the cmb and neutrinos. we can all measure the cmb t cmb =2.725 +\- 0.001 k cmb approx 1% of tv...

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The CMB and Neutrinos

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Page 1: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

The CMB and Neutrinos

Page 2: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

We can all measure the CMB

TCMB=2.725 +\- 0.001 K

CMB approx 1% of TV noise!

400 photons/cc at 0.28 eV/cc

Page 3: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

But no one has measured the neutrino background.

Page 4: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrinos

Tn=1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos.

113 neutrinos/cc/family

When I say “neutrinos”….

0.05 eV<Smn<2.3 eV (95%cl)From atmospheric neutrinos at SuperK , nm nt

Tritium end point plus mass splittings. (Kraus et al., 2005)

From particle physics:

Page 5: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrinos

Tn=1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos.

113 neutrinos/cc/family

0.05 eV<Smn<1.2 eV (95%cl)

WMAP aloneFrom atmospheric neutrinos at SuperK , nm nt

Page 6: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrinos

Tn=1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos.

113 neutrinos/cc/family

0.05 eV<Smn<0.58 eV (95%cl)From atmospheric neutrinos at SuperK , nm nt

WMAP+BAO+H0

Page 7: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrinos

Tn=1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos.

113 neutrinos/cc/family

0.05 eV<Smn<0.2 eV (95%cl)From atmospheric neutrinos at SuperK , nm nt

Expected from KATRIN (Franenkel, 2011)

Page 8: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrinos

Tn=1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos.

113 neutrinos/cc/family

0.05 eV<Smn<0.06 eV (~95%cl)From atmospheric neutrinos at SuperK , nm nt

From Planck plus fine scale CMB polarization measurements (ACT, SPT….)

Page 9: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Cosmic Evolution

Us

Decoupling at z=1030

Decoupling surface

Page 10: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Cosmic Evolution

Page 11: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Cosmic Evolution

Page 12: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Cosmic Evolution

At decoupling

Page 13: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

1972

Page 14: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

WMAP at 61 GHz, 0.5 cm

The CMB at decoupling as seen through a Lambda-dominated spacetime (and through our galaxy).

Page 15: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Angular Power

Fundamental mode

rarefaction compression

“Acoustic peaks”

Model

compression

Spectrum

Silk damping tail

Page 16: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

The Atacama Cosmology Telescope

~10X WMAP resolution

WMAP

Page 17: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

148

GH

z21

8 G

Hz

277

GH

z

Pulse Tube

4He Fridge

3He Fridge

40K Shield

3K Shield

Window

1 m

DetectorsOptics

The Millimeter Bolometric Array Camera

Page 18: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Preliminary Power Spectrum

Silk damping tail

Page 19: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Number of relativistic species, NeffDunkley et al., 2011

The key to limiting Neff is to identify the increased damping at small angular scales in the CMB.

Silk damping tail

Hou et al., 2011Bashinsky & Seljak, 2004Jungman, Kamionkowski, Kosowsky, Spergel 1996

Page 20: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neff

ACT+WMAP

ACT+WMAP+BAO+H0

Dunkley et al., 2011

WMAP

SPT+WMAP

SPT+WMAP+BAO+H0

Keisler et al., 2011

Komatsu et al., 2011

5.3 +/- 1.3

4.56 +/- 0.75

3.85 +/- 0.62

3.86 +/- 0.42

Page 21: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Compare today to that at decoupling. Greater relativistic means smaller rm/rr, enhanced potential evolution, and producing less cosmic structure.

Komatsu et al., 2009

e.g., Ichikawa et al., 2005

WMAP+BAO+SN, sum <0.58 (95%cl)

WMAP

Neutrino Mass #1

Page 22: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrino Mass #2

Use the cosmic structure between us and the surface of last

scattering to lens the CMB, especially the small angles where

a massive neutrino inhibits the formation of structure.

Lensing is characteristically sensitive to mn

Page 23: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

From Sudeep Das

Lensing smoothes out the peaks and alters the statistics of the CMB

Page 24: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Simulations

AAS, Jan 7 2010100 deg2

uK

Page 25: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

AAS, Jan 7 2010

Simulations

100 deg2

uK

Page 26: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Lensing of CMB detected at 4s

Based on Hu & Okamoto estimator plus phase randomization.

Shape sensitive to neutrino mass.

Page 27: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

And from SPT

van Engelen et al 2012

Page 28: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc
Page 29: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

“Geometric Degeneracy”

CMB alone tells us we are on the “geometric degeneracy” line

closed

open

Assume flatness

WMAP7 only best fit LCDM

{Wbh2 = 0.0226 +/- 0.00057Wch2 = 0.1109 +/- 0.0056 h = 0.710 +/- 0.025 s8 = 0.801 +/- 0.030 t = 0.088 +/- 0.015 ns = 0.963 +/- 0.014

Page 30: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

The Degeneracy

Sherwin et al. 2011

Page 31: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Lensing breaks the geometric degeneracy.

Lambda=0 excluded at 3.2 sigma from combination of WMAP and ACT.

Sherwin et al. 2011

Page 32: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Neutrino Mass #3

AAS, Jan 7 2010

Planck: sensitive to l=2000 in polarization

Can look through foregrounds in EE at l>2000.

Instruments & measurements underway by ACTPol, Polar, Polarbear, SPTPol.

Page 33: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Gravitational lensing turns E-modes into B-modes. Look for the effects of neutrinos in polarization.

Page 34: The CMB and Neutrinos. We can all measure the CMB T CMB =2.725 +\- 0.001 K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc

Thank You