CERN Program Library Long Writeup W5013 - CERNLIB ...

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PHYS Bibliography [1] H.C.Fesefeldt. Simulation of hadronic showers, physics and applications. Technical Report PITHA 85-02, III Physikalisches Institut, RWTH Aachen Physikzentrum, 5100 Aachen, Germany, September 1985. [2] P.A.Aarnio et al. Fluka user’s guide. Technical Report TIS-RP-190, CERN, 1987, 1990. [3] A.Fassò A.Ferrari J.Ranft P.R.Sala G.R.Stevenson and J.M.Zazula. FLUKA92. In Proceedings of the Workshop on Simulating Accelerator Radiation Environments, Santa Fe, USA, 11-15 January 1993. [4] A.Fassò A.Ferrari J.Ranft P.R.Sala G.R.Stevenson and J.M.Zazula. A Comparison of FLUKA Simulations with measurements of Fluence and Dose in Calorimeter Structures. Nuclear Instruments & Methods A, 332:459, 1993. [5] C.Birattari E.DePonti A.Esposito A.Ferrari M.Pelliccioni and M.Silari. Measurements and characterization of high energy neutron fields. approved for pubblication in Nuclear Instruments & Methods A. [6] P.A.Aarnio, A.Fassò, A.Ferrari, J.-H.Moehring, J.Ranft, P.R.Sala, G.R.Stevenson and J.M.Zazula. FLUKA: hadronic benchmarks and applications. In MC93 Int. Conf. on Monte-Carlo Simulation in High-Energy and Nuclear Physics, Tallahassee, Florida, 22-26 February 1993. Proceedings in press. [7] Particle Data Group. Review of particle properties. Physical Review D, 45(11), June 1992. [8] R.Brun, M.Goossens, and J.Zoll. ZEBRA Users Guide, Program Library Q100. CERN, 1991. [9] J.H.Hubbell, H.A.Gimm, and I.Overbo. Jou. Phys. Chem. Ref. Data, 9:1023, 1980. [10] J.C.Butcher and H.Messel. Nucl. Phys, 20:15, 1960. [11] J.M.Hammersley and D.S.Handscomb. Monte Carlo methods. J.Wiley et Sons Inc, New York, 1964. [12] R.Ford and W.Nelson. SLAC 210, UC 32. SLAC, June 1978. [13] Y-S.Tsai. Rev. Mod. Phys., 46:815, 1974. [14] Y-S.Tsai. Rev. Mod. Phys., 49:421, 1977. [15] W.R.Nelson et al. The EGS4 code system. Technical Report 265, SLAC, 1985. [16] O.Klein and Y.Nishina. Z. f. Physik, 52:853, 1929. [17] H.Messel and D.F.Crawford. volume 3. Pergamon Press, 1970. [18] B.Rossi. Prentice-Hall, 1952. [19] F. Biggs and R. Lighthill. Analitycal approximations for x-ray cross sections 3. Sandia National Lab., SAND87-0070 UC-34, 1987. [20] H. Bethe and E. Salpeter. Encyclopedia of Physics, volume XXXV. Springer-Verlag, Berlin, 1957. [21] H. Hall. The theory of photoelectric absorbtion for x-rays and γ-rays. Rev. Mod. Phys., 8:358, 1936. [22] R. H. Pratt. Atomic photoelectric effect at high energies. Phys. Rev., 117:1017, 1960. [23] R. H. Pratt. Photoeffect form the l shell. Phys. Rev., 119:1619, 1960. [24] WM. J. Veigele. Photon cross sections from 0.1 kev to 1 mev for elements z = 1toz= 94. Atomic Data Tables, 5:51, 1973. PHYS530 – 4 328
[25] M. Gavrila. Relativistic l-shell photoeffect. Phys. Rev., 124:1132, 1961. [26] F. Sauter. Ann. Physik, 9:217, 1931. [27] F. Sauter. Ann. Physik, 11:454, 1931. [28] M. Gavrila. Relativistic k-shell photoeffect. Phys. Rev., 113:514, 1959. [29] B. C. H. Nagel and P. O. M. Olsson. Arkiv f. Fysik, 18:1, 1960. [30] M. O. Krause. Atomic radiative and radiationless yields for k and l shells. J. Phys. Chem. Ref. Data, 8:307, 1979. [31] S.T. Perkins et al. UCRL-50400, 30, 1991. [32] J. H. Scofield. Relativistic hatree-slater values for k and l x-ray emission rates. Atomic Data and Nuclear Data Tables, 14:121, 1974. [33] J.H.Hubbell and I.Overbo. J. Phys. Chem. Ref. Data, 1/8, 1979. [34] H.Storm and H.I.Israel. Nucl. data tables. A7:565, 1970. [35] W.R.Nelson, H.Hirayama, and D.W.O.Rogers. Technical Report 265, SLAC, 1985. [36] J.D.Jackson. Classical Electrodynamics. J.Wiley et Sons, Inc, New York, 1975. [37] H.A.Bethe. Phys. Rev., 89:1256, 1953. [38] B.Rossi. Prentice-Hall, Englewood Cliffs, 1961. [39] B.Rossi and K.Greisen. Rev. Mod. Physics, 13:240, 1941. [40] V.L.Highland. Nucl. Inst. and Meth., 129:497, 1975. [41] V.L.Highland. Nucl. Inst. and Meth., 161:171, 1979. [42] G.R.Lynch and O.I.Dahl. Approximation to multiple coulomb scattering. Technical Report LBL- 28165, Physics Division, Laurence Berkeley Laboratory, University of California, Berkeley, CA 94720, February 1990. [43] G.Z.Molière. Theorie der Streuung schneller geladener Teilchen I: Einzelstreuung am abgerschmitten Coulomb-Feld. Z. Naturforsch., 2a:133, 1947. [44] G.Z.Molière. Theorie der Streuung schneller geladener Teilchen II: Merfach- und Vielfachstreuung. Z. Naturforsch., 3a:78, 1948. [45] W.T.Scott. Rev. Mod. Phys., 35:231, 1963. [46] S.Goudsmit and J.L.Saunderson. Multiple scattering of electrons. Phys. Rev., 57:24, 1940. [47] S.Goudsmit and J.L.Saunderson. Multiple scattering of electrons II. Phys. Rev., 36:36, 1940. [48] T.M.Jenkins, W.R.Nelson, and A.Rindi. MonteCarlo transport of electrons and photons. Plenum Press, New York, 1988. [49] E.Keil, E.Zeitler, and W.Zinn. Zur Einfach- und Mehrfachstreuung geladener Teilchen. Z.Naturforsch., 15a:1031, 1960. [50] S.M. Selzer M.J. Berger. Technical Report SP 3012, NASA, 1964. [51] H.A.Bethe. Ann. Phys., 5:325, 1930. 329 PHYS530 – 5
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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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Page 353 and 354: CALL GRKUTA (CHARGE,STEP,VECT,VOUT*
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Page 361 and 362: YMED R “ Center Y coordinate ”
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5 GEANT/GEOMETRY Geometry commands.
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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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