The Particle Data Scheme

The particle data scheme may take somewhat longer to understand than the settings one. In particular the set of methods to access information is rather more varied, to allow better functionality for advanced usage. However, PYTHIA does come with a sensible default set of particle properties and decay tables. Thus there is no need to learn any of the methods on this page to get going. Only when you perceive a specific need does it make sense to learn the basics.

The central section on this page is the Operation one. The preceding sections are mainly there to introduce the basic structure and the set of properties that can be accessed.

Databases

The management of particle data is based on the four classes: The objects of these classes together form a database that is continuously being used as the program has to assign particle masses, decay modes etc.

The ParticleDataTable class is purely static, i.e. you can interact with it directly by ParticleDataTable::command(argument). However, a particleData object of the ParticleDataTable class is a public member of the Pythia class, so an alternative notation would be pythia.particleData.command(argument), assuming that pythia is an instance of the Pythia class. Further, for some of the most frequent user tasks, Pythia methods have been defined, so that pythia.command(argument) would work, see further below.

A fundamental difference between the ParticleData classes and the Settings ones is that the former are accessed regularly during the event generation process, as a new particle is produced and its mass need to be set, e.g., while Settings is mainly/only used at the initialization stage. Nevertheless, it is not a good idea to change data in either of them in mid-run, since this may lead to inconsistencies.

Stored properties for particles

Currently the following particle properties are stored in the ParticleDataTable for a given PDG particle identity code id, here presented by the name used to access this property:

method  name(id)  
particle and antiparticle names are stored separately, the sign of id determines which of the two is returned, with void used to indicate the absence of an antiparticle.

method  spinType(id)  
the spin type, of the form 2 s + 1, with special code 0 for entries of unknown or indeterminate spin.

method  chargeType(id)  
three times the charge (to make it an integer), taking into account the sign of id.

method  colType(id)  
the colour type, with 0 uncoloured, 1 triplet, -1 antitriplet and 2 octet, taking into account the sign of id.

method  m0(id)  
the nominal mass m_0 (in GeV).

method  mWidth(id)  
the width Gamma of the Breit-Wigner distribution (in GeV).

method  mMin(id), mMax(id)  
the lower and upper limit, respectively, of the allowed mass range generated by the Breit-Wigner (in GeV). If mMax < mMin then no upper limit is imposed. Have no meanings for particles without width, and would typically be 0 there.

method  tau0(id)  
the nominal proper lifetime tau_0 (in mm/c).

method  isResonance(id)  
a flag telling whether a particle species are considered as a resonance or not. Here "resonance" is used as shorthand for any massive particle where the decay process should be counted as part of the hard process itself, and thus be performed before showers and other event aspects are added. Restrictions on allowed decay channels is also directly reflected in the cross section of simulated processes, while those of normal hadrons and other light particles are not. In practice, it is reserved for states above the b bbar bound systems in mass, i.e. for W, Z, t, Higgs states, supersymmetric states and (most?) other states in any new theory. All particles with m0 above 20 GeV are by default initialized to be considered as resonances.

method  mayDecay(id)  
a flag telling whether a particle species may decay or not, offering the main user switch. Whether a given particle of this kind then actually will decay also depends on it having allowed decay channels, and on other flags for particle decays. All particles with tau0 below 1000 mm are by default initialized to allow decays.

method  doExternalDecay(id)  
a flag telling whether a particle should be handled by an external decay package or not, with the latter default. Can be manipulated as described on this page, but should normally not be. Instead the pythia.decayPtr method should be provided with the list of relevant particles.

method  isVisible(id)  
a flag telling whether a particle species is to be considered as visible in a detector or not, as used e.g. in analysis routines. By default this includes neutrinos and a few BSM particles (gravitino, sneutrinos, neutralinos) that have neither strong nor electromagnetic charge, and are not made up of constituents that have it. The value of this flag is only relevant if a particle is long-lived enough actually to make it to a detector.

method  doForceWidth(id)  
a flag valid only for resonances where PYTHIA contains code to calculate the width of the resonance from encoded matrix-element expressions, i.e. the Z^0, W^+-, t, h^0, and a few more. The normal behaviour (false) is then that the width is calculated from the mass, but it is possible to force the resonance to retain the nominal width. Branching ratios and the running of the total width are unaffected.

Similarly-named methods can also be used to set these properties. We do not provide the details here, since other methods to be introduced below are the ones likely to be used for such tasks. (Normally the correspondence is obvious in the header file, but for the name you either can use two methods to set name and antiparticle name separately, or use one method that takes them both as input.)

There are some further methods for output only, i.e. properties that cannot be set directly:

method  particleDataPtr(id)  
returns a pointer to the ParticleDataEntry object.

method  hasAnti(id)  
bool whether a distinct antiparticle exists or not. Is true if an antiparticle name has been set (and is different from void).

method  charge(id)  
the electrical charge of a particle, as a double equal to chargeType(id)/3.

method  mass(id)  
returns a mass distributed according to a truncated Breit-Wigner, with parameters as above (see also the ParticleData:modeBreitWigner switch). Is equal to m0(id) for particles without width.

method  constituentMass(id)  
is the constituent mass for a quark, hardcoded as m_u = m_d = 0.325, m_s = 0.50, m_c = 1.60 and m_b = 5.0 GeV, for a diquark the sum of quark constituent masses, and for everything else the same as the ordinary mass.

method  m0Min(id), m0Max(id)  
similar to mMin() and mMax(), except that for particles with no width the m0(id) value is returned.

method  isLepton(id)  
true for a lepton or an antilepton (including neutrinos).

method  isQuark(id)  
true for a quark or an antiquark.

method  isGluon(id)  
true for a gluon.

method  isHadron(id)  
true for a hadron (made up out of normal quarks and gluons, i.e. not for R-hadrons and other exotic states).

method  heaviestQuark(id)  
extracts the heaviest quark or antiquark, i.e. one with largest id number, for a hadron.

Stored properties for decays

The following properties are stored for each decay channel:

method  onMode()  
0 if a channel is off,
1 if on,
2 if on for a particle but off for an antiparticle,
3 if on for an antiparticle but off for a particle.
If a particle is its own antiparticle then 2 is on and 3 off but, of course, for such particles it is much simpler and safer to use only 1 and 0.
The 2 and 3 options can be used e.g. to encode CP violation in B decays, or to let the W's in a q qbar -> W^+ W^- process decay in different channels.

method  bRatio()  
the branching ratio.

method  meMode()  
the mode of processing this channel, possibly with matrix elements (see the particle decays description);

method  multiplicity()  
the number of decay products in a channel, at most 8. (Is not set as such, but obtained from the products list below.)

method  product(i)  
a list of the decay products, 8 products 0 <= i < 8, with trailing unused ones set to 0.

The decay table, a vector of decay channels, also defines a few methods:

method  addChannel( branchingRatio, meMode, product1, ...)  
adds a decay channel with up to 8 products.

method  size()  
gives the number of decay channels for a particle.

method  rescaleBR(newSumBR)  
rescale all branching ratios to the provided new sum, by default unity.

method  pick()  
picks one decay channel according to their respective branching ratios.

method  dynamicPick()  
intended for resonances specifically, this picks one decay channel according to the respective partial widths for the specific mass value of the resonance; assumes that the partial widths are input beforehand, using a special dynamicBR() method.

Operation

The normal flow of the particle data operations is:
  1. When a Pythia object pythia is created, the ParticleDataTable member pythia.particleData is asked to scan the ParticleData.xml file.

    All lines beginning with <particle are scanned for information on a particle species, and all lines beginning with <channel are assumed to contain a decay channel of the enclosing particle. In both cases XML syntax is used, with attributes used to identify the stored properties, and with omitted properties defaulting back to 0 where meaningful. The particle and channel information may be split over several lines, up to the > endtoken. The format of a <particle tag is:

        <particle id="..." name="..." antiName="..." spinType="..." chargeType="..." colType="..." 
           m0="..." mWidth="..." mMin="..." mMax="..." tau0="...">
        </particle>
    
    where the fields are the properties already introduced above. Note that isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth are not set here, but are provided with default values by the rules described above. Once initialized, also these latter properties can be changed, see below.
    The format of a <channel> tag is:
        <channel onMode="..." bRatio="..." meMode="..." products="..." />
    
    again see properties above. The products are given as a blank-separated list of id codes.
    Important: the values in the .xml file should not be changed, except by the PYTHIA authors. Any changes should be done with the help of the methods described below.
  2. Between the creation of the Pythia object and the init call for it, you may use the methods of the ParticleDataTable class to modify some of the default values. Several different approaches can be chosen for this.

    a) Inside your main program you can directly set values with

        pythia.readString(string);
    
    where both the variable name and the value are contained inside the character string, separated by blanks and/or a =, e.g.
        pythia.readString("111:mayDecay = off"); 
    
    switches off the decays of the pi^0.
    The particle id (> 0) and the property to be changed must be given, separated by a colon.
    The allowed properties are: name, antiName, spinType, chargeType, colType, m0, mWidth, mMin, mMax, tau0, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidth. All of these names are case-insensitive. Names that do not match an existing variable are ignored. A warning is printed, however, unless an optional second argument false is used.
    Strings beginning with a non-alphanumeric character, like # or !, are assumed to be comments and are not processed at all. For bool values, the following notation may be used interchangeably: true = on = yes = ok = 1, while everything else gives false (including but not limited to false, off, no and 0).

    Particle data often comes in sets of closely related information. Therefore some properties expect the value to consist of several numbers. These can then be separated by blanks (or by commas). A simple example is names, which expects both the name and antiname to be given. A more interesting one is the all property,

      
        id:all = name antiName spinType chargeType colType m0 mWidth mMin mMax tau0
    
    where all the current information on the particle itself is replaced, but any decay channels are kept unchanged. Using new instead of all also removes any previous decay channels. If the string contains fewer fields than expected the trailing properties are set to vanish ("void", 0 or 0.). Note that such a truncated string should not be followed by a comment, since this comment would then be read in as if it contained the missing properties. The truncation can be done anywhere, specifically a string with only id:new defines a new "empty" particle. As before, isResonance, mayDecay, doExternalDecay, isVisible and doForceWidthare (re)set to their default values, and would have to be changed separately if required.

    A further command is rescaleBR, which rescales each of the existing branching ratios with a common factor, such that their new sum is the provided value. This may be a first step towards adding new decay channels, see further below.

    Alternatively the id code may be followed by another integer, which then gives the decay channel number. This then has to be followed by the property specific to this channel, either onMode, bRatio, meMode or products. In the latter case all the products of the channel should be given:

        id:channel:products =  product1 product2 ....  
    
    The line will be scanned until the end of the line, or until a non-number word is encountered, or until the maximum allowed number of eight products is encountered, whichever happens first. It is also possible to replace all the properties of a channel in a similar way:
        id:channel:all = onMode bRatio meMode product1 product2 ....  
    
    To add a new channel at the end, use
        id:addChannel = onMode bRatio meMode product1 product2 ....
    

    It is currently not possible to remove a channel selectively, but setting its branching ratio vanishing is as effective. If you want to remove all existing channels and force decays into one new channel you can use

        id:oneChannel = onMode bRatio meMode product1 product2 ....
    
    A first oneChannel command could be followed by several subsequent addChannel ones, to build up a completely new decay table for an existing particle.

    When adding new channels or changing branching ratios in general, note that, once a particle is to be decayed, the sum of branching ratios is always rescaled to unity. Beforehand, rescaleBR may be used to rescale an existing branching ratio by the given factor.

    There are a few commands that will study all the decay channels of the given particle, to switch them on or off as desired. The

        id:onMode = onMode
    
    will set the onMode property of all channels to the desired value. The
     
        id:offIfAny   = product1 product2 .... 
        id:onIfAny    = product1 product2 .... 
        id:onPosIfAny = product1 product2 .... 
        id:onNegIfAny = product1 product2 .... 
    
    will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain any of the enumerated products, where the matching to these products is done without distinction of particles and antiparticles. Note that "Pos" and "Neg" are slightly misleading since it refers to the particle and antiparticle of the id species rather than charge, but should still be simpler to remember and understand than alternative notations. Correspondingly
     
        id:offIfAll   = product1 product2 .... 
        id:onIfAll    = product1 product2 .... 
        id:onPosIfAll = product1 product2 .... 
        id:onNegIfAll = product1 product2 .... 
    
    will set the onMode 0, 1, 2 or 3, respectively, for all channels which contain all of the enumerated products, again without distinction of particles and antiparticles. If the same product appears twice in the list it must also appear twice in the decay channel, and so on. The decay channel is allowed to contain further particles, beyond the product list. By contrast,
     
        id:offIfMatch   = product1 product2 .... 
        id:onIfMatch    = product1 product2 .... 
        id:onPosIfMatch = product1 product2 .... 
        id:onPosIfMatch = product1 product2 .... 
    
    requires the decay-channel multiplicity to agree with that of the product list, but otherwise works as the onIfAll/offIfAll methods.

    Note that the action of several of the commands depends on the order in which they are executed, as one would logically expect. For instance, id:oneChannel removes all decay channels of id and thus all previous changes in this decay table, while subsequent additions or changes would still take effect. Another example would be that 23:onMode = off followed by 23:onIfAny = 1 2 3 4 5 would let the Z^0 decay to quarks, while no decays would be allowed if the order were to be reversed.

    b) The Pythia readString(string) method actually does not do changes itself, but sends on the string either to the ParticleData class or to the Settings one. If desired, it is possible to communicate directly with the corresponding ParticleData method:

        pythia.particleData.readString("111:mayDecay = off"); 
        pythia.particleData.readString("15:2:products = 16 -211"); 
    
    In this case, changes intended for Settings would not be understood.

    c) Underlying this are commands for all the individual properties in the ParticleDataTable class, one for each. Thus, an example now reads

        pythia.particleData.mayDecay(111, false);
    
    Boolean values should here be given as true or false.

    d) A simpler and more useful way is to collect all your changes in a separate file, with one line per change, e.g.

        111:mayDecay = off
    
    The file can be read by the
        pythia.readFile(fileName); 
    
    method, where fileName is a string, e.g. pythia.readFile("main.cmnd"). Each line is process as described for the string in 2a). This file can freely mix commands to the Settings and ParticleData classes.
  3. A routine reInit(fileName) is provided, and can be used to zero the particle data table and reinitialize from scratch. Such a call might be required if several Pythia objects are created in the same run, and requested to have different values - by default the init() call is only made the first time. Several pythia with different values would have to run sequentially and not in parallel, though; recall that there is only one instance of the particle data table.

  4. You may at any time obtain a listing of all the particle data by calling

        pythia.particleData.listAll();
    
    The listing is by increasing id number. It shows the basic quantities introduced above. Some are abbreviated in the header to fit on the lines: spn = spinType, chg = chargeType, col = colType, res = isResonance, dec = mayDecay && canDecay (the latter checks that decay channels have been defined), ext = doExternalDecay, vis = isVisible and wid = doForceWidth.
    To list only those particles that were changed (one way or another, the listing will not tell what property or decay channel was changed), instead use
        pythia.particleData.listChanged();
    
    (This info is based on a further hasChanged flag of a particle or a channel, set true whenever any of the changing methods are used. It is possible to manipulate this value, but this is not recommended.) By default the internal initialization of the widths of resonances such as gamma^*/Z^0, W^+-, t/tbar, H^0 do not count as changes; if you want to list also those changes instead call listChanged(true).
    To list only one particle, give its id code as argument to the list(...) function.. To list a restricted set of particles, give in their id codes to list(...) as a vector<int>.
  5. For wholesale changes of particle properties all available data can be written out, edited, and then read back in again. These methods are mainly intended for expert users. You can choose between two alternative syntaxes.

    a) XML syntax, using the <particle and <channel lines already described. You use the method particleData.listXML(fileName) to produce such an XML file and particleData.readXML(fileName) to read it back in after editing.

    b) Fixed/free format, using exactly the same information as illustrated for the <particle and <channel lines above, but now without any tags. This means that all information fields must be provided (if there is no antiparticle then write void), in the correct order (while the order is irrelevant with XML syntax), and all on one line. Information is written out in properly lined-up columns, but the reading is done using free format, so fields need only be separated by at least one blank. Each new particle is supposed to be separated by (at least) one blank line, whereas no blank lines are allowed between the particle line and the subsequent decay channel lines, if any. You use the method particleData.listFF(fileName) to produce such a fixed/free file and particleData.readFF(fileName) to read it back in after editing.

    As an alternative to the readXML and readFF methods you can also use the particleData.reInit(fileName, xmlFormat) method, where xmlFormat = true (default) corresponds to reading an XML file and xmlFormat = false to a fixed/free format one.

    To check that the new particle and decay tables makes sense, you can use the particleData.checkTable() method, either directly or by switching it on among the standard error checks.