Measurements of double-polarized compton scattering asymmetries and extraction of the proton spin polarizabilities.

نویسندگان

  • P P Martel
  • R Miskimen
  • P Aguar-Bartolome
  • J Ahrens
  • C S Akondi
  • J R M Annand
  • H J Arends
  • W Barnes
  • R Beck
  • A Bernstein
  • N Borisov
  • A Braghieri
  • W J Briscoe
  • S Cherepnya
  • C Collicott
  • S Costanza
  • A Denig
  • M Dieterle
  • E J Downie
  • L V Fil'kov
  • S Garni
  • D I Glazier
  • W Gradl
  • G Gurevich
  • P Hall Barrientos
  • D Hamilton
  • D Hornidge
  • D Howdle
  • G M Huber
  • T C Jude
  • A Kaeser
  • V L Kashevarov
  • I Keshelashvili
  • R Kondratiev
  • M Korolija
  • B Krusche
  • A Lazarev
  • V Lisin
  • K Livingston
  • I J D MacGregor
  • J Mancell
  • D M Manley
  • W Meyer
  • D G Middleton
  • A Mushkarenkov
  • B M K Nefkens
  • A Neganov
  • A Nikolaev
  • M Oberle
  • H Ortega Spina
  • M Ostrick
  • P Ott
  • P B Otte
  • B Oussena
  • P Pedroni
  • A Polonski
  • V Polyansky
  • S Prakhov
  • A Rajabi
  • G Reicherz
  • T Rostomyan
  • A Sarty
  • S Schrauf
  • S Schumann
  • M H Sikora
  • A Starostin
  • O Steffen
  • I I Strakovsky
  • T Strub
  • I Supek
  • M Thiel
  • L Tiator
  • A Thomas
  • M Unverzagt
  • Y Usov
  • D P Watts
  • L Witthauer
  • D Werthmüller
  • M Wolfes
چکیده

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 extract the nucleon spin polarizabilities is through polarized Compton scattering. Double-polarized Compton scattering asymmetries on the proton were measured in the Δ(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 γ(E1E1)=-3.5±1.2, γ(M1M1)=3.16±0.85, γ(E1M2)=-0.7±1.2, and γ(M1E2)=1.99±0.29, in units of 10(-4)  fm(4).

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عنوان ژورنال:
  • Physical review letters

دوره 114 11  شماره 

صفحات  -

تاریخ انتشار 2015