SIDIS Dihadron Beam Spin Asymmetry
- Spokespersons
- C. Dilks, T. Hayward, A. Vossen
- Year
- 2020
- Abstract
- The observation of beam spin asymmetries in two-pion production in semi-inclusive deep inelastic scattering off an unpolarized proton target is reported for the first time. The data presented here were taken in the fall of 2018 with the CLAS12 spectrometer using a 10.6 GeV longitudinally spin-polarized electron beam delivered by CEBAF at JLab and correspond to an integrated luminosity of 58.3~fb$^{-1}$ delivered on target. The measured asymmetries provide a first signal sensitive to the PDF $e(x)$ in the collinear framework and constitute the first observation of helicity-dependent two-pion fragmentation described by the fragmentation function $G_1^\perp$.
- Comment
Process: ep→eπ+π-X
Data tables have the following columns:- mean Q2
- mean x
- mean Mh, the dihadron invariant mass
- mean z, of the pion pair
- mean PT, more commonly written Ph⊥, is the component of the total dihadron momentum, transverse to q
- ALU amplitude, for a particular modulation
- statistical uncertainty
- systematic uncertainty
- Publication
-
- T.B. Hayward, C. Dilks, A. Vossen, H. Avakian Observation of Beam Spin Asymmetries in the Process ep→eπ+π-X with CLAS12 // (submitted to PRL)
- Quantities
- ALUsin φh ALUsin φR ALUsin (φh−φR) ALUsin (2φh−φR) ALUsin (2φh−2φR) ALUsin (−φh+2φR) ALUsin (3φh−2φR)
Measurements
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ID | Quantity | Beam | Target | Final state |
Q2min, GeV2 |
Q2max, GeV2 |
Wmin, GeV |
Wmax, GeV |
---|---|---|---|---|---|---|---|---|
E179M1 | ALUsin φh | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M2 | ALUsin φh | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M3 | ALUsin φh | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M4 | ALUsin φh | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M5 | ALUsin (φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M6 | ALUsin (φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M7 | ALUsin (φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M8 | ALUsin (φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M9 | ALUsin φR | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M10 | ALUsin φR | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M11 | ALUsin φR | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M12 | ALUsin φR | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M13 | ALUsin (2φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M14 | ALUsin (2φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M15 | ALUsin (2φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M16 | ALUsin (2φh−φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M17 | ALUsin (2φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M18 | ALUsin (2φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M19 | ALUsin (2φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M20 | ALUsin (2φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M21 | ALUsin (−φh+2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M22 | ALUsin (−φh+2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M23 | ALUsin (−φh+2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M24 | ALUsin (−φh+2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M25 | ALUsin (3φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M26 | ALUsin (3φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M27 | ALUsin (3φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
E179M28 | ALUsin (3φh−2φR) | e | p | π π + X | 1.0 | 10.6 | 2.0 | 4.0 |
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