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HLAB meeting paper 2011/1/18 T.Gogami CLAS ( CEBAF Large Acceptance Spectrometer ) Clam shell is open
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Paper
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Abstract
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Introduction
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In this article CLAS g11a data set (5/7/2004 – 7/29/2004) – γp → K + Λ differential cross section – Λ recoil polarization (P Λ )
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Experimental setup
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Tagger ΔE/E ≈ 10 -3 MAGNET photon electron 4.023 [GeV] gravity 6.06 [m] E-plane (384) T-plane (61) 4mm thickness 20mm thickness σ time ≈ 110 [ps] ( intrinsic resolution 2×10 -4 ) Radiator Gold foil (10 -4 rad. length ) The bremsstrahlung tagged photon beam in Hall B at JLab, D.I. Sober, Nuclear Instruments and Methods in Physics Research A 440 (2000) 263}284
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CLAS CLAS ( CEBAF Large Acceptance Spectrometer )
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Toroidal Magnet Superconducting toroidal magnet – Temperature : 4.4 [K] (Liquid He) – 1920 [A], 1.8 [T] ( Max : 3861[A], 3.5 [T] ) B B People
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Toroidal Magnet Superconducting toroidal magnet – Temperature : 4.4 [K] (Liquid He) – 1920 [A], 1.8 [T] ( Max : 3861[A], 3.5 [T] ) B B Magnetic field in midplane between two coils
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CLAS (CEBAF Large Acceptance Spectrometer) Target : Liquid H 2 (cylindrical Kapton chamber 40cm L × 4cm D ) Momentum resolution ~ 5×10 -3 Trigger – tagger × 2/6 ( Start × TOF ) DAQ rate ~ 5 [kHz] Tracking ~300 [μm] Timing (~80 – 160 [ps]) γp → K + Λ
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Spec The CEBAF large acceptance spectrometer (CLAS), B.A. Mecking, Nuclear Instruments and Methods in Physics Research A 503 (2003) 513–553
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DATA and EVENT selection Want to see “γp → K + Λ” – γp → K + pπ - ・・・ Tree track analysis – γp → K + p(π - ) ・・・ Two track analysis +28% of full set 1.Momentum, Energy correction 2.Loose cut – Missing mass, Invariant mass 3.Kinematic fit confidence level cut
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Confidence level cut Λ Λ σ ~ 8 [MeV/c 2 ] Confidence level The effect of the confidence level cut is dramatic ! Missing mass
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Background reduction Cut misidentified particles
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Background reduction (2) 1.Given event “i” 2.100 neighbors 3.Missing mass 4.Maximum likelihood fit – Gaussian signal (s) – linear background (b) 5.Quality factor weighted by (1-Q) All events Missing Mass √s = 2.105 GeV bin
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Other consideration Detector acceptance Extracting P Λ Normalization
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Systematic Uncertainties
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Result
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Mandelstam variables proton photon Kaon Lambda
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Cross section Count Corrected Number of photons Target Binning width Acceptance
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Cross section( イ ) Red : two track analysis Blue : three track analysis Error Statistic Acceptance
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Cross section( ロ ) Red : two track analysis Blue : three track analysis Error Statistic Acceptance
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Cross section( ハ ) Red : two track analysis Blue : three track analysis Error Statistic Acceptance
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Agreement between the two analysis Agreement between the two analysis, Very little systematic offset Consistent within statistical and acceptance uncertainties
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Weighted mean differential cross sections Weighted mean differential cross sections : i = 2,3 j = 2,3 ρ = 0.28 For kinematic points where only a two-track measurement exists, Cross section : its value Uncertainty : scaling by 1 + |μ| = 1.136
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Cross section γp → K + Λ Red : CLAS Blue : previous CLAS Green : SAPHIR Measurement of p->K+ Λ and p->K+ Σ 0 at photon energies up to 2.6 GeV, K.H. Glander, arXiv:nucl-ex/0308025v1 26 Aug 2003 The γ p → K+ and γ p → K+0 reactions at forward angles with photon energies from 1.5 to 2.4 GeV, M. Sumihama, PHYSICAL REVIEW C 73, 035214 (2006) Measurement of the γ p → K+ reaction at backward angles, K. Hicks, PHYSICAL REVIEW C 76, 042201(R) (2007) LEPS SAPHIR
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Model comparison ( イ ) K-MAID (fit with SAPHIR) – K+,K*(892),K 1 (1270) RPR (fit with p CLAS) – K+ Regge trajectory, K* Regge trajectory – N(1650)S 11,N(1710)P 11, N(1720)P 13,N(1900)P 13, missing D 13 – Forward angle Bonn-Gatchina (fit with p CLAS) – Partial wave analysis
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Model comparison ( ロ ) K-MAID (fit with SAPHIR) – K+,K*(892),K 1 (1270) RPR (fit with p CLAS) – K+ Regge trajectory, K* Regge trajectory – N(1650)S 11,N(1710)P 11, N(1720)P 13,N(1900)P 13, missing D 13 – Forward angle Bonn-Gatchina (fit with p CLAS) – Partial wave analysis
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Model comparison ( ハ ) K-MAID (fit with SAPHIR) – K+,K*(892),K 1 (1270) RPR (fit with p CLAS) – K+ Regge trajectory, K* Regge trajectory – N(1650)S 11,N(1710)P 11, N(1720)P 13,N(1900)P 13, missing D 13 – Forward angle Bonn-Gatchina (fit with p CLAS) – Partial wave analysis
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Conclusion
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END
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Start counters
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Introduction (γp → K + Λ) γp → K + Λ – Polarization Pseudoscalar nature of the K+ Self-analyzing decay of the Λ – Isospin structure of the final state Allows coupling only to I=1/2 N* (not the I=3/2 Δ*)
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PΛPΛ CLAS : Blue SAPHIR2004 : Green GRALL2007 : Black
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Tagger
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