SYNTHETIC SCATTERING MATRIX FOR the JSC-1A sample at 488 nm presented in "Experimental scattering matrix for lunar regolith simulant JSC-1A at visible wavelengths" J. Escobar-Cerezo, O. Muñoz, F. Moreno, D. Guirado, J.C. Gómez Martín, J.D. Goguen, E.J. Garboczi, A.N. Chiaramonti, T. Lafarge, R.A. West. DATA ARE FREELY AVAILABLE UNDER THE REQUEST OF CITATION OF: Escobar-Cerezo et al. ApJSS, 235, 19-27, 2018, AND Munoz et al. JQSRT, 113, 565-574, 2012. F11_au is normalized so that its average over all directions equals unity. For the extrapolation of the F11 element at forward direction we have assumed the size distribution based on Mie theory. From the extrapolated F11 element we have calculated the corresponding asymmetry parameter= = 0.74 Angle Fau11 -F12/F11 F22/F11 F33/F11 F34/F11 F44/F11 0 8.67E+04 0.00E+00 1.00E+00 1.00E+00 0.00E+00 1.00E+00 1 1.85E+03 -3.33E-04 1.01E+00 9.77E-01 1.00E-03 9.62E-01 2 3.51E+02 -6.67E-04 1.03E+00 9.53E-01 2.00E-03 9.23E-01 3 1.24E+02 -1.00E-03 1.04E+00 9.30E-01 3.00E-03 8.85E-01 5 1.40E+01 2.00E-03 1.02E+00 9.45E-01 -4.00E-03 9.27E-01 6 1.16E+01 2.00E-03 1.02E+00 9.27E-01 -3.00E-03 9.21E-01 7 9.23E+00 -0.00E+00 1.02E+00 9.45E-01 -1.00E-03 9.47E-01 8 8.49E+00 4.00E-03 9.99E-01 9.22E-01 -9.00E-03 8.92E-01 9 7.19E+00 3.00E-03 9.76E-01 9.11E-01 -5.00E-03 9.09E-01 10 6.28E+00 5.00E-03 9.90E-01 9.08E-01 -3.00E-03 8.77E-01 15 3.57E+00 3.00E-03 9.32E-01 8.77E-01 -8.00E-03 8.26E-01 20 2.42E+00 1.20E-02 9.16E-01 8.50E-01 -3.00E-03 7.90E-01 25 1.78E+00 1.40E-02 8.80E-01 8.21E-01 -1.00E-03 7.39E-01 30 1.36E+00 1.80E-02 8.62E-01 7.91E-01 3.00E-03 7.17E-01 35 1.06E+00 3.00E-02 8.55E-01 7.61E-01 1.20E-02 6.79E-01 40 8.37E-01 3.80E-02 8.05E-01 7.26E-01 2.30E-02 6.47E-01 45 6.85E-01 4.80E-02 7.53E-01 6.88E-01 3.60E-02 6.31E-01 50 5.70E-01 6.60E-02 7.35E-01 6.30E-01 4.40E-02 5.77E-01 55 4.91E-01 8.00E-02 6.77E-01 5.91E-01 5.90E-02 5.27E-01 60 4.22E-01 9.50E-02 6.41E-01 5.39E-01 6.60E-02 4.75E-01 65 3.72E-01 1.09E-01 6.09E-01 4.76E-01 8.60E-02 4.25E-01 70 3.42E-01 1.16E-01 5.74E-01 3.89E-01 1.07E-01 3.80E-01 75 3.07E-01 1.17E-01 5.34E-01 3.29E-01 1.09E-01 3.32E-01 80 2.92E-01 1.24E-01 5.10E-01 2.64E-01 1.04E-01 3.00E-01 85 2.74E-01 1.26E-01 4.82E-01 1.98E-01 1.20E-01 2.56E-01 90 2.62E-01 1.25E-01 4.62E-01 1.46E-01 1.18E-01 2.12E-01 95 2.50E-01 1.16E-01 4.44E-01 7.30E-02 1.08E-01 1.61E-01 100 2.40E-01 1.16E-01 4.10E-01 2.10E-02 9.30E-02 1.30E-01 105 2.28E-01 1.05E-01 3.95E-01 -3.60E-02 9.40E-02 1.06E-01 110 2.21E-01 1.00E-01 3.93E-01 -9.70E-02 9.10E-02 6.50E-02 115 2.13E-01 8.80E-02 3.84E-01 -1.44E-01 6.90E-02 1.20E-02 120 2.06E-01 8.40E-02 3.90E-01 -2.02E-01 5.20E-02 -2.60E-02 125 2.02E-01 8.10E-02 3.72E-01 -2.31E-01 4.50E-02 -4.50E-02 130 1.97E-01 6.40E-02 3.73E-01 -2.82E-01 4.00E-02 -8.50E-02 135 1.97E-01 4.80E-02 3.77E-01 -2.93E-01 4.50E-02 -1.07E-01 140 1.95E-01 4.10E-02 4.05E-01 -3.33E-01 2.80E-02 -1.44E-01 145 1.93E-01 1.90E-02 3.94E-01 -3.65E-01 8.00E-03 -1.48E-01 150 1.97E-01 1.50E-02 4.14E-01 -3.73E-01 1.00E-02 -1.64E-01 155 1.97E-01 4.00E-03 4.38E-01 -3.89E-01 -7.00E-03 -2.02E-01 160 2.01E-01 -1.00E-02 4.39E-01 -4.12E-01 -2.50E-02 -2.12E-01 165 2.05E-01 -1.50E-02 4.33E-01 -4.22E-01 -2.70E-02 -2.08E-01 170 2.14E-01 -1.50E-02 4.47E-01 -4.35E-01 -3.50E-02 -2.18E-01 171 2.18E-01 -1.20E-02 4.46E-01 -4.50E-01 -3.80E-02 -2.16E-01 172 2.22E-01 -1.00E-02 4.52E-01 -4.48E-01 -4.50E-02 -2.05E-01 173 2.27E-01 -1.60E-02 4.60E-01 -4.31E-01 -4.60E-02 -2.07E-01 174 2.27E-01 -1.20E-02 4.60E-01 -4.49E-01 -3.60E-02 -2.15E-01 175 2.36E-01 -1.10E-02 4.64E-01 -4.31E-01 -4.40E-02 -1.87E-01 176 2.36E-01 -1.20E-02 4.59E-01 -4.43E-01 -4.80E-02 -1.88E-01 177 2.46E-01 -1.30E-02 4.64E-01 -4.43E-01 -4.40E-02 -1.77E-01 178 2.53E-01 -8.67E-03 4.69E-01 -4.55E-01 -2.93E-02 -1.04E-01 179 2.56E-01 -4.33E-03 4.74E-01 -4.67E-01 -1.47E-02 -3.10E-02 180 2.56E-01 0.00E+00 4.79E-01 -4.79E-01 0.00E+00 4.20E-02