Research Article | Open Access
The Convergence of a Class of Parallel Newton-Type Iterative Methods
A general iterative process is proposed, from which a class of parallel Newton-type iterative methods can be derived. A unified convergence theorem for the general iterative process is established. The convergence of these Newton-type iterative methods is obtained from the unified convergence theorem. The results of efficiency analyses and numerical example are satisfactory.
Consider the following polynomial of degree :with simple zeros .
In paper , a parallel iterative method for simultaneously finding all zeros of was suggested; that is, where ; .
are distinct initial approximations for zeros of polynomial .
For appropriate starting values , method (2) is of convergence order three.
Suppose that is some iteration function and converges to zeros of with convergence order .
In particular, if , then (4) is process (2) derived in paper . If Newton iterative function is chosen as , that is, and are defined by (3), then (4) is the method discussed in paper . Because (2) is a modification of Newton method and (4) is an improvement to (2), so we call (4) modified Newton-type iteration method.
Moreover, in Section 3, three special iterative methods are derived from process (4) according to the choices of . These special methods are all modifications to process (2); their convergence and convergence order are obtained via the unified general convergence Theorem 2.
All these special modified methods are convergent with higher order and are more efficient than both Newton method and process (2).
In Section 4, the method is extended to find the multiple zeros of polynomial.
Finally, in Section 5, we give several numerical examples and the computation results are satisfactory.
2. General Convergence Theorem
In this section, we discuss the convergence of the general modified process (4).
Let , be the indices of iterations and By some simple calculation, process (4) can also be expressed as follows:where are defined by (7) andAssume that the correction iteration function in (5) is locally convergent with convergence order for each root of ; that is, converges to root with convergence order for sufficiently good starting values . Then we have the following Lemma 1.
Lemma 1. Let be defined by (5); then there exist constants and (independent of and ) such thatwhere ; .
In fact, because converges to root with convergence order for sufficiently good starting values , for every , there exist , , such that Letand then Lemma 1 holds.
Theorem 2. Suppose that initial approximations satisfy . Then the iterative process (4) converges to the zeros of , and the convergence order is .
Proof. Suppose that satisfy the condition in Theorem 2.
Then there exists a positive constant such that Hence from Lemma 1 we know that, for and ,By (10), it follows that LetIt is evident that .
Thus, from (9), we obtain that, for all , Generally, if , then we can obtain analogously thatBy mathematical induction, we know that (19) and (20) are valid for ; .
From (20), we haveIt is evident that (). That is, for
Making use of (8) and (19), we haveFurther, by (9) and , we haveHence, the convergence order of method (4) with (5) is .
3. Some Special Modified Newton Methods Derived from Formula (4)
For the correction function in (5), we will make several kinds of choice and derive some special modified Newton methods from (4). Furthermore, by the convergence Theorem 2, we give the convergence and efficiency of these special modified methods.
Definition 3. For an iteration method, we define the efficiencywhere is the convergence order; is the amount of computation required in every step of iteration.
Since are all polynomials, computational efficiency requires that the evaluation of these functions be done by Horner’s method . Then only multiplications and additions will be required to evaluate an arbitrary polynomial of degree . Since defined by (1) is a polynomial of degree , we take multiplications or divisions as a unit of the amount of computation and take no count of additions in the following. As a consequence, the evaluation of and require approximately one unit, respectively. Now the convergence and efficiency analyses of these special modified methods can be given as follows.
(ii) Let be the Halley iterative function; that is,Halley iterative function is of convergence order 3; therefore we have the following conclusion from Theorem 2.
(iii) Let where .
In particular, if we let , then (4) is the modified Newton method (2) (see ). The convergence of (2) was not proven in , but now its convergence follows directly from Theorem 2, and the convergence order is 3; therefore the efficiency .
By the way, according to our definition, the computational efficiency of Newton iterative method is .
For simultaneously finding polynomial zeros, it is evident that these modified Newton-type methods discussed in Corollaries 4–6 are convergent with higher order and are more efficient than both Newton method and process (2).
4. Extending the Iterative Method (4) to Find Multiple Zeros
In complex number field polynomial of degree can be factored as are multiple zeros of polynomial .
Here and .
By logarithmic derivation, we know thatSo we get the iterative method for simultaneously finding all zeros of .where ; . were distinct initial approximations for zeros of .
Using the same technique as in formula (4), we obtainHere,For appropriate starting values , we suppose that converges to zeros of with convergence order .
By some simple calculation, formula (31) can be expressed as follows:where
Lemma 7. Let be defined by (32); then there exist constants and (independent of and ), such that
The proof is similar to Lemma 1.
Take the constant and ; we have the following Theorem 8.
Proof. Suppose that satisfy the condition in Theorem 8. Then ThereforeFurther,Note that and ; we haveLetThenGenerally, we can obtain analogously thatBy mathematical induction, we know that (43) is valid for ; .
From (43), we get (when ).
Let , and from (42) it is inferred thatBecause , .
Hence, the convergence order of method (31) is . The proof is completed.
5. Numerical Example
In this section, we will report on three numerical examples. The computations were performed on Lenovo computer using MATLAB.
Example 1. As in , we consider complex polynomial of degree 10 ():We want to find the zeros of by method (4) with (25).
The zeros of are .
In our computation, we take error (in paper , error ) and choose the starting values just as paper ; that is,The numerical results of method (4) with (25) are listed as follows.
Numerical Results of Example 1We see from (48) that, for method (4) with (25), after two iterations the numerical results attain the precision.
Example 2. Given a polynomial is the so-called equation in theory of earthquake.
The exact roots of the equation or the zeros of are .
We want to find the zeros of by Newton method, process (2), and the three modified methods discussed in Corollaries 4–6. We choose starting values , and we take error .
The numerical results of process (2), method (4) with (25), method (4) with (26), and method (4) with (27) are listed in Table 1, but for Newton method we only give the final numerical results.
From Table 1, we see that, for Newton method, after eight iterations, the iteration approximations attain the precision; for method (2) with (3), after five iterations, the iteration approximations attain the precision; for method in Corollary 4, after four step iterations, the iteration approximations attain the precision; for methods in Corollary 5 and in Corollary 6, after three iterations, all the iteration approximations attain the precision. Hence, these modified Newton-type methods converge faster than both Newton method and iterative method (2).
Example 3. We consider polynomial . We want to find the zeros of by iterative process (31) with (45). The exact zeros of are ; the corresponding multiplicities are . We choose starting values , and , and we take error . The numerical results of the first three iterations by iterative process (31) with (45) are listed as follows.
Numerical Results of Example 3From (50) we see that, for iterative method (31) with (45), after three iterations, all the iteration approximations attain the precision .
The numerical results computed by these new parallel Newton-type iterative methods are satisfactory.
The author declares that there are no competing interests.
The author read and approved the final manuscript.
This paper was supported by a grant from Technology Bureau of Jingjiang City and Changzhou University (CDHJZ1509008).
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