Interactions Seminar 2018 - Kavli IPMU-カブリ数物連...
Transcript of Interactions Seminar 2018 - Kavli IPMU-カブリ数物連...
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M u l t i - n u c l e o n e f f e c t s ( 2 p 2 h ) p a r a m e t e r s
• Interaction in which more than one nucleon participate. • Pion-less Delta Decay (PDD-like) and N-N Correlation (non-
PDD-like) • Introduced shape parameters in addition to normalization
• +1 corresponds to fully PDD-like • -1 corresponds to fully non-PDD-like
8
Pair Correlation
Delta absorption
preliminary
M u l t i - n u c l e o n e f f e c t s ( 2 p 2 h ) p a r a m e t e r s
• Interaction in which more than one nucleon participate. • Pion-less Delta Decay (PDD-like) and N-N Correlation (non-
PDD-like) • Introduced shape parameters in addition to normalization
• +1 corresponds to fully PDD-like • -1 corresponds to fully non-PDD-like
8
Pair Correlation
Delta absorption
preliminary
HF%@+U+1=*+%h%@=Q+4& ABIi
Marco Del Tutto 26th September 2017
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M u l t i - n u c l e o n e f f e c t s ( 2 p 2 h ) p a r a m e t e r s
• Interaction in which more than one nucleon participate. • Pion-less Delta Decay (PDD-like) and N-N Correlation (non-
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• +1 corresponds to fully PDD-like • -1 corresponds to fully non-PDD-like
8
Pair Correlation
Delta absorption
preliminary
HF%@+U+1=*+%h%@=Q+4& ABIi
PBB%T)O%6,+-%+&%8)+U
CAH
!e Systematics69 A. Radovic, JETP January 2018
Signal uncertainty (%)20! 10! 0 10 20
Statistical error
Total syst. error
Extrapolation
Detector Response
Beam
Calibration
Normalization
Cross Sections"
Background uncertainty (%)30! 20! 10! 0 10 20 30
Statistical error
Total syst. error
Beam
Extrapolation
Detector Response
Normalization
Calibration
Cross Sections"
• As in !µ systematics were assessed by generating sets of shifted MC. • Those shifted datasets were used instead of our nominal MC to assess the impact on
our final result.
!" Systematics43 A. Radovic, JETP January 2018
• Systematics were assessed by generating sets of shifted MC. • Those shifted datasets were used instead of our nominal MC to assess the impact on our final result.
)-310! (23"2Uncertainty on sin50# 0 50
Statistical error
Total syst. errorCP$Value of
Scintillation Model
ScaleµRel. ENeutrino Flux
Rel. Calibration
ScaleµAbs. ENormalization
Cross SectionsAbs. Calibration
)2 eV-310! (232m"Uncertainty on
0.05# 0 0.05Statistical error
Total syst. error
ScaleµRel. ENeutrino Flux
Scintillation Model
ScaleµAbs. ENormalization
CP$Value of Cross Sections
Rel. CalibrationAbs. Calibration
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• Continue to tune MEC to match the excess in our data, now fit using default empirical MEC’s* model for energy transfer to the hadronic system (q0).
• QE RPA from the Valencia group via Richard Gran** now included in central value tune. • New MEC and RPA uncertainties that better capture limits of theory & data constraints.
Retuned Interaction Modeling25 A. Radovic, JETP January 2018
* “Meson Exchange Current (MEC) Models in Neutrino Interaction Generators”, Teppei Katori, NuInt12 Proceedings, arXiv:1304.6014! ** “Model uncertainties for Valencia RPA effect for MINERvA”, Richard Gran, FERMILAB-FN-1030-ND, arXiv:1705.02932
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Marco Del Tutto 26th September 2017
53
MicroBooNE Current EffortsParticle multiplicity
observed multiplicity1 2 3 4 5 6
even
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0.2
0.3
0.4
0.5
0.6
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MC with MEC
MC with TEM
MicroBooNE Preliminary
>82 MeVp>37 MeV,KE!,µKE
(Includes muons)
area normalized
Observed Charged Particle Tracks in Neutrino Interactions
Figure 14: A bin-by-bin fitted, area normalized, CR background-subtracted, observed neutrino multiplicitydistributions for MicroBooNE data overlaid with three GENIE predictions in linear scale. Data error barsinclude statistical errors obtained from the fit. Monte Carlo error bands include MC statistical errors fromthe fit and systematic error contributions added in quadrature.
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even
t fra
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1 MicroBooNE Data (stat only)
MC Default (stat+syst. errors)
MC with MEC
MC with TEM
MicroBooNE Preliminary
>82 MeVp>37 MeV,KE",µKE
(Includes muons)
area normalized
Observed Charged Particle Tracks in Neutrino Interactions
Figure 15: A bin-by-bin fitted, area normalized, CR background-subtracted, observed neutrino multiplicitydistributions for MicroBooNE data overlaid with three GENIE predictions in log y scale. Data error barsinclude statistical errors obtained from the fit. Monte Carlo error bands include MC statistical errors fromthe fit and systematic error contributions added in quadrature.
23
MICROBOONE-NOTE-1024-PUB
Future: improve statistics and lower threshold per particle type
Muon is included in bin 1
Observed multiplicity after event selection, no efficiency correction
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L. Cremonesi “Cross-sections at NOvA ND”
NC Coherent !0
24
• Renormalised background using energy and angle 2D space. • Measured flux-averaged cross-section using background subtraction: ! = 14.0 ± 0.9(stat.) ± 2.1(syst.)x10-40cm2/nucleus• Total uncertainty 16.7%, systematic dominant
Measurements scaled to 12C by A2/3
L. Cremonesi “Cross-sections at NOvA ND”
NC Coherent !0
23
• Fit the backgrounds to control sample data in !0 energy vs angle 2D space.
• Background fit result are applied to the backgrounds in the signal sample.
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=46.002$GENIE 2.12.4 RFG, =34.802$GiBUU 2016,
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20Ciro Riccio, Naples U. & INFN | NUFACT2017
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=98.282%GENIE 2.12.4 RFG, =12.252%GiBUU 2016,
T2K Preliminary
GENIE shape in first bin of each STV related to FSI model (“hA”)
Result =106.592NEUT 5.3.2.2 SF,
T2K Preliminary
Publication in preparation!
GIBUU with very different FSI seems close to data
Data strongly disfavor RFG in favor of LFG and Spectral Function
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10
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16 January 2018 Kevin McFarland: Neutrino Interactions 59
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Double-differential cross section - neutrino mode
27
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Double-differential cross section - antineutrino mode
28
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MINERvA Data
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challenging ! Additional uncertainty evaluated based on whether
additional strength is from np or nn initial states
Cheryl Patrick, UCL / Northwestern
Double-differential cross section - antineutrino mode
28
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Cheryl Patrick, UCL / Northwestern
Vertex energy
32
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Vertex energy: 2017
31
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MINOS sees this too...
Muon neutrino CC inclusive
Tuning procedure was not allowed to change energy scale or focusing parameters here. Just hadron production parameters. Dip remains.
Plots from Anna Holin
Tg@^<2;
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Physics Motivation
More Event Displays
6
Blobbing E�ciency
E�ciency
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CCQE Truth passing selection
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E�ciency increases with Q2ccqe as
energetic neutrons are more prone tokick out energetic protons.
More energetic protons leave longertracks
Thus more likely to be 3D
14
Plots
Preliminary Plots
Plots of the angular variables juxtaposing MC and data
✓C , ordinary cut vs ordinary cut + 2013 recoil cut
20