POWHEG Merging

The simplest merging solution, of continuing the PYTHIA shower at the LHA scale hardness where POWHEG leaves off, is obtained if you set SpaceShower:pTmaxMatch = 1 and TimeShower:pTmaxMatch = 1. But then mismatches are bound to happen: some regions may be doublecounted, while others may not be counted at all. Depending on the choice of hardness, such mismatches might be small.

There are no guarantees, however, so a (hopefully) more accurate merging scheme is coded up in the include/Pythia8Plugins/PowHegHooks.h file, with a realistic user example in the examples/main31 files. Here we would like to discuss the (POWHEG-specific) input settings for main31.cc, see main31.cmnd, and attempt to give some recommendations on how to use the main program to perform a matching of POWHEG-BOX with PYTHIA 8.

POWHEG-BOX inputs contain Born-like events (with no resolved emission) and Real-type events (containing an additional parton). The mismatch between POWHEG-hardness and PYTHIA-hardness can be minimised if the PYTHIA shower knows
a) The POWHEG-hardness criterion (through which the separation of Born- and Real-like events is defined), and
b) The POWHEG-hardness value (which separates Born- and Real-like events).
If these definitions are known, then PYTHIA can fill missing phase space regions through vetoed showering: let the shower sweep over the full phase space, using its PYTHIA-hardness ordering, and use the POWHEG-hardness to veto those emissions that POWHEG should already have covered. This is only possible since the POWHEG-hardness criterion and the shower ordering criterion are very similar. In the more general case a truncated showering would be needed Nas04.

For vetoed showering, it is necessary to define the POWHEG-hardness criterion. In the presence of multiple partons, the definition quickly becomes complicated, and allows for different choices. Similar decisions have already been made in the implementation of POWHEG, one example being the choice in defining which "hardness value" is transferred as POWHEG-hardness, e.g. by deciding if the "singular regions" of the FKS or the CS approach are used. If the POWHEG-hardness definition were to be changed, or extended to more objects, the PowhegHooks.h code would need to be modified accordingly.

The merging code is designed to be very flexible, and allows access to many possible choices. However, this flexibility means that many parameters can be changed, potentially leading to confusion. Thus, recommendations might prove helpful. All mistakes and inaccuracies rest with the author.

We recommend the usage of vetoed showers. This means using
         POWHEG:veto = 1
This means that PYTHIA will sweep over the full phase space, and apply a veto on parton shower emissions for which the POWHEG-hardness separation between radiator and emission is above the POWHEG-hardness value of the current input event. The variation POWHEG:veto = 0 can be used to assess how much phase space is under- or double-counted.

To define the POWHEG-hardness criterion, use
         POWHEG:pTdef = 1
Other values can be used by experts to assess variations.

Both POWHEG-BOX and PYTHIA 8 generate emissions through a parton shower step, meaning that both programs have a clear definition of a radiator that emits particles, which is very similar (if not identical). To fix the ambiguity if the radiator or the emitted particle should be called "the emission", use
         POWHEG:emitted = 0
More complicated choices can be used by experts. For instance, use POWHEG:emitted = 2 to check the POWHEG-hardness of both radiator and emitted.

To exhaustively fix the criterion by which to veto parton shower emissions, it is important to decide which partons/parton pairs are used to calculate the POWHEG hardness of a PYTHIA 8 emission. The minimal and recommended choice is
         POWHEG:pTemt = 0
This means that only the POWHEG hardness with respect to the radiating leg is checked, and recoil effects are neglected. This prescription should be very similar to how a hardness value is assigned to a Real-type event in the POWHEG-BOX, since in the (implementation of FKS in the) POWHEG-BOX, initial state splittings only have singular regions with the radiating initial state parton, and final state splittings only have singular regions with respect to the radiating final state line. Other choices of POWHEG:pTemt are available. A warning is that the impact of changes can be huge, particularly for inputs with many jets. Other choices therefore should only be made by experts, and a high degree of caution is advised.

It is furthermore necessary to decide on a value of the hardness criterion. POWHEG-BOX transfers this value in the SCALUP member of Les Houches Events, and we recommend using this value by setting
         POWHEG:pThard = 0
As a variation, in order to estimate the uncertainty due this choice of POWHEG-hardness definition, it can be useful to also check POWHEG:pThard = 2. This will recalculate the POWHEG-hardness value as promoted in Ole12.

You need to decide how many emissions the vetoed shower should check after an allowed emission has been constructed. If the hardness definitions in POWHEG-BOX and PYTHIA 8 where identical, all checking could be stopped after the first allowed PS emission. To be prudent, we recommend setting
         POWHEG:vetoCount = 3
which will then check up to three allowed emissions. Higher values of POWHEG:vetoCount have not lead to visible differences for the processes which have been tested.

Finally, for many POWHEG processes, the Sudakov effects from electroweak emissions (here we are concerned mainly with photon emissions, but this could apply also to W/Z emissions) are not included. This effect can be investigated using POWHEG:QEDveto = 0,1, or 2. For the default value of POWHEG:pTemt = 0, only POWHEG:QEDveto = 2 has any effect. For this choice, a hard photon and subsequent QCD radiation is retained. In many cases, particularly when the Born contributions are small, the choice has little effect.

The modes