Exclusive Neutrino Cross Sections From Mi MiniBooNE Martin Tzanov - - PowerPoint PPT Presentation

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Exclusive Neutrino Cross Sections From Mi MiniBooNE Martin Tzanov - - PowerPoint PPT Presentation

Exclusive Neutrino Cross Sections From Mi MiniBooNE Martin Tzanov University of Colorado PANIC 2008, 9-14 November, Eilat, ISRAEL Neutrino no Cross Sec ections Today ay CC world data CC world data Precise knowl wledge ge


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SLIDE 1

Exclusive Neutrino Cross Sections From Mi MiniBooNE

Martin Tzanov University of Colorado PANIC 2008, 9-14 November, Eilat, ISRAEL

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SLIDE 2

Martin Tzanov, PANIC 2008

Neutrino no Cross Sec ections Today ay

  • Precise knowl

wledge ge need eded for pr prec ecis ise e oscillat ation

  • n measurements.
  • Cross sectio

ion we well mea easured ab above 20 20 GeV.

  • Few

ew meas asurem emen ents be below 20 GeV.

  • 20-

0-30 0 years old ld bub ubble chamber ex expe periments (mos

  • stly H2, D2).
  • Neut

utral cur urrent nt cross sections are e even less und nderstood.

ν

CC world data CC world data

ν

T2K 2K, BooNE NE K2K, NO NOvA MINOS

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SLIDE 3

Martin Tzanov, PANIC 2008

The MiniBooN

  • NE Experiment

DETECTOR

  • 541

41 m downstream am of tar arget et, 3 m overburden

  • 12 m diameter sphe

here( e(10 m “fiducial al”)

  • 800

00 t (450 t fidu ducia ial) of pu pure e mineral al oil l (CH2)

  • 128

280 inner and 24 240 vet eto ph photot

  • tube

bes

The Neutrino Flux Prediction at Mini niBooNE, Submitted to PRD [arXiv:0806:1449]

BEAM:

  • Mini

niBooNE ex extracts protons from the 8 GeV eV Booster deliver ered d to a 1.7l Be target inserted into

  • a magn

gnetic ic horn (2.5 kV, 174 4 kA) that at (in increa eases es flux ux 6 times)

  • ~90

900k in interactio ions in n fiducial volume in ν mode with h small an anti- i-ν componen ent.

  • ~90

90k int nteractio ions in fidu ducial vol

  • lume in an

anti-ν mode with h 30% 0% ν component nt.

The e MiniBooNE Detector, Accepted by NIM A [arXiv:0806.4201]

ν mode flux - foc

  • cus

usin ing π+ ant nti-ν mode flux - focusing g π-

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SLIDE 4

Martin Tzanov, PANIC 2008

CCQE

µ

ν

Neutrino oscil illations:

  • dominant

nt at at this en energy.

  • golden

en channe nel for dis isap appearan ance searches. Neutrino cross section:

  • prov
  • vid

ides inf nformatio ion about nucle lear structur ure.

  • fits to ol
  • ld bu

bubble chamber experiments (D2).

  • MA = 1.03 GeV.
  • recent results on nuclear

ar target ets – hi higher MA

  • K2K SciFi (16O) MA= (1.

1.20 ± 0.12) GeV, PRD RD 74, 4, 052 52002 (2006) 6)

  • K2K Scibar

ar (12C) MA= (1.14 14 ± 0.11) 1) GeV eV MiniBooNE NE has coll llected d 198, 8,000 00 events after cuts.

p n

+ → +

µ ν µ

( )

2 2 2

1

A A A

M Q g F

+ =

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SLIDE 5

Martin Tzanov, PANIC 2008

CCQE Kinematics

µ

ν

  • tagged

ed by the stoppe ped muon n decay ay elec ectron

  • n
  • 74%

4% pur urit ity, 35% efficiency

  • measure

e θµ, Tµ → Eν, Q2

  • world MA =1.03 GeV (dashe

hed li line) dat ata disagree e in Q2

  • fit to the Q2 distribu

butio ion using ng effective e parameters MA and nd κ (Pauli li bl blocking parameter). MA = (1.23 23 ± 0.20) GeV, (high Q2) κ = 1.01 019 ± 0.011, (low Q2)

  • agr

gree ees wit ith nu nuclear target measurements.

) cos ( 2

2 2 2

µ µ µ ν µ

θ

p E E m q Q

− + − = − =

Measurement of Muon n Neutrino Quas asi- i- Elastic Scat atter erin ing on n Car arbo bon, PRL RL 10 100, 03231 310 (200 008)

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SLIDE 6

Martin Tzanov, PANIC 2008

bef efore correctio ion after correction

  • n

) cos ( 2

2 2 2

µ µ µ ν µ

θ

p E E m q Q

− + − = − =

CCQE Kinematics

  • improves agree

eement with h data for both cosθµ and Tµ Data/MC ratios

µ

ν

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SLIDE 7

Martin Tzanov, PANIC 2008

CCQE

µ

ν

  • ap

apply MA and κ from ν mode. e.

  • goo
  • od agr

gree eement with dat ata.

n p

+ → +

+

µ ν µ

  • goo
  • od agr

gree eement in othe her kinematic var ariables PRELIMINARY

PRELIMINARY

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SLIDE 8

Martin Tzanov, PANIC 2008

νµ NC π0

Neutrino oscillation:

  • very import

rtant for

  • r νe appea

earance sear arches es

  • if

if one ne of

  • f the γ’s is lost or bel

elow threshold ld π ν ν π ν ν

µ µ µ µ

+ + → + + + → +

A A N N

Wor

  • rld

d data on cohe herent production Neutrino cros

  • ss section:
  • important for
  • r understanding

g coheren ent and res esonant produ duction.

  • no
  • data bel

elow 2GeV eV.

  • Rei

ein – Sehg hgal mod

  • del used for pr

predi diction. n. resonant coherent

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SLIDE 9

Martin Tzanov, PANIC 2008

νµ NC π0

  • excelle

lent π0 con

  • ntainm

nmen ent (4π)

  • fully recon
  • nstructed π0 sam

ampl ple – 28,600 events, 97% % pur urit ity, 40 40% efficie iency

  • rewei

eighting of mom

  • men

entum distribut ution

  • n

gives ver ery go good agreement nt in in other kinematic variabl bles.

  • very differ

erent nt angular ar distrib ibution

  • ns –

coh

  • herent is muc

uch more forward

  • fit for resona

nant and coherent fractio ions yield lds [19 19.5±1. 1.1(stat at)±2.5( 5(syst)]% coh

  • herent frac

action.

First Observation of Coherent π0 Production in Neutrino Nucleus Int nteraction

  • ns with Eν<2 GeV,

Phys Lett B.664, 41 (2008)

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SLIDE 10

Martin Tzanov, PANIC 2008

NC π0

µ

ν

  • evide

dence of

  • f cohe

heren ent events.

π ν ν

µ µ

+ + → +

N N

  • ~27

2700 even ents af after cuts

  • fir

irst measurement at at 1GeV comparison w/o coherent nt fraction For

  • r details see

e poster 77 7 by V. Nguyen en

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SLIDE 11

Martin Tzanov, PANIC 2008

νµ CC π+

+ − + −

+ + → + + + → + π µ ν π µ ν

µ µ

A A N N

νµ CCπ+ world data Neu eutrino oscillat ation: n:

  • major
  • r background

nd for νµ dis isappear aranc nce

  • if π+ is absorbed

ed in n the nuc ucle leus

  • modif

ifies es νµQE energy spec ectrum um

  • results in

n larger system emat atic on os

  • scill

llation

  • n

parameters.

  • nee

eed to kno now νµCCπ+/νµCCQE(Eν) to

  • better than 5%.

Neu eutrino cross section:

  • old

ld bub ubble e chamber da data a (H2, D2).

  • few nuclear target exper

erim imen ents.

  • evid

idence of no cohe heren ent com

  • mpo

ponent at low ener ergy gy. resonant coherent Also talk by SciB iBooNE – Y. Nak akaj ajima

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SLIDE 12

Martin Tzanov, PANIC 2008

νµCCπ+/νµCCQE(Eν)

  • MiniB

iBooNE measurement nt is is consisten ent with previou

  • us measurements and

d Rein- n-Sehg hgal mod

  • del.
  • For det

etails see pos

  • ster 79

9 by J. Nowa wak.

  • tagged

d by two stopped d muon decay el electrons – 47,000 events 87% % purity, 12% % ef effic icienc ncy

  • measure θµ, Tµ → Eν, Q2
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SLIDE 13

Martin Tzanov, PANIC 2008

CC π+ - Fully Reconstruc ucted

µ

ν

  • reconstructing both

h µ and nd π

  • most pions undergo

go nuclea ear inter eractions resul ultin ing in in kinked tracks.

  • new

ew fit itter er look

  • ks for 1 straight

ht (muon

  • n) and

nd one ne kinked (pion)

  • track. Effectivel

ely it’s a three e ring fitter.

  • fir

irst delt lta peak from neu eutrino experiment in more than 20 yea ears. PRELIMINARY

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SLIDE 14

Martin Tzanov, PANIC 2008

Mor

  • re Cross Sections - νµCCπ0 and νµNC elastic

νµCC CCπ0 differ eren ential al cross section

  • n
  • tagged

ed by one stopped ed muon decay el electron.

  • onl

nly resonant compone nent.

  • new

ew three ring ng fit itter er – muon

  • n and

2 ga gamma a tracks

  • full ev

event reconstruction

  • n.

π µ ν µ + + → +

p n

νµNC elas astic different ntial l cros

  • ss section
  • preli

liminary result using g prompt ligh ght for pr proton n PID.

  • new

ew proton track fit itter will provide proton n PID D and d better recon

  • nstruction
  • n.
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SLIDE 15

Martin Tzanov, PANIC 2008

Published ed and Future Cross Section Papers

MiniBooNE NE cross section and d other relev evant nt papers:

  • Measurement of Muon Neutrino Quasi-Elastic Scattering on
  • n Carbon
  • n,

PRL 100 00, 032 3231 310 0 (2008)

  • First Observation of Coherent π0 Production in Neutrino Nucleu

eus Interactions with En<2 GeV, Phys Lett B.664, 41 (2008)

  • The Neutrino Flux Predi

diction at MiniBooNE, Submitted to PRD [arXiv:0806:1449]

  • The MiniBooNE Detector, Accepted by NIM A [arXiv:0806.4201]

Papers in in the he immedia iate e future:

  • νµCC

CCp+/νµCCQE(En) ratio io measurement nt (S. Linde den, J. Nowak)

  • NC π0 coh
  • herent/resonant

nt fraction for anti- i-ne neutrin ino (V. Nguyen n ) Papers to follow w - Dif iffer erentia ial cross section

  • ns:
  • νµCC

CCQE, (T. Katori), an anti- νµCCQE (T. Laird, d, J. Grange ge)

  • νµCC

CC π+ (M. Wilk lking)

  • νµNC

NC π0 (C. Ande derson)

  • NC elas

astic (D. Perevalov)

  • νµCC

CC π0 (R. Nelson)

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SLIDE 16

Martin Tzanov, PANIC 2008

BACKUPS

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SLIDE 17

Martin Tzanov, PANIC 2008

University of Alabama Los Alamos National Laborator

  • ry

Bucknell University Louisiana State University University of Cincinnati University of Michigan University of Color

  • rad

ado Princeton University Columbia University Saint Mary’s University of

  • f Minnesota

Embry Riddle University Virginia Polytechnic Institute Fermi National Accelerator Laboratory Wester ern n Illinois University Ind ndiana Univer ersity Yale University

MiniBoo

  • oNE Collaboration
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SLIDE 18

Martin Tzanov, PANIC 2008

Subev event nt: Multiple e hits within a ~100 ns win indow form “subev even ents” Most events are from νµ CC inter eractions (ν+n n → µ+p) wit ith cha harac acteristic ic two “subevent nt” structure e from

  • m

stop

  • pped µ→νµνee

A 19. 9.2 ms be beam trigger window w

  • enc

ncompas asses es the e 1.6 ms spill ll

  • star

arts 4 ms before e the he beam am

µ e

Tank Hits

Timing and Subevents

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SLIDE 19

Martin Tzanov, PANIC 2008

Event Topologies in MiniBooNE Detector

Muon event

  • long

ng track, small l scatter erin ing Electron

  • n/phot
  • ton event – fuzzy rin

ing

  • short trac

ack, large scat atter ering

  • g converts an

and looks like e elec ectron

  • ns

π0 event – two fuzzy rings