Solver performing calculations in 2D Cartesian or Cylindrical space using finite element method. More...

#include <solvers/electrical/ddm2d/ddm2d.hpp>

Inheritance diagram for plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >:

Collaboration diagram for plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >:

Public Member Functions
double	compute (unsigned loops=1)
	Run drift_diffusion calculations.

double	findEnergyLevels ()
	Find energy levels - TEST.

bool	checkWell (std::string _carrier)
	Check if the carriers are confined.

double	integrateCurrent (size_t vindex, bool onlyactive=false)
	Integrate vertical total current at certain level.

double	getTotalCurrent (size_t nact=0)
	Integrate vertical total current flowing vertically through active region.

void	loadConfiguration (XMLReader &source, Manager &manager) override
	Compute total electrostatic energy stored in the structure.

	DriftDiffusionModel2DSolver (const std::string &name="")

std::string	getClassName () const override
	Get name of solver.

	~DriftDiffusionModel2DSolver ()

double	integrateCurrent (size_t vindex, bool onlyactive)

double	integrateCurrent (size_t vindex, bool onlyactive)

std::string	getClassName () const
	Get name of solver.

std::string	getClassName () const
	Get name of solver.

Public Member Functions inherited from plask::FemSolverWithMesh< Geometry2DType, RectangularMesh< 2 > >
	FemSolverWithMesh (const std::string &name="")

bool	parseFemConfiguration (XMLReader &reader, Manager &manager)

FemMatrix *	getMatrix ()

FemMatrix *	getMatrix ()

Public Member Functions inherited from plask::SolverWithMesh< SpaceT, MeshT >
	SolverWithMesh (const std::string &name="")

	~SolverWithMesh ()

void	loadConfiguration (XMLReader &source, Manager &manager) override
	Load configuration from given `source`.

void	parseStandardConfiguration (XMLReader &source, Manager &manager, const std::string &expected_msg="solver configuration element")

virtual void	onMeshChange (const typename MeshT::Event &PLASK_UNUSED(evt))
	This method is called just after the mesh has been changed.

void	onGeometryChange (const Geometry::Event &PLASK_UNUSED(evt)) override
	This method is called when the geometry is changed.

MeshT &	meshRef () const
	Get current module mesh.

shared_ptr< MeshT >	getMesh () const
	Get current solver mesh.

void	setMesh (const shared_ptr< MeshT > &mesh)
	Set new mesh for the solver.

void	setMesh (shared_ptr< MeshGeneratorD< MeshT::DIM > > generator)
	Set new mesh got from generator.

Public Member Functions inherited from plask::SolverOver< SpaceT >
	SolverOver (const std::string &name="")

	~SolverOver ()

void	parseStandardConfiguration (XMLReader &source, Manager &manager, const std::string &expected_msg="solver configuration element")

shared_ptr< SpaceT >	getGeometry () const
	Get current solver geometry space.

void	setGeometry (const shared_ptr< SpaceT > &geometry)
	Set new geometry for the solver.

Public Member Functions inherited from plask::Solver
bool	initCalculation ()
	This should be called on beginning of each calculation method to ensure that solver will be initialized.

	Solver (const std::string &name="")
	Construct uninitialized solver.

virtual	~Solver ()
	Virtual destructor (for subclassing). Do nothing.

void	parseStandardConfiguration (XMLReader &source, Manager &manager, const std::string &expected_msg="solver configuration element")
	Load standard configuration (geometry, mesh) tags from `source`.

bool	isInitialized ()
	Check if solver is already initialized.

void	invalidate ()
	This method should be and is called if something important was changed: calculation space, mesh, etc.

std::string	getId () const
	Get solver id.

std::string	getName () const

virtual std::string	getClassDescription () const
	Get a description of this solver.

template<typename ArgT = double, typename ValT = double>
DataLog< ArgT, ValT >	dataLog (const std::string &chart_name, const std::string &axis_arg_name, const std::string &axis_val_name)

template<typename ArgT = double, typename ValT = double>
DataLog< ArgT, ValT >	dataLog (const std::string &axis_arg_name, const std::string &axis_val_name)

template<typename ... Args>
void	writelog (LogLevel level, std::string msg, Args &&... params) const
	Log a message for this solver.

Public Attributes
double	maxerr
	bands have to be up-shifted - we want only positive values of energy levels; unit: eV

BoundaryConditions< RectangularMesh< 2 >::Boundary, double >	voltage_boundary
	Boundary condition.

ProviderFor< Potential, Geometry2DType >::Delegate	outPotential

ProviderFor< FermiLevels, Geometry2DType >::Delegate	outFermiLevels

ProviderFor< BandEdges, Geometry2DType >::Delegate	outBandEdges

ProviderFor< CurrentDensity, Geometry2DType >::Delegate	outCurrentDensityForElectrons

ProviderFor< CurrentDensity, Geometry2DType >::Delegate	outCurrentDensityForHoles

ProviderFor< CarriersConcentration, Geometry2DType >::Delegate	outCarriersConcentration

ProviderFor< Heat, Geometry2DType >::Delegate	outHeat

ReceiverFor< Temperature, Geometry2DType >	inTemperature

bool	mRsrh
	SRH recombination is taken into account.

bool	mRrad
	radiative recombination is taken into account

bool	mRaug
	Auger recombination is taken into account.

bool	mPol
	polarization (GaN is the substrate)

bool	mFullIon
	dopant ionization = 100%

double	mSchottkyP
	Schottky barrier for p-type contact (eV)

double	mSchottkyN
	Schottky barrier for n-type contact (eV)

double	maxerrPsiI
	Maximum estimated error for initial potential during all iterations (useful for single calculations managed by external python script)

double	maxerrPsi0
	Maximum estimated error for potential at U = 0 V during all iterations (useful for single calculations managed by external python script)

double	maxerrPsi
	Maximum estimated error for potential during all iterations (useful for single calculations managed by external python script)

double	maxerrFn
	Maximum estimated error for quasi-Fermi energy level for electrons during all iterations (useful for single calculations managed by external python script)

double	maxerrFp
	Maximum estimated error for quasi-Fermi energy level for holes during all iterations (useful for single calculations managed by external python script)

size_t	loopsPsiI
	Loops limit for initial potential.

size_t	loopsPsi0
	Loops limit for potential at U = 0 V.

size_t	loopsPsi
	Loops limit for potential.

size_t	loopsFn
	Loops limit for quasi-Fermi energy level for electrons.

size_t	loopsFp
	Loops limit for quasi-Fermi energy level for holes.

Public Attributes inherited from plask::FemSolverWithMesh< Geometry2DType, RectangularMesh< 2 > >
FemMatrixAlgorithm	algorithm
	Factorization algorithm to use.

IterativeMatrixParams	iter_params
	Parameters of iterative solver.

Protected Member Functions
void	onInitialize () override
	Initialize the solver.

void	onInvalidate () override
	Invalidate the data.

size_t	getActiveRegionMeshIndex (size_t actnum) const
	Get info on active region.

void	onMeshChange (const typename RectangularMesh< 2 >::Event &evt) override

void	onGeometryChange (const Geometry::Event &evt) override
	This method is called when the geometry is changed.

void	computePsiI ()
	Calculate initial potential for all elements.

size_t	isActive (const Vec< 2 > &point) const
	Return `true` if the specified point is at junction.

size_t	isActive (const RectangularMesh< 2 >::Element &element) const
	Return `true` if the specified element is a junction.

const LazyData< double >	getPotentials (shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method) const

const LazyData< double >	getFermiLevels (FermiLevels::EnumType what, shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method) const

const LazyData< double >	getBandEdges (BandEdges::EnumType what, shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method)

const LazyData< double >	getHeatDensities (shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method)

const LazyData< Vec< 2 > >	getCurrentDensitiesForElectrons (shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method)

const LazyData< Vec< 2 > >	getCurrentDensitiesForHoles (shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method)

const LazyData< double >	getCarriersConcentration (CarriersConcentration::EnumType what, shared_ptr< const MeshD< 2 > > dest_mesh, InterpolationMethod method)

Protected Member Functions inherited from plask::SolverOver< SpaceT >
template<typename Boundary , typename ConditionT >
void	readBoundaryConditions (Manager &manager, XMLReader &reader, BoundaryConditions< Boundary, ConditionT > &dest)
	Read boundary conditions using information about the geometry of this solver.

Protected Attributes
std::size_t	size
	Number of columns in the main matrix.

double	mTx
	ambient temperature (K)

double	mEx
	energy (eV)

double	mNx
	maximal doping concentration (1/cm^3)

double	mEpsRx
	maximal dielectric constant (-)

double	mXx
	sometimes denoted as LD (um)

double	mMix
	maximal mobility (cm^2/Vs)

double	mRx
	recombination parameter (1/(cm^3*s))

double	mJx
	current density parameter (kA/cm2)

double	mAx
	radiative recombination coefficient (1/s)

double	mBx
	radiative recombination coefficient (cm^3/s)

double	mCx
	Auger recombination coefficient (cm^6/s)

double	mPx
	polarization (C/m^2)

double	dU
	default voltage step (V)

double	maxDelPsi0
	maximal correction for initial potential calculations (V)

double	maxDelPsi
	maximal correction for potential calculations (V)

double	maxDelFn
	maximal correction for quasi-Fermi levels for electrons calculations (eV)

double	maxDelFp
	maximal correction for quasi-Fermi levels for holes calculations (eV)

Stat	stat
	carriers statistics

ContType	conttype
	type of contacts (ohmic/Schottky)

DataVector< double >	dveN
	Cached electron concentrations (size: elements)

DataVector< double >	dveP
	Cached hole concentrations (size: elements)

DataVector< double >	dvePsi
	Computed potentials (size: elements)

DataVector< double >	dveFnEta
	Computed exponents of quasi-Fermi levels for electrons (size: elements)

DataVector< double >	dveFpKsi
	Computed exponents of quasi-Fermi levels for holes (size: elements)

DataVector< double >	dvnPsi0
	Computed potential for U=0V (size: nodes)

DataVector< double >	dvnPsi
	Computed potentials (size: nodes)

DataVector< double >	dvnFnEta
	Computed exponents of quasi-Fermi levels for electrons (size: nodes)

DataVector< double >	dvnFpKsi
	Computed exponents of quasi-Fermi levels for holes (size: nodes)

DataVector< Vec< 2, double > >	currentsN
	Computed current densities for electrons.

DataVector< Vec< 2, double > >	currentsP
	Computed current densities for holes.

DataVector< double >	heats
	Computed and cached heat source densities.

bool	needPsi0
	Flag indicating if we need to compute initial potential;.

double	T0
	Temperature used for compiting level estimates.

bool	strained
	Consider strain in QW?

Protected Attributes inherited from plask::SolverWithMesh< SpaceT, MeshT >
shared_ptr< MeshT >	mesh
	Mesh over which the calculations are performed.

boost::signals2::connection	mesh_signal_connection
	Connection of mesh to onMeshChange method, see http://www.boost.org/doc/libs/1_55_0/doc/html/signals2/tutorial.html#idp204830936.

Protected Attributes inherited from plask::SolverOver< SpaceT >
shared_ptr< SpaceT >	geometry
	Space in which the calculations are performed.

Protected Attributes inherited from plask::Solver
bool	initialized
	`true` only if solver is initialized

Additional Inherited Members
Public Types inherited from plask::SolverWithMesh< SpaceT, MeshT >
typedef MeshT	MeshType
	Type of the mesh for this solver.

Public Types inherited from plask::SolverOver< SpaceT >
typedef SpaceT	SpaceType
	of the space for this solver

Detailed Description

template<typename Geometry2DType>
struct plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >

Solver performing calculations in 2D Cartesian or Cylindrical space using finite element method.

Definition at line 54 of file ddm2d.hpp.

Constructor & Destructor Documentation

◆ DriftDiffusionModel2DSolver()

template<typename Geometry2DType >

plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::DriftDiffusionModel2DSolver ( const std::string & name = "" )

Definition at line 51 of file ddm2d.cpp.

◆ ~DriftDiffusionModel2DSolver()

template<typename Geometry2DType >

plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::~DriftDiffusionModel2DSolver ( )

Definition at line 162 of file ddm2d.cpp.

Member Function Documentation

◆ checkWell()

template<typename Geometry2DType >

bool plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::checkWell ( std::string _carrier )

Check if the carriers are confined.

Returns: true when carriers are confined

electrons

ne+2 because cladding elements also

filling CBel vector /// TODO

finding min. and max. for CB

max. CB at boundary

TODO

Definition at line 1095 of file ddm2d.cpp.

◆ compute()

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::compute ( unsigned loops = 1 )

Run drift_diffusion calculations.

Returns: max correction of potential against the last call

Definition at line 1151 of file ddm2d.cpp.

◆ computePsiI()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::computePsiI ( )

protected

Calculate initial potential for all elements.

Definition at line 764 of file ddm2d.cpp.

◆ findEnergyLevels()

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::findEnergyLevels ( )

Find energy levels - TEST.

Returns: nothing important

hb*hb/(2m), unit: eV*nm*nm, 10^9 is introduced to change m into nm

bands have to be up-shifted - we want only positive values of energy levels; unit: (eV)

TODO

true when electrons (el) are confined

true when heavy holes (hh) are confined

true when light holes (lh) are confined

1/(dz*dz), unit: (1/nm^2)

1/(dz), unit: (1/nm)

the order of the small matrix for central-node for CB

the order of the matrix for CB

N - Hc size

setting Hc = zeros

nn - number of nodes

centre of the left element

centre of the right element

left/central/right 1x1 local matrix

11

Re - real part., Im - imag part.

no energy levels for electrons

lev_el - vector with energy levels for electrons

n_lev_el - number of energy levels of electrons

we have to find out if this level corresponds to el

"1" in both cases because only el are considered here

sorting electron energy levels

Definition at line 950 of file ddm2d.cpp.

◆ getActiveRegionMeshIndex()

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getActiveRegionMeshIndex ( size_t actnum ) const

protected

Get info on active region.

Definition at line 167 of file ddm2d.cpp.

◆ getBandEdges()

template<typename Geometry2DType >

const LazyData< double > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getBandEdges	(	BandEdges::EnumType	what,
		shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)

protected

Definition at line 1453 of file ddm2d.cpp.

◆ getCarriersConcentration()

template<typename Geometry2DType >

const LazyData< double > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getCarriersConcentration	(	CarriersConcentration::EnumType	what,
		shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)

protected

Definition at line 1561 of file ddm2d.cpp.

◆ getClassName() [1/3]

std::string plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DCartesian >::getClassName ( ) const

virtual

Get name of solver.

Returns: name of this solver

Implements plask::Solver.

Definition at line 2196 of file ddm2d.cpp.

◆ getClassName() [2/3]

std::string plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DCylindrical >::getClassName ( ) const

virtual

Get name of solver.

Returns: name of this solver

Implements plask::Solver.

Definition at line 2197 of file ddm2d.cpp.

◆ getClassName() [3/3]

template<typename Geometry2DType >

std::string plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getClassName ( ) const

overridevirtual

Get name of solver.

Returns: name of this solver

Implements plask::Solver.

◆ getCurrentDensitiesForElectrons()

template<typename Geometry2DType >

const LazyData< Vec< 2 > > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getCurrentDensitiesForElectrons	(	shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)

protected

Definition at line 1529 of file ddm2d.cpp.

◆ getCurrentDensitiesForHoles()

template<typename Geometry2DType >

const LazyData< Vec< 2 > > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getCurrentDensitiesForHoles	(	shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)

protected

Definition at line 1545 of file ddm2d.cpp.

◆ getFermiLevels()

template<typename Geometry2DType >

const LazyData< double > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getFermiLevels	(	FermiLevels::EnumType	what,
		shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)		const

protected

Definition at line 1419 of file ddm2d.cpp.

◆ getHeatDensities()

template<typename Geometry2DType >

const LazyData< double > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getHeatDensities	(	shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)

protected

Definition at line 1624 of file ddm2d.cpp.

◆ getPotentials()

template<typename Geometry2DType >

const LazyData< double > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getPotentials	(	shared_ptr< const MeshD< 2 > >	dest_mesh,
		InterpolationMethod	method
	)		const

protected

Definition at line 1409 of file ddm2d.cpp.

◆ getTotalCurrent()

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::getTotalCurrent ( size_t nact = 0 )

Integrate vertical total current flowing vertically through active region.

Parameters

nact	number of the active region

Returns: computed total current

Definition at line 1401 of file ddm2d.cpp.

◆ integrateCurrent() [1/3]

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DCartesian >::integrateCurrent	(	size_t	vindex,
		bool	onlyactive
	)

Definition at line 1369 of file ddm2d.cpp.

◆ integrateCurrent() [2/3]

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DCylindrical >::integrateCurrent	(	size_t	vindex,
		bool	onlyactive
	)

Definition at line 1384 of file ddm2d.cpp.

◆ integrateCurrent() [3/3]

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::integrateCurrent	(	size_t	vindex,
		bool	onlyactive = `false`
	)

Integrate vertical total current at certain level.

Parameters

vindex	vertical index of the element mesh to perform integration at
onlyactive	if true only current in the active region is considered

Returns: computed total current

◆ isActive() [1/2]

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::isActive ( const RectangularMesh< 2 >::Element & element ) const

inlineprotected

Return true if the specified element is a junction.

Definition at line 160 of file ddm2d.hpp.

◆ isActive() [2/2]

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::isActive ( const Vec< 2 > & point ) const

inlineprotected

Return true if the specified point is at junction.

Parameters

point point to test

Returns: number of active region + 1 (0 for none)

Definition at line 134 of file ddm2d.hpp.

◆ loadConfiguration()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loadConfiguration	(	XMLReader &	source,
		Manager &	manager
	)

overridevirtual

Compute total electrostatic energy stored in the structure.

Returns: total electrostatic energy [J] Estimate structure capacitance.; static structure capacitance [pF] Compute total heat generated by the structure in unit time; total generated heat (mW) Return the maximum estimated error.

Reimplemented from plask::Solver.

Definition at line 112 of file ddm2d.cpp.

◆ onGeometryChange()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::onGeometryChange ( const Geometry::Event & )

inlineoverrideprotectedvirtual

This method is called when the geometry is changed.

It just calls invalidate(); but subclasses can customize it.

Parameters

evt	information about geometry changes

Reimplemented from plask::SolverOver< SpaceT >.

Definition at line 121 of file ddm2d.hpp.

◆ onInitialize()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::onInitialize ( )

overrideprotectedvirtual

Initialize the solver.

Reimplemented from plask::Solver.

Definition at line 217 of file ddm2d.cpp.

◆ onInvalidate()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::onInvalidate ( )

overrideprotectedvirtual

Invalidate the data.

Reimplemented from plask::Solver.

Definition at line 243 of file ddm2d.cpp.

◆ onMeshChange()

template<typename Geometry2DType >

void plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::onMeshChange ( const typename RectangularMesh< 2 >::Event & evt )

inlineoverrideprotected

Definition at line 117 of file ddm2d.hpp.

Member Data Documentation

◆ conttype

template<typename Geometry2DType >

ContType plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::conttype

protected

type of contacts (ohmic/Schottky)

Definition at line 82 of file ddm2d.hpp.

◆ currentsN

template<typename Geometry2DType >

DataVector<Vec<2, double> > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::currentsN

protected

Computed current densities for electrons.

Definition at line 98 of file ddm2d.hpp.

◆ currentsP

template<typename Geometry2DType >

DataVector<Vec<2, double> > plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::currentsP

protected

Computed current densities for holes.

Definition at line 99 of file ddm2d.hpp.

◆ dU

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dU

protected

default voltage step (V)

Definition at line 75 of file ddm2d.hpp.

◆ dveFnEta

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dveFnEta

protected

Computed exponents of quasi-Fermi levels for electrons (size: elements)

Definition at line 91 of file ddm2d.hpp.

◆ dveFpKsi

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dveFpKsi

protected

Computed exponents of quasi-Fermi levels for holes (size: elements)

Definition at line 92 of file ddm2d.hpp.

◆ dveN

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dveN

protected

Cached electron concentrations (size: elements)

Definition at line 88 of file ddm2d.hpp.

◆ dveP

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dveP

protected

Cached hole concentrations (size: elements)

Definition at line 89 of file ddm2d.hpp.

◆ dvePsi

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dvePsi

protected

Computed potentials (size: elements)

Definition at line 90 of file ddm2d.hpp.

◆ dvnFnEta

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dvnFnEta

protected

Computed exponents of quasi-Fermi levels for electrons (size: nodes)

Definition at line 96 of file ddm2d.hpp.

◆ dvnFpKsi

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dvnFpKsi

protected

Computed exponents of quasi-Fermi levels for holes (size: nodes)

Definition at line 97 of file ddm2d.hpp.

◆ dvnPsi

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dvnPsi

protected

Computed potentials (size: nodes)

Definition at line 95 of file ddm2d.hpp.

◆ dvnPsi0

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::dvnPsi0

protected

Computed potential for U=0V (size: nodes)

Definition at line 94 of file ddm2d.hpp.

◆ heats

template<typename Geometry2DType >

DataVector<double> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::heats

protected

Computed and cached heat source densities.

Definition at line 100 of file ddm2d.hpp.

◆ inTemperature

template<typename Geometry2DType >

ReceiverFor<Temperature, Geometry2DType> plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::inTemperature

Definition at line 392 of file ddm2d.hpp.

◆ loopsFn

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loopsFn

Loops limit for quasi-Fermi energy level for electrons.

Definition at line 416 of file ddm2d.hpp.

◆ loopsFp

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loopsFp

Loops limit for quasi-Fermi energy level for holes.

Definition at line 417 of file ddm2d.hpp.

◆ loopsPsi

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loopsPsi

Loops limit for potential.

Definition at line 415 of file ddm2d.hpp.

◆ loopsPsi0

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loopsPsi0

Loops limit for potential at U = 0 V.

Definition at line 414 of file ddm2d.hpp.

◆ loopsPsiI

template<typename Geometry2DType >

size_t plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::loopsPsiI

Loops limit for initial potential.

Definition at line 413 of file ddm2d.hpp.

◆ mAx

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::mAx

protected

radiative recombination coefficient (1/s)

Definition at line 69 of file ddm2d.hpp.

◆ maxDelFn

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxDelFn

protected

maximal correction for quasi-Fermi levels for electrons calculations (eV)

Definition at line 78 of file ddm2d.hpp.

◆ maxDelFp

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxDelFp

protected

maximal correction for quasi-Fermi levels for holes calculations (eV)

Definition at line 79 of file ddm2d.hpp.

◆ maxDelPsi

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxDelPsi

protected

maximal correction for potential calculations (V)

Definition at line 77 of file ddm2d.hpp.

◆ maxDelPsi0

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxDelPsi0

protected

maximal correction for initial potential calculations (V)

Definition at line 76 of file ddm2d.hpp.

◆ maxerr

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxerr

bands have to be up-shifted - we want only positive values of energy levels; unit: eV

Maximum relative current density correction accepted as convergence

Definition at line 371 of file ddm2d.hpp.

◆ maxerrFn

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxerrFn

Maximum estimated error for quasi-Fermi energy level for electrons during all iterations (useful for single calculations managed by external python script)

Definition at line 409 of file ddm2d.hpp.

◆ maxerrFp

template<typename Geometry2DType >

double plask::electrical::drift_diffusion::DriftDiffusionModel2DSolver< Geometry2DType >::maxerrFp

Maximum estimated error for quasi-Fermi energy level for holes during all iterations (useful for single calculations managed by external python script)

Definition at line 411 of file ddm2d.hpp.