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1: 3.9 Acceleration of Convergence
3.9.2 S = k = 0 ( 1 ) k 2 k 1 Δ k a 0 ,
Here Δ is the forward difference operator:
3.9.3 Δ k a 0 = Δ k 1 a 1 Δ k 1 a 0 , k = 1 , 2 , .
3.9.4 Δ k a 0 = m = 0 k ( 1 ) m ( k m ) a k m .
2: 3.6 Linear Difference Equations
3.6.2 a n Δ 2 w n 1 + ( 2 a n b n ) Δ w n 1 + ( a n b n + c n ) w n 1 = d n ,
where Δ w n 1 = w n w n 1 , Δ 2 w n 1 = Δ w n Δ w n 1 , and n . … If, as n , the wanted solution w n grows (decays) in magnitude at least as fast as any solution of the corresponding homogeneous equation, then forward (backward) recursion is stable. …
3: 18.1 Notation
Forward differences:
Δ x ( f ( x ) ) = f ( x + 1 ) f ( x ) ,
Δ x n + 1 ( f ( x ) ) = Δ x ( Δ x n ( f ( x ) ) ) .
4: 18.22 Hahn Class: Recurrence Relations and Differences
18.22.19 Δ x Q n ( x ; α , β , N ) = n ( n + α + β + 1 ) ( α + 1 ) N Q n 1 ( x ; α + 1 , β + 1 , N 1 ) ,
18.22.21 Δ x K n ( x ; p , N ) = n p N K n 1 ( x ; p , N 1 ) ,
18.22.23 Δ x M n ( x ; β , c ) = n ( 1 c ) β c M n 1 ( x ; β + 1 , c ) ,
18.22.25 Δ x C n ( x ; a ) = n a C n 1 ( x ; a ) ,
5: 2.9 Difference Equations
2.9.2 Δ 2 w ( n ) + ( 2 + f ( n ) ) Δ w ( n ) + ( 1 + f ( n ) + g ( n ) ) w ( n ) = 0 , n = 0 , 1 , 2 , ,
in which Δ is the forward difference operator (§3.6(i)). …
6: 18.26 Wilson Class: Continued
For comments on the use of the forward-difference operator Δ x , the backward-difference operator x , and the central-difference operator δ x , see §18.2(ii). …
18.26.16 Δ y ( R n ( y ( y + γ + δ + 1 ) ; α , β , γ , δ ) ) Δ y ( y ( y + γ + δ + 1 ) ) = n ( n + α + β + 1 ) ( α + 1 ) ( β + δ + 1 ) ( γ + 1 ) R n 1 ( y ( y + γ + δ + 2 ) ; α + 1 , β + 1 , γ + 1 , δ ) .
18.26.17 Δ y ( R n ( y ( y + γ + δ + 1 ) ; γ , δ , N ) ) Δ y ( y ( y + γ + δ + 1 ) ) = n ( γ + 1 ) N R n 1 ( y ( y + γ + δ + 2 ) ; γ + 1 , δ , N 1 ) .
7: 26.8 Set Partitions: Stirling Numbers
26.8.31 1 k ! d k d x k f ( x ) = n = k s ( n , k ) n ! Δ n f ( x ) ,
26.8.32 Δ f ( x ) = f ( x + 1 ) f ( x ) ;
26.8.37 1 k ! Δ k f ( x ) = n = k S ( n , k ) n ! d n d x n f ( x ) ,
8: Mathematical Introduction
complex plane (excluding infinity).
Δ (or Δ x ) forward difference operator: Δ f ( x ) = f ( x + 1 ) f ( x ) .
9: 18.19 Hahn Class: Definitions
  • 1.

    Hahn class (or linear lattice class). These are OP’s p n ( x ) where the role of d d x is played by Δ x or x or δ x (see §18.1(i) for the definition of these operators). The Hahn class consists of four discrete and two continuous families.

  • 2.

    Wilson class (or quadratic lattice class). These are OP’s p n ( x ) = p n ( λ ( y ) ) ( p n ( x ) of degree n in x , λ ( y ) quadratic in y ) where the role of the differentiation operator is played by Δ y Δ y ( λ ( y ) ) or y y ( λ ( y ) ) or δ y δ y ( λ ( y ) ) . The Wilson class consists of two discrete and two continuous families.

  • 10: 18.25 Wilson Class: Definitions
    For the Wilson class OP’s p n ( x ) with x = λ ( y ) : if the y -orthogonality set is { 0 , 1 , , N } , then the role of the differentiation operator d / d x in the Jacobi, Laguerre, and Hermite cases is played by the operator Δ y followed by division by Δ y ( λ ( y ) ) , or by the operator y followed by division by y ( λ ( y ) ) . …