High-precision measurement of the proton elastic form factor ratio mu pGE/GM at low Q super(2)
We report a new, high-precision measurement of the proton elastic form factor ratio mu pGE/GM for the four-momentum transfer squared [inline image]. The measurement was performed at Jefferson Lab (JLab) in Hall A using recoil polarimetry. With a total uncertainty of approximately 1%, the new data cl...
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Published in | Physics letters. B Vol. 705; no. 1-2; pp. 59 - 64 |
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Main Authors | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format | Journal Article |
Language | English |
Published |
03.11.2011
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Subjects | |
Online Access | Get full text |
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Summary: | We report a new, high-precision measurement of the proton elastic form factor ratio mu pGE/GM for the four-momentum transfer squared [inline image]. The measurement was performed at Jefferson Lab (JLab) in Hall A using recoil polarimetry. With a total uncertainty of approximately 1%, the new data clearly show that the deviation of the ratio mu pGE/GM from unity observed in previous polarization measurements at high Q super(2) continues down to the lowest Q super(2) value of this measurement. The updated global fit that includes the new results yields an electric (magnetic) form factor roughly 2% smaller (1% larger) than the previous global fit in this Q super(2) range. We obtain new extractions of the proton electric and magnetic radii, which are [inline image] and [inline image]. The charge radius is consistent with other recent extractions based on the electron-proton interaction, including the atomic hydrogen Lamb shift measurements, which suggests a missing correction in the comparison of measurements of the proton charge radius using electron probes and the recent extraction from the muonic hydrogen Lamb shift. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 content type line 23 ObjectType-Feature-2 |
ISSN: | 0370-2693 |
DOI: | 10.1016/j.physletb.2011.10.002 |