Sidi's generalized secant method

Sidi's generalized secant method is a root-finding algorithm, that is, a numerical method for solving equations of the form f(x)=0 . The method was published by Avram Sidi.[1]

The method is a generalization of the secant method. Like the secant method, it is an iterative method which requires one evaluation of f in each iteration and no derivatives of f. The method can converge much faster though, with an order which approaches 2 provided that f satisfies the regularity conditions described below.

Algorithm

We call \alpha the root of f, that is, f(\alpha)=0. Sidi's method is an iterative method which generates a sequence \{ x_i \} of approximations of \alpha. Starting with k + 1 initial approximations x_1 , \dots , x_{k+1}, the approximation x_{k+2} is calculated in the first iteration, the approximation x_{k+3} is calculated in the second iteration, etc. Each iteration takes as input the last k + 1 approximations and the value of f at those approximations. Hence the nth iteration takes as input the approximations x_n , \dots , x_{n+k} and the values f(x_n) , \dots , f(x_{n+k}).

The number k must be 1 or larger: k = 1, 2, 3, .... It remains fixed during the execution of the algorithm. In order to obtain the starting approximations x_1 , \dots , x_{k+1} one could carry out a few initializing iterations with a lower value of k.

The approximation x_{n+k+1} is calculated as follows in the nth iteration. A polynomial of interpolation p_{n,k} (x) of degree k is fitted to the k + 1 points (x_n, f(x_n)), \dots (x_{n+k}, f(x_{n+k})). With this polynomial, the next approximation x_{n+k+1} of \alpha is calculated as

 x_{n+k+1} = x_{n+k} - \frac{f(x_{n+k})}{p_{n,k}'(x_{n+k})}

 

 

 

 

(1)

with p_{n,k}'(x_{n+k}) the derivative of p_{n,k} at x_{n+k}. Having calculated x_{n+k+1} one calculates f(x_{n+k+1}) and the algorithm can continue with the (n + 1)th iteration. Clearly, this method requires the function f to be evaluated only once per iteration; it requires no derivatives of f.

The iterative cycle is stopped if an appropriate stop-criterion is met. Typically the criterion is that the last calculated approximation is close enough to the sought-after root \alpha.

To execute the algorithm effectively, Sidi's method calculates the interpolating polynomial p_{n,k} (x) in its Newton form.

Convergence

Sidi showed that if the function f is (k + 1)-times continuously differentiable in an open interval I containing \alpha (that is, f \in C^{k+1} (I)), \alpha is a simple root of f (that is, f'(\alpha) \neq 0) and the initial approximations x_1 , \dots , x_{k+1} are chosen close enough to \alpha, then the sequence \{ x_i \} converges to \alpha, meaning that the following limit holds: \lim\limits_{n \to \infty} x_n = \alpha.

Sidi furthermore showed that

 \lim_{n\to\infty} \frac{x_{n +1}-\alpha}{\prod^k_{i=0}(x_{n-i}-\alpha)} = L = \frac{(-1)^{k+1}} {(k+1)!}\frac{f^{(k+1)}(\alpha)}{f'(\alpha)},

and that the sequence converges to \alpha of order \psi_k, i.e.

 \lim\limits_{n \to \infty} \frac{|x_{n+1}-\alpha|}{|x_n-\alpha|^{\psi_k}} = |L|^{(\psi_k-1)/k}

The order of convergence \psi_k is the only positive root of the polynomial

 s^{k+1} - s^k - s^{k-1} - \dots - s - 1

We have e.g. \psi_1 = (1+\sqrt{5})/2 ≈ 1.6180, \psi_2 ≈ 1.8393 and \psi_3 ≈ 1.9276. The order approaches 2 from below if k becomes large:  \lim\limits_{k \to \infty} \psi_k = 2 [2] [3]

Related algorithms

Sidi's method reduces to the secant method if we take k = 1. In this case the polynomial p_{n,1} (x) is the linear approximation of f around \alpha which is used in the nth iteration of the secant method.

We can expect that the larger we choose k, the better p_{n,k} (x) is an approximation of f(x) around x=\alpha. Also, the better p_{n,k}' (x) is an approximation of f'(x) around x=\alpha. If we replace p_{n,k}' with f' in (1) we obtain that the next approximation in each iteration is calculated as

 x_{n+k+1} = x_{n+k} - \frac{f(x_{n+k})}{f'(x_{n+k})}

 

 

 

 

(2)

This is the Newton–Raphson method. It starts off with a single approximation x_1 so we can take k = 0 in (2). It does not require an interpolating polynomial but instead one has to evaluate the derivative f' in each iteration. Depending on the nature of f this may not be possible or practical.

Once the interpolating polynomial p_{n,k} (x) has been calculated, one can also calculate the next approximation x_{n+k+1} as a solution of p_{n,k} (x)=0 instead of using (1). For k = 1 these two methods are identical: it is the secant method. For k = 2 this method is known as Muller's method.[3] For k = 3 this approach involves finding the roots of a cubic function, which is unattractively complicated. This problem becomes worse for even larger values of k. An additional complication is that the equation p_{n,k} (x)=0 will in general have multiple solutions and a prescription has to be given which of these solutions is the next approximation x_{n+k+1}. Muller does this for the case k = 2 but no such prescriptions appear to exist for k > 2.

References

  1. Sidi, Avram, "Generalization Of The Secant Method For Nonlinear Equations", Applied Mathematics E-notes 8 (2008), 115–123, http://www.math.nthu.edu.tw/~amen/2008/070227-1.pdf
  2. Traub, J.F., "Iterative Methods for the Solution of Equations", Prentice Hall, Englewood Cliffs, N.J. (1964)
  3. 3.0 3.1 Muller, David E., "A Method for Solving Algebraic Equations Using an Automatic Computer", Mathematical Tables and Other Aids to Computation 10 (1956), 208–215