Neutrino detection Neutrino detection
Laura Rossetto Laura Rossetto
Follow–up questions
Follow–up questions
• Homestake experiment detection of solar ν
eemitted by the decay of
8B and
7Be in the Sun via the reaction
37Cl + ν
e
37Ar + e
–E
th= 0.814 MeV
• GALLEX and SAGE experiments detection of solar ν
evia the reaction
71Ga + ν
e
71Ge + e
–, E
th= 0.233 MeV
• GALLEX Gran Sasso laboratory, Italy, 1991–1997
30.3 tons of gallium as GaCl
3in an aqueous HCl solution
• SAGE Soviet–american Gallium Experiment, Baksan underground observatory, Caucasus
~ 50 tons of gallium
I – I – Explain how energy thresholds for neutrino Explain how energy thresholds for neutrino
detection depend on the absorbing medium detection depend on the absorbing medium
I – I – Explain how energy thresholds for neutrino Explain how energy thresholds for neutrino
detection depend on the absorbing medium detection depend on the absorbing medium
GALLEX, SAGE E
ν> 0.233 MeV
Homestake Homestake
E
ν> 0.814 MeV
• Because of the low energy threshold, the gallium experiments (GALLEX,
• At E > 10
17eV GZK neutrinos produced when cosmic ray protons
interact with the cosmic microwave background photons rate 1 event km
–3yr
–1• ν
µ+ N X + l leptons may propagate for 20 – 30 km before being detected in the optical Cherenkov array
II –
II – Describe radio detection of neutrinos Describe radio detection of neutrinos
ν
µ+ N X + l
hadronic shower π
+, π
–, π
0electromagnetic shower
electrons produce Cherenkov radio emission
radio spectrum
~ 100 MHz – 1 GHz
• RICE (Radio Ice Cherenkov Experiment)
16 antennas installed in the AMANDA part of IceCube peak sensitivity at 200 – 500 MHz
upper limit on the flux of high relativistic magnetic monopoles GZK neutrino detection limit set to E = 10
17eV
• ANITA (Antarctic Impulsive Transient Antenna)
balloon experiment which twice circled Antarctica at 35 – 37 km altitude radio range 200 – 1200 MHz
field of view = 1.5 · 10
6km
2 16 cosmic ray events of mean energy of 1.5 · 10
19eV
originating from the interaction of
II –
II – Describe radio detection of neutrinos Describe radio detection of neutrinos
• GLUE (Goldstone Lunar Ultrahigh energy neutrino Experiment) two radio telescopes separated by 22 km and linked by optic fiber search for microwave pulses ≤ 10 ns from the lunar regolith
such pulses would arise from subsurface electromagnetic cascades induced
by interactions of neutrinos in the lunar regolith, E
ν≥ 10
20eV
II –
II – Describe radio detection of neutrinos Describe radio detection of neutrinos
• other experiments at the South Pole: ARIANNA, IceRay, AURA 22 km
Earth Moon
III –
III – During one phase of operations, salt was added During one phase of operations, salt was added
to the heavy water in SNO. Why? to the heavy water in SNO. Why?
• In June 2001 about two tonnes of NaCl were added to the heavy water volume to give a concentration of 0.002 g(NaCl)/g(D
2O)
Neutral current reaction νx + D p + n + νx
IV –
IV – Why is a Cherenkov ring a ring and not a disk ? Why is a Cherenkov ring a ring and not a disk ?
θ θ
x
x = β · c · t β = v / c
cos θ = 1 / β · n
in water c / n < v < c
0.75 · c ≤ v < c
n = 1.33
β ≥ 0.75
β = 0.75 γ = 1.5
E
lim= ( γ – 1) m
0c
2~ 53 MeV
m
0c
2= 105.6 MeV for µ
Bibliography Bibliography
Articles:
• J.N. Abdurashitov et al., Measurement of the solar neutrino capture rate with gallium metal, arXiv:0901.2200v3, 2009
• J. Kiko, The GALLEX solar neutrino experiment at the Gran Sasso Underground Laboratory, Astrophysics and Space Science 228, 107–112, 1995
• R. Davis, A review of the Homestake Solar Neutrino Experiment, Prog. Particle Nuclear Physics 32, 13–32, 1994
• D.P. Hogan et al., Relative magnetic monopoles flux constraints from RICE, arXiv:0806.2129v2
• S. Hoover et al., Observation of ultra-high -nergy cosmic rays with the ANITA balloon-borne radio interferometer,
arXiv:1005.0035v2, 2010
• P.W. Gorham et al., Experimental limit on the cosmic diffuse ultrahigh energy neutrino flux,