are observable ! homogeneous dark energy: ρh/M4 = 7 10ˉ¹²¹ matter: ρm/M4= 3 10ˉ¹²¹

Time evolution Same explanation for small dark energy? ρm/M4 ~ aˉ³ ~ tˉ² matter dominated universe tˉ3/2 radiation dominated universe ρm/M4 ~ aˉ³ ~ ρr/M4 ~ aˉ4 ~ t -2 radiation dominated universe Huge age small ratio Same explanation for small dark energy?

Cosm. Const. | Quintessence static | dynamical

Quintessence (cosmon) Dynamical dark energy , generated by scalar field (cosmon) C.Wetterich,Nucl.Phys.B302(1988)668, 24.9.87 P.J.E.Peebles,B.Ratra,ApJ.Lett.325(1988)L17, 20.10.87

Prediction : homogeneous dark energy influences recent cosmology - of same order as dark matter - Original models do not fit the present observations …. modifications

Quintessence Cosmon – Field φ(x,y,z,t) similar to electric field , but no direction ( scalar field ) Homogeneous und isotropic Universe : φ(x,y,z,t)=φ(t) Potential und kinetic energy of the cosmon -field contribute to a dynamical energy density of the Universe !

Evolution of cosmon field Field equations Potential V(φ) determines details of the model V(φ) =M4 exp( - αφ/M ) for increasing φ the potential decreases towards zero !

exponential potential constant fraction in dark energy Ωh = 3/α2 V(φ) =M4 exp( - αφ/M ) can explain order of magnitude of dark energy !

Neutrinos in cosmology only small fraction of energy density only sub-leading role ?

Neutrino cosmon coupling Strong bounds on atom-cosmon coupling from tests of equivalence principle or time variation of couplings. No such bounds for neutrino-cosmon coupling. In particle physics : Mass generation mechanism for neutrinos differs from charged fermions. Seesaw mechanism involves heavy particles whose mass may depend on the value of the cosmon field.

neutrino mass seesaw and cascade mechanism triplet expectation value ~ doublet squared omit generation structure

neutrino mass cascade ( seesaw II ) mechanism ( ? ) …. C.Wetterich, Nucl.Phys.B187 (1981) 343 cascade ( seesaw II ) mechanism M.Magg, C.W. 1980

Neutrino cosmon coupling realized by dependence of neutrino mass on value of cosmon field β ≈ 1 : cosmon mediated attractive force between neutrinos has similar strength as gravity

growing neutrino quintessence

growing neutrinos change cosmon evolution modification of conservation equation for neutrinos

growing neutrino mass triggers transition to almost static dark energy L.Amendola, M.Baldi,…

effective cosmological trigger for stop of cosmon evolution : neutrinos get non-relativistic this has happened recently ! sets scales for dark energy !

connection between dark energy and neutrino properties = 1.27 present dark energy density given by neutrino mass present equation of state given by neutrino mass !

cosmological selection present value of dark energy density set by cosmological event : neutrinos become non – relativistic not given by ground state properties !

cosmon coupling to neutrinos basic ingredient : cosmon coupling to neutrinos

Cosmon coupling to neutrinos can be large ! interesting effects for cosmology if neutrino mass is growing growing neutrinos can stop the evolution of the cosmon transition from early scaling solution to cosmological constant dominated cosmology Fardon,Nelson,Weiner L.Amendola,M.Baldi,…

stopped scalar field mimicks a cosmological constant ( almost …) rough approximation for dark energy : before redshift 5-6 : scaling ( dynamical ) after redshift 5-6 : almost static ( cosmological constant )

cosmon evolution “stopped” scaling

neutrino lumps

neutrino fluctuations neutrino structures become nonlinear at z~1 for supercluster scales stable neutrino-cosmon lumps exist D.Mota , G.Robbers , V.Pettorino , … N.Brouzakis , N.Tetradis ,… ; O.Bertolami ; Y.Ayaita , M.Weber,…

Formation of neutrino lumps N- body simulation M.Baldi et al

N-body code with fully relativistic neutrinos and backreaction one has to resolve local value of cosmon field and then form cosmological average; similar for neutrino density, dark matter and gravitational field Y.Ayaita,M.Weber,…

Formation of neutrino lumps Y.Ayaita,M.Weber,…

backreaction cosmon field inside lumps does not follow cosmological evolution neutrino mass inside lumps smaller than in environment L.Schrempp, N.Nunes,…

importance of backreaction : cosmological average of neutrino mass Y.Ayaita , E.Puchwein,…

importance of backreaction : fraction in Dark Energy

neutrino lumps behave as non-relativistic fluid with effective coupling to cosmon Y.Ayaita, M.Weber,…

φ - dependent neutrino – cosmon coupling neutrino lumps form and are disrupted by oscillations in neutrino mass smaller backreaction

oscillating neutrino mass

oscillating neutrino lumps

small oscillations in dark energy

Tests for growing neutrino quintessence

Hubble parameter as compared to ΛCDM

Hubble parameter ( z < zc ) only small difference from ΛCDM !

bounds on average neutrino mass

Small induced enhancement of dark matter power spectrum at large scales

Enhanced bulk velocities

Enhancement of gravitational potential Test of allowed parameter space by ISW effect

Can time evolution of neutrino mass be observed ? Experimental determination of neutrino mass may turn out higher than cosmological upper bound in model with constant neutrino mass ( KATRIN, neutrino-less double beta decay ) GERDA

Conclusions Cosmic event triggers qualitative change in evolution of cosmon Cosmon stops changing after neutrinos become non-relativistic Explains why now Cosmological selection Model can be distinguished from cosmological constant

End

cascade mechanism triplet expectation value ~ M.Magg , … G.Lazarides , Q.Shafi , …

cascade

varying neutrino mass ε ≈ -0.05 triplet mass depends on cosmon field φ neutrino mass depends on φ

cascade mechanism triplet expectation value ~

“singular” neutrino mass triplet mass vanishes for φ → φt neutrino mass diverges for φ → φt

strong effective neutrino – cosmon coupling for φ → φt typical present value : β ≈ 50 cosmon mediated attraction between neutrinos is about 502 stronger than gravitational attraction

early scaling solution ( tracker solution ) neutrino mass unimportant in early cosmology

dark energy fraction determined by neutrino mass constant neutrino - cosmon coupling β variable neutrino - cosmon coupling

effective stop of cosmon evolution cosmon evolution almost stops once neutrinos get non –relativistic ß gets large This always happens for φ → φt !