Solve Integral Equation by Basis Function Expansions The eigenfunction is an integral function and difficult to solve in closed form. A general strategy for solving the eigenfunction problem in (4) is to convert the continuous eigen-analysis problem to an appropriate discrete eigen-analysis task [24]. In this paper, we use basis function expansion methods to achieve this conversion. Let { j (t )} be the series of Fourier functions. For each j, define 2j-1 2 j 2j. We expand each genetic variant profile X i (t ) as a linear combination of the basis function j : T X i (t ) Cij j (t ). (7) j 1 Define the vector-valued function X (t ) [ X 1 (t ), , X N (t )]T and the vector-valued function (t ) [1 (t ),,T (t )]T . The joint expansion of all N genetic variant profiles can be expressed as X (t ) C (t ) . (8) where the matrix C is given by C11, C1T C CN 1 CNT . . In matrix form we can express the variance-covariance function of the genetic variant profiles as 1 T X ( s ) X (t ) N 1 T ( s )C T C (t ). N R ( s, t ) (9) Similarly, the eigenfunction (t ) can be expanded as T T j 1 j1 (t ) b j j (t ) and D4(t ) 4j b j j (t ) or (t ) (t )T b and D 4(t ) (t )T S 0 b (10) 1 1 where b [b1 ,..., bT ]T and S0 diag ( 14 ,..., T4 ) . Let S diag ((1 14 ) 2 ,..., (1 T4 ) 2 ). Then, we have (t ) D 4(t ) (t )T S 2 b. (11) Substituting expansions (9) and (11) of variance-covariance R(s,t) and eigenfunction (t ) into the functional eigenequation (6), we obtain (t ) T 1 T C Cb T (t ) S 2 b , N (12) Since equation (12) must hold for all t, we obtain the following eigenequation: 1 T C Cb S 2 b , N (13) which can be rewritten as [S ( S( 1 T C C ) S ][ S 1b] [ S 1b] , or N 1 T C C ) Su u , N (14) where u S 1b . Thus, b Su and (t ) (t )T b is a solution to eigenequation (6). Note that u j , u j 1 and u j , uk 0, for k j. Therefore, we obtain a set of orthonormal eigenfunctions with an inner product of two functions defined in equation (4), as shown in equation (15): || j ||2 bTj S 2b j uTj SS 2 Su j 1 and j ,k bTj S 2bk uTj uk 0 . (15)