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DOI 10.1393/ncc/i2016-16230-1 Colloquia: IFAE 2015

IL NUOVO CIMENTO 39 C (2016) 230

Measurement of Collins asymmetries at BaBar

I. Garziaon behalf of the BaBar Collaboration

INFN, Sezione di Ferrara - Ferrara, Italy received 7 January 2016

Summary. — Inclusive hadron production cross sections and angular distributions in e+e collisions shed light on fundamental questions of hadronization and

frag-mentation processes. We present measurements of the so-called Collins azimuthal asymmetries in inclusive production of hadron pairs in e+e−→ h1h2X annihilation

process, where the two hadrons (either kaons or pions) are produced in opposite hemispheres. In particular, this is the first measurement in e+e−annihilation exper-iment of the KK and Kπ azimuthal asymmetries, which allow to better understand the fragmentation processes and the role of the strage quark, and can be used as a tool to explore the spin content of the nucleon.

Transverse spin effects in fragmentation processes were fist discussed by Collins in

ref. [1], who introduced the so called Collins function H1, a chiral-odd polarized

frag-mentation function used to describe the final state hadron’s distributions around the

momentum of the fragmenting quark. Collins effect can be accessed in e+e annihilation

experiments by studying the process e+e → h

1h2X, where two charged hadrons, either

pions or kaons, are detected in opposite jets. Detailed studies were performed for pion pairs by Belle [2] and BaBar [3] Collaborations, and a clear non zero Collins effect is observed as a function of several kinematic variables.

In this report, we present the first measurement of Collins effect for kaons in e+e

annihilation experiment using BaBar data: the analysis is based on a total integrated

luminosity of 468 fb−1 collected at the center-of-mass energy of about 10.6 GeV. In

particular, we measure the azimuthal modulation for charged KK and Kπ pairs as a

function of hadron fractional energies (z1, z2), which is proportional to the product (or

convolution) of two H1⊥. In addition, we simultaneously extract the asymmetries for ππ

pairs, which are found to be in good agreement with the measurements in ref. [3]. The Collins effect, or Collins asymmetry, can be accessed by measuring the cos φ modulations of the normalized distributions of selected hadron pairs in two different reference frames, called RF12 and RF0. Detector effects can be reduced by constructing the ratio of the azimuthal distributions for hadron pairs with opposite charge U over same charge L (or over C = U + L). Azimuthal modulations are calculated simultaneously for KK, Kπ, and ππ pairs. The measured asymmetries are corrected for the background

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2 I. GARZIA on behalf of the BABAR COLLABORATION BIN ) 2 ,z 1 (z 2 4 6 8 10 12 14 16 UL 12 A 0 0.05 0.1 0.15 0.2 KK π K π π BIN ) 2 ,z 1 (z 0 2 4 6 8 10 12 14 16 UC 12 A 0 0.02 0.04 0.06 0.08 (z1,z2)BIN 2 4 6 8 10 12 14 16 UL 0 A 0 0.02 0.04 0.06 0.08 KK π K π π BIN ) 2 ,z 1 (z 0 2 4 6 8 10 12 14 16 UC 0 A -0.010 0.01 0.02 0.03 0.04 0.2 0.3 0.15 0.5 0.2 0.30.5 0.2 0.3 0.5 0.2 0.3 0.50.9 0.15 0.2 0.3 0.5 0.9 1 z 2 z 0.9/0.15 0.9/0.15 0.9/0.15 0.150.2 0.30.5 0.2 0.30.5 0.2 0.3 0.5 0.2 0.3 0.50.9 0.15 0.2 0.3 0.5 0.9 1 z 2 z 0.9/0.15 0.9/0.15 0.9/0.15 BABAR Prellminary BABAR Prellminary

Fig. 1. – Comparison of AU L (top) and AU C (bottom) Collins asymmetries in RF12 (left) and RF0 (right) for KK, Kπ, and ππ pairs. The statistical and systematic uncertainties are repre-sented by the bars and the bands around the points, respectively. The 16 (z1, z2) bins are shown

on the x-axis: in each interval between the dashed lines, z1 is chosen in the following ranges:

[0.15, 0.2], [0.2, 0.3], [0.3, 0.5], and [0.5, 0.9], while within each interval the points correspond to the four bins in z2.

contributions, mainly coming from charm events, for the K/π contamination, for the small asymmetry values measured in the MC samples, and for the dilution effect due to

the thrust axis approximation as the true q ¯q axis. More detail can be found in ref. [4].

The results are summarized in fig. 1. We measure nonzero asymmetries, which in-crease as a function of the hadron energies in both reference frames. The largest effect is observed for KK pairs. These results are in partial agreement with the prediction reported in ref. [5], which estimates a bigger effect for kaons, about twice as big the Collins effect for pions. These measurements, combined with semi-inclusive deep inelas-tic scattering data, allow to extract the strange-quark contribution to the nucleon’s spin, and to improve the knowledge of the fragmentation processes.

REFERENCES

[1] Collins L. C., Nucl. Phys. B, 396 (1993) 161.

[2] Seidl R. et al. (Belle Collaboration), Phys. Rev. D, 78 (2008) 032011; 86 (2012) 039905(E).

[3] Lees J. P. et al. (BaBar Collaboration), Phys. Rev. D, 90 (2014) 052003. [4] Aubert B. et al. (BaBar Collaboration), arXiv:1506.05864 (2015).

[5] Bacchetta A., Gamberg L. P., Goldstein G. R. and Mukherjee A., Phys. Lett. B, 659 (2008) 234.

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