CLAS Physics Database

E99-107 CLAS experiment

Spokespersons
V. D. Burkert, R. Minehart
Year
2005
Abstract
An extensive program is currently underway at the Jefferson Laboratory to study the excitation of nucleon resonances with electromagnetic probes. The CEBAF Large Acceptance Spectrometer (CLAS) is well suited for the study of a broad rang of kinematics in the invariant mass W, photon virtuality Q2, and has nearly complete angular coverage for the hadronic resonance decays. Until recently most of the resonance studies using electron beams have employed the single π0$ or η channels to study the lower mass states, especially the Δ(1232) and the S11(1535). Many of the higher mass resonances are isospin 1/2 states and couple more strongly to the n π+ channel. The extraction of resonance information requires the analysis of the angular distribution in the hadronic center-of-mass system. With CLAS this channel becomes now fully accessible as the π+ is measured in nearly the full azimuthal and polar angular ranges. High statistics data have been taken with a variety of beam energies ranging from 1.5 GeV to 5.75 GeV covering a Q2 range from 0.3 to 3 GeV2, and the full resonance mass range. The electron beam was polarized at about 70%. Data on invariant mass distributions for $\vec{e}p -> e'π+n is presented in this thesis. Three resonant enhancement can clearly be identified in all data sets belonging to the Δ(1232), D13(1520), and F15(1680) resonances. The latter two exhibit Q2-dependences which are quite different from the Δ(1232).
Comment
asymmetry
Quantities
ALU D coeff

Measurements

ID Quantity Beam Target Final state Q2min,
GeV2
Q2max,
GeV2
Wmin,
GeV
Wmax,
GeV
E76M1 ALU e p π+n 1.56 1.87 1.1 1.14
E76M2 ALU e p π+n 1.87 2.23 1.1 1.14
E76M3 ALU e p π+n 2.23 2.66 1.1 1.14
E76M4 ALU e p π+n 2.66 3.17 1.1 1.14
E76M5 ALU e p π+n 1.56 1.87 1.14 1.18
E76M6 ALU e p π+n 1.87 2.23 1.14 1.18
E76M7 ALU e p π+n 2.23 2.66 1.14 1.18
E76M8 ALU e p π+n 2.66 3.17 1.14 1.18
E76M9 ALU e p π+n 3.17 3.79 1.14 1.18
E76M10 ALU e p π+n 1.56 1.87 1.22 1.26
E76M11 ALU e p π+n 1.87 2.23 1.22 1.26
E76M12 ALU e p π+n 2.23 2.66 1.22 1.26
E76M13 ALU e p π+n 2.66 3.17 1.22 1.26
E76M14 ALU e p π+n 3.17 3.79 1.22 1.26
E76M15 ALU e p π+n 1.56 1.87 1.26 1.3
E76M16 ALU e p π+n 1.87 2.23 1.26 1.3
E76M17 ALU e p π+n 2.23 2.66 1.26 1.3
E76M18 ALU e p π+n 2.66 3.17 1.26 1.3
E76M19 ALU e p π+n 3.17 3.79 1.26 1.3
E76M20 ALU e p π+n 1.56 1.87 1.3 1.34
E76M21 ALU e p π+n 1.87 2.23 1.3 1.34
E76M22 ALU e p π+n 2.23 2.66 1.3 1.34
E76M23 ALU e p π+n 2.66 3.17 1.3 1.34
E76M24 ALU e p π+n 3.17 3.79 1.3 1.34
E76M25 ALU e p π+n 1.56 1.87 1.34 1.38
E76M26 ALU e p π+n 1.87 2.23 1.34 1.38
E76M27 ALU e p π+n 2.23 2.66 1.34 1.38
E76M28 ALU e p π+n 2.66 3.17 1.34 1.38
E76M29 ALU e p π+n 3.17 3.79 1.34 1.38
E76M30 ALU e p π+n 1.56 1.87 1.38 1.42
E76M31 ALU e p π+n 1.87 2.23 1.38 1.42
E76M32 ALU e p π+n 2.23 2.66 1.38 1.42
E76M33 ALU e p π+n 2.66 3.17 1.38 1.42
E76M34 ALU e p π+n 3.17 3.79 1.38 1.42
E76M35 ALU e p π+n 1.56 1.87 1.46 1.5
E76M36 ALU e p π+n 1.87 2.23 1.46 1.5
E76M37 ALU e p π+n 2.23 2.66 1.46 1.5
E76M38 ALU e p π+n 2.66 3.17 1.46 1.5
E76M39 ALU e p π+n 3.17 3.79 1.46 1.5
E76M40 ALU e p π+n 1.56 1.87 1.5 1.54
E76M41 ALU e p π+n 1.87 2.23 1.5 1.54
E76M42 ALU e p π+n 2.23 2.66 1.5 1.54
E76M43 ALU e p π+n 2.66 3.17 1.5 1.54
E76M44 ALU e p π+n 3.17 3.79 1.5 1.54
E76M45 ALU e p π+n 1.56 1.87 1.54 1.58
E76M46 ALU e p π+n 1.87 2.23 1.54 1.58
E76M47 ALU e p π+n 2.23 2.66 1.54 1.58
E76M48 ALU e p π+n 2.66 3.17 1.54 1.58
E76M49 ALU e p π+n 3.17 3.79 1.54 1.58
E76M50 ALU e p π+n 1.56 1.87 1.58 1.62
E76M51 ALU e p π+n 1.87 2.23 1.58 1.62
E76M52 ALU e p π+n 2.23 2.66 1.58 1.62
E76M53 ALU e p π+n 2.66 3.17 1.58 1.62
E76M54 ALU e p π+n 3.17 3.79 1.58 1.62
E76M55 ALU e p π+n 1.56 1.87 1.62 1.66
E76M56 ALU e p π+n 1.87 2.23 1.62 1.66
E76M57 ALU e p π+n 2.23 2.66 1.62 1.66
E76M58 ALU e p π+n 2.66 3.17 1.62 1.66
E76M59 ALU e p π+n 3.17 3.79 1.62 1.66
E76M60 ALU e p π+n 1.56 1.87 1.66 1.7
E76M61 ALU e p π+n 1.87 2.23 1.66 1.7
E76M62 ALU e p π+n 2.23 2.66 1.66 1.7
E76M63 ALU e p π+n 2.66 3.17 1.66 1.7
E76M64 ALU e p π+n 3.17 3.79 1.66 1.7
E76M65 D coeff e p π+n 1.715 3.48 1.12 1.68