CERN Program Library Long Writeup W5013 - CERNLIB ...

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[52] F.Bloch. Z. fur Phys., 81:363, 1933. [53] R.M.Sternheimer. Phys. Rev. B, 3:3681, 1971. [54] H.Messel and D.F. Crawford. Pergamon Press, Oxford, 1970. [55] Particle Data Group. Lawrence Berkeley Laboratory and CERN, 1992. [56] G.N.Patrick. Physical processes in the simulation of electromagetic cascades. In Workshop on Shower Simulation for LEP Experiments, January 1985. [57] L. Landau. On the Energy Loss of Fast Particles by Ionisation J. Phys. 8:201, 1944. In D.ter Haar, editor, L.D.Landau, Collected papers, page 417. Pergamon Press, Oxford, 1965. [58] K.S.Kölbig and B.Schorr. Asymptotic expansion for the Landau density and distribution functions. Comp. Phys. Comm., 32:121, 1984. [59] R.Talman. On the statistics of particle identification using ionization. Nucl. Inst. Meth., 159:189, 1979. [60] R.Jones. Private communication to a GEANT monthly meeting. [61] P.V.Vavilov. Ionisation losses of high energy heavy particles. Soviet Physics JETP, 5:749, 1957. [62] B.Schorr. Programs for the Landau and the Vavilov distributions and the corresponding random numbers. Comp. Phys. Comm., 7:216, 1974. [63] S.M.Seltzer and M.J.Berger. Energy loss straggling of protons and mesons. In Studies in Penetration of Charged Particles in Matter. Nuclear Science Series 39, Nat. Academy of Sciences, Washington DC, 1964. [64] F.James. Program formerly in the CERN Program Library, but now replaced by G110, entry RAN- LAN. [65] J.E.Moyal. Theory of ionisation fluctuations. Phil. Mag., 46:263, 1955. [66] K.S.Kölbig and B.Schorr. A program package for the Landau distribution. Comp. Phys. Comm., 31:97, 1984. [67] A. Rotondi and P. Montagna. Fast calculation of Vavilov distribution. Nucl. Inst. Meth., B47:215, 1990. [68] W. W. M. Allison and J. H. Cobb. Ann. Rev. Nucl. Part. Sci., 30:253, 1980. [69] S. K. Kotelnikov V. M. Grishin, V. K. Ermilova. Nucl. Instr. Meth., A307:273, 1991. [70] At. data Nucl. data tables, 20:1, 1978. [71] At. data Nucl. data tables, 27:2, 1982. [72] At. data Nucl. data tables, 32:1, 1985. [73] J.B.Birks. The theory and practice of Scintillation Counting. Pergamon Press, 1964. [74] R.L.Craun and D.L.Smith. Nucl. Inst. and Meth., 80:239–244, 1970. [75] S.M. Seltzer and M.J. Berger. Nucl. Inst. Meth., B12:95, 1985. [76] A.B.Migdal. Phys. Rev., 103:1811, 1956. [77] L.Kim, R.H.Pratt, S.M.Seltzer, and M.J.Berger. Phys. Rev., A33:3002, 1986. PHYS530 – 6 330
[78] R.W.Williams. Fundamental Formulas of Physics, volume 2. Dover Pubs. Inc, 1960. [79] W.Heitler. The Quantum Theory of radiation. Clarendon Press, Oxford, 1954. [80] D. Vaughan. X-Ray Data Booklet. Center for X-Ray Optics, 1986. [81] R.Maier. In CERN Accelerator School. CERN, 17-28 September 1990. CERN 91-04. [82] C.Bricman et al. Rev. Mod. Phys., 52, 1980. [83] H.H.Andersen and J.F.Ziegler. Hidrogen stopping powers and ranges in all elements. Pergamon Press, 1977. [84] R.M.Sternheimer. Phys. Rev., 88:851, 1952. [85] R.M. Sternheimer. Phys. Rev., 183:511, 1956. [86] W.H.Barkas. Technical Report 10292, UCRL, August 1962. [87] C.R.Serre. Technical Report 67 5, CERN, March 1967. [88] C.R.Serre. Technical Report 71 18, CERN, September 1971. [89] H.K.Reynold et al. Phys. Rev., 92:742, 1953. [90] D.W.Green et al. Phys. Rev., 98:466, 1955. [91] N.Sakamoto et al. Rad. Effects and Defects in Solids, 117:193, 1991. [92] W.H.Barkas and M.J. Berger. Technical Report SP 3013, NASA, 1964. [93] H.H.Andersen and J.F.Ziegler. Helium stopping powers and ranges in all elements. Pergamon Press, 1977. [94] W.Heinrich et al. Technical Report GSI-91-30, GSI, Darmstad, June 1991. [95] F.Hubert et al. At. Data Nucle. Data Tables, 46:1, 1990. [96] C.Tschalär and H.D.Maccabee. Phys. Rev. B, 1:2863, 1970. [97] H.Geisel et al. NIM, 194:21, 1982. [98] H.Schmidt-Böring and H.Harnung. Z.f.Phys., A286:253, 1978. [99] W. Lohmann and R. Voss. Yellow Report 85 03, CERN, 1985. [100] P.Marmier and E.Sheldon. volume 1. Academic Press, 1969. [101] P.A.Aarnio, A.Fassò, A.Ferrari, J.-H.Moehring, J.Ranft, P.R.Sala, G.R.Stevenson and J.M.Zazula. Electron-photon transport: always so good as we think? Experience with FLUKA. In MC93 Int. Conf. on Monte-Carlo Simulation in High-Energy and Nuclear Physics, Tallahassee, Florida, 22-26 February 1993. Proceedings in press. [102] A.Ferrari and P.R.Sala. A New Model for hadronic interactions at intermediate energies for the FLUKA code. In MC93 Int. Conf. on Monte-Carlo Simulation in High-Energy and Nuclear Physics, Tallahassee, Florida, 22-26 February 1993. Proceedings in press. [103] J.O. Johnson and T.A. Gabriel. A User’s Guide to MICAP: A Monte Carlo Ionization Chamber Analysis Package. Technical Report TM-10340, ORNL, 1988. [104] J.O. Johnson and T.A. Gabriel. Development and Evaluation of a Monte Carlo System for Analysis of Ionization Chamber Responses. Technical Report TM-10196, ORNL, 1987. [105] C.Zeitnitz T.Gabriel. In Proc. of International Conference on Calorimetry in High Energy Physics, Tallahasse, FL, USA, February 1993. 331 PHYS530 – 7
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CERN Program Library Long Writeup W
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Chapter 1: Catalog of Geant section
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IOPA500 KINE001 KINE100 KINE199 KIN
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Geant 3.21 GEANT User’s Guide AAA
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The routines made available for GEA
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outines, then you can type the foll
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AAAA Bibliography [1] H.J. Klein an
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2 Event simulation framework The fr
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• after each tracking step along
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GUDIGI GUOUT GTRIGC UGLAST GLAST GU
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Particles JPART Materials JMATE/JTM
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3 Summary of GEANT data records 3.1
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3.4 User applications KEY N I VAR S
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Geant 3.16 GEANT User’s Guide BAS
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SUBROUTINE UGEOM + (’TGT ’,2,
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LQ(JHEAD-1) user link IQ(JHEAD+1) I
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VALUE = GARNDM (DUMMY) DUMMY (REAL)
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Geant 3.16 GEANT User’s Guide CON
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1 Energy binning IDECAD Bin number
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Particle No. Mass(GeV) Charge Life
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¯Ω + ¯Ξ 0 π + 23.60 ¯ΛK + 67
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Geant 3.16 GEANT User’s Guide DRA
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The main drawing routines are: GDRA
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Another feature which is available
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z y x C CHARACTER*4 CHNAMS(5) INTEG
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CALL GDRAWC(’OPAL’,2,0.,10.,10.
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CALL GSATT(’HB’,’FILL’,3) C
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CALL GDRAW(’CAVE’,40.,40.,0.,10
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Figure 16: Example of use of GDSPEC
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CALL GDOPEN(3) CALL GDRAWC(’ALEF
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6 NKVIEW IVIEW JDRAW NKVIEW JV = IB
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SHAD EDGE when HIDE is ON, selects
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x1xxxx 1xxxxx add the text EVENT NR
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DRAW Bibliography [1] R.Bock et al.
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2 Volumes with contents A volume ca
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The user can position a volume thro
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0 1 2 1 0 1 0 1 2 3 4 5 6 7 Figure
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2 Divisions along arbitrary axis As
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9.BL2 half-length along x of the si
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1.DZ half-length along the z axis;
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ECAL BOX specifications 18/11/93 EC
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ECAL SPHE specifications 18/11/93 E
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Geant 3.16 GEANT User’s Guide GEO
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• if the CHONLY flag is set to MA
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y y x x y y y y z z x x z z y y x x
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CAVE PAR1 specifications 20/10/94 y
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Dynamic ordering The list of neighb
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are represented by their values. A
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Where • @302 is the block number
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GEOM Bibliography [1] French Standa
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Geant 3.16 GEANT User’s Guide HIT
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ITRA NUMBV HITS NHITS (INTEGER) is
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HITS Bibliography 175 HITS510 - 3
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Geant 3.16 GEANT User’s Guide IOP
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0 if only IER] structures read in o
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Geant 3.16 GEANT User’s Guide IOP
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IOPA Bibliography [1] J.Zoll. ZEBRA
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Geant 3.16 GEANT User’s Guide KIN
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NTRACK ITRA JKINE NTRACK JK 1 2 3 4
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Geant 3.16 GEANT User’s Guide PHY
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Below are listed the data record ke
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Computation of total crosssection o
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7. Update the number of interaction
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1= generation of secondaries enable
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DEEMAX The formula used by GEANT is
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The second problem has been solved
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GPHYSI Initialisation of physics pr
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• the mean number of tries is not
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as function of the variable u = Eθ
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GEANT 3.16 GEANT User’s Guide PHY
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where N Z(Z i ) A(A i ) ρ σ Avoga
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Word # PHFN bank (data area, contin
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2 Method If the energy of the radia
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The Auger or Coster-Kronig transiti
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where: n number of energy bins q i
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• Case dielectric → metal. The
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| ⃗ k| = | ⃗ k ′′ | = k =
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Case dielectric → metal In this c
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5 Processes involving Čerenkov pho
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Much of the difficulty in approxima
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CALL GMOLIE (OMEGA,BETA2,DIN*) OMEG
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where λ 0 = ¯h/p Compton waveleng
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2.3 Sampling of the distribution fu
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X 0 is the radiation length. From (
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where we have set Θ=θ/χ α . To
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The variable DCUTE in common /GCCUT
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2.2 Total cross-sections The integr
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For the other charged particles the
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POTI POTIL (REAL) average ionisatio
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where φ(λ) = 1 ∫ c+i∞ exp (u
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Counts 900 800 Landau 700 40 600 20
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Fast simulation for n 3 ≥ 16 If t
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ξ/E Max (hereafter κ) relative im
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ln(∫ σ γ dE/norm.factor) -4 -6
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VALUE = GBFSIG (T,C) GBFSIG calcula
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Page 311 and 312: VALUE = GBRSGM (Z,T,BCUT) Z T BCUT
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Page 341 and 342: VECT,SNEXT,SAFETY Compute distance
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Page 347 and 348: SUBROUTINE GUSTEP +SEQ,GCKING,GCVOL
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Page 361 and 362: YMED R “ Center Y coordinate ”
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Print matrixes’ specifications. 5
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6 GEANT/CREATE It creates volumes o
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YES NO 6.7 SCONS name numed inrdw o
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7 GEANT/CONTROL Control commands. 7
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To change lout in /GCUNIT/ Note: un
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IPART I “Particle number” NAPAR
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8.5 CDIR [ chpath chopt ] CHPATH C
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9 GEANT/FZ ZEBRA/FZ commands 9.1 FZ
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Check the structure of one or more
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FACTL R “Scale factor for SL” D
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12 GEANT/PHYSICS Commands to set ph
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Possible IDRAY values are: 0 1 2 To
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12.14 PAIR [ ipair ] IPAIR C “Fla
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PPCUTM R “Cut for e+e- pairs by m
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LGET_15 C “user word” LGET_16 C
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13.6 GEOM [ lgeom˙1 lgeom˙2 lgeom
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LSTAT_7 C “user word” LSTAT_8 C
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Geant 3.21 GEANT User’s Guide XIN
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XINT Bibliography [1] R.Brun and P.
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This common contains the threshold
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ITR3D track being scanned (used tog
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NCLAS1 NCLAS2 NCLAS3 IHOLE CGXMIN C
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* PARAMETER (MAXJMP=30) COMMON/GCJU
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GYMAX GZMIN GZMAX GXXXX GYYYY GZZZZ
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DENS density of current material in
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RADDEG radiants to degrees conversi
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PCUTNE parameterisation threshold f
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SMULS SOMULS STMULS DPHYS3 ILABS SL
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NTETA TETMIN TETMAX MODTET number o
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S2 S3 SS1 SS2 SS3 LEP IPORLI ISUBLI
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CFIELD constant for field step eval
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NEXT 1 particle has reached the bou
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C COMMON/GCVOL2/NLEVE2,NAMES2(15),N
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STEP PLIN PLOG BE2 PLASM TRNSMA BOS
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C ESHELL - Shells potentials in eV
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Geant 3.11 GEANT User’s Guide ZZZ
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GFKINE KINE001, KINE100, KINE199 GF
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GPSTAT GEOM700 GPTMED CONS001, CONS
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ZZZZ Bibliography [1] T.Sjöstrand
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CDRSGA, 297 CGMULO, 221 CHANGEWK, 3
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GEANT/DRAWING/KHITS, 372 GEANT/DRAW
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GPART, 13, 46, 61, 293 GPCXYZ, 40,
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PATCHY, 278 PCUTS, 399 PDIGI, 389 P
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