Fragmentation function

In a sufficiently hard interaction between particles, the cross section can be factorized into parton distribution functions (PDFs), the hard scattering part, and fragmentation functions. The fragmentation functions, as are the PDFs, are non-perturbative functions describing the production of a given observed final state. In a leading order picture, it can be interpreted as the probability that the observed final state originates from a given quark or gluon.^[1]

References

^ Metz, A.; Vossen, A. (November 2016). "Parton fragmentation functions". Progress in Particle and Nuclear Physics. 91: 136–202. arXiv:1607.02521. doi:10.1016/j.ppnp.2016.08.003. ISSN 0146-6410.

This particle physics–related article is a stub. You can help Wikipedia by expanding it.

[1] Metz, A.; Vossen, A. (November 2016). "Parton fragmentation functions". Progress in Particle and Nuclear Physics. 91: 136–202. arXiv:1607.02521. doi:10.1016/j.ppnp.2016.08.003. ISSN 0146-6410.

[1]

See also

References