3 astrophysical measurements of neutrino mass

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3 astrophysical measurements of neutrino mass Neutrino mass will tend to wash out intermediate scale structure during galaxy formation. Thus the presence of such structure in the present day distributions of galaxies disfavours neutrino mass. The Z-burst model for the origin of supra-GZK cosmic rays requires a non-zero neutrino mass. See hep-ph/0308168 for a method based on supernova neutrinos observed around a gravitational lens. It only requires you to see supernova neutrinos around a gravitational lens. That shouldn’t be too hard…. and Mi xin g N e u t ri n o Mas s .. Imperial College/ ottingham Nov 17 ’04 Dave Wark

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Nottingham. 3 astrophysical measurements of neutrino mass. Nov 17 ’04. Neutrino Mass. …and Mixing. Dave Wark. Imperial College/RAL. - PowerPoint PPT Presentation

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Page 1: 3 astrophysical measurements of neutrino mass

3 astrophysical measurements of neutrino mass

• Neutrino mass will tend to wash out intermediate scale structure during galaxy formation. Thus the presence of such structure in the present day distributions of galaxies disfavours neutrino mass.

• The Z-burst model for the origin of supra-GZK cosmic rays requires a non-zero neutrino mass.

• See hep-ph/0308168 for a method based on supernova neutrinos observed around a gravitational lens. It only requires you to see supernova neutrinos around a gravitational lens. That shouldn’t be too hard….

…and M

ixin

g

Neutr

ino M

ass

..

Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 2: 3 astrophysical measurements of neutrino mass

2dF Galaxy Redshift Survey

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 3: 3 astrophysical measurements of neutrino mass

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 4: 3 astrophysical measurements of neutrino mass

P(k)=A kn T2(k)

Neutrino Free StreamingNeutrino Free Streaming

P(k)/P(k) = -8 P(k)/P(k) = -8 m (Hu et al. 1998)m (Hu et al. 1998)

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 5: 3 astrophysical measurements of neutrino mass

=0

=0.01=0.05

They derive m,tot < 1.8 eV

2dF

team

: ast

ro-p

h/02

0415

2

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 6: 3 astrophysical measurements of neutrino mass

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

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astro-ph/0302209

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Imperial College/RAL

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Dave Wark

Page 8: 3 astrophysical measurements of neutrino mass

astro-ph/0304237

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 9: 3 astrophysical measurements of neutrino mass

astro-ph/0306386

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark

Page 10: 3 astrophysical measurements of neutrino mass

Neutrino mass from Cosmology

Data Authors Mmi

2dFGRS Elgaroy et al. 02 < 1.8 eV

WMAP+2dF+… Spergel et al. 03 < 0.7 eV

WMAP+2dF Hannestad 03 < 1.0 eV

SDSS+WMAP Tegmark et al. 04 < 1.7 eV

WMAP+2dF+

SDSS

Crotty et al. 04 < 1.0 eV

Clusters +WMAP Allen et al. 04 0.56+0.30-0.26 eV

All upper limits 95% CL, but different assumed priors !All upper limits 95% CL, but different assumed priors ! Slide from Ofer Lahav

Page 11: 3 astrophysical measurements of neutrino mass

What does this mean for neutrino physics?

• Sensitivity is better than tritium, and currently comparable to 0 decay – but clearly at this time suffers from substantial model dependencies.

• Data improve with more MAP data, Planck, and the Sloan Digital Sky Survey, perhaps gaining another factor of 3-5 in potential sensitivity. (See astro-ph/0303344, which claims (m) = 0.15 eV from Planck alone, and eventually perhaps 0.04 eV from better CMBR measurements)

• What are the real model dependencies? Hubble parameter? Bias? What is a model-independent limit? Time will tell. Watch, or better yet, join in the fun.

• Real connection between particle physics and cosmology!

…and M

ixin

g

Neutr

ino M

ass

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Imperial College/RAL

NottinghamNov 17’04

Dave Wark