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CPS2201 Mikhail L.
            3.  Main definition
               In the most basic case, the bidirectional reflectance distribution function
            (BRDF),  ( ,  )) is  a  four-dimensional  function  that  defines  how  light  is
                     
                           
                        
            reflected at an opaque surface. The function takes a negative incoming light
            direction,  , and  outgoing  direction,  ,  both  defined  with  respect  to  the
                                                    
                        
            surface normal , and returns the ratio of reflected radiance exiting along 
                                                                                      
            to the irradiance incident on the surface from direction  . The BRDF was first
                                                                    
            defined by Nicodemus in Nicodemus (1965). The defining equation is:

                             ( )     ( )
            (1)  ( ,  ) =      =     
                    
                 
                       
                             ( )   ( ) cos  
                                        
                                           
                                                  
                               
                                  

            where  is radiance, or power per unit solid-angle-in-the-direction-of-a-ray
            per unit projected-areaperpendicular-to-the-ray, E is irradiance, or power per
            unit surface area, and   is the angle between   and the surface normal, .
                                                            
                                    
            The  index  indicates  incident  light,  whereas  the  index  indicates  reflected
            light.
               Suppose we have measurements of a BRDF available for the set of incoming
            angles

                         ()     ()  ()   
            (2)Ω   = {  }  = {(  ,   )}  .
                         
                            =1           =1

            Here     ≥  1  is  the  total  number  of  incoming  angles  where  the
                                                                           ()
            measurements  were  taken.  Say  that  for  an  incoming  angle {   } we  have
            measurements available for angles from the set of reflection angles
                         
            (3) Ω   = ⋃ Ω  (),
                        =1
            where

                               ()        ()
            Ω  () = {  () }  = {(  () ,   () )}  ,
                             =1                  =1

                                 
            where are {  ()} =1  (possibly different) numbers of measurements taken
            for corresponding incoming angles. Our aim is to infer the BRDF manifold (1)
            from the above observations.
               In general, the connection between the true BRDF and its measurements is
            described  via  a  stochastic  transformation   ,  i.e.,    ( ,  ) =
                                                                                
                                                                             
                                                                                   
            (  ( ,  )), where : ℳ ×  × ℱ → ℱ , with ℳ = (, , ) is an (unknown)
                      
                   
                
                                                   4
                                              4
            measurable  space,  = (Π, , ℙ) is  an  unknown  probability  space, ℱ  is  the
                                                                                4
            space of all Helmholtz-invariant energy preserving 4-dimensional BRDFs, and
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