Separate Ewald parameter for different frequencies
Former-commit-id: 0b9129fda0224411c2a1d8372fe715db4e071ecd
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@ -568,7 +568,10 @@ cdef class ScatteringSystem:
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return None
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property eta:
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"""Ewald parameter η"""
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"""Ewald parameter η (only relevant for periodic systems)
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This is the default value that will be copied into
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_ScatteringSystemAtOmega by __call__"""
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def __get__(self):
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self.check_s()
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if self.lattice_dimension:
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@ -723,7 +726,7 @@ cdef class ScatteringSystem:
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self.s, iri, 0)
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return target_np
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def translation_matrix_full(self, cdouble wavenumber, blochvector = None, J = QPMS_HANKEL_PLUS):
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def translation_matrix_full(self, cdouble wavenumber, blochvector = None, J = QPMS_HANKEL_PLUS, double eta = 0):
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"""Constructs full translation matrix of a scattering system.
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This method enables to use any wave number for the background medium ignoring the
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@ -742,6 +745,11 @@ cdef class ScatteringSystem:
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Optionally, one can replace Hankel functions of the first kind with different
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Bessel functions.
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eta : float
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Ewald parameter η, only relevant for periodic lattices;
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if set to 0 (default), the actual value is determined
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automatically.
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See Also
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--------
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ScatteringSystemAtOmega.translation_matrix_full : Translation matrix at a given frequency.
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@ -763,7 +771,7 @@ cdef class ScatteringSystem:
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raise NotImplementedError("Translation operators based on other than Hankel+ functions not supperted in periodic systems")
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blochvector_c = {'x': blochvector[0], 'y': blochvector[1], 'z': blochvector[2]}
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with pgsl_ignore_error(15):
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qpms_scatsys_periodic_build_translation_matrix_full(&target_view[0][0], self.s, wavenumber, &blochvector_c)
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qpms_scatsys_periodic_build_translation_matrix_full(&target_view[0][0], self.s, wavenumber, &blochvector_c, eta)
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return target
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def translation_matrix_packed(self, cdouble wavenumber, qpms_iri_t iri, J = QPMS_HANKEL_PLUS):
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@ -1025,6 +1033,20 @@ cdef class _ScatteringSystemAtOmega:
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def __get__(self): return self.ss_pyref.nirreps
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property wavenumber:
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def __get__(self): return self.ssw[0].wavenumber
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property eta:
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"""Ewald parameter η (only relevant for periodic systems)"""
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def __get__(self):
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self.check_s()
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if self.lattice_dimension:
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return self.ssw[0].eta
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else:
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return None
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def __set__(self, double eta):
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self.check_s()
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if self.lattice_dimension:
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self.ssw[0].eta = eta
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else:
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raise AttributeError("Cannot set Ewald parameter for finite system") # different exception?
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def modeproblem_matrix_full(self, k=None):
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@ -630,6 +630,7 @@ cdef extern from "scatsystem.h":
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cdouble omega
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qpms_epsmu_t medium
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cdouble wavenumber
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double eta
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qpms_scatsys_at_omega_t *qpms_scatsys_apply_symmetry(const qpms_scatsys_t *orig, const qpms_finite_group_t *sym,
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cdouble omega, const qpms_tolerance_spec_t *tol)
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qpms_scatsys_at_omega_t *qpms_scatsys_at_omega(const qpms_scatsys_t *ss, cdouble omega)
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@ -688,7 +689,7 @@ cdef extern from "scatsystem.h":
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const qpms_scatsys_at_omega_t *ssw
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double k[3]
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cdouble *qpms_scatsyswk_build_modeproblem_matrix_full(cdouble *target, const qpms_scatsys_at_omega_k_t *sswk)
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cdouble *qpms_scatsys_periodic_build_translation_matrix_full(cdouble *target, const qpms_scatsys_t *ss, cdouble wavenumber, const cart3_t *wavevector)
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cdouble *qpms_scatsys_periodic_build_translation_matrix_full(cdouble *target, const qpms_scatsys_t *ss, cdouble wavenumber, const cart3_t *wavevector, double eta)
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qpms_ss_LU qpms_scatsyswk_build_modeproblem_matrix_full_LU(cdouble *target, int *target_piv, const qpms_scatsys_at_omega_k_t *sswk)
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beyn_result_t *qpms_scatsys_periodic_find_eigenmodes(const qpms_scatsys_t *ss, const double *k,
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cdouble omega_centre, double omega_rr, double omega_ri, size_t contour_npoints,
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@ -59,6 +59,13 @@ static inline void qpms_ss_ensure_nonperiodic_a(const qpms_scatsys_t *ss, const
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QPMS_ENSURE(ss->lattice_dimension == 0, "This method is applicable only to nonperiodic systems. Use %s instead.", s);
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}
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// Adjust Ewald parameter to avoid high-frequency breakdown;
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// TODO make this actually do something (other than just copying ss's eta.)
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static inline double ss_adjusted_eta(const qpms_scatsys_t *ss, complex double omega) {
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qpms_ss_ensure_periodic(ss);
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return ss->per.eta;
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}
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// ------------ Stupid implementation of qpms_scatsys_apply_symmetry() -------------
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#define MIN(x,y) (((x)<(y))?(x):(y))
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@ -541,6 +548,9 @@ qpms_scatsys_at_omega_t *qpms_scatsys_apply_symmetry(const qpms_scatsys_t *orig,
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}
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ss->c = qpms_trans_calculator_init(lMax, normalisation);
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ssw->eta = ss->lattice_dimension ? ss_adjusted_eta(ss, omega) : NAN;
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return ssw;
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}
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@ -594,6 +604,7 @@ qpms_scatsys_at_omega_t *qpms_scatsys_at_omega(const qpms_scatsys_t *ss,
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ssw->ss = ss;
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ssw->medium = qpms_epsmu_generator_eval(ss->medium, omega);
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ssw->wavenumber = qpms_wavenumber(omega, ssw->medium);
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ssw->eta = ss->lattice_dimension ? ss_adjusted_eta(ss, omega) : NAN;
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QPMS_CRASHING_CALLOC(ssw->tm, ss->tm_count, sizeof(*ssw->tm));
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qpms_tmatrix_t **tmatrices_preop;
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QPMS_CRASHING_CALLOC(tmatrices_preop, ss->tmg_count, sizeof(*tmatrices_preop));
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@ -1156,7 +1167,7 @@ complex double *qpms_scatsyswk_build_translation_matrix_full(
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const qpms_scatsys_t *ss = ssw->ss;
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qpms_ss_ensure_periodic(ss);
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const cart3_t k_cart3 = cart3_from_double_array(sswk->k);
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return qpms_scatsys_periodic_build_translation_matrix_full(target, ss, wavenumber, &k_cart3);
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return qpms_scatsys_periodic_build_translation_matrix_full(target, ss, wavenumber, &k_cart3, ssw->eta);
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}
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complex double *qpms_scatsys_build_translation_matrix_e_full(
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@ -1201,17 +1212,17 @@ complex double *qpms_scatsys_build_translation_matrix_e_full(
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static inline int qpms_ss_ppair_W32xy(const qpms_scatsys_t *ss,
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qpms_ss_pi_t pdest, qpms_ss_pi_t psrc, complex double wavenumber, const cart2_t kvector,
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complex double *target, const ptrdiff_t deststride, const ptrdiff_t srcstride,
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qpms_ewald_part parts) {
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qpms_ewald_part parts, double eta) {
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const qpms_vswf_set_spec_t *srcspec = qpms_ss_bspec_pi(ss, psrc);
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const qpms_vswf_set_spec_t *destspec = qpms_ss_bspec_pi(ss, pdest);
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// This might be a bit arbitrary, roughly "copied" from Unitcell constructor. TODO review.
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const double maxR = sqrt(ss->per.unitcell_volume) * 32;
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const double maxK = 1024 * 2 * M_PI / maxR;
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const double maxR = sqrt(ss->per.unitcell_volume) * 64;
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const double maxK = 2048 * 2 * M_PI / maxR;
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return qpms_trans_calculator_get_trans_array_e32_e(ss->c,
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target, NULL /*err*/, destspec, deststride, srcspec, srcstride,
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ss->per.eta, wavenumber,
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eta, wavenumber,
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cart3xy2cart2(ss->per.lattice_basis[0]), cart3xy2cart2(ss->per.lattice_basis[1]),
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kvector,
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cart2_substract(cart3xy2cart2(ss->p[pdest].pos), cart3xy2cart2(ss->p[psrc].pos)),
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@ -1221,21 +1232,23 @@ static inline int qpms_ss_ppair_W32xy(const qpms_scatsys_t *ss,
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static inline int qpms_ss_ppair_W(const qpms_scatsys_t *ss,
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qpms_ss_pi_t pdest, qpms_ss_pi_t psrc, complex double wavenumber, const double wavevector[],
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complex double *target, const ptrdiff_t deststride, const ptrdiff_t srcstride,
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qpms_ewald_part parts) {
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qpms_ewald_part parts, double eta) {
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if(ss->lattice_dimension == 2 && // Currently, we can only the xy-plane
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!ss->per.lattice_basis[0].z && !ss->per.lattice_basis[1].z &&
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!wavevector[2])
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return qpms_ss_ppair_W32xy(ss, pdest, psrc, wavenumber, cart2_from_double_array(wavevector),
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target, deststride, srcstride, parts);
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target, deststride, srcstride, parts, eta);
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else
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QPMS_NOT_IMPLEMENTED("Only 2D xy-lattices currently supported");
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}
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complex double *qpms_scatsys_periodic_build_translation_matrix_full(
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complex double *target, const qpms_scatsys_t *ss,
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complex double wavenumber, const cart3_t *wavevector) {
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complex double wavenumber, const cart3_t *wavevector, double eta) {
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QPMS_UNTESTED;
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qpms_ss_ensure_periodic(ss);
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if (eta == 0 || isnan(eta))
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eta = ss->per.eta;
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const size_t full_len = ss->fecv_size;
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if(!target)
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QPMS_CRASHING_MALLOC(target, SQ(full_len) * sizeof(complex double));
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@ -1248,7 +1261,7 @@ complex double *qpms_scatsys_periodic_build_translation_matrix_full(
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for (qpms_ss_pi_t ps = 0; ps < ss->p_count; ++ps) {
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QPMS_ENSURE_SUCCESS(qpms_ss_ppair_W32xy(ss, pd, ps, wavenumber, cart3xy2cart2(*wavevector),
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target + deststride * ss->fecv_pstarts[pd] + srcstride * ss->fecv_pstarts[ps],
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deststride, srcstride, QPMS_EWALD_FULL));
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deststride, srcstride, QPMS_EWALD_FULL, eta));
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}
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} else
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QPMS_NOT_IMPLEMENTED("Only 2D xy-lattices currently supported");
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@ -1294,7 +1307,7 @@ static inline complex double *qpms_scatsysw_scatsyswk_build_modeproblem_matrix_f
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} else { // periodic case
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QPMS_ENSURE_SUCCESS(qpms_ss_ppair_W(ss, piR, piC, wavenumber, k,
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tmp /*target*/, bspecC->n /*deststride*/, 1 /*srcstride*/,
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QPMS_EWALD_FULL));
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QPMS_EWALD_FULL, ssw->eta));
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}
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cblas_zgemm(CblasRowMajor, CblasNoTrans, CblasNoTrans,
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@ -147,7 +147,12 @@ typedef struct qpms_scatsys_periodic_info_t {
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*/
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double unitcell_volume;
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/// Ewald parameter \f$ \eta \f$.
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/// Default Ewald parameter \f$ \eta \f$.
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/** Normally, this just gets copied into qpms_scatsys_at_omega_t,
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* which is then used in the Ewald sums.
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* However, for higher frequencies it must be adjusted to avoid
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* numerical instability.
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*/
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double eta;
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} qpms_scatsys_periodic_info_t;
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@ -241,6 +246,7 @@ typedef struct qpms_scatsys_at_omega_t {
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complex double omega; ///< Angular frequency
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qpms_epsmu_t medium; ///< Background medium optical properties at the given frequency
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complex double wavenumber; ///< Background medium wave number
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double eta; ///< Ewald parameter \f$ \eta \f$.
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} qpms_scatsys_at_omega_t;
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@ -501,7 +507,8 @@ complex double *qpms_scatsys_periodic_build_translation_matrix_full(
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complex double *target,
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const qpms_scatsys_t *ss,
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complex double wavenumber, ///< Wave number to use in the translation matrix.
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const cart3_t *wavevector ///< Wavevector / pseudomomentum in cartesian coordinates.
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const cart3_t *wavevector, ///< Wavevector / pseudomomentum in cartesian coordinates.
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double eta ///< Ewald parameter eta. Pass 0 or NaN to use the default value in \a ss.
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);
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/// Global translation matrix.
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