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ChooseInstantNonReversibleTransition kernel
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include/picongpu/particles/atomicPhysics/InstantTransitionRateLimit.hpp
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/* Copyright 2024 Brian Marre | ||
* | ||
* This file is part of PIConGPU. | ||
* | ||
* PIConGPU is free software: you can redistribute it and/or modify | ||
* it under the terms of the GNU General Public License as published by | ||
* the Free Software Foundation, either version 3 of the License, or | ||
* (at your option) any later version. | ||
* | ||
* PIConGPU is distributed in the hope that it will be useful, | ||
* but WITHOUT ANY WARRANTY; without even the implied warranty of | ||
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | ||
* GNU General Public License for more details. | ||
* | ||
* You should have received a copy of the GNU General Public License | ||
* along with PIConGPU. | ||
* If not, see <http://www.gnu.org/licenses/>. | ||
*/ | ||
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#pragma once | ||
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// need unit system and normalization | ||
#include "picongpu/defines.hpp" | ||
#include "picongpu/particles/atomicPhysics/param.hpp" | ||
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namespace picongpu::particles::atomicPhysics | ||
{ | ||
struct InstantTransitionRateLimit | ||
{ | ||
/** get limit of total state loss rate for inclusion n the time dependent rate equation solver | ||
* | ||
* @tparam T_ReturnType type and precision to use in the result | ||
*/ | ||
template<typename T_ReturnType> | ||
static constexpr T_ReturnType get() | ||
{ | ||
using picongpu::atomicPhysics::RateSolverParam; | ||
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// unit: unitless * unitless / unit_time = 1/unit_time | ||
return static_cast<T_ReturnType>( | ||
RateSolverParam::timeStepAlpha * float_X(RateSolverParam::maximumNumberSubStepsPerPICTimeStep)) | ||
/ picongpu::sim.pic.getDt<T_ReturnType>(); | ||
} | ||
} // namespace picongpu::particles::atomicPhysics |
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include/picongpu/particles/atomicPhysics/kernel/CheckForFieldEnergyOverSubscription.kernel
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/* Copyright 2024 Brian Marre | ||
* | ||
* This file is part of PIConGPU. | ||
* | ||
* PIConGPU is free software: you can redistribute it and/or modify | ||
* it under the terms of the GNU General Public License as published by | ||
* the Free Software Foundation, either version 3 of the License, or | ||
* (at your option) any later version. | ||
* | ||
* PIConGPU is distributed in the hope that it will be useful, | ||
* but WITHOUT ANY WARRANTY; without even the implied warranty of | ||
* MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | ||
* GNU General Public License for more details. | ||
* | ||
* You should have received a copy of the GNU General Public License | ||
* along with PIConGPU. | ||
* If not, see <http://www.gnu.org/licenses/>. | ||
*/ | ||
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#pragma once | ||
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#include "picongpu/defines.hpp" | ||
#include "picongpu/particles/atomicPhysics/ConvertEnum.hpp" | ||
#include "picongpu/particles/atomicPhysics/KernelIndexation.hpp" | ||
#include "picongpu/particles/atomicPhysics/kernel/CalculateRejectionProbability.hpp" | ||
#include "picongpu/particles/atomicPhysics/localHelperFields/RejectionProbabilityCache_Cell.hpp" | ||
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#include <pmacc/lockstep/ForEach.hpp> | ||
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#include <cstdint> | ||
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namespace picongpu::particles::atomicPhysics::kernel | ||
{ | ||
/** check all cells for overSubscription | ||
* | ||
* checks each superCell cell for fieldEnergyUse > fieldEnergy, | ||
* if yes mark cell as oversubscribed and stores rejection probability in rejection probability cache | ||
* | ||
* @tparam T_numberAtomicPhysicsIonSpecies specialization template parameter used to prevent compilation of all | ||
* atomicPhysics kernels if no atomic physics species is present. | ||
*/ | ||
template<uint32_t T_numberAtomicPhysicsIonSpecies> | ||
struct CheckForFieldEnergyOverSubscriptionKernel | ||
{ | ||
/** call operator | ||
* | ||
* called by CheckForOverSubscription atomic physics sub-stage | ||
* | ||
* @param worker object containing the device and block information, passed by PMACC_KERNEL call | ||
* @param areMapping mapping of blockIndex to block superCell index | ||
* @param rngFactory factory for uniformly distributed random number generator | ||
* @param eFieldBox deviceDataBox giving access to eField values for all local superCells | ||
* @param fieldEnergyUseCacheBox deviceDataBox giving access to the field energy use cache for each local | ||
* superCell | ||
* @param sharedResourcesOverSubscribedBox deviceDataBox giving access to the local shared resources over | ||
* subscription switch for each local superCell | ||
* @param rejectionProbabilityCacheCellBox deviceDataBox giving access to localRejectionProbabilityCache for | ||
* all local superCells | ||
*/ | ||
template< | ||
typename T_Worker, | ||
typename T_AreaMapping, | ||
typename T_TimeRemainingBox, | ||
typename T_EFieldBox, | ||
typename T_FieldEnergyUseCacheBox, | ||
typename T_SharedRessourcesOverSubscribedBox, | ||
typename T_RejectionProbabilityCacheCellDataBox> | ||
HDINLINE void operator()( | ||
T_Worker const& worker, | ||
T_AreaMapping const areaMapping, | ||
T_TimeRemainingBox const timeRemainingBox, | ||
T_EFieldBox const eFieldBox, | ||
T_FieldEnergyUseCacheBox const fieldEnergyUseCacheBox, | ||
T_SharedRessourcesOverSubscribedBox sharedResourcesOverSubscribedBox, | ||
T_RejectionProbabilityCacheCellDataBox rejectionProbabilityCacheCellBox) const | ||
{ | ||
auto const superCellIdx = KernelIndexation::getSuperCellIndex(worker, areaMapping); | ||
auto const superCellFieldIdx | ||
= KernelIndexation::getSuperCellFieldIndexFromSuperCellIndex(areaMapping, superCellIdx); | ||
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auto const timeRemaining = timeRemainingBox(superCellFieldIdx); | ||
if(timeRemaining <= 0._X) | ||
return; | ||
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using FieldEnergyCache = typename T_FieldEnergyUseCacheBox::ValueType; | ||
particles::atomicPhysics::localHelperFields::RejectionProbabilityCache_Cell<FieldEnergyCache::numberCells>& | ||
rejectionProbabilityCacheCell | ||
= rejectionProbabilityCacheCellBox(superCellFieldIdx); | ||
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/// @todo split rejectionProbabilityCache into cell and bin to avoid loading everything?, Brian Marre, 2024 | ||
FieldEnergyCache const& eFieldEnergyUseCache = fieldEnergyUseCacheBox(superCellFieldIdx); | ||
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bool sharedResourcesOverSubscribed = false; | ||
DataSpace<picongpu::simDim> const superCellCellOffset = superCellIdx * picongpu::SuperCellSize::toRT(); | ||
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auto forEachCell = pmacc::lockstep::makeForEach<::numberCells, T_Worker>(worker); | ||
forEachCell( | ||
[&worker, | ||
&superCellCellOffset, | ||
&eFieldBox, | ||
&eFieldEnergyUseCache, | ||
&rejectionProbabilityCacheCell, | ||
&sharedResourcesOverSubscribed](uint32_t const linearCellIndex) | ||
{ | ||
CalculateRejectionProbability::ofCell( | ||
linearCellIndex, | ||
superCellCellOffset, | ||
eFieldBox, | ||
eFieldEnergyUseCache, | ||
rejectionProbabilityCacheCell, | ||
sharedResourcesOverSubscribed); | ||
}); | ||
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uint32_t& flagField = sharedResourcesOverSubscribedBox(superCellFieldIdx); | ||
// write out flag setting to device memory | ||
alpaka::atomicOr( | ||
worker.getAcc(), | ||
&flagField, | ||
u32(sharedResourcesOverSubscribed), | ||
::alpaka::hierarchy::Threads{}); | ||
} | ||
}; | ||
} // namespace picongpu::particles::atomicPhysics::kernel |
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