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Phys. Rev. D 80, 074008 (2009) [17 pages]

NJL-jet model for quark fragmentation functions

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T. Ito1,*, W. Bentz1,†, I. C. Cloët2,‡, A. W. Thomas3,§, and K. Yazaki4,**
1Department of Physics, School of Science, Tokai University, Hiratsuka-shi, Kanagawa 259-1292, Japan
2Department of Physics, University of Washington, Seattle, Washington 98195-1560, USA
3Jefferson Lab, 12000 Jefferson Avenue, Newport News, Virginia 23606, USA and College of William and Mary, Williamsburg, Virginia 23187, USA
4Radiation Laboratory, Nishina Accelerator Research Center, RIKEN, Wako, Saitama 351-0198, Japan

Received 3 July 2009; published 8 October 2009

A description of fragmentation functions which satisfy the momentum and isospin sum rules is presented in an effective quark theory. Concentrating on the pion fragmentation function, we first explain why the elementary (lowest order) fragmentation process qqπ is completely inadequate to describe the empirical data, although the crossed process πqq̅ describes the quark distribution functions in the pion reasonably well. Taking into account cascadelike processes in a generalized jet-model approach, we then show that the momentum and isospin sum rules can be satisfied naturally, without the introduction of ad hoc parameters. We present results for the Nambu–Jona-Lasinio (NJL) model in the invariant mass regularization scheme and compare them with the empirical parametrizations. We argue that the NJL-jet model, developed herein, provides a useful framework with which to calculate the fragmentation functions in an effective chiral quark theory.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.80.074008
DOI:
10.1103/PhysRevD.80.074008
PACS:
13.60.Hb, 12.39.Ki, 13.60.Le

*Corresponding author.

8atad002@mail.tokai-u.jp

bentz@keyaki.cc.u-tokai.ac.jp

icloet@phys.washington.edu

§awthomas@jlab.org

**yazaki@phys.s.u-tokyo.ac.jp