Abstract
We present an effective field theory method to determine secondary
massive quark effects in jet production taking the thrust distribution
for e+e−
collisions in the dijet limit as a concrete example. The method is
based on the field theoretic treatment of collinear and soft mass modes
which have to be separated coherently from the collinear and ultrasoft
modes related to massless quarks and gluons. For thrust the structure of
the conceptual setup is closely related to the production of massive
gauge bosons and involves four different effective field theories to
describe all possible kinematic situations. The effective field theories
merge into one another continuously and thus allow for a continuous
description from infinitely heavy to arbitrarily small masses keeping
the exact mass dependence of the most singular terms treated through
factorization. The mass mode field theory method we present here is in
the spirit of the variable fermion number scheme originally proposed by
Aivazis, Collins, Olness and Tung and can also be applied in hadron
collisions.
Original language | English |
---|---|
Article number | 034021 |
Number of pages | 27 |
Journal | Physical Review D |
Volume | 88 |
Issue number | 3 |
DOIs | |
Publication status | Published - 15 Aug 2013 |
Austrian Fields of Science 2012
- 103036 Theoretical physics
- 103034 Particle physics
Keywords
- SUDAKOV LIMIT
- LEPTOPRODUCTION
- ANNIHILATION
- RADIATION
- QCD