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// ---------------------------------------------------------------------
//
// Copyright (C) 2001 - 2015 by the deal.II authors
//
// This file is part of the deal.II library.
//
// The deal.II library is free software; you can use it, redistribute
// it, and/or modify it under the terms of the GNU Lesser General
// Public License as published by the Free Software Foundation; either
// version 2.1 of the License, or (at your option) any later version.
// The full text of the license can be found in the file LICENSE at
// the top level of the deal.II distribution.
//
// ---------------------------------------------------------------------

#ifndef dealii__fe_dgq_h
#define dealii__fe_dgq_h

#include <deal.II/base/config.h>
#include <deal.II/base/tensor_product_polynomials.h>
#include <deal.II/base/thread_management.h>
#include <deal.II/fe/fe_poly.h>

DEAL_II_NAMESPACE_OPEN

template <int dim, int spacedim> class MappingQ;
template <int dim> class Quadrature;

/*!@addtogroup fe */
/*@{*/

/**
 * Implementation of scalar, discontinuous tensor product elements based on
 * equidistant support points.
 *
 * This is a discontinuous finite element based on tensor products of
 * Lagrangian polynomials. The shape functions are Lagrangian interpolants of
 * an equidistant grid of points on the unit cell. The points are numbered in
 * lexicographical order, with <i>x</i> running fastest, then <i>y</i>, then
 * <i>z</i> (if these coordinates are present for a given space dimension at
 * all). For example, these are the node orderings for <tt>FE_DGQ(1)</tt> in
 * 3d:
 *  @verbatim
 *         6-------7        6-------7
 *        /|       |       /       /|
 *       / |       |      /       / |
 *      /  |       |     /       /  |
 *     4   |       |    4-------5   |
 *     |   2-------3    |       |   3
 *     |  /       /     |       |  /
 *     | /       /      |       | /
 *     |/       /       |       |/
 *     0-------1        0-------1
 *  @endverbatim
 * and <tt>FE_DGQ(2)</tt>:
 *  @verbatim
 *         24--25--26       24--25--26
 *        /|       |       /       /|
 *      21 |       |     21  22  23 |
 *      /  15  16  17    /       /  17
 *    18   |       |   18--19--20   |
 *     |12 6---7---8    |       |14 8
 *     9  /       /     9  10  11  /
 *     | 3   4   5      |       | 5
 *     |/       /       |       |/
 *     0---1---2        0---1---2
 *  @endverbatim
 * with node 13 being placed in the interior of the hex.
 *
 * Note, however, that these are just the Lagrange interpolation points of the
 * shape functions. Even though they may physically be on the boundary of the
 * cell, they are logically in the interior since there are no continuity
 * requirements for these shape functions across cell boundaries. While
 * discontinuous, when restricted to a single cell the shape functions of this
 * element are exactly the same as those of the FE_Q element where they are
 * shown visually.
 *
 * @author Ralf Hartmann, Guido Kanschat 2001, 2004
 */
template <int dim, int spacedim=dim>
class FE_DGQ : public FE_Poly<TensorProductPolynomials<dim>, dim, spacedim>
{
public:
  /**
   * Constructor for tensor product polynomials of degree <tt>p</tt>. The
   * shape functions created using this constructor correspond to Lagrange
   * interpolation polynomials for equidistantly spaced support points in each
   * coordinate direction.
   */
  FE_DGQ (const unsigned int p);

  /**
   * Return a string that uniquely identifies a finite element. This class
   * returns <tt>FE_DGQ<dim>(degree)</tt>, with <tt>dim</tt> and
   * <tt>degree</tt> replaced by appropriate values.
   */
  virtual std::string get_name () const;

  /**
   * Return the matrix interpolating from the given finite element to the
   * present one. The size of the matrix is then @p dofs_per_cell times
   * <tt>source.dofs_per_cell</tt>.
   *
   * These matrices are only available if the source element is also a @p
   * FE_DGQ element. Otherwise, an exception of type
   * FiniteElement<dim>::ExcInterpolationNotImplemented is thrown.
   */
  virtual void
  get_interpolation_matrix (const FiniteElement<dim, spacedim> &source,
                            FullMatrix<double>           &matrix) const;

  /**
   * Return the matrix interpolating from a face of of one element to the face
   * of the neighboring element. The size of the matrix is then
   * <tt>source.dofs_per_face</tt> times <tt>this->dofs_per_face</tt>.
   *
   * Derived elements will have to implement this function. They may only
   * provide interpolation matrices for certain source finite elements, for
   * example those from the same family. If they don't implement interpolation
   * from a given element, then they must throw an exception of type
   * FiniteElement<dim>::ExcInterpolationNotImplemented.
   */
  virtual void
  get_face_interpolation_matrix (const FiniteElement<dim, spacedim> &source,
                                 FullMatrix<double>       &matrix) const;

  /**
   * Return the matrix interpolating from a face of of one element to the face
   * of the neighboring element. The size of the matrix is then
   * <tt>source.dofs_per_face</tt> times <tt>this->dofs_per_face</tt>.
   *
   * Derived elements will have to implement this function. They may only
   * provide interpolation matrices for certain source finite elements, for
   * example those from the same family. If they don't implement interpolation
   * from a given element, then they must throw an exception of type
   * FiniteElement<dim>::ExcInterpolationNotImplemented.
   */
  virtual void
  get_subface_interpolation_matrix (const FiniteElement<dim, spacedim> &source,
                                    const unsigned int        subface,
                                    FullMatrix<double>       &matrix) const;

  /**
   * Projection from a fine grid space onto a coarse grid space. Overrides the
   * respective method in FiniteElement, implementing lazy evaluation
   * (initialize when requested).
   *
   * If this projection operator is associated with a matrix @p P, then the
   * restriction of this matrix @p P_i to a single child cell is returned
   * here.
   *
   * The matrix @p P is the concatenation or the sum of the cell matrices @p
   * P_i, depending on the #restriction_is_additive_flags. This distinguishes
   * interpolation (concatenation) and projection with respect to scalar
   * products (summation).
   *
   * Row and column indices are related to coarse grid and fine grid spaces,
   * respectively, consistent with the definition of the associated operator.
   */
  virtual const FullMatrix<double> &
  get_restriction_matrix (const unsigned int child,
                          const RefinementCase<dim> &refinement_case=RefinementCase<dim>::isotropic_refinement) const;

  /**
   * Embedding matrix between grids. Overrides the respective method in
   * FiniteElement, implementing lazy evaluation (initialize when queried).
   *
   * The identity operator from a coarse grid space into a fine grid space is
   * associated with a matrix @p P. The restriction of this matrix @p P_i to a
   * single child cell is returned here.
   *
   * The matrix @p P is the concatenation, not the sum of the cell matrices @p
   * P_i. That is, if the same non-zero entry <tt>j,k</tt> exists in in two
   * different child matrices @p P_i, the value should be the same in both
   * matrices and it is copied into the matrix @p P only once.
   *
   * Row and column indices are related to fine grid and coarse grid spaces,
   * respectively, consistent with the definition of the associated operator.
   *
   * These matrices are used by routines assembling the prolongation matrix
   * for multi-level methods.  Upon assembling the transfer matrix between
   * cells using this matrix array, zero elements in the prolongation matrix
   * are discarded and will not fill up the transfer matrix.
   */
  virtual const FullMatrix<double> &
  get_prolongation_matrix (const unsigned int child,
                           const RefinementCase<dim> &refinement_case=RefinementCase<dim>::isotropic_refinement) const;

  /**
   * @name Functions to support hp
   * @{
   */

  /**
   * If, on a vertex, several finite elements are active, the hp code first
   * assigns the degrees of freedom of each of these FEs different global
   * indices. It then calls this function to find out which of them should get
   * identical values, and consequently can receive the same global DoF index.
   * This function therefore returns a list of identities between DoFs of the
   * present finite element object with the DoFs of @p fe_other, which is a
   * reference to a finite element object representing one of the other finite
   * elements active on this particular vertex. The function computes which of
   * the degrees of freedom of the two finite element objects are equivalent,
   * both numbered between zero and the corresponding value of dofs_per_vertex
   * of the two finite elements. The first index of each pair denotes one of
   * the vertex dofs of the present element, whereas the second is the
   * corresponding index of the other finite element.
   *
   * This being a discontinuous element, the set of such constraints is of
   * course empty.
   */
  virtual
  std::vector<std::pair<unsigned int, unsigned int> >
  hp_vertex_dof_identities (const FiniteElement<dim, spacedim> &fe_other) const;

  /**
   * Same as hp_vertex_dof_indices(), except that the function treats degrees
   * of freedom on lines.
   *
   * This being a discontinuous element, the set of such constraints is of
   * course empty.
   */
  virtual
  std::vector<std::pair<unsigned int, unsigned int> >
  hp_line_dof_identities (const FiniteElement<dim, spacedim> &fe_other) const;

  /**
   * Same as hp_vertex_dof_indices(), except that the function treats degrees
   * of freedom on quads.
   *
   * This being a discontinuous element, the set of such constraints is of
   * course empty.
   */
  virtual
  std::vector<std::pair<unsigned int, unsigned int> >
  hp_quad_dof_identities (const FiniteElement<dim, spacedim> &fe_other) const;

  /**
   * Return whether this element implements its hanging node constraints in
   * the new way, which has to be used to make elements "hp compatible".
   *
   * For the FE_DGQ class the result is always true (independent of the degree
   * of the element), as it has no hanging nodes (being a discontinuous
   * element).
   */
  virtual bool hp_constraints_are_implemented () const;

  /**
   * Return whether this element dominates the one given as argument when they
   * meet at a common face, whether it is the other way around, whether
   * neither dominates, or if either could dominate.
   *
   * For a definition of domination, see FiniteElementBase::Domination and in
   * particular the
   * @ref hp_paper "hp paper".
   */
  virtual
  FiniteElementDomination::Domination
  compare_for_face_domination (const FiniteElement<dim, spacedim> &fe_other) const;

  /**
   * @}
   */

  /**
   * This function returns @p true, if the shape function @p shape_index has
   * non-zero function values somewhere on the face @p face_index.
   */
  virtual bool has_support_on_face (const unsigned int shape_index,
                                    const unsigned int face_index) const;

  /**
   * Returns a list of constant modes of the element. For this element, it
   * simply returns one row with all entries set to true.
   */
  virtual std::pair<Table<2,bool>, std::vector<unsigned int> >
  get_constant_modes () const;

  /**
   * Determine an estimate for the memory consumption (in bytes) of this
   * object.
   *
   * This function is made virtual, since finite element objects are usually
   * accessed through pointers to their base class, rather than the class
   * itself.
   */
  virtual std::size_t memory_consumption () const;


protected:
  /**
   * Constructor for tensor product polynomials based on Polynomials::Lagrange
   * interpolation of the support points in the quadrature rule
   * <tt>points</tt>. The degree of these polynomials is
   * <tt>points.size()-1</tt>.
   *
   * Note: The FE_DGQ::clone function does not work properly for FE with
   * arbitrary nodes!
   */
  FE_DGQ (const Quadrature<1> &points);

  /**
   * @p clone function instead of a copy constructor.
   *
   * This function is needed by the constructors of @p FESystem.
   */
  virtual FiniteElement<dim, spacedim> *clone() const;

private:
  /**
   * Only for internal use. Its full name is @p get_dofs_per_object_vector
   * function and it creates the @p dofs_per_object vector that is needed
   * within the constructor to be passed to the constructor of @p
   * FiniteElementData.
   */
  static std::vector<unsigned int> get_dpo_vector (const unsigned int degree);

  /**
   * Compute renumbering for rotation of degrees of freedom.
   *
   * Rotates a tensor product numbering of degrees of freedom by 90 degrees.
   * It is used to compute the transfer matrices of the children by using only
   * the matrix for the first child.
   *
   * The direction parameter determines the type of rotation. It is one
   * character of @p xXyYzZ. The character determines the axis of rotation,
   * case determines the direction. Lower case is counter-clockwise seen in
   * direction of the axis.
   *
   * Since rotation around the y-axis is not used, it is not implemented
   * either.
   */
  void rotate_indices (std::vector<unsigned int> &indices,
                       const char                 direction) const;

  /*
   * Mutex for protecting initialization of restriction and embedding matrix.
   */
  mutable Threads::Mutex mutex;

  /**
   * Allow access from other dimensions.
   */
  template <int dim1, int spacedim1> friend class FE_DGQ;

  /**
   * Allows @p MappingQ class to access to build_renumbering function.
   */
  template <int dim1, int spacedim1> friend class MappingQ;
};



/**
 * Implementation of scalar, discontinuous tensor product elements based on
 * Lagrange polynomials with arbitrary nodes. The primary purpose of this
 * class is to provide an element for which the mass matrix can be made
 * diagonal by choosing basis functions that are not either zero or one at the
 * vertices of the cell, but instead are zero or one at a given set of
 * quadrature points. If this set of quadrature points is then also used in
 * integrating the mass matrix, then it will be diagonal. The number of
 * quadrature points automatically determines the polynomial degree chosen for
 * this element.
 *
 * See the base class documentation in FE_DGQ for details.
 *
 * @author F. Prill 2006
 */
template <int dim,int spacedim=dim>
class FE_DGQArbitraryNodes : public FE_DGQ<dim,spacedim>
{
public:
  /**
   * Constructor for tensor product polynomials based on Polynomials::Lagrange
   * interpolation of the support points in the quadrature rule
   * <tt>points</tt>. The degree of these polynomials is
   * <tt>points.size()-1</tt>.
   */
  FE_DGQArbitraryNodes (const Quadrature<1> &points);

  /**
   * Return a string that uniquely identifies a finite element. This class
   * returns <tt>FE_DGQArbitraryNodes<dim>(degree)</tt>, with <tt>dim</tt> and
   * <tt>degree</tt> replaced by appropriate values.
   */
  virtual std::string get_name () const;

protected:
  /**
   * @p clone function instead of a copy constructor.
   *
   * This function is needed by the constructors of @p FESystem.
   */
  virtual FiniteElement<dim,spacedim> *clone() const;
};


/*@}*/

DEAL_II_NAMESPACE_CLOSE

#endif