MiniBooNE Steve Brice Fermilab Overview MiniBooNE Beam MiniBooNE - - PowerPoint PPT Presentation

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MiniBooNE Steve Brice Fermilab Overview MiniBooNE Beam MiniBooNE Detector Neutrino Analyses Summary Neutrino 2004 June 15 Steve Brice FNAL Page 1 Current Oscillation Signals Unconfirmed m 2 LSND ~ 0.1-10


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Page 1 Steve Brice FNAL Neutrino 2004 June 15

MiniBooNE

Steve Brice Fermilab

Overview MiniBooNE Beam MiniBooNE Detector Neutrino Analyses Summary

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SLIDE 2

Page 2 Steve Brice FNAL Neutrino 2004 June 15

Current Oscillation Signals

  • Unconfirmed

∆m2

LSND~ 0.1-10 eV2

  • Well established

measurements

∆m2

atm ~ 2 - 3 x 10-3 eV2

∆m2

solar ~ 7 x 10-5 eV2

(Soudan, Kamiokande, MACRO, Super-K) (Homestake, SAGE, GALLEX, Super-K SNO, KamLAND)

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SLIDE 3

Page 3 Steve Brice FNAL Neutrino 2004 June 15

Sensitivity to exclude Null CP signal at 2σ

Black: No MiniBooNE Signal Red: if CPC MiniBooNE signal Blue: if CPV MiniBooNE signal

Implications

3 active, light neutrinos (Z width from LEP)

But ∆m2

solar + ∆m2 atm ≠ ∆m2 LSND

If all 3 measurements are oscillations something fundamental has to give

Sterile neutrino(s) are one possibility

add extra neutrino flavours, but don't allow them to interact weakly

Also affects offaxis sensitivity

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Page 4 Steve Brice FNAL Neutrino 2004 June 15

LSND:

Excess of νe events in a νµ beam

87.9 ± 22.4 ± 6.0 over background

~4σ evidence for ν oscillation

The LSND Result

To Check LSND you want

Experiment with

different systematics

higher statistics

similar L/E

MiniBooNE

(hep-ex 0104049)

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SLIDE 5

Page 5 Steve Brice FNAL Neutrino 2004 June 15

The Collaboration

Fermilab IL, USA

Y.Liu, I.Stancu University of Alabama S.Koutsoliotas Bucknell University E.Hawker, R.A.Johnson, J.L.Raaf University of Cincinnati T.Hart, R.H.Nelson, M.Wilking, E.D.Zimmerman University of Colorado A.A.Aguilar-Arevalo, L.Bugel,

  • J. M. Conrad, J. Link, J. Monroe,

D.Schmitz, M. H. Shaevitz,

  • M. Sorel, G. P. Zeller

Columbia University D.Smith Embry Riddle Aeronautical University L.Bartoszek, C.Bhat, S.J.Brice, B.C.Brown, D.A.Finley, B.T.Fleming, R.Ford, F.G.Garcia, P.Kasper, T.Kobilarcik, I.Kourbanis, A.Malensek, W.Marsh, P.Martin, F.Mills, C.Moore, P.Nienaber, E.Prebys, A.D.Russell, P.Spentzouris, R.Stefanski, T.Williams Fermi National Accelerator Laboratory D.C.Cox, A.Green, T.Katori, H. -O.Meyer, R.Tayloe Indiana University G.T.Garvey, C.Green, W.C.Louis, G.A.McGregor, S.McKenney, G.B.Mills, H.Ray, V.Sandberg, B.Sapp, R.Schirato, R.Van de Water, N.L.Walbridge, D. H. White Los Alamos National Laboratory R.Imlay, W.Metcalf, S.Ouedraogo, M.Sung, M.Wascko Louisiana State University J.Cao, Y.Liu, B.P.Roe, H.J.Yang University of Michigan A.O.Bazarko, P.D.Meyers, R.B.Patterson, F.C.Shoemaker, H.A.Tanaka Princeton University

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Page 6 Steve Brice FNAL Neutrino 2004 June 15

MiniBooNE Goal

Search for νe appearance in a νµ beam

L=540 m ~10x LSND

E~500 MeV ~10x LSND

Aim to be definitive

cover LSND 90% conf region at 4-5σ

this needs ~1021 delivered protons

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SLIDE 7

Page 7 Steve Brice FNAL Neutrino 2004 June 15

Beam Overview

Primary Beam

8 GeV protons from Booster

Into MiniBooNE beamline

Secondary Beam

Mesons from protons striking Be target

Focused by magnetic horn

Tertiary Beam

Neutrinos from meson decay in 50m pipe

Pass through 500m dirt (and oscillate?) to reach detector

Booster

Beamline Target and Horn LMC Decay Region 500m dirt Detector

Primary Beam (protons) Secondary Beam (mesons) Tertiary Beam (neutrinos)

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Page 8 Steve Brice FNAL Neutrino 2004 June 15

Booster Performance

In its 30 years the Fermilab Booster has never worked this hard

Currently average ...

~ 6x1016 protons/hour

Have reached 28% of total protons needed

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Page 9 Steve Brice FNAL Neutrino 2004 June 15

Horn, Target & Fluxes

Protons impinge on 71cm long, Be target

Horn focusing of secondary beam increases ν flux by factor of ~5

170 kA pulses, 143µs long at ~5 Hz

Has performed flawlessly with ~80 million pulses to date

Main νµ flux from π+

µ+ νµ

Intrinsic νe flux from

µ+

νµ e+ νe

Κ+

π0 e+ νe

K0

L

π- e+ νe

Understand fluxes with multiple monitoring systems

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SLIDE 10

Page 10 Steve Brice FNAL Neutrino 2004 June 15

Understanding ν Fluxes (1)

E910 @ BNL + previous world data fits

Basis of current MB π production model

HARP @ CERN

Measure π & K production from 8 GeV p beam

MB target slugs - thin and thick targets

Analysis in progress

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SLIDE 11

Page 11 Steve Brice FNAL Neutrino 2004 June 15

LMC muon spectrometer

Κ decays produce wider angle muons than π decays

Scintillating fibre tracker 7 degrees off axis

Understanding ν Fluxes (2)

LMC triggered from beam-on-target signal

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Page 12 Steve Brice FNAL Neutrino 2004 June 15

Detector Overview

12m diameter sphere

Filled with 950,000 litres of pure mineral

  • il

Light tight inner region with 1280 8” PMTs (10% coverage)

240 PMTs in outer veto region

Neutrino interactions in oil produce

Prompt Čerenkov light

Delayed scintillation light

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Page 13 Steve Brice FNAL Neutrino 2004 June 15

Particle ID

Identify electrons (and thus candidate νe events) from characteristic hit topology

Michel e from µ decay candidate Beam µ candidate Beam π0 candidate

νµ µ− n p W νe e− n p W νµ n ∆0 Z νµ p π0

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Page 14 Steve Brice FNAL Neutrino 2004 June 15

Neutrino Candidates

DAQ triggered on beam from Booster

Detector read out for 19.2 µs

ν pulse through detector lasts 1.6 µs

With a few very simple cuts non- neutrino/neutrino rate is ~10-3

ν event every 1.5 minutes, ~300k to date

Constant n rate per incident proton

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SLIDE 15

Page 15 Steve Brice FNAL Neutrino 2004 June 15

Laser Calibration System

Measure tube timing response (needed for event reconstruction)

4 Flasks distributed about the tank

Measure tube charge response (needed for energy measurement)

Fully automated calibration system

New calibration every 4 days

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Page 16 Steve Brice FNAL Neutrino 2004 June 15

Optical Model

Light Creation

Cerenkov – well known

Scintillation

yield

spectrum

decay times

Light Propagation

Fluoresence

rate

spectrum

decay times

  • Scattering

Rayleigh (λ4, 1+COS2θ)

Particulate (Mie)

Absorption

In Situ

Cosmics muons, Michel electrons, Laser

Ex Situ

Scintillation from p beam (IUCF)

Scintillation from cosmic µ (Cincinnati)

P

Goniometry (Princeton)

Fluorescence Spectroscopy (FNAL)

Time resolved spectroscopy (JHU)

Attenuation (Cincinnati)

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Page 17 Steve Brice FNAL Neutrino 2004 June 15

Muon Tracker and Cubes

Muon tracker system provides muons of known direction in the tank

Key to understanding energy and reconstruction

7 Scintillator cubes throughout the tank

Provide muons & Michel electrons of known position

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Page 18 Steve Brice FNAL Neutrino 2004 June 15

Electron Energy Response

Michel Electrons from Cosmic µ Decays

Used to set energy scale

Cosmic Michel data Analytic fit

π0 Mass Reconstruction

In Beam Time window

Tank hits > 200, Veto hits < 6

In fiducial volume

Both rings > ~40MeV and well separated

)

2

mass (GeV/c π 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55

2

Events/0.005 GeV/c 100 200 300 400 500 600 700

PRELIMINARY

2

0.001 GeV/c ± Mass = 0.1391 /NDF = 150.08/98

2

χ 144 ± ’s = 7208 π No. MC signal + background MC background Data

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Page 19 Steve Brice FNAL Neutrino 2004 June 15

CC quasi-elastic NC π0 production NC elastic

Use to understand νe CCQE cross-section

resonant: coherent:

background to νe appearance Use to understand lower vertex Z

p/n p/n

νµ Analyses

Z

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Page 20 Steve Brice FNAL Neutrino 2004 June 15

Charged Current QE

Selection:

Cosmic ray cuts

Single µ-like ring

Topology

MC & Data relatively normalized.

Red Band: MC 1σ uncertainty from...

flux shape

cross-section

Yellow Region: idea of variation from...

  • ptical properties (atten. length,

scintillation, scattering, ...)

Visible Energy (GeV) 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18 0.2 0.22 0.24

Data Shape Errors σ , Φ MC: Shape Errors + σ , Φ MC: Optical Model Variations

)

beam

θ Cosine (

  • 1
  • 0.5

0.5 1 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16 0.18 0.2

Data Shape Errors σ , Φ MC: Shape Errors + σ , Φ MC: Optical Model Variations

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Page 21 Steve Brice FNAL Neutrino 2004 June 15

CCQE Reconstruction

Assume: (CCQE)

Get Eν

CCQE and Q2 from Eµ , θµ

Sensitive to νµ disappearance

(GeV)

QE ν

E 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 0.02 0.04 0.06 0.08 0.1 0.12 0.14 0.16

Data Shape Errors σ , Φ MC: Shape Errors + σ , Φ MC: Optical Model Variations

)

2

(GeV

2

Q 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 0.05 0.1 0.15 0.2 0.25 0.3

Data Shape Errors σ , Φ MC: Shape Errors + σ , Φ MC: Optical Model Variations

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Page 22 Steve Brice FNAL Neutrino 2004 June 15

NC π0

Ntank > 200, Nveto < 6, Fid.Vol.

No Michel electron

Clear 2-ring fit on all events

Each ring: Eγ1, Eγ2 > 40 MeV.

Signal yield extracted from fit with background MC.

)

2

mass (GeV/c π 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5 0.55

2

Events/0.005 GeV/c 100 200 300 400 500 600 700

PRELIMINARY

2

0.001 GeV/c ± Mass = 0.1391 /NDF = 150.08/98

2

χ 144 ± ’s = 7208 π No. MC signal + background MC background Data

π

θ Cos

  • 1
  • 0.8 -0.6 -0.4 -0.2

0.2 0.4 0.6 0.8 1 Fraction of Signal Events/0.2 0.05 0.1 0.15 0.2 0.25 0.3 Unit area normalization

PRELIMINARY

Data flux shape error σ MC 1 MC flux shape error + representative

  • il optical model

variation

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Page 23 Steve Brice FNAL Neutrino 2004 June 15

π0 Variables

High Momentum tail

from ν flux

distorted by 2 ring cut No preferred CM γ direction, but distorted by Lab Eγ and 2 ring cuts.

Momentum (GeV/c) π 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Fraction of Signal Events/0.1 GeV/c 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 Unit area normalization

PRELIMINARY

Data flux shape error σ MC 1 MC flux shape error + representative

  • il optical model

variation

CM

θ Cos 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Fraction of Signal Events/0.1 0.02 0.04 0.06 0.08 0.1 0.12 0.14 Unit area normalization

PRELIMINARY

Data flux shape error σ MC 1 MC flux shape error + representative

  • il optical model

variation

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Page 24 Steve Brice FNAL Neutrino 2004 June 15

NC Elastic Scattering

Select NTANK < 150 NVETO< 6 clear beam excess use random triggers to subtract non-beam background

p/n

Z

p/n

PRELIMINARY

beam with unrelated background

PRELIMINARY

normalized strobe data

PRELIMINARY

beam after strobe subtraction

Monte Carlo

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Page 25 Steve Brice FNAL Neutrino 2004 June 15

Updated Appearance Sensitivity

νe signal events

q

NC π0 misIDs

r

Beam νe events

s

νe signal and background breakdown

t

Reasonable signal separation with 1021 POT

Monte Carlo Monte Carlo

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Page 26 Steve Brice FNAL Neutrino 2004 June 15

Summary

All hardware systems working well

We're at 28% of 1021 protons on target

Already amassed world's largest ν dataset in ~1GeV range

Sample of neutrino physics shows that reconstruction and analysis algorithms are working well

νe appearance analysis should be ready in time for 1021 POT. Hopefully in 2005