Cosmic Ray Acceleration in Supernova Remanants Vladimir Ptuskin IZMIRAN, Russia
Supernova Watches and HALO
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Transcript of Supernova Watches and HALO
Supernova Watches and HALO
SNOLAB Grand Opening WorkshopMay 14-16, 2012
Clarence J. Virtue
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Supernova neutrinos –First order expectations Approximate equipartition of neutrino fluxes Several characteristic timescales for the phases of the explosion
(collapse, burst, accretion, cooling) Time-evolving νe, νe, ν”μ” luminosities reflecting aspects of SN dynamics
Presence of neutronization pulse Hardening of spectra through accretion phase then cooling
Fermi-Dirac thermal energy distributions characterized by a temperature, Tν, and pinching parameter, ην
Hierarchy and time-evolution of average energies at the neutrinosphere
T(ν”μ” ) > T(νe) > T(νe ) ν-ν scattering collective effects and MSW oscillations
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Put another way...An observed SN signal potentially has
information in its: The time evolution of the luminosities The time evolution of the average energies The values of the pinching parameters Deviation from the equiparition of fluxes Modifications of the above due to ν-ν scattering
collective effects and MSW oscillations
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What is to be learned? Astrophysics
Explosion mechanism Accretion process Black hole formation (cutoff) Presence of Spherical accretion shock instabilities (3D effect) Proto-neutron star EOS Microphysics and neutrino transport (neutrino temperatures and pinch
parameters) Nucleosynthesis of heavy elements
Particle Physics Normal or Inverted neutrino mass hierarchy, θ13
Presence of axions, exotic physics, or extra large dimensions (cooling rate) Etc.
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Opportunity to alert the astronomical community Through participation in a global network of neutrino
sensitive detectors - SNEWS Provide prompt and positive alert to astronomical
community in event of galactic SN in the event of a coincidence between experiments
Also provides machinery for an “INDIVIDUAL” announcement of SN by participating experiments
Design: Coincidence server(s) – 10 second UT time window Maximum rate of alarms is 1 per 10 days per experiment For 2-fold coincidence, 4 experiments < 1 false
alarm/century
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SNEWS – current configuration
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Alert to theAstronomicalCommunity
PGP signed e-mail
Bologna
RedundantSecure
CoincidenceServers
10 s window(UT time)
2-fold coincidence
SSL
SSL
SSL
SSL
Super-Kamiokande LVD
IceCubeBorexino
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PGP-signed e-mail
To amateur astronomersVia Sky & Telescope
Go to skyandtelscope.comto “subscribe to astroalert”
> 2000 subscribers
To neutrino physicistsand astronomers
Subscribe to receive analert at snews.bnl.gov
> 250 subscribers
Direct clients:- Gravitational wave detectors- Dark Matter detectors- Gamma-ray burst Coordinates Network (GCN)- etc.
• operating since March 23, 2004• live since March 30, 2006• all experiments sending automated alarms since April 17, 2006
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Super-Kamiokande 50 kton water
Cerenkov For 10 kpc SN
7000 IBD 410 NC on 16O 300 ES 4◦ pointing
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νe CC
NCES
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Large Volume Detector (LVD)
1000 tonne liquid scintillator with PMTs and limited streamer tubes
5 MeV threshold
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M. Selvi, arXiv:hep-ex/0608061v1
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5160 PMTs monitoring ~ 1 km3 of ice
~0.6 kt / PMT (~3Mt for SN)
Statistical increase in dark current / singles rate (20 σ at 30 kpc)
May 14, 2012
Astronomy and Astrophysics 535 (2011) A109
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Borexino Liquid scintillator (PC)
100 ton fiducial 300 ton viewed (SN)
For 10 kpc SN CC (IBD) 79 CC (12C) 5 NC (12C) 23 ES 5
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NC
νe CC ES
νe CCL. Cadonati et al., Astropart.Phys.16:361-372,2002
Includes~100νx + p
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Near future experiments Gadzooks! (S-K plus Gd)
For DSNB detection through tagged IBD MicroBoone (170 t LArTPC) 2014
SNEWS client (would buffer 1500 TB / ~30 minutes of data containing 17 SN events for 10 kpc SN)
ICARUS Noνa HALO SNO+May 14, 2012
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Generically, how do we detect a SN? We can instrument as large a mass as possible,
for as long as possible, and watch for a burst of the subtle effects of the SN neutrino’s weak interactions
We get to chose the target and the technology To date we’ve concentrated almost exclusively on
electrons, protons, and PMTs Some other “nuclear” targets are “along for the
ride” and only a few others seem worthy of consideration
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The ideal SN detector would... Be reliable
Target and detector would be stable and reliable for decades Low tech Good aging properties longevity
Be large and scalable Target and detector technology should be modular and
easily expanded Have large neutrino cross-sections
Very helpful, constrains shielding and costs Additionally, secondaries need sufficient mean free paths to
permit detection, constrains # readout channels and costs
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The ideal detector would... Have diverse sensitivities to different reaction channels and the
ability to tag those channels on an event-by-event basis Have a day job that does not conflict with supernova readiness Be able to measure the energy and direction of the SN neutrinos Have low background / noise levels above a threshold that
permits reliable SNEWS alerts from the far-side of the galaxy, or much further.
Be able to record the data without loss from the nearest conceivable SN
We don’t achieve all of this with any one technology!... But HALO fills a niche
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HALO - a Helium and Lead Observatory
“Helium” – because of the availability of the 3He neutron detectors from the final phase of SNO +“Lead” – because of high -Pb cross-sections, low n-capture cross-sections, complementary sensitivity to water Cerenkov and liquid scintillator SN detectors
HALO is using lead blocks from a decommissioned cosmic ray monitoring station
A “SN detector of opportunity” / An evolution of LAND – the Lead Astronomical Neutrino Detector, C.K. Hargrove et al., Astropart. Phys. 5 183, 1996.
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Comparative ν-nuclear cross-sections
Kate ScholbergSNOwGLoBES
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High Z increases νe CC cross-sections relative to νe CC and NC due to Coulomb enhancement.
CC and NC cross-sections are the largest of any reasonable material though thresholds are high ( CC-1n: 10.3 MeV, CC-2n: 18.4 MeV, NC-1n: 7.4 MeV, NC-2n: 14.1 MeV)
Neutron excess (N > Z) Pauli blocks
further suppressing the νe CC channel Results in flavour sensitivity complimentary to water
Cerenkov and liquid scintillator detectorsOther Advantages High Coulomb barrier no (α, n) Low neutron absorption cross-section (one of the
lowest in the table of the isotopes) a good medium for moderating neutrons down to epithermal energies
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Pb nuclear physics
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NC
νe CC
νe CC
ES
WaterCherenkov
NC
LiquidScintillator
LiquidArgon(needs updatingfor large θ13)
Lead
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NCNC
νe CC
νe CC
Iron
Flavour Sensitivities
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Goals to provide νe (dominantly) and νx sensitivity to the SN detection
community as soon as possible to build a long-term, high live-time dedicated supernova detector to explore the feasibility of scaling a lead-based detector to kt
mass
Philosophy Achieve these goals by keeping HALO
Very low cost Low maintenance Low impact in terms of lab resources
Goals and Philosophy
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Design Overview Lead Array (79 +/- 1% tonnes)
32 three meter long columns of annular Lead blocks
864 blocks total at 91kg each Neutron detectors
4 three meter long 3He detectors per column
384 meters total length 200 grams total 3He
Moderator HDPE tubing
Shielding (12 tonnes) 30 cm of water (5 sides) ~18 cm average PE (bottom)
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Supernova signal In 79 tonnes of lead for a SN @ 10kpc†,
Assuming FD distribution with T=8 MeV for μ’s, τ’s. 68 neutrons through e charged current channels
30 single neutrons 19 double neutrons (38 total)
20 neutrons through νx neutral current channels 8 single neutrons 6 double neutrons (12 total)
~ 88 neutrons liberated; ie. ~1.1 n/tonne of Pb†- cross-sections from Engel, McLaughlin, Volpe, Phys. Rev. D 67, 013005 (2003)
For HALO neutron detection efficiencies of 50% have been obtained in MC studies optimizing the detector geometry, the mass and location of neutron moderator, and enveloping the detector in a neutron reflector.
CC:
NC:
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HALO – March 2010
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Cutting apart welded sections from SNO installation and adding new endcaps. Six months of careful work!
3He neutron detectors
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4/5th of shielding in place
Cabling complete Readout complete HV on all channels and
full detector being read-out since May 8th 2012.
Upgrade of electronics pending
Calibration / characterization started
Plans shielding compete in
June Participate in SNEWS
by year end
Status today
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Signal and Backgrounds
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Preamp / ADC pairing with best resolution (left) Preamp / ADC pairing with best γ / n separation (right)
Performance
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A trigger condition of 6 neutrons in a 2 second window gives sensitivity out to ~20 kpc (for T=8 MeV for ”μ” )
Fast and thermal neutrons in SNOLAB occur at 4000 and 4100 neutrons/m2/day respectively
A background event rate of 150 mHz from all sources will randomly satisfy the trigger condition once per month. We take this as the target false alert rate for SNEWS (presently at 170 mHz with partial shielding)
Bulk α contamination in the CVD nickel tubes gives a negligible 22 +/- 1 events in neutron window per day for the whole array
(α, n) reactions not simulated in the HALO GEANT MC but the threshold in Pb is 15.2 MeV
Cosmic ray muon rate is < 2 per day. Rate of spallation events not yet calculated.
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Backgrounds and SNEWS
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Physics with HALO
K. ScholbergMarch 2012 APS
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Physics with HALO
K. ScholbergMarch 2012 APS
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HALO is effectively complete and continuous operation of the full detector began on May 8th providing sensitivity to the νe and νx components of a supernova
HALO will participate in SNEWS once the behaviour of the detector is well understood
Experience gained will feed into the design of a next generation detector taking advantage of the scalability of the lead plus neutron detector technology
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Summary
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With assistance this past year from: Kurt Nicholson – Guelph U. Axel Boeltzig – TU Dresden Ben Bellis, Leigh Schaefer, Zander Moss – Duke U. Victor Buza, Olivia Zigler – U. Minnesota Duluth Brian Redden – Armstrong Atlantic State U Thomas Corona – U. North Carolina Andre-Philippe Olds – Laurentian U.
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The HALO Collaboration
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