6533b833fe1ef96bd129c40d
RESEARCH PRODUCT
Neutron polarizabilities investigated by quasi-free Compton scattering from the deuteron
F. WissmannR. BeckW. WeihofenO. JahnJ. AhrensMartin SchumacherJ. C. McgeorgeH. J. ArendsK. KossertA.i. L'vovA. NatterAnthony W. ThomasG. CaselottiM. CamenV. Olmos De LeónF. SmendF. ZapadtkaP. JenneweinV.a. Petrun'kinM.i. LevchukP. GrabmayrJrm AnnandG. RosnerB. Seitzsubject
Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaCompton scatteringGeneral Physics and AstronomyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Deuterium0103 physical sciencesNeutronHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentEnergy (signal processing)Astrophysics::Galaxy Astrophysicsdescription
Measuring Compton scattered photons and recoil neutrons in coincidence, quasifree Compton scattering by the neutron has been investigated at MAMI (Mainz) at ${\ensuremath{\theta}}_{\ensuremath{\gamma}}^{\mathrm{lab}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}136\ifmmode^\circ\else\textdegree\fi{}$ in an energy range from 200 to 400 MeV. From the data a polarizability difference of ${\ensuremath{\alpha}}_{n}\ensuremath{-}{\ensuremath{\beta}}_{n}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}9.8\ifmmode\pm\else\textpm\fi{}3.6(\mathrm{stat}{)}_{\ensuremath{-}1.1}^{+2.1}(\mathrm{syst})\ifmmode\pm\else\textpm\fi{}2.2(\mathrm{model})$ in units of ${10}^{\ensuremath{-}4}{\mathrm{fm}}^{3}$ has been determined. In combination with the polarizability sum ${\ensuremath{\alpha}}_{n}+{\ensuremath{\beta}}_{n}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}15.2\ifmmode\pm\else\textpm\fi{}0.5$ deduced from photoabsorption data, the first precise results for the neutron electric and magnetic polarizabilities, ${\ensuremath{\alpha}}_{n}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}12.5\ifmmode\pm\else\textpm\fi{}1.8(\mathrm{stat}{)}_{\ensuremath{-}0.6}^{+1.1}(\mathrm{syst})\ifmmode\pm\else\textpm\fi{}1.1(\mathrm{model})$ and ${\ensuremath{\beta}}_{n}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}2.7\ensuremath{\mp}1.8(\mathrm{stat}{)}_{\ensuremath{-}1.1}^{+0.6}(\mathrm{syst})\ensuremath{\mp}1.1(\mathrm{model})$, are obtained.
year | journal | country | edition | language |
---|---|---|---|---|
2002-01-23 |