miniboone cross section results

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MiniBooNE Cross Section Results H. Ray, University of Florida ICHEP 2012 1 Interactions of the future!

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MiniBooNE Cross Section Results. Interactions of the future!. Booster. Target Hall. decay region. absorber. target and horn. detector. FNAL Booster. dirt . Booster. primary beam. secondary beam. tertiary beam. (protons). (mesons). (neutrinos). MiniBooNE Neutrino Beam. - PowerPoint PPT Presentation

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Page 1: MiniBooNE Cross Section Results

H. Ray, University of Florida 1

MiniBooNE Cross Section Results

ICHEP 2012

Interactions of the future!

Page 2: MiniBooNE Cross Section Results

MiniBooNE Neutrino Beam

2

Booster

target and horn detectordirt absorber

primary beam tertiary beamsecondary beam(protons) (mesons) (neutrinos)

decay regionFNAL Booster

Booster TargetHall

8.9 GeV/c momentum protons extracted from Booster

Directed on to a Beryllium

Maximum rate of 5 Hz

H. Ray, University of Florida ICHEP 2012

Page 3: MiniBooNE Cross Section Results

MiniBooNE Neutrino Beam

3

Booster

target and horn detectordirt absorber

primary beam tertiary beamsecondary beam(protons) (mesons) (neutrinos)

nm

decay regionFNAL Booster

p+

p+p-

p-

Magnetic horn with reversible polarity

Focuses either neutrino or anti-neutrino parent mesons

Collect data in neutrino, anti-neutrino mode, <Eν> ~700 MeV

H. Ray, University of Florida ICHEP 2012

Page 4: MiniBooNE Cross Section Results

MiniBooNE Detector

12.2 meter diameter spherePure mineral oil, interactions on CH22 regions

Inner light-tight region, 1280 PMTs (10% coverage), 4π coverageOptically isolated outer veto-region, 240 PMTs

Nucl. Instr. Meth. A599 (2009) 28-46

ICHEP 2012 4H. Ray, University of Florida

Page 5: MiniBooNE Cross Section Results

MiniBooNE Detector

ICHEP 2012 5

Cerenkov detector ring imaging for event reconstruction and PID, use particle decays for event ID (μ e, π+ μ e)

Separate clusters of PMT hits in time

Scintillation light enables NC EL measurement

muon candidate

H. Ray, University of Florida

Page 6: MiniBooNE Cross Section Results

MiniBooNE Detector

ICHEP 2012 6

Cerenkov detector ring imaging for event reconstruction and PID, use particle decays for event ID (μ e, π+ μ e)

Separate clusters of PMT hits in time

Scintillation light enables NC EL measurementH. Ray, University of Florida

m+

e+

pEither bound

(12C) or quasi-free

(H)

n

m

e

80% CCQE purity 25% efficiency

Page 7: MiniBooNE Cross Section Results

7

Measuring a Cross Section

ICHEP 2012

Efficiencies of event selection

Flux of incoming particle beam

Targets seen by beam

M. Catanesi et al., Eur. Phys. J. C52, 29 (2007)

Precision xsecs require firm knowledge of flux!

Use external data for flux prediction no in-situ tuning!

HARP: dedicated hadro-production expt

same beam E, exact replica target

BNL E910

Overall 9% flux uncertainty, dominates error on xsec measurement

H. Ray, University of Florida

Page 8: MiniBooNE Cross Section Results

H. Ray, University of Florida 8

QE

NC EL

CC π+

multi-π +CC π 0NC π +/-NC π 0otherWS

PRD 81, 092005 (2010)PRL 100, 032301 (2008)

PRD 82, 092005 (2010)

PRL 103, 081801 (2009)PRD 83, 052007 (2011)

PRD 83, 052009 (2011)PRD 81,

013005 (2010)

PL B664, 41 (2008)

Neutrino Cross Sections

ICHEP 2012

8 n cross section publications

Collected ν data2002-2005, 20076.46e20 POT

39.7%

17.1%

23.5%

Nuance MC Prediction

Page 9: MiniBooNE Cross Section Results

H. Ray, University of Florida 9

QE

NC EL

CC π+

multi-π +CC π 0NC π +/-NC π 0otherWS

Neutrino Cross Sections

ICHEP 2012

Collected ν data2002-2005, 20076.46e20 POT

1st time full kinematics have been reported for many of these reaction channels!

Page 10: MiniBooNE Cross Section Results

H. Ray, University of Florida 10

Neutrino CC Exclusive Intrigue

ICHEP 2012

* NOMADFermi Gas (MA=1.35 GeV)Fermi Gas (MA=1.03 GeV)

Fermi Gas (MA=1.35 GeV)Fermi Gas (MA=1.03 GeV)

30%

• MiniBooNE

* NOMAD

T. Katori, Indiana U, Ph.D. thesis

Tension between existing CC exclusive measurements, different expts

Tension between CC exclusive measurements and theory, QE, π+, π0

nuclear interactions may be the key

Need to understand CC scattering as a whole

… but MB consistent with SciBooNE, MINOS, K2K

Page 11: MiniBooNE Cross Section Results

H. Ray, University of Florida 11

Neutrino CC Inclusive

ICHEP 2012

Can’t do straight sum of exclusive channels; would sum systematic errors too!Correlations exist between exclusive channelsRequire at least 2 clusters of hits in time (μe)~344k events after cuts, purity of 96%

Full 6.46e20 POTM. Tzanov, LSU

PRELIMINARY

PRD 83, 012005, 2011

MiniBooNE

Cross Section

Coming Soon!!

Page 12: MiniBooNE Cross Section Results

H. Ray, University of Florida 12

Anti-neutrino Cross Sections

ICHEP 2012

Collected anti-ν data2005-2006, 2008-201210.1e20 POT

QE

NC EL CC π-

multi-π+

CC π0

NC π+/-

NC π0

other

WS νPRD 84, 072005 (2011)

29.6%

13.8% 9.3%

Nuance MC Prediction

35.1%

PRD 81, 013005 (2010)

Page 13: MiniBooNE Cross Section Results

13

Anti-neutrino Wrong Sign Contamination

Large wrong-sign contribution to data sampleLargest in region not covered by HARP

Measure WS in-situ, using complementary methods1st measurement of WS in a non-magnetized detector!

ICHEP 2012H. Ray, University of Florida

Phys. Rev. D84, 072005 (2011)

Page 14: MiniBooNE Cross Section Results

H. Ray, University of Florida 14

Anti-Neutrino CC Cross Sections

ICHEP 2012

MiniBooNE <Eν> = 700 MeV

World anti-ν CC results

J. Formaggio and G. Zeller, RMP, to be published (2012)

World anti-ν CCQE results

Page 15: MiniBooNE Cross Section Results

H. Ray, University of Florida 15

Anti-neutrino CCQE Cross Section

ICHEP 2012

Applying identical cuts as neutrino-mode CCQE PRD analysis~77,000 events pass CCQE cuts (not bkg subtracted or efficiency corrected)More than 10x the statistics of all other previously published anti-neutrino CCQE samples!Next step: neutrino/anti-neutrino, exploit error correlations, narrow down correct model(s)

Full 10.1e20 POTJ. Grange, University of Florida

Cross Section

Coming Soon!!

Page 16: MiniBooNE Cross Section Results

H. Ray, University of Florida 16

Anti-neutrino NC Elastic Cross Section

ICHEP 2012

• Only 1 nucleon in final state• Below Cerenkov threshold• Reconstruct recoiling nucleon via a small amount of

scintillation light• Uses Likelihood ratio to distinguish protons from low energy

electrons• Largest bgd from NC π± where π is missed due to absorption in

oil

ν or anti-ν12C

p

scintillation light

Page 17: MiniBooNE Cross Section Results

H. Ray, University of Florida 17

Anti-neutrino NC Elastic Cross Section

ICHEP 2012

~44,000 NCE events, 40% purityWorld record anti-ν NCE sample!Next step: neutrino/anti-neutrino ratio

7.4e20 POTR. Dharmaplalan, University of Alabama

Cross Section

Coming Soon!!

Page 18: MiniBooNE Cross Section Results

H. Ray, University of Florida 18

Future Plans!

ICHEP 2012

• Neutrino CC inclusive (Martin Tzanov, LSU)

• Antineutrino CCQE (Joe Grange, U Florida)

• Antineutrino NC elastic (Ranjan Dharmapalan, U Alabama)

• Neutrino CCQE with proton reconstruction (Athula Wickremasinghe, U Cincinnati)

MiniBooNE has performed ν-nucleon scattering measurements in a variety of interaction channels!

8 publications so far!These analyses will complete the highly successful

MiniBooNE cross section program