## SUSY Les Houches Accord

The PYTHIA 8 program does not contain an internal spectrum calculator (a.k.a. RGE package) to provide supersymmetric couplings, mixing angles, masses and branching ratios. Thus the SUSY Les Houches Accord (SLHA) [Ska04][All08] is the only way of inputting SUSY models, and SUSY processes (see the SUSYProcesses page) cannot be run unless such an input has taken place.

The SLHA input format can also be extended for use with more general BSM models, beyond SUSY. Information specific to how to use the SLHA interface for generic BSM models is collected below, under Using SLHA for generic BSM Models, with more elaborate explanations and examples in [Des11].

Most of the SUSY implementation in PYTHIA 8 is compatible with both the SLHA1 [Ska04] and SLHA2 [All08] conventions (with some limitations for the NMSSM in the latter case). Internally, PYTHIA 8 uses the SLHA2 conventions and translates SLHA1 input to these when necessary. See the section on SUSY Processes and [Des11] for more information. Note that PYTHIA assumes that a spectrum is either fully SHLA1 or fully SLHA2 compliant. Mixing of the two standards is discouraged, as this can lead to ambiguities and inconsistencies.

When reading LHEF files, Pythia automatically looks for SLHA information between `<slha>...</slha>` tags in the header of such files. When running Pythia without LHEF input (or if reading an LHEF file that does not contain SLHA information in the header), a separate file containing SLHA information may be specified using `SLHA:file` (see below).

Normally the LHEF would be in uncompressed format, and thus human-readable if opened in a text editor. A possibility to read gzipped files has been added, based on the Boost and zlib libraries, which therefore have to be linked appropriately in order for this option to work. See the `README` file in the main directory for details on how to do this.

Finally, the SLHA input capability can of course also be used to input SLHA-formatted `MASS` and `DECAY` tables for other particles, such as the Higgs boson, furnishing a less sophisticated but more universal complement to the standard PYTHIA 8-specific methods for inputting such information (for the latter, see the section on Particle Data and the scheme to modify it). This may at times not be desirable, so a few options can be used to curb the right of SLHA to overwrite particle data. Conversely, it is sometimes useful to allow the user to modify eg a mass parameter relative to its value in the SLHA spectrum. This is normally not permitted (the SLHA spectrum is normally self-consistent and should not be modified), but an option for allowing it is provided.

The reading-in of information from SLHA or LHEF files is handled by the `SusyLesHouches` class, while the subsequent calculation of derived quantities of direct application to SUSY processes is done in the `CoupSUSY`, `SigmaSUSY`, and `SUSYResonanceWidths` classes.

### Sanity Checks

As an aid for basic validation, some checks and ranges are imposed on SLHA input during initialization, as follows:

- Several parameters (`minMassSM`, and `SLHA:allowUserOverride`) provide some safety against unintentionally overwriting PYTHIA's Standard-Model information. These parameters can be altered to hand over more or less control to the SLHA interface. In particular, a lot of mass and decay-table information may be included by default in some SLHA files, without it being the explicit intention of the user to overwrite the corresponding PYTHIA information. The default values of the SLHA safety parameters have been chosen so as to eliminate at least the most obvious causes of Garbage In Garbage Out. (E.g., there is usually no reason to modify the masses of well-measured SM particles, like the W and Z bosons, nor to replace their sophisticated internal decay treatments by the simplified isotropic treatment used for SLHA DECAY tables.)
- For SLHA SUSY spectra, the interface checks the mass-ordering of the Higgs, Neutralino, and Chargino sectors, and the unitarity/orthogonality of the mixing matrices. It also performs some additional self-consistency checks on whether the correct SLHA BLOCKs for the given SUSY model have been included, and whether all required entries have been defined.
- If MASS or DECAY information for a particle has been changed by SLHA input, the following sanity checks will be carried out. The particle will be declared stable unless there is at least one on-shell decay channel open (regardless of the presence of any DECAY information). In particular, massless particles will always be declared stable. A lower cutoff is imposed on the Breit-Wigner shape of the particle, requiring its mass to remain above the sum of masses for the lightest decay channel. Subject to that constraint, the `mMin` and `mMax` cutoffs will normally be placed at 5 times the width or the on-shell mass divided by two, whichever is smaller, so that the default gives a decent sampling of the shape without straying too far from the on-shell value. The user is allowed to use the `mMin` and `mMax` parameters to choose a different sampling range if so desired (still subject to the constraint of at least one decay channel remaining open for on-shell decay products).
- For each decay channel in an SLHA DECAY table, PYTHIA will checks the available phase space. If the channel is on shell (sum of daughter masses is less than mass of decaying particle), then the threshold dependence is given by `SLHA:meMode`. If the channel is off shell, then an `meMode` of 100 is always used. As a further protection against GIGO, if the channel appears to be physically impossible (defined as requiring fluctuations of more than more than 100 times the effective combined widths), it is switched of and a warning message is printed.
- DECAY table branching fractions are always interpreted as positive. However, a negative sign for one or more channels can be given, and will then be interpreted to mean that the corresponding channel(s) should be switched off for the current run. This furnishes a simple way to switch SLHA DECAY channels on and off while preserving the sum of branching fractions equal to unity.

Note that these sanity checks will not catch all possible cases of Garbage In Garbage Out, so human verification of the input files is always a good idea, as is taking a look at any warnings or error messages printed by the SLHA interface during initialization. It is ultimately up to the user to ensure that sensible input is being given.

### SLHA Switches and Parameters

`mode` SLHA:readFrom (`default = 1`; `minimum = 0`; `maximum = 2`)
Controls from where SLHA information is read.
`option` 0 : is not read at all. Useful when SUSY is not simulated and normal particle properties should not be overwritten.
`option` 1 : read in from the `<slha>...</slha>` block of a LHEF, if such a file is read during initialization, and else from the `SLHA:file` below.
`option` 2 : read in from the `SLHA:file` below.

`word` SLHA:file (`default = void`)
Name of an SLHA (or LHEF) file containing the SUSY/BSM model definition, spectra, and (optionally) decay tables. Default `void` signals that no such file has been assigned.

`parm` SLHA:minMassSM (`default = 100.0`)
This parameter provides an alternative possibility to ignore SLHA input for all particles with identity codes below 1,000,000 (which mainly means SM particle, but also includes e.g. the Higgs bosons in two-Higgs-doublet scenarios) whose default masses in PYTHIA lie below some threshold value, given by this parameter. The default value of 100.0 allows SLHA input to modify the top quark, but not, e.g., the Z^0 and W^+- bosons.

`flag` SLHA:allowUserOverride (`default = off`)
Flag to set whether the user is allowed to modify the parameters read from an SLHA spectrum. Is normally kept `off` to preserve the internal self-consistency of SLHA spectra. If this flag is switched `on`, the mass values read from the SLHA block MASS are allowed to be modified by the user, using PYTHIA's standard `readString` and related methods.

### SLHA DECAY Tables

In addition to SUSY spectra, the SLHA also defines a set of conventions for decay tables. These are not restricted to SUSY models, but can be used for arbitrary particles, either in combination with or independently of the SUSY parts of the Accord. The settings in this section control whether and how PYTHIA will make use of such tables. See also the comments under sanity checks above.
Note: the PYTHIA SLHA interface is limited to at most `1→8` decays.

`flag` SLHA:useDecayTable (`default = on`)
Switch to choose whether to read in SLHA `DECAY` tables or not. If this switch is set to off, PYTHIA will ignore any decay tables found in the SLHA file, and all decay widths will be calculated internally by PYTHIA. If switched on, SLHA decay tables will be read in, and will then supersede PYTHIA's internal calculations, with PYTHIA only computing the decays for particles for which no SLHA decay table is found. (To set a particle stable, you may either omit an SLHA `DECAY` table for it and then use PYTHIA's internal `id:MayDecay` switch for that particle, or you may include an SLHA `DECAY` table for it, with the width set explicitly to zero.)

`flag` SLHA:allowOnlyOffShell (`default = off`)
Switch to allow a decay table with only off-shell decays. By default, internal checks require particles to have at least one on-shell decay mode.

`mode` SLHA:meMode (`default = 100`; `minimum = 100`; `maximum = 103`)
This value specifies how threshold, off-shell, and phase-space weighting effects for SLHA decay channels should be treated, using the same numbering scheme as for resonances. The default (100) is to use the branching fraction given in the SLHA DECAY tables without any modifications. The corresponding partial widths remain unchanged when the resonance fluctuates in mass. Specifically there are no threshold corrections. That is, if the resonance fluctuates down in mass, to below the nominal threshold for some decay mode, it is assumed that one of the daughters could also fluctuate down to keep the channel open. (If not, there may be problems later on.) Alternative options (with values 101+) documented under resonances allow for some flexibility to apply threshold factors expressing the closing of the on-shell phase space when the daughter masses approach or exceed the parent one. Note that modes that are extremely far off shell (defined as needing a fluctuation of more than 100 times the root-sum-square of the widths of the mother and daughter particles) will always be assigned `meMode = 100` and should be switched off by hand if so desired. It is up to the user to ensure that the final behaviour is consistent with what is desired (and/or to apply suitable post facto reweightings). Plotting the generator-level resonance and decay-product mass distributions (and e.g., mass differences), effective branching fractions, etc, may be of assistance to validate the behaviour of the program.

### Internal SLHA Variables

`mode` SLHA:verbose (`default = 1`; `minimum = 0`; `maximum = 3`)
Controls amount of text output written by the SLHA interface, with a value of 0 corresponding to the most quiet mode. The following variables are used internally by PYTHIA as local copies of SLHA information. User changes will generally have no effect, since these variables will be reset by the SLHA reader during initialization.

`flag` SLHA:NMSSM (`default = off`)
Corresponds to SLHA block MODSEL entry 3.

### Using SLHA for generic BSM Models

Using the `QNUMBERS` extension [Alw07], the SLHA can also be used to define new particles, with arbitrary quantum numbers. This already serves as a useful way to introduce new particles and can be combined with `MASS` and `DECAY` tables in the usual way, to generate isotropically distributed decays or even chains of such decays. (If you want something better than isotropic, sorry, you'll have to do some actual work ...)

A more advanced further option is to make use of the possibility in the SLHA to include user-defined blocks with arbitrary names and contents. Obviously, standalone PYTHIA 8 does not know what to do with such information. However, it does not throw it away either, but instead stores the contents of user blocks as strings, which can be read back later, with the user having full control over the format used to read the individual entries.

The contents of both standard and user-defined SLHA blocks can be accessed in any class inheriting from PYTHIA 8's `SigmaProcess` class (i.e., in particular, from any semi-internal process written by a user), through its SLHA pointer, `slhaPtr`, by using the following methods:

    bool slhaPtr->getEntry(string blockName, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, int jndx, double& val);
    bool slhaPtr->getEntry(string blockName, int indx, int jndx, int kndx, double& val);

This particular example assumes that the user wants to read the entries (without index, indexed, matrix-indexed, or 3-tensor-indexed, respectively) in the user-defined block `blockName`, and that it should be interpreted as a `double`. The last argument is templated, and hence if anything other than a `double` is desired to be read, the user has only to give the last argument a different type. If anything went wrong (i.e., the block doesn't exist, or it doesn't have an entry with that index, or that entry can't be read as a double), the method returns false; true otherwise. This effectively allows to input completely arbitrary parameters using the SLHA machinery, with the user having full control over names and conventions. Of course, it is then the user's responsibility to ensure complete consistency between the names and conventions used in the SLHA input, and those assumed in any user-written semi-internal process code.

Note that PYTHIA 8 always initializes at least the SLHA blocks MASS and SMINPUTS, starting from its internal SM parameters and particle data table values (updated to take into account user modifications). These blocks can therefore be accessed using the `slhaPtr->getEntry()` methods even in the absence of SLHA input. Note: in the SMINPUTS block, PYTHIA outputs physically correct (i.e., measured) values of GF, m_Z, and alpha_EM(m_Z). However, if one attempts to compute, e.g., the W mass, at one loop from these quantities, a value of 79 GeV results, with a corresponding value for the weak mixing angle. We advise to instead take the physically measured W mass from block MASS, and recompute the EW parameters as best suited for the application at hand.