(tau neutrino magnetic moment) reinhard schwienhorst university of minnesota donut analysis talk at...
TRANSCRIPT
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(tau neutrino magnetic moment)
Reinhard Schwienhorst
University of Minnesota
Donut analysis
Talk at Nagoya University, 6/9/99
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Outline• Introduction
• Physics– magnetic moment interaction– Expected event yield
• Spectrometer analysis:– Monte Carlo Analysis– Cuts
• Preliminary Physics result
• Conclusions
All of the numbers in this presentation are preliminary
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Introduction• Standard Model
– =0
• current experimental limit: – e:<1.810-10B
– :<7.410-10B
– :<5.410-7B
(all obtained in neutrino-electron scattering experiments)
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Magnetic moment interaction
e
e
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Magnetic moment interaction example (MC)Title:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
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Magnetic moment interaction example (MC)Title:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
Title:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
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Physics reminder
• Neutrino-electron scattering– no hadronic activity in the event– small forward angle
• magnetic moment interaction– cross section
÷øö
çèæ -µ 12
T
E
dT
d s
• : neutrino magnetic moment• E: neutrino energy• T: electron kinetic energy
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Electron energy and angleTitle:pawprint.epsCreator:HIGZ Version 1.23/09Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
Title:pawprint.epsCreator:HIGZ Version 1.23/09Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
Production angle and energy for the electron in a magnetic moment interaction
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Expected event yield• If =5.410-7B (the current limit):
– with an electron energy cutoff at 5GeV• current cat3 neutrino event sample
• expect 10 magnetic moment interactions
• (compared to 40 CC interaction)
– with an electron energy cutoff at 0.5GeV• .nustrip files
• expect 30 magnetic moment interactions
– with an electron energy cutoff at 10MeV• emulsion analysis
• expect 80 magnetic moment interactions
• we must scan at least 1/3 of the emulsion to improve the sensitivity
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Emulsion-only analysis• Scan a large volume of the emulsion
• Search for single electron tracks in the direction of the beam – challenges:
• identify electrons down to very low energies
• many straight tracks in the emulsion
• Advantage: independent of the spectrometer, time, trigger
• disadvantages: – must scan a large volume– background from pair production
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Spectrometer analysis outline• Optimize cuts for magnetic moment events
– cross-check with CC events (data and MC)
• easy to find
determine efficiency
• apply to neutrino candidate events– apply first to MC events, determine expected # of events
– blind analysis
• apply to nustrip files– find (almost) all candidate events
– not quite a blind analysis
• at the end, scan emulsion for confirmation– identify hadrons, decays, secondary interactions, nuclear
breakup
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Monte Carlo analysis
• So far only periods 3 and 4
• Trigger efficiency =65% for magnetic moment interactions with T>0.5GeV
• Tune each cut to remove no more than ~5% of the magnetic moment interactions
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Cuts• Muon ID
– remove muons and hadrons
– watch out for noise require <2 MID hits (sum over all tracks)
• EMCAL– require EEMCAL<20GeV
– require for each track with P>4GeV that EEMCAL<P/2 for blocks within 0.2m of the track
– check the rectangle with |x-xvtx|<0.7m and |y-yvtx|<0.2m :• require at least 50% of the EMCAL energy to be inside the rectangle
• require the energy outside the rectangle to be less than 1GeV
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Cuts II• SF system:
– require small # of SF hits (< 12000)
– remove events with:• hadrons: highly ionizing tracks (large fiber pulseheight)
• tracks not coming from the emulsion (muons interacting in the shielding)
• tracks that go straight through a module (electrons are required to shower)
– require at least one straight SF line in each view (<0.1rad)• put the vertex at the origin of this line
– require the vertex to be in the emulsion volume
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Cuts III• Trigger counters:
– remove backward trigger O O O O O O O O T1O O X X O O O O O T2 O O X O O O O O T3
– require a trigger panel hit on a straight line behind the vertex
• VDC:– require VDC hits on a straight line behind the vertex
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Cut efficiency:electronic analysis
Percentage ofevents removed in periods 3+4
Data:cat 3
Data:nustrip
MC: CC
MC:e CC
MC:NC
MC:magmom
Begin # of events 700 120000Muon ID cut 60% 10% 86% 48% 52% 8.3%First EMCAL cut 23% 18% 16% 52% 12% 6.4%Hadrons in SF, olddecoder
35% 26% 23% 39% 28% 0.9%
SF lines not fromemulsion
65% 79% 6.4% 21% 3.6% 8.2%
Long SF lines 20% 22% 41% 41% 21% 3.3%
Remaining # ofevents
38 (5%) 20000(17%)
(5%) (7%) (23%) (75%)
# of SF hits 0% 0.1% 0% 0% 0% 0%Hadrons in SF, newdecoder
20% 1.1% 6.6% 21% 6.7% 2.8%
Straight SF line Not used 95.4% 42% 29% 15% 31.1%Vtx in emulsion 13% 24% 4% 4.7% 5.2% 3.8%Backwards trigger Not used 23% 8.2% 14.1% 15.1% 11.7%Trigger counterbehind vertex
4% 40% 3.4% 0% 0% 0%
VDC hits behindvertex
33% 45% 10.5% 2.4% 2.7% 2.4%
vertex in EMCAL 50% 75% 50% 85% 6% 11.8%
Resulting # ofevents
5(0.7%)
81(0.07% )
(1%)(1.8%forcat3)
(0.5%)(0.8%forcat3)
(7.8%)(10.8%forcat3)
(37%)(61%forcat3)
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Cuts IV• Refit and find the vertex
• remove events “by hand” if:– a straight muon is in the SF– the event has only a single track with P>0– there are slow hadrons in the SF
• apply all of the previous cuts again
• output: 3 cat3 events, 14 nustrip events– periods 3 and 4– MC efficiency for these cuts 100%
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Cuts V
• Careful visual inspection of each event– Can it be scanned?
– Check EEMCAL/P for each track
– Check track straightness (angle <0.1rad in X and Y)– check trigger timing
• Output: 0 cat3 events, 1 nustrip event– if current limit: expect 6 cat3 events, 11 nustrip
events
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Candidate eventTitle:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
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Candidate eventTitle:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
Title:event.ps (Landscape A 4)Creator:HIGZ Version 1.25/05Preview:This EPS picture was not savedwith a preview included in it.Comment:This EPS picture will print to aPostScript printer, but not toother types of printers.
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Preliminary Physics result
• Data analysis:– 0 events for T>5GeV– 1 events for T>0.5GeV– systematic error: not determined yet, assume
0.5events
• preliminary 90% confidence limit for the magnetic moment:
B
7103 -´<
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Conclusions
• The magnetic moment analysis is still in progress
• Searching for event candidates in the nustrip files will give the best limit
• Emulsion information for candidate events is very important
• An emulsion-only analysis is only useful if we scan a considerable fraction of the emulsion volume