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Kaon Production on the Nucleon. D. G. Ireland. Kaon Photoproduction. very high momentum transfer (pQCD). Baryon Summary Table (PDG 2008). Baryon Summary Table (PDG 2012). “Missing” Baryon Resonances. Resonances in Quark Models. Baryon Spectrum on the Lattice.
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Kaon Production on the Nucleon D. G. Ireland Rome, September 30 – October 4, 2013
KaonPhotoproduction very high momentum transfer (pQCD)
Baryon Spectrum on the Lattice Excited state baryon spectroscopy from lattice QCD. Edwards, Dudek, Richards, Wallace Phys. Rev. D 84, 074508 (2011)
Resonance Hunting… Total Cross-sections + differential cross-sections + Partial Wave Analysis + ... • Mostly done with pN scattering • Missing resonances may decay through other channels
g*p →KYElectroproduction Cross Section: Hyperon is self-analysing … with electron polarization… proton
g*p →KLSeparated Structure Functions D. Carman et al. (CLAS), Phys. Rev. C 87, 025204, 2013
g*p →KSSeparated Structure Functions D. Carman et al. (CLAS), Phys. Rev. C 87, 025204, 2013
g*p →KLQ2 Dependence D. Carman et al. (CLAS), Phys. Rev. C 87, 025204, 2013
g*p →KSQ2 Dependence D. Carman et al. (CLAS), Phys. Rev. C 87, 025204, 2013
gp →KLPhotoproduction K+ proton Hyperon is self-analysing proton
CLAS results γp→K+Λ→K+pπ- Bonn-Gatchina Coupled Channel Analysis, A.V. Anisovich et al, EPJ A48, 15 (2012) (Includes nearly all new photoproduction data) M. McCracken et al. (CLAS), Phys. Rev. C 81, 025201, 2010
CLAS results γp→K+Λ→K+pπ- Bonn-Gatchina Coupled Channel Analysis, A.V. Anisovich et al, EPJ A48, 15 (2012) (Includes nearly all new photoproduction data) M. McCracken et al. (CLAS), Phys. Rev. C 81, 025201, 2010 R. Bradford et al. (CLAS), Phys.Rev. C75, 035205, 2007
Fit to K+Λ with PDG2010 states < 2 GeV EBAC group: Kamano, Nakamura, Lee, Sato (2012) Includes ***, **** states 1965 1965 PDG states insufficient to fit KΛ data
Evidence for new N* states and couplings Bonn-Gatchina Analysis – A.V. Anisovich et al., EPJ A48, 15 (2012) (First coupled-channel analysis that includes nearly all new photoproduction data)
N* K+L Amplitude Analysis Ref: Scaling and Resonances in Elementary K+L Photoproduction [R.A. Schumacher and M.M. Sargsian, Phys. Rev. C 83, 025207 (2011)] Compute coherent total amplitude: Fit to observed angular distributions: Test various resonance sets vs. mass Free parameters: mass, width, couplings Spin observables neglected Sensitive to smaller contributions to reaction Structure appears when scaling utilised.
Linearly Polarized Photons Diamond radiator mounted on target ladder Polarization determined by fit to coherent bremsstrahlung spectrum Alignment checked by observing symmetric “Stonehenge Plot” Radiator in goniometer
FROzen Spin Target (FROST) Target can be longitudinally or transversely polarised [See talk by Barry Ritchie]
Transversity Amplitudes } b1 = < | M | > } b2 = < | M | > } b3 = < | M | ‖> } b4 = < | M | ‖>
Comparison with other measurements LEPS LEPS CLAS g8 CLAS g8 GRAAL GRAAL
Beam Asymmetry Comparison Preliminary
Beam-Recoil Comparison Preliminary
Beam Asymmetry Comparison Preliminary
Summary • CLAS has measured a large set of data involving Kaon production • Electroproduction: • Separated structure functions • Q2 dependence – information on form factors • Needs theoretical work • Photoproduction: • Cross sections and recoil polarizations sensitive to N* physics • Exact interpretation of N* spectrum still ambiguous • Outlook: • More polarization data to come (electro- and photo-production) • Results from (quasi-free) neutron • Full set of observables in KL and KS in resonance region • Exciting prospect for N* physics (with results from other channels)