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~1 km Development of Telescopes for Extremely Energetic Neutrinos Steven W. Barwick, UC-Irvine ~1 km Development of Telescopes for Extremely Energetic Neutrinos Steven W. Barwick, UC-Irvine

Neutrino Telescopes: Agenda • 10 years of progress with optical Cherenkov Detectors • Extremely Neutrino Telescopes: Agenda • 10 years of progress with optical Cherenkov Detectors • Extremely Energetic Neutrinos - New Technologies Radio Cherenkov: ARIANNA Teraton -Petaton

PHOTONS: not deflected, but: reprocessed in sources, absorbed in IR (100 Te. V), and PHOTONS: not deflected, but: reprocessed in sources, absorbed in IR (100 Te. V), and CBR PROTONS: deflection in magnetic fields, GZK cutoff NEUTRINOS: not absorbed or deflected, hard to see

E 2 d. N/d. E (Ge. Vcm-2 s-1 sr-1) WB A. Silvestri, Ph. D E 2 d. N/d. E (Ge. Vcm-2 s-1 sr-1) WB A. Silvestri, Ph. D Dissertation, 2008 1997: Unlimited Opportunity Log 10(E [Ge. V])

2010 ~100 x improvement Auger x 3 ANITA AMANDA-UHE WB Log 10(E [Ge. V]) 2010 ~100 x improvement Auger x 3 ANITA AMANDA-UHE WB Log 10(E [Ge. V]) A. Silvestri, Ph. D Dissertation, 2008 E 2 d. N/d. E (Ge. Vcm-2 s-1 sr-1) 13 Years of Diffuse Progress

Excluded Excluding AGN Model Predictions for Diffuse Flux Normalization to x-ray or 1 -1000 Excluded Excluding AGN Model Predictions for Diffuse Flux Normalization to x-ray or 1 -1000 Me. V ’s overproduces neutrino flux

GZK neutrinios [ one of the most secure predictions in the field ] New GZK neutrinios [ one of the most secure predictions in the field ] New Technologies

Cosmogenic (or GZK) Neutrinos Predictions are secure: p + cmb -> n + + Cosmogenic (or GZK) Neutrinos Predictions are secure: p + cmb -> n + + n -> lower energy protons -> However, -Flux Calculations depend on: 1. 2. 3. 4. Elemental composition (p, Fe, mixed) Cosmology ( =0. 7) Injection Spectra, E- and Emax Evolution of sources with redshift, (1+z)m § Star formation, QSO, GRB, little or no

E d. N/d. E (cm-2 s-1 sr-1) GZK Model-Specific limits all) ITA AN -08 E d. N/d. E (cm-2 s-1 sr-1) GZK Model-Specific limits all) ITA AN -08 109 Ge. V Log 10(E [Ge. V])

Why Big Detectors? • • GZK Flux, (E~1018 e. V): 100 /km 2/yr Interaction Why Big Detectors? • • GZK Flux, (E~1018 e. V): 100 /km 2/yr Interaction Length, : 500 km Event Rate/km 3/yr = [ ] ~ 0. 2 Efficiency, livetime, nice if more than one So GZK detection requires > 10 km 3 (aperture > 60 km 3 sr) Note: ARIANNA has ~ 2400 km 3 sr

ARIANNA Sensitivity Greatly increases sensitivity to GZK in E=10181019 e. V ARIANNA Energy Res: ARIANNA Sensitivity Greatly increases sensitivity to GZK in E=10181019 e. V ARIANNA Energy Res: d. E/E~1, Angular Res: ~1 deg ARIANNA + ESS Flux: 40 events/yr

EHE Neutrinos Explore Higher Dimensions CC: sm ARIANNA-GZK ~100 sm For GZK E (Anchordoqui, EHE Neutrinos Explore Higher Dimensions CC: sm ARIANNA-GZK ~100 sm For GZK E (Anchordoqui, et al, hep-ph/0307228)

Neutrino Cross-Section A. Connolly, 2006 ARIANNA - 10 years GQRS [ ] = 0. Neutrino Cross-Section A. Connolly, 2006 ARIANNA - 10 years GQRS [ ] = 0. 24 If Nev = 400 If =0. 5 o If =2 GQRS 2 parameter fit: Normalization cross-section

New Techniques to Observe Cosmogenic Neutrinos Current Under Development Radio RICE, ANITA ARIANNA, ARA, New Techniques to Observe Cosmogenic Neutrinos Current Under Development Radio RICE, ANITA ARIANNA, ARA, Ice. Ray, SALSA, etc Air Shower Hi. Res, Auger TA, Auger N, OWL Acoustic SPATS, AMADEUS

Askaryan Radio Emission from SLAC beam in Ice Gorham, Barwick, et al. , astro-ph/0611008 Askaryan Radio Emission from SLAC beam in Ice Gorham, Barwick, et al. , astro-ph/0611008 Absolute RF power and frequency dependence confirmed Width of cherenkov cone and frequency dependence confirmed

31 x 31 array [30 km x 30 km] ARIANNA UCI, LBL, OSU, Wash. 31 x 31 array [30 km x 30 km] ARIANNA UCI, LBL, OSU, Wash. U, KU, UC-London, S. Korea Barwick, astro-ph/0610631 600 m 1 km

Satellite Image of Victoria Land Ross Ice Shelf Dry Valleys ~120 km wireless internet Satellite Image of Victoria Land Ross Ice Shelf Dry Valleys ~120 km wireless internet (2009) Ross Island Minna Bluff ARIANNA 2 30 x 30 km Ice Thickness ~600 m south

ARIANNA Advantages • Straightforward logistics – not far (~120 km) from main US science ARIANNA Advantages • Straightforward logistics – not far (~120 km) from main US science station – surface deployment (no drilling) • Excellent site properties – Protected from man-made noise – Remarkable attenuation length and reflectivity from bottom • Lightweight, robust technologies (so low $$) • Internet access 24/7 • Array is reconfigurable to follow science

ARIANNA Characteristics log(E ) e. V Peak response at “sweet spot” of GZK spectrum ARIANNA Characteristics log(E ) e. V Peak response at “sweet spot” of GZK spectrum Zenith Angle Nearly uniform response over the entire sky

Optimal Antenna Gain = 7 higher gain restricts viewing of reflected events but accesses Optimal Antenna Gain = 7 higher gain restricts viewing of reflected events but accesses lower energy cascades LPDA

Impact of firn ice on LPDA Antenna (not much, except at f<100 MHz) L. Impact of firn ice on LPDA Antenna (not much, except at f<100 MHz) L. Gerhardt, et al, NIMA, 2010

Time-domain is rich in information on-cone -10 Time(ns) off-cone 10 -10 Time(ns) J. Alvarez-Muniz, Time-domain is rich in information on-cone -10 Time(ns) off-cone 10 -10 Time(ns) J. Alvarez-Muniz, A. Romero-Wolf, and E. Zas, ar. Xiv: 1002. 3873 v 1 10

Modification by antenna+amp Interesting structure, well suited to pattern trigger Similar pulse structure for Modification by antenna+amp Interesting structure, well suited to pattern trigger Similar pulse structure for oncone and off-cone Time(ns)

Camping at Moore’s Bay Site David Saltzberg Camping at Moore’s Bay Site David Saltzberg

ARIANNA Site Studies T. Barrella, et al, J. Glaciology, 2010, submitted Arbitrary amplitude scaling ARIANNA Site Studies T. Barrella, et al, J. Glaciology, 2010, submitted Arbitrary amplitude scaling Preliminary Value assumed prior to this work Amazing fidelity of reflected pulse from sea-water bottom -behaves as nearly flawless mirror 1 -way attenuation length, averaged over depth and temperature And Radio Quiet!

L. Gerhardt, et al, NIMA, 2010 ARIANNA Prototype Station (deployed Dec. 2009) “lab” Power L. Gerhardt, et al, NIMA, 2010 ARIANNA Prototype Station (deployed Dec. 2009) “lab” Power Tower Wireless

Housekeeping Data Outside Temp windy Wind speed Power Supply Voltage Jan 1, 2010 Feb Housekeeping Data Outside Temp windy Wind speed Power Supply Voltage Jan 1, 2010 Feb 4, 2010

Trigger rates ~ 10 -2 s-1 Randomly distributed in time Trigger: 2 of 3 Trigger rates ~ 10 -2 s-1 Randomly distributed in time Trigger: 2 of 3 majority, 5*Vrms

Prelim. Event Analysis (Jan 5 -Feb 4, 2010) No events in signal region Prelim. Event Analysis (Jan 5 -Feb 4, 2010) No events in signal region

ARIANNA Visualization ARIANNA Visualization

Outlook • To probe the GZK neutrino fluxes and particle physics at highest energies, Outlook • To probe the GZK neutrino fluxes and particle physics at highest energies, new techniques are being developed based on radio cherenkov , air shower and acoustic detection. • ARIANNA has the right combination of size and simplicity of deployment to keep costs down – Ice studies in Nov’ 06 astonishingly good – Recent protostation studies show low Anthropogenic noise over 1 month periods • 7 -station engineering array approved by NSF in April 2010

Air Shower vs Ice Shower (time profiles quite different!) 100 MHz-1 GHz Air Shower vs Ice Shower (time profiles quite different!) 100 MHz-1 GHz

L. Gerhardt, et al, NIMA, 2010 Electronic Module Schematics L. Gerhardt, et al, NIMA, 2010 Electronic Module Schematics

Solar Panel Power Electronic Module Solar Panel Power Electronic Module