6533b871fe1ef96bd12d1b0a

RESEARCH PRODUCT

Measurements of Double-Polarized Compton Scattering Asymmetries and Extraction of the Proton Spin Polarizabilities

B. OussenaD. P. WattsI. KeshelashviliI. I. StrakovskyA. B. LazarevA. NikolaevI. SupekD. HowdleA. BraghieriS. N. PrakhovG. ReicherzK. LivingstonT. C. JudeM. H. SikoraB. M. K. NefkensTh. StrubM. UnverzagtS. SchraufN. S. BorisovMichaela ThielV. L. KashevarovDavid HamiltonC. S. AkondiD. M. ManleyM. KorolijaL. TiatorW. J. BriscoeP. Hall BarrientosAnthony W. ThomasD. HornidgeM. OstrickD. I. GlazierW. MeyerP. P. MartelP. PedroniI. J. D. MacgregorA. StarostinA. J. SartyA. RajabiS. GarniR. KondratievR. A. MiskimenA. KaeserA. N. MushkarenkovS. SchumannB. KruscheJ. AhrensG. M. GurevichG. M. HuberJ. R. M. AnnandA. G. DenigYu. A. UsovE. J. DownieLilian WitthauerP. Aguar-bartoloméP. B. OtteA. B. NeganovT. RostomyanL. V. Fil'kovW. BarnesC. CollicottD. WerthmüllerS. CherepnyaM. WolfesA. PolonskiW. GradlJ. MancellSusanna CostanzaM. OberleR. BeckM. DieterleAron M. BernsteinH. J. ArendsD. G. MiddletonO. SteffenV. PolyanskyV. LisinH. Ortega SpinaP. Ott

subject

PhysicsPhotonProtonNuclear TheoryCompton scatteringGeneral Physics and AstronomyFOS: Physical sciences7. Clean energy3. Good healthBaryonNuclear physicsProton spin crisisspin polarizabilities; nucleon; photon; ∆(1232) region; MAMINuclear Experiment (nucl-ex)NucleonNuclear ExperimentMicrotronNuclear ExperimentSpin-½

description

The spin polarizabilities of the nucleon describe how the spin of the nucleon responds to an incident polarized photon. The most model-independent way to measure the nucleon spin polarizabilities is through polarized Compton scattering. Double-polarized Compton scattering asymmetries on the proton were measured in the $\Delta(1232)$ region using circularly polarized incident photons and a transversely polarized proton target at the Mainz Microtron. Fits to asymmetry data were performed using a dispersion model calculation and a baryon chiral perturbation theory calculation, and a separation of all four proton spin polarizabilities in the multipole basis was achieved. The analysis based on a dispersion model calculation yields $\gamma_{E1E1} = -3.5 \pm 1.2$, $\gamma_{M1M1}= 3.16 \pm 0.85$, $\gamma_{E1M2} = -0.7 \pm 1.2$, and $\gamma_{M1E2} = 1.99 \pm 0.29$, in units of $10^{-4}$ fm$^4$.

10.1103/physrevlett.114.112501http://arxiv.org/abs/1408.1576