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K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009
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K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Jan 18, 2018

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Dorcas Webb

CLAS data (2007) I. Hleiqawi et al., Phys. Rev. C 76 (2007) E.
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Page 1: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

K* photoproduction from g11

K. HicksOhio University

HSG meeting, 12 June 2009

Page 2: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

OUTLINE

• Review of K* photoproduction data• Theoretical interest• Presentations of preliminary analysis

(Ohio students).

Page 3: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

CLAS data (2007)I. Hleiqawi et al., Phys. Rev. C 76 (2007) 039905E.

Page 4: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

New Data

Page 5: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

ComparisonRed (open) = CLAS, Black (solid) = TAPS

Note the strong forward-peaking of TAPS data at higher photon energies.

Page 6: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

K*+ (CLAS preliminary)L. Guo and D. Weygand, N* 2005 Conf., hep-ex/060101.

K*+ shown by the RED points, quoted with 20% uncertainty.

Page 7: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Theory calculations: K*0+

Y. Oh and H. Kim, hep-ph/0605105.

Model I (blue): no kappa form factor; Model II (red): with kappa form factor.

Page 8: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Theory comparison: K*+Y. Oh and H. Kim, PRC 73:065202 (2006).

Full calculation (solid line)K+ t-channel only (dashed)

Regge model (kaon trajectory)

Page 9: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Theory: a) K*+ , b) K*0+

SOLID BLUE: no kappa form factor; DASHED RED: with kappa form factor

Y. Oh and H. Kim, hep-ph/0605105.

Page 10: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

New: K*+ Photoproduction

• Analysis by Wei Tang (Ohio grad student)• Using g11 data set• Detecting: pair plus another .• Missing mass of Lambda and Sigma• Acceptance using fsgen + GSIM• Absolute normalization (new)

– Checked using K+ photoproduction.

Page 11: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Details on data and cuts

• Runs 43526 – 44107 used (E=4.02 GeV).• Bad paddles were removed.• Photon identified using 1.0 ns time cuts.• Particle ID from SC and tagger time cuts.• Standard fiducial and vertex cuts applied.• Sideband subtraction to isolate K0 events.• K*+ mass cut from 0.80-0.98 GeV.

Page 12: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Details on Normalization

• Used gflux method to get photons.• Applied “trigger efficiency” map.

– Mike Williams supplied this method.• Applied “dead time” correction.

– INFN’s “current dependent correction” (18%)• No additional correction for start counter.

– Lambda decay products not needed to fire the trigger (a la Mike McCracken).

Page 13: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

K0 mass peak

Page 14: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

K*+ Mass

Left s.b.

Right s.b.

K0 peak

K0 peak minus sidebands

Page 15: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

K*+ Missing Mass

K*+ peak minusSidebands.

Page 16: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

MM: one kinematic binE=1.6-1.7 GeV and -1 < cos < -.078

Page 17: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

MM: higher-E binE = 2.3-2.4 GeV and -0.11 < cos < 0.11

Page 18: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Sample fit using gaussians

Page 19: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

p K*+ Cross Sections

E (GeV)

W (GeV)

Units: b

Page 20: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Check: K0+ cross sections

Page 21: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Previous K0+ dataE = 1.65 GeV

B. Carnahan, PhD, Catholic U. (pub. in Sarantsev et al., Eur. Phys. J. A25, 411 (2005).

SAPHIR data(not shown) also published.

Page 22: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Status of K*+ analysis

• Preliminary differential cross sections OK.• Next step: systematic studies.• Just started: Lambda decay asymmetry

– Statistics reduced by about ¼.• Plan:

– Finish cross sections (1 month)– Preliminary Lambda asymmetries (1 month)– Write analysis note by end of summer.

Page 23: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Status of K*0+ analysis

• This analysis is at a similar stage.– Normalization check requires more work

• This is a “redo” of the published data.– I. Hleiqawi et al. (CLAS publication).

• Overlap with nucleon resonances– Final state requires a PWA-like analysis.– This procedure was done for Hleiqawi data,

but now we have good statistics!

Page 24: K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.

Summary

• K*0 and K*+ final states are nearly final. – Normalization issues took a lot of time.– Good agreement with previous data, but much

higher precision.– For K*+, can also do asymmetry.

• Plan to have analysis note by the end of the summer.– This will be part of the PhD thesis of W. Tang.