The effective number of neutrinos: standard and non-standard - - PowerPoint PPT Presentation

the effective number of neutrinos standard and non
SMART_READER_LITE
LIVE PREVIEW

The effective number of neutrinos: standard and non-standard - - PowerPoint PPT Presentation

The effective number of neutrinos: standard and non-standard scenarios Pablo Fernndez de Salas IFIC CSIC / Universitat de Valncia 28th Texas Symposium on Relativistic Astrophysics Geneva 15th December 2015 Radiation-dominated epoch


slide-1
SLIDE 1

The effective number of neutrinos: standard and non-standard scenarios

Pablo Fernández de Salas

IFIC – CSIC / Universitat de València

28th Texas Symposium on Relativistic Astrophysics Geneva – 15th December 2015

slide-2
SLIDE 2

Radiation-dominated epoch of the universe

The universe has passed through epochs of domination of different components

slide-3
SLIDE 3

Radiation-dominated epoch of the universe

The universe has passed through epochs of domination of different components During the radiation-dominated era

slide-4
SLIDE 4

Radiation-dominated epoch of the universe

The universe has passed through epochs of domination of different components During the radiation-dominated era

slide-5
SLIDE 5

Neutrino decoupling and e e annihilations ⁺ ⁻

Instantaneous decoupling approximation: 1) Neutrinos decouple completely 2) e⁺e⁻ annihilate

slide-6
SLIDE 6

Neutrino decoupling and e e annihilations ⁺ ⁻

Beyond the Instantaneous decoupling approximation:

  • Neutrino decoupling and e⁺e⁻ annihilations were not

fully disconnected

  • After e⁺e⁻ annihilations: &
slide-7
SLIDE 7

Effective number of neutrinos

Neff accounts for any contribution to radiation other than photons Another definition Standard scenario: only neutrinos → Neff ≈ 3 Measured value: Neff = 3.04 ± 0.18 (68% C.L.) Planck TT,TE,EE+lowP+BAO

slide-8
SLIDE 8

Deviation from Neff = 3 due only to neutrinos

  • Neutrino decoupling is not complete when e e annihilate

⁺ ⁻

  • Finite temperature QED corrections
  • Non-Standard neutrino-electron Interactions (NSI)
  • Very Low-Reheating scenarios (Neff < 3)
slide-9
SLIDE 9

Finite temperature QED corrections

  • Particles are in a thermal bath with a temperature T
  • Photons and electrons acquire an additional effective mass
slide-10
SLIDE 10

Neutrino decoupling not complete when e± annihilate

  • Interactions with e and e

⁻ ⁺

  • Neutrino oscillations
  • Neutrino self-interactions

Main source of deviation Also important

→ Deviation of fν from equilibrium

slide-11
SLIDE 11

Neutrino decoupling not complete when e± annihilate

Density matrix formalism Solve Boltzmann equations with Icoll ≠ 0

→ Computing the deviation from equilibrium

slide-12
SLIDE 12

Neutrino decoupling not complete when e± annihilate

  • Reduce analytically from 9 to 2 integrals
  • Solve numerically with a grid on the incoming neutrino momentum
  • We do not consider damping factors

for the off-diagonal terms of the density matrix When oscillations are added we need to solve 9 collision integrals, one for each real entry of the density matrix

→ Collision integrals treatment

slide-13
SLIDE 13

Neutrino decoupling not complete when e± annihilate

  • Reduce analytically from 9 to 2 integrals
  • Solve numerically with a grid on the incoming neutrino momentum
  • We do not consider damping factors

for the off-diagonal terms of the density matrix When oscillations are added we need to solve 9 collision integrals, one for each real entry of the density matrix

→ Collision integrals treatment

Neff = 3.044

slide-14
SLIDE 14

Non-Standard neutrino-electron Interactions

D.V. Forero & M.M. Guzzo (2011)

3.040 ≤ Neff ≤ 3.059

slide-15
SLIDE 15

Very Low-Reheating scenarios

The last radiation-dominated era of the universe usually arises from the decaying of a massive particle, a process known as reheating This affects their contribution to the radiation content of the universe In the specific scenario where the so-called reheating temperature is as low as

TRH ~ few MeV, neutrinos do not have

time to thermalize.

Standard case: Neff = 3.046

  • P. F. de Salas et al (2015)

PRD in press (arXiv:1511.00672)

slide-16
SLIDE 16

Very Low-Reheating scenarios

  • We assume a massive particle

ϕ decaying into relativistic particles

  • ther than neutrinos
  • Neutrinos will be populated via weak

interactions with charged leptons

→ Neutrino production in LR scenarios

  • P. F. de Salas et al (2015)

PRD in press (arXiv:1511.00672)

slide-17
SLIDE 17

Conclusions and results

Low-Reheating scenarios → Bound from BBN (95% C.L.) Standard scenario → Neutrinos only Non-Standard Interaction (NSI) scenario → neutrino-electron NSI 3.040 ≤ Neff ≤ 3.059 Neff = 3.044 → Bound from CMB (95% C.L.)

No significant possible deviation from the standard case

Can be interpreted as

slide-18
SLIDE 18

Backup

slide-19
SLIDE 19
slide-20
SLIDE 20

Neff and Σmν simultaneous constraint

slide-21
SLIDE 21

Why not to consider damping factors

slide-22
SLIDE 22

Why not to consider damping factors

slide-23
SLIDE 23
slide-24
SLIDE 24
slide-25
SLIDE 25