CERN-TH/96-158
UTHEP-96-0601
S. Jadach
Institute of Nuclear Physics,
ul. Kawiory 26a, Kraków, Poland
CERN, Theory Division, CH-1211 Geneva 23, Switzerland
W. P
aczek
Department of Physics and Astronomy,
The University of Tennessee, Knoxville, TN 37996-1200,
E. Richter-Was
Institute of Computer Science, Jagellonian University,
Kraków, ul. Reymonta 4, Poland,
CERN, Theory Division, CH-1211 Geneva 23, Switzerland
B.F.L. Ward
Department of Physics and Astronomy,
The University of Tennessee, Knoxville, TN 37996-1200,
SLAC, Stanford University, Stanford, CA 94309
Z. Was
Institute of Nuclear Physics,
Kraków, ul. Kawiory 26a, Poland,
CERN, Theory Division, CH-1211 Geneva 23, Switzerland
Submitted to Computer Physics Communications
CERN-TH/96-158
UTHEP-96-0601
June 1996
NEW VERSION SUMMARY
Title of the program: BHLUMI version 4.04
Reference to original program:
Comput. Phys. Commun. 70 (1992) 305
Computer: IBM rs6000, HP9000 and other UNIX workstations
Operating system: UNIX
Programming language used: FORTRAN 77
High speed storage required: < 5 MB
No. of bits in a word: 32
Peripherals used: Line printer
No. of cards in combined program and test deck: about 12000
Keywords: Radiative corrections, Monte Carlo simulation,
Bhabha scattering, bremsstrahlung, Quantum Electrodynamics (QED),
electroweak theory, structure functions.
Nature of physical problem:
The small-angle Bhabha scattering process is used in all
electron-positron colliders to calculate machine luminosity.
This process is subject to QED radiative corrections, which
have to be known for arbitrary cut-offs and/or acceptance
with a precision at least a factor of 2 better than the pure
experimental precision.
This means that the level of 0.05% should be reached.
A realistic simulation should include multiple emission
of the bremsstrahlung photons.
Method of solution: The Monte Carlo
simulation of the small-angle process is an ideal solution.
It provides the integrated cross-section for arbitrary cuts.
Direct simulation of the final state electrons and photons
is precisely what is needed for detector simulation purposes.
Restrictions on the complexity of the problem:
The overall precision of the QED calculation is restricted to 0.11%,
for a typical LEP/SLC luminometer angular range of
, where
is the scattering angle.
Typical running time:
The efficiency for multi-photon sub-generator
is typically 6 million variable-weight events
and 4 million constant-weight events per hour for
an HP9000-735/100 MHz machine.
LONG WRITE--UP