Growing Neutrinos and Quintessence Dark Energy dominates the

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Growing Neutrinos and Quintessence

Growing Neutrinos and Quintessence

Dark Energy dominates the Universe Energy - density in the Universe = Matter +

Dark Energy dominates the Universe Energy - density in the Universe = Matter + Dark Energy 25 % + 75 %

Matter : everything that clumps ---------- Dark Energy density is the same at every

Matter : everything that clumps ---------- Dark Energy density is the same at every point of space “ homogeneous “ Space between clumps is not empty

What is Dark Energy ? Cosmological Constant or Quintessence ?

What is Dark Energy ? Cosmological Constant or Quintessence ?

Cosmological Constant - Einstein n Constant λ compatible with all symmetries n No time

Cosmological Constant - Einstein n Constant λ compatible with all symmetries n No time variation in contribution to energy density n Why so small ? λ/M 4 = 10 -120 n Why important just today ?

Cosm. Const | Quintessence static | dynamical

Cosm. Const | Quintessence static | dynamical

Cosmological mass scales n Energy density ρ ~ ( 2. 4× 10 -3 e.

Cosmological mass scales n Energy density ρ ~ ( 2. 4× 10 -3 e. V )- 4 Reduced Planck mass M=2. 44× 1018 Ge. V n Newton’s constant GN=(8πM²) n Only ratios of mass scales are observable ! homogeneous dark energy: ρh/M 4 = 6. 5 10ˉ¹²¹ matter: ρm/M 4= 3. 5 10ˉ¹²¹

Time evolution tˉ² matter dominated universe n ρm/M 4 ~ aˉ³ ~ n ρr/M

Time evolution tˉ² matter dominated universe n ρm/M 4 ~ aˉ³ ~ n ρr/M 4 ~ aˉ4 ~ t -2 radiation dominated universe Huge age tˉ3/2 radiation dominated universe small ratio Same explanation for small dark energy?

Quintessence Dynamical dark energy , generated by scalar field (cosmon) C. Wetterich, Nucl. Phys.

Quintessence Dynamical dark energy , generated by scalar field (cosmon) C. Wetterich, Nucl. Phys. B 302(1988)668, 24. 9. 87 P. J. E. Peebles, B. Ratra, Ap. J. Lett. 325(1988)L 17,

Prediction : homogeneous dark energy influences recent cosmology - of same order as dark

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

Cosmon n Scalar field changes its value even in the present cosmological epoch n

Cosmon n Scalar field changes its value even in the present cosmological epoch n Potential und kinetic energy of cosmon contribute to the energy density of the Universe n Time - variable dark energy : ρh(t) decreases with time ! V(φ) =M 4 exp( - αφ/M )

“Fundamental” Interactions Strong, electromagnetic, weak interactions On astronomical length scales: graviton + cosmon gravitation

“Fundamental” Interactions Strong, electromagnetic, weak interactions On astronomical length scales: graviton + cosmon gravitation cosmodynamics

Evolution of cosmon field Field equations Potential V(φ) determines details of the model V(φ)

Evolution of cosmon field Field equations Potential V(φ) determines details of the model V(φ) =M 4 exp( - αφ/M ) for increasing φ the potential decreases towards zero !

Cosmic Attractors Solutions independent of initial conditions typically V~t -2 φ ~ ln (

Cosmic Attractors Solutions independent of initial conditions typically V~t -2 φ ~ ln ( t ) Ωh ~ const. details depend on V(φ) or kinetic term early cosmology

exponential potential constant fraction in dark energy Ωh = 2 3(4)/α can explain order

exponential potential constant fraction in dark energy Ωh = 2 3(4)/α can explain order of magnitude of dark energy !

realistic quintessence fraction in dark energy has to increase in “recent time” !

realistic quintessence fraction in dark energy has to increase in “recent time” !

Quintessence becomes important “today” No reason why w should be constant in time !

Quintessence becomes important “today” No reason why w should be constant in time !

cosmic coincidence

cosmic coincidence

coincidence problem What is responsible for increase of Ωh for z < 6 ?

coincidence problem What is responsible for increase of Ωh for z < 6 ? Why now ?

growing neutrino mass triggers transition to almost static dark energy growing neutrino mass

growing neutrino mass triggers transition to almost static dark energy growing neutrino mass

basic ingredient : cosmon coupling to neutrinos

basic ingredient : cosmon coupling to neutrinos

Cosmon coupling to neutrinos n can be large ! Fardon, Nelson, Weiner interesting effects

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

growing neutrinos

growing neutrinos

end of matter domination n growing mass of neutrinos n at some moment energy

end of matter domination n growing mass of neutrinos n at some moment energy density of neutrinos becomes more important than energy density of dark matter n end of matter dominated period similar to transition from radiation domination to matter domination this transition happens in the recent past cosmon plays crucial role n n n

cosmological selection n present value of dark energy density set by cosmological event (

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

connection between dark energy and neutrino properties present dark energy density given by neutrino

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

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

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

varying neutrino – cosmon coupling specific model n can naturally explain why neutrino –

varying neutrino – cosmon coupling specific model n can naturally explain why neutrino – cosmon coupling is much larger than atom – cosmon coupling n

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

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

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

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

varying neutrino mass ε ≈ -0. 05 triplet mass depends on cosmon field φ

varying neutrino mass ε ≈ -0. 05 triplet mass depends on cosmon field φ neutrino mass depends on φ

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

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

strong effective neutrino – cosmon coupling for φ → φt

strong effective neutrino – cosmon coupling for φ → φt

crossover from early scaling solution to effective cosmological constant

crossover from early scaling solution to effective cosmological constant

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

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

growing neutrinos change cosmon evolution modification of conservation equation for neutrinos

growing neutrinos change cosmon evolution modification of conservation equation for neutrinos

effective stop of cosmon evolution almost stops once n neutrinos get non –relativistic n

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

effective cosmological trigger for stop of cosmon evolution : neutrinos get non-relativistic n this

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

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

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

cosmon evolution

cosmon evolution

neutrino fraction remains small Ων mν = 0. 45 e. V z

neutrino fraction remains small Ων mν = 0. 45 e. V z

equation of state present equation of state given by neutrino mass !

equation of state present equation of state given by neutrino mass !

oscillating neutrino mass

oscillating neutrino mass

Hubble parameter as compared to ΛCDM mν=0. 45 e. V

Hubble parameter as compared to ΛCDM mν=0. 45 e. V

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

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

Can time evolution of neutrino mass be observed ? n Experimental determination of neutrino

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

neutrino fluctuations neutrino structures become nonlinear at z~1 for supercluster scales D. Mota ,

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

How can quintessence be distinguished from a cosmological constant ?

How can quintessence be distinguished from a cosmological constant ?

Time dependence of dark energy cosmological constant : Ωh ~ t² ~ (1+z)-3 M.

Time dependence of dark energy cosmological constant : Ωh ~ t² ~ (1+z)-3 M. Doran, …

small early and large present dark energy fraction in dark energy has substantially increased

small early and large present dark energy fraction in dark energy has substantially increased since end of structure formation expansion of universe accelerates in present epoch

effects of early dark energy n modifies cosmological evolution (CMB) n slows down the

effects of early dark energy n modifies cosmological evolution (CMB) n slows down the growth of structure

interpolation of Ωh G. Robbers, M. Doran, …

interpolation of Ωh G. Robbers, M. Doran, …

Early quintessence slows down the growth of structure

Early quintessence slows down the growth of structure

Little Early Dark Energy can make large effect ! Non – linear enhancement Cluster

Little Early Dark Energy can make large effect ! Non – linear enhancement Cluster number relative to ΛCDM Two models with 4% Dark Energy during structure formation Fixed σ8 ( normalization dependence ! ) More clusters at high redshift ! Bartelmann, Doran, …

Conclusions Cosmic event triggers qualitative change in evolution of cosmon n Cosmon stops changing

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

End

End

How to distinguish Q from Λ ? A) Measurement Ωh(z) H(z) i) Ωh(z) at

How to distinguish Q from Λ ? A) Measurement Ωh(z) H(z) i) Ωh(z) at the time of structure formation , CMB - emission or nucleosynthesis ii) equation of state wh(today) > -1 B) Time variation of fundamental “constants” C) Apparent violation of equivalence principle D) Possible coupling between Dark Energy and Dark Mater

Quintessence and Time dependence of “fundamental constants” n Fine structure constant depends on value

Quintessence and Time dependence of “fundamental constants” n Fine structure constant depends on value of cosmon field : α(φ) (similar in standard model: couplings depend on value of Higgs scalar field) n Time evolution of φ Time evolution of α Jordan, …

baryons : the matter of stars and humans Ωb = 0. 045

baryons : the matter of stars and humans Ωb = 0. 045

primordial abundances for three GUT models He present observations : 1σ D Li T.

primordial abundances for three GUT models He present observations : 1σ D Li T. Dent, S. Stern, …

three GUT models unification scale ~ Planck scale n 1) All particle physics scales

three GUT models unification scale ~ Planck scale n 1) All particle physics scales ~ΛQCD n 2) Fermi scale and fermion masses ~ unification scale n 3) Fermi scale varies more rapidly than ΛQCD n Δα/α ≈ 4 10 -4 allowed for GUT 1 and 3 , larger for GUT 2 Δln(Mn/MP) ≈40 Δα/α ≈ 0. 015 allowed

time varying Fermi scale yields triplet expectation value as function of doublet insert :

time varying Fermi scale yields triplet expectation value as function of doublet insert : t=

time varying electron mass time variation of quantities not related to triplet

time varying electron mass time variation of quantities not related to triplet

Time variation of coupling constants must be tiny – would be of very high

Time variation of coupling constants must be tiny – would be of very high significance ! Possible signal for Quintessence

Summary o Ωh = 0. 75 o Q/Λ : dynamical und static dark energy

Summary o Ωh = 0. 75 o Q/Λ : dynamical und static dark energy will be distinguishable o growing neutrino mass can explain why now problem o Q : time varying fundamental coupling “constants” violation of equivalence principle

? ? ? ? ? ? Are dark energy and dark matter related ?

? ? ? ? ? ? Are dark energy and dark matter related ? Can Quintessence be explained in a fundamental unified theory ?

Quintessence and solution of cosmological constant problem should be related !

Quintessence and solution of cosmological constant problem should be related !

End

End

A few references C. Wetterich , Nucl. Phys. B 302, 668(1988) , received 24.

A few references C. Wetterich , Nucl. Phys. B 302, 668(1988) , received 24. 9. 1987 P. J. E. Peebles, B. Ratra , Astrophys. J. Lett. 325, L 17(1988) , received 20. 1987 B. Ratra, P. J. E. Peebles , Phys. Rev. D 37, 3406(1988) , received 16. 2. 1988 J. Frieman, C. T. Hill, A. Stebbins, I. Waga , Phys. Rev. Lett. 75, 2077(1995) P. Ferreira, M. Joyce , Phys. Rev. Lett. 79, 4740(1997) C. Wetterich , Astron. Astrophys. 301, 321(1995) P. Viana, A. Liddle , Phys. Rev. D 57, 674(1998) E. Copeland, A. Liddle, D. Wands , Phys. Rev. D 57, 4686(1998) R. Caldwell, R. Dave, P. Steinhardt , Phys. Rev. Lett. 80, 1582(1998) P. Steinhardt, L. Wang, I. Zlatev , Phys. Rev. Lett. 82, 896(1999)

Quintessence C. Wetterich A. Hebecker, M. Doran, M. Lilley, J. Schwindt, C. Müller, G.

Quintessence C. Wetterich A. Hebecker, M. Doran, M. Lilley, J. Schwindt, C. Müller, G. Schäfer, E. Thommes, R. Caldwell, M. Bartelmann, K. Kharwan, G. Robbers, T. Dent, S. Steffen, L. Amendola, M. Baldi , N. Brouzakis , N. Tetradis, V. Pettorino, D. Mota, M. Neubert, T. Krueger

fixed point behaviour : apparent tuning

fixed point behaviour : apparent tuning

Cosmon coupling to atoms Tiny !!! n Substantially weaker than gravity. n Non-universal couplings

Cosmon coupling to atoms Tiny !!! n Substantially weaker than gravity. n Non-universal couplings bounded by tests of equivalence principle. n Universal coupling bounded by tests of Brans. Dicke parameter ω in solar system. n Only very small influence on cosmology. n

Cosmon coupling to Dark Matter Only bounded by cosmology n Substantial coupling possible n

Cosmon coupling to Dark Matter Only bounded by cosmology n Substantial coupling possible n Can modify scaling solution and late cosmology n Role in clustering of extended objects ? n L. Amendola

effective cosmological constant realistic value for α φt / M ≈ 276

effective cosmological constant realistic value for α φt / M ≈ 276

effective cosmological constant linked to neutrino mass realistic value α φt / M ≈

effective cosmological constant linked to neutrino mass realistic value α φt / M ≈ 276 : needed for neutrinos to become non-relativistic in recent past as required for observed mass range of neutrino masses φt / M : essentially determined by present neutrino mass adjustment of one dimensionless parameter in order to obtain for the present time the correct ratio between dark energy and neutrino energy density no fine tuning !

crossing time from matching between early solution and late solution

crossing time from matching between early solution and late solution

neutrino fluctuations n n n time when neutrinos become non – relativistic sets free

neutrino fluctuations n n n time when neutrinos become non – relativistic sets free streaming scale neutrino structures become nonlinear at z~1 for supercluster scales D. Mota , G. Robbers , V. Pettorino , … n stable neutrino-cosmon lumps exist N. Brouzakis , N. Tetradis , …

crossover to dark energy dominated universe starts at time when “neutrino force” becomes important

crossover to dark energy dominated universe starts at time when “neutrino force” becomes important for the evolution of the cosmon field

cosmological selection !

cosmological selection !