## Jet Matching

This manual page describes the parton-jet matching interfaces for PYTHIA8. In this approach, usually referred to as MLM matching [Man02, Man07], the final jets after parton-shower evolution and jet clustering are matched to the original partons. The event is accepted if a reasonable match is found, and rejected if not. The rejection step in an approximate way introduces a Sudakov form factor on to the hard processes. Notably the parton shower should not generate an emission that would doublecount hard activity already included in the matrix-element description. Within this general ansatz, different technical solutions can be adopted. We provide two alternatives, one based on the algorithm used in ALPGEN [Man03], and another on the one used in Madgraph [Alw11], both reimplemented from scratch here. The main points of these two algorithms are outlined further down on this page.

We also allow for two alternative sources of external events, one in the ALPGEN native format and one in the Madgraph LHEF-based one. All four combinations of input format and matching style are implemented. In the following it is therefore important to keep the two aspects apart, whenever the ALPGEN and Madgraph labels are used.

Currently all the files of interest are located in the `examples/` subdirectory:

- `JetMatching.h` contains the machinery for the parton-jet matching, in the two `JetMatchingAlpgen` and `JetMatchingMadgraph` classes.
- `GeneratorInput.h` contains three classes for the reading of ALPGEN event and parameter files, and one for the reading of Madgraph parameters.
- `CombineMatchingInput.h` contains three classes that combine the reading of events with the matching of them.
- `main32.cc, main32.cmnd` : a sample main program and card file showing the usage of the previous files/classes.

## Event input source

External sources of partons are used in the parton-jet matching process. The source of the partons has been separated from the implementation of the matching algorithm. By default, PYTHIA8 contains a machinery to process Les Houches Event Files (LHEFs) as described on the Les Houches Accord and Beam Parameters pages. Madgraph5 adheres to this format, but also contains some further non-standardized information that can be used. The parsing of the native ALPGEN file format is described on the Alpgen Event Interface page.

Commonly, the source of external partons also contains information about how a particular type of matching algorithm should be employed. This information is handled by the `AlpgenPar` class for ALPGEN files, and `MadgraphPar` for LHEFs. The user can choose to set default matching parameters using the `Alpgen:setMLM` flag for ALPGEN files. For LHEFs, instead, the setting of default parameters is controlled with the `JetMatching:setMad` flag:

`flag` JetMatching:setMad (`default = on`)
When enabled, the merging parameters are set according to the values in the LHEF header. Specifically, the header must set the `ickkw`, `xqcut`, `maxjetflavor` and `alpsfact` values, and `ickkw` must be nonzero. Note that these labels are Madgraph-specific. For other programs with LHEF output, or for Madgraph files lacking this information, these parameters should be set by the user (or one can rely on the default values). The following parameters (described below) must then be specified:

- `JetMatching:doMerge = ickkw`,
- `JetMatching:qCut = xqcut`,
- `JetMatching:nQmatch = maxjetflavor`,
- `JetMatching:clFact = alpsfact.`

With this flag on, the values from the LHEF for these parameters take precedence over other values.

## Jet Matching parameters

A class `JetMatching`, derived from `UserHooks`, is used to define the basic structure of a parton-jet matching algorithm. Two versions are implemented here, based on the FORTRAN code provided by the ALPGEN and Madgraph packages, respectively: `JetMatchingAlpgen` and `JetMatchingMadgraph`. The matching parameters are defined with the `JetMatching:*` keyword.

### Scheme and Usage

`flag` JetMatching:merge (`default = off`)
Master switch to activate parton-jet matching. When off, all external events are accepted (unless they are rejected due to weighting or event processing problems).

`mode` JetMatching:scheme (`default = 1`; `minimum = 1`; `maximum = 2`)
The parton-jet MLM-style matching scheme.
`option` 1 : The one inspired by the Madgraph matching code, here implemented in the `JetMatchingMadgraph` class.
`option` 2 : The one inspired by the ALPGEN matching code, here implemented in the `JetMatchingAlpgen` class.

### Jet algorithm

The choice of jet algorithm and associated parameters can be adjusted with the settings below. The PYTHIA8 internal `CellJet` and `SlowJet` routines are used for jet finding. See the Event Analysis page for more details.

`mode` JetMatching:jetAlgorithm (`default = 1`; `minimum = 1`; `maximum = 2`)
The choice of jet algorithm to use when merging against hard partons. Currently, only `SlowJet` with the kT algorithm (and `useStandardR = false`) is supported for Madgraph-style matching, while there is full freedom for the ALPGEN-style matching.
`option` 1 : The `CellJet` cone algorithm.
`option` 2 : The `SlowJet` clustering algorithm.

`mode` JetMatching:slowJetPower (`default = -1`; `minimum = -1`; `maximum = 1`)
The power to use in the `SlowJet` algorithm.
`option` -1 : The anti-kT algorithm.
`option` 0 : The Cambridge/Aachen algorithm.
`option` 1 : The kT algorithm.

`mode` JetMatching:nEta (`default = 100`; `minimum = 50`)
Specific to the `CellJet` algorithm, the number of bins in pseudorapidity.

`mode` JetMatching:nPhi (`default = 60`; `minimum = 30`)
Specific to the `CellJet` algorithm, the number of bins in phi.

`parm` JetMatching:eTseed (`default = 1.5`; `minimum = 0.0`)
Specific to the `CellJet` algorithm, the minimum eT for a cell to be acceptable as the trial center of a jet.

`parm` JetMatching:eTthreshold (`default = 0.1`)
Specific to the `CellJet` algorithm, cells with eT < eTthreshold are completely neglected by the jet algorithm.

### Merging parameters

The following options are the three main parameters for the merging procedure. Although here they are in principle free parameters, they should be heavily influenced by the hard process generation cuts. These values can be set automatically based on the information in the ALPGEN file or LHEF.

`parm` JetMatching:eTjetMin (`default = 20.0`; `minimum = 5.0`)
For the `CellJet` algorithm, this gives the minimum transverse energy inside a cone for a jet to be accepted. For the `SlowJet` algorithm, this is instead the minimum transverse momentum required for a cluster to be accepted as a jet. For Madgraph-style matching, this parameter should match the `qCut` parameter described later.

`parm` JetMatching:coneRadius (`default = 0.7`; `minimum = 0.1`)
For the `CellJet` algorithm, this gives the size of the cone in (eta, phi) space drawn around the geometric center of the jet. For the `SlowJet` algorithm, this gives the R parameter.

`parm` JetMatching:etaJetMax (`default = 2.5`; `minimum = 0.1`)
For both jet algorithms, this defines the maximum pseudorapidity that the detector is assumed to cover. In this context, however, it is tied to the phase space region in which partons have been generated. For the Alpgen-style matching, particles within etaJetMax + coneRadius are passed to the jet algorithm, with only jets within etaJetMax retained in the merging. For the Madgraph-style matching, only particles within etaJetMax are used.

### Exclusive mode

The following settings determine whether clustered jets which do not match an original hard parton are allowed. They are typically permitted in the highest jet multiplicity sample, where the parton shower may produce extra hard jets, without risk of double counting. Any extra jet produced by the shower must be softer than any matched light jet, or else the event is vetoed.

`mode` JetMatching:exclusive (`default = 2`; `minimum = 0`; `maximum = 2`)
Exclusive or inclusive merging.
`option` 0 : The merging is run in inclusive mode. All partons must match jets, but additional jets are allowed, provided they are not harder than the matched jets.
`option` 1 : The merging is run in exclusive mode. All partons must match jets, and no additional jets are allowed.
`option` 2 : If nJet < nJetMax, then the merging is run in exclusive mode, otherwise it is run in inclusive mode. For Madgraph-style matching, this is checked on an event-by-event basis, which is useful when an LHEF contains a "soup" of partonic multiplicities. If nJetMax < 0 or nJet < 0, then the algorithm defaults to exclusive mode.

`mode` JetMatching:nJet (`default = -1`; `minimum = -1`)
When `JetMatching:exclusive = 2`, nJet indicates the minimum number of additional light jets in the incoming process. This value may be set automatically.

`mode` JetMatching:nJetMax (`default = -1`; `minimum = -1`)
When `JetMatching:exclusive = 2`, nJetMax is used to indicate the maximum number of jets that will be matched.

### Jet matching

The following parameters control the criteria for matching a clustered jet to a hard parton.

`mode` JetMatching:jetAllow (`default = 1`; `minimum = 1`; `maximum = 2`)
Controls which particles are clustered by the jet algorithm.
`option` 1 : This option explicitly disallows top quarks, leptons and photons. All other particle types are passed to the jet algorithm.
`option` 2 : No extra particles are disallowed.

### Alpgen-specific parameters

`mode` JetMatching:jetMatch (`default = 1`; `minimum = 1`; `maximum = 2`)
Criteria for matching a clustered jet to a parton.
`option` 1 : This option can be used with both the `CellJet` and `SlowJet` algorithms. The delta R between each parton and jet is taken, and the minimal value compared against coneMatchLight * coneRadius for light jets or coneMatchHeavy * coneRadiusHeavy for heavy jets. Note that by default coneRadiusHeavy = coneRadius, see below. If below this value, the parton and jet are considered to match. With `CellJet`, the delta R measure is in (eta, phi), while with `SlowJet` it is in (y, phi).
`option` 2 : This option can only be used with the `SlowJet` algorithm. The hard partons are inserted into the parton level event as "ghost" particles, but at the correct (y, phi) position. If this particle is then clustered into a jet, it is considered a match.

`parm` JetMatching:coneMatchLight (`default = 1.5`; `minimum = 0.1`)
The coneMatchLight parameter used when `JetMatching:jetMatch = 1`.

`parm` JetMatching:coneRadiusHeavy (`default = -1.0`)
The coneRadiusHeavy parameter used when `JetMatching:jetMatch = 1`. When assigned a negative value, the value of `JetMatching:coneRadius` is used.

`parm` JetMatching:coneMatchHeavy (`default = 1.0`; `minimum = 0.1`)
The coneMatchHeavy parameter used when `JetMatching:jetMatch = 1`.

### Madgraph-specific parameters

`flag` JetMatching:doShowerKt (`default = off`)
This switch changes the merging prescription to the shower-kT matching scheme outlined in [Alw08]. This scheme differs from "classical" MLM jet matching with respect to when the matching veto is checked. The shower-kT scheme considers already immediately after the first shower emission if an event should be discarded. A detailed comparison of the "classical" MLM prescription (e.g. Madgraph-style matching with `JetMatching:doShowerKt = off`) and the shower-kT scheme are in preparation.

`parm` JetMatching:qCut (`default = 10.0`; `minimum = 0.0`)
kT scale for merging shower products into jets.

`mode` JetMatching:nQmatch (`default = 5`; `minimum = 3`; `maximum = 6`)
Controls the treatment of heavy quarks.
`option` 5 : All quarks (except top) are treated as light quarks for matching.
`option` 4 : Bottom quarks are treated separately. Currently, they are unmatched.

`parm` JetMatching:clFact (`default = 1.0`)
The clFact parameter determines how jet-to parton matching is done. A match is defined as a squared cluster scale that equals:
|clFact| * qCut for inclusive mode,
|clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
|clFact| * min(kT(parton)) for exclusive mode, clFact < 0.

A preliminary implementation of the FxFx prescription for combining multiple NLO calculations [Fre12] is available. We would like to stress that this implementation is still undergoing validation. FxFx merging with aMC@NLO shares most parameters with the leading-order (MadGraph-style) MLM prescriptions and can be activated by using the three additional settings below.

`flag` JetMatching:doFxFx (`default = off`)
If turned on, then FxFx merging with aMC@NLO inputs is performed. Note that this requires event samples that are specifically generated for this task.

`mode` JetMatching:nPartonsNow (`default = -1`)
The number of partons in Born-like events for the current input LHEF. If the current sample e.g. contains pp → e+e- + 2 partons Born-like configurations, and pp → e+e- + 3 partons Real-emission-type events, then `JetMatching:nPartonsNow = 2` applies.

`parm` JetMatching:qCutME (`default = 10.0`)
The cut applied to regulate multi-jet matrix elements. Note that this cut can differ from the matching scale.

## Alpgen-style parton-jet matching and merging

This section describes the Alpgen-style MLM merging algorithm for PYTHIA8. The most common reference to the algorithm is [Man02]. In many respects, however, the implementation provided in the ALPGEN package should be considered the official description of the MLM merging procedure. Although designed primarily to work with events generated with ALPGEN, it can in principle also be used with events from a different source. This should not be done without thought, however, and it is up to the user to understand the details of the algorithm and the implications of using a different hard process generator.

First, either the `CellJet` or `SlowJet` jet algorithm is chosen. Both of these algorithms have an R and an etaMax parameter. In addition, `CellJet` has an eTmin and `SlowJet` has a pTmin parameter. These are the primary three parameters of the merging procedure, and in practice are set dependent on the cuts applied to the matrix element (ME) generation. We stress that the merging procedure is not tied to the geometry of a specific physical detector, but only to the match between the original partons and the resulting jets, using standard jet algorithms in the phase space region where partons have been generated.

ME samples with different jet multiplicities are run through the event generator, and the generation interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. Note in particular that top quarks will not yet be decayed, which may lead to slight differences with the PYTHIA 6 interface included with the ALPGEN package. In what follows, the hardness measure of jets/partons is taken to be eT when `CellJet` is used and pT when `SlowJet` is used. The hard system (ignoring all MPI systems) is then analysed:

- The particles in the original matrix element process are sorted into light partons, heavy partons and other particles. For backwards compatibility, a light parton is defined as the set (d, u, s, c, b, g) with zero mass. A heavy parton is defined as the set (c, b, t) with non-zero mass.
- All particles not originating from the heavy partons or other particles are passed to the jet algorithm and clustered.
- Clustered jets are matched to the light partons in the original ME process. There are two different methods which can be used:
  - Method 1: The following is done for each parton, in order of decreasing hardness. The delta R between the parton and all jets is calculated and the smallest value taken. If this is less than the jet R parameter, possibly multiplied by a constant, the jet and parton are considered to match, and the jet is removed from further consideration. Note that for `CellJet` the delta R measure is in (eta, phi), while for `SlowJet`, it is in (y, phi).
  - Method 2: This method is only possible when using the `SlowJet` algorithm. Before the clustering is performed, extremely soft "ghost" particles are added to the event at the (y, phi) coordinates of the original matrix element partons. If such a particle is clustered into a jet, the parton and jet are considered to match. The idea of "ghost" particles was originally introduced by FastJet as a way to measure jet areas [Cac06] and should not affect clustering with an infrared-safe jet algorithm.
- If there is a light ME parton remaining which has not been matched to a jet, then the event is vetoed. If all ME partons have been matched to a jet, but there are still some extra jets remaining, then two options are possible:
  - Exclusive mode: the event is vetoed. This is typically used when there are ME samples with higher jet multiplicities, which would fill in the extra jets.
  - Inclusive mode: the event is retained if the extra jets are softer than the softest matched jet. This is typically used when there is no ME sample with higher jet multiplicity, so the parton shower should be allowed to give extra jets.
- All particles originating from the heavy partons are passed to the jet algorithm and clustered.
- The clustered jets are again matched to the original partons, but there is no requirement for a match to be present; all matched jets are immediately discarded. The matching procedure is much the same as for light partons, but with two differences when delta R matching is used. First, a different R parameter than that used by the jet algorithm may optionally be given. Second, all jets that are within the given radius of the parton are matched, not just the one with the smallest delta R measure. If there are still extra jets remaining then in exclusive mode the event is immediately vetoed, while in inclusive mode the event is retained if the extra jets are softer than the softest light matched jet.

Some different options are provided, specified further above in the parameters section. These are set so that, by default, the algorithm closely follows the official MLM interface provided in the ALPGEN package.

All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from `Pythia::stat()`, the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when ALPGEN input is used and the hard process parameters are used to guide the merging procedure, it is enough to set the `JetMatching:nJetMax` parameter.

## Madgraph-style parton-jet Merging and Matching

This section describes the Madgraph-style parton-jet matching algorithm for PYTHIA8.

First, the kT jet algorithm is applied using the PYTHIA8 `SlowJet` implementation. The `useStandardR = false` is used, ie. the (delta R)^2 separation is defined as 2 (cosh(delta y) - cos(delta phi)) rather than the more common (delta y)^2 + delta phi)^2. The R, etaMax, and a pTmin parameters are specified. By default, R = 1 and pTmin = qCut . It is not recommended to change these. These should match the algorithm parameters used in the Madgraph Matrix Element (ME) generation.

ME samples with different jet multiplicities are run through the event generator, and the generation is interrupted after parton showers have been applied, but before resonance decays and beam remnants have been processed. In what follows, the hardness measure of jets/partons is taken to be kT relative to qCut. The hard system (ignoring all MPI systems) is analyzed:

- The hard partons in the original matrix element process, provided by the LHEF, are sorted into light partons, heavy partons and other particles. A heavy parton is defined by the `JetMatching:nQmatch` or by the `maxjetflavor` value in the LHEF. nQmatch refers to the absolute value of the quark PDG identity code.
- All partons arising from the parton shower are sorted based on their motherhood. A showered parton arising from a heavy parton or "other" parton classified in the previous step is not passed to the jet algorithm. All other partons are clustered into light jets.
- It is checked whether there are "too few" or "too many" light jets. If the number of light jets is less than the number of light partons defined by nQmatch, the event is vetoed. If the number is larger, the event is vetoed only in exclusive mode (defined below).
- In exclusive mode, the number of jets matches the number of light partons. In inclusive mode, the jets are re-clustered until the number of jets equals the number of light partons. Next, each light hard parton is clustered, one at a time, with the jets until a match is found. A match is defined as a squared cluster scale that equals:
  - |clFact| * qCut for inclusive mode,
  - |clFact| * max(qCut,min(pT(parton))) for exclusive mode, clFact ≥ 0, or
  - |clFact| * min(kT(parton)) for exclusive mode, clFact < 0.
  If no match is found, the event is vetoed. When a parton matches a jet, the jet is removed from the collection, and the process continues. The process terminates when all partons are matched to a jet, or a parton is unmatched.
- All particles originating from the heavy partons are not used.

In exclusive mode, it is expected that ME samples with higher parton multiplicity are available to fill the phase space above qCut. The inclusive mode is when there are no such samples, and the parton shower is used to fill the phase space.

Some different options are provided, specified further above. These are set so that, by default, the algorithm closely follows the FORTRAN interface `ME2Pythia` provided in the Madgraph package.

All vetoing of events is done through the usual User Hooks machinery, and is therefore already taken into account in the cross section. In the output from `Pythia::stat()`, the difference between the "Selected" and "Accepted" columns gives the number of events that have not survived the vetoing procedure. It is still the responsibility of the user to add together the results from runs with different jet multiplicities. In the simplest case, when the hard process parameters are used to guide the merging procedure, events will be matched in the exclusive mode.

### A note on combining UserHooks

As have been noted above, the matching is implemented using classes derived from the `UserHooks` class, thereby gaining access to the event generation process at the relevant locations. For native ALPGEN files, which do not adhere to the Les Houches standards, it is also necessary to intervene with a `UserHooks`-derived `AlpgenHooks` to handle the extraction and setting of relevant extra information.

One must then combine multiple `UserHooks` classes, such that the functionality of both is present. A prerequisite is that the different `UserHooks` classes should be declared with virtual inheritance, e.g.

      class JetMatching : virtual public UserHooks

Without this option, when combining two `UserHooks`-derived classes, two copies of the base `UserHooks` class would be created, leading to ambiguities.

The two first classes in `CombineMatchingInput.h` combine ALPGEN input with the two different matching schemes, e.g. for the first

    class JetMatchingAlpgenInputAlpgen : public AlpgenHooks,
      public JetMatchingAlpgen {
    public:
      // Constructor and destructor.
      JetMatchingAlpgenInputAlpgen(Pythia& pythia) : AlpgenHooks(pythia),
        JetMatchingAlpgen() { }
      ~JetMatchingAlpgenInputAlpgen() {}
      // Initialisation.
      virtual bool initAfterBeams() {
        if (!AlpgenHooks::initAfterBeams()) return false;
        if (!JetMatchingAlpgen::initAfterBeams()) return false;
        return true;
      }
      // Process level vetos.
      virtual bool canVetoProcessLevel() {
        return JetMatchingAlpgen::canVetoProcessLevel();
      }
      ....
    };

This class inherits from both `AlpgenHooks` and `JetMatchingAlpgen`. Any functions which are present in both classes should be overridden with a function that calls the different parent methods in the desired order. In the above example, the only shared methods are the constructor and `initAfterBeams()`.