✍ Scribed by K. Hänssgen; S. Ritter
No coin nor oath required. For personal study only.
In high energy particle collision secondary particles will be Catalogue number: ACFS created, among which are also unstable hadron resonances. The code DECAY samples the decay of unpolarized baryon and Program obtainable from: CPC Program Library, Queen's Uni-meson resonances in the laboratory frame. DECAY treats some versity of Belfast, N. Ireland (see application form in this issue) of the resonances including all baryon resonances of the spin 3/2 + decuplet and all meson resonances of the spin 1 -nonet. Computer: ESER and IBM System 370; Installation: Karl-A given resonance decays via two or three particle decay steps Marx-Universität Leipzig, DDR and CERN, Geneva, Switzer-until all decay products are stable particles. land method of solution Operating system: MVT 6.1 The decay of baryon and meson resonances is simulated by a two and three body phase space Monte Carlo model. Programming language used: FORTRAN IV Restriction on the complexity of the problem High -speed storage required: 70 Kbytes Only decay modes according to the particle group tables [1] with branching ratio greater than 1% are considered. The Number of bits in a word: 32 program also treats some decays of charmed mesons and baryons. Peripherals used: card reader and line printer Typical running time Number of lines in combined program and test deck: 899 The decay of a typical resonance into three final stable particle needs approximately 0.01 s of central processor time on an Other program necessary for DECAY:
ESER 1040 computer.
-Function RNDM(DUMMY) generates random numbers uniformly distributed between 0 and 1 Reference [11Particle Data Group, M. Roos et al., Phys. Lett. I11B (1982)
📜 SIMILAR VOLUMES
Title of the program: MCSDA transport in thin films. It uses the continuous slowing down approximation (CSDA) suitably corrected to include energy Catalogue number: AALC straggling. Elastic and inelastic cross sections in the Born approximation, allowing analytical random sampling, are de-Program ob
Experimental kineticists are always faced with the problem of reducing kinetic data to extract physically meaningful information. A particularly vexing problem arises when different models reproduce the data but yield different values for the physical parameters. For over forty-five years Monte Carl
## Abstract Contributions of the covalent and ionic species to the chain building in cationic reversible polymerizations are analyzed by means of Monte Carlo simulations and by solving the formulated set of equations. The validity of the equation for the contribution of covalent propagation, derive
## Abstract By use of the pivot algorithm, star‐branched chains with __F__ = 4, 8 and 12 arms of length __n__ and linear chains (__F__ = 2) are generated on a tetrahedral lattice (120 ≤ __nF__ ≤ 3 840). By taking into account nearest neighbour interactions (each contact contributes an energy ϕ __kT