Fig. 2a (alpha_ee.csv) . Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless electric polarisability alpha_ee over the impinging wavelength (in micron, first column).Fig. 2b (alpha_em.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless electric-magneto polarisability alpha_em over the impinging wavelength (in micron, first column).Fig. 2c (alpha_me.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless magneto-electric polarisability alpha_me over the impinging wavelength (in micron, first column).Fig. 2d (alpha_mm.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless magnetic polarisability alpha_mm over the impinging wavelength (in micron, first column).Fig. 2e (ReEpsEff.csv) . Dependence of the real part of the effective permittivity (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2f (ReKappasumEff.csv). Dependence of the real part of the sum of effective chirality parameter kappa (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2g (ImKappasumEff.csv). Dependence of the imaginary part of the sum of effective chirality parameter kappa (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2h (MuEff.csv). Dependence of the real part of the sum of effective permeability mu_eff-1 (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3a (ORD.csv). Dependence of ORD (in degree, third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3b (ASF.csv). Dependence of ASF (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3c (ORD_dnmol.csv). Dependence of ORD (in degree, third column) over enantiomeric imbalance (first column), and NS filling fraction (second column).Fig. 3d (ASF_dnmol.csv). Dependence of ASF (third column) over enantiomeric imbalance (first column), and NS filling fraction (second column).Fig. 4a (ORD_enhance_Compare.csv). Dependence of ORD enhancement factor for Ag (second column), and for AZO (third column) over impinging wavelength (in micron, first column).Fig. 4b (ASF_enhance_Compare.csv). Dependence of ASF enhancement factor for Ag (second column), and for AZO (third column) over impinging wavelength (in micron, first column).

Fig. 2a (alpha_ee.csv) . Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless electric polarisability alpha_ee over the impinging wavelength (in micron, first column).Fig. 2b (alpha_em.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless electric-magneto polarisability alpha_em over the impinging wavelength (in micron, first column).Fig. 2c (alpha_me.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless magneto-electric polarisability alpha_me over the impinging wavelength (in micron, first column).Fig. 2d (alpha_mm.csv). Dependence of the real (third column) and imaginary (second column ) parts of the dimensionless magnetic polarisability alpha_mm over the impinging wavelength (in micron, first column).Fig. 2e (ReEpsEff.csv) . Dependence of the real part of the effective permittivity (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2f (ReKappasumEff.csv). Dependence of the real part of the sum of effective chirality parameter kappa (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2g (ImKappasumEff.csv). Dependence of the imaginary part of the sum of effective chirality parameter kappa (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 2h (MuEff.csv). Dependence of the real part of the sum of effective permeability mu_eff-1 (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3a (ORD.csv). Dependence of ORD (in degree, third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3b (ASF.csv). Dependence of ASF (third column) over impinging wavelength (in micron, first column), and NS filling fraction (second column).Fig. 3c (ORD_dnmol.csv). Dependence of ORD (in degree, third column) over enantiomeric imbalance (first column), and NS filling fraction (second column).Fig. 3d (ASF_dnmol.csv). Dependence of ASF (third column) over enantiomeric imbalance (first column), and NS filling fraction (second column).Fig. 4a (ORD_enhance_Compare.csv). Dependence of ORD enhancement factor for Ag (second column), and for AZO (third column) over impinging wavelength (in micron, first column).Fig. 4b (ASF_enhance_Compare.csv). Dependence of ASF enhancement factor for Ag (second column), and for AZO (third column) over impinging wavelength (in micron, first column).