file src/IndirectDetectionYields.cpp
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Namespaces
| Name |
|---|
| Gambit TODO: see if we can use this one: |
| Gambit::DarkBit |
Detailed Description
Author:
- Christoph Weniger (c.weniger@uva.nl)
- Sebastian Wild (sebastian.wild@ph.tum.de)
- Sanjay Bloor (sanjay.bloor12@imperial.ac.uk)
- Pat Scott (pat.scott@uq.edu.au)
- Patrick Stoecker (stoecker@physik.rwth-aachen.de)
Date:
- 2013 Jul - 2015 May
- 2016 Aug
- 2018 Aug
- 2020 Nov, Dec
- 2021 Mar
Routines for the calculation of particle yields from dark matter annihilation / decay.
Authors (add name and date if you modify):
Source code
// GAMBIT: Global and Modular BSM Inference Tool
// *********************************************
/// \file
///
/// Routines for the calculation of particle yields
/// from dark matter annihilation / decay.
///
/// *********************************************
///
/// Authors (add name and date if you modify):
///
/// \author Christoph Weniger
/// (c.weniger@uva.nl)
/// \date 2013 Jul - 2015 May
///
/// \author Sebastian Wild
/// (sebastian.wild@ph.tum.de)
/// \date 2016 Aug
///
/// \author Sanjay Bloor
/// (sanjay.bloor12@imperial.ac.uk)
/// \date 2018 Aug
///
/// \author Pat Scott
/// (pat.scott@uq.edu.au)
/// \date 2020 Nov, Dec
///
/// \author Patrick Stoecker
/// (stoecker@physik.rwth-aachen.de)
/// \date 2021 Mar
///
/// *********************************************
#include "gambit/Elements/gambit_module_headers.hpp"
#include "gambit/DarkBit/DarkBit_rollcall.hpp"
#include "gambit/Utils/ascii_table_reader.hpp"
#include "gambit/DarkBit/DarkBit_utils.hpp"
//#define DARKBIT_DEBUG
namespace Gambit
{
namespace DarkBit
{
/*! \brief Boosts an energy spectrum of isotropic particles into another
* frame (and isotropizes again).
* Parameters:
* gamma: Lorentz boost factor
* dNdE: Spectrum
* mass: mass of particle
*/
daFunk::Funk boost_dNdE(daFunk::Funk dNdE, double gamma, double mass)
{
if ( gamma < 1.0 + .02 ) // Ignore less than 2% boosts
{
if (gamma < 1.0)
DarkBit_error().raise(LOCAL_INFO,
"boost_dNdE: Requested Lorentz boost with gamma < 1");
return dNdE;
}
double betaGamma = sqrt(gamma*gamma-1);
daFunk::Funk E = daFunk::var("E");
daFunk::Funk lnE = daFunk::var("lnE");
daFunk::Funk Ep = daFunk::var("Ep");
daFunk::Funk halfBox_int = betaGamma*sqrt(E*E-mass*mass);
daFunk::Funk halfBox_bound = betaGamma*sqrt(Ep*Ep-mass*mass);
daFunk::Funk integrand = dNdE/(2*halfBox_int);
return integrand->gsl_integration("E", Ep*gamma-halfBox_bound, Ep*gamma+halfBox_bound)
->set_epsabs(0)->set_limit(100)->set_epsrel(1e-3)->set_use_log_fallback(true)->set("Ep", daFunk::var("E"));
//
// Note: integration over lnE causes problems in the WIMP example (3) as the singularity is dropped.
// return (integrand*E)->set("E", exp(lnE))->gsl_integration("lnE", log(Ep*gamma-halfBox_bound), log(Ep*gamma+halfBox_bound))
// ->set_epsabs(0)->set_epsrel(1e-3)->set("Ep", daFunk::var("E"));
}
/*! \brief Helper function returning yield from
* a given DM process.
*/
daFunk::Funk getYield(const str& yield, const bool is_annihilation, const str& DMid, const str& DMbarid,
TH_ProcessCatalog catalog, SimYieldTable table, double line_width, stringFunkMap cascadeMC_spectra)
{
using DarkBit_utils::gamma3bdy_limits;
// Make sure that the ProcessCatalog process matches the is_annihilation flag.
const TH_Process* p = (is_annihilation ? catalog.find(DMid, DMbarid) : catalog.find(DMid));
if (p == NULL) DarkBit_error().raise(LOCAL_INFO, "Process does not match type indicated by is_annihilation flag.");
// Get particle mass from process catalog
const double mass = catalog.getParticleProperty(DMid).mass;
const double Ecm(is_annihilation ? 2*mass : mass);
// Get annihilation or decay process from process catalog and set up yield vector
TH_Process process(is_annihilation ? catalog.getProcess(DMid, DMbarid) : catalog.getProcess(DMid));
daFunk::Funk Yield(is_annihilation ? daFunk::zero("E", "v") : daFunk::zero("E"));
// Adding two-body channels
for (std::vector<TH_Channel>::iterator it = process.channelList.begin();
it != process.channelList.end(); ++it)
{
bool added = false; // If spectrum is not available from any source
// Here only take care of two-body final states
if (it->nFinalStates != 2) continue;
// Get final state masses
double m0 = catalog.getParticleProperty(it->finalStateIDs[0]).mass;
double m1 = catalog.getParticleProperty(it->finalStateIDs[1]).mass;
// Ignore channels that are kinematically closed for v=0
if ( m0 + m1 > Ecm ) continue;
// Ignore channels with 0 BR in v=0 limit (if "v" is a variable of genRate, i.e. not a decay).
if (it->genRate->hasArg("v") && it->genRate->bind("v")->eval(0.) <= 0.0) continue;
else if ( !(it->genRate->hasArgs()) && it->genRate->bind()->eval() <=0.0) continue;
double E0 = 0.5*(Ecm*Ecm+m0*m0-m1*m1)/Ecm;
double E1 = Ecm-E0;
// Check whether two-body hard process final state is in SimYield table
if ( table.hasChannel(it->finalStateIDs[0], it->finalStateIDs[1], yield) )
{
Yield = Yield +
it->genRate*(table)(
it->finalStateIDs[0], it->finalStateIDs[1], yield, Ecm);
added = true;
}
// Deal with composite final states
else
{
daFunk::Funk spec0 = daFunk::zero("E");
daFunk::Funk spec1 = daFunk::zero("E");
added = true;
// Final state particle one
// Tabulated spectrum available?
if ( table.hasChannel(it->finalStateIDs[0], yield) )
{
spec0 = (table)(it->finalStateIDs[0], yield)->set("Ecm",E0);
}
// Monochromatic line?
else if ( it->finalStateIDs[0] == yield )
{
daFunk::Funk E = daFunk::var("E");
spec0 = daFunk::delta("E",E0,E0*line_width);
}
// MC spectra available?
else if ( cascadeMC_spectra.count(it->finalStateIDs[0]) )
{
double gamma0 = E0/m0;
//std::cout << it->finalStateIDs[0] << " " << gamma0 << std::endl;
spec0 = boost_dNdE(cascadeMC_spectra.at(it->finalStateIDs[0]), gamma0, 0.0);
}
else added = false;
// Final state particle two
if ( table.hasChannel(it->finalStateIDs[1], yield) )
{
spec1 = (table)(it->finalStateIDs[1], yield)->set("Ecm", E1);
}
else if ( it->finalStateIDs[1] == yield )
{
daFunk::Funk E = daFunk::var("E");
spec1 = daFunk::delta("E",E1,E1*line_width);
}
else if ( cascadeMC_spectra.count(it->finalStateIDs[1]) )
{
double gamma1 = E1/m1;
//std::cout << it->finalStateIDs[1] << " " << gamma1 << std::endl;
spec1 = boost_dNdE(cascadeMC_spectra.at(it->finalStateIDs[1]), gamma1, 0.0);
}
else added = false;
#ifdef DARKBIT_DEBUG
std::cout << it->finalStateIDs[0] << " " << it->finalStateIDs[1] << std::endl;
//std::cout << "gammas: " << gamma0 << ", " << gamma1 << std::endl;
daFunk::Funk chnSpec = (daFunk::zero("v", "E")
+ spec0
+ spec1)-> set("v", 0.);
auto x = daFunk::logspace(0, 3, 10);
std::vector<double> y = chnSpec->bind("E")->vect(x);
std::cout << it->finalStateIDs[0] << it->finalStateIDs[1] << ":\n";
std::cout << " E: [";
for (std::vector<double>::iterator it2 = x.begin(); it2 != x.end(); it2++)
std::cout << *it2 << ", ";
std::cout << "]\n";
std::cout << " dNdE: [";
for (std::vector<double>::iterator it2 = y.begin(); it2 != y.end(); it2++)
std::cout << *it2 << ", ";
std::cout << "]\n";
#endif
if (!added)
{
DarkBit_warning().raise(LOCAL_INFO, "DarkBit::getYield (with yield = " + yield + ") cannot "
"find spectra for " + it->finalStateIDs[0] + " " + it->finalStateIDs[1]);
}
Yield = Yield + (spec0 + spec1) * it->genRate;
}
} // End adding two-body final states
// Adding three-body final states
//
// NOTE: Three body processes are added even if they are closed at v=0
for (std::vector<TH_Channel>::iterator it = process.channelList.begin();
it != process.channelList.end(); ++it)
{
bool added = true;
// Here only take care of three-body final states
if (it->nFinalStates != 3) continue;
/*
// Implement tabulated three-body final states
// Keep this for future use
if ( it->nFinalStates == 3
and table->hasChannel(it->finalStateIDs[0], yield)
and table->hasChannel(it->finalStateIDs[1], yield)
and table->hasChannel(it->finalStateIDs[2], yield) )
{
daFunk::Funk dNdE1dE2 = it->genRate->set("v",0.);
daFunk::Funk spec0 = (table)(it->finalStateIDs[0], yield);
daFunk::Funk spec1 = (table)(it->finalStateIDs[1], yield);
daFunk::Funk spec2 = (table)(it->finalStateIDs[2], yield);
Yield = Yield + convspec(spec0, spec1, spec2, dNdE1dE2);
}
*/
if ( it->finalStateIDs[0] == yield )
{
if ( it->finalStateIDs[1] == yield or it->finalStateIDs[2] == yield)
{
DarkBit_warning().raise(LOCAL_INFO, "Second and/or third primary "+yield+" in three-body final states ignored.");
}
double m1 = catalog.getParticleProperty(it->finalStateIDs[1]).mass;
double m2 = catalog.getParticleProperty(it->finalStateIDs[2]).mass;
daFunk::Funk E1_low = daFunk::func(gamma3bdy_limits<0>, daFunk::var("E"),
mass, m1, m2);
daFunk::Funk E1_high = daFunk::func(gamma3bdy_limits<1>, daFunk::var("E"),
mass, m1, m2);
daFunk::Funk dsigmavde = it->genRate->gsl_integration(
"E1", E1_low, E1_high);
Yield = Yield + dsigmavde;
}
else added = false;
if (!added)
{
DarkBit_warning().raise(LOCAL_INFO,
"DarkBit::getYield ignoring final state "
+ it->finalStateIDs[0] + " " + it->finalStateIDs[1] + " " + it->finalStateIDs[2]);
}
}
// Rescale the yield by the correct kinematic factor
if (is_annihilation)
{
// If process involves non-self-conjugate DM then we need to add a factor of 1/2
// to the final spectrum. This must be explicitly set in the process catalog.
double k = (process.isSelfConj) ? 1. : 0.5;
Yield = k*daFunk::ifelse(1e-6 - daFunk::var("v"), Yield/(mass*mass),
daFunk::throwError("Spectrum currently only defined for v=0."));
}
else
{
Yield = Yield/mass;
}
return Yield;
}
/// \brief General routine to derive gamma-ray annihilation yield.
/// This function returns
/// k*dN/dE*(sv)/mDM**2 (E, v) [cm^3/s/GeV^3]
/// the energy spectrum of photons times sigma*v/m^2, as function of energy (in GeV)
/// and velocity (as a fraction of c), multiplied by k=1 for self-conjugate DM or k=1/2
/// for non-self conjugate. By default, only the v=0 component is calculated.
void GA_AnnYield_General(daFunk::Funk &result)
{
using namespace Pipes::GA_AnnYield_General;
std::string DMid= *Dep::DarkMatter_ID;
std::string DMbarid = *Dep::DarkMatterConj_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("gamma", true, DMid, DMbarid, *Dep::TH_ProcessCatalog, *Dep::GA_SimYieldTable,
line_width, *Dep::cascadeMC_gammaSpectra);
}
/// \brief General routine to derive gamma-ray decay yield.
/// This function returns
/// dN/dE*(Gamma)/mDM (E) [1/s/GeV^2]
/// the energy spectrum of photons times Gamma/m, as function of energy (in GeV).
void GA_DecayYield_General(daFunk::Funk &result)
{
using namespace Pipes::GA_DecayYield_General;
std::string DMid = *Dep::DarkMatter_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("gamma", false, DMid, "null", *Dep::TH_ProcessCatalog, *Dep::GA_SimYieldTable,
line_width, *Dep::cascadeMC_gammaSpectra);
}
/// \brief General routine to derive electron annihilation yield.
/// This function returns
/// k*dN/dE*(sv)/mDM**2 (E, v) [cm^3/s/GeV^3]
/// the energy spectrum of electrons times sigma*v/m^2, as function of energy (in GeV)
/// and velocity (as a fraction of c), multiplied by k=1 for self-conjugate DM or k=1/2
/// for non-self conjugate. By default, only the v=0 component is calculated.
void electron_AnnYield_General(daFunk::Funk &result)
{
using namespace Pipes::electron_AnnYield_General;
std::string DMid= *Dep::DarkMatter_ID;
std::string DMbarid = *Dep::DarkMatterConj_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("e-_1", true, DMid, DMbarid, *Dep::TH_ProcessCatalog, *Dep::electron_SimYieldTable,
line_width, *Dep::cascadeMC_electronSpectra);
}
/// \brief General routine to derive electron decay yield.
/// This function returns
/// dN/dE*(Gamma)/mDM (E) [1/s/GeV^2]
/// the energy spectrum of electrons times Gamma/m, as function of energy (in GeV).
void electron_DecayYield_General(daFunk::Funk &result)
{
using namespace Pipes::electron_DecayYield_General;
std::string DMid = *Dep::DarkMatter_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("e-_1", false, DMid, "null", *Dep::TH_ProcessCatalog, *Dep::electron_SimYieldTable,
line_width, *Dep::cascadeMC_electronSpectra);
}
/// \brief General routine to derive positron annihilation yield.
/// This function returns
/// k*dN/dE*(sv)/mDM**2 (E, v) [cm^3/s/GeV^3]
/// the energy spectrum of positrons times sigma*v/m^2, as function of energy (in GeV)
/// and velocity (as a fraction of c), multiplied by k=1 for self-conjugate DM or k=1/2
/// for non-self conjugate. By default, only the v=0 component is calculated.
void positron_AnnYield_General(daFunk::Funk &result)
{
using namespace Pipes::positron_AnnYield_General;
std::string DMid= *Dep::DarkMatter_ID;
std::string DMbarid = *Dep::DarkMatterConj_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("e+_1", true, DMid, DMbarid, *Dep::TH_ProcessCatalog, *Dep::positron_SimYieldTable,
line_width, *Dep::cascadeMC_positronSpectra);
}
/// \brief General routine to derive positron decay yield.
/// This function returns
/// dN/dE*(Gamma)/mDM (E) [1/s/GeV^2]
/// the energy spectrum of positrons times Gamma/m, as function of energy (in GeV).
void positron_DecayYield_General(daFunk::Funk &result)
{
using namespace Pipes::positron_DecayYield_General;
std::string DMid = *Dep::DarkMatter_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("e+_1", false, DMid, "null", *Dep::TH_ProcessCatalog, *Dep::positron_SimYieldTable,
line_width, *Dep::cascadeMC_positronSpectra);
}
/// \brief General routine to derive antiproton annihilation yield.
/// This function returns
/// k*dN/dE*(sv)/mDM**2 (E, v) [cm^3/s/GeV^3]
/// the energy spectrum of antiprotons times sigma*v/m^2, as function of energy (in GeV)
/// and velocity (as a fraction of c), multiplied by k=1 for self-conjugate DM or k=1/2
/// for non-self conjugate. By default, only the v=0 component is calculated.
void antiproton_AnnYield_General(daFunk::Funk &result)
{
using namespace Pipes::antiproton_AnnYield_General;
std::string DMid= *Dep::DarkMatter_ID;
std::string DMbarid = *Dep::DarkMatterConj_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("pbar", true, DMid, DMbarid, *Dep::TH_ProcessCatalog, *Dep::antiproton_SimYieldTable,
line_width, *Dep::cascadeMC_antiprotonSpectra);
}
/// \brief General routine to derive antiproton decay yield.
/// This function returns
/// dN/dE*(Gamma)/mDM (E) [1/s/GeV^2]
/// the energy spectrum of antiprotons times Gamma/m, as function of energy (in GeV).
void antiproton_DecayYield_General(daFunk::Funk &result)
{
using namespace Pipes::antiproton_DecayYield_General;
std::string DMid = *Dep::DarkMatter_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("pbar", false, DMid, "null", *Dep::TH_ProcessCatalog, *Dep::antiproton_SimYieldTable,
line_width, *Dep::cascadeMC_antiprotonSpectra);
}
/// \brief General routine to derive antideuteron annihilation yield.
/// This function returns
/// k*dN/dE*(sv)/mDM**2 (E, v) [cm^3/s/GeV^3]
/// the energy spectrum of antideuterons times sigma*v/m^2, as function of energy (in GeV)
/// and velocity (as a fraction of c), multiplied by k=1 for self-conjugate DM or k=1/2
/// for non-self conjugate. By default, only the v=0 component is calculated.
void antideuteron_AnnYield_General(daFunk::Funk &result)
{
using namespace Pipes::antideuteron_AnnYield_General;
std::string DMid= *Dep::DarkMatter_ID;
std::string DMbarid = *Dep::DarkMatterConj_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("Dbar", true, DMid, DMbarid, *Dep::TH_ProcessCatalog, *Dep::antideuteron_SimYieldTable,
line_width, *Dep::cascadeMC_antideuteronSpectra);
}
/// \brief General routine to derive antideuteron decay yield.
/// This function returns
/// dN/dE*(Gamma)/mDM (E) [1/s/GeV^2]
/// the energy spectrum of antideuterons times Gamma/m, as function of energy (in GeV).
void antideuteron_DecayYield_General(daFunk::Funk &result)
{
using namespace Pipes::antideuteron_DecayYield_General;
std::string DMid = *Dep::DarkMatter_ID;
/// Option line_width<double>: Set relative line width used in gamma-ray spectra (default 0.03)
const double line_width = runOptions->getValueOrDef<double>(0.03, "line_width");
result = getYield("Dbar", false, DMid, "null", *Dep::TH_ProcessCatalog, *Dep::antideuteron_SimYieldTable,
line_width, *Dep::cascadeMC_antideuteronSpectra);
}
// SimYields =======================================================
/// Combined SimYieldTable containing final yields of all stable particles
void Combine_SimYields(SimYieldTable& result)
{
using namespace Pipes::Combine_SimYields;
static bool initialized = false;
if ( not initialized )
{
if (Downstream::neededFor("cascadeMC_gammaSpectra")) Dep::GA_SimYieldTable->donateChannels(result);
if (Downstream::neededFor("cascadeMC_electronSpectra")) Dep::positron_SimYieldTable->donateChannels(result);
if (Downstream::neededFor("cascadeMC_positronSpectra")) Dep::electron_SimYieldTable->donateChannels(result);
if (Downstream::neededFor("cascadeMC_antiprotonSpectra")) Dep::antiproton_SimYieldTable->donateChannels(result);
if (Downstream::neededFor("cascadeMC_antideuteronSpectra")) Dep::antideuteron_SimYieldTable->donateChannels(result);
initialized = true;
}
}
/// Gamma-ray SimYieldTable based on DarkSUSY5 tabulated results. (DS6 below)
void GA_SimYieldTable_DS5(SimYieldTable& result)
{
using namespace Pipes::GA_SimYieldTable_DS5;
static bool initialized = false;
if ( not initialized )
{
int flag = 0; // some flag
int yieldk = 152; // gamma ray yield
using DarkBit_utils::str_flav_to_mass;
double mDM_min, mDM_max;
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
if ( allow_yield_extrapolation )
{
mDM_min = 0.0; // in this case, the minimally allowed dark matter mass will later be set to be the mass of the final state particle,
// with an additional factor 0.99 for the case of Z, W or t final states (following DarkSUSY)
mDM_max = 1.0e6;
}
else
{
mDM_min = 10.0; // minimal dark matter mass simulated in DarkSUSY.
mDM_max = 5000.; // maximal dark matter mass simulated in DarkSUSY.
}
auto add_channel = [&](int ch, str P1, str P2, str FINAL, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("mwimp"),
daFunk::var("Ekin"), ch, yieldk, flag)->set("mwimp", daFunk::var("Ecm")/2);
result.addChannel(dNdE, str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions);
};
// The following routine adds an annihilation channel, for which the yields are extrapolated below Ecm_ToScale
// using the approximation that x*dN/dx is a constant function of the dark matter mass.
auto add_channel_with_scaling = [&](int ch, str P1, str P2, str FINAL, double EcmMin, double EcmMax, double Ecm_ToScale)
{
daFunk::Funk Ecm_ToUse = fmax(Ecm_ToScale, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor = Ecm_ToUse/daFunk::var("Ecm");
daFunk::Funk dNdE = ScalingFactor * daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("mwimp"),
ScalingFactor * daFunk::var("Ekin"), ch, yieldk, flag)->set("mwimp", Ecm_ToUse/2);
result.addChannel(dNdE, str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions);
};
// Specifies also center of mass energy range
add_channel(12, "Z0", "Z0", "gamma", 2*90.288, 2*mDM_max);
add_channel(13, "W+", "W-", "gamma", 2*79.4475, 2*mDM_max);
add_channel(14, "nu_e", "nubar_e", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(15, "e+", "e-", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(16, "nu_mu", "nubar_mu", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(17, "mu+", "mu-", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel(18, "nu_tau", "nubar_tau", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(19, "tau+", "tau-", "gamma", 2*std::max(mDM_min, 1.7841), 2*mDM_max);
//add_channel(20, "u", "ubar", "gamma", 0., 2*mDM_max); // Zero
add_channel(22, "u", "ubar", "gamma", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
//add_channel(21, "d", "dbar", "gamma", 0., 2*mDM_max); // Zero
add_channel(22, "d", "dbar", "gamma", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
add_channel(22, "c", "cbar", "gamma", 2*std::max(mDM_min, 1.35), 2*mDM_max);
//add_channel(23, "s", "sbar", "gamma", 0., 2*mDM_max); // Zero
add_channel(22, "s", "sbar", "gamma", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
add_channel_with_scaling(24, "t", "tbar", "gamma", 2*160.0, 2*mDM_max, 2*173.3);
add_channel(25, "b", "bbar", "gamma", 2*std::max(mDM_min, 5.0), 2*mDM_max);
add_channel(26, "g", "g", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max);
// Add approximations for single-particle cases.
// TODO: Replace by boosted rest frame spectrum Z0
daFunk::Funk dNdE;
dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("Ecm"), daFunk::var("Ekin"), 12, yieldk, flag);
result.addChannel(dNdE/2, "Z0", "gamma", 90.288, mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("Ecm"), daFunk::var("Ekin"), 13, yieldk, flag);
result.addChannel(dNdE/2, "W+", "gamma", 79.4475, mDM_max, runOptions);
result.addChannel(dNdE/2, "W-", "gamma", 79.4475, mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("Ecm"), daFunk::var("Ekin"), 15, yieldk, flag);
result.addChannel(dNdE/2, str_flav_to_mass("e+"), "gamma", std::max(mDM_min, 0.0), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("e-"), "gamma", std::max(mDM_min, 0.0), mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("Ecm"), daFunk::var("Ekin"), 17, yieldk, flag);
result.addChannel(dNdE/2, str_flav_to_mass("mu+"), "gamma", std::max(mDM_min, 0.0), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("mu-"), "gamma", std::max(mDM_min, 0.0), mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("Ecm"), daFunk::var("Ekin"), 19, yieldk, flag);
result.addChannel(dNdE/2, str_flav_to_mass("tau+"), "gamma", std::max(mDM_min, 1.7841), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tau-"), "gamma", std::max(mDM_min, 1.7841), mDM_max, runOptions);
double Ecm_ToScale_top = 173.3;
daFunk::Funk Ecm_ToUse_top = fmax(Ecm_ToScale_top, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor_top = Ecm_ToUse_top/daFunk::var("Ecm");
dNdE = ScalingFactor_top * daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), Ecm_ToUse_top,
ScalingFactor_top * daFunk::var("Ekin"), 24, yieldk, flag);
result.addChannel(dNdE/2, str_flav_to_mass("t"), "gamma", 160.0, mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tbar"), "gamma", 160.0, mDM_max, runOptions);
// add channels with "mixed final states", i.e. final state particles with (potentially) different masses
daFunk::Funk Ecm = daFunk::var("Ecm");
auto add_channel_mixedmasses = [&](int ch1, int ch2, str P1, str P2, str FINAL, double m1, double m2, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE_1 = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("E1"),
daFunk::var("Ekin"), ch1, yieldk, flag)->set("E1", Ecm/2 + (m1*m1 - m2*m2)/(2*Ecm));
daFunk::Funk dNdE_2 = daFunk::func_fromThreadsafe(BEreq::dshayield.pointer(), daFunk::var("E2"),
daFunk::var("Ekin"), ch2, yieldk, flag)->set("E2", Ecm/2 + (m2*m2 - m1*m1)/(2*Ecm));
result.addChannel(0.5*(dNdE_1 + dNdE_2), str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions);
};
// - In the following: approximate spectra from u,d,s (20,21,23) by spectrum from c (22).
// - The numerical values for EcmMin and EcmMax are obtained from applying the corresponding two-body kinematics
// to the minimally/maximally allowed center-of-mass energies. Hence, EcmMin depends on the flag allow_yield_extrapolation.
// If it is false, the assigmnents of Ecm_min assume the value mDM_min = 10.0.
add_channel_mixedmasses(22, 22, "u", "dbar", "gamma", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(22, 22, "d", "ubar", "gamma", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(22, 22, "u", "sbar", "gamma", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(22, 22, "s", "ubar", "gamma", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(22, 25, "u", "bbar", "gamma", 0.0, 5.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses(25, 22, "b", "ubar", "gamma", 5.0, 0.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses(22, 22, "c", "dbar", "gamma", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(22, 22, "d", "cbar", "gamma", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(22, 22, "c", "sbar", "gamma", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(22, 22, "s", "cbar", "gamma", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(22, 25, "c", "bbar", "gamma", 1.35, 5.0, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses(25, 22, "b", "cbar", "gamma", 5.0, 1.35, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses(24, 22, "t", "dbar", "gamma", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(22, 24, "d", "tbar", "gamma", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(24, 22, "t", "sbar", "gamma", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(22, 24, "s", "tbar", "gamma", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(24, 25, "t", "bbar", "gamma", 175.0, 5.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
add_channel_mixedmasses(25, 24, "b", "tbar", "gamma", 5.0, 175.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
initialized = true;
}
}
/// Construct a SimYieldTable based on DarkSUSY6 tabulated results.
SimYieldTable SimYieldTable_DarkSUSY(const str& yield, const bool allow_yield_extrapolation, double(*dsanyield)(double&,double&,int&,char*,int&,int&,int&), safe_ptr<Options> runOptions)
{
using DarkBit_utils::str_flav_to_mass;
const int flag = 0; // some flag
const int diff=1; // differential yields (=1)
char*hel = (char *)"0"; // helicity
int yieldpdg; // PDG code of final state
double mDM_min, mDM_max; // Boundaries of tabulation
SimYieldTable result; // The table itself
// Determine PDG code of the particle for which the yield has been requested
if (yield == "gamma")
yieldpdg = 22;
else if (yield == "e+_1")
yieldpdg = -11;
else if (yield == "pbar")
yieldpdg = -2212;
else if (yield == "Dbar")
yieldpdg = -1000010020;
else if (yield == "pi0")
yieldpdg = 111;
else if (yield == "nu_e + nu_ebar")
yieldpdg = 12;
else if (yield == "nu_mu + nu_mubar")
yieldpdg = 14;
else if (yield == "nu_tau + nu_taubar")
yieldpdg = 16;
else
DarkBit_error().raise(LOCAL_INFO, "SimYieldTable_DarkSUSY called with unrecognised final state " + yield);
if ( allow_yield_extrapolation )
{
mDM_min = 0.0; // in this case, the minimally allowed dark matter mass will later be set to be the mass of the final state particle,
// with an additional factor 0.99 for the case of Z, W or t final states (following DarkSUSY)
mDM_max = 1.0e6;
}
else
{
mDM_min = 3.0; // minimal dark matter mass simulated in DarkSUSY6.
mDM_max = 20000.; // maximal dark matter mass simulated in DarkSUSY6.
}
auto add_channel = [&](int pdg, str p1, str p2, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("mwimp"),
daFunk::var("Ekin"), pdg, hel, yieldpdg, diff, flag)->set("mwimp", daFunk::var("Ecm")/2);
result.addChannel(dNdE, str_flav_to_mass(p1), str_flav_to_mass(p2), yield, EcmMin, EcmMax, runOptions);
};
// The following routine adds an annihilation/decay channel, for which the yields are extrapolated below Ecm_ToScale
// using the approximation that x*dN/dx is a constant function of the dark matter mass.
auto add_channel_with_scaling = [&](int pdg, str P1, str P2, double EcmMin, double EcmMax, double Ecm_ToScale)
{
daFunk::Funk Ecm_ToUse = fmax(Ecm_ToScale, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor = Ecm_ToUse/daFunk::var("Ecm");
daFunk::Funk dNdE = ScalingFactor * daFunk::func_fromThreadsafe(dsanyield, daFunk::var("mwimp"),
ScalingFactor * daFunk::var("Ekin"), pdg, hel, yieldpdg, diff, flag)->set("mwimp", Ecm_ToUse/2);
result.addChannel(dNdE, str_flav_to_mass(P1), str_flav_to_mass(P2), yield, EcmMin, EcmMax, runOptions);
};
// specifies also center of mass energy range
add_channel(23, "Z0", "Z0", 2*90.288, 2*mDM_max);
add_channel(24, "W+", "W-", 2*79.4475, 2*mDM_max);
add_channel(12, "nu_e", "nubar_e", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(11, "e+", "e-", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(14, "nu_mu", "nubar_mu", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(13, "mu+", "mu-", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel(16, "nu_tau", "nubar_tau", 2*std::max(mDM_min, 0.0), 2*mDM_max); // Zero
add_channel(15, "tau+", "tau-", 2*std::max(mDM_min, 1.7841), 2*mDM_max);
//add_channel(2, "u", "ubar", 0., 2*mDM_max); // Zero
add_channel(2, "u", "ubar", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
//add_channel(1, "d", "dbar", 0., 2*mDM_max); // Zero
add_channel(1, "d", "dbar", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
add_channel(4, "c", "cbar", 2*std::max(mDM_min, 1.35), 2*mDM_max);
//add_channel(3, "s", "sbar", 0., 2*mDM_max); // Zero
add_channel(3, "s", "sbar", 2*std::max(mDM_min, 1.35), 2*mDM_max); // approx by cc
add_channel_with_scaling(6, "t", "tbar", 2*160.0, 2*mDM_max, 2*173.3);
add_channel(5, "b", "bbar", 2*std::max(mDM_min, 5.0), 2*mDM_max);
add_channel(21, "g", "g", 2*std::max(mDM_min, 0.0), 2*mDM_max);
// Add approximations for single-particle cases.
// TODO: Replace by boosted rest frame spectrum Z0
daFunk::Funk dNdE;
dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("Ecm"), daFunk::var("Ekin"), 23, hel,yieldpdg, diff,flag);
result.addChannel(dNdE/2, "Z0", yield, 90.288, mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("Ecm"), daFunk::var("Ekin"), 24, hel,yieldpdg, diff, flag);
result.addChannel(dNdE/2, "W+", yield, 79.4475, mDM_max, runOptions);
result.addChannel(dNdE/2, "W-", yield, 79.4475, mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("Ecm"), daFunk::var("Ekin"), 11, hel, yieldpdg, diff, flag);
result.addChannel(dNdE/2, str_flav_to_mass("e+"), yield, std::max(mDM_min, 0.0), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("e-"), yield, std::max(mDM_min, 0.0), mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("Ecm"), daFunk::var("Ekin"), 13, hel, yieldpdg, diff, flag);
result.addChannel(dNdE/2, str_flav_to_mass("mu+"), yield, std::max(mDM_min, 0.0), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("mu-"), yield, std::max(mDM_min, 0.0), mDM_max, runOptions);
dNdE = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("Ecm"), daFunk::var("Ekin"), 15, hel, yieldpdg, diff, flag);
result.addChannel(dNdE/2, str_flav_to_mass("tau+"), yield, std::max(mDM_min, 1.7841), mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tau-"), yield, std::max(mDM_min, 1.7841), mDM_max, runOptions);
double Ecm_ToScale_top = 173.3;
daFunk::Funk Ecm_ToUse_top = fmax(Ecm_ToScale_top, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor_top = Ecm_ToUse_top/daFunk::var("Ecm");
dNdE = ScalingFactor_top * daFunk::func_fromThreadsafe(dsanyield, Ecm_ToUse_top,
ScalingFactor_top * daFunk::var("Ekin"), 6, hel, yieldpdg, diff, flag);
result.addChannel(dNdE/2, str_flav_to_mass("t"), yield, 160.0, mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tbar"), yield, 160.0, mDM_max, runOptions);
// Add channels with "mixed final states", i.e. final state particles with (potentially) different masses
daFunk::Funk Ecm = daFunk::var("Ecm");
auto add_channel_mixedmasses = [&](int pdg1, int pdg2, str P1, str P2, double m1, double m2, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE_1 = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("E1"),
daFunk::var("Ekin"), pdg1, hel, yieldpdg, diff, flag)->set("E1", Ecm/2 + (m1*m1 - m2*m2)/(2*Ecm));
daFunk::Funk dNdE_2 = daFunk::func_fromThreadsafe(dsanyield, daFunk::var("E2"),
daFunk::var("Ekin"), pdg2, hel, yieldpdg, diff, flag)->set("E2", Ecm/2 + (m2*m2 - m1*m1)/(2*Ecm));
result.addChannel(0.5*(dNdE_1 + dNdE_2), str_flav_to_mass(P1), str_flav_to_mass(P2), yield, EcmMin, EcmMax, runOptions);
};
// - The numerical values for EcmMin and EcmMax are obtained from applying the corresponding two-body kinematics
// to the minimally/maximally allowed center-of-mass energies. Hence, EcmMin depends on the flag allow_yield_extrapolation.
add_channel_mixedmasses(2, -1, "u", "dbar", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(1, -2, "d", "ubar", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(2, -3, "u", "sbar", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(3, -2, "s", "ubar", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 20.0), 2*mDM_max);
add_channel_mixedmasses(2, -5, "u", "bbar", 0.0, 5.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses(5, -2, "b", "ubar", 5.0, 0.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses(4, -1, "c", "dbar", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(1, -4, "d", "cbar", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(4, -3, "c", "sbar", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(3, -4, "s", "cbar", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses(4, -5, "c", "bbar", 1.35, 5.0, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses(5, -4, "b", "cbar", 5.0, 1.35, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses(6, -1, "t", "dbar", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(1, -6, "d", "tbar", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(6, -3, "t", "sbar", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(3, -6, "s", "tbar", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses(6, -5, "t", "bbar", 175.0, 5.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
add_channel_mixedmasses(5, -6, "b", "tbar", 5.0, 175.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
return result;
}
/// Gamma-ray SimYieldTable based on DarkSUSY6 tabulated results.
void GA_SimYieldTable_DarkSUSY(SimYieldTable& result)
{
using namespace Pipes::GA_SimYieldTable_DarkSUSY;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
result = SimYieldTable_DarkSUSY("gamma", allow_yield_extrapolation, BEreq::dsanyield_sim.pointer(), runOptions);
initialized = true;
}
}
/// Positron SimYieldTable based on DarkSUSY6 tabulated results.
void positron_SimYieldTable_DarkSUSY(SimYieldTable& result)
{
using namespace Pipes::positron_SimYieldTable_DarkSUSY;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
result = SimYieldTable_DarkSUSY("e+_1", allow_yield_extrapolation, BEreq::dsanyield_sim.pointer(), runOptions);
initialized = true;
}
}
/// Anti-proton SimYieldTable based on DarkSUSY6 tabulated results.
void antiproton_SimYieldTable_DarkSUSY(SimYieldTable& result)
{
using namespace Pipes::antiproton_SimYieldTable_DarkSUSY;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
result = SimYieldTable_DarkSUSY("pbar", allow_yield_extrapolation, BEreq::dsanyield_sim.pointer(), runOptions);
initialized = true;
}
}
/// Anti-deuteron SimYieldTable based on DarkSUSY6 tabulated results.
void antideuteron_SimYieldTable_DarkSUSY(SimYieldTable& result)
{
using namespace Pipes::antideuteron_SimYieldTable_DarkSUSY;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
result = SimYieldTable_DarkSUSY("Dbar", allow_yield_extrapolation, BEreq::dsanyield_sim.pointer(), runOptions);
initialized = true;
}
}
/// Gamma-ray SimYieldTable based on MicrOmegas tabulated results.
void GA_SimYieldTable_MicrOmegas(SimYieldTable& result)
{
using namespace Pipes::GA_SimYieldTable_MicrOmegas;
using DarkBit_utils::str_flav_to_mass;
static bool initialized = false;
const int outN = 0; // gamma
if ( not initialized )
{
double mDM_max;
if ( runOptions->getValueOrDef(false, "allow_yield_extrapolation") )
{
mDM_max = 1.0e6;
}
else
{
mDM_max = 5000.; // maximal dark matter mass simulated in micromegas.
}
auto add_channel = [&](int inP, str P1, str P2, str FINAL, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE = daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("Ecm"), daFunk::var("E"), inP, outN)/daFunk::var("E");
result.addChannel(dNdE, str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions); // specifies also center of mass energy range
};
// The following routine adds an annihilation channel, for which the yields are extrapolated below Ecm_ToScale
// using the approximation that x*dN/dx is a constant function of the dark matter mass.
auto add_channel_with_scaling = [&](int inP, str P1, str P2, str FINAL, double EcmMin, double EcmMax, double Ecm_ToScale)
{
daFunk::Funk Ecm_ToUse = fmax(Ecm_ToScale, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor = Ecm_ToUse/daFunk::var("Ecm");
daFunk::Funk dNdE = ScalingFactor * daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), Ecm_ToUse,
ScalingFactor * daFunk::var("E"), inP, outN)/(ScalingFactor * daFunk::var("E"));
result.addChannel(dNdE, str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions);
};
add_channel(0, "g", "g", "gamma", 2*2., 2*mDM_max);
add_channel(1, "d", "dbar", "gamma", 2*2., 2*mDM_max);
add_channel(2, "u", "ubar", "gamma", 2*2., 2*mDM_max);
add_channel(3, "s", "sbar", "gamma", 2*2., 2*mDM_max);
add_channel(4, "c", "cbar", "gamma", 2*2., 2*mDM_max);
add_channel(5, "b", "bbar", "gamma", 2*5., 2*mDM_max);
add_channel_with_scaling(6, "t", "tbar", "gamma", 2*160.0, 2*mDM_max, 2.0*176.0);
add_channel(7, "e+", "e-", "gamma", 2*2., 2*mDM_max);
add_channel(8, "mu+", "mu-", "gamma", 2*2., 2*mDM_max);
add_channel(9, "tau+", "tau-", "gamma", 2*2., 2*mDM_max);
add_channel(10, "Z0", "Z0", "gamma", 2*90.288, 2*mDM_max);
add_channel(13, "W+", "W-", "gamma", 2*79.497, 2*mDM_max);
result.addChannel(daFunk::zero("Ecm", "E"), "nu_e", "nubar_e", "gamma", 2*2., 2*mDM_max, runOptions);
result.addChannel(daFunk::zero("Ecm", "E"), "nu_mu", "nubar_mu", "gamma", 2*2., 2*mDM_max, runOptions);
result.addChannel(daFunk::zero("Ecm", "E"), "nu_tau", "nubar_tau", "gamma", 2*2., 2*mDM_max, runOptions);
// Add approximations for single-particle cases.
daFunk::Funk dNdE;
dNdE = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("_Ecm"), daFunk::var("E"), 8, outN)
/daFunk::var("E"))->set("_Ecm", daFunk::var("Ecm")*2);
result.addChannel(dNdE/2, str_flav_to_mass("mu+"), "gamma", 2., mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("mu-"), "gamma", 2., mDM_max, runOptions);
dNdE = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("_Ecm"), daFunk::var("E"), 9, outN)
/daFunk::var("E"))->set("_Ecm", daFunk::var("Ecm")*2);
result.addChannel(dNdE/2, str_flav_to_mass("tau+"), "gamma", 2., mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tau-"), "gamma", 2., mDM_max, runOptions);
dNdE = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("_Ecm"), daFunk::var("E"), 10, outN)
/daFunk::var("E"))->set("_Ecm", daFunk::var("Ecm")*2);
result.addChannel(dNdE/2, "Z0", "gamma", 90.288, mDM_max, runOptions);
dNdE = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("_Ecm"), daFunk::var("E"), 13, outN)
/daFunk::var("E"))->set("_Ecm", daFunk::var("Ecm")*2);
result.addChannel(dNdE/2, "W+", "gamma", 79.497, mDM_max, runOptions);
result.addChannel(dNdE/2, "W-", "gamma", 79.497, mDM_max, runOptions);
// Add single particle lookup for t tbar to prevent them from being tagged as missing final states for cascades.
double Ecm_ToScale_top = 176.0;
daFunk::Funk Ecm_ToUse_top = fmax(Ecm_ToScale_top, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor_top = Ecm_ToUse_top/daFunk::var("Ecm");
dNdE = ScalingFactor_top * (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("_Ecm"), ScalingFactor_top * daFunk::var("E"), 6, outN)
/(ScalingFactor_top * daFunk::var("E")))->set("_Ecm", Ecm_ToUse_top*2.0);
result.addChannel(dNdE/2, str_flav_to_mass("t"), "gamma", 160.0, mDM_max, runOptions);
result.addChannel(dNdE/2, str_flav_to_mass("tbar"), "gamma", 160.0, mDM_max, runOptions);
// Add channels with "mixed final states", i.e. final state particles with (potentially) different masses
daFunk::Funk Ecm = daFunk::var("Ecm");
auto add_channel_mixedmasses = [&](int inP1, int inP2, str P1, str P2, str FINAL, double m1, double m2, double EcmMin, double EcmMax)
{
daFunk::Funk dNdE_1 = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("Ecm1"),
daFunk::var("E"), inP1, outN)->set("Ecm1", Ecm + (m1*m1 - m2*m2)/Ecm))/daFunk::var("E");
daFunk::Funk dNdE_2 = (daFunk::func_fromThreadsafe(BEreq::dNdE.pointer(), daFunk::var("Ecm2"),
daFunk::var("E"), inP2, outN)->set("Ecm2", Ecm + (m2*m2 - m1*m1)/Ecm))/daFunk::var("E");
result.addChannel(0.5*(dNdE_1 + dNdE_2), str_flav_to_mass(P1), str_flav_to_mass(P2), FINAL, EcmMin, EcmMax, runOptions);
};
// - The numerical values for EcmMin and EcmMax are obtained from applying the corresponding two-body kinematics
// to the minimal/maximal center-of-mass energies allowed by the micromegas tables
add_channel_mixedmasses(2, 1, "u", "dbar", "gamma", 0.0, 0.0, 2*2., 2*mDM_max);
add_channel_mixedmasses(1, 2, "d", "ubar", "gamma", 0.0, 0.0, 2*2., 2*mDM_max);
add_channel_mixedmasses(2, 3, "u", "sbar", "gamma", 0.0, 0.0, 2*2., 2*mDM_max);
add_channel_mixedmasses(3, 2, "s", "ubar", "gamma", 0.0, 0.0, 2*2., 2*mDM_max);
add_channel_mixedmasses(2, 5, "u", "bbar", "gamma", 0.0, 5.0, 7.386, 2*mDM_max);
add_channel_mixedmasses(5, 2, "b", "ubar", "gamma", 5.0, 0.0, 7.386, 2*mDM_max);
add_channel_mixedmasses(4, 1, "c", "dbar", "gamma", 1.35, 0.0, 4.413, 2*mDM_max);
add_channel_mixedmasses(1, 4, "d", "cbar", "gamma", 0.0, 1.35, 4.413, 2*mDM_max);
add_channel_mixedmasses(4, 3, "c", "sbar", "gamma", 1.35, 0.0, 4.413, 2*mDM_max);
add_channel_mixedmasses(3, 4, "s", "cbar", "gamma", 0.0, 1.35, 4.413, 2*mDM_max);
add_channel_mixedmasses(4, 5, "c", "bbar", "gamma", 1.35, 5.0, 7.214, 2*mDM_max);
add_channel_mixedmasses(5, 4, "b", "cbar", "gamma", 5.0, 1.35, 7.214, 2*mDM_max);
add_channel_mixedmasses(6, 1, "t", "dbar", "gamma", 176.0, 0.0, 178.011, 2*mDM_max);
add_channel_mixedmasses(1, 6, "d", "tbar", "gamma", 0.0, 176.0, 178.011, 2*mDM_max);
add_channel_mixedmasses(6, 3, "t", "sbar", "gamma", 176.0, 0.0, 178.011, 2*mDM_max);
add_channel_mixedmasses(3, 6, "s", "tbar", "gamma", 0.0, 176.0, 178.011, 2*mDM_max);
add_channel_mixedmasses(6, 5, "t", "bbar", "gamma", 176.0, 5.0, 181.0, 2*mDM_max);
add_channel_mixedmasses(5, 6, "b", "tbar", "gamma", 5.0, 176.0, 181.0, 2*mDM_max);
initialized = true;
}
}
/// Positron SimYieldTable based on MicrOmegas tabulated results.
void positron_SimYieldTable_MicrOmegas(SimYieldTable& /*result*/)
{
using namespace Pipes::positron_SimYieldTable_MicrOmegas;
static bool initialized = false;
if ( not initialized )
{
DarkBit_error().raise(LOCAL_INFO,
"positron_SimYieldTable_MicrOmegas is not implemented yet. Use e.g. positron_SimYieldTable_DarkSUSY instead.");
}
}
SimYieldTable SimYieldTable_PPPC(const str& yield, bool allow_yield_extrapolation, double(*PPPC_yield)(double,double,std::string), safe_ptr<Options> runOptions)
{
using DarkBit_utils::str_flav_to_mass;
SimYieldTable result;
const double mDM_min = 5.0;
const double mDM_max = 100000.0;
auto add_channel = [&](const str& p1, const str& p2, const str& channel, double EcmMin, double EcmMax)
{
daFunk::Funk m = daFunk::var("m");
daFunk::Funk x = daFunk::var("x");
daFunk::Funk E = daFunk::var("Ekin");
daFunk::Funk Ecm = daFunk::var("Ecm");
daFunk::Funk dNdE = daFunk::func( PPPC_yield, daFunk::var("m"), daFunk::var("x"), channel);
dNdE = dNdE->set("x", E/m);
if (p2.size() > 0)
{
dNdE = dNdE->set("m",Ecm/2);
result.addChannel(dNdE, str_flav_to_mass(p1), str_flav_to_mass(p2), yield, EcmMin, EcmMax, runOptions);
}
else
{
dNdE = dNdE->set("m",Ecm);
result.addChannel(dNdE/2, str_flav_to_mass(p1), yield, EcmMin, EcmMax, runOptions);
}
};
// The following routine adds an annihilation/decay channel, for which the yields are extrapolated below Ecm_ToScale
// using the approximation that x*dN/dx is a constant function of the dark matter mass.
auto add_channel_with_scaling = [&](const str& p1, const str& p2, const str& channel, double EcmMin, double EcmMax, double Ecm_ToScale)
{
daFunk::Funk m = daFunk::var("m");
daFunk::Funk x = daFunk::var("x");
daFunk::Funk E = daFunk::var("Ekin");
daFunk::Funk Ecm_ToUse = fmax(Ecm_ToScale, daFunk::var("Ecm"));
daFunk::Funk ScalingFactor = Ecm_ToUse/daFunk::var("Ecm");
daFunk::Funk dNdE = daFunk::func( PPPC_yield, daFunk::var("m"), daFunk::var("x"), channel);
dNdE = (ScalingFactor*dNdE)->set("x", E/m);
if (p2.size() > 0)
{
dNdE = dNdE->set("m",Ecm_ToUse/2);
result.addChannel(dNdE, str_flav_to_mass(p1), str_flav_to_mass(p2), yield, EcmMin, EcmMax, runOptions);
}
else
{
dNdE = dNdE->set("m",Ecm_ToUse);
result.addChannel(dNdE/2, str_flav_to_mass(p1), yield, EcmMin, EcmMax, runOptions);
}
};
add_channel("e+", "e-", "e", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel("mu+", "mu-", "mu", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel("tau+", "tau-", "tau", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel("u", "ubar", "q", 2*std::max(mDM_min, 1.35), 2*mDM_max); // u,d,s are treated as one species
add_channel("d", "dbar", "q", 2*std::max(mDM_min, 1.35), 2*mDM_max);
add_channel("s", "sbar", "q", 2*std::max(mDM_min, 1.35), 2*mDM_max);
add_channel("c", "cbar", "c", 2*std::max(mDM_min, 1.35), 2*mDM_max);
add_channel("b", "bbar", "b", 2*std::max(mDM_min, 5.0), 2*mDM_max);
add_channel_with_scaling("t", "tbar", "t", 2*std::max(mDM_min, 160.0), 2*mDM_max, 2*173.3);
add_channel("W+", "W-", "W", 2*std::max(mDM_min, 79.4475), 2*mDM_max);
add_channel("Z0", "Z0", "Z", 2*std::max(mDM_min, 90.288), 2*mDM_max);
add_channel("g", "g", "g", 2*std::max(mDM_min, 0.0), 2*mDM_max);
//add_channel("gamma", "gamma", "gamma", 2*std::max(mDM_min, 0.0), 2*mDM_max);
//add_channel("h", "h", "h", 2*std::max(mDM_min, 125.1), 2*mDM_max);
add_channel("nu_e", "nubar_e", "nu_e", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel("nu_mu", "nubar_mu", "nu_mu", 2*std::max(mDM_min, 0.0), 2*mDM_max);
add_channel("nu_tau", "nubar_tau", "nu_tau", 2*std::max(mDM_min, 0.0), 2*mDM_max);
// Add approximations for single-particle cases.
add_channel("Z0", "", "Z", std::max(mDM_min, 90.288), mDM_max);
add_channel("W+", "", "W", std::max(mDM_min, 79.4475), mDM_max);
add_channel("W-", "", "W", std::max(mDM_min, 79.4475), mDM_max);
add_channel("e+", "", "e", std::max(mDM_min, 0.0), mDM_max);
add_channel("e-", "", "e", std::max(mDM_min, 0.0), mDM_max);
add_channel("mu+", "", "mu", std::max(mDM_min, 0.0), mDM_max);
add_channel("mu-", "", "mu", std::max(mDM_min, 0.0), mDM_max);
add_channel("tau+", "", "tau", std::max(mDM_min, 0.0), mDM_max);
add_channel("tau-", "", "tau", std::max(mDM_min, 0.0), mDM_max);
add_channel_with_scaling("t", "", "t", std::max(mDM_min, 160.0), mDM_max, 173.3);
add_channel_with_scaling("tbar", "", "t", std::max(mDM_min, 160.0), mDM_max, 173.3);
// Add channels with "mixed final states", i.e. final state particles with (potentially) different masses
auto add_channel_mixedmasses = [&](const str& p1, const str& p2, const str& ch1, const str& ch2, double m1, double m2, double EcmMin, double EcmMax)
{
daFunk::Funk m = daFunk::var("m");
daFunk::Funk x = daFunk::var("x");
daFunk::Funk E = daFunk::var("Ekin");
daFunk::Funk Ecm = daFunk::var("Ecm");
daFunk::Funk dNdE1 = daFunk::func( PPPC_yield, daFunk::var("m"), daFunk::var("x"), ch1);
dNdE1 = dNdE1->set("x", E/m)->set("m", Ecm/2 + (m1*m1 - m2*m2)/(2*Ecm));
daFunk::Funk dNdE2 = daFunk::func( PPPC_yield, daFunk::var("m"), daFunk::var("x"), ch2);
dNdE2 = dNdE2->set("x", E/m)->set("m", Ecm/2 + (m2*m2 - m1*m1)/(2*Ecm));
result.addChannel((dNdE1+dNdE2)/2, str_flav_to_mass(p1), str_flav_to_mass(p2), yield, EcmMin, EcmMax, runOptions);
};
// - The numerical values for EcmMin and EcmMax are obtained from applying the corresponding two-body kinematics
// to the minimally/maximally allowed center-of-mass energies. Hence, EcmMin depends on the flag allow_yield_extrapolation
add_channel_mixedmasses("u", "dbar", "q","q", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 10.0), 2*mDM_max);
add_channel_mixedmasses("d", "ubar", "q","q", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 10.0), 2*mDM_max);
add_channel_mixedmasses("u", "sbar", "q","q", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 10.0), 2*mDM_max);
add_channel_mixedmasses("s", "ubar", "q","q", 0.0, 0.0, (allow_yield_extrapolation ? 2*1.35 : 10.0), 2*mDM_max);
add_channel_mixedmasses("u", "bbar", "q","b", 0.0, 5.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses("b", "ubar", "b","q", 5.0, 0.0, (allow_yield_extrapolation ? 6.530 : 21.181), 2*mDM_max);
add_channel_mixedmasses("c", "dbar", "c","q", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses("d", "cbar", "q","c", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses("c", "sbar", "c","q", 1.35, 0.0, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses("s", "cbar", "q","c", 0.0, 1.35, (allow_yield_extrapolation ? 3.260 : 20.091), 2*mDM_max);
add_channel_mixedmasses("c", "bbar", "c","b", 1.35, 5.0, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses("b", "cbar", "b","c", 5.0, 1.35, (allow_yield_extrapolation ? 6.35 : 21.099), 2*mDM_max);
add_channel_mixedmasses("t", "dbar", "t","q", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses("d", "tbar", "q","t", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses("t", "sbar", "t","q", 175.0, 0.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses("s", "tbar", "q","t", 0.0, 175.0, (allow_yield_extrapolation ? 176.355 : 185.285), 2*mDM_max);
add_channel_mixedmasses("t", "bbar", "t","b", 175.0, 5.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
add_channel_mixedmasses("b", "tbar", "b","t", 5.0, 175.0, (allow_yield_extrapolation ? 180.0 : 185.214), 2*mDM_max);
return result;
}
// Functions for the PPPC yields are defined elsewhere
// (in PPPC.cpp if someone asks)
double PPPC_dNdE_gamma(double m, double x, std::string channel);
double PPPC_dNdE_positron(double m, double x, std::string channel);
/// Gamma-ray SimYieldTable based on PPPC4DMID Cirelli et al. 2010
void GA_SimYieldTable_PPPC(SimYieldTable& result)
{
using namespace Pipes::GA_SimYieldTable_PPPC;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
//bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
bool allow_yield_extrapolation = false;
result = SimYieldTable_PPPC("gamma", allow_yield_extrapolation, &PPPC_dNdE_gamma, runOptions);
initialized = true;
}
}
/// Positron SimYieldTable based on PPPC4DMID Cirelli et al. 2010
void positron_SimYieldTable_PPPC(SimYieldTable& result)
{
using namespace Pipes::positron_SimYieldTable_PPPC;
static bool initialized = false;
if ( not initialized )
{
/// Option allow_yield_extrapolation<bool>: Spectra extrapolated for masses beyond Pythia results (default false)
//bool allow_yield_extrapolation = runOptions->getValueOrDef(false, "allow_yield_extrapolation");
bool allow_yield_extrapolation = false;
result = SimYieldTable_PPPC("e+_1", allow_yield_extrapolation, &PPPC_dNdE_positron, runOptions);
initialized = true;
}
}
/// Bypasses to skip specific yields in FullSimYieldTable
void GA_SimYieldTable_empty(SimYieldTable& result)
{
static const SimYieldTable empty_table;
result = empty_table;
}
void positron_SimYieldTable_empty(SimYieldTable& result)
{
static const SimYieldTable empty_table;
result = empty_table;
}
void antiproton_SimYieldTable_empty(SimYieldTable& result)
{
static const SimYieldTable empty_table;
result = empty_table;
}
void antideuteron_SimYieldTable_empty(SimYieldTable& result)
{
static const SimYieldTable empty_table;
result = empty_table;
}
/// Electron SimYieldTable based on positron table
void electron_SimYieldTable_from_positron_SimYieldTable(SimYieldTable& result)
{
static bool initialized = false;
if ( not initialized )
{
// Just duplicate the positron yield. DarkSUSY at least does not offer separate electron yields.
result = *Pipes::electron_SimYieldTable_from_positron_SimYieldTable::Dep::positron_SimYieldTable;
result.replaceFinalState("e+_1","e-_1");
initialized = true;
}
}
// Dumper functions ================================================
/// \brief Helper function to dump any spectra
int dump(const str& filename, const daFunk::Funk& spectrum)
{
std::ofstream myfile (filename);
if (myfile.is_open())
{
for (int i = 0; i<=1200; i++)
{
double energy = pow(10., i/200. - 4.);
myfile << energy << " " << spectrum->bind("E")->eval(energy) << "\n";
}
myfile.close();
return 0;
}
else
{
DarkBit_error().raise(LOCAL_INFO, "Failed to open file " + filename + ".");
}
return 1;
}
/// \brief Helper function to dump gamma-ray spectra.
void dump_gammaSpectrum(int &result)
{
using namespace Pipes::dump_gammaSpectrum;
daFunk::Funk spectrum = (*Dep::GA_Yield)->set("v", 0.);
// Option filename<string>: Filename for gamma-ray spectrum dump
// (default: dNdE_gamma.dat)
std::string filename = runOptions->getValueOrDef<std::string>("dNdE_gamma.dat", "filename");
logger() << "FILENAME for gamma dump: " << filename << EOM;
result = dump(filename, spectrum);
}
/// \brief Helper function to dump electron spectra.
void dump_electronSpectrum(int &result)
{
using namespace Pipes::dump_electronSpectrum;
daFunk::Funk spectrum = (*Dep::electron_Yield)->set("v", 0.);
// Option filename<string>: Filename for electron spectrum dump
// (default: dNdE_electron.dat)
std::string filename = runOptions->getValueOrDef<std::string>("dNdE_electron.dat", "filename");
logger() << "FILENAME for electron dump: " << filename << EOM;
result = dump(filename, spectrum);
}
/// \brief Helper function to dump positron spectra.
void dump_positronSpectrum(int &result)
{
using namespace Pipes::dump_positronSpectrum;
daFunk::Funk spectrum = (*Dep::positron_Yield)->set("v", 0.);
// Option filename<string>: Filename for positron spectrum dump
// (default: dNdE_positron.dat)
std::string filename = runOptions->getValueOrDef<std::string>("dNdE_positron.dat", "filename");
logger() << "FILENAME for positron dump: " << filename << EOM;
result = dump(filename, spectrum);
}
/// \brief Helper function to dump anti-proton spectra.
void dump_antiprotonSpectrum(int &result)
{
using namespace Pipes::dump_antiprotonSpectrum;
daFunk::Funk spectrum = (*Dep::antiproton_Yield)->set("v", 0.);
// Option filename<string>: Filename for antiproton spectrum dump
// (default: dNdE_antiproton.dat)
std::string filename = runOptions->getValueOrDef<std::string>("dNdE_antiproton.dat", "filename");
logger() << "FILENAME for antiproton dump: " << filename << EOM;
result = dump(filename, spectrum);
}
/// \brief Helper function to dump anti-deuteron spectra.
void dump_antideuteronSpectrum(int &result)
{
using namespace Pipes::dump_antideuteronSpectrum;
daFunk::Funk spectrum = (*Dep::antideuteron_Yield)->set("v", 0.);
// Option filename<string>: Filename for antideuteron spectrum dump
// (default: dNdE_antideuteron.dat)
std::string filename = runOptions->getValueOrDef<std::string>("dNdE_antideuteron.dat", "filename");
logger() << "FILENAME for antideuteron dump: " << filename << EOM;
result = dump(filename, spectrum);
}
}
}
Updated on 2023-06-26 at 21:36:55 +0000