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// Multiple Coulomb scattering Monte Carlo for electron in pure elements
// based on mcsda.f
// F. Salvat, J.D. Martinez, R. Mayol, J. Parellada
// COMP. PHYS. COMMUN. 42 (1986) 93
// AALC
// C++ by Daniel Pitzl, DESY, Sep 2019
// ELASTIC SCATTERING EVENTS ARE DESCRIBED BY USING AN ANALYTICAL FIT
// TO THE RELATIVISTIC MOTT CROSS-SECTION.
// THE MEAN RATE OF ENERGY LOSS PER UNIT PATH LENGTH IS DERIVED FROM
// THE RELATIVISTIC BETHE STOPPING POWER, I.E. FROM THE CONTINUOUS SLOWING
// DOWN APPROXIMATION (CSDA).
// THE STRAGGLING EFFECT IS SIMULATED BY MEANS OF THE LENZ INELASTIC (TOTAL)
// CROSS-SECTION AND THE CLASSICAL 1/W**2 DISTRIBUTION OF ENERGY LOSSES.
// ANGULAR DEFLECTIONS OF THE ELECTRON PATH DUE TO INELASTIC COLLISIONS ARE
// COMPUTED FROM THE CLASSICAL THEORY OF BINARY COLLISIONS.
// REFERENCES:
// (1) F. SALVAT ET AL., J. PHYS. D: APPL. PHYS. 17 (1984) 185
// (2) F. SALVAT ET AL., J. PHYS. D: APPL. PHYS. 17 (1984) 1545
// (3) R. MAYOL ET AL., ANALES DE FISICA A80 (1984) 130
// (4) M.J. BERGER AND S.M. SELTZER, NBSIR 82-2550-A (1982)
//
// ***** ATOMIC DATA
//
// FREE ATOMS
// --------------------------------------------------------------
// ATOM Z AW A ALPHA1 ALPHA2 I
// --------------------------------------------------------------
// He 2 4.0026 1.00000 2.20564 2.20564 41.8 (GAS)
// Li 3 6.941 0.60453 2.81743 0.66246 40.0
// Be 4 9.01218 0.32784 4.54284 0.98509 63.7
// B 5 10.81 0.23268 5.99011 1.21345 76.0
// C 6 12.011 0.15364 8.04166 1.49140 78.0
// N 7 14.0067 0.09957 10.8127 1.76869 82.0 (GAS)
// O 8 15.9994 0.06245 14.8346 2.04052 95.0 (GAS)
// F 9 18.9984 0.03678 21.4093 2.30606 115 (GAS)
// Ne 10 20.179 0.01801 35.0596 2.56643 137 (GAS)
// Na 11 22.98977 0.74440 4.12051 0.87184 149
// Mg 12 24.305 0.64234 4.72661 1.00249 156
// Al 13 26.98154 0.60013 5.14064 1.01539 166
// Si 14 28.0855 0.51591 5.84957 1.17330 173
// P 15 30.97376 0.43866 6.67081 1.34106 173
// S 16 32.06 0.37130 7.60432 1.50676 180
// Cl 17 35.453 0.31314 8.67077 1.66877 174 (GAS)
// Ar 18 39.948 0.26299 9.90260 1.82787 188 (GAS)
// K 19 39.0983 0.62732 5.87615 0.98798 190
// Ca 20 40.08 0.58800 6.32192 1.00940 191
// Sc 21 44.9559 0.55431 6.63300 1.10236 216
// Ti 22 47.88 0.53593 6.89381 1.18766 233
// V 23 50.9415 0.52216 7.11955 1.26815 245
// Cr 24 51.996 0.50646 7.31623 1.42531 257
// Mn 25 54.9380 0.50356 7.49501 1.41970 272
// Fe 26 55.847 0.49731 7.65419 1.49227 286
// Co 27 58.9332 0.49262 7.79761 1.56304 297
// Ni 28 58.69 0.48921 7.92752 1.63224 311
// Cu 29 63.546 0.46600 8.20246 1.82639 322
// Zn 30 65.38 0.48531 8.15505 1.76715 330
// Ga 31 69.72 0.57810 7.45294 1.47922 334
// Ge 32 72.59 0.55193 7.81505 1.52669 350
// As 33 74.9216 0.51813 8.27460 1.60648 347
// Se 34 78.96 0.48352 8.78654 1.69690 348
// Br 35 79.904 0.45033 9.33526 1.79016 357
// Kr 36 83.80 0.41895 9.91986 1.88404 352 (GAS)
// Rb 37 85.4678 0.66732 7.38694 1.13156 363
// Sr 38 87.62 0.65417 7.60914 1.10652 366
// Y 39 88.9059 0.62196 7.98456 1.19369 379
// Zr 40 91.22 0.59406 8.34255 1.27785 393
// Nb 41 92.9064 0.55591 8.81359 1.43082 417
// Mo 42 95.94 0.53108 9.19190 1.51654 424
// Tc 43 97.907 0.52988 9.33183 1.50495 428
// Ru 44 101.07 0.48905 9.92161 1.67634 441
// Rh 45 102.9055 0.47090 10.2776 1.75229 449
// Pd 46 106.42 0.36860 12.2194 2.09718 470
// Ag 47 107.868 0.43878 10.9799 1.18991 470
// Cd 48 112.41 0.45464 10.8499 1.84361 469
// In 49 114.82 0.52418 9.95823 1.62066 488
// Sn 50 118.69 0.51613 10.1882 1.62396 488
// Sb 51 121.75 0.50244 10.5023 1.64840 487
// Te 52 127.60 0.48399 10.9022 1.69203 485
// I 53 126.9045 0.46451 11.3435 1.74292 491
// Xe 54 131.29 0.44503 11.8150 1.79736 482 (GAS)
// Cs 55 132.9054 0.63099 9.27951 1.21804 488
// Ba 56 137.33 0.63153 9.37847 1.16983 491
// La 57 138.9055 0.60457 9.78322 1.23954 501
// Ce 58 140.12 0.60176 9.89662 1.26964 523
// Pr 59 140.9077 0.59961 10.0029 1.29867 535
// Nd 60 144.24 0.61818 9.84443 1.29305 546
// Pm 61 144.913 0.61655 9.94325 1.32107 560
// Sm 62 150.36 0.61524 10.0389 1.34861 574
// Eu 63 151.96 0.61408 10.0134 1.37597 580
// Gd 64 157.25 0.59470 10.4721 1.43349 591
// Tb 65 158.9254 0.61231 10.3185 1.42998 614
// Dy 66 162.5 0.61163 10.4097 1.45675 628
// Ho 67 164.9304 0.61105 10.5006 1.48342 650
// Er 68 167.26 0.61054 10.5913 1.51003 658
// Tm 69 168.9342 0.61006 10.6828 1.53672 674
// Yb 70 173.04 0.60962 10.7746 1.56339 684
// Lu 71 174.967 0.59607 11.0553 1.60432 694
// Hf 72 178.49 0.57730 11.4181 1.66925 705
// Ta 73 180.9479 0.55928 11.7897 1.73462 718
// W 74 183.85 0.54238 12.1611 1.79841 727
// Re 75 186.207 0.52646 12.5334 1.85940 736
// Os 76 190.2 0.51112 12.9161 1.92009 746
// Ir 77 192.22 0.49632 13.3110 1.98039 757
// Pt 78 195.08 0.46317 14.0902 2.12491 790
// Au 79 196.9665 0.44855 14.5490 2.18774 790
// Hg 80 200.59 0.45535 14.5388 2.15774 800
// Tl 81 204.383 0.51102 13.5079 1.94984 810
// Pb 82 207.2 0.51405 13.5898 1.92284 823
// Bi 83 208.9804 0.52372 13.5429 1.87088 823
// Po 84 208.982 0.51902 13.7725 1.87223 830
// At 85 209.987 0.50987 14.0959 1.89216 825
// Rn 86 222.018 0.49903 14.4661 1.92060 794 (GAS)
// Fr 87 223.020 0.63069 12.2398 1.42884 827
// Ra 88 226.0254 0.63838 12.2521 1.36251 826
// Ac 89 227.0278 0.50967 14.1001 1.89316 841
// Th 90 232.0381 0.60184 13.0792 1.46078 847
// Pa 91 231.0359 0.60180 13.1874 1.48806 878
// U 92 238.0289 0.59396 13.4427 1.52547 890
//
//
// WIGNER-SEITZ ATOMS
// ----------------------------------------------
// ATOM Z RWS A ALPHA1 ALPHA2
// ----------------------------------------------
// Li 3 3.25 0.37731 3.19082 1.28284
// Na 11 3.94 0.49868 5.08096 1.51901
// Al 13 2.99 0.31543 7.28752 1.77451
// Si 14 3.18 0.31186 7.76730 1.71824
// P 15 3.57 0.31007 8.17973 1.67147
// K 19 4.87 0.42851 7.49488 1.42250
// Ca 20 4.11 0.40255 8.05513 1.42620
// V 23 2.81 0.22974 12.2348 1.96899
// Cr 24 2.68 0.19633 13.6659 2.14626
// Mn 25 2.70 0.21946 12.9263 2.10354
// Fe 26 2.67 0.21948 13.0520 2.16581
// Ni 28 2.60 0.21892 13.2947 2.30276
// Cu 29 2.65 0.21374 13.4817 2.42997
// Ge 32 3.34 0.35634 10.2486 2.09847
// Rb 37 5.21 0.53376 8.61480 1.52016
// Sr 38 4.48 0.52902 8.81678 1.48175
// Nb 41 3.07 0.37795 11.4676 1.93243
// Mo 42 2.93 0.35710 12.0620 1.99956
// Rh 45 2.81 0.32521 13.2919 2.13494
// Pd 46 2.87 0.31116 13.8007 2.21950
// Ag 47 3.02 0.32982 13.4086 2.17450
// Cs 55 5.64 0.52081 10.6875 1.54308
// Ba 56 4.72 0.51198 10.9485 1.53695
// Ce 58 3.87 0.45633 12.1097 1.72503
// Eu 63 4.26 0.47914 12.1247 1.81620
// Yb 70 4.05 0.47457 12.8767 2.03486
// Ta 73 3.08 0.41974 14.4589 2.22411
// W 74 2.94 0.40817 14.8914 2.26673
// Ir 77 2.84 0.39894 15.5877 2.30243
// Pt 78 2.90 0.39375 15.8661 2.33737
// Au 79 2.98 0.39511 15.9768 2.34208
// Pb 82 3.65 0.42298 15.6563 2.24990
// Th 90 3.76 0.49879 15.0981 1.84375
// Z ................... ATOMIC NUMBER
// AW .................. ATOMIC WEIGHT
// A, ALPHA1,ALPHA2 .... DENSITY PARAMETERS DERIVED FROM SELF-CONSISTENT
// DHFS CALCULATIONS (REFERENCE 3)
// I ................... MEAN EXCITATION POTENTIAL FOR SINGLE-ELEMENT
// MATERIALS (EV) RECOMMENDED IN REFERENCE 4
// RWS ................. RADIUS OF THE WIGNER-SEITZ SPHERE (A.U.)
// ***** NUMERICAL AND PHYSICAL CONSTANTS IN THE SOURCE LISTING
// PI = 3.1415926535897931D+00
// 36/PI = 1.1459155902616464D+01
// 2*PI = 6.2831853071795862D+00
// 2**31-1 = 2.1474836470000000D+09
// 1/(2**31-1) = 4.6566128752457969D-10
// 2*PI/(2**31-1) = 2.9258361598967678D-09
// (2*E**3)**1/2 = 6.3380654656113586D+00 E=DEXP(1.)
// 2*(2/E)**3/4 = 1.5888453635426958D+00
// 2/3*(E/2)**3/4 = 8.3918382740555711D-01
// RADIAN (RAD) = 5.7295779513082323D+01 DEG
// RAD/2 = 2.8647889756541161D+01
// LOG(2) = 6.9314718055994533D-01
// atomic units: hbar = m = e = 1
// AVOGADRO'S NUMBER (AVOG) = 6.022094D23MOL**-1
// SPEED OF LIGHT (SL) = 137.036 ATOMIC UNITS
// BOHR RADIUS (a0b) = 5.291771D-9 CM
// HARTREE ENERGY (HRKEV) = 2.721160D-2 KEV
#include <iostream> // cout
#include <cmath> // sqrt, sin, cos, log
#include <random>
#include <ctime>
using namespace std;
//------------------------------------------------------------------------------
void DIRECT( double CDT, double DF, double & u, double & v, double & w )
{
// update DIRECTION COSINES AFTER A DEFLECTION DT, DF IN THE
// PARTICLE REFERENCE SYSTEM.
// INPUT:
// U, V, W ..... INITIAL DIRECTION COSINES
// CDT ....... COSINE OF THE POLAR SCATTERING ANGLE
// DF ........ AZIMUTHAL SCATTERING ANGLE ( RAD )
// OUTPUT:
// U, V, W ..... NEW DIRECTION COSINES
// (CDT AND DF REMAIN UNCHANGED)
double din[3];
double sdt = sqrt( 1 - CDT*CDT );
din[0] = sdt*cos(DF);
din[1] = sdt*sin(DF);
din[2] = CDT;
double cz = w; // old direction
double sz = sqrt( 1.0 - cz*cz );
double f = atan2( v, u );
double sf = sin(f);
double cf = cos(f);
u = cz*cf * din[0] - sf * din[1] + sz*cf * din[2];
v = cz*sf * din[0] + cf * din[1] + sz*sf * din[2];
w =-sz * din[0] + cz * din[2];
} // direct
//------------------------------------------------------------------------------
int main()
{
// tracks:
int ntotal = 10*1000;
cout << " NUMBER OF TRAJECTORIES DESIRED .. " << ntotal << endl;
// THICKNESS:
double dz = 0.0100; // [cm]
cout << " THICKNESS ....................... " << dz*10 << " mm" << endl;
// incident energy:
double e0mev = 1000;
cout << " INITIAL ELECTRON ENERGY ( E0 ) .. " << e0mev << " MeV" << endl;
// ABSORPTION ENERGY:
double eabs = 10; // keV
cout << " LOWER ELECTRON ENERGY ( EABS ) .. " << eabs << " keV" << endl;
// ELEMENT DATA:
double Z = 13; // Al
double A = 26.984; // g/mol
double rho = 2.702; // g/cm3
cout << endl
<< " ATOMIC NUMBER " << Z << endl
<< " ATOMIC WEIGHT " << A << endl
<< " DENSITY " << rho << " g/cm3" << endl;
// SCREENING PARAMETERS:
double AA = 0.31543;
double AL1 = 7.28752;
double AL2 = 1.77451;
cout << " SCREENING CONSTANTS:" << endl
<< " A = " << A << endl
<< " alpha1 = " << AL1 << endl
<< " alpha2 = " << AL2 << endl;
// - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
// physical constants:
double AVOG = 6.022094e23; // [atoms/Mol]
double a0b = 5.291771e-9; // Bohr radius [cm]
double HRKEV = 2.721160e-2; // Hartree aomic units
// POWERS OF THE SPEED OF LIGHT in atomic units:
double SL2 = 1.877887e4; // c^2
double SL22 = 3.755773e4; // 2c^2
double SL22I = 2.662568e-5; // 1/2c^2
double pi = 4*atan(1);
double twopi = 2*pi;
// CROSS-SECTION PARAMETERS:
double ZT = twopi * Z;
double Z4 = 2*twopi * Z;
double ZZ4 = Z*Z4;
double A1A = 1 - AA;
double AA1 = AA*AA;
double AL12 = AL1*AL1;
double AL22 = AL2*AL2;
double AA2 = A1A*A1A;
double AA3 = 2*AA*A1A/( AL12-AL22 );
double AA4 = log( AL22/AL12 );
double AB2 = 2*AA/AL12 - AA3;
double AB3 = 2*A1A/AL22 + AA3;
// MEAN EXCITATION POTENTIAL ( SEMIEMPIRICAL FORMULA )
double expot = 1.35e-2 * Z;
if( Z > 11.5 )
expot = Z * ( 9.76e-3 + 5.88e-2 / pow( Z, 1.19 ) );
cout << " MEAN EXCITATION POTENTIAL ....... " << expot << " keV" << endl;
expot = expot/HRKEV;
expot = 1/expot;
double expot2 = expot*expot;
// FIRST IONIZATION ENERGY:
double fie = 6; // eV
cout << " FIRST IONIZATION ENERGY " << fie << " eV" << endl;
fie = fie*1e-3 / HRKEV; // Hartree
double AB1 = 0.125*fie*fie;
// NUMBER OF 'MOLECULES' PER UNIT VOLUME
double VMOL = AVOG*rho/A * pow( a0b, 3 ); // a0b = Bohr
double e0kev = e0mev*1e3;
double E0 = e0kev/HRKEV; // atomic units
eabs = eabs/HRKEV;
// Moliere angles:
double chic2 = 0.157 * Z*(Z+1) * dz*rho / A / e0mev / e0mev;
double chia2 = 2.007e-5 * pow( Z, 2.0/3.0 ) * ( 1 + 3.34*Z/137*Z/137 ) / e0mev / e0mev;
cout << endl;
cout << " Moliere chic " << sqrt(chic2) << endl;
cout << " Moliere chia " << sqrt(chia2) << endl;
cout << " Moliere ratio " << chic2/chia2 << endl;
// Lynch-Dahl rms scattering:
double f = 0.98; // central fraction
double xnu = 0.5*chic2/chia2/(1-f);
double vartet = chic2/(1+f*f) * ( (1+xnu)/xnu*log(1+xnu) - 1 );
double rmstet = sqrt(vartet) * sqrt(2); // 2-D
cout << " Lynch-Dahl RMS scattering " << rmstet*1e3 << " mrad in 2D" << endl;
cout << endl;
dz = dz / a0b; // atomic units
// INITIAL DIRECTION:
double c0 = 1; // forward
double s0 = sqrt(1-c0*c0);
ranlux24 rgen;
rgen.seed( time(NULL) ); // seconds since 1.1.1970
uniform_real_distribution <double> unirnd( 0, 1 );
int N[3];
N[0] = 0;
N[1] = 0;
N[2] = 0;
double EM = 0;
double VEM = 0;
double vang = 0;
double vtet = 0;
int ntet = 0;
double disp = 0;
double vdisp = 0;
unsigned long mscat = 0;
unsigned long vmscat = 0;
unsigned long mloss = 0;
unsigned long vmloss = 0;
int ntot = 0;
while( ntot < ntotal ) { // tracks
ntot += 1;
double x = 0;
double y = 0;
double z = 0;
double TL = 0; // track length
unsigned long nscat = 0;
unsigned long nloss = 0;
double W = c0; // direction cosines
double phi = twopi*unirnd(rgen);
double U = s0*cos(phi);
double V = s0*sin(phi);
double E = E0; // atomic units
bool newE = 1;
double EMFP = dz;
double XMFP = dz;
double TMFP = dz;
double AFP = dz;
double WM = fie;
int iexit = 0;
double EINV = 1/E;
double RB = E + SL22; // E+2mc2
double QFACT = E;
double QME = E;
double SE0 = 0;
double SE1 = 0;
double SE2 = 0;
double SET = 0;
while(1) { // steps
// energy changed, update:
if( newE ) {
EINV = 1/E;
double FA = E + SL2; // E+mc2
RB = E + SL22; // E+2mc2
double BETA = E*RB/( FA*FA );
double SFACT = BETA*SL2;
double QMI = ( E+E )*RB*SL22I;
QFACT = QMI + QMI;
QME = QFACT + QFACT;
// cout << " E " << E*HRKEV << endl;
// ELASTIC CROSS-SECTION ( MOTT'S FORMULA )
FA = AL12 + QME;
double FB = AL22 + QME;
SE0 = log( FB/FA ) - AA4;
SE1 = AA1 * ( QME / ( AL12*FA ) );
SE2 = AA2 * ( QME / ( AL22*FB ) );
SET = SE1 + SE2 + AA3*SE0;
EMFP = ZZ4 * SET;
// INELASTIC CROSS-SECTION ( LENZ'S FORMULA )
// F. Lenz, Z. Naturf. 3A 1954 78
double Q02 = AB1*EINV;
FA = AL12 + Q02;
FB = AL22 + Q02;
double FT = AL12 + QMI;
double FNT = AL22 + QMI;
XMFP = Z4 * (
AB2*log( QMI*FA/( FT*Q02 ) ) +
AB3*log( QMI*FB/( FNT*Q02 ) ) +
AA1*( 1/FT-1/FA ) +
AA2*( 1/FNT-1/FB ) );
TMFP = EMFP + XMFP;
AFP = SFACT / ( VMOL*TMFP ); // atomic units
// cout << " path " << EMFP << ", " << XMFP << ", " << AFP << ", " << AFP*a0b*1e4 << endl;
// AVERAGE ENERGY LOSS PER INELASTIC COLLISION:
double WA = fie;
double CSI = E*expot;
if( CSI < 6.338065465611359 )
WA = ZT*EINV * 3.1776907270853916 * sqrt( CSI ) / XMFP;
else {
FA = 1 - BETA;
FB = sqrt( FA );
FT = 1 - FB;
WA = 2*ZT*EINV * ( log( E*expot2*SFACT/FA ) -
( FB+FB+BETA ) * 6.931471805599453e-1 +
FA + 0.125*FT*FT ) / XMFP;
}
// cout << " csi " << csi << ", wavg " << WA << endl;
// MINIMUM ENERGY LOSS. HALLEY'S METHOD:
WM = pow( WA, 1 + 3.3 / ( 3.3 - log( WA ) ) );
FT = log( WM );
// cout << " wm " << WM << ", ft " << FT << endl;
double W0 = WA*( 1-WM ) + WM*FT;
double W1 = 1 - WA + FT;
WM = WM - 2*W0*W1 / ( 2*W1*W1 - W0/WM );
FT = log( WM );
// cout << " wm " << WM << ", ft " << FT << endl;
W0 = WA*( 1 - WM ) + WM*FT;
W1 = 1 - WA + FT;
WM = WM - 2*W0*W1 / ( 2*W1*W1 - W0/WM );
// cout << " wmin " << WM << endl;
newE = 0;
} // newE
double rnd = unirnd(rgen); // uniform 0..1
double s = -log( 1-rnd )*AFP;
TL = TL + s;
x = x + U*s;
y = y + V*s;
z = z + W*s;
// cout << " z " << z*a0b*1d4; // [um]
// ----------------------------------------------------- TEST BOUNDS
if( z > dz ) {
iexit = 0;
break;
}
else if( z < 0 ) {
iexit = 1;
break;
}
// --------------------------------------------------- NEW COLLISION
rnd = unirnd(rgen);
if( rnd*TMFP < XMFP ) { // INELASTIC COLLISION
double ft = unirnd(rgen);
double DE = 0.5 * E*WM / ( 1 - ft * ( 1-WM ) );
nloss += 1;
E = E-DE;
if( E <= eabs ) {
iexit = 2;
break;
}
newE = 1;
// SCATTERING ANGLES
double CDT = sqrt( ( 1 - DE*EINV ) * RB / ( RB-DE ) );
double DF = twopi*unirnd(rgen);
DIRECT( CDT, DF, U, V, W );
// cout << " inelastic ", cdt, de
} // inelastic
else { // ELASTIC COLLISION
double rnd = unirnd(rgen);
double FB = rnd*SET;
double FNT = SE1;
double fa = unirnd(rgen);
double CDT = 1;
if( FNT > FB )
CDT = fa * AL12 * QME / ( AL12 + ( 1-fa )*QME );
else {
FNT += SE2;
if( FNT > FB )
CDT = fa * AL22 * QME / ( AL22 + ( 1-fa )*QME );
else {
double FT = exp( fa*SE0 + AA4 );
CDT = ( AL12*FT - AL22 ) / ( 1 - FT );
}
}
CDT = 1 - CDT / QFACT;
double DF = twopi*unirnd(rgen);
DIRECT( CDT, DF, U, V, W );
nscat += 1;
// cout << " elastic ", cdt
}
} // do steps
// ---------------------------------------------- INCREMENT COUNTERS
N[iexit] += 1;
if( iexit == 0 ) { // transmitted
EM += E; // exit energy [atomic]
VEM += E*E;
double fa = acos( W ); // exit angle, 0..pi
vang += fa*fa;
if( fa < 3*rmstet ) {
vtet += fa*fa;
ntet += 1;
}
double dd = sqrt( x*x + y*y )*a0b*1e4; // displacement [um]
disp += dd;
vdisp += dd*dd;
if( ntot < 100 || ntot%100 == 0 )
cout << ntot << ": scat " << nscat << ", loss " << nloss
<< ", angle " << fa*1e3 << " mrad, offset " << dd << " um"
<< endl;
mscat += nscat;
vmscat += nscat*nscat;
mloss += nloss;
vmloss += nloss*nloss;
} // exit
} // tracks
cout << endl;
cout << "energy " << e0mev << " MeV" << endl;
cout << "thickness " << dz*a0b*1e4 << " um" << endl;
cout << endl;
cout << "tracks " << ntot << endl;
cout << "transmitted " << N[0] << endl;
cout << "backscattered " << N[1] << endl;
cout << "absorbed " << N[2] << endl;
if( N[0] > 0 ) {
cout << endl << "transmitted:" << endl;
double n0 = 1.0 / N[0];
double uscat = n0 * sqrt( vmscat - n0 * mscat*mscat );
cout << " elastics " << n0*mscat << " +- " << uscat << endl;
double uloss = n0 * sqrt( vmloss - n0 * mloss*mloss );
cout << "inelastics " << n0*mloss << " +- " << uloss << endl;
double uem = n0*HRKEV * sqrt( VEM - n0 * EM*EM );
EM = n0*EM*HRKEV;
cout << endl << "energy " << EM*1e-3 << " +- " << uem*1e-3 << " MeV"
<< endl << "loss " << e0kev-EM << " +- " << uem << " keV"
<< endl;
vang = sqrt( vang * n0 ); // rms scat ang
cout << endl << "RMS angle " << vang*1e3 << " mrad" << endl;
if( ntet )
cout << "limited " << sqrt( vtet / ntet )*1E3 << " mrad" << endl;
double udisp = n0 * sqrt( vdisp - n0 * disp*disp );
cout << endl << "displacement " << n0*disp << " +- " << udisp << " um" << endl;
} // trans
cout << endl;
} // main