#include <utils/TypeConfig.h>
#include <utils/MemorySpaceType.h>
#include <linearAlgebra/LinearAlgebraTypes.h>
#include <linearAlgebra/LinearSolverFunction.h>
#include <linearAlgebra/OperatorContext.h>
#include <electrostatics/LaplaceOperatorContextFE.h>
#include <linearAlgebra/PreconditionerJacobi.h>
#include <linearAlgebra/PreconditionerNone.h>
#include <basis/FEBasisManager.h>
#include <basis/FEBasisOperations.h>
#include <basis/FEBasisDataStorage.h>
#include <quadrature/QuadratureValuesContainer.h>
#include <vector>
#include <memory>
#include <utils/Profiler.h>
#include <electrostatics/PoissonLinearSolverFunctionFE.t.cpp>

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Classes
class	dftefe::electrostatics::PoissonLinearSolverFunctionFE< ValueTypeOperator, ValueTypeOperand, memorySpace, dim >
	A derived class of linearAlgebra::LinearSolverFunction to encapsulate the Poisson partial differential equation (PDE) discretized in a finite element (FE) basis. The Possion PDE is given as: $\nabla^2 v(\textbf{r}) = -4 \pi \rho(\textbf{r})$\f with the boundary condition on $@_fakenlv(\textbf{r})\|_{\partial \Omega}=g(\textbf{r})$\f ( $\\partial Omega$\f denoting the boundary of a domain $\Omega$\f). Here $v$\f has the physical notion of a potential (e.g., Hartree potential, nuclear potential, etc.) arising due to a charge distributin $\rho$\f. More...

Namespaces
namespace	dftefe
	dealii includes

namespace	dftefe::electrostatics

Classes

Namespaces