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Subsections
Definition of the observable
It is useful to start by recalling the definition of the Durham jet
finding algorithm [13], given in terms of a resolution
parameter
as follows:
- For all pairs of (pseudo-)particles
calculate
 |
(22) |
with
is the visible energy defined as
, here
are the energies before any recombination.
- Go back to step 1.
- If all
stop. The number of
jets is then defined to be equal to the number of (pseudo-)particles
left.
- Otherwise recombine the pair with the smallest
into a single pseudoparticle of momentum
according to the
P-recombination scheme:
 |
(23) |
- Go back to step 1.
The three-jet resolution parameter
is defined as the maximum
value of
that leads to a
-jet event.
This observable was fully resummed at NLL accuracy for the first time
in [3].
The hard scale (Q) is taken to be the center-of-mass energy.
| Test |
result |
| check number of jets |
T |
| all legs positive |
T |
| globalness |
T |
leg  |
 |
 |
 |
 |
 |
| 1 |
2.000 |
 |
1 |
1.000 |
0 |
| 2 |
2.000 |
 |
1 |
1.000 |
0 |
| Test |
result |
| continuously global |
T |
| exponentiation (condition 1) |
T |
| exponentiation (condition 2a) |
T |
| exponentiation (condition 2b) |
T |
| exponentiation |
T |
| additivity |
F |
| eliminate subleading effects |
F |
| opt. probe region exists |
F |
No zeroes or small values found.
Number of events used: 1000000
Result for each colour configuration
For a precise definition of the configurations see [5].
Number of events used: 4050
y3_DurP_ee.tar.gz
collects all files produced automatically by Caesar.
Next: Durham-P0 3-jet resolution y3
Up: Observables in e+e-
Previous: Single-jet squared mass
Giulia Zanderighi
2004-11-19