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Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science...

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Form Factor BATES  New technique: polarized beam and target  Exploits unique features of BLAST »internal target: low dilution, fast spin reversal »large acceptance: simultaneous measurement of all Q 2 points »symmetric detector: ratio measurement  Different systematics »insensitive to P b and P t  Q 2 = 0.07 – 0.9 (GeV/c) 2 »overlap with JLab data and RpEX (future exp. at Bates to measure r p )
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Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for the BLAST collaboration
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Page 1: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Precision Measurement of GE

p/GMp with BLAST

Chris CrawfordMIT Laboratory for Nuclear Sciencefor the BLAST collaboration

Page 2: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Motivation

†Nucleon Electromagnetic Form Factors, Haiyan Gao, Int. J. of Mod. Phys. E, 12,

No. 1, 1-40(Review) (2003)

Page 3: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Form Factor Ratio @ BATES

New technique: polarized beam and target Exploits unique features of BLAST

» internal target: low dilution, fast spin reversal» large acceptance: simultaneous measurement of all Q2 points » symmetric detector: ratio measurement

Different systematics » insensitive to Pb and Pt

Q2 = 0.07 – 0.9 (GeV/c) 2 » overlap with JLab data

and RpEX (future exp.at Bates to measure rp)

Page 4: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Asymmetry Super-ratio Method

Polarized cross section

Super-ratio

Page 5: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Detector Package

BLAST CoilsBackward-Angle TOFTOF ScintillatorsWire ChambersCerenkov DetectorsNeutron DetectorsLADS Detectors

Page 6: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

BLAST

Page 7: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Wire Chamber Tracking

Garfield drift time simulation Newton-Rhapson track fitter

200μm resolution 20:1 signal to noise ratio

Page 8: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Preliminary Data

Theta Resolution

Beam AsymmetryYield

Page 9: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

Projected Results

Statistics» A1, A2

Systematics» θ*

1, θ*2

Δp, Δθ, Δβ

Errors are minimized as a function of β (target spin angle)

Page 10: Precision Measurement of G E p /G M p with BLAST Chris Crawford MIT Laboratory for Nuclear Science for…

BLAST Collaboration

R. Alarcon, E. Geis, J. Prince, B. Tonguc, A. YoungArizona State University

 J. Althouse, C. D’Andrea, A. Goodhue, J. Pavel, T. Smith,

Dartmouth CollegeT. Akdogan, W. Bertozzi, T. Botto, M. Chtangeev,

B. Clasie, C. Crawford, A. Degrush, K. Dow, M. Farkhondeh, W. Franklin, S. Gilad,

D. Hasell, E. Ilhoff, J. Kelsey, H. Kolster, A. Maschinot, J. Matthews, N. Meitanis,

R. Milner, R. Redwine, J. Seely, S.Sobczynski, C. Tschalaer, E. Tsentalovich,

W. Turchinetz, Y. Xiao, H. Xiang, C. Zhang, V. Ziskin, T. Zwart

Massachusetts Institute of TechnologyBates Linear Accelerator Center

D. Dutta, H. Gao, W. XuDuke University

J. Calarco, W. Hersman, M. Holtrop, O. Filoti, P. Karpius, A. Sindile, T. Lee

University of New Hampshire 

J. RapaportOhio University 

K. McIlhany, A. MosserUnited States Naval Academy

 J. F. J. van den Brand, H. J. Bulten, H. R. Poolman

Vrije Universitaet and NIKHEF 

W. Haeberli, T. WiseUniversity of Wisconsin


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