
2 MERGING PROCEDURE
the leading order (LO) prediction and applies the leading logarithmic- (LL-)accurate high energy
corrections to processes which at tree level contribute at LL or NLL accuracy [6].
The HEJ-resummable processes at LL (for pure dijet production) are scatterings of the form
f1,f2→f1,g, . . . , g,f2where the final state is understood to be ordered in rapidity. We refer to
such configurations as “Fadin-Kuraev-Lipatov” or “FKL” configurations. The subleading configu-
rations which receive LL resummation in HEJ include those where the rapidity ordering between
any two neighbours in the final state is relaxed1. Additional subleading processes include those
with t-channel quark propagators (allowing for central qq emissions). The event output of HEJ
is exclusive to its logarithmic accuracy compared to the inclusive event input generated at leading
order.
In the limit of soft-collinear parton splittings a different class of logarithms emerge which
typically manifest as ratios of transverse energy scales:
log2tj
tk, (2)
where thas mass dimension +2. Such double logarithms may be recast into the product of a soft
logarithm and a collinear logarithm, each of which diverges respectively when partons in an event
have low transverse momenta or have small angular separation. Just as with the high energy log-
arithms log(ˆ
s/k2
⊥), the presence of these spoils the rapid convergence of the perturbative series in
the regions of phase space where such logarithms are large. This includes, most plainly expressed
in Eq. (2) for a transverse momentum-based evolution scale, configurations with hierarchies in p⊥
and collinear splittings inside jet cones.
These effects may be accounted for with Monte Carlo parton showers which resum the leading
logarithmic soft-collinear effects to all orders in perturbation theory. Most often inclusive fixed-
order events are merged with parton shower resummation. Merging events generated at fixed-
order with parton showers is a well-established field of research with many well-proven procedures
including CKKW-L [7,8]merging for leading order input events. Methods for matching to higher
orders in perturbation theory, including MC@NLO [9]and the POWHEG [10]methods for NLO events
are also widely used. Further generalisations of these methods for NLO matching which increase
the accuracy below the merging scale to full NLO have additionally been developed, including
MENLOPS [11,12]and UNLOPS [13,14]. The result of these are exclusive showered events with
an all-order description of the soft and collinear splittings.
We discuss here the implementation of a new procedure for merging the exclusive high-energy-
resummed event output of HEJ with the exclusive parton shower resummation of PYTHIA8[15]
which accounts for both missing higher order perturbative effects and systematically removes the
double counted contributions. The software implementation of this procedure is HEJ+PYTHIA.
2 Merging Procedure
To produce high energy- and soft-collinear-resummed predictions, we express the resummation
of HEJ in the language of the parton shower by defining a splitting kernel corresponding to the
1Sec 1.2.3 of ref [6]provides an overview of contributions from subleading configurations and how these are re-
summed in HEJ.
2