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# Line 2 | Line 2
2   <!-- RCSid $Id$ -->
3   <head>
4   <title>
5 < The RADIANCE 5.0 Synthetic Imaging System
5 > The RADIANCE 5.4 Synthetic Imaging System
6   </title>
7   </head>
8   <body>
# Line 10 | Line 10 | The RADIANCE 5.0 Synthetic Imaging System
10   <p>
11  
12   <h1>
13 < The RADIANCE 5.0 Synthetic Imaging System
13 > The RADIANCE 5.4 Synthetic Imaging System
14   </h1>
15  
16   <p>
# Line 798 | Line 798 | unless the line integrals consider enclosed geometry.
798  
799   <dd>
800          Trans2 is the anisotropic version of <a HREF="#Trans">trans</a>.  
801 <        The string arguments  are  the same as for plastic2, and the real arguments are the same as  for  trans  but  with  an  additional roughness value.
801 >        The string arguments  are  the same as for <a HREF="#Plastic2">plastic2</a>,
802 >        and the real arguments are the same as  for  trans  but  with  an  additional roughness value.
803  
804   <pre>
805          mod trans2 id
# Line 810 | Line 811 | unless the line integrals consider enclosed geometry.
811   <p>
812  
813   <dt>
814 +        <a NAME="Ashik2">
815 +        <b>Ashik2</b>
816 +        </a>
817 +
818 + <dd>
819 +        Ashik2 is the anisotropic reflectance model by Ashikhmin & Shirley.
820 +        The string arguments are the same as for <a HREF="#Plastic2">plastic2</a>, but the real
821 +        arguments have additional flexibility to specify the specular color.
822 +        Also, rather than roughness, specular power is used, which has no
823 +        physical meaning other than larger numbers are equivalent to a smoother
824 +        surface.
825 + <pre>
826 +        mod ashik2 id
827 +        4+ ux uy uz funcfile transform
828 +        0
829 +        8 dred dgrn dblu sred sgrn sblu u-power v-power
830 + </pre>
831 +
832 + <p>
833 +
834 + <dt>
835          <a NAME="Dielectric">
836          <b>Dielectric</b>
837          </a>
# Line 1132 | Line 1154 | unless the line integrals consider enclosed geometry.
1154   <p>
1155  
1156   <dt>
1157 +        <a NAME="aBSDF">
1158 +        <b>aBSDF</b>
1159 +        </a>
1160 +
1161 + <dd>
1162 +        The aBSDF material is identical to the BSDF type with two
1163 +        important differences.  First, proxy geometry is not
1164 +        supported, so there is no thickness parameter.  Second, an
1165 +        aBSDF is assumed to have some specular through component
1166 +        (the &rsquo;a&rsquo; stands for &quot;aperture&quot;),
1167 +        which is treated specially during the direct calculation
1168 +        and when viewing the material.  Based on the BSDF data, the
1169 +        coefficient of specular transmission is determined and used
1170 +        for modifying unscattered shadow and view rays.
1171 +
1172 + <pre>
1173 +        mod aBSDF id
1174 +        5+ BSDFfile ux uy uz funcfile transform
1175 +        0
1176 +        0|3|6|9
1177 +             rfdif gfdif bfdif
1178 +             rbdif gbdif bbdif
1179 +             rtdif gtdif btdif
1180 + </pre>
1181 +
1182 + <p>
1183 +        If a material has no specular transmitted component, it is
1184 +        much better to use the BSDF type with a zero thickness
1185 +        than to use aBSDF.
1186 + <p>
1187 +
1188 + <dt>
1189          <a NAME="Antimatter">
1190          <b>Antimatter</b>
1191          </a>
# Line 1415 | Line 1469 | or:
1469   </h4>
1470  
1471   A mixture is a blend of one or more materials or textures and patterns.
1472 + Blended materials should not be light source types or virtual source types.
1473   The basic types are given below.
1474  
1475   <p>
# Line 1487 | Line 1542 | A mixfunc mixes  two  modifiers  procedurally.   It  i
1542          arguments, the red, green and blue values
1543          corresponding to the pixel at (u,v).
1544  
1490 </dl>
1545   <p>
1546  
1547   <dt>
# Line 1891 | Line 1945 | Ecole  Polytechnique  Federale de Lausanne (EPFL Unive
1945   </h2>
1946   <p>
1947   <ul>
1948 +    <li>Wang, Taoning, Gregory Ward, Eleanor Lee,
1949 +      &quot;<a href="https://authors.elsevier.com/a/1XQ0a1M7zGwT7v">Efficient
1950 +      modeling of optically-complex, non-coplanar exterior shading:
1951 +      Validation of matrix algebraic methods</a>&quot;
1952 +      <em>Energy & Buildings</em>, vol. 174, pp. 464-83, Sept. 2018.
1953 +    <li>Lee, Eleanor S., David Geisler-Moroder, Gregory Ward,
1954 +      &quot;<a href="https://eta.lbl.gov/sites/default/files/publications/solar_energy.pdf">Modeling
1955 +      the direct sun component in buildings using matrix
1956 +      algebraic approaches: Methods and
1957 +      validation</a>,&quot; <em>Solar Energy</em>,
1958 +      vol. 160, 15 January 2018, pp 380-395.
1959 +    <li>Narain, Rahul, Rachel A. Albert, Abdullah Bulbul,
1960 +       Gregory J. Ward, Marty Banks, James F. O'Brien,
1961 +       &quot;<a href="http://graphics.berkeley.edu/papers/Narain-OPI-2015-08/index.html">Optimal
1962 +       Presentation of Imagery with Focus
1963 +       Cues on Multi-Plane Displays</a>,&quot;
1964 +       <em>SIGGRAPH 2015</em>.
1965 +    <li>Ward, Greg, Murat Kurt, and Nicolas Bonneel,
1966 +        &quot;<a href="papers/WMAM14_Tensor_Tree_Representation.pdf">Reducing
1967 +        Anisotropic BSDF Measurement to Common Practice</a>,&quot;
1968 +        <em>Workshop on Material Appearance Modeling</em>, 2014.
1969 +    <li>Banks, Martin, Abdullah Bulbul, Rachel Albert, Rahul Narain,
1970 +        James F. O'Brien, Gregory Ward,
1971 +        &quot;<a href="http://graphics.berkeley.edu/papers/Banks-TPO-2014-05/index.html">The
1972 +        Perception of Surface Material from Disparity and Focus Cues</a>,&quot;
1973 +        <em>VSS 2014</em>.
1974      <li>McNeil, A., C.J. Jonsson, D. Appelfeld, G. Ward, E.S. Lee,
1975          &quot;<a href="http://gaia.lbl.gov/btech/papers/4414.pdf">
1976          A validation of a ray-tracing tool used to generate

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