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where χt is the characteristic function of E defined asχ t ⎧ ⎨ ⎩ 1, if t ∈ E, Now let us recall some of the previous results on the linear differential equation where Bz is an entire fun

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Volume 2010, Article ID 428936, 8 pages

doi:10.1155/2010/428936

Research Article

On the Exponent of Convergence for the Zeros of

Abdullah Alotaibi

Department of Mathematics, King Abdulaziz University, P.O Box 80203, Jeddah 21589, Saudi Arabia

Correspondence should be addressed to Abdullah Alotaibi,mathker11@hotmail.com

Received 1 July 2010; Accepted 12 September 2010

Academic Editor: P J Y Wong

Copyrightq 2010 Abdullah Alotaibi 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

Let B and C be entire functions of order less than 1 with C / ≡ 0 and B transcendental We prove that every solution f / ≡ 0 of the equation y Ay By  0, Az  Cze αz , α∈C \ {0} being has zeros with infinite exponent of convergence

1 Introduction

It is assumed that the reader of this paper is familiar with the basic concepts of Nevanlinna theory1,2 such as Tr, f, mr, f, Nr, f, and Sr, f Suppose that f is a meromorphic function, then the order of growth of the function f and the exponent of convergence of the zeros of f are defined, respectively, as

ρ

f

 lim sup

r→ ∞

log T

r, f

log r , λ



f

 lim sup

r→ ∞

log N

r, 1/f

Let E be a measurable subset of 1, ∞ The lower logarithmic density and the upper logarithmic density of E are defined, respectively, by

log densE  lim inf

r→ ∞

r

1



χ tdt/t log r , log densE  lim sup

r→ ∞

r

1



χ tdt/t log r , 1.2

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where χt is the characteristic function of E defined as

χ t 

1, if t ∈ E,

Now let us recall some of the previous results on the linear differential equation

where Bz is an entire function of finite order, When Bz is polynomial, many authors 3 6 have studied the properties of the solutions of1.4 If Bz is a transcendental entire function with ρ B / 1, Gundersen 7 proved that every nontrivial solution of 1.4 has infinite order

of growth In8, Wang and Laine considered the nonhomogeneous equation of type

y A1ze az y A0ze bz y  Hz, 1.5

where A0z, A1z, Hz are entire functions of order less than one and a, b are complex

numbers In fact, they have proved the following theorem

suppose that a, b ∈ C with ab / 0 and a / b Then every nontrivial solution of 1.5 is of infinite

order.

1 and b ∈ C with b / 0, −1 Then every nontrivial solution of 1.4 is of infinite order.

2 Results

We observe that all the above results concern the order of growth only In this paper, we are going to prove the following theorem which concerns the exponent of convergence

Theorem 2.1 Let B and C be entire functions of order less than 1 with C /≡ 0 and B being

transcendental Then every solution f / ≡ 0 of the equation

y Ay By  0,

has zeros with infinite exponent of convergence.

The hypothesis that B is transcendental is not redundant since Frei4 has shown that

has solutions of finite order, for certain constants K.

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We notice thatTheorem 2.1fails for ρB ≥ 1 For any entire function D the function

f  e Dsolves2.1 with

−B  f

f  A f

3 Some Lemmas

Throughout this paper we need the following lemmas In 1965, Hayman 9 proved the following lemma

Lemma 3.1 Let the function g be meromorphic of finite order ρ in the plane and let 0 < δ < 1 Then

T

2r, g

≤ Cρ, δ

T

r, g

3.1

for all r outside a set E of upper logarithmic density δ, where the positive constant C ρ, δ depends

only on ρ and δ.

In 1962, Edrei and Fuchs10 proved the following lemma

Lemma 3.2 Let g be a meromorphic function in the complex plane and let I  Ir ⊆ 0, 2π have

1



I

log g re iθ dθ ≤ 22μ 1 log1



2r, g

In 2007, Bergweiler and Langley11 proved the following lemma

Lemma 3.3 Let H be a transcendental entire function of order ρ < ∞ For large r > 0 define θr

to be the length of the longest arc of the circle |z|  r on which |Hz| > 1, with θr  2π if the

minimum modulus m0r, H  min{|Hz| : |z|  r} satisfies m0r, H > 1 Then at least one of the

following is true:

i there exists a set F ⊆ 1, ∞ of positive upper logarithmic density such that m0r, H > 1

for r ∈ F;

ii for each τ ∈ 0, 1 the set F r  {r : θr > 2π1 − τ} has lower logarithmic density at

least 1 − 2ρ1 − τ/τ.

We deduce the following

density 1 Let F be a transcendental entire function such that |Fz| ≤ |z| N on a path γ tending to infinity and for all z with

that

H z  F z − Pz

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is transcendental entire Then we have|Hz| ≤ 1 for all z ∈ γ and for all z with |z| ∈ G and

Lemma 3.3, we see that m0r, H ≤ 1 for all large r, and

so we must have case

Since G has logarithmic density 1 this gives

2ρ1 − τ ≥ 1, ρ ≥ 21 − τ1  π

Let A, B and C be as in the hypotheses We can assume that α  1 Suppose that f is a solution

of2.1 having zeros with finite exponent of convergence Then we can write

whereΠ and h are entire functions with ρΠ < ∞ We can assume that h/ ≡ 0, since if h is constant we can replace hz by hz  z and Πz by Πze −z Using2.1 and 4.1, we get

Π

Π  2

Π

Πh h h

Π

Lemma 4.1 One has ρh ≤ 1.

Proof Suppose that |hz| ≥ 1 Dividing 4.2 by h, we get

hz ≤ Πz

Πz

 2 ΠΠzz  h hz z

 |Az| ΠΠzz  1  |Bz|. 4.3

Hence, provided r lies outside a set of finite measure,

T

r, h

 mr, h

≤ Olog r

 Tr, A  Tr, B  oT

r, h

and so, using the fact that B and C have order less than 1, we obtain

T

r, h

This holds outside a set E0 of finite measure and so for all large r, since we may take s / ∈ E0

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with r ≤ s ≤ 2r so that

T

r, h

≤ Ts, h

Lemma 4.1is proved

Let M1, M2, denote large positive constants Choose σ with

max

ρ B, ρC< σ < 1. 4.7

There exists an R-set U2, page 84 such that for all large z outside U, we have

ΠΠzz  ΠΠzz  h hz z

and using the Poisson-Jensen formula,

Moreover, there exists a set G ⊆ 1, ∞ of logarithmic density 1 such that for r ∈ G the circle

|z|  r does not meet the R-set U.

or h A is a polynomial Let z be large

B z  O|z| M2

by arg z  θ is bounded ApplyingLemma 3.4to the function B−z, with γ a subpath of L,

The next step is to estimate hin the right half-plane

arg z ≤ π

one has, either

or

hz  Az ≤ |z| N 4.12

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Proof Let z be large and satisfy 4.10, and assume that 4.11 does not hold Then 4.8 implies that

ΠΠzz  hz

Also,4.7, and 4.9 give

log|Bz| ≤ |z|σ , log|Az| ≥ Rez − |z|σ|z|

2 cos 2

 c1|z|. 4.14

4.12 and 4.14 we get, from 4.2,

log hz ≥ c2|z|. 4.15 Now divide4.2 by hz We obtain, using 4.15,

hz  Az

⎝1 O |z|

M1

hz

⎠  O |z| M1

which gives|hz| ∼ |Az| and 4.12 This provesLemma 4.3

Lemma 4.3 Choose θ0∈ −π/4, π/4 such that the ray arg z  θ0

has bounded intersection with the R-set U Let V be the union of the ray arg z  θ0 and the arcs

4.9 Then one of

the following holds:

i one has 4.11 for all large z in V ;

ii one has 4.12 for all large z in V

Proof This follows simply from continuity For each large z in V we have4.11 or 4.12, but

we cannot have both because of4.14 This provesLemma 4.4

log hz  O|z| σ

, log hz  Az  O|z| σ

Proof Let z be as in the hypotheses Since A z  o1 we only need to prove 4.17 for |hz|.

Assume that|hz| ≥ 1 Then dividing 4.2 by hgives

4.18

by4.8, and so 4.17 follows using 4.7 This provesLemma 4.5

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Lemma 4.6 If conclusion (i) of Lemma 4.4 holds then ρ h < 1, while if conclusion (ii) of Lemma 4.4 holds then ρ h A < 1.

and let δ > 0 be small compared to δ1 Lemma 4.4is small compared to δ,

in particular so small that

1 log 1 C

ρ h, δ≤ 1

where Cρh, δ is the positive constant fromLemma 3.1 Let

I r  π

2

π

2





2

2



and let E be the exceptional set ofLemma 3.1, with g  h Then for large r ∈ G \ E we have,

using4.20 and Lemmas3.1,3.2, and4.5,

T

r, h

 mr, h

≤ Or σ   Olog r

 1



I rlog h re iθ dθ

≤ Or σ

1 log 1 T

2r, h

≤ Or σ

1 log 1 C

ρ h, δT

r, h

≤ Or σ 1

2T



r, h

.

4.22

We then have

T

r, h

for large r ∈ G\E Now take any large r Since G has logarithmic density 1, while E has upper logarithmic density at most δ, and since δ/δ1is small, there exists s with

r ≤ s ≤ r1δ 1, s ∈ G \ E, Tr, h

≤ Ts, h

 Os σ   O r σ 1δ1 

, 4.24

which provesLemma 4.6in this case The alternative case, in which we have conclusionii

inLemma 4.4, is proved the same way, using h A in place of h

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To finish the proof suppose first that conclusion ii of Lemma 4.4 holds Then

Lemma 3.4implies that hhas order at least π/

small, this contradictsLemma 4.6 The same contradiction, with hreplaced by h A, arises

if conclusioni ofLemma 4.4holds, and the proof of the theorem is complete

Acknowledgment

The author thanks Professor J K Langley for the invaluable discussions on the results of this paper during his visit in summer 2008 and summer 2010 to the University of Nottingham in the U.K

References

1 W K Hayman, Meromorphic Functions, Oxford Mathematical Monographs, Clarendon Press, Oxford,

UK, 1964

2 I Laine, Nevanlinna Theory and Complex Differential Equations, vol 15 of de Gruyter Studies in

Mathematics, W de Gruyter, Berlin, Germany, 1993.

3 I Amemiya and M Ozawa, “Nonexistence of finite order solutions of w

 e −z w Qzw  0,”

Hokkaido Mathematical Journal, vol 10, pp 1–17, 1981.

4 M Frei, “ ¨Uber die subnormalen L¨osungen der Differentialgleichung w

 e −z wKonst. w  0,”

Commentarii Mathematici Helvetici, vol 36, pp 1–8, 1961.

5 J K Langley, “On complex oscillation and a problem of Ozawa,” Kodai Mathematical Journal, vol 9,

no 3, pp 430–439, 1986

6 M Ozawa, “On a solution of w

 e −z  az  bw  0,” Kodai Mathematical Journal, vol 3, no 2, pp.

295–309, 1980

7 G G Gundersen, “On the question of whether f

 e −z f Bzf  0 can admit a solution f /≡ 0 of finite order,” Proceedings of the Royal Society of Edinburgh Section A, vol 102, no 1-2, pp 9–17, 1986.

8 J Wang and I Laine, “Growth of solutions of second order linear differential equations,” Journal of

Mathematical Analysis and Applications, vol 342, no 1, pp 39–51, 2008.

9 W K Hayman, “On the characteristic of functions meromorphic in the plane and of their integrals,”

Proceedings of the London Mathematical Society Third Series, vol 3, no 14, pp 93–128, 1965.

10 A Edrei and W H J Fuchs, “Bounds for the number of deficient values of certain classes of

meromorphic functions,” Proceedings of the London Mathematical Society Third Series, vol 12, pp 315–

344, 1962

11 W Bergweiler and J K Langley, “Zeros of differences of meromorphic functions,” Mathematical

Proceedings of the Cambridge Philosophical Society, vol 142, no 1, pp 133–147, 2007.

... Applications, vol 342, no 1, pp 39–51, 2008.

9 W K Hayman, ? ?On the characteristic of functions meromorphic in the plane and of their integrals,”

Proceedings of the London Mathematical... this contradictsLemma 4.6 The same contradiction, with hreplaced by h A, arises

if conclusioni ofLemma 4.4holds, and the proof of the theorem... the ray arg z  θ0

has bounded intersection with the R-set U Let V be the union of the ray arg z  θ0 and the arcs

4.9 Then one

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