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Topics The case for remote radio detection of neutrinos

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Presentation on theme: "Topics The case for remote radio detection of neutrinos"— Presentation transcript:

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2 Topics The case for remote radio detection of neutrinos
Overview (increasing remoteness) Balloon Satellite Telescope Not remote enough ANITA

3 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?

4 Go Remote: aperture v threshold

5 Overview of remote techniques
Telescope Satellite Balloon Remotish-ground operations

6 Radio telescope observations of moon
Parkes GLUE (Goldstone) Kalyazin LUNASKA (Parkes/ACTA) nuMoon (WSRT) RESUN (EVLA) LOFAR SKA

7 Prize for best drawing (Jeager, Mutel, Gayley)

8 Overview of lunar cherenkov (JMG)

9 Frequency, TIR, and Dq Scholten, etal

10 frequency: aperture v threshold

11 Fine … until compare to CR events: Jeong, Reno, Sarkevic

12 Events

13 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

14 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

15 Satellites: Lunar sats …
Stal, etal

16 LORD From “ARENA”

17 FORTE (Lehtinen, etal.)

18 PRIDE (Miller, etal.: Europa)

19 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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21 Overview

22 Neutrino detection Simulation Detector Operations Analysis
event generator event simulation Detector Operations Analysis calibration backgrounds reconstruction

23 Neutrino interactions

24 Cherenkov and Total Internal Reflection

25 Aperture

26 ANITA flight(s)

27 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

28 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

29 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.

30 Scaling of Askaryan signals
R: Moliere radius L: Width of shower max Hadronic EM: LPM effect

31 Askaryan

32 Find launch angle (ray tracing)

33 Propagation: Attenuation

34 Propagation: Attenuation

35 Propagation: focusing

36 Propagation: birefringence
We don’t simulate this, but … dn/n ~ 10-3 is possible dt = 5 ns per km. Predict Hpol arrives first

37 Cerenkov Beam

38 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

39 ANITA Payload Weight Rigidity Form-factor Power Thermal Remote

40 Front end: antennas

41 RF subsystems (ANITA-I)

42 Triggers

43 Digitizing electronics (Anita-I)
Key component: Switched Capacitor Array (SCA) by G. Varner.

44 Operations Campaign operations C3 NH preparations McMurdo Flight
Recovery Taylor Dome C3

45 ANITA-View display

46 Analysis Timing Calibration Interferometry Backgrounds
Thermal (reconstruction amplitude) Anthropogenic (clustering) I: 0 neutrino candidates II: 1 neutrino candidate Limits

47 Calibration

48 Interferometry

49 Backgrounds

50 Clustering

51 Candidate events

52 ANITA GZK flux limit Also – no news from GRBs

53 Cosmic Ray Detection

54 ANITA-I analysis Event selection Strong interference amplitude
14 below horizon 2 above Consistent waveforms w/reflection Correlated with B

55 Air shower highlites 16 events in ANITA I
WaveForms: 2 direct, 14 reflected Tan(V/H) vs. B

56 MC and Energy Scale exposure reflection w/roughness freq-spectrum
E-spectrum angular offset see Konstantin’s talk

57 Magnetic Monopoles

58 Worlds best limit for (relativistic) monopoles

59 ANITA-III ANITA-III Fly 2013/14
Low resolution phased trigger (improve S/N) Dual triggers UHECR/UHEN More antennas

60 ExaVolt Antenna (Gorham, etal - 1102.3883v2)

61 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.

62 extra slides

63 Constant index of refraction

64 Comparison – for discussion only (Dec 2009)


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