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ultrarelativistic corrections
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@ -412,6 +412,31 @@ double bethek_lindhard_X(const Projectile &p){
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//return sum;
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}
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double pair_production(const Projectile &p, const Target &t){
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double s=0.0;
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double gamma=1.0 + p.T/atomic_mass_unit;
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double d = 1.0/sqrt(gamma);
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double logd2 = log(d*d);
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double l0 = log(2.0*gamma);
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double Zt13 = 183.0*power(t.Z,-1.0/3.0);
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double L0screen = (19.0/9.0)*log(Zt13/(1.0 + 25.018803808*Zt13/gamma));
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double L1 = (4178.0/(81.0*M_PI*M_PI))
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- (21.0/27.0)
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- (248.0*l0/(27.0*M_PI*M_PI))
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+ ( ((28.0*l0/(9.0)) - 446.0/27.0)*logd2/(M_PI*M_PI))
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+ (14.0*logd2*logd2/(9.0*M_PI*M_PI));
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L1 *= d;
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s = 0.25*dedx_constant*fine_structure*fine_structure*p.Z*p.Z*t.Z*t.Z*gamma*(1.0+(1.0/t.Z))*(L0screen + L1)/t.A;
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return (s<0.0)?0.0:s;
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};
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double bremsstrahlung(const Projectile &p, const Target &t){
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double gamma=1.0 + p.T/atomic_mass_unit;
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double R = 1.18*(catima::power(p.A, 1.0/3.0) + catima::power(t.A, 1.0/3.0));
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double Lbs = log(1.0 + 2.0*gamma*0.1*hbar*c_light/atomic_mass_unit/R/p.A);
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double C = dedx_constant*fine_structure*(electron_mass/atomic_mass_unit);
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return 16.0*C*gamma*p.Z*p.Z*p.Z*p.Z*t.Z*t.Z*Lbs/(t.A*p.A*3.0*4.0*M_PI);
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};
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double sezi_p_se(double energy,const Target &t){
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@ -59,6 +59,16 @@ namespace catima{
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*/
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double bethek_lindhard_X(const Projectile &p);
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/**
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* calculates pair production stopping power
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*/
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double pair_production(const Projectile &p, const Target &t);
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/**
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* calculates bremsstrahlung stopping power
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*/
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double bremsstrahlung(const Projectile &p, const Target &t);
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/**
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* returns linhard correction (L) calulated from tabulated precalculated data
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* if energy is less than minimal calculated energy the LS coefficient of at minimal
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@ -36,6 +36,7 @@ constexpr double fine_structure = 1/137.035999139;
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constexpr double fine_structure_inverted = 1/fine_structure;
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constexpr double c_light = 299.792458; //Mm/s
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constexpr double bohr_velocity = 2.19 / c_light; // in c unit
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constexpr double hbar = 6.582119514; // in eV*s * 10^-16
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constexpr double dedx_constant = 0.3070749187; //4*pi*Na*me*c^2*r_e^2 //MeV cm^2
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constexpr double domega2dx_constant = dedx_constant*electron_mass; //4*pi*Na*me*c^2*r_e^2 //MeV^2 cm^2
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@ -119,6 +119,17 @@ const lest::test specification[] =
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p.T = 2794.4822;
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EXPECT( f()== approx(1.768018).R(0.01) );
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},
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CASE("ultrarelativistic corrections"){
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catima::Projectile p{238,92};
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catima::Target t{27,13};
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EXPECT(catima::pair_production(p(1e3),t) == approx(0.0,1e-3));
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EXPECT(catima::bremsstrahlung(p(1e3),t) == approx(0.0,1e-3));
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EXPECT(catima::pair_production(p(1e6),t) == approx(1900,300));
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EXPECT(catima::bremsstrahlung(p(1e6),t) == approx(170,20));
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EXPECT(catima::pair_production(p(7e6),t) == approx(21000,3000));
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EXPECT(catima::bremsstrahlung(p(7e6),t) == approx(6000,500));
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},
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CASE("dEdx for compounds"){
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catima::Projectile p{1,1,1,1000};
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catima::Material water({
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@ -385,7 +396,12 @@ const lest::test specification[] =
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EXPECT(res3[0] == approx(catima::dedx_from_range(p,energies[0],graphite),0.1));
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EXPECT(res3[1] == approx(catima::dedx_from_range(p,energies[1],graphite),0.1));
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EXPECT(res3[2] == approx(catima::dedx_from_range(p,energies[2],graphite),0.1));
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}
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},
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CASE("constants"){
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using namespace catima;
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EXPECT(0.1*hbar*c_light/atomic_mass_unit == approx(0.21183,0.0001));
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EXPECT(16.0*dedx_constant*electron_mass*fine_structure/(atomic_mass_unit*3.0*4.0*M_PI) == approx(5.21721169334564e-7).R(1e-3));
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}
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};
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