Abstract
We report the first measurements of transverse single-spin asymmetries for inclusive jet and jet + $\pi^{\pm}$ production at midrapidity from transversely polarized proton-proton collisions at $\sqrt{s} = 500$ GeV. The data were collected in 2011 with the STAR detector sampled from 23 pb$^{-1}$ integrated luminosity with an average beam polarization of 53%. Asymmetries are reported for jets with transverse momenta $6 < p_{T, jet} < 55$ GeV/c and pseudorapidity $|\eta| < 1$. Presented are measurements of the inclusive-jet azimuthal transverse single-spin asymmetry, sensitive to twist-3 initial-state quark-gluon correlators; the Collins asymmetry, sensitive to quark transversity coupled to the polarized Collins fragmentation function; and the first measurement of the "Collins-like" asymmetry, sensitive to linearly polarized gluons. Within the present statistical precision, inclusive-jet and Collins-like asymmetries are small, with the latter allowing the first experimental constraints on gluon linear polarization in a polarized proton. At higher values of jet transverse momenta, we observe the first non-zero Collins asymmetries in polarized-proton collisions, with a statistical significance of greater than $5\sigma$. The results span a range of x similar to results from SIDIS but at much higher $Q^{2}$. The Collins results enable tests of universality and factorization-breaking in the transverse momentum-dependent formulation of perturbative quantum chromodynamics.
Highlights
The partonic structure of the nucleon at leading twist in a collinear picture can be described by three parton distribution functions (PDFs): the unpolarized parton distribution, fðx; Q2Þ; the parton helicity distribution, Δfðx; Q2Þ; and the transversity distribution, h1ðx; Q2Þ [1]
We report the first measurements of transverse single-spin asymmetries for inclupsivffiffie jet and jet þ πÆ production at midrapidity from transversely polarized proton-proton collisions at s 1⁄4 500 GeV
Final results for the inclusive-jet, Collins, and Collinslike asymmetries are presented in Figs. 9 through 13
Summary
The partonic structure of the nucleon at leading twist in a collinear picture can be described by three parton distribution functions (PDFs): the unpolarized parton distribution, fðx; Q2Þ; the parton helicity distribution, Δfðx; Q2Þ; and the transversity distribution, h1ðx; Q2Þ [1]. Helicity distribution constraints have required observables from the interaction of spin-polarized probes. Recent global analyses have combined data from polarized deep-inelastic scattering (DIS), semi-inclusive DIS (SIDIS), and proton-proton experiments to extract helicity distributions for quarks, antiquarks, and gluons [3–6]. Of the three leading-twist PDFs, transversity, which describes the transverse polarization of quarks inside a transversely polarized nucleon, has proven the most difficult to probe. This is due to its chiral-odd nature that requires transversity to couple to another chiral-odd quantity in order to be observed
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