stockholm, may 2-6, 2006 snow 20061 sub-mev solar neutrinos: experimental techniques and backgrounds...
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![Page 1: Stockholm, May 2-6, 2006 SNOW 20061 Sub-MeV solar neutrinos: experimental techniques and backgrounds Aldo Ianni Gran Sasso Laboratory, INFN](https://reader038.vdocuments.site/reader038/viewer/2022103022/56649d365503460f94a0e76f/html5/thumbnails/1.jpg)
Stockholm, May 2-6, 2006
SNOW 2006 1
Sub-MeV solar neutrinos: experimental techniques
and backgrounds
Aldo Ianni
Gran Sasso Laboratory, INFN
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Stockholm, May 2-6, 2006
SNOW 2006 2
Why do we need to measure sub-MeV solar neutrinos? Neutrino physics Astrophysics
How can they be observed? Upcoming:
100-ton scale ultra-pure organic Liquid Scintillator (high photon yield below 1 MeV)
Elastic Scattering Future:
liquid noble gases, metal loaded LS, TPC ES + Inverse Electron Capture
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Why?
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Only 0.01% of solar neutrino spectrum measured in real time
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SNOW 2006 5
Measurements vs unknowns
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MSW-LMA to explain observations
Transition of Pee
Obtained with SSM constraints!
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What do we want to measure and why do it?
( )
pep
ppBeeeppBe
ppBe
CC
ppBeppBe
eeppBe
eeppBe
ppBe
ES
f
Pf
fPPf
measure
Mmeasure/SS
1Mmeasure/SS
,,
,
,,,
,
,
⋅=
⋅−⋅+⋅= ρ
02.099.0 4.1L
L
0.0051.010 02.002.1
07.1 91.0
%)5(2.03.0
Be(5%)
05.007.0
Be(5%)24.062.0
±⏐⏐ →⏐=
±⏐⏐ →⏐±=
⏐⏐ →⏐=
+−
+−
+−
Be
pp
Be
f
f
γ
ν energieslow or middleat up showsmight
neutrino sterilelight a and qq , 0
as such physics standard Non
fl +→+≠ ννμν
astrophysics Neutrino physics
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How difficult is it going to be?
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• What detection channel
– ES: not a specific signature, better with Be and pep + asks for a ultra-pure Fiducial Mass
– CC: strong signature via inverse electron capture. Internal background may become less important
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Signatures and requirements for the ES channel
200 400 600 800 1000
75
80
85
90
95
100 SimulatedseasonalSignal+BackgroundinBOREXINO
S0=33counts?dayB=50counts?day
timeHdaysL
stnuoc
?yad
?001
not
0 20 40 60 80 100 120 140
1
2
3
4
5
6
3s level
5yr
3yr
2yr
BackgroundHevents?dayLC.L.
Hs
L10-16g/g
With U,Th at 10-16 g/g and 40K at 10-14 g/g• internal backg. ~ 20 cpd/100 tonsin [0.25,0.8]MeV
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• ES + Ultra-pure liquid scintillators
– First thoughts/tests ~1988 to address radiopurity issues • High photon yield (104 /MeV) allows to perform spectroscopic
measurements• SSM predicts ~ 0.5 cpd/ton for Be with ES => 100t FM
– Borexino a pioneer experiment with a 4-ton prototype showed (1997):
• that 238U and 232Th can be below or on the order of 10-16 g/g (~10-6Bq/ton)• that 14C/12C ~ 10-18 allows to set a thereshold at 250 keV for ES• that self-shielding design works with organic scintillator ( ~ 1 g/cm3) to reduce external background
– KamLAND (2002) with a 500 ton-scale mass has measured 238U and 232Th at the level of 10-17-10-18 g/g => pep meas. opportunity
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Beyond U and Th
Asking for 1cpd/100tons
[0.1 μBq/m3 PC] it implies:• System sealed against 222Rn
~10-5Bq/ton
• 0.4 ppm 39Ar in N2
• 0.2 ppt 85Kr in N2
210Pb and 210Po are often found not in equlibriumdue to a different chemistry
All spectra normalized to 1
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Removing/Reducing 210Bi, 210Po, 85Kr, 39Ar• High level of cleanliness • Purification of scintillator
– Distillation (thought to be the best method on the basis of small set-up tests)
– Water extraction– High level nitrogen sparging
Beyond U and Th
Check radioisotope impurities before filling!
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What about pep neutrinos?
• Cosmogenic background: 11C• Possible 11C background
reduction by tagging the sequence (in Borexino and KamLAND): muon + neutron capture + 11C decay [see Galbiati et al, PRC, 71, 055805 (2005)]
• Method already tested with Borexino prototype [see hep-ex/0601035 ]
• SNO+ main goal due to SNOlab depth
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Reduction of background for pep neutrinos
Cylindrical cut Around muon-track
Spherical cut around⏐neutron capture vertex to reject 11C event correlated in time and space
Neutron production
vertex
Muon going through
In 95% of cases a neutron is produced together with a 11CSignal/Noise as large as 2 with only 3% of data rejected @ Gran Sasso
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11C tagged with the Borexino prototype
Taken from Borexino coll. hep-ex/0601035
11C decays + with Q~1MeV and min Measured production rate ~0.14 events/day/ton at Gran Sasso depth
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Backgrounds for pep besides U,Th,11C
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Next generation projects
Goals• real-time observation of pp (CC/ES)• real-time observation of Be with a CC channel
ProjectsXMASS : LXe, ESCLEAN : LNe, ES(see D. McKinsey this workshop)
MOON : 100Mo CCLENS : 115In CC
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Liquid Xe [XMASS]• Multi-purpose detector• Channel: ES• No 14C!• Target: 23t [10t FV] of LXe• Design: use of 30cm self-
shielding ( = 3.06 g/cm3)• Backgrounds (main tasks):
– 85Kr: to be reduced to 4x10-15g/g from 10ppm (by distillation)
– 136Xe 0ν: isotope separation (<1/100 of natural)
• 100kg(NOW)->1E3->1E4
2.5 m
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LENS SneIne115115 s]4.5 [delayed, 2 [prompt] +=+→+ − μγν
•115In abundance = 95.7%•Threshold of capture = 0.114 MeV•B(GT) = 0.17 [precise measurement with neutrino source in TF]•LS stability tested : > 2yr•Backgrounds:
decay of 115In + following Bremsstrahlung
Multiple In decay •Desing: high segmentation with 125t on LS [10t of In]
~4% pp meas. in 5yr
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MOON• Multi-purpose detector [0ν, supernova ν’s]• Channel: inverse e- capture (prompt) + delayed b decay•Threshold of capture = 0.168 MeV•(gA/gV)2 B(GT) = 0.52±0.06•Backgrounds:
• U,Th at 10-3 Bq/ton • 214Pb->214Bi->214Po•2ν•Surface contamination
•Design: •3.3ton 100Mo •module 6m x 6m x 5m•Mo foils 0.05 g/cm2
•x, y reading with scintillators•~10-9 spatial resolution required
•Signal: • pp: ~337 events/yr/3.3tons•Be: ~167 events/yr/3.3tons
•Test Facility in operation since April 2005 @ Oto underground lab.
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Conclusions• It is great opportunity to measure low energy
solar neutrinos• First thoughts: 1988!• When: Borexino and KamLAND->2007• 10% Be meas. [5%] gives 10%Be,1%pp [5%Be,0.5%pp]• New goal: pep neutrinos. Precise meas. @
SNO+• Complementary projects under-way >=2010(?)
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From Galbiati et al, PRC, 71, 055805 (2005)
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From Galbiati et al, PRC, 71, 055805 (2005)
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From Galbiati et al, PRC, 71, 055805 (2005)
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From Galbiati et al, PRC, 71, 055805 (2005)
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He Ne Ar Kr XeA 2 10 18 36 54
Ion. Potent. (eV)
24.6 21.6 15.7 14 12.1
Boiling point (K)
4.2 27 87 119.8 165
p.e./MeV 4E4 4E4 4.3E4
long lived isotopes
39Ar,42Ar 85Kr
Density (g/cm3)
0.125 1.2 1.4 2.6 3.06
Rad. Length (cm)
756 24 14 2.4
From hep-ph/0008296
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800kg detector
10 ton detector
~ 30cm~ 80cm
~ 2.5m
R&DDark Matter Search
Multipurpose Detector
(DM, Solar Neutrino, )
With light guide
XMASS Program with LXe
100kg Prototype
M. Nakahata
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General Properties
νx+ e- → νx+ e- in 22 tonnes Helium
Ultra-pure (superfluid self-cleaning)
Scintillation + rotons or e-bubbles
Event discrimination
Position & energy reconstruction
ν
R. Lanou
Coded ApertureWafer Array
Progress
Frozen N2 + acrylic to replace graphite
moderator
Successful extraction of electrons from
drifted e-bubbles
… more powerful than rotons
Prospects
Technique & physics potential established
… Requires large scale prototyping