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Leading and next-to-leading order gluon polarization in the nucleon and longitudinal double spin asymmetries from open charm muoproduction

C. Adolph et al. (COMPASS Collaboration)
Phys. Rev. D 87, 052018 – Published 25 March 2013

Abstract

The gluon polarization in the nucleon was measured using open charm production by scattering 160GeV/c polarized muons off longitudinally polarized protons or deuterons. The data were taken by the COMPASS Collaboration between 2002 and 2007. A detailed account is given of the analysis method that includes the application of neural networks. Several decay channels of D0 mesons are investigated. Longitudinal spin asymmetries of the D meson production cross sections are extracted in bins of D0 transverse momentum and energy. At leading order QCD accuracy, the average gluon polarization is determined as Δg/gLO=0.06±0.21(stat.)±0.08(syst.) at the scale μ213(GeV/c)2 and an average gluon momentum fraction x0.11. The average gluon polarization is also obtained at next-to-leading order QCD accuracy as Δg/g NLO=0.13±0.15(stat.)±0.15(syst.) at the scale μ213(GeV/c)2 and x0.20.

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  • Received 28 November 2012

DOI:https://doi.org/10.1103/PhysRevD.87.052018

© 2013 American Physical Society

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Vol. 87, Iss. 5 — 1 March 2013

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Images

  • Figure 1
    Figure 1

    Photon-Gluon Fusion into a pair of charm quarks, cc¯. Symbols in parentheses denote four-vectors.

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  • Figure 2
    Figure 2

    Distribution of reconstructed vertex positions zvtx along the beam axis for the target with two (left) and three (right) cells. Dark horizontal bars at the bottom mark the target fiducial regions, arrows denote the target polarization directions. See text for details.

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  • Figure 3
    Figure 3

    Distribution of zD0 for the DKπ* data sample (background is subtracted using the background model described in Sec. 4a2) and corresponding Monte Carlo events. D0 mesons are selected in the ±80MeV/c2 mass window around the D0 mass.

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  • Figure 4
    Figure 4

    Invariant mass spectra for the DKπ0 and DKπ* samples with the approximate number of D0 mesons above background. Events in the spectra fulfill all the cuts in Table 4. The structure visible at about 250MeV/c2 is due to events with D0Kπ+π0 decays with the neutral pion not reconstructed in the analysis.

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  • Figure 5
    Figure 5

    Invariant mass spectra for the DKππ0*, DKπππ* and DKsubπ* samples. The purity of the samples was improved using the Neural Network. The approximate number of D0 mesons above background is given.

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  • Figure 6
    Figure 6

    A scatter plot of Q2 vs xB and a distribution of y for the 2006 DKπ* sample selected as in Fig. 3 except that the background is not subtracted.

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  • Figure 7
    Figure 7

    Example of the Kπ-invariant mass spectrum for the DKπ* sample with good (gcc) and wrong (wcc) combination of pion and kaon charge signs. See text for details. Data were collected in 2007 with the proton (NH3) target.

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  • Figure 8
    Figure 8

    Example of the distribution of |cosθ*| (polar angle of kaon in the D0 center of mass relative to the D0 momentum) for the gcc and wcc events (DKπ* sample, 2006 data). Top: region of the D0 signal. Bottom: outside the D0 signal.

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  • Figure 9
    Figure 9

    The Kπ-invariant mass spectra in bins of the NN signal purity [s/(s+b)]NN for the DKπ* sample. The last panel shows a comparison of the two purities, [s/(s+b)]NN and [s/(s+b)]fit (see text for details). Curves show the background component of the invariant mass fits described in the text. The significance of the DKπ* signal is shown as ratio s/b. Signal purities are defined in a ±40MeV/c2 mass window around average mass values from the measured D0 signals.

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  • Figure 10
    Figure 10

    A compilation of gluon polarization measurements from open charm and high-pT hadron production. The star denotes a result of the present, open charm analysis, Eq. (14), obtained at LO accuracy, 2002–2007 data and all values of Q2. Full squares denote a Compass result [18] for high-pT hadron production on 2002–2006 data, for Q2>1(GeV/c)2 while a full circle corresponds to 2002–2003 data and Q2<1(GeV/c)2 [15]. The empty square shows the SMC measurement [13] for Q2>1(GeV/c)2 and the empty triangle the Hermes result [14] obtained for all values of Q2. The horizontal bars mark the range in x for each measurement, the vertical ones give the statistical precision or the total uncertainties.

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  • Figure 11
    Figure 11

    Examples of the NLO processes contributing to the muoproduction of the cc¯ pair: (a) virtual correction, (b), (c) gluon bremsstrahlung, (d) light quark background.

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  • Figure 12
    Figure 12

    Distributions of the gluon momentum fractions x for the simulated DKπ* events at the LO accuracy (marked “AROMA”) and at LO with parton shower (AROMA+PS). Note different normalizations of the samples.

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  • Figure 13
    Figure 13

    The present NLO measurement of the gluon polarization Δg(x)/g(x) at μ2=13(GeV/c)2, compared to the NLO QCD fits of Compass with Δg(x)>0 (continuous line) and Δg(x)<0 (long-dashed) with their respective error bands, of LSS [12] (dashed and dotted curves, respectively, with Δg>0 and Δg changing sign) and of DSSV [42] (dashed-dotted curve), all at the same value of Q2=13(GeV/c)2. The measurement error and the error bands are statistical only; the horizontal bar marks the range of x in which Δg(x)/g(x) is determined.

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