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CompHEP: Present and Future

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Title: CompHEP: Present and Future


1
CompHEP Present and Future
  • Alexandre Kryukov
  • on behalf of CompHEP collaboration
  • (E. Boos, V. Bunichev, M. Dubinin, L. Dudko, V.
    Ilyin, A. Kryukov, V. Edneral
  • V. Savrin, A. Semenov, A. Sh.)

2
  • General motivation and goals
  • How CompHEP works symbolic and numerical parts
  • Physics Models
  • Flavour combinatorics simplification
  • Large-scale calculations distributive
    calculation, batch scripts
  • Interface to PYTHIA
  • MCDB MC Database for particle event samples -gt
    L.Dudko, next report.
  • Concluding remarks

3
  • The increase of the collider energies requires
    simulation of processes for more and more complex
    processes with better and better precision (NLO,
    NNLO, NLL resummation)
  • LEP I basically 2 fermion physics
  • LEP II basically 4 fermion physics
  • TEVATRON, LHC and LC 4,5,6 and even 8 fermion
    physics with additional hard photons and/or
    gluons (jets)
  • Single top in the t-channel mode 5 fermions
  • Top pair production with decays 6 fermions
  • Strongly interacting Higgs sector in hadron
    collisions
    6 fermions
  • Yukawa coupling 8 fermions

4
Large number of diagrams and large number of
subprocesses (Tevatron, LHC)
  • A number of automatic (may be partly) programs
    can be found on the market CompHEP, GRACE,
    MadGraph, AlpGen, Omega/WHIZARD, Amegic, ...
  • Goals
  • Automation of tree level diagram calculations
  • A full computational chain from Lagrangian until
    event flow.
  • Interfacing to other generators (for showering
    and hadronization) for full simulation.
  • Interfacing to NLO cross section calculators
    (programs calculating full NLO or higher
    number)

5
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6
  • CompHEP generates Tree Level Feynman diagrams for
    a given parton process
  • Symbolically calculates squared Feynman diagrams.
    User (mostly for theoretical investigation) can
    output precise symbolic formular for squared
    matrix elements.
  • MC algorithm to obtain total cross section,
    different distribution and generation of event
    flow.
  • Rich set of model CompHEP can work with
    0,1/2,1-spin particles, Majorana and Dirac
    spinors, ghosts fields, 3- and 4-leg vertices.
  • User-friendly interface GUI interfaces for
    symbolic and numerical CompHEP parts, case
    sensitive build-in help (F1), simple batch
    scripts.

7
  • Choose physics model SM, MSSM, your own. User
    can change model parameters (masses, couplings,
    etc.), add/remove/change vertices and composite
    particles in existing models or in his(her) own
    models.
  • Set initial beams or decay particle and set a
    final state. CompHEP generates corresponding
    Feynman diagrams. User can look at and remove
    some particular diagrams or subprocesses.
  • Prepare a numerical MC generator. CompHEP squares
    and symbolically calculates the diagrams. After
    that it can keep them as a C/REDUCE/FORM code.
    The most applicable case C code. By standard
    make CompHEP compiles and links a program for
    numerical calculations for the process (numerical
    Monte-Carlo generator)

8
  • Set necessary kinematic cuts, Q2, PDF set, etc.
  • Customize numerical MC generator. The most
    complicated part is selection of right phase
    space parametrization and regularizations of
    singularities.
  • Calculate full cross section and distributions.
    CompHEP uses adaptive VEGAS algorithm for MC
    calculations. User may set different variables
    (PT, inv. mass, rapidity, etc.) to draw
    corresponding distributions.
  • Generates events. After cross section calculation
    CompHEP can generate events for the given
    process. User set a number of the events.
  • If the process consists of some subprocesses, the
    procedure applies to the each subprocess.

9
  • There are several models implemented in CompHEP
  • Simple teaching models QED and Fermi Model
  • Standard Model both in unitary and
    t'Hooft-Feynman gauges
  • Complete MSSM both in unitary and t'Hooft-Feynman
    gauges with the Higgs sector .
  • mSUGRA and GMSB models.
  • The FeynHiggs and ISASUSY library are necessary.
  • Some models are available by request
  • Top quark Lagrangian with anomalous couplings as
    follows from the dimension 6 effective operators
  • Excited fermion Model
  • Complete two-Higgs-doublet Model with conserved
    or broken CP invariance

LanHEP program (the part of the CompHEP project)
allows to generate Fynmann rules for new models
from (effective) Lagrangian.
10
  • A serious computational problem is the large
    number of partonic subprocesses at hadron
    machines (for example, pp-gt Wjj consist of 472
    subprocesses).
  • Reasons
  • Many quark partons with different flavors
  • Many additional diagrams for each subprocess
    because of CKM quark mixing
  • Basic ideas
  • Rotation of down quarks thus, transfering the
    mixing matrix elements from vertices of
    subprocess Feynman diagrams to PDFs
  • Diagrams are divided into gauge invariant classes
    which are convoluted with different combinations
    of PDFs

E.Boos, et al. JHEP 0005 (2000) 052
11
  • Hash models in CompHEP. Transferring of CKM
    elements to PDFs allows to unify two generations
    of light quarks to one hash generation
    (u, d)
  • Two approximations
  • 1) Mu Md Ms Mc 0
  • Advantage
  • SM, pp--gtWjj 472 processes, 6160 diagrams
  • Hash SM 42 subprocesses, 532 diagrams

12
  • Symbolic batch (symb_batch.pl)
  • All parameters are set in a file (process.dat)
    and scipts launches CompHEP in a non-GIU mode
    with these parameters
  • Numerical batch (num_batch.pl)
  • MC generators parameters are kept in one file
    (batch.dat) for all subprocesses
  • The batch script starts numerical calculations
    including all (or some) usual steps in CompHEP
    cross section calculation, event generation
  • MC generator customization is realized by hands
    or in GUI mode.
  • num_batch.pl has detailed help (run
    ./num_batch.pl help)

13
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14
  • The CompHEP-PYTHIA interface allows to use
    processes 2--gt2..6 computed by CompHEP as new
    processes for PYTHIA
  • Main goal provide ISR/FSR, hadronization
    (including jet fragmentation) and decays by
    PYTHIA.
  • CompHEP generates unweighted events and writes to
    event files.
  • Special mix_flows utility mixes several event
    files in one event file according to their
    relative contributions to cross section. The file
    can is used by PYTHIA as input.
  • We provide the interface library and an example
    of program (main.f).

15
  • CompHEP with the interface to PYTHIA is a
    powerful tool for a simulation of different
    physical processes at hadron and lepton
    colliders.
  • CompHEP allows to study problem for wide set of
    physics models SM, MSSM (two gauges, some SUSY
    violation scenarios). Physicist can create and
    use own model.
  • Comphep calculates cross section, prepares
    different distributions, generates unweighted
    event flow and more.
  • CompHEP is compatible with Les Houches Accord I.
    The interface with Pythia allows to generate
    event flow that is ready for further
    investigations by phenomenologiests and/or
    experimentalists.
  • Symbolic and numerical batch modes simplify
    large-scale calculations
  • The CompHEP is the LO program. However it allows
    to include (partly) some NLO corrections NLO
    Tree Level 2--gtN1 corrections to the process
    2-gtN can be computed. One can include NLO
    structure functions, loop relations between
    parameters (K-factors), and existing from papers
    loop contributions as effective vertices
    (functions).

16
  • The nearest plans
  • Development of distributed Monte-Carlo
    calculation and event generation on computer
    clusters as well as GRID capabilities.
  • Implementation of the FORM computer algebra
    program for symbolic calculations form-factors,
    new symbolic algorithms, models with extra
    dimensions, dimensional regularization, spin
    density matrices for external lines of squared
    diagrams
  • Les Houches Accord I based interface to HERWIG
  • Les Houches Accord II based interface to PDFs
  • SUSY Les Houches Accord (III) based interface to
    various SUSY parameter, mass (etc.) calculation
    codes.
  • The long term plans
  • Amplitude techniques for symbolical and numerical
    calculations including the 1-loop case.
  • Automation of regularization singularities.
  • Incorporation of the gauge invariant classes of
    diagrams.

17
  • CompHEP collaboration E. Boos, V. Bunichev, M.
    Dubinin, L. Dudko, V. Ilyin, A. Kryukov, V.
    Edneral, V. Savrin, A. Semenov, A. Sh.
  • CompHEP homepage http//theory.sinp.msu.ru/comphe
    p There are CompHEP itself, LanHEP, cpyth
    (CompHEP-PYTHIA interface)
  • References
  • early CompHEP versions (3., 41.10) A. Pukhov
    et al., Preprint INP MSU 98-41/542,
    hep-ph/9908288.
  • recent CompHEP versions (4.2p1, 4.4.0) E. Boos
    et all., CompHEP 4.4.0, hep-ph/0403123, will be
    published in Proceedings of ACAT03

18
CompHEP Collaboration(incomplete list)
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