C99 standard compliance for static const initialisers.
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@ -2044,15 +2044,14 @@ ccart3_t qpms_scatsysw_scattered_E(const qpms_scatsys_at_omega_t *ssw,
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}
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static const int DIPSPECN = 3;
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#define DIPSPECN 3 // We have three basis vectors
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// Evaluates the regular electric dipole waves in the origin. The returned
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// value is not to be freed as in the usual case.
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static inline const qpms_vswf_set_spec_t qpms_fill_regdipoles_0(
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ccart3_t regdipoles_0[DIPSPECN], qpms_normalisation_t normalisation) {
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static const int dipspecn = DIPSPECN; // We have three basis vectors
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// bspec containing only electric dipoles
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const qpms_vswf_set_spec_t dipspec = {
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.n = dipspecn,
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.n = DIPSPECN,
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.ilist = (qpms_uvswfi_t[]){
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qpms_tmn2uvswfi(QPMS_VSWF_ELECTRIC, -1, 1),
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qpms_tmn2uvswfi(QPMS_VSWF_ELECTRIC, 0, 1),
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@ -2064,17 +2063,16 @@ static inline const qpms_vswf_set_spec_t qpms_fill_regdipoles_0(
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};
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const sph_t origin_sph = {.r = 0, .theta = M_PI_2, .phi=0}; // Should work with any theta/phi (TESTWORTHY)
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csphvec_t regdipoles_0_sph[dipspecn];
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csphvec_t regdipoles_0_sph[DIPSPECN];
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QPMS_ENSURE_SUCCESS(qpms_uvswf_fill(regdipoles_0_sph, &dipspec,
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sph2csph(origin_sph), QPMS_BESSEL_REGULAR));
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for(int i = 0; i < dipspecn; ++i)
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for(int i = 0; i < DIPSPECN; ++i)
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regdipoles_0[i] = csphvec2ccart(regdipoles_0_sph[i], origin_sph);
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return dipspec;
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}
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// Alternative implementation, using translation operator and regular dipole waves at zero
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ccart3_t qpms_scatsys_scattered_E__alt(const qpms_scatsys_t *ss,
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qpms_bessel_t btyp,
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