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16 March 2009 EuNPC, Bochum 1 Kaon Photoproduction Results from CLAS D. G. Ireland

Kaon Photoproduction Results from CLAS

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Kaon Photoproduction Results from CLAS. D. G. Ireland. “Missing” Baryon Resonances. Resonance Hunting…. Total Cross-sections + differential cross-sections + Partial Wave Analysis +. D(1232) P 33 N(1440)P 11 N(1520)D 13 N(1535)S 11 D (1600)P 33. Cross section. - PowerPoint PPT Presentation

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Page 1: Kaon Photoproduction Results from CLAS

16 March 2009 EuNPC, Bochum 1

Kaon Photoproduction Results from CLAS

D. G. Ireland

Page 2: Kaon Photoproduction Results from CLAS

2

“Missing” Baryon Resonances

Page 3: Kaon Photoproduction Results from CLAS

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Resonance Hunting…

Mostly done with N scattering or photoproductionMissing resonances may decay through other channels

Total Cross-sections+ differential cross-sections+ Partial Wave Analysis + ...

0.5 1.0 1.5

Cro

ss s

ecti

on

E (GeV)

P33

N(1440)P11

N(1520)D13

N(1535)S11

(1600)P33

Page 4: Kaon Photoproduction Results from CLAS

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Meson Photoproduction Cross Sections

Page 5: Kaon Photoproduction Results from CLAS

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Evidence for new resonance?

With D13

Without D13

Mart & Benhold, Phys. Rev. C 61 012201(R) (1999)

Page 6: Kaon Photoproduction Results from CLAS

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Transversity Amplitudes

b1 = 1/2[(S1 + S2) + i(N - D)] p

K }} p

K }} p

K }} p

K }}

b2 = 1/2[(S1 + S2) - i(N - D)]

b3 = 1/2[(S1 - S2) - i(N + D)]

b4 = 1/2[(S1 - S2) + i(N + D)]

N, S1,S2, D: Helicity Amplitudes

Page 7: Kaon Photoproduction Results from CLAS

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Experimental Observables

Page 8: Kaon Photoproduction Results from CLAS

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p →K Reaction Kinematics

proton

zy

x

z

y

x

zy

x

p

. .c m

K

proton

K+

zzzz

yy

xxxx

CPOP

TPP

CPOP

Pd

d

cos2sincos

2coscoscos

cos2sincos

2cos10

Cross Section without target polarisationHyperon is self-analysing

Page 9: Kaon Photoproduction Results from CLAS

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CEBAF at Jefferson Laboratory

Page 10: Kaon Photoproduction Results from CLAS

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CLAS

Page 11: Kaon Photoproduction Results from CLAS

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Tagged Photons at CLAS

• E = E0 – E’

• Circular Polarisation: polarised electron beam, amorphous radiator

• Linear polarisation: Crystal (diamond) radiator

Page 12: Kaon Photoproduction Results from CLAS

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p →K Cross Section Measurements

R. Bradford et al., Phys. Rev. C 73, 035202 (2006).

Page 13: Kaon Photoproduction Results from CLAS

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Recoil Polarisation

proton

zy

x

z

y

x

zy

x

p

. .c m

K

proton

K+

zzzz

yy

xxxx

CPOP

TPP

CPOP

Pd

d

cos2sincos

2coscoscos

cos2sincos

2cos10

Hyperon is self-analysing

Page 14: Kaon Photoproduction Results from CLAS

14

Recoil Polarisation (P) p→K

Guidal, Laget, VanderhaeghenGuidal, Laget, Vanderhaeghen

GENTGENT Kaon-MAIDKaon-MAID

J. McNabb J. McNabb et alet al. (CLAS) Phys. Rev. C . (CLAS) Phys. Rev. C 6969, 042201 (2004)., 042201 (2004).

Page 15: Kaon Photoproduction Results from CLAS

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Beam-Recoil Double Polarisation (Cx’,Cz’)

proton

zy

x

z

y

x

zy

x

p

. .c m

K

proton

K+

zzzz

yy

xxxx

CPOP

TPP

CPOP

Pd

d

cos2sincos

2coscoscos

cos2sincos

2cos10

Hyperon is self-analysing

Page 16: Kaon Photoproduction Results from CLAS

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Polarisation

2 2 2x zR P C C

→ fully polarised

R. Bradford et al., Phys. Rev. C 75, 035205 (2007).

Page 17: Kaon Photoproduction Results from CLAS

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Photon Beam Asymmetry ()

proton

zy

x

z

y

x

zy

x

p

. .c m

K

proton

K+

zzzz

yy

xxxx

CPOP

TPP

CPOP

Pd

d

cos2sincos

2coscoscos

cos2sincos

2cos10

Page 18: Kaon Photoproduction Results from CLAS

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Linear Polarisation analysis

Photon Linear Polarisation Particle ID

Thesis work of Craig Paterson (Glasgow)

Page 19: Kaon Photoproduction Results from CLAS

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p →K Photon Beam Asymmetry

Page 20: Kaon Photoproduction Results from CLAS

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p →K Photon Beam Asymmetry

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Page 21: Kaon Photoproduction Results from CLAS

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p →K Photon Beam Asymmetry

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Page 22: Kaon Photoproduction Results from CLAS

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Beam-Recoil Double Polarisation (x,Oz)

proton

zy

x

z

y

x

zy

x

p

. .c m

K

proton

K+

zzzz

yy

xxxx

CPOP

TPP

CPOP

Pd

d

cos2sincos

2coscoscos

cos2sincos

2cos10

Page 23: Kaon Photoproduction Results from CLAS

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p →K Extracting Ox and Oz

Page 24: Kaon Photoproduction Results from CLAS

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p →K Beam-Recoil Ox and Oz

O x

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O z

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Page 25: Kaon Photoproduction Results from CLAS

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Experimental Observables

Page 26: Kaon Photoproduction Results from CLAS

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Outlook – Deuterium Target

• Data taking completed

• Currently being analysed

• Data on quasifree neutron and proton

• Circular and Linear Polarisation

Page 27: Kaon Photoproduction Results from CLAS

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Outlook – FROzen Spin Target (FROST)

Target can be longitudinally or transversely polarised

• “Complete” measurement possible• First part of run complete• Undergoing calibration• Second period to run soon…

Page 28: Kaon Photoproduction Results from CLAS

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Conclusions

Kaon Photoproduction results from CLAS:

• Published results: , P, Cx, Cz

• Preliminary results: , T, Ox, Oz

In the near future:

• Same set of results for 2H target (quasifree neutron and proton)

• “Complete” results (FROST)

Next few years:

• Complete set on 2H and p (HDIce)

Page 29: Kaon Photoproduction Results from CLAS

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Backup Slides…

Page 30: Kaon Photoproduction Results from CLAS

30

Resonances in Quark Models

Page 31: Kaon Photoproduction Results from CLAS

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Kaon Photoproduction

Page 32: Kaon Photoproduction Results from CLAS

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Contributing Processes

+ channel coupling…

Page 33: Kaon Photoproduction Results from CLAS

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Helicity Amplitudes

N No overall helicity flip = |–p |

p

K }}S1 Single helicity flip

p

K }}S2 Single helicity flip

p

K }}D Double helicity flip

p

K }}

Page 34: Kaon Photoproduction Results from CLAS

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Cross Section Measurements

R. Bradford et al., Phys. Rev. C 73, 035202 (2006).

Page 35: Kaon Photoproduction Results from CLAS

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Cross Section Measurements

R. Bradford et al., Phys. Rev. C 73, 035202 (2006).

Page 36: Kaon Photoproduction Results from CLAS

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Cross Section Measurements

R. Bradford et al., Phys. Rev. C 73, 035202 (2006).

Page 37: Kaon Photoproduction Results from CLAS

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Beam-Recoil Double Polarisation Cz

R. Bradford et al., Phys. Rev. C 75, 035205 (2007).

Saclay, Argonne, PittsburghSaclay, Argonne, Pittsburgh

Bonn, Giessen, GatchinaBonn, Giessen, GatchinaKaon-MAIDKaon-MAID

Regge+ResonanceRegge+Resonance GENTGENT

Shklyar Shklyar Lenske Lenske MoselMosel

Page 38: Kaon Photoproduction Results from CLAS

38

Beam-Recoil Double Polarisation Cx

GENTGENT

Saclay, Argonne, PittsburghSaclay, Argonne, Pittsburgh

Bonn, Giessen, GatchinaBonn, Giessen, Gatchina

Kaon-MAIDKaon-MAID

Regge+ResonanceRegge+Resonance

Shklyar Lenske Shklyar Lenske MoselMosel

R. Bradford et al., Phys. Rev. C 75, 035205 (2007).

Page 39: Kaon Photoproduction Results from CLAS

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Photon Beam Asymmetry

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Photon Beam Asymmetry

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Photon Beam Asymmetry

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Recoil - Comparison

g8b

Prev CLAS

GRAAL

~Factor of 4 increase in statistics from best previous measurements

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