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This article was downloaded by: [Northeastern University] On: 13 November 2014, At: 22:33 Publisher: Taylor & Francis Informa Ltd Registered in England and Wales Registered Number: 1072954 Registered office: Mortimer House, 37-41 Mortimer Street, London W1T 3JH, UK Complex Variables, Theory and Application: An International Journal Publication details, including instructions for authors and subscription information: http://www.tandfonline.com/loi/gcov19 Zeros of higher order logarithmic derivatives J.D. Hinchliffe a a School of Mathematical Sciences , University of Nottingham , NG7 2RD, UK b Communicated by B. Gustafsson Published online: 22 Aug 2006. To cite this article: J.D. Hinchliffe (2004) Zeros of higher order logarithmic derivatives, Complex Variables, Theory and Application: An International Journal, 49:2, 79-86 To link to this article: http://dx.doi.org/10.1080/02781070310001634575 PLEASE SCROLL DOWN FOR ARTICLE Taylor & Francis makes every effort to ensure the accuracy of all the information (the “Content”) contained in the publications on our platform. However, Taylor & Francis, our agents, and our licensors make no representations or warranties whatsoever as to the accuracy, completeness, or suitability for any purpose of the Content. Any opinions and views expressed in this publication are the opinions and views of the authors, and are not the views of or endorsed by Taylor & Francis. The accuracy of the Content should not be relied upon and should be independently verified with primary sources of information. Taylor and Francis shall not be liable for any losses, actions, claims, proceedings, demands, costs, expenses, damages, and other liabilities whatsoever or howsoever caused arising directly or indirectly in connection with, in relation to or arising out of the use of the Content. This article may be used for research, teaching, and private study purposes. Any substantial or systematic reproduction, redistribution, reselling, loan, sub-licensing, systematic supply, or distribution in any form to anyone is expressly forbidden. Terms & Conditions of access and use can be found at http://www.tandfonline.com/page/terms- and-conditions

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Page 1: Zeros of higher order logarithmic derivatives

This article was downloaded by: [Northeastern University]On: 13 November 2014, At: 22:33Publisher: Taylor & FrancisInforma Ltd Registered in England and Wales Registered Number: 1072954 Registeredoffice: Mortimer House, 37-41 Mortimer Street, London W1T 3JH, UK

Complex Variables, Theory andApplication: An International JournalPublication details, including instructions for authors andsubscription information:http://www.tandfonline.com/loi/gcov19

Zeros of higher order logarithmicderivativesJ.D. Hinchliffe aa School of Mathematical Sciences , University of Nottingham , NG72RD, UKb Communicated by B. GustafssonPublished online: 22 Aug 2006.

To cite this article: J.D. Hinchliffe (2004) Zeros of higher order logarithmic derivatives, ComplexVariables, Theory and Application: An International Journal, 49:2, 79-86

To link to this article: http://dx.doi.org/10.1080/02781070310001634575

PLEASE SCROLL DOWN FOR ARTICLE

Taylor & Francis makes every effort to ensure the accuracy of all the information (the“Content”) contained in the publications on our platform. However, Taylor & Francis,our agents, and our licensors make no representations or warranties whatsoever as tothe accuracy, completeness, or suitability for any purpose of the Content. Any opinionsand views expressed in this publication are the opinions and views of the authors,and are not the views of or endorsed by Taylor & Francis. The accuracy of the Contentshould not be relied upon and should be independently verified with primary sourcesof information. Taylor and Francis shall not be liable for any losses, actions, claims,proceedings, demands, costs, expenses, damages, and other liabilities whatsoever orhowsoever caused arising directly or indirectly in connection with, in relation to or arisingout of the use of the Content.

This article may be used for research, teaching, and private study purposes. Anysubstantial or systematic reproduction, redistribution, reselling, loan, sub-licensing,systematic supply, or distribution in any form to anyone is expressly forbidden. Terms &Conditions of access and use can be found at http://www.tandfonline.com/page/terms-and-conditions

Page 2: Zeros of higher order logarithmic derivatives

Complex Variables, Vol. 49, No. 2, pp. 79–86, 10 February 2004

Zerosof Higher OrderLogarithmic Derivatives

J.D.HINCHLIFFE*

School of Mathematical Sciences,University of Nottingham, NG7 2RD,UK

Communicatedby B.Gustafsson

(Received 3 February 2003; In final form 22 June 2003)

We extend a result of Langley and Shea [J.K. Langley and D. Shea (1998). On multiple points ofmeromorphic functions. J. London Math. Soc., 57(2), 371–384.] concerning the distribution of zeros of thelogarithmic derivative f 0/f to higher order logarithmic derivatives of the form f (k)/f, k 2 N.

Keyword: Nevanlinna theory

MSC 2000 Subject Classification: 30D35

1 INTRODUCTION

For a meromorphic function f [2], the zeros of the logarithmic derivative f 0/f are thosezeros of f 0 at which f is non-zero. Clunie et al., proved in [1] that if f is transcendentaland meromorphic of at most order 1/2, minimal type, then f 0/f has infinitely manyzeros, and further that if f is transcendental and entire of at most order 1, minimaltype, then f 0/f has infinitely many zeros. These bounds are sharp; for example, ez isentire with order 1 but mean type, and its logarithmic derivative is identically l, andtan2

ffiffiffiz

pis meromorphic with order 1/2 and mean type, but its logarithmic derivative

omits the value 0.It is natural to attempt to generalise these results to f (k)/f, where k� 2. However, this

situation is more complicated, because while a zero of f 0/f must correspond to a zero off 0 at which f is non-zero, a zero of f (k)/f, for k� 2, need not exclude any value of f.Langley considers the problem of higher order logarithmic derivatives in [5], obtaining:

THEOREM A Suppose that k is a positive integer and f is meromorphic of finite order inthe plane such that f (k)/f is transcendental of order less than 1/2. Then f (k)/f has infinitely

* Corresponding author. E-mail: [email protected]

ISSN 0278-1077 print: ISSN 1563-5066 online � 2004 Taylor & Francis Ltd

DOI: 1080/02781070310001634575

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many zeros. The same conclusion holds if f has only finitely many poles and

limr!1

infTðr, f Þ

r¼ 0: ð1Þ

Thus far, we have only considered results pertaining to the number of zeros, not theirfrequency. For the k¼ 1 case, Langley and Shea prove the following in [6]:

THEOREM B Suppose d1 is an odd positive integer and that f is a transcendental mero-morphic function with T(r, f )¼O(rd1 ) as r ! 1, and that f satisfies (1). Then either

lim infr!1

Tðr, f Þ �r1=2

2

Z 1

r

Nðt, f Þ

t3=2dt

� �< 1

or

lim infr!1

Tðr, f 0=f Þ �r1=2

2

Z 1

r

Nðt, f =f 0Þ

t3=2dt�

5þ d1

2log r

� �< 1:

We note that (1) ensures that f 0/ f is transcendental, and that the conclusionsshow that either f has a lot of poles, or f 0/ f has a lot of zeros. Combining thisresult with ideas from the proof of Theorem 1 of [4], we generalise this result forhigher derivatives of f.

THEOREM 1 With f and d1 as in Theorem B, in particular such that f satisfies (1), letk 2 N be such that f (k)/f is transcendental. Then either

lim infr!1

Tðr, f Þ �r1=2

2

Z 1

r

Nðt, f Þ

t3=2dt� ðk� 1Þ log r

� �< 1 ð2Þ

or

lim infr!1

Tðr, f ðkÞ=f Þ �r1=2

2

Z 1

r

Nðt, f =f ðkÞÞ

t3=2dt�

5þ d1 þ 4k

2log r

� �< 1: ð3Þ

Note that we must explicitly assume f (k)/f to be transcendental, whereas (1) guaran-tees f 0/f to be transcendental. It is perhaps worth noting that the proof of Theorem 1obviates the need to employ a rather complex lemma with multiple conclusionswhich was essential in the original proof of Theorem B. The following corollaryperhaps elucidates the implications of Theorem 1 more readily.

COROLLARY Suppose that f is transcendental meromorphic in the plane, of finite order,with lower order �< 1. If f (k)/f has lower order at least �, then N(r, f )þN(r, f/f (k))has order at least min{�, 1/2}.

This work was carried out as part of a Ph.D. thesis, and as such the author wouldlike to acknowledge the numerous useful conversations with J.K. Langley whichcontributed to this result.

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2 PRELIMINARIES

LEMMA 2.1 ([3]) Suppose that f is transcendental and meromorphic in the planesuch that

mðr, f Þ � r1=2Z 1

r

nðt, f Þ

t3=2dt ! 1 ð4Þ

as r ! 1, and suppose that | f (z)|�M<1 on a path � tending to infinity. Then thereexists a function v, non-constant, non-negative and sub-harmonic in the plane, such thatvðzÞ � logþ j f ðzÞj þOð1Þ for all z. Property (4) suffices to ensure that 1 is an asymptoticvalue of f.

LEMMA 2.2 ([6]) Let f be transcendental and meromorphic in the plane, and supposethat d� 1 is such that T(r, f )¼O(rd ) for all large r. Denote by L (r,R, f ) thetotal length of the level curves | f (z)|¼R lying in the region |z|< r. Then there existarbitrarily large positive R such that f (z) has no critical values on the circle S(0,R)¼ {z: |z|¼R} and

Lðr,R, f Þ ¼ Oðrd2 Þ

as r ! 1, where d2¼ (3þ d )/2.

LEMMA 2.3 Let v be a non-constant sub-harmonic function in the plane, and let � be apath in C tending to infinity such that v<T on � for some positive constant T. Then

Mðr, vÞ

log r! 1:

LEMMA 2.4 Let v1 and v2 be non-constant sub-harmonic functions in the plane, let s1 ands2 be real constants, and let U1 and U2 be disjoint, unbounded domains such that vj� sj on@Uj and vj(zj)> sj for at least one point zj in Uj. Then

logBðr, v1Þ þ logBðr, v2Þ � 2 log r�Oð1Þ

for all large r, in which B(r, v)¼ sup{v(z): |z|¼ r}.

Both Lemmas 2.3 and 2.4 can be proved by a standard application of Tsuji’s estimatefor harmonic measure [8] (see also [6]).

LEMMA 2.5 Let f be transcendental and meromorphic such that T(r, f )¼O(rd1 ) asr ! 1 for some odd positive integer dl. Let k 2 N, set

hðzÞ ¼ f ðzÞ=f ðkÞðzÞ, ð5Þ

and assume h is transcendental. Let

h1ðzÞ ¼ hðzÞ=zN1 and f1ðzÞ ¼f ðzÞ

zk�1, ð6Þ

ZEROS OF HIGHER ORDER LOGARITHMIC DERIVATIVES 81

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where N1¼ d2þ 2kþ 1, d2¼ (3þ d1)/2 is the constant associated with d1 via Lemma 2.2.Suppose further that the constant T> 0 is such that L(r,T, h1)¼Oðrd2Þ as r ! 1 andthere are no critical values of h1 on S(0,T ) (arbitrarily large such T exist by Lemma2.2), and that C is an unbounded component of the set {z: |h1(z)|>T} such thatC � fz: jzj � Rg, for some R> 1. Then f1(z)¼O(1) and f (z)¼O(|z|k� 1) as z ! 1 in C.

Proof The proof is based on part of the proof of Theorem 1 in [5]. We partition theboundary @C of C into its intersections with the annuli Am¼ {z: 2m�1

� |z|<2m}. On @C,we have |h1|¼T, so on Am \ @C, we have |h|>Tð2m�1Þ

N1 , and hence |h|�1� c2�N1ðm�1Þ,

using c here and henceforth to denote a positive constant, not necessarily the same ateach occurrence. Now,

ZAm\@C

jtj2kjhðtÞj�1jdtj � cLð2m,T , h1Þð2mÞ

2k2�N1ðm�1Þ

� cð2mÞd222km2�N1ðm�1Þ

by assumption, and so

Z@C

jtj2kjhðtÞj�1jdtj �X1m¼1

cð2mÞd222km2�N1ðm�1Þ ¼ c2N1

X1m¼1

2�m < 1: ð7Þ

Fix a point z0 in C. Any point � in the closure C of C can be joined to z0 by a path �&consisting of a part of the circle |z|¼ |z0| and part of the ray arg z¼ arg �. Replacing anypart of �& which leaves �CC with an arc of @C gives |h1|�T on ��, and we now have

Z��

jtj2kjhðtÞj�1jdtj � c < 1: ð8Þ

To see this, consider the contributions made to the integral by the part �1 of the ray,the part �2 of the circle and the arcs �3 of @C, separately. We have

Z�1

jtj2kjhðtÞj�1jdtj � c

Z 1

jz0j

s2ks�N1 ds � c

for �l,

Z�2

jtj2kjhðtÞj�1jdtj � 2�jz0j

2kþ1�N1

T� c

for �2, and finally

Z�3

jtj2kjhðtÞj�1jdtj � c

for �3, using Eq. (7). Note that the constants are independent of �. We now set

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vðzÞ ¼

Z z

z0

ðz� tÞk�1

ðk� 1Þ!f ðkÞðtÞ dt� f ðzÞ,

and note that, by expanding out the (z� t)k�1 term, it can be seen that v admits unres-tricted analytic continuation in C. We differentiate to obtain

v0ðzÞ ¼

Z z

z0

ðz� tÞk�2

ðk� 2Þ!f ðkÞðtÞ dt� f 0ðzÞ,

and so on, up to

vðk�1ÞðzÞ ¼

Z z

z0

f ðkÞðtÞ dt� f ðk�1ÞðzÞ and vðkÞðzÞ ¼ f ðkÞðzÞ � f ðkÞðzÞ � 0:

Hence v(z) is a polynomial P(z) of degree at most k� 1. Now, near z0,

f ðzÞ þ PðzÞ ¼

Z z

z0

ðz� tÞk�1

ðk� 1Þ!f ðkÞðtÞ dt ¼ uðzÞ, ð9Þ

i.e. fþP� u� 0 near z0.Now take any � in C, and suppose we have a path � joining z0 to � in C. Consider

the function f�P� u, which is identically zero on a neighbourhood of z0, and canbe analytically continued along � to �. Hence, since f and P are both single-valued,so too is u, and Eq. (9) holds throughout C.

We now estimate the function f on C. First note that since C � fz: jzj � R > 1g andthe degree of P is at most k� l, we have

PðzÞ

zk�1

�������� � c

on C. Now, for � 2 C, we parametrize �� with respect to arc length s. Since f1(z)¼f(z)/zk� 1, it follows from (9) that

j f1ð��ðsÞÞj � cþ

Z s

0

ð��ðsÞ � ��ðtÞÞk�1��ðtÞ

k�1f1ð��ðtÞÞ

ðk� 1Þ!��ðsÞk�1hð��ðtÞÞ

���������� dt, ð10Þ

and, using

j��ðsÞ � ��ðtÞÞk�1

j �Xk�1

p¼0

k� 1p

� �j��ðsÞ

p��ðtÞk�1�p

j � kðk� 1Þ! j��ðsÞk�1��ðtÞ

k�1j,

we arrive at

ZEROS OF HIGHER ORDER LOGARITHMIC DERIVATIVES 83

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j f1ð��ðsÞÞj � WðsÞ ¼ cþ

Z s

0

kj��ðtÞ2k�2f1ð��ðtÞÞhð��ðtÞÞ

�1j dt:

Hence,

dW

ds� kj��ðsÞj

2k�2j f1ð��ðsÞÞjjhð��ðsÞÞj�1 � kj��ðsÞj

2k�2jhð��ðsÞÞj�1WðsÞ

and so

WðsÞ � c exp

Z s

0

kj��ðtÞj2k�2jhð��ðtÞÞj

�1 dt

� �� c,

using (8), which gives f1(z)¼O(1),

f ðzÞ ¼ Oðjzjk�1Þ

for z 2 C:

3 PROOF OF THEOREM 1

We assume the existence of a transcendental meromorphic function f of finite orderas in the hypothesis, in particular satisfying (1) and such that, for some k 2 N, f ðkÞ=ftranscendental and meromorphic. We set h, h1 and f1 as in (5) and (6), and notethat Nl¼ (5þ d1þ 4k)/2.

We begin by assuming both (2) and (3) are false. Then

Tðr, f Þ �r1=2

2

Z 1

r

Nðt, f Þ

t3=2dt� ðk� 1Þ log r ! 1 ð11Þ

and

Tðr, f ðkÞ=f Þ �r1=2

2

Z 1

r

Nðt, f =f ðkÞÞ

t3=2dt�

5þ d1 þ 4k

2log r ! 1 ð12Þ

as r ! 1, and straightforward integration by parts gives

mðr, f1Þ � r1=2Z 1

r

nðt, f1Þ

t3=2dt ! 1 ð13Þ

and

mðr, h1Þ � r1=2Z 1

r

nðt, h1Þ

t3=2dt ! 1, ð14Þ

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respectively. Hence, by Lemma 2.1, we have paths �fl and �h1 tending to infinity onwhich f1 and h1 tend to infinity respectively.

Choose r0 2 ½1, 2� such that h1 is finite on |z|¼ r0, and choose R¼T1>M(r0, h1)large satisfying the conclusions of Lemma 2.2. By the existence of �h1 , there exists anunbounded component, V, say, of the set {z: |h1(z)>T1}, and V is contained in{z: |z|� r0} by the choice of T1. We consider two cases:

Case (i) @V has no unbounded component. Then, by the choice of T1, @V consistsof countably many Jordan curves, and V is the only unbounded component of{z: |h1(z)|>T1}. By Lemma 2.5, f1(z)¼O(1) as z ! 1 in V, and this contradicts theexistence of the path �f1

Case (ii) @V has an unbounded component. If this is so, we have a path tendingto infinity on which |hl (z)|¼T1, and this, together with (14), enables us to useLemma 2.1 to obtain a function vhl, sub-harmonic, non-constant and non-negative inthe plane, such that

vh1 ðzÞ � logþ jh1ðzÞj þOð1Þ ð15Þ

for all z. By Lemma 2.3 and a result of Lewis et al. [7], there exists a path �1 tending toinfinity such that

vh1 ðxÞ

log jzj! þ1 ð16Þ

as z tends to infinity on �1, and

Z�1

e��vh1 ðzÞjdzj < 1 ð17Þ

for all �>0. Equation (15) implies that

log jh1ðzÞj

log jzj! þ1

on �1 also. So there exists an unbounded component Ul of {z: |h1 (z)|>Tl } such that�1\Ul is bounded. On U1, we have by Lemma 2.5 that f1 is bounded by some finite posi-tive constant, M, say, and vh1 is unbounded since �1 \U1 is unbounded. However,vh1 � logT1 þOð1Þ � M1, say, on �U1. In particular, j f1ðzÞj � M as z ! 1, on �1,and so there exists, by Lemma 2.1, a non-constant, non-negative sub-harmonic functionvf1, such that

vf1 ðzÞ � logþ jf1ðzÞj þOð1Þ:

Lewis et al. results [7] show there is a path �2 tending to infinity on which vf1 tends toinfinity. On U1, clearly vf1 � M2, say, so we take an unbounded component U2 of theset {z: vf1 >M2þ 1} (such a component must exist by the existence of the path �2) and

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we have immediately that U1 and U2 are disjoint. We therefore have the requiredconditions for the employment of Lemma 2.4. We obtain, for large r,

logBðr, vh1 Þ þ logBðr, vf1 Þ � 2 log r�Oð1Þ, ð18Þ

where B(r,v)¼ sup{v(z): |z|¼ r}. Using a standard result for sub-harmonic functions, wehave

Bðr, vh1Þ �3

2�

Z 2�

0

vh1ð2rei�Þ d� � 3mð2r, hÞ þOð1Þ � OðTð2r, f ÞÞ,

with a similar result holding for B(r, vf1 ). We therefore obtain from (18) that

2 logTð2r, f Þ � 2 log r�Oð1Þ,

so

Tð2r, f Þ

r� c,

where the constant is positive. However, this contradicts (1) and so at least one of (2) or(3) holds.

References

[1] J. Clunie, A. Eremenko and J. Rossi (1993). On equilibrium points of logarithmic and Newtonian poten-tials. J. London Math. Soc., 47(2), 309–320.

[2] W.K. Hayman (1964). Meromorphic Functions. Clarendon Press, Oxford.[3] W.K. Hayman (1978). On Iversen’s theorem for meromorphic functions with few poles. Acta.Math., 141,

115–145.[4] J.K. Langley (2001). The second derivative of a meromorphic function. Proc. Edin. Math. Soc., 44,

455–478.[5] J.K. Langley (1998). On the Zeros of f (k)/f Complex Variables, 37, 385–394.[6] J.K. Langley and D. Shea (1998). On multiple points of meromorphic functions. J. London Math. Soc.,

57(2), 371–384.[7] J. Lewis, J. Rossi and A. Weitsman (1984). On the growth of subharmonic functions along paths. Ark.

Mat., 22(1), 109–119.[8] M. Tsuji (1959). Potential Theory in Modern Function Theory. Maruzen, Tokyo.

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