Title: ARIANNA: Searching for Extremely Energetic Neutrinos
1ARIANNA Searching for Extremely Energetic
Neutrinos
- Lisa Gerhardt
- Lawrence Berkeley National Laboratory
University of California, Berkeley - NSD Monday Morning Meeting
- November 23, 2009
2Cosmic Rays
Energetic nuclei create massive showers when the
slam into our atmosphere Spectrum falls as
E-2.7 From galactic and extra-galactic sources
IndirectMeasurements
Direct Measurements
LHC
RHIC
3The Most Energetic in the World
1 particle/(km2yr) Need a massive detector to
see highest energy cosmic rays Auger 3000 km2,
seen O(100) cosmic rays with E gt
4 x 1019 eV since 2004
4Highest Energy CRs Are Protons?
Centaurus-A Closest AGN (2 events)
- Auger sees a correlation between the direction of
CR events with E gt 6 x 1019 eV and AGNs within 75
Megaparsecs away (244 million light years) - Suggests these CRs must be protons
5Or Not
But other observables are consistent with a
mixed composition, in disagreement with AGN
coincidence results.
Turn towards heavier composition
6Neutrinos from CRs
- Only 100 CRs seen ever with energy above 4 x
1019 eV - Flux falls E-3
- At these energies cosmic microwave
- background photons look pretty tasty
- Further reduces flux, but produces neutrinos via
? decay - Called GZK or cosmogenic neutrinos, E? gt 1017
eV
7Guaranteed Neutrinos
- CMB flux and p? interaction cross section are
well known - Flux of GZK neutrinos depends on the composition
of the CRs - And evolution of the universe
- A lot of interesting potential,
- but a really low flux
8Need a Big Detector
Current Limits
- GZK Flux 10/km2/yr
- interaction length 500 km
- Event rate (per km3yr) 0.02
- Only see half the sky 0.01
Expected Flux Band
Need O(100 km3) detector and gt5 years to see 10
events
9Towards a GZK Neutrino Detector
- Instrumenting 100 km3 for optical neutrino
detection is prohibitively expensive - IceCube 1km3 cost 300 million
- Seeing GZK neutrinos requires
- Clear signal emission (large S/N)
- Large natural medium with a long attenuation
length - Ice, sand
- Radio detection of neutrinos satisfies both
10Radio Signals From Cascades Askaryans Idea
?
- GZK neutrino interaction will produce an
electron-gamma shower - Shower in matter will be 20 more electrons than
positrons - ? e-(atom) ? ? e- e e- ? ? ?
- Excess charge moving faster than c in medium
emits Cherenkov radiation
11Askaryans Idea Cont
Zas, Halzen, and Stanev PRD 45362 (1992)
- Cherenkov radiation will add coherently if
- ? gtgt Lshower
- In dense material Lshower 10 cm
- At optical wavelengths (400 nm) ? ltlt Lshower
Power ? Nelec - At radio wavelengths (gtm) ? gtgt Lshower
- Power ? (Nelec)2
12Observations of Askaryan Effect
- Used beamline at SLAC
- 109 electrons at 28.5 GeV
- Total shower energy 3 x 1019 eV
e-
Ten tons of high quality carving ice Hand chipped!
ANITA Radio telescope
PRL 99171101 (2007)
13Coherent Emission Measured
Coherent radiation
PRL 99171101 (2007)
Power ? E2 Good agreement with predictions for
ice, salt, and sand
14GZK Neutrino Detection Requirements
- Clear signal emission (large S/N)
- Power ? E2
- Excellent for GZK ? Egt1018 eV
- Large natural medium with a long attenuation
length - Ice is a strong candidate
15Ross Ice Shelf
- 650 m thick ice sheet over Ross Sea
- 800 km across, roughly the size of Texas
- Near McMurdo Station, so easy to get to
- Used ANITA antennas to measure attenuation
- length and reflection from ice/sea water
interface
16On the Shelf
Cold Scientist (David Saltzberg)
Horn Antennas
Tent!
Ingenious Use of Natural Building Materials
17Ice/Sea Mirror
- Nice reflection of radio waves seen at ice/water
interface - lt3 dB loss measured
- Attenuation length 350 m
- Conservative, assumes no loss at reflection
- Anthropogenic background is very low
- A few flights over in the summer
Arbitrary Amplitude Scaling
18GZK Neutrino Detection Requirements
- Clear signal emission (large S/N)
- Power ? E2
- Excellent for GZK ? Egt1018 eV
- Large natural medium with a long attenuation
length - Ice, sand
19Radio Neutrino Experiments
- GLUE, LOFAR, look for neutrinos skimming the
surface of the Moon - High energy threshold (gt1020 eV)
- FORTE satellite that looks for neutrino
interactions in Greenland - ANITA balloon circled the South Pole for 45
days - RICE Radio antenna buried in the South Pole
amongst AMANDA (optical ? detector)
20Existing Limits
Moon and balloon far from active volume. Requires
a high neutrino energy to see signal.
21ARIANNA
- Designed to fill in gap between optical and
balloon neutrino detectors - Surface deployment on Ross Ice Shelf
- Antennas buried 1 m in the ice, listen for
neutrinos below - Placement in active volume gains 2-3 decades in
lower energy range - Takes advantage of ice/water reflection
- Allows surface detectors to see the downgoing GZK
neutrinos - Greatly increases visible solid angle
- Surface deployment is much cheaper than in-ice
(drilling, etc.)
22ARIANNA Array
- Each station will have 8 antennas
- Allow resolution of GZK neutrino direction
- Ultimate plan is to have 10,000 stations on 300 m
a grid 1000 km3 viewing volume - Total cost comparable to IceCube (1 km3) array
23ARIANNA Sensitivity
Estimated sensitivity of full ARIANNA array
ARIANNA energy range an excellent match for GZK
signal. Expect O(100) events/year.
24Prototype Station
- Field camp this Austral summer to test prototype
station - Hybrid hardware Previous ANITA hardware and LBNL
developed upgrades - S. Klein and T. Stezelberger depart on 11/28/09
with prototype - Verify attenuation lengths and reflection
- Test antenna behavior in snow
Picture from a previous deployment
25Conclusion
- GZK neutrinos offer insight into the composition
of the highest energy CRs and the evolution of
the universe - GZK neutrino interactions emit radio signals
which scale with neutrino energy and can be heard
over long distances - ARIANNA proposed to use excellent ice/water radio
reflection of the Ross ice shelf to look for GZK
neutrinos - Prototype station testing begins next week
- Spencer and Thorsten Good luck and stay warm
26(No Transcript)
27Why Neutrinos?
- Protons are bent by the magnetic field of the
galaxy - Photons and protons can be absorbed by
intervening objects and will annihilate with CMB - Neutrinos are the only particles that can reach
us from distant energetic objects
28Anatomy of a CR Shower
- Very energetic nuclei that create showers of
charged leptons, hadrons and photons in the
atmosphere - Most energetic particles ever 3 x 1020
eV - 3 orders of magnitude higher than LHC
- Detect CRs through secondaries in their enormous
cascades - Use intricate simulation models to determine CR
composition and energy from these measurements