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Published byAlexander Morrison Modified over 9 years ago
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The CMB and Neutrinos
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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
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But no one has measured the neutrino background.
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Neutrinos T =1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos. 113 neutrinos/cc/family When I say “neutrinos”…. 0.05 eV < m < 2.3 eV (95%cl) From atmospheric neutrinos at SuperK, Tritium end point plus mass splittings. (Kraus et al., 2005) From particle physics:
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Neutrinos T =1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos. 113 neutrinos/cc/family 0.05 eV < m < 1.2 eV (95%cl) WMAP alone From atmospheric neutrinos at SuperK,
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Neutrinos T =1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos. 113 neutrinos/cc/family 0.05 eV < m < 0.58 eV (95%cl) From atmospheric neutrinos at SuperK, WMAP+BAO+H 0
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Neutrinos T =1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos. 113 neutrinos/cc/family 0.05 eV < m < 0.2 eV (95%cl) From atmospheric neutrinos at SuperK, Expected from KATRIN (Franenkel, 2011)
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Neutrinos T =1.945 K 3 known families, ~equal numbers of neutrinos and antineutrinos. 113 neutrinos/cc/family 0.05 eV < m < 0.06 eV (~95%cl) From atmospheric neutrinos at SuperK, From Planck plus fine scale CMB polarization measurements (ACT, SPT….)
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Cosmic Evolution Us Decoupling at z=1030 Decoupling surface
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Cosmic Evolution
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At decoupling
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1972
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WMAP at 61 GHz, 0.5 cm The CMB at decoupling as seen through a Lambda-dominated spacetime (and through our galaxy).
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Angular Power Fundamental mode rarefaction compression “Acoustic peaks” Model compression Spectrum Silk damping tail
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The Atacama Cosmology Telescope ~10X WMAP resolution WMAP
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148 GHz 218 GHz 277 GHz Pulse Tube 4 He Fridge 3 He Fridge 40K Shield 3K Shield Window 1 m Detectors Optics The Millimeter Bolometric Array Camera
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Preliminary Power Spectrum Silk damping tail
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Number of relativistic species, N eff Dunkley et al., 2011 The key to limiting N eff is to identify the increased damping at small angular scales in the CMB. Silk damping tail Hou et al., 2011 Bashinsky & Seljak, 2004 Jungman, Kamionkowski, Kosowsky, Spergel 1996
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N eff ACT+WMAP ACT+WMAP+BAO+H 0 Dunkley et al., 2011 WMAP SPT+WMAP SPT+WMAP+BAO+H 0 Keisler et al., 2011 Komatsu et al., 2011 5.3 +/- 1.3 4.56 +/- 0.75 3.85 +/- 0.62 3.86 +/- 0.42
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Compare today to that at decoupling. Greater relativistic means smaller m / r, 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
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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 m
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From Sudeep Das Lensing smoothes out the peaks and alters the statistics of the CMB
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Simulations AAS, Jan 7 2010 100 deg 2 uK
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AAS, Jan 7 2010 Simulations 100 deg 2 uK
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Lensing of CMB detected at 4 Based on Hu & Okamoto estimator plus phase randomization. Shape sensitive to neutrino mass.
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And from SPT van Engelen et al 2012
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“Geometric Degeneracy” CMB alone tells us we are on the “geometric degeneracy” line closed open Assume flatness WMAP7 only best fit LCDM { b h 2 = 0.0226 +/- 0.00057 c h 2 = 0.1109 +/- 0.0056 h = 0.710 +/- 0.025 8 = 0.801 +/- 0.030 = 0.088 +/- 0.015 n s = 0.963 +/- 0.014
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The Degeneracy Sherwin et al. 2011
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Lensing breaks the geometric degeneracy. Lambda=0 excluded at 3.2 sigma from combination of WMAP and ACT. Sherwin et al. 2011
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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.
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Gravitational lensing turns E-modes into B-modes. Look for the effects of neutrinos in polarization.
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Thank You
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