/* * (c) Copyright 2019 CORSIKA Project, corsika-project@lists.kit.edu * * This software is distributed under the terms of the GNU General Public * Licence version 3 (GPL Version 3). See file LICENSE for a full version of * the license. */ #include <corsika/modules/Sibyll.hpp> #include <corsika/modules/sibyll/ParticleConversion.hpp> #include <corsika/framework/core/ParticleProperties.hpp> #include <corsika/framework/core/PhysicalUnits.hpp> #include <corsika/framework/geometry/Point.hpp> #include <corsika/framework/random/RNGManager.hpp> #include <corsika/framework/utility/COMBoost.hpp> #include <catch2/catch.hpp> #include <tuple> /* NOTE, WARNING, ATTENTION The sibyll/Random.hpp implements the hook of sibyll to the C8 random number generator. It has to occur excatly ONCE per linked executable. If you include the header below in multiple "tests" and link them togehter, it will fail. */ #include <corsika/modules/sibyll/Random.hpp> using namespace corsika; using namespace corsika::sibyll; TEST_CASE("Sibyll", "modules") { logging::set_level(logging::level::info); SECTION("Sibyll -> Corsika") { CHECK(Code::Electron == corsika::sibyll::convertFromSibyll(corsika::sibyll::SibyllCode::Electron)); } SECTION("Corsika -> Sibyll") { CHECK(corsika::sibyll::convertToSibyll(Electron::code) == corsika::sibyll::SibyllCode::Electron); CHECK(corsika::sibyll::convertToSibyllRaw(Proton::code) == 13); CHECK(corsika::sibyll::convertToSibyll(XiStarC0::code) == corsika::sibyll::SibyllCode::XiStarC0); } SECTION("canInteractInSibyll") { CHECK(corsika::sibyll::canInteract(Code::Proton)); CHECK(corsika::sibyll::canInteract(Code::XiCPlus)); CHECK_FALSE(corsika::sibyll::canInteract(Code::Electron)); CHECK_FALSE(corsika::sibyll::canInteract(Code::SigmaC0)); CHECK_FALSE(corsika::sibyll::canInteract(Code::Iron)); CHECK_FALSE(corsika::sibyll::canInteract(Code::Helium)); } SECTION("cross-section type") { CHECK(corsika::sibyll::getSibyllXSCode(Code::Proton) == 1); CHECK(corsika::sibyll::getSibyllXSCode(Code::Electron) == 0); CHECK(corsika::sibyll::getSibyllXSCode(Code::K0Long) == 3); CHECK(corsika::sibyll::getSibyllXSCode(Code::SigmaPlus) == 1); CHECK(corsika::sibyll::getSibyllXSCode(Code::PiMinus) == 2); CHECK(corsika::sibyll::getSibyllXSCode(Code::Helium) == 0); } SECTION("sibyll mass") { CHECK_FALSE(corsika::sibyll::getSibyllMass(Code::Electron) == 0_GeV); // Nucleus not a particle CHECK_THROWS(corsika::sibyll::getSibyllMass(Code::Iron)); // Higgs not a particle in Sibyll CHECK_THROWS(corsika::sibyll::getSibyllMass(Code::H0)); } } #include <corsika/framework/geometry/Point.hpp> #include <corsika/framework/geometry/RootCoordinateSystem.hpp> #include <corsika/framework/geometry/Vector.hpp> #include <corsika/framework/core/PhysicalUnits.hpp> #include <corsika/framework/core/ParticleProperties.hpp> #include <SetupTestEnvironment.hpp> #include <SetupTestStack.hpp> #include <corsika/media/Environment.hpp> #include <corsika/media/HomogeneousMedium.hpp> #include <corsika/media/NuclearComposition.hpp> #include <corsika/media/UniformMagneticField.hpp> template <typename TStackView> auto sumMomentum(TStackView const& view, CoordinateSystemPtr const& vCS) { Vector<hepenergy_d> sum{vCS, 0_eV, 0_eV, 0_eV}; for (auto const& p : view) { sum += p.getMomentum(); } return sum; } TEST_CASE("SibyllInterface", "modules") { logging::set_level(logging::level::trace); // the environment and stack should eventually disappear from here auto [env, csPtr, nodePtr] = setup::testing::setup_environment(Code::Oxygen); auto const& cs = *csPtr; { [[maybe_unused]] auto const& env_dummy = env; } auto [stack, viewPtr] = setup::testing::setup_stack( Code::Proton, 10_GeV, (setup::Environment::BaseNodeType* const)nodePtr, cs); setup::StackView& view = *viewPtr; RNGManager<>::getInstance().registerRandomStream("sibyll"); SECTION("InteractionInterface - valid targets") { corsika::sibyll::InteractionModel model; // sibyll only accepts protons or nuclei with 4<=A<=18 as targets CHECK_FALSE(model.isValid(Code::Proton, Code::Electron, 100_GeV)); CHECK(model.isValid(Code::Proton, Code::Hydrogen, 100_GeV)); CHECK_FALSE(model.isValid(Code::Proton, Code::Deuterium, 100_GeV)); CHECK(model.isValid(Code::Proton, Code::Helium, 100_GeV)); CHECK_FALSE(model.isValid(Code::Proton, Code::Helium3, 100_GeV)); CHECK_FALSE(model.isValid(Code::Proton, Code::Iron, 100_GeV)); CHECK(model.isValid(Code::Proton, Code::Oxygen, 100_GeV)); // beam particles CHECK_FALSE(model.isValid(Code::Electron, Code::Oxygen, 100_GeV)); CHECK_FALSE(model.isValid(Code::Iron, Code::Oxygen, 100_GeV)); // energy too low CHECK_FALSE(model.isValid(Code::Proton, Code::Proton, 9_GeV)); CHECK(model.isValid(Code::Proton, Code::Proton, 11_GeV)); // energy too high CHECK_FALSE(model.isValid(Code::Proton, Code::Proton, 1000001_GeV)); CHECK(model.isValid(Code::Proton, Code::Proton, 999999_GeV)); // hydrogen target == proton target == neutron target FourMomentum const aP4(100_GeV, {cs, 99_GeV, 0_GeV, 0_GeV}); FourMomentum const bP4(1_GeV, {cs, 0_GeV, 0_GeV, 0_GeV}); auto const [xs_prod_pp, xs_ela_pp] = model.getCrossSectionInelEla(Code::Proton, Code::Proton, aP4, bP4); auto const [xs_prod_pn, xs_ela_pn] = model.getCrossSectionInelEla(Code::Proton, Code::Neutron, aP4, bP4); auto const [xs_prod_pHydrogen, xs_ela_pHydrogen] = model.getCrossSectionInelEla(Code::Proton, Code::Hydrogen, aP4, bP4); CHECK(xs_prod_pp == xs_prod_pHydrogen); CHECK(xs_prod_pp == xs_prod_pn); CHECK(xs_ela_pp == xs_ela_pHydrogen); CHECK(xs_ela_pn == xs_ela_pHydrogen); // invalids auto const xs_prod_0 = model.getCrossSection(Code::Electron, Code::Proton, aP4, bP4); CHECK(xs_prod_0 / 1_mb == Approx(0)); CHECK_THROWS(model.doInteraction(view, Code::Electron, Code::Proton, aP4, bP4)); CHECK_THROWS(convertFromSibyll(corsika::sibyll::SibyllCode::Unknown)); } SECTION("InteractionInterface - low energy") { const HEPEnergyType P0 = 60_GeV; MomentumVector const plab = MomentumVector(cs, {P0, 0_eV, 0_eV}); // also print particles after sibyll was called corsika::sibyll::InteractionModel model; model.setVerbose(true); HEPEnergyType const Elab = sqrt(static_pow<2>(P0) + static_pow<2>(Proton::mass)); FourMomentum const projectileP4(Elab, plab); FourMomentum const nucleusP4(Oxygen::mass, MomentumVector(cs, {0_eV, 0_eV, 0_eV})); view.clear(); model.doInteraction(view, Code::Proton, Code::Oxygen, projectileP4, nucleusP4); auto const pSum = sumMomentum(view, cs); /* Interactions between hadrons (h) and nuclei (A) in Sibyll are treated in the hadron-nucleon center-of-mass frame (hnCoM). The incoming hadron (h) and nucleon (N) are assumed massless, such that the energy and momentum in the hnCoM are : E_i_cm = 0.5 * SQS and P_i_cm = +- 0.5 * SQS where i is either the projectile hadron or the target nucleon and SQS is the hadron-nucleon center-of-mass energy. The true energies and momenta, accounting for the hadron masses, are: E_i = ( S + m_i**2 - m_j**2 ) / (2 * SQS) and Pcm = +- sqrt( (S-(m_j+m_i)**2) * (s-(m_j-m_i)**2) ) / (2*SQS) where m_i is the projectiles mass and m_j is the target particles mass. In terms of lab. frame variables Pcm = m_j * Plab_i / SQS, where Plab_i is the momentum of the projectile (i) in the lab. and m_j is the mass of the target, i.e. the particle at rest (usually a nucleon). Any hadron-nucleus event can contain several nucleon interactions. In case of Nw (number of wounded nucleons) nucleons interacting in the hadron-nucleus interaction, the total energy and momentum in the hadron(i)-nucleon(N) center-of-mass frame are: momentum: p_projectile + p_nucleon_1 + p_nucleon_2 + .... p_nucleon_Nw = -(Nw-1) * Pcm with center-of-mass momentum Pcm = p_projectile = - p_nucleon_i. For the energy: E_projectile + E_nucleon_1 + ... E_nucleon_Nw = E_projectile + Nw * E_nucleon. Using the above definitions of center-of-mass energies and momenta this leads to the total energy: E_tot = SQS/2 * (1+Nw) + (m_N**2-m_i**2)/(2*SQS) * (Nw-1) and P_tot = -m_N * Plab_i / SQS * (Nw-1). A Lorentztransformation of these quantities to the lab. frame recovers Plab_i for the total momentum, so momentum is exactly conserved, and Elab_i + Nw * m_N for the total energy. Not surprisingly the total energy differs from the total energy before the collision by the mass of the additional nucleons (Nw-1)*m_N. In relative terms the additional energy is entirely negligible and as it is not kinetic energy there is zero influence on the shower development. Due to the ommission of the hadron masses in Sibyll, the total energy and momentum in the center-of-mass system after the collision are just: E_tot = SQS/2 * (1+Nw) and P_tot = SQS/2 * (1-Nw). After the Lorentztransformation the total momentum in the lab. thus differs from the initial value by (1-Nw)/2 * ( m_N + m_i**2 / (2 * Plab_i) ) and momentum is NOT conserved. Note however that the second term quickly vanishes as the lab. momentum of the projectile increases. The first term is fixed as it depends only on the number of additional nucleons, in relative terms it is always small at high energies. For this reason the numerical precision in these tests is limited to 5% to still pass at low energies and no absolute check is implemented, e.g. CHECK(pSum.getComponents(cs).getX() / P0 == Approx(1).margin(0.05)); CHECK((pSum - plab).norm()/1_GeV == Approx(0).margin(plab.norm() * 0.05/1_GeV)); /FR'2020 See also: Issue 272 / MR 204 https://gitlab.iap.kit.edu/AirShowerPhysics/corsika/-/merge_requests/204 */ CHECK(pSum.getComponents(cs).getX() / P0 == Approx(1).margin(0.05)); CHECK(pSum.getComponents(cs).getY() / 1_GeV == Approx(0).margin(1e-3)); CHECK(pSum.getComponents(cs).getZ() / 1_GeV == Approx(0).margin(1e-3)); CHECK((pSum - plab).getNorm() / 1_GeV == Approx(0).margin(plab.getNorm() * 0.05 / 1_GeV)); CHECK(pSum.getNorm() / P0 == Approx(1).margin(0.05)); [[maybe_unused]] CrossSectionType const cx = model.getCrossSection(Code::Proton, Code::Oxygen, projectileP4, nucleusP4); CHECK(cx / 1_mb == Approx(300).margin(1)); // CHECK(view.getEntries() == 9); //! \todo: this was 20 before refactory-2020: check // "also sibyll not stable wrt. to compiler // changes" } SECTION("NuclearInteractionInterface") { HEPMomentumType const P0 = 50_TeV; MomentumVector const plab = MomentumVector(cs, {P0, 0_eV, 0_eV}); corsika::sibyll::InteractionModel hmodel; NuclearInteractionModel model(hmodel, *env); CHECK(model.isValid(Code::Helium, Code::Oxygen, 100_GeV)); CHECK_FALSE(model.isValid(Code::PiPlus, Code::Oxygen, 100_GeV)); CHECK_FALSE(model.isValid(Code::Electron, Code::Oxygen, 100_GeV)); Code const pid = Code::Oxygen; HEPEnergyType const Elab = sqrt(static_pow<2>(P0) + static_pow<2>(get_mass(pid))); FourMomentum const P4(Elab, plab); FourMomentum const targetP4(get_mass(Code::Oxygen), MomentumVector(cs, {0_eV, 0_eV, 0_eV})); model.doInteraction(view, pid, Code::Oxygen, P4, targetP4); CrossSectionType const cx = model.getCrossSection(pid, Code::Oxygen, P4, targetP4); CHECK(cx / 1_mb == Approx(1250).margin(100)); // this is not physics validation CHECK(view.getSize() == Approx(150).margin(140)); // this is not physics validation // invalid to underlying model FourMomentum P4mu( 100_GeV, {cs, {sqrt(static_pow<2>(100_GeV) - static_pow<2>(MuPlus::mass)), 0_eV, 0_eV}}); CrossSectionType const cx0 = model.getCrossSection(Code::MuPlus, Code::Oxygen, P4mu, targetP4); CHECK(cx0 / 1_mb == Approx(0)); CHECK_THROWS(model.doInteraction(view, Code::MuPlus, Code::Oxygen, P4mu, targetP4)); } } #include <corsika/framework/geometry/Point.hpp> #include <corsika/framework/geometry/RootCoordinateSystem.hpp> #include <corsika/framework/geometry/Vector.hpp> #include <corsika/framework/core/PhysicalUnits.hpp> #include <corsika/framework/core/ParticleProperties.hpp> #include <SetupTestEnvironment.hpp> #include <SetupTestStack.hpp> #include <corsika/media/Environment.hpp> #include <corsika/media/HomogeneousMedium.hpp> #include <corsika/media/NuclearComposition.hpp> #include <corsika/media/UniformMagneticField.hpp> TEST_CASE("SibyllDecayInterface", "modules") { logging::set_level(logging::level::info); auto [env, csPtr, nodePtr] = setup::testing::setup_environment(Code::Oxygen); auto const& cs = *csPtr; { [[maybe_unused]] auto const& env_dummy = env; } RNGManager<>::getInstance().registerRandomStream("sibyll"); SECTION("DecayInterface") { auto [stackPtr, viewPtr] = setup::testing::setup_stack( Code::Lambda0, 10_GeV, (setup::Environment::BaseNodeType* const)nodePtr, cs); setup::StackView& view = *viewPtr; auto& stack = *stackPtr; auto particle = stack.first(); Decay model; model.printDecayConfig(); [[maybe_unused]] TimeType const time = model.getLifetime(particle); auto const gamma = particle.getEnergy() / particle.getMass(); CHECK(time == get_lifetime(Code::Lambda0) * gamma); model.doDecay(view); // run checks // lambda decays into proton and pi- or neutron and pi+ CHECK(stack.getEntries() == 3); } SECTION("DecayInterface - decay not handled") { // sibyll does not know the higgs for example auto [stackPtr, viewPtr] = setup::testing::setup_stack( Code::H0, 10_GeV, (setup::Environment::BaseNodeType* const)nodePtr, cs); setup::StackView& view = *viewPtr; auto& stack = *stackPtr; auto particle = stack.first(); Decay model; CHECK(model.getLifetime(particle) == std::numeric_limits<double>::infinity() * 1_s); CHECK_THROWS(model.doDecay(view)); } SECTION("DecayConfiguration") { Decay model({Code::PiPlus, Code::PiMinus}); model.printDecayConfig(); CHECK(model.isDecayHandled(Code::PiPlus)); CHECK(model.isDecayHandled(Code::PiMinus)); CHECK_FALSE(model.isDecayHandled(Code::KPlus)); std::vector<Code> const particleTestList = {Code::PiPlus, Code::PiMinus, Code::KPlus, Code::Lambda0Bar, Code::D0Bar}; // setup decays model.setHandleDecay(particleTestList); for (auto& pCode : particleTestList) CHECK(model.isDecayHandled(pCode)); // set decay individually model.setHandleDecay(Code::KMinus); // fail CHECK_THROWS(model.setHandleDecay(Code::H0)); // possible decays CHECK_FALSE(model.canHandleDecay(Code::H0)); CHECK_FALSE(model.canHandleDecay(Code::Proton)); CHECK_FALSE(model.canHandleDecay(Code::Electron)); CHECK(model.canHandleDecay(Code::PiPlus)); CHECK(model.canHandleDecay(Code::MuPlus)); } }