SpECTRE Documentation Coverage Report
Current view: top level - Elliptic/Systems/SelfForce/Scalar - Equations.hpp Hit Total Coverage
Commit: a18e59fda1a195609825c55450f7d61ad20a91a4 Lines: 6 24 25.0 %
Date: 2026-06-11 22:10:41
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          Line data    Source code
       1           0 : // Distributed under the MIT License.
       2             : // See LICENSE.txt for details.
       3             : 
       4             : #pragma once
       5             : 
       6             : #include <cstddef>
       7             : #include <pup.h>
       8             : 
       9             : #include "DataStructures/ComplexDataVector.hpp"
      10             : #include "DataStructures/DataVector.hpp"
      11             : #include "DataStructures/Tensor/Tensor.hpp"
      12             : #include "DataStructures/Variables.hpp"
      13             : #include "DataStructures/VariablesTag.hpp"
      14             : #include "Domain/Tags.hpp"
      15             : #include "Elliptic/Systems/SelfForce/Scalar/Tags.hpp"
      16             : #include "Elliptic/Tags.hpp"
      17             : #include "NumericalAlgorithms/DiscontinuousGalerkin/Tags.hpp"
      18             : #include "PointwiseFunctions/GeneralRelativity/Tags.hpp"
      19             : #include "PointwiseFunctions/InitialDataUtilities/Background.hpp"
      20             : #include "Utilities/Gsl.hpp"
      21             : #include "Utilities/MakeWithValue.hpp"
      22             : #include "Utilities/TMPL.hpp"
      23             : 
      24             : namespace ScalarSelfForce {
      25             : 
      26             : /*!
      27             :  * \brief The first-order flux
      28             :  * $F^i=\{\partial_{r_\star}, \alpha \partial_{\cos\theta}\}\Psi_m$.
      29             :  */
      30           1 : void fluxes(gsl::not_null<tnsr::I<ComplexDataVector, 2>*> flux,
      31             :             const tnsr::I<ComplexDataVector, 2>& alpha,
      32             :             const tnsr::i<ComplexDataVector, 2>& field_gradient);
      33             : 
      34             : /*!
      35             :  * \brief The first-order flux on an element face
      36             :  * $F^i=\{n_{r_\star}, \alpha n_{\cos\theta}\}\Psi_m$.
      37             :  */
      38           1 : void fluxes_on_face(gsl::not_null<tnsr::I<ComplexDataVector, 2>*> flux,
      39             :                     const tnsr::I<ComplexDataVector, 2>& alpha,
      40             :                     const tnsr::I<DataVector, 2>& face_normal_vector,
      41             :                     const Scalar<ComplexDataVector>& field);
      42             : 
      43             : /*!
      44             :  * \brief The source term $\beta \Psi_m + \gamma_i \partial_i \Psi_m$.
      45             :  */
      46           1 : void add_sources(gsl::not_null<Scalar<ComplexDataVector>*> source,
      47             :                  const Scalar<ComplexDataVector>& beta,
      48             :                  const tnsr::i<ComplexDataVector, 2>& gamma,
      49             :                  const Scalar<ComplexDataVector>& field,
      50             :                  const tnsr::i<ComplexDataVector, 2>& field_gradient);
      51             : 
      52             : /// Fluxes $F^i$ for the scalar self-force system.
      53             : /// \see ScalarSelfForce::FirstOrderSystem
      54           1 : struct Fluxes {
      55           0 :   using argument_tags = tmpl::list<Tags::Alpha>;
      56           0 :   using volume_tags = tmpl::list<>;
      57           0 :   using const_global_cache_tags = tmpl::list<>;
      58           0 :   static constexpr bool is_trivial = false;
      59           0 :   static constexpr bool is_discontinuous = false;
      60           0 :   static void apply(gsl::not_null<tnsr::I<ComplexDataVector, 2>*> flux,
      61             :                     const tnsr::I<ComplexDataVector, 2>& alpha,
      62             :                     const Scalar<ComplexDataVector>& /*field*/,
      63             :                     const tnsr::i<ComplexDataVector, 2>& field_gradient);
      64           0 :   static void apply(gsl::not_null<tnsr::I<ComplexDataVector, 2>*> flux,
      65             :                     const tnsr::I<ComplexDataVector, 2>& alpha,
      66             :                     const tnsr::i<DataVector, 2>& /*face_normal*/,
      67             :                     const tnsr::I<DataVector, 2>& face_normal_vector,
      68             :                     const Scalar<ComplexDataVector>& field);
      69             : };
      70             : 
      71             : /// Source terms for the scalar self-force system.
      72             : /// \see ScalarSelfForce::FirstOrderSystem
      73           1 : struct Sources {
      74           0 :   using argument_tags = tmpl::list<Tags::Beta, Tags::Gamma>;
      75           0 :   using const_global_cache_tags = tmpl::list<>;
      76           0 :   static void apply(gsl::not_null<Scalar<ComplexDataVector>*> scalar_equation,
      77             :                     const Scalar<ComplexDataVector>& beta,
      78             :                     const tnsr::i<ComplexDataVector, 2>& gamma,
      79             :                     const Scalar<ComplexDataVector>& field,
      80             :                     const tnsr::i<ComplexDataVector, 2>& field_gradient,
      81             :                     const tnsr::I<ComplexDataVector, 2>& flux);
      82             : };
      83             : 
      84             : /*!
      85             :  * \brief Modifies the received boundary data to account for jump conditions.
      86             :  *
      87             :  * \par Worldtube jump conditions
      88             :  * The `apply` method adds or subtracts the singular field to/from
      89             :  * the received data on element boundaries.
      90             :  *
      91             :  * In the regularized region we solve for the regularized field
      92             :  * \begin{equation}
      93             :  *   \Psi_m^R = \Psi_m - \Psi_m^P
      94             :  *   \text{,}
      95             :  * \end{equation}
      96             :  * so we subtract the singular field on the regularized side and add it on the
      97             :  * other side of the boundary. We do the same for the received normal dot flux
      98             :  * $n_i F^i$, but with an extra minus sign because this quantity is defined with
      99             :  * the face normal from the perspective of the sending element (see
     100             :  * `elliptic::protocols::FirstOrderSystem`).
     101             :  *
     102             :  * \par VTU-slicing jump conditions
     103             :  * The `apply_linearized` method imposes the jump conditions at the
     104             :  * interfaces between domains with different slicings (v-t and t-u transitions).
     105             :  * At these interfaces the boost function $H(r_*)$ is discontinuous, which
     106             :  * produces a jump in the radial derivative of $\Psi_m$
     107             :  * [Eqs. (2.36)-(2.37) in \cite Vu:2026ypc ].
     108             :  */
     109           1 : struct ModifyBoundaryData {
     110             :  private:
     111           0 :   static constexpr size_t Dim = 2;
     112           0 :   using singular_vars_on_mortars_tag =
     113             :       ::Tags::Variables<tmpl::list<Tags::SingularField,
     114             :                                    ::Tags::NormalDotFlux<Tags::SingularField>>>;
     115             : 
     116             :  public:
     117           0 :   using argument_tags =
     118             :       tmpl::list<Tags::FieldIsRegularized,
     119             :                  ::Tags::Mortars<Tags::FieldIsRegularized, Dim>,
     120             :                  ::Tags::Mortars<singular_vars_on_mortars_tag, Dim>>;
     121             :  public:
     122           0 :   using argument_tags_linearized = tmpl::list<
     123             :       domain::Tags::Element<Dim>, Tags::NullSlicingBlocks<Dim>,
     124             :       elliptic::Tags::Background<elliptic::analytic_data::Background>>;
     125           0 :   using const_global_cache_tags = tmpl::list<
     126             :       Tags::NullSlicingBlocks<Dim>,
     127             :       elliptic::Tags::Background<elliptic::analytic_data::Background>>;
     128           0 :   static void apply(
     129             :       gsl::not_null<Scalar<ComplexDataVector>*> field,
     130             :       gsl::not_null<Scalar<ComplexDataVector>*> n_dot_flux,
     131             :       const DirectionalId<Dim>& mortar_id, bool field_is_regularized,
     132             :       const DirectionalIdMap<Dim, bool>& neighbors_field_is_regularized,
     133             :       const DirectionalIdMap<Dim, typename singular_vars_on_mortars_tag::type>&
     134             :           singular_vars_on_mortars);
     135           0 :   static void apply_linearized(
     136             :       gsl::not_null<Scalar<ComplexDataVector>*> field_remote,
     137             :       gsl::not_null<Scalar<ComplexDataVector>*> n_dot_flux_remote,
     138             :       const Scalar<ComplexDataVector>& field_local,
     139             :       const Scalar<ComplexDataVector>& n_dot_flux_local,
     140             :       const DirectionalId<Dim>& mortar_id, const Element<Dim>& element,
     141             :       const std::vector<size_t>& null_slicing_blocks,
     142             :       const elliptic::analytic_data::Background& background);
     143             : };
     144             : 
     145             : }  // namespace ScalarSelfForce

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