Disable "hard" examples in CI

[qpms.git] / qpms / scatsystem.h

/*! \file scatsystem.h
 * \brief Modern interface for finite lattice calculations, including symmetries.
 *
 * N.B. Only "reasonably normalised" waves are supported now in most of the
 * functions defined here, i.e. those that can be rotated by the usual
 * Wigner matrices, i.e. the "power" or "spharm" -normalised ones.
 * 
 * TODO FIXME check whether Condon-Shortley phase can have some nasty influence
 * here; I fear that yes.
 */
#ifndef QPMS_SCATSYSTEM_H
#define QPMS_SCATSYSTEM_H
#include "qpms_types.h"
#include "vswf.h"
#include "tmatrices.h"
#include <stdbool.h>

/// Overrides the number of threads spawned by the paralellized functions.
/** TODO MORE DOC which are those? */
void qpms_scatsystem_set_nthreads(long n);

/// A particle, defined by its T-matrix and position.
/** This is rather only an auxillary intermediate structure to ultimately 
 * build an qpms_scatsys_t instance */
typedef struct qpms_particle_t {
        // Does it make sense to ever use other than cartesian coords for this?
        cart3_t pos; ///< Particle position in cartesian coordinates.
        const qpms_tmatrix_function_t *tmg; ///< T-matrix function; not owned by qpms_particle_t.
        qpms_tmatrix_operation_t op; ///< T-matrix transformation operation w.r.t. \a tmg.
} qpms_particle_t;

struct qpms_finite_group_t;
typedef struct qpms_finite_group_t qpms_finite_group_t;

/// A particle, defined by its T-matrix INDEX and position, to be used in qpms_scatsys_t.
typedef struct qpms_particle_tid_t {
        // Does it make sense to ever use other than cartesian coords for this?
        cart3_t pos; ///< Particle position in cartesian coordinates.
        qpms_ss_tmi_t tmatrix_id; ///< T-matrix index
} qpms_particle_tid_t;


typedef qpms_gmi_t qpms_ss_orbit_pi_t; ///< Auxilliary type used in qpms_ss_orbit_type_t for labeling particles inside orbits.
typedef qpms_ss_tmi_t qpms_ss_oti_t; ///< Auxilliary type used for labeling orbit types.

/// Structure describing a particle's "orbit type" under symmetry group actions in a system.
/**
 * Each particle has its orbit with respect to a symmetry group of the system in which the particle lies,
 * i.e. a set of particles onto which the group operations map the original particle.
 * 
 * (TODO DOC improve the following explanation:)
 * Typically, there will be only a small number of different (T-matrix, particle 
 * <a href="https://en.wikipedia.org/wiki/Group_action#Fixed_points_and_stabilizer_subgroups">stabiliser</a>)
 * pairs in the system. We can group the particles accordingly, into the same "orbit types"
 * that will allow to do certain operations only once for each "orbit type", saving memory and (perhaps) time.
 *
 * Each particle will then have assigned:
 *   1. an orbit type,
 *   2. an ID inside that orbit.
 *
 *
 * TODO DOC how the process of assigning the particle IDs actually work, orbit type (non-)uniqueness.
 *
 *
 * Memory is managed by qpms_scatspec_t; qpms_ss_orbit_type_t does not own anything.
 *
 */
typedef struct qpms_ss_orbit_type_t {
        qpms_ss_orbit_pi_t size; ///< Size of the orbit (a divisor of the group order), i.e. number of particles on the orbit.
        size_t bspecn; ///< Individual particle's coefficient vector length. The same as ss->tm[this.tmatrices[0]]->spec->n.
        /// Action of the group elements onto the elements in this orbit.
        /** Its size is sym->order * this.size
         *  and its values lie between 0 and \a this.size − 1.
         *
         *  Action of the group element g onto the pi-th particle
         *  is given by action[g + pi*sym->order].
         *  
         */
        qpms_ss_orbit_pi_t *action;
        /// T-matrix IDs of the particles on this orbit (type).
        /**
         * We save all the tmi's of the particles on the orbit here to make the number of array lookups
         * and pointer dereferences constant.
         *
         * The size of this array is \a size.
         */
        qpms_ss_tmi_t *tmatrices;
        /// Sizes of the per-orbit irrep bases. 
        /**
         * The order of the irreps corresponds to the order in \a ss->sym->irreps.
         * The size of this array is (obviously) \a ss->sym->nirreps.
         *
         * TODO different type? 
         * TODO doc.
         */
        size_t *irbase_sizes;
        //The following are pretty redundant, TODO reduce them at some point.
        /// Cumulative sums of irbase_sizes.
        size_t *irbase_cumsizes;
        /// TODO doc.
        size_t *irbase_offsets;
        /// Per-orbit irreducible representation orthonormal bases.
        /** This also defines the unitary operator that transforms the orbital excitation coefficients
         * in the symmetry-adapted basis.
         *
         * The size is (\a this->size * \a this->tmatrices[0].spec->n)**2.
         *
         * TODO doc.
         */
        complex double *irbases;
        /// TODO doc.
        size_t instance_count;
        /// Cumulative sum of the preceding ot->siza * ot->instance_count;
        qpms_ss_pi_t p_offset;
} qpms_ss_orbit_type_t;


typedef ptrdiff_t qpms_ss_osn_t; ///< "serial number" of av orbit in a given type.

/// Auxillary type used in qpms_scatsys_t that identifies the particle's orbit and its id inside that orbit.
typedef struct qpms_ss_particle_orbitinfo {
        qpms_ss_oti_t t; ///< Orbit type.
#define QPMS_SS_P_ORBITINFO_UNDEF (-1) ///< This labels that the particle has not yet been assigned to an orbit.
        qpms_ss_osn_t osn; ///< "Serial number" of the orbit in the given type. TODO type and more doc.
        qpms_ss_orbit_pi_t p; ///< Order (sija, ei rankki) of the particle inside that orbit type.
} qpms_ss_particle_orbitinfo_t;

/// Auxillary type used in qpms_scatsys_t: A recepy to create another T-matrices by symmetry operations.
typedef struct qpms_ss_derived_tmatrix_t {
        qpms_ss_tmgi_t tmgi; ///< Index of the corresponding qpms_scatsys_t::tm element.
        struct qpms_tmatrix_operation_t op; ///< Operation to derive this particular T-matrix.
} qpms_ss_derived_tmatrix_t;

typedef struct qpms_scatsys_periodic_info_t {   
        /// (Direct) lattice basis of the system (only \a lattice_dimension elements are used)
        /** This is mandatory for \a lattice_dimension != 0 */
        cart3_t lattice_basis[3];

        /// Reciprocal lattice basis. 
        /**(TODO specify whether it includes 2π or not) */
        cart3_t reciprocal_basis[3];

        /// Unitcell volume (irrelevant for non-periodic systems).
        /** The dimensionality of the volume corresponds to lattice_dimension, so
         * for lattice_dimension == 1, this will actually be lenght and for
         * lattice_dimension == 2, a 2D area.
         */
        double unitcell_volume;

        /// Default Ewald parameter \f$ \eta \f$.
        /** Normally, this just gets copied into qpms_scatsys_at_omega_t,
         * which is then used in the Ewald sums.
         * However, for higher frequencies it must be adjusted to avoid
         * numerical instability.
         */
        double eta;
} qpms_scatsys_periodic_info_t;


struct qpms_trans_calculator;
struct qpms_epsmu_generator_t;

/// Common "class" for system of scatterers, both periodic and non-periodic.
/**
 * Infinite periodic structures (those with \a lattice_dimension > 0) 
 * have the \a per filled.
 * These are ignored for finite systems (lattice_dimension == 0).
 */
typedef struct qpms_scatsys_t {
        /// Number of dimensions in which the system is periodic from the range 0–3.
        int lattice_dimension;
        struct qpms_epsmu_generator_t medium; ///< Optical properties of the background medium.
        
        /// (Template) T-matrix functions in the system.
        /** The qpms_abstract_tmatrix_t objects (onto which this array member point)
         *  are NOT owned by this and must be kept alive for the whole lifetime
         *  of all qpms_scatsys_t objects that are built upon them.
         */
        qpms_tmatrix_function_t *tmg; 
        qpms_ss_tmgi_t tmg_count; ///< Number of all different original T-matrix generators in the system.

        /// All the different T-matrix functions in the system, including those derived from \a tmg elements by symmetries.
        qpms_ss_derived_tmatrix_t *tm; 
        qpms_ss_tmi_t tm_count; ///< Number of all different T-matrices in the system (length of tm[]).
        qpms_ss_tmi_t tm_capacity; ///< Capacity of tm[].
        
        qpms_particle_tid_t *p; ///< Particles.
        qpms_ss_pi_t p_count; ///< Size of particles array.
        qpms_ss_pi_t p_capacity; ///< Capacity of p[].

        //TODO the index types do not need to be so big.
        const struct qpms_finite_group_t *sym; ///< Symmetry group of the array
        qpms_ss_pi_t *p_sym_map; ///< Which particles map onto which by the symmetry ops.
        ///< p_sym_map[idi + pi * sym->order] gives the index of pi-th particle under the idi'th sym op.
        qpms_ss_tmi_t *tm_sym_map; ///< Which t-matrices map onto which by the symmetry ops. Lookup by tm_sum_map[idi + tmi * sym->order].

        qpms_ss_oti_t orbit_type_count;
        qpms_ss_orbit_type_t *orbit_types; ///< (Array length is \a orbit_type_count.)

        qpms_ss_particle_orbitinfo_t *p_orbitinfo; ///< Orbit type identification of each particle. (Array length is \a p_count.)

        size_t fecv_size; ///< Number of elements of a full excitation coefficient vector size. 
        size_t *saecv_sizes; ///< Number of elements of symmetry-adjusted coefficient vector sizes (order as in sym->irreps).

        size_t *fecv_pstarts; ///< Indices of where pi'th particle's excitation coeffs start in a full excitation coefficient vector.
        size_t *saecv_ot_offsets; ///< TODO DOC. In the packed vector, saecv_ot_offsets[iri * orbit_type_count + oti] indicates start of ot
        /**< TODO maybe move it to qpms_ss_orbit_type_t, ffs. */
        //size_t **saecv_pstarts; ///< NI. Indices of where pi'th particle's excitation coeff start in a symmetry-adjusted e.c.v.
        ///**< First index is irrep index as in sym->irreps, second index is particle index. */

        // TODO shifted origin of the symmetry group etc.
        // TODO some indices for fast operations here.
        // private
        size_t max_bspecn; ///< Maximum tm[...]->spec->n. Mainly for workspace allocation.
        
        /// Particles grouped by orbit (in the order corresponding to the packed memory layout).
        qpms_ss_pi_t *p_by_orbit;

        // We keep the p_orbitinfo arrays in this chunk in order to avoid memory fragmentation
        char *otspace;
        char *otspace_end;
        double lenscale; // radius of the array, used as a relative tolerance measure
        struct qpms_trans_calculator *c;

        /// Periodic lattice metadata.
        qpms_scatsys_periodic_info_t per;
} qpms_scatsys_t;

/// Retrieve the bspec of \a tmi'th element of \a ss->tm.
static inline const qpms_vswf_set_spec_t *qpms_ss_bspec_tmi(const qpms_scatsys_t *ss, qpms_ss_tmi_t tmi) {
        return ss->tmg[ss->tm[tmi].tmgi].spec;
}

/// Retrieve the bspec of \a pi'th particle in \a ss->p.
static inline const qpms_vswf_set_spec_t *qpms_ss_bspec_pi(const qpms_scatsys_t *ss, qpms_ss_pi_t pi) {
        return ss->tmg[ss->tm[ss->p[pi].tmatrix_id].tmgi].spec;
}

typedef struct qpms_scatsys_at_omega_t {
        const qpms_scatsys_t *ss; ///< Parent scattering system.
        /// T-matrices from \a ss, evaluated at \a omega.
        /** The T-matrices are in the same order as in \a ss,
         * i.e in the order corresponding to \a ss->tm.
         */
        qpms_tmatrix_t **tm;
        complex double omega; ///< Angular frequency
        qpms_epsmu_t medium; ///< Background medium optical properties at the given frequency
        complex double wavenumber; ///< Background medium wave number
} qpms_scatsys_at_omega_t;


/// Creates a new scatsys by applying a symmetry group onto a "proto-scatsys", copying particles if needed.
/** In fact, it copies everything except the vswf set specs and qpms_abstract_tmatrix_t instances,
 * so keep them alive until scatsys is destroyed.
 *  
 *  The following fields must be filled in the "proto- scattering system" \a orig:
 *  * orig->lattice_dimension
 *  * orig->medium – The pointers are copied to the new qpms_scatsys_t instance; 
 *    the target qpms_abstract_tmatrix_t objects must be kept alive before all the resulting 
 *    qpms_scatsys_t instances are properly destroyed.
 *  * orig->tmg – The pointers are copied to the new qpms_scatsys_t instance; 
 *    the target qpms_abstract_tmatrix_t objects must be kept alive before all the resulting 
 *    qpms_scatsys_t instances are properly destroyed. The pointers from orig->tmg, however, are copied.
 *  * orig->tmg_count
 *  * orig->tm – Must be filled, although the operations will typically be identities
 *    (QPMS_TMATRIX_OPERATION_NOOP). N.B. these NOOPs might be replaced with some symmetrisation operation
 *    in the resulting "full" qpms_scatsys_t instance.
 *  * orig->tm_count
 *  * orig->p
 *  * orig->p_count
 *
 *  For periodic systems, the corresponding number of orig->per->lattice_basis[] elements
 *  must be filled as well.
 *
 *  For periodic systems, only trivial group is currently supported. Non-trivial 
 *  groups will cause undefined behaviour.
 *
 *  The resulting qpms_scatsys_t is obtained by actually evaluating the T-matrices
 *  at the given frequency \a omega and where applicable, these are compared
 *  by their values with given tolerances. The T-matrix generators are expected
 *  to preserve the point group symmetries for all frequencies.
 *
 *  This particular function will likely change in the future.
 *
 *  \returns An instance \a sso of qpms_scatsys_omega_t. Note that \a sso->ss
 *  must be saved by the caller before destroying \a sso 
 *  (with qpms_scatsys_at_omega_free(), and destroyed only afterwards with 
 *  qpms_scatsys_free() when not needed anymore.
 *  \a sso->ss can be reused for different frequency by a
 *  qpms_scatsys_at_omega() call.
 *
 */
qpms_scatsys_at_omega_t *qpms_scatsys_apply_symmetry(const qpms_scatsys_t *orig, const struct qpms_finite_group_t *sym,
                complex double omega, const struct qpms_tolerance_spec_t *tol);

/// Destroys the result of qpms_scatsys_apply_symmetry or qpms_scatsys_load.
void qpms_scatsys_free(qpms_scatsys_t *s);

/// Destroys a qpms_scatsys_at_omega_t.
/** Used on results of qpms_scatsys_apply_symmetry() and qpms_scatsys_at_omega(). */
void qpms_scatsys_at_omega_free(qpms_scatsys_at_omega_t *ssw);

/// Evaluates scattering system T-matrices at a given frequency.
/** Free the result using qpms_scatsys_at_omega_free() when done. */
qpms_scatsys_at_omega_t *qpms_scatsys_at_omega(const qpms_scatsys_t *ss,
                complex double omega);

/// Creates a "full" transformation matrix U that takes a full vector and projects it onto an symmetry adapted basis.
/** Mostly as a reference and a debugging tool, as multiplicating these big matrices would be inefficient.
 * 
 * TODO doc about shape etc.
 */
complex double *qpms_scatsys_irrep_transform_matrix(complex double *target_U,
                const qpms_scatsys_t *ss, qpms_iri_t iri);

/// Projects a "big" matrix onto an irrep (slow reference implementation).
/** TODO doc */
complex double *qpms_scatsys_irrep_pack_matrix_stupid(complex double *target_packed,
                const complex double *orig_full, const qpms_scatsys_t *ss,
                qpms_iri_t iri);

/// Transforms a big "packed" matrix into the full basis (slow reference implementation).
/** TODO doc */
complex double *qpms_scatsys_irrep_unpack_matrix_stupid(complex double *target_full,
                const complex double *orig_packed, const qpms_scatsys_t *ss,
                qpms_iri_t iri, bool add);

/// Projects a "big" matrix onto an irrep.
/** TODO doc */
complex double *qpms_scatsys_irrep_pack_matrix(complex double *target_packed,
                const complex double *orig_full, const qpms_scatsys_t *ss,
                qpms_iri_t iri);

/// Transforms a big "packed" matrix into the full basis.
/** TODO doc */
complex double *qpms_scatsys_irrep_unpack_matrix(complex double *target_full,
                const complex double *orig_packed, const qpms_scatsys_t *ss,
                qpms_iri_t iri, bool add);

/// Projects a "big" vector onto an irrep.
/** TODO doc */
complex double *qpms_scatsys_irrep_pack_vector(complex double *target_packed,
                const complex double *orig_full, const qpms_scatsys_t *ss,
                qpms_iri_t iri);

/// Transforms a big "packed" vector into the full basis.
/** TODO doc */
complex double *qpms_scatsys_irrep_unpack_vector(complex double *target_full,
                const complex double *orig_packed, const qpms_scatsys_t *ss,
                qpms_iri_t iri, bool add);

/// Global translation matrix.
/**
 * The diagonal (particle self-) block are filled with zeros (even for regular Bessel waves).
 * This may change in the future.
 */
complex double *qpms_scatsys_build_translation_matrix_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_t *ss,
                complex double k ///< Wave number to use in the translation matrix.
                );

/// Creates the full \f$ (I - WS) \f$ matrix of the periodic scattering system.
/**
 * \returns \a target on success, NULL on error.
 */
complex double *qpms_scatsysw_build_modeproblem_matrix_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_t *ssw
                );

/// As qpms_scatsys_build_translation_full() but with choice of Bessel function type.
/** Might be useful for evaluation of cross sections and testing.
 */
complex double *qpms_scatsys_build_translation_matrix_e_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_t *ss,
                complex double k, ///< Wave number to use in the translation matrix.
                qpms_bessel_t J
                );

/// Global translation matrix with selectable Bessel function, projected on an irrep.
/**
 * The diagonal (particle self-) blocks are currently filled with zeros.
 * This may change in the future.
 */
complex double *qpms_scatsys_build_translation_matrix_e_irrep_packed(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_t *ss,
                qpms_iri_t iri,
                complex double k, ///< Wave number to use in the translation matrix.
                qpms_bessel_t J
                );

/// Creates the mode problem matrix \f$ (I - TS) \f$ directly in the irrep-packed form.
/**
 * \returns \a target on success, NULL on error.
 */
complex double *qpms_scatsysw_build_modeproblem_matrix_irrep_packed(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_t *ssw,
                qpms_iri_t iri ///< Index of the irreducible representation in ssw->ss->sym
                );
/// Alternative implementation of qpms_scatsysw_build_modeproblem_matrix_irrep_packed().
/**
 * \returns \a target on success, NULL on error.
 */
complex double *qpms_scatsysw_build_modeproblem_matrix_irrep_packed_orbitorderR(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_t *ssw,
                qpms_iri_t iri ///< Index of the irreducible representation in ssw->ss->sym
                );
/// Alternative (serial reference) implementation of qpms_scatsysw_build_modeproblem_matrix_irrep_packed().
/**
 * \returns \a target on success, NULL on error.
 */
complex double *qpms_scatsysw_build_modeproblem_matrix_irrep_packed_serial(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_t *ssw,
                qpms_iri_t iri ///< Index of the irreducible representation in ssw->ss->sym
                );

struct qpms_scatsys_at_omega_k_t; // Defined below.
/// LU factorisation (LAPACKE_zgetrf) result holder.
typedef struct qpms_ss_LU {
        const qpms_scatsys_at_omega_t *ssw;
        const struct qpms_scatsys_at_omega_k_t *sswk; ///< Only for periodic systems, otherwise NULL.
        bool full; ///< true if full matrix; false if irrep-packed.
        qpms_iri_t iri; ///< Irrep index if `full == false`.
        /// LU decomposition array.
        complex double *a;
        /// Pivot index array, size at least max(1,min(m, n)).
        int *ipiv; 
} qpms_ss_LU;
void qpms_ss_LU_free(qpms_ss_LU);

/// Builds an LU-factorised mode/scattering problem \f$ (I - TS) \f$ matrix from scratch. Nonperiodic systems only.
qpms_ss_LU qpms_scatsysw_build_modeproblem_matrix_full_LU(
                complex double *target, ///< Pre-allocated target array. Optional (if NULL, new one is allocated).
                int *target_piv, ///< Pre-allocated pivot array. Optional (if NULL, new one is allocated).
                const qpms_scatsys_at_omega_t *ssw
                );

/// Builds an irrep-packed LU-factorised mode/scattering problem matrix from scratch.
qpms_ss_LU qpms_scatsysw_build_modeproblem_matrix_irrep_packed_LU(
                complex double *target, ///< Pre-allocated target array. Optional (if NULL, new one is allocated).
                int *target_piv, ///< Pre-allocated pivot array. Optional (if NULL, new one is allocated).
                const qpms_scatsys_at_omega_t *ssw,
                qpms_iri_t iri
                );

/// Computes LU factorisation of a pre-calculated mode/scattering problem matrix, replacing its contents.
qpms_ss_LU qpms_scatsysw_modeproblem_matrix_full_factorise(
                complex double *modeproblem_matrix_full, ///< Pre-calculated mode problem matrix (I-TS). Mandatory.
                int *target_piv, ///< Pre-allocated pivot array. Optional (if NULL, new one is allocated).
                const qpms_scatsys_at_omega_t *ssw, ///< Must be filled for non-periodic systems.
                const struct qpms_scatsys_at_omega_k_t *sswk ///< Must be filled for periodic systems, otherwise must be NULL.
                );

/// Computes LU factorisation of a pre-calculated irrep-packed mode/scattering problem matrix, replacing its contents.
qpms_ss_LU qpms_scatsysw_modeproblem_matrix_irrep_packed_factorise(
                complex double *modeproblem_matrix_irrep_packed, ///< Pre-calculated mode problem matrix (I-TS). Mandatory.
                int *target_piv, ///< Pre-allocated pivot array. Optional (if NULL, new one is allocated).
                const qpms_scatsys_at_omega_t *ssw,
                qpms_iri_t iri
                );

/// Solves a (possibly partial, irrep-packed) scattering problem \f$ (I-TS)f = Ta_\mathrm{inc} \f$ using a pre-factorised \f$ (I-TS) \f$.
complex double *qpms_scatsys_scatter_solve(
                complex double *target_f, ///< Target (full or irrep-packed, depending on `ludata.full`) array for \a f. If NULL, a new one is allocated.
                const complex double *a_inc, ///< Incident field expansion coefficient vector \a a (full or irrep-packed, depending on `ludata.full`).
                qpms_ss_LU ludata ///< Pre-factorised \f$ I - TS \f$ matrix data.
                );

// ======================= Periodic system -only related stuff =============================

/// Scattering system at a given frequency and k-vector. Used only with periodic systems.
/**
 * N.B. use as a stack variable now, but this might become heap-allocated in the future (with own con- and destructor)
 */
typedef struct qpms_scatsys_at_omega_k_t {
        const qpms_scatsys_at_omega_t *ssw;
        double k[3]; ///< The k-vector's cartesian coordinates.
        double eta; ///< Ewald parameter η.
} qpms_scatsys_at_omega_k_t;

/// Creates the full \f$ (I - WS) \f$ matrix of the periodic scattering system. 
/**
 * \returns \a target on success, NULL on error.
 */
complex double *qpms_scatsyswk_build_modeproblem_matrix_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_k_t *sswk
                );

/// Global translation matrix.
complex double *qpms_scatsys_periodic_build_translation_matrix_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_t *ss,
                complex double wavenumber, ///< Wave number to use in the translation matrix.
                const cart3_t *wavevector, ///< Wavevector / pseudomomentum in cartesian coordinates.
                double eta ///< Ewald parameter eta. Pass 0 or NaN to use the default value in \a ss.
                );

/// Global translation matrix. 
complex double *qpms_scatsyswk_build_translation_matrix_full(
                /// Target memory with capacity for ss->fecv_size**2 elements. If NULL, new will be allocated.
                complex double *target,
                const qpms_scatsys_at_omega_k_t *sswk
                );


/// Builds an LU-factorised mode/scattering problem \f$ (I - TS) \f$ matrix from scratch. Periodic systems only.
qpms_ss_LU qpms_scatsyswk_build_modeproblem_matrix_full_LU(
                complex double *target, ///< Pre-allocated target array. Optional (if NULL, new one is allocated).
                int *target_piv, ///< Pre-allocated pivot array. Optional (if NULL, new one is allocated).
                const qpms_scatsys_at_omega_k_t *sswk
                );

/// Searches for periodic scattering system's eigenmodes using Beyn's algorithm.
/**
 * Currently, elliptical contour is used.
 *
 * TODO In the future, this will probably support irrep decomposition as well,
 * but for the case of periodic / small systems,
 * the bottleneck is the T-matrix and translation matrix evaluation
 * rather than the linear algebra.
 */
struct beyn_result_t *qpms_scatsys_periodic_find_eigenmodes(
                const qpms_scatsys_t *ss, 
                /// Wavevector in cartesian coordinates (must lie in the lattice plane).
                const double k[3],
                complex double omega_centre, ///< Center of the ellipse inside which the eigenfreqs are searched for.
                double omega_rr, ///< Real half-axis of the ellipse inside which the eigenfreqs are searched for.
                double omega_ri, ///< Imaginary half-axis of the ellipse inside which the eigenfreqs are searched for.
                size_t contour_npoints, ///< Number of elliptic contour discretisation points (preferably even number)
                double rank_tol, ///< (default: `1e-4`) TODO DOC.
                size_t rank_sel_min, ///< Minimum number of eigenvalue candidates, even if they don't pass \a rank_tol.
                double res_tol ///< (default: `0.0`) TODO DOC.
                );

// ======================= Periodic system -only related stuff end =========================


/// NOT IMPLEMENTED Dumps a qpms_scatsys_t structure to a file.
qpms_errno_t qpms_scatsys_dump(qpms_scatsys_t *ss, char *path);

/// NOT IMPLEMENTED Reads a qpms_scatsys_t structure from a file.
qpms_scatsys_t *qpms_scatsys_load(char *path);

struct qpms_finite_group_t;

/// Constructs a "full matrix action" of a point group element for an orbit type.
/** TODO detailed doc */
complex double *qpms_orbit_action_matrix(
                /// Target array. If NULL, a new one is allocated.
                /** The size of the array is (orbit->size * bspec->n)**2
                 * (it makes sense to assume all the T-matrices share their spec).
                 */
                complex double *target,
                /// The orbit (type).
                const qpms_ss_orbit_type_t *orbit,
                /// Base spec of the t-matrices (we don't know it from orbit, as it has 
                /// only T-matrix indices.
                const qpms_vswf_set_spec_t *bspec,
                /// The symmetry group used to generate the orbit (must have rep3d filled).
                const struct qpms_finite_group_t *sym,
                /// The index of the operation in sym to represent.
                const qpms_gmi_t g);

/// Constructs a dense matrix representation of a irrep projector for an orbit type.
/** TODO detailed doc */
complex double *qpms_orbit_irrep_projector_matrix(
                /// Target array. If NULL, a new one is allocated.
                /** The size of the array is (orbit->size * bspec->n)**2
                 * (it makes sense to assume all the T-matrices share their spec).
                 */
                complex double *target,
                /// The orbit (type).
                const qpms_ss_orbit_type_t *orbit,
                /// Base spec of the t-matrices (we don't know it from orbit, as it has 
                /// only T-matrix indices.
                const qpms_vswf_set_spec_t *bspec,
                /// The symmetry group used to generate the orbit (must have rep3d filled).
                const struct qpms_finite_group_t *sym,
                /// The index of the irreducible representation of sym.
                const qpms_iri_t iri);

/// TODO DOC!!!!!
complex double *qpms_orbit_irrep_basis(
                /// Here theh size of theh basis shall be saved,
                size_t *basis_size,
                /// Target array. If NULL, a new one is allocated.
                /** The size of the array is basis_size * (orbit->size * bspec->n)
                 * (it makes sense to assume all the T-matrices share their spec).
                 */
                complex double *target,
                /// The orbit (type).
                const qpms_ss_orbit_type_t *orbit,
                /// Base spec of the t-matrices (we don't know it from orbit, as it has 
                /// only T-matrix indices.
                const qpms_vswf_set_spec_t *bspec,
                /// The symmetry group used to generate the orbit (must have rep3d filled).
                const struct qpms_finite_group_t *sym,
                /// The index of the irreducible representation of sym.
                const qpms_iri_t iri);


/// Creates an incident field vector in the full basis, given a function that evaluates the field expansions at points.
/** TODO detailed doc!
 * \returns target_full if target_full was not NULL, otherwise the newly allocated array. */
complex double *qpms_scatsys_incident_field_vector_full(
                /// Target array. If NULL, a new one is allocated.
                /** The length of the array is ss->fecv_size. */
                complex double *target_full,
                const qpms_scatsys_t *ss,
                qpms_incfield_t field_at_point,
                const void *args, ///< Pointer passed as the last argument to (*field_at_point)()
                bool add ///< If true, add to target_full; rewrite target_full if false.
                );

/// Applies T-matrices onto an incident field vector in the full basis.
complex double *qpms_scatsysw_apply_Tmatrices_full(
                complex double *target_full, /// Target vector array. If NULL, a new one is allocated.
                const complex double *inc_full, /// Incident field coefficient vector. Must not be NULL.
                const qpms_scatsys_at_omega_t *ssw
                );

struct beyn_result_t; // See beyn.h for full definition

/// Searches for finite scattering system's eigenmodes using Beyn's algorithm.
/**
 * Currently, elliptical contour is used.
 *
 * TODO In the future, this will probably support irrep decomposition as well,
 * but it does not make much sense for periodic / small systems, as in their
 * case the bottleneck is the T-matrix and translation matrix evaluation
 * rather than the linear algebra.
 */
struct beyn_result_t *qpms_scatsys_finite_find_eigenmodes(
                const qpms_scatsys_t *ss, 
                /// A valid irrep index to search only in one irrep, or QPMS_NO_IRREP for solving the full system.
                qpms_iri_t iri,
                complex double omega_centre, ///< Center of the ellipse inside which the eigenfreqs are searched for.
                double omega_rr, ///< Real half-axis of the ellipse inside which the eigenfreqs are searched for.
                double omega_ri, ///< Imaginary half-axis of the ellipse inside which the eigenfreqs are searched for.
                size_t contour_npoints, ///< Number of elliptic contour discretisation points (preferably even number)
                double rank_tol, ///< (default: `1e-4`) TODO DOC.
                size_t rank_sel_min, ///< Minimum number of eigenvalue candidates, even if they don't pass \a rank_tol.
                double res_tol ///< (default: `0.0`) TODO DOC.
                );

#if 0
/// Searches for scattering system's eigenmodes using Beyn's algorithm.
/**
 * Currently, elliptical contour is used.
 *
 * TODO In the future, this will probably support irrep decomposition as well,
 * but it does not make much sense for periodic / small systems, as in their
 * case the bottleneck is the T-matrix and translation matrix evaluation
 * rather than the linear algebra.
 */
struct beyn_result_t *qpms_scatsys_find_eigenmodes(
                const qpms_scatsys_t *ss,
                double eta, ///< Ewald sum parameter
                const double *beta_, ///< k-vector of corresponding dimensionality, NULL/ignored for finite system.
                complex double omega_centre, ///< Center of the ellipse inside which the eigenfreqs are searched for.
                double omega_rr, ///< Real half-axis of the ellipse inside which the eigenfreqs are searched for.
                double omega_ri, ///< Imaginary half-axis of the ellipse inside which the eigenfreqs are searched for.
                size_t contour_npoints, ///< Number of elliptic contour discretisation points (preferably even number)
                double rank_tol, ///< (default: `1e-4`) TODO DOC.
                size_t rank_sel_min, ///< Minimum number of eigenvalue candidates, even if they don't pass \a rank_tol.
                double res_tol ///< (default: `0.0`) TODO DOC.
                );
#endif


#if 0
/// Creates a (partial) incident field vector in the symmetry-adapted basis, given a function that evaluates the field expansions at points.
/** TODO detailed doc! */
complex double *qpms_scatsys_incident_field_vector_irrep_packed(
                /// Target array. If NULL, a new one is allocated.
                /** The length of the array is ss->fecv_size. */
                complex double *target_full,
                const qpms_scatsys_t *ss,
                const qpms_iri_t iri, ///< The index of given irreducible representation of ss->sym.
                qpms_incfield_t field_at_point,
                const void *args, ///< Pointer passed as the last argument to (*field_at_point)()
                bool add ///< If true, add to target_full; rewrite target_full if false.
                );
#endif

/// Evaluates scattered electric field at a point, given a full vector of scattered field coefficients.
/**
 * This function evaluates the field \f$ \vect E (\vect r ) \f$, with any given wavenumber of the
 * background medium and any given vector of the excitation coefficients \f$ \wckcout \f$.
 *
 * \return Complex electric field at the point defined by \a evalpoint.
 * 
 * \see qpms_scatsysw_scattered_E()
 *
 * \see qpms_scatsyswk_scattered_E() for periodic systems.
 *
 * 
 */
ccart3_t qpms_scatsys_scattered_E(
                const qpms_scatsys_t *ss,
                qpms_bessel_t typ, ///< Bessel function kind to use (for scattered fields, use QPMS_HANKEL_PLUS).
                complex double wavenumber, ///< Wavenumber of the background medium.
                const complex double *scatcoeff_full, ///< Full vector of the scattered field coefficients \f$ \wckcout \f$.
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the field is evaluated.
                );

/// Evaluates scattered electric field at a point, given a full vector of scattered field coefficients.
/**
 * This function evaluates the field \f$ \vect E (\vect r ) \f$, with any 
 * given vector of the excitation coefficients \f$ \wckcout \f$.
 *
 * \return Complex electric field at the point defined by \a evalpoint.
 * 
 * \see qpms_scatsys_scattered_E()
 *
 * \see qpms_scatsyswk_scattered_E() for periodic systems.
 */
ccart3_t qpms_scatsysw_scattered_E(
                const qpms_scatsys_at_omega_t *ssw,
                qpms_bessel_t typ, ///< Bessel function kind to use (for scattered fields, use QPMS_HANKEL_PLUS).
                const complex double *scatcoeff_full, ///< Full vector of the scattered field coefficients \f$ \wckcout \f$.
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the field is evaluated.
                );

/// Evaluates scattered electric field at a point, given a full vector of scattered field coefficients.
/**
 * This is an alternative implementation of qpms_scatsys_scattered_E(), and should give the same results
 * up to rounding errors.
 *
 * \return Complex electric field at the point defined by \a evalpoint.
 *
 * \see qpms_scatsys_scattered_E()
 */
ccart3_t qpms_scatsys_scattered_E__alt(
                const qpms_scatsys_t *ss,
                qpms_bessel_t typ, ///< Bessel function kind to use (for scattered fields, use QPMS_HANKEL_PLUS).
                complex double wavenumber, ///< Wavenumber of the background medium.
                const complex double *scatcoeff_full, ///< Full vector of the scattered field coefficients \f$ \wckcout \f$.
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the field is evaluated.
                );

/// Evaluates scattered electric field at a point, given a full vector of scattered field coefficients.
/**
 * This is an alternative implementation of qpms_scatsys_scattered_E(), and should give the same results
 * up to rounding errors.
 *
 * \return Complex electric field at the point defined by \a evalpoint.
 *
 * \see qpms_scatsysw_scattered_E()
 */
ccart3_t qpms_scatsysw_scattered_E__alt(
                const qpms_scatsys_at_omega_t *ssw,
                qpms_bessel_t typ, ///< Bessel function kind to use (for scattered fields, use QPMS_HANKEL_PLUS).
                const complex double *scatcoeff_full, ///< Full vector of the scattered field coefficients \f$ \wckcout \f$.
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the field is evaluated.
                );


/// Evaluates scattered electric field at a point, given a full vector of scattered field coefficients. (Periodic system.)
/**
 * This function evaluates the field \f$ \vect E (\vect r ) \f$, with any 
 * given vector of the excitation coefficients \f$ \wckcout \f$.
 *
 * \return Complex electric field at the point defined by \a evalpoint.
 *
 * \bug Currently implemented only for btyp == QPMS_HANKEL_PLUS.
 *
 * \see qpms_scatsys_scattered_E(), qpms_scatsysw_scattered_E() for finite systems.
 */
ccart3_t qpms_scatsyswk_scattered_E(
                const qpms_scatsys_at_omega_k_t *sswk,
                qpms_bessel_t typ, ///< Bessel function kind to use (only QPMS_HANKEL_PLUS is currently supported).
                const complex double *scatcoeff_full, ///< Full vector of the scattered field coefficients \f$ \wckcout \f$.
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the field is evaluated.
                );

/// Evaluates "scattered" field basis functions in a periodic system.
/**
 *
 * \see qpms_uvswf_fill() evaluates a set of VSWF basis functions (for finite systems).
 */
qpms_errno_t qpms_scatsyswk_scattered_field_basis(
                ccart3_t *target, ///< Target array of size sswk->ssw->ss->fecv_size
                const qpms_scatsys_at_omega_k_t *sswk,
                qpms_bessel_t typ, ///< Bessel function kind to use (only QPMS_HANKEL_PLUS is currently supponted).
                cart3_t evalpoint ///< A point \f$ \vect r \f$, at which the basis is evaluated.
                );


/// Adjusted Ewadl parameter to avoid high-frequency breakdown.
// TODO DOC
double qpms_ss_adjusted_eta(const qpms_scatsys_t *ss, complex double wavenumber, const double wavevector[3]);

#if 0
/** Evaluates partial scattered fields (corresponding to a given irrep-reduced excitation vector)
 * at a given point.
 *
 * \return Complex electric field at the point defined by \a where.
 */
ccart3_t qpms_scatsys_scattered_E_irrep(const qpms_scatsys_t *ss,
                qpms_iri_t iri, ///< Irreducible representation
                const complex double *coeff_vector, ///< A reduced excitation vector, corresponding to \a iri.
                cart3_t where, ///< Evaluation point.
                complex double k ///< Wave number.
                );
#endif

#endif //QPMS_SCATSYSTEM_H