Lund string model
 | This article needs additional citations for verification. (January 2025) |
In particle physics, the Lund string model is a phenomenological model of hadronization. It treats all but the highest-energy gluons as field lines, which are attracted to each other due to the gluon self-interaction and so form a narrow tube (or string) of strong color field. Compared to electric or magnetic field lines, which are spread out because the carrier of the electromagnetic force, the photon, does not interact with itself.
The model is named after the particle theory group of Lund University who developed it. It derived from the 1977 PhD thesis of Carsten Peterson, supervised by Bo Andersson and Gösta Gustafson.[1] The model was refined by the contributions by researchers of the group like Torbjörn Sjöstrand, Bo Söderberg, Gunnar Ingelman, Hans-Uno Bengtsson and Ulf Pettersson.[1] In 1979, the model was able to describe gluon jet fragmentation by considered the force field to be similar to a massless relativistic string.[1] The model successfully predicted a specific asymmetry in the particles produced in electron–positron collisions, observed in 1980.[1]
String fragmentation is one of the parton fragmentation models used in the PYTHIA/Jetset and the University of California, Los Angeles as event generators, and explains many features of hadronization quite well. In particular, the model predicts that in addition to the particle jets formed along the original paths of two separating quarks, there will be a spray of hadrons produced between the jets by the string itself—which is precisely what is observed.
See also
[edit]References
[edit]- ^ a b c d Forkman, Bengt; Verdozzi, Kristina Holmin, eds. (2016). "The Lund model for high energy collisions" (PDF). Physics in Lund: in time and space. Lund University.
 | This particle physics–related article is a stub. You can help Wikipedia by expanding it. |