Exclusive π 0 e lectroproduction in the resonance region at high Q 2 .

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Exclusive π 0 e lectroproduction in the resonance region at high Q 2 . Maurizio Ungaro , Kyungseon Joo University of Connecticut Jefferson Laboratory for the CLAS collaboration. Resonance Discovery. $1750. p + + P  p + + P p - + P  p - + P p - + P  p 0 + N. - PowerPoint PPT Presentation

Transcript of Exclusive π 0 e lectroproduction in the resonance region at high Q 2 .

APS Meeting, April 30 2011

Exclusive π0 electroproductionin the resonance region at high Q2.

Maurizio Ungaro, Kyungseon Joo

University of ConnecticutJefferson Laboratory

for the CLAS collaboration

1M.Ungaro

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Resonance Discoveryp+ + P p+ + P p- + P p- + P

p- + P p0 + N€

13A3 / 2 + 2

3A1/ 2

A3 / 2

23

(A3 / 2 − A1/ 2)

s++:s--:s-0 = 9:1:2

dσdΩ

= a + bcosθ + c cos2θ

L2I 2J = P33

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$1750

$200

Search for Quarks

Friday, May 19, 1967

Beyond CQM

gg

1,0

Constituent Counting Rule:

A12∝1/Q3

A32∝1/Q3

GM* ∝1/Q4

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Map the NN* electrocouplings as a function of photon virtuality with a combined analysis of electroproduction channels

Access active degrees of freedom at various distances

Explore the non-perturbative strong interactions responsible for nucleon formation and the origin of quark confinement

N* Program in CLAS

Investigate the origin of 98% of nucleon mass through DCSB

JLABCarnegie Mellon

Univ. of MarylandTrinity College (Dublin)

DSE FrameworkDCSBLCSR

Dist. Amplitudes

Form Factors

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p+ in the resonance region

Q2: 1.6 5.4 GeV2

W: 1.1 1.8 GeV58000 data points

High Q2 p electroproduction

e

e’

γv N*, △*

p+, p

n, p’p

Single p+, p production p in the Delta

Q2: 2 6.5 GeV2

W: 1.1 1.4 GeV7200 data points

Missing:p in the resonance region

Q2: 2.0 6.5 GeV2

W: 1.1 2.0 GeV~75000 data points

No prior data

h electroproduction from the same dataset1.1 W 2.0

0

Q

2

6

M. Ungaro Phys.Rev.Lett.97:112003,2006

K. Park Phys.Rev.C77:015208,2008I.G. Aznauryan Phys.Rev.C78:045209,2008

Nick Markov, UCONN

This analysis

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Experiment Overview

N

s s(W,Q2,cos(q*))

ds/dWp = sT + esL + esTTcos2f + √2e(e+)sLTcosf + h√2e(e-1)sLT’sinf

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Detect:Electron, Proton

Will Extract:

• Cross sections, Structure Functions

• Beam Spin Asymmetries• Helicity amplitudes and their

Q2 dependence

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B.H. Separation:The typical angle between the emitted photon and the electron in B.H. processes is θ m/E∼

Analysis Overview

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45 bins in W, DW=20 MeV7 bins in Q2 DQ2/Q2 ~ 0.18

10 bins in cos(q*)24, 48, 96 bins in f*

W [GeV]

Q2

[GeV

2 ]

W=1.59 Q2=3.5

Total: 75600 CS points

p0 Analysis Overview

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Preliminary Results

aTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

ds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

240 pointsout of 75K

CLAS P

relim

inary

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Preliminary Resultsds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

240 pointsout of 75K

CLAS P

relim

inaryaTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

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Preliminary Resultsds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

CLAS P

relim

inary

aTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

APS Meeting, April 30 2011 Williamsburg, VA 13M.Ungaro

Preliminary Resultsds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

CLAS P

relim

inary

aTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

APS Meeting, April 30 2011 Williamsburg, VA 14M.Ungaro

Preliminary Resultsds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

CLAS P

relim

inary

aTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

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Preliminary Resultsds/dW* = sT + esL + esTTcos2f + √2e(e+1)sLTcosf

CLAS P

relim

inary

aTL +ess

sLT =b

sinθ 2ε (ε +1)

TTT

cqe

s 2sin

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Summary, OutlookCL

AS Pre

limina

ry

To do list:JANR, DR (Being Done)SAID analysis

Review:p0 (by this summer)h (by this fall/winter)

The combined analysis of single and double meson channels is key to the N* program and to provide a high definition picture of the nucleon

Explore the non-perturbative strong interactions responsible for nucleon formation and the origin of quark confinement

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Backup Slides

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exclurad (Afanasev, Akushevich, Burkert, Joo)

Input: Exclusive cross section

No peaking approximation No soft-hard photon discrimination Radiation of 4 SF with angular dependence of each one (exclusive electroproduction)

Radiative Correction

W=1.29

Analysis Overview

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exclurad (Afanasev, Akushevich, Burkert, Joo)

Input: Exclusive cross section

No peaking approximation No soft-hard photon discrimination Radiation of 4 SF with angular dependence of each one (exclusive electroproduction)

Radiative Correction

W=1.63

Analysis Overview

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S1 S2

S3

S5 S6

S4

Normalization check: Good electron PID, fiducial cut Good acceptance from simulation Vertex Correction, Cuts Kinematic Corrections Elastic Scattering Inclusive scattering

Data Keppel Brasse

W [GeV]

W [GeV]

W [GeV]

W [GeV]

W [GeV]

W [GeV]

Analysis Overview

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Data:

Electron ID Proton ID Vertex Correction, Selections Electron Fiducial Cut Proton Fiducial Cut Electron Momentum Correction Proton Momentum Correction Normalization Check Radiative Correction Bin Averaging Correctionp0, h selection

Simulation:

Electron ID Proton ID Vertex Correction, Selections Electron Fiducial Cut Proton Fiducial Cut Timing Resolution Match Momentum Resolution Match Acceptance Correction

To do list:Finalize Systematic ErrorsCollaboration ReviewAmplitudes extraction (JANR, DR, SAID)

Analysis Overview

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24 f bins200M Generated Events

MAID2007AAO_RAD

Electron ID Proton ID Vertex Correction, Selections Electron Fiducial Cut Proton Fiducial Cut Timing Resolution Match Momentum Resolution Match Drift Chamber Efficiencies p0 selection

Analysis Overview

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Analysis Overview

96 f bins200M Generated Events

MAID2007AAO_RAD

Electron ID Proton ID Vertex Correction, Selections Electron Fiducial Cut Proton Fiducial Cut Timing Resolution Match Momentum Resolution Match Drift Chamber Efficiencies p0 selection

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What about h?

eP missing mass2 [GeV2]

p0

h

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What about h?

25 bins in W, DW=20 MeV7 bins in Q2 DQ2/Q2 ~ 0.18

10 bins in cos(q*)24 bins in f*

W [GeV]

Q2

[GeV

2 ]

W=1.53 Q2=3.0

Total: 43750 points

h

W [GeV]

Q2

[GeV

2 ]

W=1.65 Q2=3.0

W [GeV]

Q2

[GeV

2 ]

W=1.79 Q2=3.0

W [GeV]

Q2

[GeV

2 ]

W=1.95 Q2=3.0