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Volume 2012, Article ID 653914,9pages doi:10.1155/2012/653914

Research Article

Localization and Perturbations of Roots to Systems

of Polynomial Equations

Michael Gil’

Department of Mathematics, Ben Gurion University of the Negev, P.O. Box 653, Beer-Sheva 84105, Israel

Correspondence should be addressed to Michael Gil’,gilmi@bezeqint.net

Received 20 March 2012; Accepted 28 May 2012

Academic Editor: Andrei Volodin

Copyrightq2012 Michael Gil’. This is an open access article distributed under the Creative

Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

We establish estimates for the sums of absolute values of solutions of a zero-dimensional polynomial system. By these estimates, inequalities for the counting function of the roots are derived. In addition, bounds for the roots of perturbed systems are suggested.

1. Introduction and Statements of the Main Results

Let us consider the system:

fx, ygx, y0, 1.1

where

fx, y

m1

j0

n1

k0

ajkxm1−jyn1−k am1n1/0,

gx, y

m2

j0

n2

k0

bjkxm2−jyn2−k bm2n2/0.

1.2

The coefficientsajk, bjkare complex numbers.

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we establish estimates for sums of absolute values of the roots of1.1. By these estimates, bounds for the number of solutions in a given disk are suggested. In addition, we discuss perturbations of system 1.1. Besides, bounds for the roots of a perturbed system are suggested.

We use the approach based on the resultant formulations, which has a long history; the literature devoted to this approach is very rich, compared to1,3,4. We combine it with the recent estimates for the eigenvalues of matrices and zeros of polynomials. The problem of solving polynomial systems and systems of transcedental equations continues to attract the attention of many specialists despite its long history. It is still one of the burning problems of algebra, because of the absence of its complete solution, compared to the very interesting recent investigations2,5–8and references therein. Of course we could not survey the whole subject here.

A pair of complex numbers x, y is a solution of 1.1 if fx, y gx, y 0. Besidesxwill be called anX-root coordinatecorresponding toyandyaY-root coordinate

corresponding tox. All the considered roots are counted with their multiplicities. Put

aj

y

n1

k0

ajkyn1−k

j0, . . . , m1

, bj

y

n2

k0

bjkyn2−k

j0, . . . , m2

. 1.3

Then

fx, y

m1

j0

aj

yxm1−j,

gx, y

m2

j0

bj

yxm2−j.

1.4

Withmm1m2introduce them×mSylvester matrix

Sy

⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝

a0 a1 a2 · · · am1−1 am1 0 0 · · · 0

0 a0 a1 · · · am1−2 am1−1 am1 0 · · · 0

· · · ·

0 0 0 · · · a0 a1 a2 a3 · · · am1

b0 b1 b2 · · · bm2−1 bm2 0 0 · · · 0

0 b0 b1 · · · bm2−2 bm2−1 bm2 0 · · · 0

· · · ·

0 0 0 · · · b0 b1 b2 b3 · · · bm2

⎞ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎟ ⎠

, 1.5

withakakyandbkbky. PutRy detSyand consider the expansion:

Ry

n

k0

Rkynk, wheren:degR

(3)

Furthermore, denote

θR:

⎡ ⎣ 1

2π

2π

0

Reit

R0

2

dt−1

⎤ ⎦

1/2

. 1.7

Clearly,

θR≤sup

|y|1

Ry

R0

, R0 lim

y→ ∞

Ry

yn , R0

1 2π

2π

0

eintReitdt. 1.8

Thanks to the Hadamard inequality, we have

Ry2≤

m 1

k0

ak

y2

m2m 2

k0

bk

y2

m1

. 1.9

Assume that

Rn/0. 1.10

Theorem 1.1. TheY-root coordinatesykof 1.1(if, they exist), taken with the multiplicities and

ordered in the decreasing way:|yk| ≥ |yk1|, satisfy the estimates:

j

k1

yk< θR1 j

j 1,2, . . . , n. 1.11

If, in addition, condition1.10holds, then

j

k1

1 yk

< R0θR 1

Rn

j j 1,2, . . . , n, 1.12

whereykare theY-root coordinates of 1.1taken with the multiplicities and ordered in the increasing

way:|yk| ≤ |yk1|.

This theorem and the next one are proved in the next section. Note that another bound forjk1|yk|is derived in9, Theorem 11.9.1; besides, in the mentioned theoremaj·and

bj·have the sense different from the one accepted in this paper.

From1.12it follows that

min

k yk>

Rn

R0θR 1 Rn

. 1.13

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To estimate theX-root coordinates, assume that

inf

|y|≤θR1

a0

y>0 1.14

and put

ψf sup

|y|θR1

1 a0

y

⎡ ⎣m1

j1

aj

y2

⎤ ⎦

1/2

. 1.15

Theorem 1.2. Let condition1.14holds. Then theX-root coordinatesxky0of1.1corresponding

to aY-root coordinatey0 (if they exist), taken with the multiplicities and ordered in the decreasing

way, satisfy the estimates:

j

k1

xk

y0< ψfj

j1,2, . . . ,min{m1, m2}

. 1.16

InTheorem 1.2one can replacefbyg.

Furthermore, sinceykare ordered in the decreasing way, byTheorem 1.1we getj|yj|<

jθRand

yj< rj:1θR

j

j1, . . . , n. 1.17

Thus1.1has in the disc{z∈C:|z| ≤rj}no more thann−j Y-root coordinates. If we denote

byνYrthe number ofY-root coordinates of1.1inΩr : {z ∈C : |z| ≤r}for a positive

numberr, then we get

Corollary 1.3. Under condition1.10, the inequalityνYrnj1 is valid for any

r≤1θR

j . 1.18

Similarly, byTheorem 1.2, we get the inequality:

xj

y0≤1

ψf

j

j1,2, . . . ,min{m1, m2}

. 1.19

Denote byνXy0, rthe number ofX-root coordinates of1.1inΩr, corresponding to aY

coordinatey0.

Corollary 1.4. Under conditions1.14, for anyY-root coordinatey0, the inequality:

νX

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is valid, provided

r ≤1ψf

j . 1.21

In this corollary also one can replacefbyg.

2. Proofs of Theorems

1.1

and

1.2

First, we need the following result.

Lemma 2.1. LetPz : znc

1zn−1· · ·cn be a polynomial with complex coefficients. Then its

rootszkPordered in the decreasing way satisfy the inequalities:

j

k1

|zkP| ≤

1 2π

2π

0

Peit2dt−1 1/2

j j1, . . . , n. 2.1

Proof. As it is proved in9, Theorem 4.3.1 see also10,

j

k1

|zkP| ≤

n

k1

|ck|2

1/2

j. 2.2

But thanks to the Parseval equality, we have

n

k1

|ck|21

1 2π

2π

0

Peit2dt. 2.3

Hence the required result follows.

Proof ofTheorem 1.1. The bound 1.11 follows from the previous lemma with Py

Ry/R0. To derive bound1.12note that

RyRnynW

1

y

, whereWz 1

Rn

n

k0

Rkzk

n

k0

dkznk, 2.4

withdk Rnk/Rn. So any zerozWofWzis equal to 1/y, whereyis a zero ofRy. By

the previous lemma

j

k1

|zkW|<

1 2π

2π

0

Weit2dt−1 1/2

(6)

Thus,

j

k1

1 yk

<

1 2π

2π

0

Weit2dt−1 1/2

j j 1, . . . , n. 2.6

ButWz znR1/z/R

n. Thus,|Weit| 1/Rn|Reit|. This proves the required result.

Proof ofTheorem 1.2. Due to Theorem 1.1, for any fixed Y-root coordinate y0 we have the

inequality:

y0θR 1. 2.7

We seek the zeros of the polynomial:

fx, y0

m1

j0

aj

y0

xm1−j. 2.8

Besides, due to1.14and2.7,a0y0/0. Put

Qx f

x, y0

a0y0 , θQ :

1 a0

y0

⎡ ⎣m1

j1

aj

y02

⎤ ⎦

1/2

. 2.9

Clearly,

Qx xm1 1

a0y0

m1

j1

aj

y0

xm1−j.

2.10

Due to the above mentioned9, Theorem 4.3.1we have

j

k1

xk

y0< θQj

j1,2, . . . , n. 2.11

But according to2.7,θQψf. This proves the theorem.

3. Perturbations of Roots

Together with1.1, let us consider the coupled system:

(7)

where

fx, y

m1

j0

n1

k0

ajkxm1−jyn1−k,

gx, y

m2

j0

n2

k0

bjkxm2−jyn2−k.

3.2

Hereajk,bjkare complex coefficients. Put

aj

y

n1

k1

ajkyn1−k

j 0, . . . , m1

,

bj

y

n2

k0

bjkyn2−k

j 0, . . . , m2

.

3.3

Let Sy be the Sylvester matrix defined as above with ajy instead of ajy, and bjy

instead ofbjy, and putRy detSy. It is assumed that

degRydegRyn. 3.4

Consider the expansion:

Ry

n

k0

Rkynk. 3.5

Due to3.4,R0 /0. Denote

qR,R:

⎡ ⎣ 1

2π

2π

0

Reit

R0

Reit

R0

2

dt

⎤ ⎦

1/2

,

ηR θ2R n−11/2.

3.6

Clearly,

qR,R≤max

|z|1

Ry

R0 −

Ry

R0

. 3.7

Theorem 3.1. Under condition 3.4, for any Y-root coordinate y0 of 3.1, there is a Y-root

coordinatey0of1.1, such that

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whereμRis the unique positive root of the equation:

ynqR,R

n−1

k0

ηkRynk−1

k! . 3.9

To proveTheorem 3.1, for a finite integern, consider the polynomials:

n

k0

ckλnk,

n

k0

ckλnk c0 c0 1, 3.10

with complex coefficients. Put

q0

n

k1

|ckck|2

1/2 ,

ηP

n

k1

|ck|2n−1

1/2 .

3.11

Lemma 3.2. For any rootzPofPy, there is a rootzPofPy, such that|zPzP| ≤rq0,

whererq0is the unique positive root of the equation

ynq0

n−1

k0

ηkPynk−1

k! . 3.12

This result is due to Theorem 4.9.1 from the book9and inequality9.2on page 103 of that book.

By the Parseval equality we have

n

k0

|ck|2

1 2π

2π

0

Peit2dt,

q20 1

2π

2π

0

PeitPeit2dt≤max

|z|1

PyPy2.

3.13

Thus

η2P 1

2π

2π

0

Peit2dtn−2≤max

|z|1

P

y2n−2. 3.14

The assertion of Theorem 3.1 now follows from in the previous lemma with Py

(9)

Further more, denote

pR :q

R,R

n−1

k0

ηkR

k! ,

δR:

n

p

R ifpR ≤1,

pR ifpR >1.

3.15

Due to Lemma 1.6.1 from11, the inequalityμRδR is valid. NowTheorem 3.1implies the

following.

Corollary 3.3. Under condition 3.4, for any Y-root coordinate y0 of 3.1, there is a Y-root

coordinatey0of1.1, such that|y0−y0| ≤δR.

Similarly, one can consider perturbations of theX-root root coordinates.

To evaluate the quantityRyRyone can use the following result: let A and B two complexn×n-matrices. Then

|detA−detB| ≤ N2AB

nn/2

11

2N2AB N2AB n

, 3.16

whereN2

2A TraceAAis the Hilbert-Schmidt norm andA∗ is the adjoint toA. For the

proof of this inequality see12. TakingBSy,ASywe get a bound for|RzRz|.

References

1 I. M. Gel’fand, M. M. Kapranov, and A. V. Zelevinsky, Discriminants, Resultants, and Multidimensional

Determinants, Mathematics: Theory & Applications, Birkh¨auser, Boston, Mass, USA, 1994.

2 B. Sturmfels, “Solving algebraic equations in terms ofA-hypergeometric series,” Discrete Mathematics,

vol. 210, no. 1–3, pp. 171–181, 2000.

3 B. Mourrain, “Computing the isolated roots by matrix methods,” Journal of Symbolic Computation, vol.

26, no. 6, pp. 715–738, 1998, Symbolic numeric algebra for polynomials.

4 B. Sturmfels, Solving Systems of Polynomial Equations, vol. 97 of CBMS Regional Conference Series in

Mathematics, American Mathematical Society, Providence, RI, USA, 2002.

5 W. Forster, “Homotopies for systems of polynomial equations,” Acta Mathematica Vietnamica, vol. 22,

no. 1, pp. 107–122, 1997.

6 J. McDonald, “Fiber polytopes and fractional power series,” Journal of Pure and Applied Algebra, vol.

104, no. 2, pp. 213–233, 1995.

7 J. McDonald, “Fractional power series solutions for systems of equations,” Discrete & Computational

Geometry, vol. 27, no. 4, pp. 501–529, 2002.

8 Z. K. Wang, S. L. Xu, and T. A. Gao, Algebraic Systems of Equations and Computational Complexity Theory,

vol. 269 of Mathematics and Its Applications, Kluwer Academic Publishers, Dordrecht, The Netherlands, 1994.

9 M. Gil’, Localization and Perturbation of Zeros of Entire Functions, vol. 258 of Lecture Notes in Pure and

Applied Mathematics, CRC Press, Boca Raton, Fla, USA, 2010.

10 M. I. Gil’, “Bounds for counting functions of finite order entire functions,” Complex Variables and

Elliptic Equations, vol. 52, no. 4, pp. 273–286, 2007.

11 M. I. Gil’, Operator Functions and Localization of Spectra, vol. 1830 of Lecture Notes in Mathematics,

Springer, Berlin, Germany, 2003.

12 M. I. Gil’, “A bound for functions defined on a normed space,” Journal of Physics A, vol. 40, no. 15, pp.

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