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International Summer School on Particle and Nuclear Astrophysics in Nijmegen 2003. An Improved Limit on the Muon Neutrino Mass from Pion Decay in Flight. NuMass Experiment. Carmen-Miruna An ă st ă soaie Alex Eduardo de Bernardini Sven Laf è bre Martin Vlček. Nijmegen’03. - PowerPoint PPT Presentation
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An Improved Limit on the Muon Neutrino Mass from Pion Decay in Flight
Carmen-Miruna AnăstăsoaieAlex Eduardo de BernardiniSven LafèbreMartin Vlček
NuMass Experiment
International Summer School on
Particle and Nuclear Astrophysics
in Nijmegen 2003
What is the aim of the project?
NuMass will improve the value of the upper limit of the mass of the muon neutrino.
Current limits:
m(e) 4.35 - 15 eV Tritium -decay endpoint 23 eV TOF spread from SN1987A 0.5 - 9 eV Double -decay for Majorana ’s
m(170 keV (stopping ’s)
m( 18.2 MeV Inv. Mass of hadrons (e+e- Colliders)
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improvement by NuMass by order of 20 to m() < 8 keV
History of the Muon Neutrino Mass Limit
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Why is this measurement so important?
verification of theoretical backgrounds- neutrino mass generation mechanism- complementary information to neutrino oscillation results- neutrino decays understanding - chiral left-right symmetry
improvement of the theoretical description of the Fermi constant understand some loopholes in cosmology
- lack of dark matter- limits to the density of Universe
minimal left-right model verification some propagation phenomena related to supernova pulses it is, after all, a fundamental constant !
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Highlights of the experimental technique
“origin”
In a perfectly uniform magnetic field any charged particle returns to origin independent of B or p or angle
Uniformity is more important value of B
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Highlights of the experimental technique
Injection
decay orbit
24 g-2 calorimetersrestrict late decays
identify electron bkginitial beam tuning C-veto: restrict
incoming ’s
J-veto: restrict early ‘s at large angles
J-cal: 2nd turn electron id
Beam counter
S1 S2
Trigger Hodoscope
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observed event by eventwe will need SEB
Highlights of the experimental technique
NuMass will use the existing G-2 Storage Ring in the BNL facility at Brookhaven with only minor modifications
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Highlights of the experimental technique
Embedded Scintillator:2 mm Prescale Strips
Trigger pads
BerylliumDegrader
S2
S1
Silicon μ-strip Detectors
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Endpoint structure
Expected distance between first pass pion and second pass muon (in mm)
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Sources of background
Beam-gas scatters => vacuum is 10-6 torr
Injected p (27 %) => rejected in embedded scintilators ΔT = 7 ns / turn slower
Injected e (12 %) => rejected in J-veto, calorimeter or position, lose 1 MeV / turn
μ → e=> rejected by g-2 calorimeter
< 10-4 of good π-μ events π → e=> rejected by calorimeter in inner
J-veto
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J-Veto
S1 S2
g-2 Cal’s
C-Veto
Advantages of NuMass
run in dedicated mode or in conjuction with K-decay (E949) or MECO experiment
another project may run nearly immediately after our beamtime, there are only minor changes on beam
pure 2 body decay no model dependent nuclear/atomic environment
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Responsibilities
Beamline and Ring BNLSSD and readout electronics CERN, MinnesotaActive Vetoes and Scint Trigger BU, Illinois, Tokyo ITFeedthrus and positioners Tokyo IT, Heidelberg, BNLDAQ and g-2 electronics Minnesota, BUField Measurements Yale, Heidelberg, BNLOrbital dynamics, Monte Carlo Cornell, BNL, Yale, NYU,
Minnesota, BUAnalysis The team!
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Budget
$ 770k BNL- modifications on G-2 and SEB- improved sensitivity for the V1 beamline
instrumentation- beam time
$ 330k CERN, Universities- silicon detectors, degrader, active vetoes- feedthrus, positioners- electronics, DAQ
$ 1.1 M TOTAL COST
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Scheduling Year 2000
build 2-SSD detectors plus removable degrader unitbuild active vetos or simple prototypewrite software for new electronics readout and integrate with g-2
Year 2001install and test prototype detectors by running parasiticallyunderstand the π-μ orbital parameterstest AGS/beamline modifications for slow extraction to g-2build and test final silicon detector + degrader
Year 2002commission slow extraction to g-2run the experiment parasitically with E 949
Year 2003dedicated experiment or further parasitic running to completion
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Thank you for your attention ...
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Neutrino oscillation
Neutrino oscillation experimental results are theoretically dependent. Some effects surrounding the standard formulation of neutrino oscillation phenomena:
Neutrino oscillation Δm2 DIRECT !!!
(flavor) quantum number oscillation
existence of sterile neutrino
understanding of the mixing angles
chiral oscillation
Dirac formulation of neutrino oscillation
matter effect
wave packet description
I’m
If you believe atmospheric neutrino result:
=>with onlym2~.002
Then this experiment reduces the neutrino mass limit
by 3 orders of magnitude!
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Neutrino oscillation
Inflector
Degrader
T0 J-Veto
collimator
Pion on orbit
pion => pion residual profile
Muon hits J-Vetoon 1st turn
Flash Counter
pion 2nd time around
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Some background configurations
5 mm endpt (q=70 MeV/c)
SR shrinks it 2 mm
e
e
g-2 Calorimeters
J-Calorimeter
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Cross section of g-2 superconducting magnet
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Cross section of the field
Contours every 1 ppm of field gradient represents lines every 1.5 μTesla
Magnetic field is 1.45 Tesla
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Proposed Parasitic Running with AGS Crystal ExtractionProposed Parasitic Running with AGS Crystal Extraction
E949 Running Conditions25 Gev protons70 TP in a 4.1 s spill / 6.4 s cycle
E952 Parameters2.8 x 106 into g-2 ring/TP5.4 x 1012 for an 8 keV result
Triggers Offline
Entering Ring Detector +vetoes
8 x 106 part/s 1 x 106 part/s 1.8 x 105 s-1 910 s-1 42 s-1
400 Hz/strip 55 s/SSD 11 ms/SSD
100 MB/s 0.5 MB/s
Prescale in trigger
Instantaneous rates (100% extr. eff.)
Running Time
5% of SEB beam => 492 hrs (crystal extr. eff.)
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