KT Jet Algorithm Working Group

Group Leaders: H.Schellman, V.Daniel Elvira


The aim of the group is to produce physics measurements using Run I (1992-1995) data, and improve our understanding of the KT  algorithm in a hadron collider environment (the Fermilab Tevatron) towards its use in Run II. We are also participating in Run II Workshops.

You can read Minutes which are produced weekly after the meeting.


Why the KT algorithm?

As an alternative to the fixed cone algorithm, the D0 experiment has implemented a successive combination type of algorithm (KT) to reconstruct jets. This algorithm has been widely used at the DESY electron-proton and the CERN electron-positron colliders. It presents several advantages over its fixed cone predecessor. First , the absence of cone boundaries avoids out-of-cone showering losses. Second,  it can be implemented in the same way at all levels (parton level theoretical calculation, final state particle level  Monte Carlo, calorimeter cells), therefore eliminating the split/merge ambiguity. In addition, the algorithm is infrared safe at all orders in a perturbative QCD calculation.

For a description of the D0 KT algorithm (as compared with the fixed cone algorithm) click here.


redball.gifPhysics Analyses


redball.gifRun II Workshops:

         Suppersymmetry/Higgs(home page)

      QCD and Weak Bosons  (home page)
V.Daniel Elvira

Last modified: Mon Aug 30 15:01:42 CDT 1999