CERN Program Library Long Writeup W5013 - CERNLIB ...

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RMAX R “ External radius of tube ” D=0.1 ZDEM R “ Half length of tube axis ” D=0.1 XMED R “ Center X coordinate ” D=-10000. YMED R “ Center Y coordinate ” D=-10000. ZMED R “ Center Z coordinate ” D=-10000. This command performs a boolean subtraction between the volume CNVV and a tube; the tube has the given parameters and is placed in the MARS according the given coordinates of its center. See also CVOL. The following commands will clip, by a tube, positioned according to the given parameters, the volume specified by NAME (a valid string for the NAME of the volume can be found using the DTREE command). EXAMPLE - dopt hide on satt * seen -2 drawNAME 40 40 0 10 10 .01 .01 next tube * 500 1000 500 0 0 drawNAME 40 40 0 10 10 .01 .01 box . 2.3 CONE cnvv [ rmax1 rmax2 zdem xmed ymed zmed ] CNVV C “ Name of volume to be clipped ” D=’* ’ RMAX1 R “ Min external radius ” D=0.1 RMAX2 R “ Max external radius ” D=0.1 ZDEM R “ Half length of cone axis ” D=0.1 XMED R “ Center X coordinate ” D=-10000. YMED R “ Center Y coordinate ” D=-10000. ZMED R “ Center Z coordinate ” D=-10000. This command performs a boolean subtraction between the volume CNVV and a cone; the cone has the given parameters and is placed in the MARS according to the given coordinates of its center. See also CVOL. The following commands will clip by a cone, positioned according the given parameters, the volume specified by NAME (a valid string for the NAME of the volume can be found using the DTREE command). EXAMPLE - dopt hide on satt * seen -2 drawNAME 40 40 0 10 10 .01 .01 next cone * 1 750 1000 0 0 1000 drawNAME 40 40 0 10 10 .01 .01 box . 2.4 SPHE cnvv [ rmax xmed ymed zmed ] CNVV C “ Name of volume to be clipped ” D=’* ’ RMAX R “ External radius of sphere ” D=0.1 XMED R “ Center X coordinate ” D=-10000. XINT002 – 2 358
YMED R “ Center Y coordinate ” D=-10000. ZMED R “ Center Z coordinate ” D=-10000. This command performs a boolean subtraction between the volume CNVV and a sphere; the sphere has the given parameters and is placed in the MARS according to the given coordinates of its center. See also CVOL. The following commands clip by a sphere, positioned according to the given parameters, the volume specified by NAME (a valid string for the NAME of the volume can be found using the DTREE command). EXAMPLE - dopt hide on satt * seen -2 drawNAME 40 40 0 10 10 .01 .01 next sphe * 500 0 0 500 drawNAME 40 40 0 10 10 .01 .01 box . 2.5 VALCUT xcut ycut zcut XCUT R “x coordinate of cutted value” D=0. YCUT R “y coordinate of cutted value” D=0. ZCUT R “z coordinate of cutted value” D=0. It allows the cutting in the ray-tracing. All the volumes are cutted from XCUT to +BIG along the x axis, from YCUT to +BIG along the y axis and from ZCUT to +BIG along the z axis. 359 XINT002 – 3
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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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∆σ σ = { 12 − 15% for T ≤ 1
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T(MeV) C Pb ∆El 0 ∆E l ∆σ l
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1. sample x from 1 1 ln 1 x c x set
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E bind , eV 10 5 10 20 30 40 50 60
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eV). At present the values recommen
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calculated dE dx − dE measured dx
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Figure 43: Stopping powers in Carbo
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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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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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GPART, 13, 46, 61, 293 GPCXYZ, 40,
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PATCHY, 278 PCUTS, 399 PDIGI, 389 P
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