Cosmology(from(the( microwave( background( Jo(Dunkley( - - PowerPoint PPT Presentation

cosmology from the microwave background
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Cosmology(from(the( microwave( background( Jo(Dunkley( - - PowerPoint PPT Presentation

Cosmology(from(the( microwave( background( Jo(Dunkley( University(of(Oxford( Jo Dunkley History of early universe Inflation? T 10 15 GeV t 10 -35 s CDM decoupling? T 10 GeV? t 10 -8 s Neutrino decoupling T 1 MeV t


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Cosmology(from(the( microwave( background(

Jo(Dunkley( University(of(Oxford(

Jo Dunkley

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History of early universe

Inflation? T ∼ 1015 GeV t ∼ 10-35 s CDM decoupling? T ∼ 10 GeV? t ∼ 10-8 s Neutrino decoupling T ∼ 1 MeV t ∼ 1s Big Bang Nucleosynthesis T ∼ 100 keV t ∼ 10 min Matter-Radiation Equality T ∼ 0.8 eV t ∼ 60,000 yr Recombination T ∼ 0.3 eV t ∼ 380,000 yr Later: Neutrinos become ‘cold’ < t~100,000,000 yr

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z=1000, 380 000 yrs

t

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Seeds of structure

1. Inflation (?) imprints quantum fluctuations. 2. Space expands, regions enter into causal contact and start to evolve. 3. Coupled baryons and photons produce oscillations in plasma. After 380,000 years the fluctuations have evolved, and we see a snapshot

  • f them as anisotropies in CMB.

Linearity means we can use the anisotropies to infer the initial fluctuations and the contents of the Universe.

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Planck(Collaboration(2015

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100 GHz 143 GHz 217 GHz

Plus(6(other(wavelengths

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AQ

cmb

AU

cmb

−3 3 µK Stokes(vectors

largest(scales(removed

Planck(Collaboration(2015

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Q E U B

ACTPol maps, scale 15 uK, 10 degrees, Naess et al 2014

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ˆ φWF (Data) Lensing(potential,(phi

d) =  T(n + ∇φ) T(n) =

Planck(Collaboration(2015

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What(are(the(geometry,(contents,(and(initial(conditions(

  • f(the(Universe?(

What(happened(to(start(the(expansion?(Why?( What(are(the(properties(of(the(dark(sector?(

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Rough(description(of(CMB(analysis(process:( ‘Data’(((((=(maps(of(the(blackbody(sky((temp,(pol,(lensing)( Statistic(=(angular(power(spectrum(of(maps( Output(((=(cosmological(parameters((reliable(codes(
 (((((((((((((((((((((((((((((predict(their(theory(power(spectra)

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2 10 30 101 102 103 104

D`[µK2]

90 18 1000 2000 3000 4000

Multipole moment, `

Planck ACT SPT 1 0.2 0.1 0.07 0.05

Angular scale

Planck(Collaboration(2015

6Rparameter(LCDM(fits(extremely(well:(constraints(on(baryon,(CDM(and(Lambda(fractions,(and(size(

  • f(initial(fluctuations.(Relic(DM(density(Ωch2= 0.120 ± 0.003(

CMB(temperature

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20 40 60 80 100

CEE

`

[10−5 µK2]

Planck(Collaboration(2015

Greatly(limits(vast(zoo(of(alternatives(to(LCDM,(e.g.(

  • different(contents:(extra(relativistic(species,(early(dark(energy(
  • different(initial(fluctuations:(scale5dependent(power,(tensor(or(isocurvature(fluctuations(
  • extra(components:(cosmic(defects,(magnetic(fields(
  • non5standard(BBN(or(recombination(history,(dark(matter(annihilation

CMB(polarization((ERmode)

2000 30 500 1000 1500 2000

  • 4
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16

1 10 100 1000 10000 mχ[GeV] 10−27 10−26 10−25 10−24 10−23 feff σv [cm3 s−1]

Thermal relic Planck TT,TE,EE+lowP WMAP9 CVL Possible interpretations for: AMS-02/Fermi/Pamela Fermi GC

dE dtdV (z) = 2 g ρ2

critc2Ω2 c(1 + z)6pann(z),

(81) where pann is defined as pann(z) ⌘ f(z)hσ3i mχ , (82) the critical density of the Universe today, m is the mass of

Dark(Matter( annihilation

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50 100 150 200 250 300 350 400 0.0 0.4 0.8 1.2 1.6 [( + 1)]2 C

/2 [×107]

T only T + P 2 ]

Planck(Collaboration(2015

Lensing(limits(curvature(to(2%,(and(neutrino(mass(sum(to(0.7(eV.

CMB(lensing

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(1) Number(of(species:( (2) Neutrino(mass

Neutrino(properties(from(cosmology

Neff = 3.13 ± 0.32 Planck TT N 3 15 0 23 Planck TT

Planck(Collaboration(2015

X mν < 0.68 eV More species: longer radiation domination, suppress acoustic oscillations, anisotropic stress shifts peaks More mass: neutrinos switch from being relativistic (hot) to non-relativistic (cold) earlier. Hot neutrinos free-stream, reducing matter clustering and damping of photon-baryon oscillations compared to CDM.

0.018 0.020 0.022 0.024 0.026 ωb 1 2 3 4 5 6 7 8 Neff A v e r e t a l . ( 2 1 3 ) C

  • k

e e t a l . ( 2 1 4 ) Planck TT+lowP Planck TT+lowP+BAO Planck TT,TE,EE+lowP

X mν < 0.23 eV

2

Planck TT Planck TT Planck TT Planck TT

+(BAO

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In(next(decade:(measure(neutrino(mass?

Forecasted(errors:( 2015(((Planck(((+(BOSS(((((100(meV( 2017(((ACTPol((+(BOSS((((((60( 2019(((AdvACT(+(BOSS((((((40( 2021(((AdvACT(+(DESI(((((((20( 2020s(CMBRS4(+(DESI(((((((16

Aberzajian(et(al(2014

From(oscillation(expt,(minimum( mass(sum(=(60(meV.(

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Inflation(status(from(Planck

Planck Collaboration: Cosmological

100 500 1000 2000

Multipole moment

500 1000 1500

2D[mK2]

ns = 0.96 ns = 1.00

Planck(Collaboration(2014,(2015(

n<1 Universe(is(flat(to(0.5%,(fluctuations(are(super5horizon,(Gaussian(and(adiabatic

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Gravitational(waves

From(K(Story

˙ ˙ h

k + 2 ˙

a a ˙ h

k − k 2hk = 0

T

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Gravitational(waves

From(K(Story

˙ ˙ h

k + 2 ˙

a a ˙ h

k − k 2hk = 0

T

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New(limits(on(tensor(modes

φ2

0.95 0.96 0.97 0.98 0.99 1.00

ns

0.00 0.05 0.10 0.15 0.20 0.25

r0.002

N = 5 N = 6 Convex Concave

φ

Planck TT+lowP Planck TT+lowP+BKP +lensing+ext

50 100 150 200 250 300 −0.01 0.01 0.02 0.03 0.04 0.05 Multipole BKxBK (BKxBK−αBKxP)/(1−α)

Planck(Collaboration(2015 Planck/BICEP2(Collaborations(2015

BRmode(power

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10 30 100 300 1000

Frequency (GHz)

10

  • 1

10 10

1

10

2

RMS brightness temperature (µK)

CMB Thermal dust Synchrotron 30 44 70 100 143 217 353 Sum fg

Planck(Collaboration(2015
 (level(over(70R90%(of(sky)

Planck(gave(us(new(view(of(the(Galaxy

Until(Planck,(dust(level( uncertain(to(order%of% magnitude%

AP d

20 200 µKRJ @ 353 GHz

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Next:(CMBRS4(campaign(from(~2020R25( Now:(’StageR3’(CMB:(Spider,(PolarBear,(BICEP3,(Keck,(CLASS,(SPTR3G,(GroundBird( My(project((led(in(Princeton):(AdvACT(( Targeting(r=0.01(with(five(wavelengths(2016R18.

Path(ahead

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Cosmic(microwave(background(data(continue(to(demand( LCDM(cosmological(model.(It(holds(up(very(well(to(new(lensing( and(polarization(measurements(from(the(Planck(satellite.(

  • If(inflation(is(not(correct(scenario,(it(has(to(look(a(lot(like(

it.(Gravitational(wave(search(still(firmly(on.(

  • Neutrino(sector(holds(questions(that(cosmology(can(help(

answer(in(coming(decade.(