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The program contains parameterizations, separately, of the total
first-order 3-jet rate, the total second-order 3-jet rate,
and the total 4-jet rate, all as functions of (with
as a separate prefactor).
These parameterizations have been obtained as follows:
-
- The first-order 3-jet matrix element is almost analytically
integrable; some small finite pieces were obtained by a truncated
series expansion of the relevant integrand.
-
- The GKS second-order 3-jet matrix elements were integrated for
40 different -cut values, evenly distributed in between
a smallest value and the kinematical limit .
For each value, 250000 phase-space points were generated,
evenly in
, , and the
second-order 3-jet rate in the point evaluated. The properly
normalized sum of weights in each of the 40 points were
then fitted to a polynomial in . For the ERT(Zhu)
matrix elements the parameterizations in eq. ()
were used to perform a corresponding Monte Carlo integration for
the five values available.
-
- The 4-jet rate was integrated numerically, separately for
and
events, by generating large
samples of 4-jet phase-space points
within the boundary . Each point was classified according
to the actual minimum between any two partons. The same
events could then be used to update the summed weights for 40
different counters, corresponding to values evenly distributed
in between and the kinematical limit .
In fact, since
the weight sums for large values only received contributions
from few phase-space points, extra (smaller) subsamples of events were
generated with larger cuts. The summed weights,
properly normalized, were then parameterized in terms of
polynomials in
.
Since it turned out to be difficult to obtain one single good fit
over the whole range of values, different parameterizations are
used above and below . As originally given, the
parameterization only took into account four
flavours, i.e. secondary
pairs were not generated,
but this has been corrected for LEP.
In the generation stage, each event is treated on its own, which means
that the
and values may be allowed to vary from event to
event. The main steps are the following.
- 48.
- The value to be used in the current event is determined. If
possible, this is the value given by you, but additional
constraints exist from the validity of the parameterizations
( for GKS,
for ERT(Zhu))
and an extra (user-modifiable) requirement of a minimum absolute
invariant mass between jets (which translates into varying cuts
due to the effects of initial-state QED radiation).
- 49.
- The
value is calculated.
- 50.
- For the and
values given, the relative
two/three/four-jet composition is determined. This is achieved by
using the parameterized functions of for 3- and 4-jet rates,
multiplied by the relevant number of factors of
.
In ERT(Zhu), where the second-order 3-jet rate is available
only at a few values, intermediate results are obtained by linear
interpolation in the ratio of second-order to first-order
3-jet rates. The 3-jet and 4-jet rates are normalized to
the analytically known second-order total event rate, i.e. divided
by
of eq. (). Finally, the 2-jet rate is
obtained by conservation of total probability.
- 51.
- If the combination of and
values is such that the total
3- plus 4-jet fraction is larger than unity, i.e. the remainder
2-jet fraction negative, the -cut value is raised (for that event),
and the process is started over at point 3.
- 52.
- The choice is made between generating a 2-, 3- or 4-jet event,
according to the relative probabilities.
- 53.
- For the generation of 4-jets, it is first necessary to make a choice
between
and
events, according to
the relative (parameterized) total cross sections. A phase-space point
is then selected, and the differential cross section at this point is
evaluated and compared with a parameterized maximum weight. If the
phase-space point is rejected, a new one is selected, until an
acceptable 4-jet event is found.
- 54.
- For 3-jets, a phase-space point is first chosen according to the
first-order cross section. For this point, the weight
|
(32) |
is evaluated. Here is analytically given for GKS
[Gut84], while it is approximated by the parameterization
of eq. () for ERT(Zhu). Again, linear
interpolation of has to be applied for intermediate
values. The weight is compared with a maximum weight
|
(33) |
which has been numerically determined beforehand and suitably
parameterized. If the phase-space point is rejected, a
new point is generated, etc.
- 55.
- Massive matrix elements are not available for second-order
QCD (but are in the first-order option). However, if a
3- or 4-jet event determined above falls outside
the phase-space region allowed for massive quarks, the event is
rejected and reassigned to be a 2-jet event. (The way the
and variables of 4-jet events should be
interpreted for massive quarks is not even unique, so some latitude
has been taken here to provide a reasonable continuity from
3-jet events.) This procedure is known not to give the expected full
mass suppression, but is a reasonable first approximation.
- 56.
- Finally, if the event is classified as a 2-jet event, either
because it was initially so assigned, or because it failed the
massive phase-space cuts for 3- and 4-jets, the
generation of 2-jets is trivial.
Next: Optimized perturbation theory
Up: Annihilation Events in the
Previous: Second-order three-jet matrix elements
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Stephen Mrenna
2005-07-11