6533b85afe1ef96bd12b94ad

RESEARCH PRODUCT

Backward spin polarizabilityγπof the proton

M. CamenF. WissmannR. BeckJ. C. McgeorgeG. CaselottiW. WeihofenV. LisinA.i. L'vovO. JahnM.i. LevchukA. NatterV. Olmos De LeónR. KondratievK. KossertJ. AhrensMartin SchumacherH. J. ArendsF. ZapadtkaP.d. HartyAndy ThomasF. SmendP. JenneweinB. SeitzP. Grabmayr

subject

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsHadronElementary particle01 natural sciencesOrientation (vector space)Nuclear physicsBaryon0103 physical sciences010306 general physicsNucleonEnergy (signal processing)

description

Using the Mainz $48\mathrm{cm}\ensuremath{\emptyset}\ifmmode\times\else\texttimes\fi{}64\mathrm{cm}$ NaI(Tl) detector and the segmented G\"ottingen recoil detector SENECA in coincidence, Compton scattering by the proton at ${\ensuremath{\theta}}_{\ensuremath{\gamma}}^{\mathrm{lab}}=136\ifmmode^\circ\else\textdegree\fi{}$ has been measured at MAMI (Mainz) in the energy range from 200 to 470 MeV. The new data confirm the previous observation that there is a systematic discrepancy between MAMI and LEGS (Brookhaven) data leading to different spin polarizabilities ${\ensuremath{\gamma}}_{\ensuremath{\pi}}=\ensuremath{-}38.7\ifmmode\pm\else\textpm\fi{}1.8$ and $\ensuremath{-}27.2\ifmmode\pm\else\textpm\fi{}3.1$ $(\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}{\mathrm{fm}}^{4}),$ respectively.

https://doi.org/10.1103/physrevc.65.032202