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New Compact Low Energy Neutrino Source using Isotope Beta Decay
Mike Shaevitz - Columbia UniversityMike Shaevitz - Columbia University
Workshop on Low Threshold Detectors for Detection of Coherent Neutrino Scattering
Dec. 6-7, 2012Livermore Valley Open Campus, Livermore, California
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Overview
• High-power cyclotrons can be used to make an intense, compact neutrino source.
• Daedalus CP violation program using 800 MeV proton cyclotrons– High intensity DAR source of to complement long-baseline
neutrino oscillation program– Use NC coherent scattering to search for STERILE with DAR beam
• IsoDAR sterile neutrino experiment using a 60 MeV proton cyclotron– Cost effective, intense , compacte source from 8Li isotope decay.– Synergy with industrial interest in medical isotope production
• High intensity IsoDAR typee source could also be used for a neutral current coherent neutrino scattering experiment– Need to couple the IsoDAR source with a low threshold (~few keV)
10 to 1000 kg detector
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3DAEDALUS 800 MeV Cyclotron System (Under Development)
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H2+ Ion
Source
InjectorCyclotron(Resistive
Isochronous)
Ring Cyclotron(Superconducting)
“Isochronous cyclotron” where mag. field changes with radius,
but RF does not change with time. This can accelerate many bunches
at once.
DAR Target-Dump (about 6x6x9 m3)
IsoDARCyclotron
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Submitted to NIM
Columbia, Huddersfield, IBA, Maryland, MIT,PSI, INFN-Catania, INFN –Legnaro, RIKEN, Wisconsin
Academics: Neutrino Physicists, Accelerator PhysicistsAnd also Scientists at a Corporation
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Ionsource Injector Superconducting
Ring CyclotronTarget/Dump
Phase I: The Ion Source
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source solenoidlens slits &
diagnostics
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7Beam to be characterized at Best Cyclotrons, Inc, VancouverThis winter (NSF funded)
Results to be available by Cyclotrons’13 Conference, Sept 2013, Vancouver
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Ionsource Injector Superconducting
Ring CyclotronTarget/Dump
We have a workable ion source for a Phase II
IsoDAR: A sterile neutrino experimentOn its own!
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Base Design Injector60 MeV/n @ 5 mA of H2
+
~1 mA p machines are madeBy industry (IBA, BEST)For isotope production
(That’s 10 mA of protons)
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Ionsource
Base DesignInjector
SuperconductingRing Cyclotron
Target/Dump
Phases III and IV
Establish the “standard” systemAnd the high-power system
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Our proposed 800 MeV cyclotronis very similar to theexisting Riken, Japan, cyclotron
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12Why Are We Developing These High Intensity Cyclotrons? To Make High Intensity Neutrino Sources
proton+
+
e+
High Intensity Cyclotron (~800 MeV protons)
e
e
Oscillations?
Dump
Decay-at-Rest(DAR) Beam
High Intensity Injector Cyclotron (60 MeV protons)
p(60 MeV) 9Be / 7Li (shielding) Lots of 8Li 8Li 8Be + e +e
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Daedalus CP Violation Programin Combination with Longbaseline Neutrino Exps
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14Long-Baseline Neutrino Experiment (LBNE)(Being set up to measure the mass hierarchy and CP violation)
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Phase 1: 700kW beam with 10kton LiqArgon Detector on surface (data in ~2023)Phase 2: >1MW beam with >20kton LiqArgon Detector underground
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Long Baseline experiments are usually low in antineutrino statistics due to lower production and cross section
… and the backgrounds are significant compared to signal plus the antineutrino beam has neutrino contamination
Main Limitation of LBNE Approach
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16DAEALUS Experiment: Antineutrino Source for CP Measurements
proton+
+
e+
High Intensity Cyclotron (~800 MeV KE proton)
e
e
Oscillations?
Dump
5MW 2MW 1MW
( Described in: Conrad/Shaevitz, PRL104,141802 (2010), Alonso et al., arXiv:1006.0260 [physics.ins-det] and 1008.4967 [hep-ex] )
• Combine:– High statistics
DaealusAntineutrinos e
– High statisticsLongbaselineNeutrinos e
Single Ultra-large DetectorWith Free Protons as Targets(Oil or Water) plusMultiple-baselines fromcyclotron sources.
Oil orWater
Decay-at-Rest(DAR) Beam
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Using Cyclotron Neutrino Sources to Search for Sterile Neutrinos
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Possible Oscillations to/thru Sterile Neutrinos
• Several hints for neutrino oscillations with large m2 ~ 1 eV2
– Cannot be explained with the 3 standard neutrinos (e, , ), since already have two m2 value at 2.510-3 and 7.610-5 eV2
– And there are strong constraints that there are only 3 neutrinos with normal weak interactions
Need a new type of neutrino that does not interact weakly and therefore is “sterile”
• Sterile neutrinos– Have no weak interactions (through the standard W/Z bosons)– Would be produced and decay through mixing with the standard
model neutrinos– Can affect oscillations through this mixing
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LSND and MiniBooNE Indications ofe Appearance
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e
MiniBooNEAllowed Regions
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20e Disappearance Has Maybe Been Observed? Reactor Antineutrino Anomaly
At least three alternatives: Wrong prediction of ν-spectra ? Bias in all experiments ? New physics at short baselines: Mixing with 4th ν-state
Red: 3 sin2(2θ13) = 0.15Blue: 4 ∆m2
new ≫ 2 eV2 and sin2(2θnew)=0.12, with sin2(2θ13) = 0.085arXiv: 1204.5379
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Current ReactorExperiments
Older ReactorExps at Close DistancesR = 0.927 0.023 (3.0 )
Region to Explorefor Sterile Neutrinos
3
4
e s ? RE
NO
Day
a B
ay
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Many Ideas for Future Experiments
• Establishing the existence of sterile neutrinos would be a major result for particle physics but …..
• Need definitive experiments– Significance at the > 5 level– Observation of oscillatory behavior within detector
• The disappearance of neutrinos using the neutral current interactions is a strict probe of active-to-sterile oscillations.– Observation of oscillations for coherent NC scattering would
definitively establish the existence of sterile neutrinos.
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22Future Experimental Oscillation Proposals/Ideas
Type of Exp App/Disapp Osc Channel Experiments
Reactor Source Disapp e e
Nucifer, Ricochet, SCRAMM, NIST, Neutrino4, DANSS
Radioactive Sources Disapp e e
(e e)
Baksan, LENS, Borexino, SNO+, CeLAND, Daya-Bay
Isotope Source Disapp e e IsoDAR
Pion / Kaon Decay-at-Rest Source
Appearance & Disapp
e
e e
OscSNS, CLEAR, DAEALUS, KDAR
Accelerator using Pion Decay-in-Flight
Appearance & Disapp
e , e
, e e
MINOS+, MicroBooNE, LAr1kton+MicroBooNE, CERN SPS
Low-Energy -Factory
Appearance & Disapp
e ,e
, e e
STORM at Fermilab
()
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23Very-short Baseline Oscillation Experiments
• Can observe oscillatory behavior within the detector if neutrino source has small extent .– Look for a change in event rate as a function of position and
energy within the detector– Bin observed events in L/E (corrected for the 1/L2) to search
for oscillations
• Backgrounds produce fake events that do not show the oscillation L/E behavior and are easily separated from signal
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- Detector
1 / L2 flux rate modulated by Probosc =i2 2θ ⋅i2 2L/ E( )
- SourceRadioactive Source
orIsotope Source
orReactor Source
orProton into Dump Source
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Pion or Kaon Decay-at-Rest Neutrino Sources
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Decay-at-Rest (or Beam Dump) Neutrino Sources
Each + decay gives one , one e , and one with known energy spectrum
Decay-at-Rest gives isotropic neutrino source
~1 ma of 800 MeV protons (like LSND) 0.17 +/proton 2.3 1024 / yr
proton+
+
e+
Cyclotron or Other Proton Source ( >800 MeV proton for production)
e
e
Capturesbeforedecay
Appearance?
Dump
Disappearance?
e
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26Using Coherent Scattering with DAR Beam
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arXiv: 1201.3805
100kg 76Ge5yr
456kg 40Ar5yr
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IsoDAR Experiment
Isotope Decay-at-Rest Neutrino Source (e Disappearance )
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• High intensitye source using -decay at rest of 8Li isotope IsoDAR
• 8Li produced by high intensity (10ma) proton beam from 60 MeV cyclotron being developed as prototype injector for DAEALUS cyclotron system
• Put a cyclotron-isotope source near one of the large (kton size) liquid scintillator/water detectors such as KAMLAND, SNO+, Borexino, Super-K….
• Physics measurements: e disappearance measurement in the region of the LSND and reactor-
neutrino anomalies.– Measure oscillatory behavior within the detector.
IsoDARe Disappearance Exp
DetectorBlanket/Shield
Targetcyclotronprotons
Phys Rev Lett 109 141802 (2012) arXiv:1205.4419
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29IsoDAR Neutrino Source and Events
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arXiv:1205.4419
• p (60 MeV) + 9Be 8Li + 2p– plus many neutrons since low
binding energy
• n + 7Li (shielding) 8Li
• 8Li 8Be + e +e
– Meane energy = 6.5 MeV
– 2.61022e / yr
• Example detector: Kamland (900 t)– Use IBDe + p e+ + n process– Detector center 16m from source– ~160,000 IBD events / yr – 60 MeV protons @ 10ma rate– Observe changes in the IBD rate
as a function of L/E
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5 yrs
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IsoDAR e Disappearance Oscillation Sensitivity (3+1)
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5 yrs
e e
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IsoDAR’s high statistics and good L/E resolution gives good sensitivity to distinguish (3+1) and (3+2) oscillation models
Oscillation L/E Waves in IsoDAR
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5 yrs 5 yrs
Observed/Predicted event ratio vs L/E including energy and position smearing
e e
e e
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32Use IsoDARe Source for Coherent NC Measurement
• Cyclotron driven neutrino source from beta decay of isotopes produced in proton target/dump system– High intensity isotropic neutrino beam with well known spectrum
• Advantages:– About x2 higher energy than reactor neutrinos (but lower flux)– IsoDAR experimental site should offer a close, low-background location to
put a ~ton scale coherent scattering detector– Can turn off cyclotron to give measurement of non-beam backgrounds– Source size ~0.5m so might explore doing an oscillation search with
coherent scattering events.– Can vary distance with cyclotron beam to multiple sources– Can go deep to reduce cosmic backgrounds– Do dark matter searches during cyclotron-off periods
• Disadvantage:– To get needed rates, one needs to push the detection thresholds down to
the few keV range– High-intensity cyclotron needs to be developed
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Example Coherent Rates with 1ton LArgon with IsoDAR
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34Visible Energy Spectrum for LAr and LNe
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Integral = 690 eventsEthresh > 1keV
LAr @ 10m1ton for 1 yr
LNe @ 10m1ton for 1 yr
Ethresh > 1keV
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Visible Energy Spectrum for Ge Detectors
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475 events/yr EThresh > 20 eV
Ge @ 10m100kg for 1 yr
Ge @ 10m100kg for 1 yr
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Summary
• Cyclotron neutrino sources are an option for a number of neutrino measurements– CP violation studies using a DAR beam– Oscillation searches using a DAR beam with IBD events– Sterile neutrino searches using an IsoDAR type isotope decay
beams
• Coherent scattering studies are also possible with both the DAR and IsoDAR type beams– Measurements of the coherent scattering cross section– Use coherent scattering events to search for sterile neutrinos
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Backup
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An “isochronous cyclotron” design: magnetic field changes with radius Allowing multibunch acceleration
Use Cyclotrons to produce the 800 MeV protons!
Inexpensive,Only practical below ~1 GeV
(ok for us!)Only good if you don’t need short timing structure (ok!)Typically single energy (ok!)Taps into existing industry
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Engineering design,Assembly Plan,Structural analysis,Cryo system design
Engineering Study of Sector Magnet for the Daedalus Experiment,http://arxiv.org/abs/1209.4886
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40IsoDAR at Kamland
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41IsoDAR Measurement Sensitivity
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LBNE: Mass Hierarchy and CP Violation Sensitivity
• Phase I: 10 kton LiqAr surface detector at the Homestake site (Start 2023 with 5yr plus 5yr )
LBNE: 5yr + 5yrNova: 3yr + 3yrT2K: 6yr
LBNE: 5yr + 5yrNova: 3yr + 3yrT2K: 6yr
Mas
s H
iera
rchy
Det
erm
inat
ion
()
CP
Viol
atio
n D
isco
very
Pot
entia
l ()
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Example: 200kt Water Cherenkov + Daealus
0
1
2
3
4
5
6
-180 -135 -90 -45 0 45 90 135 180
CP
Sigificace (
_)
200k WC uoly +aealu (10yr)aealu oly 200 k (10yr)200k WC (5yr u + 5y uar)
i22θ13 = 0.10