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Published byOwen Webster Modified over 6 years ago
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Topics The case for remote radio detection of neutrinos
Overview (increasing remoteness) Balloon Satellite Telescope Not remote enough ANITA
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Cosmic rays since 1912 Flux Sources Neutrinos
Above GeV, steeply falling flux UHE large signals, starved for events Sources Acceleration: charged particles Propagation: still charged! dE/dx: interactions with CMBR: GZK threshold Magnetic deflection Neutrinos produced in source/propagation point back to source detect at EeV and above?
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Go Remote: aperture v threshold
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Overview of remote techniques
Telescope Satellite Balloon Remotish-ground operations
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Radio telescope observations of moon
Parkes GLUE (Goldstone) Kalyazin LUNASKA (Parkes/ACTA) nuMoon (WSRT) RESUN (EVLA) LOFAR SKA
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Prize for best drawing (Jeager, Mutel, Gayley)
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Overview of lunar cherenkov (JMG)
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Frequency, TIR, and Dq Scholten, etal
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frequency: aperture v threshold
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Fine … until compare to CR events: Jeong, Reno, Sarkevic
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Events
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CR 100x n – what to do separate n from CR? (spatially, by features (e.g. g-ray astronomy)) proximity of surface suppresses CR signal up rate dominates? return to high-f? true for orbiter, too. (LORD) (JRS) fluxes already nu-optimistic some science still OK? point sources cross-sections
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Lunar technique promising for CR
techniques going forward – see other talks ATCA: coherent addition of signals from several ants LOFAR: triggering(?) difficult for nu’s a lot of detail still to be done see ANITA list of details
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Satellites: Lunar sats …
Stal, etal
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LORD From “ARENA”
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FORTE (Lehtinen, etal.)
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PRIDE (Miller, etal.: Europa)
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BB radio detection of cosmic particles
Overview Neutrino detection event generation event simulation ANITA detector analysis results Cos-Ray detection Monopoles EVA
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Overview
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Neutrino detection Simulation Detector Operations Analysis
event generator event simulation Detector Operations Analysis calibration backgrounds reconstruction
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Neutrino interactions
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Cherenkov and Total Internal Reflection
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Aperture
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ANITA flight(s)
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Event Simulation Askaryan mechanism Determine list of sources
Signal Characteristics Determine list of sources For each source Determine launch angle via ray tracing Propagation effects Emission spectrum Spectrum at detector Sum spectra from sources
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Event ® source list CC events Better modeling of fluctuations
ne em + hadronic shower nt, nm brem/photonuclear ® secondary showers nt decay Better modeling of fluctuations multiple sub-showers Multiple paths reflection from bottom internal refraction (not for ANITA) Exotica Monopoles: quasi-continuous photonuclear
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Askaryan Frequency domain – linear response
ice attenuation velocity of propagation antenna, amps, filters (time domain for discriminators) Spectrum from Alvarez-Muniz, Zas, & Friends Could be improved.
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Scaling of Askaryan signals
R: Moliere radius L: Width of shower max Hadronic EM: LPM effect
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Askaryan
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Find launch angle (ray tracing)
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Propagation: Attenuation
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Propagation: Attenuation
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Propagation: focusing
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Propagation: birefringence
We don’t simulate this, but … dn/n ~ 10-3 is possible dt = 5 ns per km. Predict Hpol arrives first
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Cerenkov Beam
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ANITA detector Efficient data handling
Airframe and payload infrastructure Analog front end Antennas Low Noise Amps, filter, splitter Cables/connectors/boxes Trigger multistage, narrow dt: reduce accidentals Digitizer Low power switched capacitor array Efficient data handling
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ANITA Payload Weight Rigidity Form-factor Power Thermal Remote
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Front end: antennas
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RF subsystems (ANITA-I)
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Triggers
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Digitizing electronics (Anita-I)
Key component: Switched Capacitor Array (SCA) by G. Varner.
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Operations Campaign operations C3 NH preparations McMurdo Flight
Recovery Taylor Dome C3
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ANITA-View display
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Analysis Timing Calibration Interferometry Backgrounds
Thermal (reconstruction amplitude) Anthropogenic (clustering) I: 0 neutrino candidates II: 1 neutrino candidate Limits
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Calibration
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Interferometry
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Backgrounds
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Clustering
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Candidate events
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ANITA GZK flux limit Also – no news from GRBs
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Cosmic Ray Detection
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ANITA-I analysis Event selection Strong interference amplitude
14 below horizon 2 above Consistent waveforms w/reflection Correlated with B
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Air shower highlites 16 events in ANITA I
WaveForms: 2 direct, 14 reflected Tan(V/H) vs. B
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MC and Energy Scale exposure reflection w/roughness freq-spectrum
E-spectrum angular offset see Konstantin’s talk
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Magnetic Monopoles
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Worlds best limit for (relativistic) monopoles
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ANITA-III ANITA-III Fly 2013/14
Low resolution phased trigger (improve S/N) Dual triggers UHECR/UHEN More antennas
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ExaVolt Antenna (Gorham, etal - 1102.3883v2)
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Summary Remote techniques sacrifice threshold for aperture
Lunar observations hold promise for CR, but confirming a neutrino flux will be difficult Satellites ? Balloon borne radio detection provides large aperture at modest cost. Sensitive to GZK neutrinos. Constrain optimistic models, approaching baseline models. Detect UHE cosmic ray induced air showers at inclined angles. Energy scale still somewhat uncertain.
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extra slides
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Constant index of refraction
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Comparison – for discussion only (Dec 2009)
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