FELDSPAR - 632.8nm Measured scattering matrix elements as functions of scattering angle theta (in degrees), corresponding to curves presented in Volten et al. JGR, 106, 17375-17401,2001, for feldspar at 632.8 nm. The experimental errors are also given. F11 is normalized to 1 at a scattering angle of 30 degrees. DATA ARE FREELY AVAILABLE UNDER THE REQUEST OF CITATION OF: Volten et al. JGR, 106, 17375-17401, 2001, AND Munoz et al. JQSRT, 113, 565-574, 2012. angle F11/F11(30deg) error -F12/F11 error F22/F11 error F33/F11 error F34/F11 error F44/F11 error 5 14.627 0.100 -0.010 0.002 0.954 0.066 0.977 0.008 -0.018 0.002 0.982 0.013 10 6.266 0.193 -0.002 0.001 0.974 0.005 0.966 0.004 -0.022 0.001 0.977 0.012 15 3.498 0.086 -0.001 0.001 0.967 0.011 0.962 0.003 -0.026 0.001 0.968 0.009 20 2.174 0.059 0.005 0.001 0.958 0.008 0.956 0.016 -0.026 0.001 0.961 0.015 25 1.443 0.027 0.015 0.001 0.942 0.012 0.947 0.014 -0.026 0.001 0.947 0.010 30 1.000 0.000 0.024 0.002 0.923 0.011 0.931 0.011 -0.026 0.001 0.931 0.012 35 0.717 0.013 0.034 0.001 0.917 0.009 0.911 0.012 -0.020 0.001 0.913 0.011 40 0.534 0.009 0.049 0.001 0.909 0.004 0.878 0.010 -0.011 0.001 0.895 0.009 45 0.409 0.006 0.062 0.001 0.889 0.003 0.850 0.010 -0.003 0.001 0.870 0.010 50 0.320 0.004 0.079 0.001 0.868 0.002 0.817 0.007 0.010 0.001 0.840 0.010 55 0.256 0.003 0.095 0.003 0.845 0.004 0.780 0.006 0.026 0.001 0.802 0.014 60 0.209 0.003 0.116 0.004 0.818 0.005 0.735 0.001 0.041 0.001 0.768 0.016 65 0.174 0.002 0.136 0.004 0.792 0.006 0.693 0.016 0.058 0.004 0.737 0.016 70 0.147 0.001 0.154 0.001 0.759 0.003 0.634 0.006 0.076 0.002 0.693 0.018 75 0.126 0.001 0.170 0.002 0.734 0.012 0.568 0.005 0.091 0.001 0.653 0.018 80 0.110 0.001 0.186 0.004 0.700 0.011 0.503 0.005 0.105 0.002 0.616 0.015 85 0.097 0.001 0.200 0.004 0.666 0.007 0.432 0.004 0.119 0.003 0.570 0.016 90 0.087 0.001 0.212 0.002 0.634 0.008 0.361 0.003 0.128 0.001 0.526 0.016 95 0.079 0.001 0.219 0.003 0.602 0.006 0.288 0.002 0.139 0.002 0.471 0.019 100 0.072 0.001 0.223 0.003 0.569 0.007 0.208 0.003 0.141 0.002 0.416 0.019 105 0.067 0.001 0.226 0.007 0.539 0.009 0.130 0.002 0.144 0.001 0.359 0.010 110 0.062 0.001 0.226 0.003 0.518 0.008 0.049 0.001 0.145 0.001 0.304 0.010 115 0.058 0.001 0.219 0.002 0.495 0.006 -0.031 0.002 0.141 0.002 0.243 0.011 120 0.055 0.001 0.204 0.001 0.480 0.004 -0.107 0.001 0.136 0.002 0.183 0.010 125 0.053 0.001 0.182 0.001 0.465 0.004 -0.179 0.001 0.131 0.001 0.125 0.010 130 0.051 0.001 0.156 0.004 0.463 0.006 -0.242 0.002 0.122 0.001 0.064 0.008 135 0.050 0.001 0.132 0.001 0.471 0.004 -0.302 0.001 0.110 0.001 0.006 0.008 140 0.049 0.002 0.099 0.002 0.480 0.005 -0.356 0.003 0.100 0.001 -0.055 0.009 145 0.050 0.001 0.068 0.001 0.505 0.015 -0.406 0.001 0.087 0.002 -0.116 0.009 150 0.049 0.002 0.038 0.001 0.520 0.010 -0.443 0.008 0.071 0.001 -0.164 0.009 155 0.049 0.002 0.010 0.001 0.541 0.006 -0.479 0.002 0.055 0.001 -0.206 0.008 160 0.051 0.003 -0.017 0.001 0.569 0.006 -0.503 0.005 0.035 0.002 -0.246 0.009 165 0.052 0.003 -0.036 0.003 0.589 0.006 -0.516 0.007 0.014 0.001 -0.278 0.005 170 0.056 0.003 -0.029 0.011 0.607 0.015 -0.542 0.001 -0.010 0.004 -0.298 0.004 171 0.061 0.003 -0.013 0.001 0.618 0.005 -0.534 0.001 -0.012 0.001 -0.312 0.001 172 0.063 0.003 -0.009 0.001 0.615 0.004 -0.539 0.001 -0.011 0.005 -0.304 0.001 173 0.064 0.004 -0.008 0.001 0.614 0.010 -0.544 0.001 -0.010 0.005 -0.302 0.001