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Certain Subclasses of Analytic Functions Associated with Conic Domains
By
Sarfraz Nawaz CIIT/SP09–PMT–015/ISB
PhD Thesis
In Mathematics
COMSATS Institute of Information Technology
Islamabad, Pakistan Spring, 2012
ii
COMSATS Institute of Information Technology
Certain Subclasses of Analytic Functions
Associated with Conic Domains
A Thesis Presented to
COMSATS Institute of Information Technology, Islamabad
In partial fulfillment
of the requirement for the degree of
PhD Mathematics
By
Sarfraz Nawaz
CIIT/SP09–PMT–015/ISB
Spring, 2012
iii
Certain Subclasses of Analytic Functions Associated with Conic Domains
A Post Graduate thesis submitted to the Department of Mathematics as partial fulfillment of the requirement for the award of Degree of PhD Mathematics.
Name Registration Number
Sarfraz Nawaz CIIT/SP09–PMT–015/ISB
Supervisor Dr. Khalida Inayat Noor Professor, Department of Mathematics Islamabad Campus. COMSATS Institute of Information Technology (CIIT) Islamabad Campus. July, 2012
iv
Final Approval
This thesis titled
Certain Subclasses of Analytic Functions
Associated with Conic Domains By
Sarfraz Nawaz CIIT/SP09 –PMT– 015/ISB
Has been approved For the COMSATS Institute of Information Technology, Islamabad.
External Examiner 1 : __________________________ Prof. Dr. Ghulam Shabbir Professor GIKI, Topi KPK, Pakistan
External Examiner 2 : __________________________
Prof. Dr. Noor Ahmed Sheikh Professor University of Sindh, Jamshoro, Pakistan
Supervisor : __________________________
Prof. Dr. Khalida Inayat Noor Professor CIIT, Islamabad, Pakistan
HoD : __________________________ Dr. Moiz ud Din Khan Associate Professor
CIIT, Islamabad, Pakistan
Dean, Faculty of Sciences : __________________________ Prof. Dr. Arshad Saleem Bhatti
v
Declaration
I, Sarfraz Nawaz, CIIT/SP09–PMT–015/ISB hereby declare that I have produced the
work presented in this thesis, during the scheduled period of study. I also declare that I
have not taken any material from any source except referred to wherever due that amount
of plagiarism is within acceptable range. If a violation of HEC rules on research has
occurred in this thesis, I shall be liable to punishable action under the plagiarism rules of
the HEC.
Date:
Signature of student:
Sarfraz Nawaz
CIIT/SP09–PMT– 015/ISB
vi
Certificate It is certified that Sarfraz Nawaz CIIT/SP09-PMT-015/ISB has carried out all the work
related to this thesis under my supervision at the Department of Mathematics,
COMSATS Institute of Information Technology, Islamabad and the work fulfills the
requirement for award of PhD degree.
Date: ________________
Supervisor:
___________________________ Prof. Dr. Khalida Inayat Noor Professor
Head of Department:
__________________
Dr. Moiz ud Din Khan
Associate Professor
Mathematics Department
vii
DEDICATION
This work is dedicated
To
My Father Muhammad Nawaz Malik
Who
Always has Faith in me and his Faith and Love made me what I am today.
viii
ACKNOWLEDGEMENTS
All thanks and acknowledgments to Almighty ALLAH, the Most Merciful and
Compassionate, the Most Gracious and Beneficent, Who is the sole source of knowledge
and wisdom, Who has endowed human beings with the faculty of reasoning and pursuing
knowledge and Who through his Kindness, Graciousness and Countless Blessings
enabled me to pursue higher ideals in life.
I wish to assert my sincere, humble and deep gratitude to my Respected Supervisor
Prof. Dr. Khalida Inayat Noor, Department of Mathematics, CIIT, Islamabad, for her
constant and scholarly guidance, enriching and enlightening suggestions, precious and
insightful advice and her kind and sympathetic demeanor, which not only enabled me to
carry out this research work and bring my thesis into final shape but also helped me to
build a strong and viable foundation for the future research ventures. Besides providing
wonderful insight into research areas, she has left deep and lasting imprints on my
thinking and personality.
I also humbly acknowledge insightful and inspiring guidance of Respected
Prof. Dr. Muhammad Aslam Noor, Department of Mathematics, CIIT, Islamabad, for
his scholarly, perceptive and insightful guidance during my course work.
I also humbly acknowledge and appreciate the role of Honorable Rector
Dr. S.M. Junaid Zaidi, CIIT, Pakistan, the Dean, Faculty of Sciences and the
Head, Department of Mathematics, CIIT, Islamabad, in providing a truly international
standard research environment, state of the art research facilities and a student friendly
atmosphere.
Words always fail to me to acknowledge my parents who have always been guiding stars
and a constant source of inspiration and encouragement for me. I also acknowledge the
moral and financial support of my family members who have always backed me up and
motivated me to achieve my goals.
ix
I also acknowledge and appreciate the open and warm hearted support and helpful
advices of my fellow Mohsan and seniors Asif, Saira, Zakir who always spared
precious hours for me inspite of their own hectic schedules.
Last but not the least, I also express my deep gratitude to Higher Education
Commission of Pakistan for providing me the much needed financial support in the
form of Indigenous Fellowship Program as well as the access to the latest research.
Sarfraz Nawaz
CIIT/SP09–PMT– 015/ISB
x
ABSTRACT
Certain Subclasses of Analytic Functions Associated
with Conic Domains
Geometric Function Theory is the branch of Complex Analysis which deals with the
study of geometric properties of analytic functions. While studying the geometric
properties of analytic functions, we are mainly concerned with the geometry of image
domains of analytic functions. On the basis of shape and other properties of image
domain, analytic functions are categorized into many classes and then into subclasses.
Only a few geometrical structures have been introduced as image domain in which conics
is of great importance.
The main focus of this study is to develop conic domains and to introduce some new
geometrical structures as image domains. Our aim is to develop and refine already known
conic domains and also to introduce certain new generalized domains and their associated
functions. Also we deal with generalized circular domain and introduce certain new
classes of analytic functions representing conic and circular domains simultaneously
which is the main motivation of this work.
TABLE OF CONTENTS
1 Introduction 8
1.1 Historical background . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
1.2 Geometric Function Theory in today�s sciences . . . . . . . . . . . . . . . 11
1.3 Preface . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12
2 Preliminary Concepts and De�nitions 17
2.1 Analytic and univalent functions . . . . . . . . . . . . . . . . . . . . . . . 18
2.1.1 Analytic Functions . . . . . . . . . . . . . . . . . . . . . . . . . . 18
2.1.2 Univalent Functions . . . . . . . . . . . . . . . . . . . . . . . . . . 19
2.2 The class P of functions with positive real part . . . . . . . . . . . . . . 21
2.3 Some subclasses of univalent functions . . . . . . . . . . . . . . . . . . . 23
2.4 Certain subclasses of analytic functions of order beta . . . . . . . . . . . 26
2.5 Subordination and di¤erential subordination . . . . . . . . . . . . . . . . 27
2.6 Conic domains and associated functions . . . . . . . . . . . . . . . . . . . 28
2.6.1 Hyperbolic, parabolic and elliptic domains . . . . . . . . . . . . . 28
2.6.2 Circular domains . . . . . . . . . . . . . . . . . . . . . . . . . . . 34
2.7 The class Vm of functions with bounded boundary rotation and related
classes . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 36
2.7.1 The class Vm of functions with bounded boundary rotation . . . . 36
2.7.2 The class Rm of functions with bounded radius rotation . . . . . . 37
2.7.3 The class Pm . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
2.8 Ruscheweyh derivative . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
1
2.9 Hypergeometric functions . . . . . . . . . . . . . . . . . . . . . . . . . . 40
2.9.1 Con�uent hypergeometric function . . . . . . . . . . . . . . . . . 40
2.9.2 Gaussian hypergeometric function . . . . . . . . . . . . . . . . . . 41
2.10 Preliminary results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 41
3 On Generalized �-Convex Functions Associated with Conic Domain 44
3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
3.2 Main results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 47
3.3 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 60
4 On a New Class of Analytic Functions Associated with Conic Domain 61
4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 62
4.2 Main results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 67
4.3 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77
5 On Bounded Boundary and Bounded Radius Rotation Related with
Janowski Function 78
5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 79
5.2 Preliminary Lemmas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81
5.3 Main Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 82
5.4 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 92
6 OnGeneralization of a Class of Analytic Functions De�ned by Ruscheweyh
Derivative 93
6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 94
6.2 Preliminary Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 95
6.3 Main Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 96
6.4 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 107
7 On Janowski Functions Associated with Conic Domains 108
2
7.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 110
7.2 Main results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 114
7.3 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 128
8 Conclusion 129
9 References 131
3
4
LIST OF FIGURES
Fig 2.1 Convex and starlike domains ...………………………………………24
Fig 2.2 Boundaries of conic regions defined by kΩ ...……………………….30
Fig 4.1 View of 1.2 , 0.5Ω ………………………………………………………65
Fig 4.2 Contraction of kΩ ……………………………………………………66
Fig 4.3 Magnification of kΩ …………………………………………………66
Fig 7.1 Boundary of domain [ ]0.5, 0.5kΩ − ………………………..………111
Fig 7.2 Boundary of domain [ ]0.8,0.2kΩ …………………..…...…………111
Fig 7.3 View of [ ],k A BΩ when 1, 1A B→ →− ……….…….….………..112
Fig 7.4 Close view of Fig. 7.3 ……………………………….…………..….112
5
LIST OF ABBREVIATIONS
Set of complex numbers
E Open unit disk
A The class of normalized analytic functions
S Class of univalent functions
C Class of convex univalent functions *S Class of starlike univalent functions
( )k z Koebe function
P Class of analytic functions with positive real parts
( )0L z Möbius function
Mα Class of α -convex functions
( )P β Class of analytic functions with real part greater than beta
( )C β Class of convex univalent functions of order beta
( )*S β Class of starlike univalent functions of order beta
≺ Subordination symbol
Δ Family of Schwarz functions
UCV Class of uniformly convex functions
UST Class of uniformly starlike functions
ST Class of corresponding starlike functions
Ω Parabolic domain
kΩ Conic domain
k UCV− Class of k-uniformly convex functions
6
k ST− Class of k-starlike functions
( ),G k β , ,k βΩ Conic domain of order beta
( ),KD k β Class of k-uniformly convex functions of order beta
( ),SD k β Class of k-starlike functions of order beta
[ ],P A B Class of Janowski functions
[ ],A BΩ Circular domain
[ ],C A B Janowski convex functions
[ ]* ,S A B Janowski starlike functions
[ ], ,A B βΩ Circular domain of order beta
[ ], ,P A B β Class of Janowski functions of order beta
mV Class of functions with bounded boundary rotation
mR Class of functions with bounded radius rotation
mP Class of functions with bounded turnings
f g∗ Convolution of f and g
Dδ Ruscheweyh derivative of order δ
( ). n Pochhammer symbol
( )1 1 , ;F a c z Confluent hypergeometric function
( )2 1 , , ;F a b c z Gaussian hypergeometric function
( ),UM k α Class of α -convex functions associated with conic domain
( ), ,k UB α β γ− Class of generalizedα -convex functions associated with
conic domain
( ),k a bΩ Generalized conic domain
7
( ),k UCV a b− Class of k-uniformly convex functions of type ( ),a b
( ),k ST a b− Class of k-starlike functions of type ( ),a b
[ ], ,mV A B β Class of Janowski functions with bounded boundary
rotation and order beta
[ ], ,mR A B β Class of Janowski functions with bounded radius rotation
and order beta
[ ],k A BΩ Modified conic domain
[ ],k UCV A B− Class of k-uniformly Janowski convex functions
[ ],k ST A B− Class of k-starlike Janowski functions
Chapter 1
Introduction
8
1.1 Historical background
Geometric Function Theory is the branch of complex analysis which deals with the geo-
metric properties of analytic functions. This branch of mathematics is not as old as
the other branches are. We know that there are mappings in complex valued functions
f (z) ; z 2 D � C; in which the image domains f (D) are of major interest. The analytic
functions got more attraction in 1851, when Bernard Riemann allowed to replace any
arbitrary domain D with the open unit disk E = fz : jzj < 1g, by giving the famous
Riemann Mapping Theorem. This theorem gave rise to the birth of fascinating area of
mathematics, called Geometric Function Theory. Riemann made signi�cant contribution
to develop this area of mathematics.
In 1907, Koebe [24] initiated the theory of univalent functions by discovering functions
which are both analytic and univalent in open unit disk E: The set of such functions f
which are analytic and univalent in open unit disk E and are normalized by the conditions
f (0) = 0; f 0 (0) = 1 was then called the class S: This class S became the core ingredient
of advance research in this �eld. Many subclasses of class S of univalent functions were
de�ned on the basis of geometry of image domains, from which the classes C and S�
of convex and starlike univalent functions respectively have been of major interest. The
class P of functions with positive real part played an important role in setting the criteria
for convexity and starlikeness of univalent functions. In 1913, Study [105] used this class
P in setting the criteria for convexity of univalent functions. In 1915, Alexander [7]
established a beautiful relation between these classes of starlike and convex functions.
After Koebe, Bieberbach[24] in 1916 proved the second coe¢ cient estimate of func-
tions of S. He made remarkable contribution to this �eld by giving a famous open
problem regarding the coe¢ cient estimates of functions of S and named this problem as
Bieberbach�s conjecture. This problem remained open as a challenge for a wide number
of mathematicians working in this area and was �nally settled by de-Branges [19] in
1984. Bieberbach�s conjecture lasted as an ambitious problem of the �eld and got the at-
traction of many researchers. Due to complications in proving the famous Bieberbach�s
9
conjecture, researchers used to prove it for particular types of univalent functions. In
1921, Nevanlinna [55] proved the coe¢ cient estimate of starlike functions and gave the
criteria for starlikeness of univalent functions, see [24]. After that, a chain of researchers
contributed a lot to many developments and innovations in these two basic subclasses of
univalent functions and applied several di¤erential and integral operators, see for example
[20, 24, 27, 38, 53, 90, 91, 98, 103].
In 1917, Löwner [50] introduced the concept of functions with bounded boundary
rotation which was developed in more re�ned and systematic way by Paatero [84]. He
denoted the class of function with bounded boundary rotation by Vm; m � 2: Tammi
[106] introduced the class Rm; m � 2 of functions with bounded radius rotation in
1952. These concepts of bounded boundary and bounded radius rotation opened a new
direction of research and drew much attention of scholars. Several authors like Kirwan
[37], Brannan [11, 12], Pinchuk [87] and Noor [61, 64, 69, 76, 77, 78] wrote remarkable
research articles and played signi�cant role in developing this area of Geometric Functions
Theory. In 1971, Pinchuk [87] introduced the class Pm; m � 2 by using the concept of
functions with bounded boundary rotations and gave the criterion for functions to be
from Vm or Rm:
As we have discussed in the beginning that while studying the analytic functions f;
their image domain f (E) is of great importance. On the basis of the shapes of image
domains, various classes have been de�ned and studied. In 1973, by using the concept of
subordination which was given by Lindelöf [41], Janowski [30] introduced the concept of
circular domain [A;B] and de�ned the class P [A;B] of functions which map the open
unit disk onto the circular regions, called Janowski functions. A number of renowned
researchers studied these functions and several new classes of analytic functions associated
with circular domains have been introduced and studied, see for example [26, 47, 67, 68].
In 1991, Goodman [22, 23] initiated the idea of conic domains by introducing the classes
of uniformly convex and uniformly starlike functions. Later, Rønning [95], Ma and Minda
[51] independently found a most suitable form of Goodman criteria of these classes and
10
re�ned the parabolic domain. With the analogy of Alexander relation, Rønning [97]
introduced and studied the class of starlike functions corresponding to uniformly convex
functions, we will discuss these developments in section 1.3. Finally, in 1999, Kanas and
Wisniowska [36, 35] generalized the parabolic domain and introduced the general conic
domain k; k � 0 which represents all the three conic structures(hyperbola, parabola
and ellipse). They contributed remarkably in the study of conic domains. Furthermore, a
large number of renowned mathematicians like Sirivastava, Noor, Acu, Owa etc. studied
these conic domains, see [1, 2, 3, 34, 82, 104].
Geometric Function Theory is a wide research area. In above, we took a glimpse of
the developments which lead us to the theme of this thesis and to keep into the essence,
we omit the rest of developments in this �eld.
1.2 Geometric Function Theory in today�s sciences
Geometric Function Theory has recently found many applications in various �elds of ap-
plied sciences such as nonlinear integrable system theory, �uid dynamics, modern math-
ematical physics and the theory of partial di¤erential equations. Conformal mapping is
used to solve eigen value problem in plane and that method is called conformal transplan-
tation, see [38]. The theory of compact Riemann surfaces is widely used in constructing
�nite-gap solutions to nonlinear integrable systems, see [10] To compute the uniform po-
tential �ow around an assembly of circular obstacles is a basic and fundamental problem
in �uid mechanics and it is also a prototypical example of a physical problem involving a
multiply connected domains. The Schottky-Klein prime function is a special function of
complex variable which proves to be very useful in solving a range of problems in Geo-
metric Function Theory. Crowdy [17] made a comprehensive survey on the applications
of Geometric Functions Theory and used the Schottky-Klein prime function in prob-
lems involving multiply connected domain. For more applications of Geometric Function
Theory, we refer to [17, 18, 25, 107, 108].
11
1.3 Preface
As it is evident from the title "Certain Subclasses of Analytic Functions Asso-
ciated with Conic Domains" of this thesis, we are mainly focusing on the study of
conic domains including the circular domains, because somehow circle is a special case of
ellipse. But in the study of image domains, we see that circular domains are de�ned in a
distinctive way and are not deduced from general conic domains as special cases, so we
study them in separate manner. Our aim is to develop and re�ne these already known
conic domains and also to introduce certain new generalized domains and their associ-
ated functions. Also we deal with generalized circular domain and introduce certain new
classes of analytic functions representing conic and circular domains simultaneously.
From the above sequential historical overview of this �eld, we �nd that Goodman
[22, 23] in 1991 initiated the concept of conic domain but unintentionally. It is well
known that for any convex function f (z) ; not only f (E) but also the images of all
circles lying in E centered at origin are convex arcs. Pinchuk raised a question that
whether this property remains valid for circles centered at other points or not. Goodman
[22] replied in negative and introduced the class of functions which obey this property.
He named such functions as uniformly convex functions and denoted the class of such
functions by UCV: He also introduced the class UST of uniformly starlike functions
which map the circles lying in E centered at other points onto star shaped arcs, see [23].
He not only just de�ned these classes but also gave the analytic conditions for uniform
convexity and uniform starlikeness. By using these analytic conditions, these classes can
be de�ned as
UCV =
�f 2 A : Re
�1 + (z � �)
f 00 (z)
f 0 (z)
�> 0; z; � 2 E
�;
UST =
�f 2 A : Re
�(z � �) f 0 (z)
f (z)� f (�)
�> 0; z; � 2 E
�:
These classes coincide with the classes C and S� respectively when we take circles centered
12
at origin (that is � = 0). The famous Alexander�s relation stating the fact that f 2 C
if and only if zf 0 2 S� is fails to hold between UCV and UST: This fact is evident
from above de�nitions and can also be illustrated by two counter examples, given in [22].
Due to this reason, the class UST became unpopular but Rønning [97] �lled this gap by
introducing the class
ST = ff 2 A : f (z) = zg0 (z) ; g 2 UCV g
which is associated with the class UCV by Alexander type relation. He further proved
in [97] that neither UST ST nor ST UST: Later, again Rønning [95], and Ma
and Minda [51] independently gave the most suitable one variable characterization of the
class UCV and de�ned it as
UCV =
�f 2 A : Re
�1 +
zf 00 (z)
f 0 (z)
�>
����zf 00 (z)f 0 (z)
���� ; z 2 E� :Similarly, the class ST took the following form.
ST =
�f 2 A : Re
�zf 0 (z)
f (z)
�>
����zf 0 (z)f (z)� 1���� ; z 2 E� :
This characterization gave birth to the �rst conic (parabolic) domain
= fw : Rew > jw � 1jg :
This domain was then generalized by kanas and Wisniowska [36, 35] and introduced the
domain
k = fw : Rew > k jw � 1j ; k � 0g :
This conic domain represents the right half plane for k = 0; hyperbolic regions when
0 < k < 1; parabolic region for k = 1 and elliptic regions when k > 1: They also
introduced the class k�UCV of k-uniformly convex functions and k�ST of corresponding
13
k-starlike functions.
This thesis is aimed with the study of these classes associated with conic domains
and to introduce certain new classes of analytic functions associated with conic domains.
The chapter wise overview is as under.
Chapter 2 consists of some preliminary concepts and de�nitions. It starts with
the concept of analytic functions and normalized univalent functions in open unit disk
E and covers the basic subclasses of univalent functions. The class P of functions with
positive real parts is discussed in some detail and its generalization with regard to order �
(0 � � < 1) is discussed. The concept of subordination followed by a short survey of conic
domains is included. Also a detailed introduction of circular domains given by Janowski
[30] is provided. The functions with bounded boundary and bounded radius rotation are
reviewed. A well-known linear operator named as the Ruscheweyh di¤erential operator is
given which will be used in one of our upcoming chapters. At the end, some preliminary
results are included which will be utilized in subsequent chapters. It is important to
mention that no new de�nition or result is included in this chapter and all the contents
are known and properly referred.
The class UM (�; k) of �-convex functions associated with conic domains is intro-
duced by Kanas [31] and this class gives k-uniformly convex and corresponding k-starlike
functions as special cases. Also the class M� of �- convex functions is obtained as the
special case of UM (�; k) as UM (�; 0) � M�: In chapter 3, we generalize the class
UM (�; k) and introduce the generalized class k � UB (�; �; ) : This class gives several
known classes as special cases. Many interesting properties of this class are investigated
here and many known results are deduced from our main results as special cases. This
work has been published in "Mathematical and Computer Modelling, Vol 55; 2012; Pages
844� 852", see [74].
As mentioned earlier, the conic domain k; k � 0 was introduced and comprehen-
sively studied by Kanas and Wisniowska [36, 35]. These conic regions were restricted
to have �xed vertices and lengths of latus rectum. These conic domains could neither
14
be contracted nor magni�ed. We have recently removed this de�ciency of conic domain
k; k � 0 by introducing a generalized conic domain k (a; b) ; k � 0: This generalized
conic domain gives contraction as well as magni�cation of the conic domain k; k � 0: A
number of conic regions of any size can be obtained from this generalized conic domain
k (a; b) ; k � 0 by assigning suitable values to parameters a and b: In chapter 4, we
have given a detailed overview of generalized conic domain k (a; b) ; k � 0 and discussed
all of its aspects. Di¤erent views of this generalized conic domain for speci�c values of pa-
rameters are shown graphically for better understanding of the behaviour of this domain.
The class k�P (a; b) of functions which map the open unit disk E onto these generalized
conic regions is de�ned and some of its properties are discussed. Related to the class
k� P (a; b) ; two more classes k�UCV (a; b) and k� ST (a; b) are introduced and some
results concerning these classes are investigated. All contents of this chapter have been
published in a well reputed journal "Computers and Mathematics with Applications, Vol
62; 2011; Pages 367� 375", see [70].
In chapter 5, we have studied the class P [A;B; �] of generalized Janowski functions
of order � along with the functions with bounded boundary and bounded radius rotation.
The order of a function from the class Vm[A;B; �] of Janowski functions with bounded
boundary rotation to be from Rm[A;B; �] of Janowski functions with bounded radius
rotation is of major interest and some of its applications are also the part of our discussion.
Our main results present an advancement of already known results. It is to be mentioned
here that this work has also been published in "World Applied Sciences Journal, Vol
12(6) 2011, Pages 895� 902", see [79].
In 1994, Latha and Nanjunda [39] introduced the class Vm (�; b; �) of analytic func-
tions by using the Ruscheweyh derivative. In chapter 6, we have generalized this class
Vm (�; b; �) with the concept of Janowski functions and introduced the class V�m [A;B; �; b] :
This generalized class contains many known classes. The coe¢ cient bound, inclusion re-
sult and a radius problem are investigated here. Several known results are also deducted
from our main results as special cases by assigning particular values to di¤erent parame-
15
ters.
In the study of analytic functions, geometry of image domain is no doubt of great
importance. Analytic functions are classi�ed into many classes and then into subclasses
depending upon the shape of image domain and other geometrical properties. It has
been a matter of discussion that there always exist analytic functions with di¤erent
geometrical structures as their image domains. In chapter 7, we have introduced a
few geometrical structures of oval and petal type shape as image domain which are
new in nature and de�ned the classes of functions which give these types of mappings.
The concepts of Janowski functions and conic domains are combined together to de�ne
a new domain k [A;B] which represents the oval and petal type regions. Di¤erent
graphical views of this new domain for speci�c values of parameters are shown in order
to have better understanding of the behaviour of this domain k [A;B] : This domain
gives both conic and circular domains as special cases which is the main motivation of
this chapter. Moreover, two new classes k�UCV [A;B] of k-uniformly Janowski convex
and k � ST [A;B] of k- Janowski starlike functions are introduced and our main results
are based on their properties. A number of already known classes of analytic functions
can easily be obtained from our new classes as special cases. The class SD (k; �) is also a
special case of our new class k�ST [A;B] : The coe¢ cient bound for the class SD (k; �),
proved by Owa et al. [83] is improved, that is, the coe¢ cient bound for class SD (k; �)
obtained from our main results as special case gives much better results as compared
to that one, proved by Owa et al. [83]. It is worthy to be mentioned that some of the
contents of this chapter have also been published in a well reputed journal "Computers
and Mathematics with Applications, Vol 62; 2011; Pages 2209� 2217", see[73].
16
Chapter 2
Preliminary Concepts and De�nitions
17
In this chapter, we will give a brief introduction of elementary concepts in order to have
a better understanding of the work presented in this thesis. It will start with the concept
of analytic and univalent functions. The class S of normalized univalent functions along
with its basic subclasses will be discussed. we will also give basic de�nition and properties
of functions with positive real part and discuss the functions with real part greater than
� (0 � � < 1). A short survey of conic domains with various interesting properties
will also be given. The concept of circular domains given by Janowski functions will be
included in detail. At the end, there will be some preliminary known results to be used
in henceforth coming chapters.
2.1 Analytic and univalent functions
In this �rst section, we brie�y discuss the class A of normalized analytic functions de�ned
in the open unit disk E = fz : jzj < 1g and the class S of normalized univalent functions.
Some properties of the class S are also discussed.
2.1.1 Analytic Functions
Analytic functions play a vital role in Geometric Function Theory. They are de�ned as
follows.
De�nition 2.1.1 A complex valued function w = f (z) of complex variable z is said to
be analytic at the point z0 in the domain D; if it is di¤erentiable at z0 and at every point
in the neighbourhood of z0: The function w = f (z) is analytic in D; if it has derivative
at each point of D:
The functions which are analytic in the whole complex plane are called entire func-
tions. The functions exp (z) ; sin z; cos z and the polynomial function are entire in nature.
For more details, see [20, 24].
18
In Geometric Function Theory, we are always concerned with a domain D: An as-
sumption of replacing an arbitrary domain D with an open unit disk E = fz : jzj < 1g
can be made due to the following Riemann Mapping Theorem [20, 24].
Theorem 2.1.1 (Riemann Mapping Theorem) For every simply connected domain
D � C with at least two boundary points, there exists a unique analytic function which
maps D onto the open unit disk E = fz : jzj < 1g :
Now we de�ne the basic class A of normalized analytic functions as follows.
De�nition 2.1.2 A function f is said to be in the class A; if it is analytic in the open
unit disk E and is normalized by the conditions f (0) = 0 and f 0 (0) = 1: That is, the
class A consists of analytic functions having Taylor�s series expansion of the form
f (z) = z +1Xn=2
anzn; z 2 E: (2.1.1)
2.1.2 Univalent Functions
A single valued function f is said to be univalent in an open unit disk E if it provides a
one-to-one correspondence between the open unit disk E and the image domain f (E) :
Various other terms (like simple or schlicht) are used for this concept. The domain f (E)
of univalent function f is simple domain (a domain which is not self overlapping). More
precisely, we de�ne univalent functions as follows. For details, we refer to [20, 24].
De�nition 2.1.3 A single valued function f is said to be univalent in an open unit disk
E if for z1; z2 2 E;
f (z1) = f (z2) implies that z1 = z2:
The function f is said to be locally univalent at a point z0 2 E if it is univalent in
some neighborhood of z0:
We are mainly interested in univalent functions that are also analytic in E. Such
functions form the class S which is de�ned as follows.
19
De�nition 2.1.4 The functions analytic, univalent and normalized by the conditions
f (0) = 0 and f 0 (0) = 1 are said to form the class S: That is
S = ff 2 A : f is univalent in Eg :
The leading example of a function of class S is the Koebe function
k (z) =z
(1� z)2= z +
1Xn=2
nzn: (2.1.2)
The Koebe function maps E onto the entire plane minus the negative real axis from �14
to �1: Some other examples of functions in S are as follows.
1. f (z) = z; the identity mapping.
2. f (z) = z1�z2 ; which maps E onto the entire plane except the two half lines
12� x <
1 and �1 < x � �12:
3. f (z) = 12log�1+z1�z�; which maps E onto the horizontal strip ��
4< Im (w) < �
4:
The class S is preserved under a number of elementary transformations, see [20, 24].
Some of these transformations are given in the following theorem.
Theorem 2.1.2 [24] If f 2 S; then each of the following functions g is in S:
1. Conjugation
g (z) = f (z):
2. Rotation
g (z) = e�i�f�ei�z
�; � real.
3. Dilation
g (z) =1
tf (tz) ; 0 < t < 1:
20
4. Disk automorphism
g (z) =f�z+�1+�z
�� f (�)�
1� j�j2�f 0 (�)
; j�j < 1:
5. Omitted-value transformation
g (z) =f (z)
1� f(z)!
; where f (z) 6= !:
6. k-fold symmetry
g (z) = kpf (zk); where k is a positive integer.
In 1916, Bieberbach conjectured that if f 2 S and has the form (2:1:1), then janj �
n; n � 2; see [24]. Many attempts were made to prove it. A number of mathematicians
tried to prove it but �nally, Louis De�Branges got the honor to settle this conjecture and
now it is named as �de�Branges Theorem�, see [19].
2.2 The class P of functions with positive real part
It was observed that wherever there are so many complex valued functions whose image
domains cover the whole complex plane, there also exist functions with image domains
restricted to the open half plane. It was needed that such functions should be normalized
as it was done in the study of univalent functions. The class of such functions was named
as the class P; see [24].
De�nition 2.2.1 The class P consists of those analytic functions p which are normalized
by the condition p (0) = 1 and Re p (z) > 0; z 2 E: That is,
p 2 P : p (z) = 1 +1Xn=1
cnzn if and only if Re p (z) > 0; z 2 E: (2.2.1)
21
The most common example of functions from this class is the Möbius function
L0 (z) =1 + z
1� z: (2.2.2)
We note that
1. The class P is a convex set.
2. The function p 2 P need not be univalent. Justi�cation can be given by taking
p (z) = 1 + zn because it is in P for all n � 0 but it is not univalent for n � 2:
Herglotz [28] de�ned the function from class P in some other way by introducing their
valuable integral representation as follows.
Theorem 2.2.1 A function p is in the class P if and only if it can be expressed as
p (z) =1
2�
2�Z0
1 + ze�it
1� ze�itd� (t) ; for every z 2 E;
where � (t) is a non-decreasing real valued function such that
2�Z0
d� (t) = 2�:
In the following, we discuss the coe¢ cient estimate of functions from the class P; see
[24].
Theorem 2.2.2 Let p 2 P and be given by (2:2:1) : Then, for n � 1;
jcnj � 2:
This bound is sharp. Equality holds for L0; given by (2:2:2) :
22
In 1935, Noshiro [81] and Warschawski [109] independently gave the following beau-
tiful and simple criteria for univalence which connects the class P to the univalent func-
tions. They used the general convex domain which we will discuss in next section in some
detail.
Theorem 2.2.3 (Noshiro-Warschawski Theorem) Suppose that for some real �; we
have
Re�ei�f 0 (z)
�> 0
for all z in a convex domain D: Then f is univalent in D:
For proof, see [24].
2.3 Some subclasses of univalent functions
Analytic functions are classi�ed into certain subclasses on the basis of geometry of their
image domains. The most commonly studied classes are the classes of starlike, convex,
close-to-convex and quasi-convex functions. This classi�cation was started when the at-
tempts to prove the Bieberbach conjecture were made. Due to the complications and then
failure in proving the coe¢ cient bound for the class S of univalent functions, researchers
used to prove it for particular types of univalent functions and as a result we have many
subclasses of univalent functions which have also been studied in multivalent feature.
Now we take a little view of certain subclasses of normalized univalent functions which
are de�ned by natural geometrical conditions. We will also discuss their inter relations
and coe¢ cient bounds. For details, we refer to [20, 24].
De�nition 2.3.1 A set D in a plane is said to be starlike with respect to a point w0 2 D
if the linear segment joining w0 to every other point w 2 D lies entirely in D: In more
picturesque language, the requirement is that every point of D be �visible� from w0: A
function which maps the open unit disk E onto a domain that is starlike with respect
to the origin is called starlike function. The subclass of S consisting of all the starlike
23
functions is denoted by S�: The Koebe function de�ned by (2:1:2) is the best example of
starlike function. Example of starlike domain is shown in Figure 2.1 (ii).
De�nition 2.3.2 A set D in a plane is said to be convex if it is starlike with respect to
each of its points; that is, if the linear segment joining any two points of D lies entirely in
D: A function which maps the open unit disk E onto a convex domain is called a convex
function. The subclass of S consisting of all the convex functions is denoted by C: The
function
f (z) =z
1� z
is the leading example of the convex function. Example of convex domain is shown in
Figure 2.1 (i).
Figure 2.1: Convex and starlike domains
The following two theorems give an analytic description of starlike and convex functions.
The following theorem is due to Nevanlinna [55].
Theorem 2.3.1 A function f 2 S is said to be in the class S� of starlike univalent
functions if and only ifzf 0 (z)
f (z)2 P: (2.3.1)
The following analytic condition for convex functions is due to Study [105].
24
Theorem 2.3.2 A function f 2 S is said to be in the class C of convex univalent
functions if and only if(zf 0 (z))0
f 0 (z)2 P: (2.3.2)
It is noted that C � S� � S: In 1915, Alexander [7] built the following beautiful
relation between the classes of starlike and convex functions, for more detail, see[24].
Theorem 2.3.3 (Alexander�s Relation) Let f 2 A: Then f 2 C if and only if zf 0 2
S�:
This can be rephrased as:
If F (z) is in S�; thenzR0
F (�)�d� is in the class C:
The following two theorems give the coe¢ cient bounds for starlike and convex func-
tions, for reference, see [24].
Theorem 2.3.4 Let f 2 S� and be given by (2:1:1) : Then for z 2 E;
janj � n; n = 2; 3; 4; : : : :
This bound is sharp and equality holds for any rotation of the Koebe function de�ned by
(2:1:2) :
Theorem 2.3.5 Let f 2 C and be given by (2:1:1) : Then for z 2 E;
janj � 1; n = 2; 3; 4; : : : :
This bound is sharp and equality holds for the function f0 (z) = z1�z :
In 1969, Mocanu [54] introduced the concept of ��convexity as follows.
De�nition 2.3.3 Let � � 0 and if f 2 A; f(z)zf 0 (z) 6= 0 and
(1� �)zf 0 (z)
f (z)+ �
(zf 0 (z))0
f 0 (z)2 P;
25
then f is said to be an �-convex function. The class of such functions will be denoted by
M�:
We see that M0 � S� and M1 � C: It has been shown in [54] that M� � S�; � � 0
and for � � 1; M� consists entirely of convex functions.
2.4 Certain subclasses of analytic functions of order
beta
In 1936, Robertson [92] introduced the concept of order of analytic functions. He de�ned
as follows.
De�nition 2.4.1 A function p is said to be in the class P (�) ; 0 � � < 1; if and only
if there exists a function p1 2 P such that
p (z) = (1� �) p1 (z) + �; z 2 E: (2.4.1)
That is, the class P (�) ; 0 � � < 1 consists of functions for which Re p (z) > � for
z 2 E and is the subclass of the class P:
Using the class P (�) ; 0 � � < 1; the classes of starlike and convex functions of order
� can be de�ned as follows.
S� (�) =
�f 2 A : zf
0 (z)
f (z)2 P (�) ; z 2 E
�;
C (�) =
�f 2 A : (zf
0 (z))0
f 0 (z)2 P (�) ; z 2 E
�:
For more details, see [20, 24, 92].
26
2.5 Subordination and di¤erential subordination
The concept of subordination was introduced by Lindelöf [41] and further enriched by
Littlewood [42, 43] and Rogosinski [93, 94]. The concept of subordination is heavily
depending on the Schwarz functions. So before going to the de�nition of subordination,
we give the de�nition of Schwarz function.
De�nition 2.5.1 Let � be the family of functions w; analytic in the open unit disk E
and satisfying the condition w (0) = 0; jw (z)j < 1 for z 2 E: Then the function w is
called the Schwarz function.
De�nition 2.5.2 If f and g are analytic in E, we say that f is subordinate to g; written
symbolically as f � g; if there exists a Schwarz function w in E such that
f (z) = g (w (z)) ; z 2 E:
If g is univalent in E, then the subordination is equivalent to f (0) = g (0) and f (E) �
g (E) : That is, f � g will mean that every value taken by f in E is also taken by g:
Derivatives play an important role in function theory, specially in geometrical analysis
of functions. Obtaining information about the properties of function from the properties
of its derivative is a signi�cant practice in functions of real variables. A large number
of di¤erential inequalities have been de�ned and studied by many renowned mathemati-
cians. Also in the theory of complex valued functions, there are several di¤erential
implications in which a characterization of a function is determined from a di¤erential
condition as we have seen in analytic conditions for starlikeness and convexity, de�ned
respectively by (2:3:1) and (2:3:2) :
De�nition 2.5.3 ([53]) A di¤erential subordination is merely a generalization of dif-
ferential inequality of real variable. For example
First order di¤erential subordination (p (z) ; zp0 (z) ; z) � h (z) ;
27
Second order di¤erential subordination �p (z) ; zp0 (z) ; z2p00 (z) ; z
�� h (z) :
De�nition 2.5.4 ([53]) Let : C3 � E �! C and let h be univalent in E. If p is
analytic in E and satis�es the di¤erential subordination (second order)
�p (z) ; zp0 (z) ; z2p00 (z) ; z
�� h (z) ; (2.5.1)
then p is called a solution of the di¤erential subordination. The univalent function q
is called a dominant of the solutions of the di¤erential subordination, or more simply a
dominant, if p � q for all p satisfying (2:5:1). A dominant ~q that satis�es ~q � q for all
dominants q of (2:5:1) is said to be the best dominant of (2:5:1).
2.6 Conic domains and associated functions
In this section, we shall discuss about the main component of this work, called conic
domains and circular domains will also be included in second part of this section. Some-
how circle is a special case of ellipse but here we shall see that circular domains are not
acting as the special case of general conic domains. That�s why, we shall discuss circular
domains in a separate way.
2.6.1 Hyperbolic, parabolic and elliptic domains
In 1991, Goodman [22, 23] initiated the concept of conic domain but unintentionally. It
is well known that for any convex function f (z) ; not only f (E) but also the images of
all circles lying in E centered at origin are convex arcs. Pinchuk raised a question that
whether this property is still valid for circles centered at other points. Goodman [22]
replied in negative answer and introduced the class of functions which obey this property.
He named such functions as uniformly convex functions and denoted the class of such
functions by UCV: He also introduced the class UST of uniformly starlike functions
which map the circles lying in E centered at other points onto star shaped arcs, see [23].
28
He not only just de�ned these classes but also gave the analytic conditions for uniform
convexity and uniform starlikeness. By using these analytic conditions, these classes can
be de�ned as follows.
De�nition 2.6.1 A function f 2 A is said to be in the class UCV of uniformly convex
functions, if
Re
�1 + (z � �)
f 00 (z)
f 0 (z)
�> 0; z; � 2 E:
De�nition 2.6.2 A function f 2 A is said to be in the class UST of uniformly starlike
functions, if
Re
�(z � �) f 0 (z)
f (z)� f (�)
�> 0; z; � 2 E:
We see that when we take � = 0; these classes coincide with the classes C and S�
respectively. From above de�nitions of UCV and UST , we see that famous Alexander�s
relation is failed to hold between UCV and UST: This fact can also be illustrated by
two counter examples, given in [22]. Rønning [97] introduced the class
ST = ff 2 A : f (z) = zg0 (z) ; g 2 UCV g
which is associated with the class UCV by Alexander type relation. He further proved
in [97] that neither UST ST nor ST UST: Later, again Rønning [95], and Ma
and Minda [51] independently gave the most suitable one variable characterization of the
class UCV and de�ned it as follows.
De�nition 2.6.3 A function f 2 A is said to be in the class UCV of uniformly convex
functions, if
Re
�1 +
zf 00 (z)
f 0 (z)
�>
����zf 00 (z)f 0 (z)
���� ; z 2 E:Similarly, the class ST was de�ned in the following form.
De�nition 2.6.4 A function f 2 A is said to be in the class ST of corresponding starlike
functions, if
Re
�zf 0 (z)
f (z)
�>
����zf 0 (z)f (z)� 1���� ; z 2 E:
29
This one variable characterization gave birth to the �rst conic (parabolic) domain
= fw : Rew > jw � 1jg :
In 1999, Kanas and Wisniowska [36, 35] generalized the above parabolic domain and
introduced the conic domain k; k � 0 and studied it comprehensively. This domain is
de�ned as
k =
�u+ iv : u > k
q(u� 1)2 + v2
�: (2.6.1)
This domain represents the right half plane for k = 0; hyperbolic regions (right branch)
when 0 < k < 1; a parabolic region for k = 1 and elliptic regions when k > 1 as shown
in Figure 2.2 below.
Figure 2.2: Boundaries of conic regions de�ned by k
30
The functions which play the role of extremal functions for these conic regions are
given as:
pk(z) =
8>>>>>>>>><>>>>>>>>>:
1+z1�z , k = 0,
1 + 2�2
�log 1+
pz
1�pz
�2, k = 1,
1 + 21�k2 sinh
2��
2�arccos k
�arctanh
pz�, 0 < k < 1,
1 + 1k2�1 sin
0@ �2R(t)
u(z)ptR
0
1p1�x2
p1�(tx)2
dx
1A+ 1k2�1 , k > 1,
(2.6.2)
where u(z) = z�pt
1�ptz, t 2 (0; 1), z 2 E and z is chosen such that k = cosh
��R0(t)4R(t)
�, R(t)
is the Legendre�s complete elliptic integral of the �rst kind and R0(t) is complementary
integral of R(t), for more detail, see [36, 35]. If pk(z) = 1 + �kz + � � � ; then it is shown
in [32] that from (2:6:2) ; one can have
�k =
8>>><>>>:8(arccos k)2
�2(1�k2) ; 0 � k < 1;
8�2; k = 1;
�2
4(k2�1)pt(1+t)R2(t)
; k > 1:
(2.6.3)
These conic regions are being studied by several authors, for example see [4, 5, 6, 59, 75,
83, 101]. Kanas and Wisniowska [36] de�ned the class P (pk) of functions which map the
open unit disk E onto these conic regions as follows.
De�nition 2.6.5 A function p (z) such that p (0) = 1; is said to be in the class P (pk)
if it subordinates to pk (z) with z 2 E: That is, p (E) � pk (E) = k:
Moreover, a function p (z) from class P (pk) possesses the following properties, see
[36].
1. Re p (z) > kk+1
: That is, P (pk) � P�
kk+1
�; the class of functions with real part
greater than kk+1
:
31
2. jarg p (z)j <
8<: arctan 1k; 0 < k <1;
�2; k = 0:
Kanas and Wisniowska [36, 35] also de�ned and studied the class k � UCV of k-
uniformly convex functions and the corresponding class k � ST of k-starlike functions.
These classes were de�ned subject to the conic domain k; k � 0.
The classes k � UCV and k � ST are de�ned as follows:
De�nition 2.6.6 A function f (z) 2 A is said to be in the class k � UCV , if and only
if,(zf 0(z))0
f 0 (z)2 P (pk) ;
that is,(zf 0(z))0
f 0 (z)� pk(z); z 2 E; k � 0;
or equivalently,
Re
�(zf 0(z))0
f 0 (z)
�> k
����(zf 0(z))0f 0 (z)� 1���� ; k � 0:
De�nition 2.6.7 A function f (z) 2 A is said to be in the class k � ST , if and only if,
zf 0(z)
f (z)2 P (pk) ;
that is,zf 0(z)
f (z)� pk(z); z 2 E; k � 0; (2.6.4)
or equivalently,
Re
�zf 0(z)
f (z)
�> k
����zf 0(z)f (z)� 1���� ; k � 0:
The famous Alexander relation holds between these classes, in fact, the class k � ST
was de�ned from k � UCV by mean of Alexander relation as
k � ST = fg : g (z) = zf 0 (z) ; f (z) 2 k � UCV g :
32
That�s why it is called the corresponding class of k�UCV: Now we include some results
related to these classes which we will use in subsequent chapters as special cases.
Theorem 2.6.1 [36] A function f 2 A and of the form (2:1:1) is in the class k�UCV;
if it satis�es the condition
1Xn=2
n fn+ k (n� 1)g janj < 1; k � 0: (2.6.5)
Theorem 2.6.2 [35] A function f 2 A and of the form (2:1:1) is in the class k�ST; if
it satis�es the condition
1Xn=2
fn+ k (n� 1)g janj < 1; k � 0: (2.6.6)
Theorem 2.6.3 [36] Let f (z) 2 S: Then f (z) 2 k � UCV for jzj < r0; where
r0 =1
2 (k + 1) +p4k2 + 6k + 3
=2 (k + 1)�
p4k2 + 6k + 3
2k + 1:
The conic domain k was then generalized to G (k; �) ; k � 0; 0 � � < 1 by Shams
et al. [101] and is de�ned as
G (k; �) = fw : Rew > k jw � 1j+ �g : (2.6.7)
Subject to this conic domain, the classesKD (k; �) and SD (k; �) are de�ned and studied
by Shams et al. [101]. These classes are de�ned as follows.
De�nition 2.6.8 A function f (z) from A is said to be a member of the class KD (k; �)
if
Re
�(zf 0(z))0
f 0 (z)
�> k
����(zf 0(z))0f 0 (z)� 1����+ �; k � 0; 0 � � < 1:
Similarly, by mean of Alexander relation, the class SD (k; �) is de�ned as
SD (k; �) = fg : g (z) = zf 0 (z) ; f (z) 2 KD (k; �)g :
33
Shams et al. [101] also gave the following su¢ cient conditions for these classes.
Theorem 2.6.4 [101] A function f 2 A and of the form (2:1:1) is in the classKD (k; �) ;
if it satis�es the condition
1Xn=2
n fn (k + 1)� (k + �)g janj < 1� �;
where k � 0; 0 � � < 1:
Theorem 2.6.5 [101] A function f 2 A and of the form (2:1:1) is in the class SD (k; �) ;
if it satis�es the condition
1Xn=2
fn (k + 1)� (k + �)g janj < 1� �;
where k � 0; 0 � � < 1:
The domain G (k; �) is a generalization of k with regard to order � (0 � � < 1).
Noor [59] generalized the conic domain k with regard to order � on the other way. She
de�ned the conic domain k;� as
k;� = (1� �) k + �; 0 � � < 1:
2.6.2 Circular domains
It was Janowski [30] who introduced the circular domain in 1973 by de�ning Janowski
functions. He de�ned these functions as:
De�nition 2.6.9 A function h (z) is said to be in the class P [A;B] if it is analytic in
E with h (0) = 1 and
h (z) � 1 + Az
1 +Bz; � 1 � B < A � 1:
34
Geometrically, a function h (z) 2 P [A;B] maps the open unit disk E onto the domain
[A;B] de�ned by
[A;B] =
�w :
����w � 1� AB
1�B2
���� < A�B
1�B2
�: (2.6.8)
This domain represents an open circular disk centered on the real axis with diameter end
points D1 =1�A1�B and D2 =
1+A1+B
with 0 < D1 < 1 < D2: The class P [A;B] is connected
with the class P of functions with positive real parts by the relation
h (z) 2 P , (A+ 1)h (z)� (A� 1)(B + 1)h (z)� (B � 1) 2 P [A;B] : (2.6.9)
It is known [66] that P [A;B] is a convex set and also noted that P [1;�1] = P; the class
of functions with positive real parts and P [1� 2�;�1] = P (�) ; 0 � � < 1; the class of
functions with real part greater than �:
Janowski [30] also de�ned the classes C [A;B] and S� [A;B] of Janowski convex and
Janowski starlike functions as follows.
De�nition 2.6.10 A function f 2 A is said to be the class C [A;B], if and only if
(zf 0 (z))0
f 0 (z)2 P [A;B] :
De�nition 2.6.11 A function f 2 A is said to be the class S� [A;B], if and only if
zf 0 (z)
f (z)2 P [A;B] :
It is noted that the famous Alexander�s relation also holds for these classes, that is
f (z) 2 C [A;B] () zf 0 (z) 2 S� [A;B] :
These Janowski functions are being studied by several renowned mathematicians like
Noor [67, 68, 71, 72], Polato¼glu [88, 89], Cho [13, 14, 15, 16], Liu[44, 45, 46, 47, 48, 49]
35
etc.
The circular domain [A;B] was then generalized to [A;B; �] ; �1 � B < A �
1; 0 � � < 1 by Polato¼glu et al. [89]. This generalized domain is de�ned as
[A;B; �] =
�w :
����w � 1� [(1� �)A+ �B]B
1�B2
���� < (1� �) (A�B)
1�B2
�:
The class of functions which map the unit disk E onto the circular domain [A;B; �]
was named as P [A;B; �] : It is de�ned as follows.
De�nition 2.6.12 A function h (z) is said to be in the class P [A;B; �] if it is analytic
in E with h (0) = 1 and
h (z) � (1� �)1 + Az
1 +Bz+ �
=1 + [(1� �)A+ �B] z
1 +Bz; � 1 � B < A � 1; 0 � � < 1:
It is noted that P [A;B; 0] � P [A;B] and P [1;�1; 0] � P:
2.7 The class Vm of functions with bounded bound-
ary rotation and related classes
2.7.1 The class Vm of functions with bounded boundary rotation
It was Löwner [50] who initiated the concept of functions with bounded boundary rotation
but its extensive study was done by Paatero [84, 85]. Paatero explored the class Vm of
functions with bounded boundary rotations in following systematic way.
De�nition 2.7.1 A function f 2 A is said to be in the class Vm; if the variation of
36
tangent angle at the boundary of f (E) is at most m�; m � 2: That is, for m � 2;
2�Z0
����Re (zf 0 (z))0f 0 (z)
���� d� � m�; z 2 E;
Paatero [84, 85] also proved that for 2 � m � 4; the functions from Vm are univalent
also, that is, Vm � S; 2 � m � 4 and for m > 4; Vm consists of non-univalent functions
with radius of univalence ru = tan��m
�; proved by Kirwan [37]. It can easily be seen
that V2 consists of only convex univalent functions, that is, V2 � C: The class Vm has
been appearing as the ultimate part of advance research in this �eld of mathematics.
Noor wrote a number of article on its properties and applications, for example, see
[61, 64, 69, 76].
2.7.2 The class Rm of functions with bounded radius rotation
The class Rm of functions with bounded radius rotations was introduced by Tammi [106].
He de�ned it as follows.
De�nition 2.7.2 A function f 2 A is said to be in the class Rm; if for m � 2;
2�Z0
����Re zf 0 (z)f (z)
���� d� � m�; z 2 E;
It is noted that R2 consists of only starlike univalent functions, that is, R2 � S�: Also
the Alexander type relation holds between the classes Vm and Rm; that is
f 2 Vm () zf 0 2 Rm:
Noor wrote a number of article on its properties and applications, for example, see [78, 77].
37
2.7.3 The class Pm
In 1971, Pinchuk [87] introduced the class Pm of functions with bounded turnings. He
de�ned these functions as follows.
De�nition 2.7.3 A function p is said to be in the class Pm; if it is analytic in E satis-
fying p (0) = 1 and
p (z) =1
2�
2�Z0
1 + ze�it
1� ze�itd� (t) ; for every z 2 E;
where � (t) is a non-decreasing real valued function with bounded variation on [0; 2�] such
that, for m � 2;2�Z0
d� (t) = 2 and
2�Z0
jd� (t)j � m
or equivalently, if p is analytic in E satisfying p (0) = 1 and
2�Z0
jRe p (z)j d� � m�; m � 2:
This class Pm is connected with the class P of functions with positive real part by
the following relation.
For p (z) 2 Pm; we have
p (z) =
�m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z) ; (2.7.1)
where p1 (z) ; p2 (z) 2 P: It can easily be seen that P2 � P:
Using this class, the above classes Vm and Rm can also be de�ned as:
Vm =
�f 2 A : (zf
0 (z))0
f 0 (z)2 Pm
�;
Rm =
�f 2 A : zf
0 (z)
f (z)2 Pm
�:
38
2.8 Ruscheweyh derivative
Before going to discuss about Ruscheweyh derivative, we need the concept of convolution
which is de�ned as follows.
De�nition 2.8.1 Let f (z) =P1
n=0 anzn and g (z) =
P1n=0 bnz
n be two power series,
convergent in E: Then convolution or Hadamard product of these series, denoted by f �g;
is de�ned as
(f � g) (z) =1Xn=0
anbnzn; z 2 E:
In 1975, using the concept of convolution, Ruscheweyh [99] introduced a linear oper-
ator D� : A �! A: it is de�ned as
D�f (z) =z
(1� z)�+1� f (z)
= z +1Xn=2
'n (�) an zn; (� > �1) (2.8.1)
with
'n (�) =(� + 1)n�1(n� 1)! ; (2.8.2)
where (:)n is a Pochhammer symbol given as
(�)n =
8<: 1; n = 0;
� (�+ 1) (�+ 2) : : : (�+ n� 1) ; n 2 N:(2.8.3)
Moreover; we note that D0f (z) = f (z) ; D1f (z) = zf 0 (z) and
Dnf (z) =z (zn�1f (z))
(n)
n!; n 2 N0 = f0; 1; 2; :::g :
The symbol Dnf is called nth order Ruscheweyh derivative of the function f: The fol-
lowing identity can easily be established.
39
For a real number � (� > �1) ; we have
z�D�f (z)
�0= (� + 1)D�+1f (z)� �D�f (z) : (2.8.4)
For the applications of Ruscheweyh derivative; see [58, 60, 62, 63].
2.9 Hypergeometric functions
Hypergeometric functions are special functions, obtained as the solution of special types
of di¤erential equations. We discuss the following two types of hypergeometric functions.
2.9.1 Con�uent hypergeometric function
Let a and c be complex numbers with c 6= 0;�1;�2; :::. Then the con�uent (or Kummer)
hypergeometric function, denoted by 1F1 (a; c; z) or � (a; c; z) ; is de�ned as
1F1 (a; c; z) = 1 +a
c
z
1!+a (a+ 1)
c (c+ 1)
z2
2!+ :::
=1Xk=0
(a)k(c)k
zk
k!;
where (:)k is the Pochhammer symbol given by (2:8:3) :The following are some properties
of con�uent hypergeometric functions which will be used in our subsequent work.
Remark 2.9.1 [53] For real or complex numbers a; c (c 6= 0;�1;�2; : : :) and Re c >
Re a > 0; we have
1Z0
ta�1 (1� t)c�a�1 etzdt =� (a) � (c� a)
� (c)1F1 (a; c; z) ; (2.9.1)
1F1 (a; c; z) = ez 1F1 (c� a; c;�z) : (2.9.2)
40
2.9.2 Gaussian hypergeometric function
Let a; b and c be complex numbers with c 6= 0;�1;�2; :::. Then the Gaussian hyperge-
ometric function, denoted by 2F1 (a; b; c; z) or F (a; b; c; z) ; is de�ned as
2F1 (a; b; c; z) = 1 +ab
c
z
1!+a (a+ 1) b (b+ 1)
c (c+ 1)
z2
2!+ :::
=
1Xk=0
(a)k (b)k(c)k
zk
k!;
where (:)k is the Pochhammer symbol given by (2:8:3) : The following are some properties
of Gaussian hypergeometric functions which will be used in our subsequent work.
Remark 2.9.2 [53] For real or complex numbers a; b; c (c 6= 0;�1;�2; : : :) and Re c >
Re b > 0; we have
1Z0
tb�1 (1� t)c�b�1 (1� tz)�a dt =� (b) � (c� b)
� (c)2F1 (a; b; c; z) ; (2.9.3)
2F1 (a; b; c; z) = (1� z)�a 2F1
�a; c� b; c;
z
z � 1
�; (2.9.4)
2F1 (a; b; c; z) = 2F1 (b; a; c; z) : (2.9.5)
For more details of hypergeometric functions, we refer to [53].
2.10 Preliminary results
We need the following lemmas in our main results of subsequent chapters.
Lemma 2.10.1 [33] Let 0 � k < 1: Also, let �; � 2 C be such that � 6= 0 and
Re (�k= (k + 1) + �) > 0: If p (z) is analytic in E; p (0) = 1; p (z) satis�es
p (z) +zp0 (z)
�p (z) + �� pk (z) ; (2.10.1)
41
and q (z) is analytic solution of
q (z) +zq0 (z)
�q (z) + �= pk (z) ;
then q (z) is univalent, p (z) � q (z) � pk (z) ; and q (z) is best dominant of (2:10:1) :
Moreover, the solution q (z) is given by
q (z) =
��
Z 1
0
�t�+��1 exp
Z tz
z
pk (u)� 1u
du
��dt
��1� �
�:
For more details of best dominant, we refer to [33, 53].
Lemma 2.10.2 If f (z) � H (z) and g (z) � H (z) ; then for t 2 [0; 1] ;
(1� t) f (z) + tg (z) � H (z) :
Lemma 2.10.3 [29] Let the function w (z) be non-constant analytic in E with w (0) = 0:
If jw (z)j attains its maximum value on the circle jzj = r < 1 at a point z0; then
z0w0 (z0) = cw (z0) ;
c is real and c � 1:
Lemma 2.10.4 [53] Let u = u1 + iu2, v = v1 + iv2 and (u; v) be a complex valued
function satisfying the conditions:
(i) : (u; v) is continuous in a domain D � C2;
(ii) : (1; 0) 2 D and Re (1; 0) > 0;
(iii) : Re (iu2; v1) � 0; whenever (iu2; v1) 2 D and v1 � �12(1 + u22) :
If h (z) = 1 + c1z + � � � is a function analytic in E such that (h(z); zh0(z)) 2 D and
Re (h(z); zh0(z)) > 0 for z 2 E; then Reh(z) > 0 in E:
42
Lemma 2.10.5 [94] Let h (z) = 1 +1Pn=1
cnzn be subordinate to H (z) = 1 +
1Pn=1
Cnzn: If
H (z) is univalent in E and H (E) is convex, then
jcnj � jC1j ; n � 1:
43
Chapter 3
On Generalized �-Convex Functions Associated with
Conic Domain
44
The classM� of �- convex functions is de�ned in De�nition 2.3.3 and a detailed overview
of conic domains along with the relevant classes of functions is given in section 2.6.1. It
is evident from the de�nition of �-convex functions, convex and starlike functions can
be obtained as special cases of �-convex functions. The class UM (�; k) of �-convex
functions associated with conic domains is introduced by Kanas [31] and this class gives
k-uniformly convex and corresponding k-starlike functions as special cases. This class is
de�ned by subordinating the function
J (�; f (z)) = (1� �)zf 0 (z)
f (z)+ �
(zf 0 (z))0
f 0 (z)
to the extremal function pk (z) given by (2:6:2) : Also the classM� of �- convex functions
is obtained as the special case of UM (�; k) as UM (�; 0) �M�:
In this chapter, we will generalize the class UM (�; k) by generalizing the function
J (�; f (z)) and introduce the generalized class k � UB (�; �; ) : This class gives several
known classes as special cases. Many interesting properties of this class will be investi-
gated here and many known results can be deduced from our main results, we will show
this fact as corollaries.
It is also to be mentioned here that all the contents of this chapter have been published
in "Mathematical and Computer Modelling, Vol 55; 2012; Pages 844� 852", see [74].
3.1 Introduction
Let S� (�) ; C (�) denote the well-known classes of starlike and convex functions of order
� (0 � � < 1) respectively as discussed in section 2.4. The class k�UCV of k-uniformly
convex functions and corresponding class k � ST of k-starlike functions are introduced
and studied by Kanas and Wisniowska [36, 35] and discussed in section 2.6.1. These
classes were generalized to KD (k; �) and SD (k; �) respectively by Shams et al. [101]
as discussed in section 2.6.1.
Now we de�ne the following.
45
De�nition 3.1.1 A function f (z) 2 A is said to be in the class k�UB (�; �; ) ; k � 0;
if and only if, for � � 0; 0 � � < 1; 0 � < 1;
Re J (�; �; ; f (z)) > k jJ (�; �; ; f (z))� 1j ; (3.1.1)
where
J (�; �; ; f (z)) =1� �
1� �
�zf 0 (z)
f (z)� �
�+
�
1�
�1� +
zf 00 (z)
f 0 (z)
�: (3.1.2)
Special Cases
(i) k�UB (1; �; 0) = k�UCV and k�UB (0; 0; ) = k� ST; the well-known classes
of k-uniformly convex and k-starlike functions respectively, introduced by Kanas
and Wisniowska [36, 35].
(ii) k � UB (0; �; ) = SD (k; �) and k � UB (1; �; ) = KD (k; ) ; the well-known
classes, introduced and studied in [101].
(iii) k�UB (�; 0; 0) = UM (�; k) ; the well-known class, introduced and studied in [31].
(iv) 0� UB (�; 0; 0) =M�; the well-known class of alpha-convex functions, introduced
and studied in [54].
Similarly, several more special cases can be obtained from k � UB (�; �; ) by giv-
ing particular values to di¤erent parameters. That are 1 � UB (0; 0; ) = ST; 1 �
UB (1; �; 0) = UCV; 0�UB (0; 0; ) = S�; 0�UB (1; �; 0) = C; 0�UB (0; �; ) = S� (�)
and 0� UB (1; �; ) = C ( ) : For detail of these classes, see [22, 24, 97].
Geometrically, a function f (z) 2 A is said to be in the class k � UB (�; �; ), if and
only if, the function J (�; �; ; f (z)) takes all values in the conic domain k; given by
(2:6:1) : Taking this geometrical interpretation into consideration, one can rephrase the
above de�nition as:
46
A function f (z) 2 A is said to be in the class k�UB (�; �; ) ; k � 0; if and only if,
for � � 0; 0 � � < 1; 0 � < 1;
J (�; �; ; f (z)) � pk (z) ; (3.1.3)
where pk (z) is de�ned by (2:6:2) :
3.2 Main results
Our �rst result is a su¢ cient condition for a function f (z) 2 A to be from k�UB (�; �; ) :
It gives many known results as special cases as discussed after this result.
Theorem 3.2.1 A function f (z) of the form (2:1:1) is in the class k � UB (�; �; ) if
1Xn=2
n (k;�; �; ) < (1� �) (1� ) ; (3.2.1)
where
n (k;�; �; )
= (k + 1) f(n� 1) (1� �) (1� ) + n� (1� �) (n� 1)g janj
+ (k + 1)n�1Xj=2
f(j � 1) (1� �) (1� ) + � (1� �) (n� j)g (n+ 1� j) jajan+1�jj
+ (1� �) (1� ) (n+ 1) janj+ (1� �) (1� )n�1Xj=2
(n+ 1� j) jajan+1�jj :
Proof. Assuming that (3:2:1) holds, then it su¢ ces to show that
k jJ (�; �; ; f (z))� 1j � Re fJ (�; �; ; f (z))� 1g < 1:
47
Now consider
jJ (�; �; ; f (z))� 1j
=
����1� �
1� �
�zf 0 (z)
f (z)� �
�+
�
1�
�1� +
zf 00 (z)
f 0 (z)
�� 1����
=
����1� �
1� �
zf 0 (z)
f (z)� (1� �) �
1� �+ �+
�
1�
zf 00 (z)
f 0 (z)� 1����
=
����1� �
1� �
zf 0 (z)
f (z)� 1� �
1� �+
�
1�
zf 00 (z)
f 0 (z)
����
=
������������
(1� �) (1� ) zf 0 (z) f 0 (z)
� (1� �) (1� ) f (z) f 0 (z) + � (1� �) zf (z) f 00 (z)
(1� �) (1� ) f (z) f 0 (z)
������������: (3.2.2)
Now from (2:1:1) ; we have
zf 0 (z) f 0 (z) = z
1Xn=0
nanzn�1
! 1Xn=0
nanzn�1
!; a0 = 0; a1 = 1
=1
z
1Xn=0
nanzn
! 1Xn=0
nanzn
!
=1
z
1Xn=0
nXj=0
j (n� j) ajan�j
!zn
=1Xn=0
nXj=0
j (n� j) ajan�j
!zn�1
= z +
1Xn=3
nXj=0
j (n� j) ajan�j
!zn�1
48
= z +1Xn=2
n+1Xj=0
j (n+ 1� j) ajan+1�j
!zn
= z +1Xn=2
2nan +
n�1Xj=2
j (n+ 1� j) ajan+1�j
!zn:
Similarly, we can have
f (z) f 0 (z) = z +
1Xn=2
(n+ 1) an +
n�1Xj=2
(n+ 1� j) ajan+1�j
!zn
and
zf (z) f 00 (z) =1Xn=2
n (n� 1) an +
n�1Xj=2
(n+ 1� j) (n� j) ajan+1�j
!zn:
Using the above equalities in (3:2:2) ; we have
jJ (�; �; ; f (z))� 1j
=
����������������������
1Pn=2
[f2n (1� �) (1� )� (n+ 1) (1� �) (1� )
+n� (1� �) (n� 1)g an +n�1Pj=2
fj (1� �) (1� )
� (1� �) (1� ) + � (1� �) (n� j)g (n+ 1� j) ajan+1�j] zn
(1� �) (1� )
(z +
1Pn=2
(n+ 1) an +
n�1Pj=2
(n+ 1� j) ajan+1�j
!zn
)
����������������������
49
�
1Pn=2
j(n� 1) (1� �) (1� ) + n� (1� �) (n� 1)j janj
+1Pn=2
�����n�1Pj=2 f(j � 1) (1� �) (1� ) + � (1� �) (n� j)g (n+ 1� j) ajan+1�j
�����(1� �) (1� )
(1�
1Pn=2
(n+ 1) janj �1Pn=2
�����n�1Pj=2 (n+ 1� j) ajan+1�j
�����) :
(3.2.3)
Now from (3:2:3) ; we have
k jJ (�; �; ; f (z))� 1j � Re fJ (�; �; ; f (z))� 1g
� (k + 1) jJ (�; �; ; f (z))� 1j
�
(k + 1)1Pn=2
j(n� 1) (1� �) (1� ) + n� (1� �) (n� 1)j janj
+(k + 1)1Pn=2
�����n�1Pj=2 f(j � 1) (1� �) (1� ) + � (1� �) (n� j)g (n+ 1� j) ajan+1�j
�����(1� �) (1� )
(1�
1Pn=2
(n+ 1) janj �1Pn=2
�����n�1Pj=2 (n+ 1� j) ajan+1�j
�����) :
The last expression is bounded by 1 if
1Xn=2
[(k + 1) j(n� 1) (1� �) (1� ) + n� (1� �) (n� 1)j janj
+ (k + 1)n�1Xj=2
jf(j � 1) (1� �) (1� ) + � (1� �) (n� j)g (n+ 1� j) ajan+1�jj
+(1� �) (1� ) (n+ 1) janj+ (1� �) (1� )
n�1Xj=2
(n+ 1� j) jajan+1�jj#
< (1� �) (1� ) :
This completes the proof.
50
Corollary 3.2.1 When � = 0; then (3:2:1) reduces to
(1� �) (1� )
>1Xn=2
((k + 1) (n� 1) (1� ) janj+ (k + 1)
n�1Xj=2
(j � 1) (1� ) (n+ 1� j) jajan+1�jj
+(1� �) (1� ) janj+ (1� �) (1� )n�1Xj=1
(n+ 1� j) jajan+1�jj)
> (1� )1Xn=2
f(k + 1) (n� 1) + (1� �)g janj :
This implies that1Xn=2
fn (k + 1)� (k + �)g janj < 1� �;
which is the su¢ cient condition for f (z) 2 SD (k; �) ; proved in [101].
Corollary 3.2.2 When � = 1; then (3:2:1) reduces to
(1� �) (1� )
>1Xn=2
(n (k + 1) (n� 1) (1� �) janj+ (k + 1)
n�1Xj=2
(1� �) (n� j) (n+ 1� j) jajan+1�jj
+n (1� �) (1� ) janj+ (1� �) (1� )
nXj=2
(n+ 1� j) jajan+1�jj)
> (1� �)
1Xn=2
n f(k + 1) (n� 1) + (1� )g janj :
51
This implies that1Xn=2
n fn (k + 1)� (k + )g janj < 1� ;
which is the su¢ cient condition for f (z) 2 KD (k; ) ; proved in [101].
When � = 0; = 0; then Theorem 3.2.1 gives the following su¢ cient condition for
f (z) 2 UM (�; k) ; the class introduced by Kanas [31].
Corollary 3.2.3 A function f (z) of the form (2:1:1) is in the class UM (�; k) if
1Xn=2
n (k;�) < 1; (3.2.4)
where
n (k;�) = (k + 1) (n� 1) (1� �+ n�) janj
+(k + 1)n�1Xj=2
f(j � 1) (1� �) + � (n� j)g (n+ 1� j) jajan+1�jj
+(n+ 1) janj+n�1Xj=2
(n+ 1� j) jajan+1�jj :
Corollary 3.2.4 When � = 1; = 0; then (3:2:1) reduces to
1Xn=2
n fn+ k (n� 1)g janj < 1;
which is the su¢ cient condition for f (z) 2 k � UCV; proved in [36].
Corollary 3.2.5 When � = 0; � = 0; then (3:2:1) reduces to
1Xn=2
fn+ k (n� 1)g janj < 1;
which is the su¢ cient condition for f (z) 2 k � ST; proved in [35].
52
Corollary 3.2.6 When � = 0; k = 0; then (3:2:1) reduces to
1Xn=2
(n� �) janj < 1� �;
which is the su¢ cient condition for f (z) 2 S� (�) ; proved in [100].
Similarly, several more results can also be deduced from Theorem 3.2.1 by giving
particular values to the parameters.
The following is an inclusion result stating the fact that k�UB (�; �; ) � SD (k; �)
for some � = � (�; �; ) de�ned below.
Theorem 3.2.2 Let f (z) 2 k � UB (�; �; ) : Then f (z) 2 SD (k; �) ; where
� = 1� (1� �) (1� )
(1� �) (1� ) + � (1� �): (3.2.5)
Proof. Let1
1� �
�zf 0 (z)
f (z)� �
�= p (z) ; (3.2.6)
where p (z) is analytic in E and p (0) = 1: This implies that
zf 0 (z)
f (z)= (1� �) p (z) + �: (3.2.7)
Now di¤erentiating logarithmically, we have
1 +zf 00 (z)
f 0 (z)= (1� �) p (z) + � +
(1� �) zp0 (z)
(1� �) p (z) + �: (3.2.8)
53
Using (3:2:7) and (3:2:8) ; we have
J (�; �; ; f (z)) =1� �
1� �f(1� �) p (z) + � � �g
+�
1�
�(1� �) p (z) + � +
(1� �) zp0 (z)
(1� �) p (z) + ��
�
=
�1� �
1� �+
�
1�
�f(1� �) p (z) + �g
�(1� �) �
1� �� �
1� +
�
1�
(1� �) zp0 (z)
(1� �) p (z) + �:
Now for � = 1� (1��)(1� )(1��)(1� )+�(1��) ; we have
J (�; �; ; f (z)) = p (z) +1� �
1� �+
�
1� � 1
�(1� �) �
1� �� �
1� +
zp0 (z)1� �p (z) + �
1��
= p (z) +zp0 (z)
1� �p (z) + �
1��:
Since f (z) 2 k � UB (�; �; ) ; so we obtain
p (z) +zp0 (z)
1� �p (z) + �
1��� pk (z) ;
where pk (z) is de�ned by (2:6:2) : Since Ren1� �
kk+1
+ �1��
o> 0; z 2 E; therefore apply-
ing Lemma 2.10.1, we have
1
1� �
�zf 0 (z)
f (z)� �
�= p (z) � pk (z) ;
which implies that f (z) 2 SD (k; �) :
By giving particular values to di¤erent parameters in Theorem 3.2.2 we get the fol-
lowing well-known result, proved by Mocanu in [54].
54
Corollary 3.2.7 Let f (z) 2 0� UB (�; 0; 0) = M�: Then f (z) 2 SD (0; 0) = S�: That
is,
M� � S�; � � 0:
The following is the integral representation of functions from k � UB (�; �; ) :
Theorem 3.2.3 A function f (z) 2 k � UB (�; �; ) ; � 6= 0; if and only if, there is a
function g (z) 2 k � ST such that
f (z) =
24� zZ0
t��1�g (t)
t
� 1� �
dt
35 1�
; (3.2.9)
where � = 1 + (1��)(1� )�(1��) :
Proof. From (3:2:9) ; we can have
1
�(f (z))� =
zZ0
t��1�g (t)
t
� 1� �
dt
which reduces to
(f (z))��1 f 0 (z) = z��1�g (z)
z
� 1� �
:
Logarithmic di¤erentiation leads us to
(� � 1) zf0 (z)
f (z)+zf 00 (z)
f 0 (z)= (� � 1) + 1�
�
�zg0 (z)
g (z)� 1�
which implies that
zg0 (z)
g (z)=� (� � 1)1�
zf 0 (z)
f (z)+
�
1�
zf 00 (z)
f 0 (z)� � (� � 1)
1� + 1:
For � = 1 + (1��)(1� )�(1��) ; we have
zg0 (z)
g (z)=1� �
1� �
zf 0 (z)
f (z)+
�
1�
zf 00 (z)
f 0 (z)+�� �
1� �
55
which implies that
zg0 (z)
g (z)=
1� �
1� �
�zf 0 (z)
f (z)� �
�+
�
1�
�1� +
zf 00 (z)
f 0 (z)
�= J (�; �; ; f (z)) :
Now from (3:1:3) and using (2:6:4), we obtain the required result.
Theorem 3.2.4 Let f (z) 2 k � UB (�; �; ) : Then the function
g (z) = z
�f (z)
z
� 1��1��
(f 0 (z))�1� (3.2.10)
belongs to k � ST for all z 2 E:
Proof follows immediately from logarithmic di¤erentiation of (3:2:10).
Theorem 3.2.5 For � > �1 � 0;
k � UB (�; �; ) � k � UB (�1; �; ) :
Proof. Let f (z) 2 k � UB (�; �; ) : Then consider
J (�1; �; ; f (z)) =1� �11� �
�zf 0 (z)
f (z)� �
�+
�11�
�1� +
zf 00 (z)
f 0 (z)
�
=�1� �1
�
� 1
1� �
�zf 0 (z)
f (z)� �
�+�1�
�1� �
1� �
�zf 0 (z)
f (z)� �
�+
�
1�
�1� +
zf 00 (z)
f 0 (z)
��
=�1� �1
�
�J (0; �; ; f (z)) +
�1�J (�; �; ; f (z)) :
Now as f (z) 2 k � UB (�; �; ) ; so
J (�; �; ; f (z)) � pk (z) ;
56
which implies by Theorem 3.2.2,
J (0; �; ; f (z)) � pk (z) :
Using these along with the Lemma 2.10.2, we have
J (�1; �; ; f (z)) � pk (z) ;
which implies that f (z) 2 k � UB (�1; �; ) :
For the function f (z) 2 A; we consider the integral operator
Ia (f) =a+ 1
za
zZ0
ta�1f (t) dt; a = 1; 2; 3; � � � : (3.2.11)
This operator Ia was introduced by Bernardi [9]. In particular, the operator I1 was
studied earlier by Libera [40]. Now we prove the following.
Theorem 3.2.6 Let f (z) 2 k�UB (�; �; ) : Then Ia (f) 2 SD (k; �) ; where � is de�ned
by (3:2:5) :
Proof. From (3:2:11) ; we have
(a+ 1) za�1f (z) = (za (Iaf (z)))0
= za (Iaf (z))0 + aza�1 (Iaf (z))
which implies that
(a+ 1) f (z) = z (Iaf (z))0 + aIaf (z) :
57
Di¤erentiating logarithmically, we have
zf 0 (z)
f (z)=
z�z (Iaf (z))
0�0 + za (Iaf (z))0
z (Iaf (z))0 + aIaf (z)
=
z(z(Iaf(z))0)0
Iaf(z)+ a z(Iaf(z))
0
Iaf(z)
z(Iaf(z))0
Iaf(z)+ a
: (3.2.12)
Let z(Iaf(z))0
Iaf(z)= (1� �) p (z) + � with p (z) analytic in E and p (0) = 1: Then
z (Iaf (z))0 = f(1� �) p (z) + �g Iaf (z) :
Di¤erentiating, we have
�z (Iaf (z))
0�0 = (1� �) p0 (z) (Iaf (z)) + f(1� �) p (z) + �g (Iaf (z))0
which implies that
z�z (Iaf (z))
0�0Iaf (z)
= (1� �) zp0 (z) + [(1� �) p (z) + �]2 :
Using this in (3:2:12) ; we have
zf 0 (z)
f (z)=
(1� �) zp0 (z) + [(1� �) p (z) + �]2 + a [(1� �) p (z) + �]
[(1� �) p (z) + �] + a
= (1� �) p (z) + � +(1� �) zp0 (z)
(1� �) p (z) + � + a
= (1� �)h (z) + �; (3.2.13)
where
h (z) = p (z) +zp0 (z)
(1� �) p (z) + � + a: (3.2.14)
58
Now from (3:2:13) ; we have
1 +zf 00 (z)
f 0 (z)= (1� �)h (z) + � +
(1� �) zh0 (z)
(1� �)h (z) + �: (3.2.15)
Using (3:2:13) and (3:2:15) ; we have
J (�; �; ; f (z)) =1� �
1� �f(1� �)h (z) + � � �g
+�
1�
�(1� �)h (z) + � +
(1� �) zh0 (z)
(1� �)h (z) + ��
�
=
�1� �
1� �+
�
1�
�f(1� �)h (z) + �g
�(1� �) �
1� �� �
(1� )+
�
1�
(1� �) zh0 (z)
(1� �)h (z) + �:
Now for � = 1� (1��)(1� )(1��)(1� )+�(1��) ; we have
J (�; �; ; f (z)) = h (z) +1� �
1� �+
�
1� � 1
�(1� �) �
1� �� �
(1� )+
zh0 (z)1� �h (z) + �
1��
= h (z) +zh0 (z)
1� �h (z) + �
1��:
Since f (z) 2 k � UB (�; �; ) ; so
h (z) +zh0 (z)
1� �h (z) + �
1��� pk (z) ;
where pk (z) is de�ned by (2:6:2) : Since Ren1� �
kk+1
+ �1��
o> 0; z 2 E; therefore apply-
ing Lemma 2.10.1, we have
p (z) +zp0 (z)
(1� �) p (z) + � + a= h (z) � pk (z) :
59
Now as Re�(1� �) k
k+1+ � + a
> 0; z 2 E; so again using Lemma 2.10.1, we have
p (z) � pk (z) ;
which implies that Iaf (z) 2 SD (k; �) :
From the above theorem, one can easily deduce the following known [101, 9] results.
Corollary 3.2.8 Let f (z) 2 k � UB (0; �; ) = SD (k; �) : Then Ia (f) 2 SD (k; �) :
Corollary 3.2.9 Let f (z) 2 k � UB (0; 0; ) = k � ST: Then Ia (f) 2 k � ST:
Corollary 3.2.10 Let f (z) 2 0� UB (0; 0; ) = S�: Then Ia (f) 2 S�:
3.3 Conclusion
We generalized the class UM (�; k) by generalizing the function J (�; f (z)) and intro-
duced the class k�UB (�; �; ) : Several known classes are obtained from k�UB (�; �; )
as special cases. Many interesting properties of this class are investigated and many
known results are deduced from our main results which are included as corollaries.
60
Chapter 4
On a New Class of Analytic Functions Associated
with Conic Domain
61
In the geometry of image domain of analytic functions, conic domains have got great
importance due to their convexity and symmetry about the positive real axis. The study
of conic domains was initiated by Goodman [22, 23] for a particular case (parabolic
domain) and later, general conic domain k; k � 0 (all three cases) which we have
discussed in section 2.6.1 in some detail, was comprehensively studied by Kanas and
Wisniowska [36, 35] but these conic regions were restricted to have �xed vertices and
lengths of latus rectum. These conic domains could neither be contracted nor magni�ed.
We have removed this de�ciency of conic domain k; k � 0 by introducing a gen-
eralized conic domain k (a; b) ; k � 0: This generalized conic domain gives contraction
as well as magni�cation of the conic domain k; k � 0: A number of conic regions of
any size can be obtained from our de�ned generalized conic domain k (a; b) ; k � 0 by
assigning suitable values to parameters a and b:
In this chapter, we will give a detailed overview of generalized conic domaink (a; b) ; k �
0 and discuss all of its aspects. Di¤erent graphical views of this generalized conic domain
for speci�c values of parameters will be shown for better understanding of the behaviour
of this domain. The class k � P (a; b) of functions which map the open unit disk E onto
these generalized conic regions will be de�ned and some of its properties will be discussed.
Related to the class k � P (a; b) ; two more classes k � UCV (a; b) and k � ST (a; b) will
be introduced and some results concerning to these classes will be investigated.
All contents of this chapter have been published in the well reputed journal "Com-
puters and Mathematics with Applications, Vol 62; 2011; Pages 367 � 375", for detail,
see [70].
4.1 Introduction
As we have mentioned above, we are to generalize the conic domain k; k � 0, introduced
by Kanas and Wisniowska [36, 35], discussed in section 2.6.1. we de�ne the following.
62
De�nition 4.1.1 A function p (z) is said to be in the class k � P (a; b) ; if and only if,
p (z) � pk (a; b; z) ; (4.1.1)
where k 2 [0;1) ;
pk (a; b; z) = 1 + a+ (1� b) fpk(z)� 1g (4.1.2)
= a+ b+ (1� b) pk(z);
and pk(z) is de�ned by (2:6:2) : Also a and b must be chosen accordingly, as:
(i) For k = 0; we take b = 0;
(ii) For k 2�0; 1p
2
�; we take b 2
�1
2k2�1 ; 1�;
(iii) For k 2h1p2; 1i; we take b 2 (�1; 1) ;
(iv) For k 2 (1;1) ; we take b 2��1; 1
2k2�1�:
9>>>>>>=>>>>>>;(4.1.3)
and
k2(1�b)1�k2 � � � a < 1� k2(1�b)
k2�1 + �; 0 � k < 1;
�1+b2� a < 1�b
2; k = 1;
max�k2(1�b)1�k2 � �; 1� k2(1�b)
k2�1 � ��� a < 1� k2(1�b)
k2�1 + �; k > 1;
9>>>>>>>>>=>>>>>>>>>;(4.1.4)
where � = kpk2(1�b)2+(1�k2)(1�b2)
k2�1 :
Geometrically, the function p (z) 2 k�P (a; b) takes all values from the conic domain
k (a; b) which is de�ned as:
k (a; b) =�u+ iv : (u� a)2 > k2
�(u� a+ b� 1)2 + v2 + 2b (1� b)
�: (4.1.5)
63
The conic domain k (a; b) represents the right half plane when k = 0; a hyperbola
(right branch) when 0 < k < 1; a parabola when k = 1 and an ellipse when k > 1: It
can be seen that k (0; 0) = k; the conic domain de�ned by Kanas and Wisniowska
[36, 35], consequently, k � P (0; 0) = P (pk) ; the well-known class introduced by Kanas
and Wisniowska [36]. The function p1 (a; b; z) = Qa;b (z) is de�ned by Kanas in [33]. Here
are some basic facts about the class k � P (a; b) :
Remark 4.1.1 1. k � P (a; b) � P (�) ; where
� =
8>>><>>>:a+ 1+b
2; k = 1;
a+k2(1�b)�k
pk2(1�b)2+(1�k2)(1�b2)k2�1 ; k 6= 1:
(4.1.6)
That is, for p (z) 2 k � P (a; b) we have Re p (z) > �; z 2 E where � is de�ned by
(4:1:6) :
2. k � P (a1; b) � k � P (a2; b) ; a1 > a2; k 2 [0; 1] :
3. k � P (a; b1) � k � P (a; b2) ; b1 > b2; k 2 (0;1) :
The domain k (a; b) always ensures that the point (1; 0) is contained inside it whereas
the domain k;�; introduced in [59], de�ned by
k;� = (1� �) k + �; 0 � � < 1; k � 0; (4.1.7)
is not well de�ned because (1; 0) =2 k;� in general. For example, in particular (1; 0) =2
1:2;0:5 as shown in �gure below.
64
Figure 4.1: View of 1:2;0:5
From (4:1:7) ; we note that (u; v) 2 k;� if
u2 > k2�(u+ � � 1)2 + v2 + 2� (1� �)
�(4.1.8)
and for (u; v) = (1; 0) ; k = 1:2; � = 0:5; the relation (4:1:8) reduces to 1 > 1:08 which
clearly shows that (1; 0) =2 1:2;0:5: We see that the conic domain k (0; b) coincides with
k;b only when b is chosen according to (4:1:3) : This means that for k;� to contain the
point (1; 0) inside, � must be chosen accordingly, as:
� 2
8>>><>>>:[0; 1) ; if 0 � k � 1;
h0; 1�
pk2�1k
�; if k > 1:
(4.1.9)
According to this criteria de�ned in (4:1:9) ; for k = 1:2; there must be � 2 [0; 0:4472292)
to contain the point (1; 0) inside.
The domain k;� gives only the contraction of k whereas the domain k (a; b) gives
contraction as well as magni�cation of k depending upon b: For b > 0; the domain
k (a; b) gives the contraction as shown in �gure below.
65
Figure 4.2: Contraction of k
For b < 0; the domain gives the magni�cation of k as can be seen from the �gure below.
Figure 4.3: Magni�cation of k
Now we de�ne the classes k � UCV (a; b) and k � ST (a; b) as follows.
De�nition 4.1.2 A function f (z) 2 A is said to be in the class k�UCV (a; b) ; k � 0;
a; b satisfy (4:1:3) and (4:1:4) ; if and only if ,
�Re
�(zf 0(z))0
f 0 (z)� a
��2> k2
"����(zf 0(z))0f 0 (z)� a+ b� 1
����2 + 2b (1� b)
#(4.1.10)
66
or equivalently(zf 0(z))0
f 0 (z)� pk (a; b; z) ; (4.1.11)
where pk (a; b; z) is de�ned by (4:1:2) :
De�nition 4.1.3 A function f (z) 2 A is said to be in the class k � ST (a; b) ; k � 0;
a; b satisfy (4:1:3) and (4:1:4) ; if and only if ,
�Re
�zf 0(z)
f (z)� a
��2> k2
"����zf 0(z)f (z)� a+ b� 1
����2 + 2b (1� b)
#(4.1.12)
or equivalentlyzf 0(z)
f (z)� pk (a; b; z) ; (4.1.13)
where pk (a; b; z) is de�ned by (4:1:2) :
It can be easily seen that
f (z) 2 k � UCV (a; b) () zf 0 (z) 2 k � ST (a; b) :
Special Cases
(i) k � UCV (0; 0) = k � UCV; the well-known class of k-uniformly convex functions,
introduced by Kanas and Wisniowska [36].
(ii) k � ST (0; 0) = k � ST; the well-known class of k-starlike functions, introduced by
Kanas and Wisniowska [35].
4.2 Main results
The following �rst result is the su¢ cient condition for a function f (z) 2 A to be from
the class k � ST (a; b) :
67
Theorem 4.2.1 If f (z) 2 A satis�es the inequality
Re
( zf 00(z)f 0(z)
zf 0(z)f(z)
� 1
)<3� �
2� �;
where � is de�ned by (4:1:6) ; then f (z) 2 k � ST (a; b) ; k 2 [0; 1] ; b � 0 with a and b
satisfying (4:1:3) and (4:1:4) :
Proof. We consider the function w (z) as
zf 0 (z)
f (z)� 1 = (1� �)w (z) ; (4.2.1)
where � is de�ned by (4:1:6) : We see that w (z) is analytic in E and w (0) = 0: Loga-
rithmic di¤erentiation of (4:2:1) gives us
1 +zf 00 (z)
f 0 (z)� zf 0 (z)
f (z)=
(1� �) zw0 (z)
(1� �)w (z) + 1:
This implies thatzf 00 (z)
f 0 (z)= (1� �)w (z) +
(1� �) zw0 (z)
(1� �)w (z) + 1: (4.2.2)
Now from (4:2:1) and (4:2:2) ; we have
zf 00(z)f 0(z)
zf 0(z)f(z)
� 1= 1 +
zw0 (z)
w (z) f(1� �)w (z) + 1g :
Suppose that there exists a point z0 2 E such that
maxjzj�jz0j
jw (z)j = jw (z0)j = 1; w (z0) 6= 1
and also w (z0) = ei� (� 6= ��): Then applying Lemma 2.10.3, we have
z0w0 (z0) = cw (z0) ; c � 1:
68
Using this, we can have
Re
( zf 00(z0)f 0(z0)
zf 0(z0)f(z0)
� 1
)= Re
�1 +
z0w0 (z0)
w (z0) f(1� �)w (z0) + 1g
�= Re
�1 +
cw (z0)
w (z0) f(1� �)w (z0) + 1g
�= 1 + cRe
�1
(1� �)w (z0) + 1
�= 1 + cRe
�1
(1� �) ei� + 1
�= 1 + c
1 + (1� �) cos �
(1� �)2 + 2 (1� �) cos � + 1= F (�) ; say.
Now as we know that F (�) � minF (�) and it can easily be seen that
minF (�) = F (�)
= 1 + c1 + (1� �) cos �
(1� �)2 + 2 (1� �) cos � + 1
= 1 + c1� (1� �)
(1� �)2 � 2 (1� �) + 1
= 1 + c�
(1� � � 1)2
= 1 +c
�
� 1 +1
�
> 1 +1
2� �for � < 1
=3� �
2� �:
Therefore, we have
Re
( zf 00(z0)f 0(z0)
zf 0(z0)f(z0)
� 1
)>3� �
2� �;
69
which is a contradiction to our hypothesis. Thus, we must have jw (z)j < 1 for all z 2 E
and therefore we have from (4:2:1) ;����zf 0 (z)f (z)� 1���� < 1� �;
which shows that zf0(z)f(z)
lies inside a circle centered at (1; 0) and having radius 1�� and we
know from (4:1:5) that this circle lies inside the conic domain k (a; b) ; k 2 [0; 1] ; b � 0
with a and b satisfying (4:1:3) and (4:1:4) : This implies that f (z) 2 k � ST (a; b) ; k 2
[0; 1] ; b � 0 with a and b satisfying (4:1:3) and (4:1:4) :
From the Theorem 4.2.1, we see that when a = 0; b = 0 and k = 1; we have the
following result which is the special case (when p = 1) of the result proved by Al-Kharsani
et.al [6].
Corollary 4.2.1 If f (z) 2 A satis�es the inequality
Re
( zf 00(z)f 0(z)
zf 0(z)f(z)
� 1
)<5
3;
then f (z) is uniformly starlike in E (that is f (z) 2 1� ST ).
The following are the inclusion relations of both classes k�UCV (a; b) and k�ST (a; b)
based on the nested conic regions by varying the parameter b:
Theorem 4.2.2 For b1 > b2;
i. k � UCV (a; b1) � k � UCV (a; b2) :
ii. k � ST (a; b1) � k � ST (a; b2) :
Proof follows directly from Remark 3:1:1(3), (4:1:1) ; (4:1:11) and (4:1:13) :
The following is a radius problem which estimates the radius of k (a; b)-uniform con-
vexity of univalent functions. It gives many known results as special cases, discussed
after the following result.
70
Theorem 4.2.3 Let f (z) 2 S: Then f (z) 2 k � UCV (a; b) for jzj < r0 < 1 with
r0 =2�
p3 + �2
1 + �;
where � is de�ned by (4:1:6) :
Proof. Let f (z) 2 S: Then, for jzj = r < 1; we have����zf 00 (z)f 0 (z)� 2r2
1� r2
���� � 4r
1� r2;
for detail, see [24]. This implies that����(zf 0 (z))0f 0 (z)� 1 + r
2
1� r2
���� � 4r
1� r2: (4.2.3)
The boundary of this disk intersects the real axis at the points�1�4r+r21�r2 ; 0
�and
�1+4r+r2
1�r2 ; 0�:
Now we have to �nd the largest value of r such that the disk (4:2:3) lies completely inside
the conic domain k (a; b) ; that is�1�4r+r21�r2 ; 0
�2 k (a; b) : For this, we must have
1� 4r + r2
1� r2> �;
where � is de�ned by (4:1:6) : This gives us
(1 + �) r2 � 4r + 1� � > 0; 0 < r < 1:
This holds only if
r < r0 =2�
p3 + �2
1 + �:
Now it can also be seen that the curve
(u� a)2 = k2 (u� a+ b� 1)2 + k2v2 + 2k2b (1� b)
71
and for r < r0 =2�p3+�2
1+�; the circle
�u� 1 + r
2
1� r2
�2+ v2 =
16r2
(1� r2)2
do not intersect any where. Therefore, the disk (4:2:3) lies completely inside the conic
domain k (a; b) ; that is, from (4:2:3) we have
(zf 0 (z))0
f 0 (z)2 k (a; b)
which implies that f (z) 2 k � UCV (a; b) : Hence the proof.
When a = 0 and b = 0; then we have the following result, proved by Kanas and
Wisniowska [36].
Corollary 4.2.2 Let f (z) 2 S: Then f (z) 2 k � UCV for jzj < r0 < 1 with
r0 =2 (k + 1)�
p4k2 + 6k + 3
2k + 1:
When a = 0; b = 0 and k = 1; then we have the following result, proved in [96].
Corollary 4.2.3 Let f (z) 2 S: Then f (z) 2 UCV for jzj < r0 < 1 with
r0 =4�
p13
3:
When a = 0; b = 0 and k = 0; then we have the following result, proved in [24].
Corollary 4.2.4 Let f (z) 2 S: Then f (z) 2 C for jzj < r0 < 1 with r0 = 2�p3:
Now we have an extension of the Lemma 2.10.1 proved in [33].
Lemma 4.2.1 Let 0 � k <1: Also, let �; 2 C be such that � 6= 0 and Re (�� + ) >
0; where � is de�ned by (4:1:6) : If p (z) is analytic in E; p (0) = 1; p (z) satis�es
p (z) +zp0 (z)
�p (z) + � pk (a; b; z) ; (4.2.4)
72
and q (z) is analytic solution of
q (z) +zq0 (z)
�q (z) + = pk (a; b; z) ;
then q (z) is univalent, p (z) � q (z) � pk (a; b; z) and q (z) is the best dominant of (4:2:4) :
Proof follows similarly as given in [33].
Moreover, the solution q (z) is given by
q (z) =
��
Z 1
0
�t�+ �1 exp
Z tz
z
pk (a; b;u)� 1u
du
��dt
��1�
�:
For more details of best dominant, we refer to [33, 53].
As a special case, when � = 1 and = 0; we have the function q (z) as
q (z) =
24 1Z0
0@exp tzZz
pk (a; b;u)� 1u
du
1A dt
35�1 : (4.2.5)
Now we see a few applications of the Lemma 4.2.1. When k > 1; the conic domain
k (a; b) may be characterized by the circular domain having its diameter end points as
the vertices of ellipse. As we see that the vertices of ellipse are (�; 0) and (�1; 0) ; where
� is de�ned by (4:1:6) and
�1 = a+k2 (1� b) + k
qk2 (1� b)2 + (1� k2) (1� b2)
k2 � 1 :
The circle K (X;R) having diameter end points (�; 0), (�1; 0) has its center at
X
�a(k2�1)+(1�b)k2
k2�1 ; 0
�and radius R as
R =kqk2 (1� b)2 + (1� k2) (1� b2)
k2 � 1 :
73
The point z = 1 is contained inside the circle K (X;R) and then the function �a;b : E �!
K (X;R) has the form
�a;b (z) = a+k2 (1� b) + kz
p(1� b) (1� b� 2b (k2 � z2))
k2 � z2: (4.2.6)
Theorem 4.2.4 Let k 2 (1;1) and b = 0: Also, let p (z) be analytic in E with p (0) = 1
and p (z) satis�es (4:2:4) : Then
p (z) � 1
(k � z)1R0
ta
k�tzdt
and
Re p (z) >1
(k + 1)1R0
ta
k+tdt
;
where � kk+1
� a < 1k+1
:
Proof. From (4:2:6) ; we have for b = 0;
�a;0 (z) = a+k
k � z:
Since p satis�es (4:2:4) and for each �xed k; pk (a; b; z) � �a;0 (z) ; so p (z) � �a;0 (z) :
This implies from (4:2:5) ;
q (z) =
24 1Z0
0@exp tzZz
�a;0 (u)� 1u
du
1A dt
35�1
=
24 1Z0
0@exp tzZz
a+ kk�u � 1u
du
1A dt
35�1
74
=
24 1Z0
0@exp tzZz
�a
u+
1
k � u
�du
1A dt
35�1
=
24 1Z0
�exp
�log
(tz)a
k � tz� log za
k � z
��dt
35�1
=
24 1Z0
(k � z) ta
k � tzdt
35�1
=1
(k � z)1R0
ta
k�tzdt
:
Also we have
Re p (z) > q (�1) = 1
(k + 1)1R0
ta
k+tdt
for z 2 E:
When a = 0; we have the following result, proved by Kanas [33].
Corollary 4.2.5 Let k 2 (1;1) and let p (z) be analytic in E with p (0) = 1 and p (z)
satis�es (4:2:4) : Then
p (z) � z
(z � k) log�1� z
k
�and
Re p (z) >1
(k + 1) log�1 + 1
k
� :Now we check the integral preservation property of the class k � ST (a; b) under an
integral operator, de�ned in [59]. The technique used in the following result is similar to
that, used by Noor in [59].
Theorem 4.2.5 Let f (z) ; g (z) 2 k � ST (a; b) and let �; c and � be positive reals.
75
Then the function F (z) ; de�ned by
F (z) =
24cz��c zZ0
tc���1 (f (t))� (g (t))��� dt
35 1�
(4.2.7)
belongs to k � ST (a; b) :
Proof. From (4:2:7) ; we have
zc�� (F (z))� = c
zZ0
tc���1 (f (t))� (g (t))��� dt:
This implies that
(c� �) zc���1 (F (z))� + �zc�� (F (z))��1 F 0 (z) = czc���1 (f (z))� (g (z))��� :
Let h (z) = zF 0(z)F (z)
: Then, we have
(F (z))� f(c� �) + �h (z)g = c (f (z))� (g (z))��� :
Di¤erentiating logarithmically, we have
�zF 0 (z)
F (z)+
�zh0 (z)
�h (z) + (c� �)= �
zf 0 (z)
f (z)+ (�� �)
zg0 (z)
g (z):
Now let h1 (z) =zf 0(z)f(z)
and h2 (z) =zg0(z)g(z)
: Then we have
h (z) +zh0 (z)
�h (z) + (c� �)=�
�h1 (z) +
�1� �
�
�h2 (z) :
76
Since f (z) ; g (z) 2 k � ST (a; b) ; so h1 (z) ; h2 (z) 2 k � P (a; b) : And we know by
subordination technique that the class k � P (a; b) is convex. Therefore,
h (z) +zh0 (z)
�h (z) + (c� �)� pk (a; b; z) ;
which implies by using Lemma 4.2.1,
h (z) � pk (a; b; z) :
This shows that F (z) 2 k � ST (a; b) :
When a = 0; b = 0; we get the following result which is a special case of result,
proved by Noor in [59].
Corollary 4.2.6 Let f (z) ; g (z) 2 k � ST and let �; c and � be positive reals. Then
the function F (z) ; de�ned by
F (z) =
24cz��c zZ0
tc���1 (f (t))� (g (t))��� dt
35 1�
(4.2.8)
belongs to k � ST:
4.3 Conclusion
We generalized conic domain k; k � 0 and introduced the conic domain k (a; b) ; k � 0
and discussed various of its aspects. Di¤erent graphical views of this generalized conic
domain for speci�c values of parameters are shown for better understanding of the be-
haviour of this domain. The class k�P (a; b) of functions which map the open unit disk
E onto this generalized conic regions are de�ned and some of its properties are discussed.
Related to the class k � P (a; b) ; two more classes k � UCV (a; b) and k � ST (a; b) are
introduced and some results concerning to these classes are investigated.
77
Chapter 5
On Bounded Boundary and Bounded Radius
Rotation Related with Janowski Function
78
The functions with bounded boundary and bounded radius rotation are discussed in
section 2.7 and the generalized Janowski functions of order � are discussed in section
2.6.2.
In this chapter, we will study the class P [A;B; �] of generalized Janowski functions
of order � along with the functions with bounded boundary and bounded radius rotation.
The order of a function from the class Vm[A;B; �] of Janowski functions with bounded
boundary rotation to be from Rm[A;B; �] of Janowski functions with bounded radius
rotation is our major interest. Some of its applications will also be the part of our
discussion. Our main results present an advancement of already known results.
It is to be mentioned here that all the contents of this chapter have also been published
in "World Applied Sciences Journal, Vol 12(6) 2011, Pages 895 � 902", for detail, see
[79].
5.1 Introduction
The class P [A;B] of Janowski functions is de�ned in De�nition 2.6.9 and its connection
with the class P of functions with positive real part is shown from (2:6:9) : This connection
on the other way can also be seen as:
h (z) 2 P [A;B] () (B � 1)h (z)� (A� 1)(B + 1)h (z)� (A+ 1) 2 P: (5.1.1)
Let P [A;B; �] be the class of functions p1, analytic in E with p1 (0) = 1 and
p1 (z) �1 + [(1� �)A+ �B] z
1 +Bz; �1 � B < A � 1; 0 � � < 1; z 2 E; (5.1.2)
or equivalently,
p1 (z) �1 + Cz
1 +Bz; �1 � B < C � 1; 0 � � < 1; z 2 E;
79
where C = (1� �)A+ �B. It can also be noted that
(1� �) p1 + � 2 P [A;B; �], p1 2 P [A;B] : (5.1.3)
Now we consider the following class, introduced by Noor [56].
De�nition 5.1.1 A function p (z) is said to be in the class Pm[A;B; �], if and only if,
p (z) =
�m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z) ; (5.1.4)
where p1 (z) ; p2 (z) 2 P [A;B; �] ; �1 � B < A � 1; m � 2 and 0 � � < 1:
It is clear that P2[A;B; �] � P [A;B; �] and Pm[1;�1; 0] � Pm, the well-known class
given and studied by Pinchuk [87]. The important fact about the class Pm[A;B; �] is
that this class is convex set. That is, for pi (z) 2 Pm[A;B; �] and �i � 0 withnXi=1
�i = 1,
we havenXi=1
�ipi (z) 2 Pm[A;B; �]. (5.1.5)
This can be easily seen from (5:1:3), (5:1:4) and with the fact that the set P [A;B] is
convex [66]. By using all these concepts, we consider the following classes.
Rm[A;B; �] =
�f 2 A : zf
0(z)
f(z)2 Pm [A;B; �] ; z 2 E
�,
Vm[A;B; �] = ff 2 A : zf 0(z) 2 Rm[A;B; �]; z 2 Eg ,
where �1 � B < A � 1, m � 2, and 0 � � < 1. For � = 0 and �1 � B < A � 1,
the classes Vm[A;B; �] and Rm[A;B; �] reduces to the classes Vm[A;B] and Rm[A;B]
respectively, studied by Noor [61, 64, 69].
Throughout this chapter, we assume that C = (1� �)A+ �B unless otherwise men-
tioned. In order to derive our main results, we need the following lemmas.
80
5.2 Preliminary Lemmas
In order to prove our main results, we need the following results.
Lemma 5.2.1 [52] If �1 � B < A � 1; � > 0 and the complex number satis�es
Re f g � �� (1� A) = (1�B) ; (5.2.1)
then the di¤erential equation
q (z) +zq0 (z)
�q (z) + =1 + Az
1 +Bz; z 2 E;
has a univalent solution in E given by
q (z) =
8>>>>>>>>>>><>>>>>>>>>>>:
z�+ (1+Bz)�(A�B)=B
�
zZ0
t�+ �1(1+Bt)�(A�B)=Bdt
� �; B 6= 0;
z�+ e�Az
�
zZ0
t�+ �1e�Atdt
� �; B = 0:
If h (z) = 1 + c1z + c2z2 + : : : is analytic in E and satis�es
h (z) +zh0 (z)
�h (z) + � 1 + Az
1 +Bz; z 2 E; (5.2.2)
then
h (z) � q (z) � 1 + Az
1 +Bz;
and q (z) is the best dominant which can also be written in hypergeometric form as
q (z) =1
�G (z)�
�;
81
where
G(z) =
8>>><>>>:2F1
��(B�A)nB
; 1; �+ +nn
; Bz1+Bz
�(�+ )�1 ; B 6= 0;
1F1�1; �+ +n
n;��
nAz�(�+ )�1 ; B = 0:
Lemma 5.2.2 [110] Let � be a positive measure on [0; 1] and let h (z; t) be a complex-
valued function de�ned on E�[0; 1] such that h (:; t) is analytic in E for each t 2 [0; 1] and
that h (z; :) is �-integrable on [0; 1] for all z 2 E: In addition, suppose that Re fh (z; t)g >
0; h (�r; t) is real and
Re
�1
h (z; t)
�� 1
h (�r; t) for jzj � r < 1 and t 2 [0; 1] :
If H (z) =
1Z0
h (z; t) d� (t) ; then Re�
1H(z)
�� 1
H(�r) :
5.3 Main Results
Theorem 5.3.1 Let f (z) 2 Vm [A;B; �] with m � 2; 0 � � < 1; and �1 � B < A � 1
satisfying (5:2:1) : Then, f (z) 2 Rm [A;B; �1] ; where A < �B(1+�)1�� ; B 2 [�1; 0) and
�1 = �1(�; 1; 0) =C
(1�B)B�CB � (1�B)
: (5.3.1)
Proof. Let
zf 0(z)
f(z)= p(z) (5.3.2)
=
�m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z) : (5.3.3)
Logarithmic di¤erentiation of (5:3:2) yields
(zf 0(z))0
f 0(z)= p(z) +
zp0(z)
p(z).
82
Since f (z) 2 Vm [A;B; �], it follows that
p(z) +zp0(z)
p(z)2 Pm [A;B; �] . (5.3.4)
Now consider a function 'a;b(z) de�ned by Noor [65]
'a;b(z) = z +1Xn=2
b+ 1
b+ (n� 1) a zn
with a = 1; b = 0 and then by using the same convolution technique as used by Noor
[65], we have' (z)
z� p (z) = p(z) +
zp0(z)
p(z): (5.3.5)
From (5:3:3), (5:3:4) and (5:3:5), we obtain
�m
4+1
2
��p1 (z) +
zp01(z)
p1(z)
���m
4� 12
��p2 (z) +
zp02(z)
p2(z)
�2 Pm [A;B; �] : (5.3.6)
From this, we have
pi(z) +zp0i(z)
pi(z)2 P [A;B; �] , i = 1; 2.
We use Lemma 5.2.1 for n = 1, = 0, � = 1 > 0, � 2 [0; 1): and h = pi in (5:2:2), to
have
pi(z) � q (z) � 1 + Cz
1 +Bz: (5.3.7)
This estimate is best possible, extremal function q (z) is given by
q(z) =1
G (z)=
8>>>>><>>>>>:Cz
(1+Bz)�(1+Bz)B�CB
, if B 6= 0,
(1��)Az1�e�(1��)(Az) ; if B = 0.
(5.3.8)
83
From(5:3:7) ; we have
Minjzj=r
Re pi(z) � Minjzj=r
Re q (z) :
Now we show that minRe q(z) = q(�1): Setting a = B�CB; b = 1; c = b + 1 such that
Re c > Re b > 0 and using (2:9:3) ; (2:9:4) and (2:9:5), we have
G (z)= (1 +Bz)a1Z0
tb�1 (1 +Btz)�a dt =� (b)
� (c)2F1
�1; a; c;
Bz
1 +Bz
�; B 6= 0: (5.3.9)
Now we have to show that Re f1=G (z)g � 1=G (�1) ; z 2 E: For A < �B(1+�)1�� ;with
�1 � B < A (Re c > Re a > 0) and using (2:9:3) in (5:3:9), we have
G (z) =
1Z0
g (t; z) d� (t)
where g (z; t) = 1+Bz1+(1�t)Bz and d� (t) =
�(b)�(a) �(c�a)t
a (1� t)c�a�1 dt is a positive measure
on [0; 1] : Now for �1 � B < 0; we have Re g (z; t) > 0 and g (�r; t) is real for 0 � r <
1; t 2 [0; 1] : Also for jzj � r < 1 and t 2 [0; 1] ;
Re
�1
g (z; t)
�= Re
�1 + (1� t)Bz
1 +Bz
�� 1� (1� t)Br
1�Br=
1
g (�r; t) :
Now using the lemma 5.2.2, we obtain Re f1=G (z)g � 1=G (�r) ; (jzj � r < 1) let-
ting r ! 1�; we obtain Re f1=G (z)g � 1=G (�1) : Taking A !��B(1+�)1��
�+and using
(5:3:7) we have consequently from (5:3:8)
�1 = �1(�; 1; 0) = q (�1) = C
(1�B)B�CB � (1�B)
; A < �B (1 + �)1� �
; B 2 [�1; 0) :
This Shows that pi (z) 2 P [A;B; �1], where �1 is given by (5:3:1) and consequently
p (z) 2 Pm [A;B; �1], which gives the required result.
If A = 1; B = �1 in Theorem 5.3.1, we obtain the following result proved in [80].
84
Corollary 5.3.1 Let f (z) 2 Vm(�). Then f (z) 2 Rm(�1), where
�1 = �1(�; 1; 0) =
8><>:2��1
2�22(1��) ; if � 6= 12;
12 ln 2
; if � = 12.
(5.3.10)
If m = 2; A = 1; B = �1 in Theorem 5.3.1, we obtain the following result proved in
[21].
Corollary 5.3.2 Let f (z) 2 C(�). Then f (z) 2 S�(�1), where
�1 = �1(�; 1; 0) =
8><>:2��1
2�22(1��) ; if � 6= 12;
12 ln 2
; if � = 12.
(5.3.11)
Theorem 5.3.2 Let f (z) 2 Vm[A;B; �]: Then f (z) 2 Rm [1;�1; �1], where �1 is one of
the roots of
4 (B2 � 1) �41 + [4 (1� 2�) (B2 � 1)� 8 (1� �) (AB � 1)] �31+
��4�2 � 4� � 3
� �B2 � 1
�+ 4 (1� �)2
�A2 � 1
�� 4 (1� �) (1� 2�) (AB � 1)
��21+
�4 (1� �) (AB � 1)� 2 (1� 2�)
�B2 � 1
���1 +
�B2 � 1
�= 0 (5.3.12)
with 0 � �1 < 1:
Proof. Let
zf 0(z)
f(z)= (1� �1)p(z) + �1 (5.3.13)
= (1� �1)
��m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z)
�+ �1; (5.3.14)
p(z) is analytic in E with p (0) = 1: Then, di¤erentiating (5:3:13) logarithmically, we
have(zf 0(z))0
f 0(z)= (1� �1)p(z) + �1 +
(1� �1)zp0(z)
(1� �1)p(z) + �1,
85
that is,
1
1� �
�(zf 0(z))0
f 0(z)� �
�=
1
1� �
�(1� �1)p(z) + �1 � � +
(1� �1)zp0(z)
(1� �1)p(z) + �1
�
=(�1 � �)
1� �+(1� �1)
1� �
"p(z) +
1(1��1)
zp0(z)
p(z) + �1(1��1)
#.
Since f (z) 2 Vm[A;B; �]; it implies that
�1 � �
1� �+1� �11� �
"p(z) +
1(1��1)
zp0(z)
p(z) + �1(1��1)
#2 Pm[A;B]; z 2 E. (5.3.15)
Now consider a function 'a;b(z) de�ned by Noor [65]
'a;b(z) = z +1Xn=2
b+ 1
b+ (n� 1) a zn (5.3.16)
with a = 11��1
; b = �11��1
: By using (5:3:16) with the same convolution technique as
used by Noor [65], we have
'a;b(z)
z� p(z) =
�m
4+1
2
��'a;b(z)
z� p1(z)
���m
4� 12
��'a;b(z)
z� p2(z)
�
which implies that
p(z) +azp0(z)
p(z) + b=
�m
4+1
2
��p1(z) +
azp01(z)
p1(z) + b
���m
4� 12
��p2(z) +
azp02(z)
p2(z) + b
�:
(5.3.17)
Thus, from (5:3:15) and (5:3:17), we have
�1 � �
1� �+1� �11� �
�pi(z) +
azp0i(z)
pi(z) + b
�2 P [A;B] ; i = 1; 2: (5.3.18)
86
Using the fact illustrated in (5:1:1), we have
(B � 1)��+ �
hpi(z) +
azp0i(z)pi(z)+b
i�� (A� 1)
(B + 1)��+ �
hpi(z) +
azp0i(z)pi(z)+b
i�� (A+ 1)
2 P;
where � = �1��1�� and � = 1��1
1�� : This implies that
(B � 1) [(�+ �pi(z)) (pi(z) + b) + a�zp0i(z)]� (A� 1) (pi(z) + b)
(B + 1) [(�+ �pi(z)) (pi(z) + b) + a�zp0i(z)]� (A+ 1) (pi(z) + b)2 P:
We now form the functional (u; v) by choosing u = pi(z); v = zp0i(z) and note that the
�rst two conditions of Lemma 2.10.4 are clearly satis�ed. We check condition (iii) as
follows.
(u; v) =(B � 1) [(�+ �u) (u+ b) + a�v]� (A� 1) (u+ b)
(B + 1) [(�+ �u) (u+ b) + a�v]� (A+ 1) (u+ b)
=�1 + a� (B � 1) v + [(�+ � (u+ b)) (B � 1)� (A� 1)]u�2 + a� (B + 1) v + [(�+ � (u+ b)) (B + 1)� (A+ 1)]u ;
where �1 = b [� (B � 1)� (A� 1)] and �2 = b [� (B + 1)� (A+ 1)] : Now
(iu2; v1) =�1 + � (av1 � u22) (B � 1) + [(�+ �b) (B � 1)� (A� 1)] iu2�2 + � (av1 � u22) (B + 1) + [(�+ �b) (B + 1)� (A+ 1)] iu2
:
Taking real part of (iu2; v1), we have
Re (iu2; v1) =
[��1 + � (av1 � u22) (1�B)] [�2 + � (av1 � u22) (B + 1)]�
[(�+ �b) (B � 1)� (A� 1)] [(�+ �b) (B + 1)� (A+ 1)]u22� [�2 + � (av1 + u2) (B + 1)]
2 � [(�+ �b) (B + 1)� (A+ 1)]2 u22:
As a > 0; � > 0, so applying v1 � �12(1 + u22) and after a little simpli�cation, we have
Re (iu2; v1) �A1 +B1u
22 + C1u
42
D1
; (5.3.19)
87
where
A1 =1
4[2�1 � a� (B � 1)] [2�2 � a� (B + 1)] ;
B1 = �12� (a+ 2)
��1 (B + 1)� a�
�B2 � 1
�+ �2 (B � 1)
�+
(�+ �b)2�B2 � 1
�� 2 (�+ �b) (AB � 1) +
�A2 � 1
�;
C1 = �14�2�1�B2
�(a+ 2)2 ;
and
D1 = [�2 + � (av1 + u2) (B + 1)]2 + [(�+ �b) (B + 1)� (A+ 1)]2 u22:
The right hand side of (5:3:19) is negative if A1 � 0 and B1 � 0: From A1 � 0, we have
�1 to be one of the roots of
4�B2 � 1
��41 +
�4 (1� 2�)
�B2 � 1
�� 8 (1� �) (AB � 1)
��31+��
4�2 � 4� � 3� �B2 � 1
�+ 4 (1� �)2
�A2 � 1
�� 4 (1� �) (1� 2�) (AB � 1)
��21+�
4 (1� �) (AB � 1)� 2 (1� 2�)�B2 � 1
���1 +
�B2 � 1
�= 0
with 0 � �1 < 1 and also for 0 � �1 < 1, we have
B1 = 4�B2 � 1
��31 + 4
�(1 + �)
�B2 � 1
�+ (1� �) (AB � 1)
��21���
2�2 + 2� + 5� �B2 � 1
�+ 2 (1 + 2�) (1� �) (AB � 1) + 2
�A2 � 1
�(1� �)2
��1+��
3 + 2�2� �B2 � 1
�+ 4� (1� �) (AB � 1) + 2
�A2 � 1
�(1� �)2
�� 0:
Since all the conditions of Lemma 2.10.4 are satis�ed, it follows that pi (z) 2 P in E for
i = 1; 2 and consequently p (z) 2 Pm [1;�1] and hence f (z) 2 Rm [1;�1; �1], where �1 is
one of the roots of (5:3:12) with 0 � �1 < 1:
88
By setting A = 1; B = �1 in Theorem 5.3.2, we obtain the following result proved in
[80].
Corollary 5.3.3 Let f (z) 2 Vm (�) : Then f (z) 2 Rm (�1), where �1 is one of the roots
of
2�21 � (2� � 1) �1 � 1 = 0 with 0 � �1 < 1;
which is
�1 =1
4
�(2� � 1) +
q4�2 � 4� + 9
�:
If m = 2; A = 1; B = �1 in Theorem 5.3.2, we obtain the following result proved in
[21].
Corollary 5.3.4 Let f (z) 2 C (�) : Then f (z) 2 S� (�1), where �1 is one of the roots
of
2�21 � (2� � 1) �1 � 1 = 0 with 0 � �1 < 1;
which is
�1 =1
4
�(2� � 1) +
q4�2 � 4� + 9
�:
Application of Theorem 5.3.1
Theorem 5.3.3 Let f (z) and g (z) belong to Vm [A;B; �] with m � 2; 0 � � < 1; and
�1 � B < A � 1: Then the function F (z) de�ned by
(F (z))�1 =c
zc��1
zZ0
t(c����)�1 (f (t))� (g (t))� dt; �1; c; �; � > 0; (5.3.20)
is in the class Rm [A;B; �1] ; where
�1 =c
�1 2F1�1; �1(1� �)
�1� A
B
�; c+ 1; B
B�1� � c� �1
�1(5.3.21)
and c > �1; A < � [(c+1)��1(1��)]B�1(1��) ; (� + �) = �1:
89
Proof. Let
(zF 0(z))0
F 0(z)= p (z) (5.3.22)
=
�m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z) : (5.3.23)
Then, p (z) is analytic in E and p (0) = 1: With zf 0(z)f(z)
= p1 (z) ;zg0(z)g(z)
= p2 (z) ; we have
from (5:3:20) and by using (5:3:22)
p (z) +zp0(z)
�1p(z) + (c� �1)=
�
�1p1 (z) +
�
�1p2 (z) = H0 (z) :
Since f (z) ; g (z) 2 Vm [A;B; �] and this means that f (z) ; g (z) 2 Rm [A;B; �1] ; so
p1 (z) ; p2 (z) 2 Pm [A;B; �1] : It is known that Pm [A;B; �1] is convex set: Therefore,
H0 (z) 2 Pm [A;B; �1] and �1 = �1 (�) is given by (5:3:1) : This implies that
p (z) +zp0(z)
�1p(z) + (c� �1)2 Pm [A;B; �1] : (5.3.24)
Now consider a function 'a;b(z) de�ned by Noor [65]
'a;b(z) = z +1Xn=2
b+ 1
b+ (n� 1) a zn
with a = �1; b =c��1�1
and using (5:3:23) with the same convolution technique as used
by Noor [65], we have
'a;b(z)
z� p (z) =
�m
4+1
2
��'a;b(z)
z� p1 (z)
���m
4� 12
��'a;b(z)
z� p2 (z)
�;
90
which implies that
p(z) +zp0(z)
�1p(z) + (c� �1)=
�m
4+1
2
��p1 (z) +
zp01(z)
�1p1(z) + (c� �1)
���m
4� 12
��p2 (z) +
zp02(z)
�1p2(z) + (c� �1)
�:(5.3.25)
Thus, from (5:3:24) and (5:3:25), we have
pi (z) +zp0i(z)
�1pi(z) + (c� �1)2 P [A;B; �1] , i = 1; 2.
Therefore,
pi (z) +zp0i(z)
�1pi(z) + (c� �1)� 1 + f(1� �1)A+ �1Bg z
1 +Bz:
Using Lemma 5.2.1 for � = �1; = c� �1; we have
pi (z) � q (z) � 1 + f(1� �1)A+ �1Bg z1 +Bz
; (5.3.26)
where
q (z) =c
�1G (z)� c� �1
�1;
and
G(z) =
8><>: 2F1
�1; �1(B�C)
B; c+ 1; Bz
1+Bz
�; if B 6= 0;
1F1 (1; c+ 1;��1Az) ; if B = 0:
From (5:3:26) ; we have
Minjzj=r
Re pi(z) � Minjzj=r
Re q (z) :
By using the Lemma 5.2.2, we have minRe q(z) = q(�1): Consequently, we have p (z) 2
Pm [A;B; �1] where �1 is given by (5:3:21) : This shows that F (z) 2 Rm [A;B; �1].
Theorem 5.3.4 Let f (z) and g (z) belong to Vm [A;B; �] with m � 2; 0 � � < 1; and
�1 � B < A � 1: Then, the function F (z) with �1 = c = 1; de�ned by (5:3:20) is in the
91
class Vm [A;B; �] ; where 0 � � < � � 1;
� = �(�) = (1� (� + �) (1� �1)) (5.3.27)
and �1(�) is given by (5:3:1) :
Proof. From (5:3:20) ; we can easily write
(zF 0(z))0
F 0(z)= �
zf 0(z)
f(z)+ �
zg0(z)
g(z)+ 1� (� + �): (5.3.28)
Since f (z) and g (z) belong to Vm [A;B; �], then, by Theorem 5.3.1, zf 0(z)f(z)
and zg0(z)g(z)
belong to Pm [A;B; �1], where �1 = �1(�) is given by (5:3:1) : Using
zf 0(z)
f(z)= (1� �1)p1(z) + �1, p1 (z) 2 Pm [A;B] ;
andzg0(z)
g(z)= (1� �1)p2(z) + �1, p2 (z) 2 Pm [A;B] ;
in (5:3:28) ; we have
1
1� �
�(zF 0(z))0
F 0(z)� �
�=
�
� + �p1(z) +
�
� + �p2(z): (5.3.29)
Now by using the well known fact that the class Pm [A;B] is a convex set together with
(5:3:29), we obtain the required result.
5.4 Conclusion
We studied the class P [A;B; �] of generalized Janowski functions of order � along with
the functions with bounded boundary and bounded radius rotation. We investigated the
inclusion result with regard to order from the class Vm[A;B; �] to the class Rm[A;B; �]
in two di¤erent prospectives and some of its applications are also discussed.
92
Chapter 6
On Generalization of a Class of Analytic Functions
De�ned by Ruscheweyh Derivative
93
In 1994, Latha and Nanjunda [39] introduced the class Vm (�; b; �) of analytic functions
by using the Ruscheweyh derivative. As we discussed in Chapter 2 and 3 that the classes
of convex and starlike functions can be obtained from the class of �-convex functions
as special cases. This can also be done by Vm (�; b; �) ; that is, for speci�c values of the
parameters m; � and b; the class Vm (�; b; �) gives convex and starlike functions.
In this chapter, we will generalize the class Vm (�; b; �) with the concept of Janowski
functions and introduce the class V�m [A;B; �; b] : This generalized class contains many
known classes. The coe¢ cient bound, inclusion result and a radius problem will be
investigated here. Several known results will also be deducted from our main results as
special cases by assigning particular values to di¤erent parameters.
6.1 Introduction
Using the concept of generalized Janowski functions of order �; denoted by the class
P [A;B; �] ; discussed in section 2.6.2, we generalize the class Vm (�; b; �) ; introduced
by Latha and Nanjunda [39] but �rst we recall the de�nition of Pm[A;B; �]; given by
De�nition 5.1.1, for �1 � B < A � 1:
De�nition 6.1.1 A function p (z) is said to be in the class Pm[A;B; �]; if and only if;
p (z) =
�m
4+1
2
�p1 (z)�
�m
4� 12
�p2 (z) ; (6.1.1)
where p1 (z) ; p2 (z) 2 P [A;B; �] ; �1 � B < A � 1; m � 2; and 0 � � < 1.
It is clear that P2[A;B; �] � P [A;B; �] and Pm[1;�1; 0] � Pm; the well-known class
given and studied by Pinchuk [87].
Now using the concepts Ruscheweyh derivative along with the above class, we de�ne
the following.
94
De�nition 6.1.2 A function f (z) 2 A is in the class V�m [A;B; �; b] ; if and only if;�1� 2
b+2
b
D�+1f(z)
D�f(z)
�2 Pm [A;B; �] ; z 2 E;
where m � 2; � > �1; �1 � B < A � 1; 0 � � < 1 and b 2 C� f0g.
Assigning certain values to di¤erent parameters, we have di¤erent well-known classes
of analytic functions as can be seen below.
Special Cases
(i) V�m [1;�1; �; b] � Vm (�; b; �) ; the well-known class de�ned by Latha and Nanjunda
Rao in [39].
(ii) V12 [A;B; �; 1] � C [A;B; �] ; V02 [A;B; �; 2] � S� [A;B; �] ; the well-known class
de�ned by Polato¼glu [89].
(iii) V1m [A;B; 0; 1] � Vm [A;B] ; V02 [A;B; 0; 2] � Rm [A;B] ; where Vm [A;B] andRm [A;B]
denote the classes of Janowski functions with bounded boundary and bounded ra-
dius rotations respectively; given and studied by Noor [61, 64, 69].
6.2 Preliminary Results
We need the following results to obtain our main results.
Lemma 6.2.1 Let p (z) = 1 +1Pn=1
qnzn 2 Pm [A;B; �] : Then; for all n � 1;
jqnj �m (A�B) (1� �)
2: (6.2.1)
This inequality is sharp.
The proof follows from (2.4.1) ; (6.1.1) and the coe¢ cient bound of h 2 P [A;B] given
by Aouf [8]:
95
Lemma 6.2.2 Let p (z) 2 Pm [A;B; 0] with m � 2: Then; for jzj = r < 1;
2� (A�B)mr � 2ABr22 (1�B2r2)
� Rep(z) � jp(z)j � 2 + (A�B)mr � 2ABr22 (1�B2r2)
: (6.2.2)
The proof is immediate by using (6.1.1) and the growth result of h 2 P [A;B] ; see
[86].
Lemma 6.2.3 Let p (z) 2 Pm [A;B; 0] with m � 2: Then; for jzj = r < 1;
jzp0(z)j � r f(A�B)m� 4B (A�B) r +B2 (A�B)mr2gRep(z)(1�B2r2) (2 + (A�B)mr � 2ABr2) : (6.2.3)
The proof follows directly by using Lemma 6.2.2.
6.3 Main Results
Theorem 6.3.1 Let f (z) 2 V�m [A;B; �; b] with �1 � B < A � 1; � > �1; b 2
C� f0g ; 0 � � < 1: Then
janj �(�)n�1
(n� 1)!'n (�); n � 2; (6.3.1)
where � =m jbj (A�B) (1� �) (� + 1)
4and 'n (�) is given by (2.8.2) :
This result is sharp.
Proof. Set
1� 2b+2
b
D�+1f(z)
D�f(z)= p (z) ; (6.3.2)
so that p (z) 2 Pm [A;B; �] : Let p (z) = 1 +1Pn=1
qn zn: Then (6.3.2) can be written as
2�D�+1f(z)�D�f(z)
�= bD�f(z)
1Xn=1
qn zn;
96
which implies that
21Xn=2
('n (� + 1)� 'n (�)) anzn = b
1Xn=1
'n (�) anzn
! 1Xn=1
qn zn
!:
This implies that
21Xn=2
�� + n
� + 1'n (�)� 'n (�)
�anz
n =1Xn=2
bn�1Xj=1
'j (�) aj qn�j
!zn; a1 = 1:
Equating coe¢ cients of zn; we have
2'n (�) (n� 1) an(� + 1)
= bn�1Xj=1
'j (�) aj qn�j:
Using Lemma 6.2.1; we obtain
janj �m jbj (A�B) (1� �) (� + 1)
4 (n� 1)'n (�)
n�1Xj=1
'j (�) jajj
=�
(n� 1)'n (�)
n�1Xj=1
'j (�) jajj ; (6.3.3)
where � =m jbj (A�B) (1� �) (� + 1)
4: Now we prove that
n�1Xj=1
'j (�) jajj �n�2Yj=1
�1 +
�
j
�: (6.3.4)
For this, we use induction method. We see that it is true for n = 2; 3: Let it be true for
n = t; that is,t�1Xj=1
'j (�) jajj �t�2Yj=1
�1 +
�
j
�(6.3.5)
97
which gives along with (6:3:3)
jatj ��
(t� 1)'t (�)
t�2Yj=1
�1 +
�
j
�: (6.3.6)
Then considertXj=1
'j (�) jajj =t�1Xj=1
'j (�) jajj+ 't (�) jatj :
Using (6:3:5) and (6:3:6) in above relation, we have
tXj=1
'j (�) jajj �t�2Yj=1
�1 +
�
j
�+ 't (�)
�
(t� 1)'t (�)
t�2Yj=1
�1 +
�
j
�
=
�1 +
�
t� 1
� t�2Yj=1
�1 +
�
j
�
=t�1Yj=1
�1 +
�
j
�;
which shows that (6:3:4) is true for all n � 2: Thus from (6:3:3) and (6:3:4) ; we have
janj ��
(n� 1)'n (�)
n�2Yj=1
�1 +
�
j
�
=�
(n� 1)'n (�)
n�2Qj=1
(� + j)
n�2Qj=1
j
=(�)n�1
(n� 1)!'n (�):
98
This result is sharp for � > �1; 0 � � < 1; b 2 C� f0g and m � 2 as can be seen from
the functions f0 (z) which are given as
1� 2b+2
b
D�+1f0 (z)
D�f0 (z)= (1� �)
��m
4+1
2
�1 + Az
1 +Bz��m
4� 12
�1� Az
1�Bz
�+ �:
For di¤erent values of A; B; �; b and �; we obtain the following known results, proved
by Noor [57].
Corollary 6.3.1 If f (z) 2 V0m [1;�1; �; 2] = Rm (�) ; then
janj �(m (1� �))n�1(n� 1)! ; 8 n � 2:
This result is sharp.
Corollary 6.3.2 If f (z) 2 V1m [1;�1; �; 1] = Vm (�) ; then
janj �(m (1� �))n�1
n!; 8 n � 2:
This result is sharp.
Theorem 6.3.2 For real b > 0; V�+1m [A;B; �; b] � V�m [1;�1; �2; b+ 1] ; z 2 E; where
�2 (0 � �2 < 1) is one of the roots of
�1�2b2 (� + 2)2 (1� �)2 � b (� + 2) (1� �) [�1 (B + 1) + �2 (B � 1)] +
�B2 � 1
�= 0;
(6.3.7)
where
�1 =(1� b) + � (1 + b)
(1 + b) (1� �)
��1� (1 + b) (� + 1) (1� �)
b (� + 2) (1� �)
�(B � 1)� (A� 1)
�(6.3.8)
99
and
�2 =(1� b) + � (1 + b)
(1 + b) (1� �)
��1� (1 + b) (� + 1) (1� �)
b (� + 2) (1� �)
�(B + 1)� (A+ 1)
�: (6.3.9)
Proof. Suppose f (z) 2 V�+1m [A;B; �; b] and set
p (z) = 1� 2
b+ 1+
2
b+ 1
D�+1f(z)
D�f(z): (6.3.10)
where p (z) is analytic in E with p (0) = 1: Then
p (z) +2
b+ 1� 1 = 2
b+ 1
D�+1f(z)
D�f(z):
Di¤erentiating logarithmically, we have
zp0 (z)
p (z) + 2b+1
� 1=z�D�+1f(z)
�0D�+1f(z)
�z�D�f(z)
�0D�f(z)
which implies by using (2.8.4) that
zp0 (z)
p (z) + 2b+1
� 1=
(� + 2)D�+2f(z)� (� + 1)D�+1f(z)
D�+1f(z)� (� + 1)D
�+1f(z)� �D�f(z)
D�f(z)
=(� + 2)D�+2f(z)
D�+1f(z)� 1� (� + 1)D
�+1f(z)
D�f(z):
This implies that
1� 2b+2
b
D�+2f(z)
D�+1f(z)= 1� 2
b+
2
b (� + 2)+2 (� + 1)
b (� + 2)
D�+1f(z)
D�f(z)
+2
b (� + 2)
zp0 (z)
p (z) + 2b+1
� 1;
100
which reduces to
1� 2b+2
b
D�+2f(z)
D�+1f(z)= 1� b+ 1
b
� + 1
� + 2+b+ 1
b
� + 1
� + 2
�1� 2
b+ 1+
2
b+ 1
D�+1f(z)
D�f(z)
+2
(b+ 1) (� + 1)
zp0 (z)
p (z) + 2b+1
� 1
#
= (1� �1) + �1
�p(z) +
�2 zp0 (z)
p (z) + �3
�; (6.3.11)
where �1 =�+1�+2
b+1b; �2 =
2(�+1)(b+1)
; �3 =2b+1�1: Since f (z) 2 V�+1m [A;B; �; b] ; it follows
that
(1� �1) + �1
�p(z) +
�2 zp0 (z)
p (z) + �3
�2 Pm [A;B; �] ;
or, equivalently
(1� � � �1)
1� �+
�11� �
�p(z) +
�2 zp0 (z)
p (z) + �3
�2 Pm [A;B] : (6.3.12)
De�ne
' (z) =1
(1 + �3)
z
(1� z)�2+
�3(1 + �3)
z
(1� z)�2+1;
and by using convolution technique given by Noor [56], we have
p(z) +�2 zp
0 (z)
p (z) + �3=
�m
4+1
2
��p1 (z) +
�2 zp01 (z)
p1 (z) + �3
�
��m
4� 12
��p2 (z) +
�2 zp02 (z)
p2 (z) + �3
�:
By using (6.3.12) ; we see that
(1� � � �1)
1� �+
�11� �
�pi (z) +
�2 zp0i (z)
pi (z) + �3
�2 P [A;B] ; z 2 E; i = 1; 2:
101
Now; we want to show that pi (z) 2 P [A;B; �2] ; where �2 (0 � �2 < 1) is one of the
roots of (6.3.7). Let
pi (z) = (1� �2)hi (z) + �2; i = 1; 2:
Then
1� � � �1 (1� �2)
1� �+�1 (1� �2)
1� �
"hi (z) +
�2(1��2)
zh0i (z)
hi (z) +�3+�2(1��2)
#2 P [A;B] :
Using the fact illustrated in (5.1.1) ; we have
(B � 1)h�+ �
�hi (z) +
!1 zh0i(z)hi(z)+!2
�i� (A� 1)
(B + 1)h�+ �
�hi (z) +
!1 zh0i(z)hi(z)+!2
�i� (A+ 1)
2 P
where !1 =�21��2
; !2 =�3+�21��2
; � = 1����1(1��2)1�� and � = �1(1��2)
1�� : This implies that
(B � 1) [(�+ �hi(z)) (hi(z) + !2) + !1�zh0i(z)]� (A� 1) (hi(z) + !2)
(B + 1) [(�+ �hi(z)) (hi(z) + !2) + !1�zh0i(z)]� (A+ 1) (hi(z) + !2)2 P;
We now form the functional (u; v) by choosing u = hi(z); v = zh0i(z) and note that the
�rst two conditions of Lemma 2.10.4 are clearly satis�ed. We check condition (iii) as
follows.
(u; v) =(B � 1) [(�+ �u) (u+ !2) + !1�v]� (A� 1) (u+ !2)
(B + 1) [(�+ �u) (u+ !2) + !1�v]� (A+ 1) (u+ !2)
=�1 + !1� (B � 1) v + [(�+ � (u+ !2)) (B � 1)� (A� 1)]u�2 + !1� (B + 1) v + [(�+ � (u+ !2)) (B + 1)� (A+ 1)]u
:
where �1 = !2 [� (B � 1)� (A� 1)] and �2 = !2 [� (B + 1)� (A+ 1)] : Now
(iu2; v1) =�1 + � (!1v1 � u22) (B � 1) + [(�+ �!2) (B � 1)� (A� 1)] iu2�2 + � (!1v1 � u22) (B + 1) + [(�+ �!2) (B + 1)� (A+ 1)] iu2
:
Taking real part of (iu2; v1); we have
102
Re (iu2; v1) =
[��1 + � (!1v1 � u22) (1�B)] [�2 + � (!1v1 � u22) (B + 1)]�
[(�+ �!2) (B � 1)� (A� 1)] [(�+ �!2) (B + 1)� (A+ 1)]u22�[�2+�(!1v1+u2)(B+1)]2�[(�+�!2)(B+1)�(A+1)]2u22
:
As !1 > 0; � > 0; so applying v1 � �12(1 + u22) and after a little simpli�cation; we have
Re (iu2; v1) �A1 +B1u
22 + C1u
42
D1
; (6.3.13)
where
A1 =1
4[2�1 � !1� (B � 1)] [2�2 � !1� (B + 1)] ;
B1 = �12� (!1 + 2)
��1 (B + 1)� !1�
�B2 � 1
�+ �2 (B � 1)
�+
(�+ �!2)2 �B2 � 1
�� 2 (�+ �!2) (AB � 1) +
�A2 � 1
�;
C1 = �14�2�1�B2
�(!1 + 2)
2 ;
and
D1 = [�2 + � (!1v1 + u2) (B + 1)]2 + [(�+ �!2) (B + 1)� (A+ 1)]2 u22:
The right hand side of (6.3.13) is negative if A1 � 0 and B1 � 0: From A1 � 0; we have
�2 to be one of the roots of
�1�2b2 (� + 2)2 (1� �)2 � b (� + 2) (1� �) [�1 (B + 1) + �2 (B � 1)] +
�B2 � 1
�= 0
with 0 � �2 < 1 and also for 0 � �2 < 1; we have B1 � 0:
Since all the conditions of Lemma 2.10.4 are satis�ed; it follows that hi (z) 2 P; i = 1; 2
and consequently p (z) 2 Pm [1;�1; �2] :Hence from (6.3.10) ; f (z) 2 V�m [1;�1; �2; b+ 1] :
103
By choosing the parameters A = 1; B = �1; b = 1 and � = 0; we obtain the following
known result; proved in [80].
Corollary 6.3.3 Let f (z) 2 Vm (�) : Then f (z) 2 Rm (�2) ; where �2 is a root of
2�22 � (2� � 1) �2 � 1 = 0 with 0 � �2 < 1;
which is
�2 =1
4
�(2� � 1) +
q4�2 � 4� + 9
�:
Corollary 6.3.4 For � = 0; m = 2 in Corollary 6.3.3; we have the following well known
result [24].
V2 (0) = C � R2
�1
2
�= S�
�1
2
�; for z 2 E.
Theorem 6.3.3 Let f (z) 2 V�m [A;B; 0; b] ; � > �1; b > 0 (real); m � 2 and 0 < a =
b(�+1)2
� 1. Then D�f(z) maps jzj < r0 onto a convex domain; where r0 is the least
positive root of the equation
a1r4 + a2r
3 + a3r2 + a4r + 4 (2a� 1) = 0 with 0 � r < 1; (6.3.14)
where
a1 = 4a2A2B2 � 4 (a� 1)2B4;
a2 = 2a (2a� 1) (B � A)B2m;
a3 = 8a2 (a� 2) + 8a (1� a)AB � a2 (A�B)2m2;
and
a4 = 2a (2a� 3) (A�B)m:
This result is sharp.
104
Proof. Since f (z) 2 V�m [A;B; 0; b] ; then
D�+1f(z)
D�f(z)=b (p (z)� 1) + 2
2; (6.3.15)
where p (z) 2 Pm [A;B; 0] : Using the identity (2.8.4) ; we consider
z�D�f(z)
�0D�f(z)
= (� + 1)D�+1f(z)
D�f(z)� �:
Using (6.3.15) in above relation, we obtain
z�D�f(z)
�0D�f(z)
=b (p (z)� 1) (� + 1) + 2
2: (6.3.16)
Logarithmic di¤erentiation of (6.3.16) yields
�z�D�f(z)
�0�0(D�f(z))0
�z�D�f(z)
�0D�f(z)
=b(�+1)2
zp0 (z)b(�+1)2
p (z)� b(�+1)2
+ 1
which implies that
�z�D�f(z)
�0�0(D�f(z))0
= ap(z)� a+ 1 +zp0(z)
p(z)� 1 + 1a
;
where a = b(�+1)2
: Then; we have
Re
1 +
z�D�f(z)
�00(D�f(z))0
!� aRe p(z) + (1� a)� a jzp0(z)j
jap(z) + 1� aj : (6.3.17)
105
Now using Lemma 6.2.2, we see that
1
jap(z) + 1� aj � 1
a jp(z)j � j1� aj
� 1
a2�(A�B)mr�2ABr2
2(1�B2r2) � (1� a); a � 1
=2 (1�B2r2)
2 (2a� 1)� a (A�B)mr + 2 (B2 � a (A+B)B) r2:(6.3.18)
Using (6:3:18) ; Lemma 6.2.2 and Lemma 6.2.3; we have from (6:3:17) ;
Re
1 +
z�D�f(z)
�00(D�f(z))0
!� Re p(z)
�a+
2 (1� a) (1�B2r2)
2 + (A�B)mr � 2ABr2
� 2ar f(A�B)m� 4B (A�B) r +B2 (A�B)mr2g(2 + (A�B)mr � 2ABr2) �
�
= Re p(z)
�a1r
4 + a2r3 + a3r
2 + a4r + 4 (2a� 1)(2 + (A�B)mr � 2ABr2) �
�> 0;
provided
T (r) = a1r4 + a2r
3 + a3r2 + a4r + 4 (2a� 1) > 0;
where
a1 = 4a2A2B2 � 4 (a� 1)2B4;
a2 = 2a (2a� 1) (B � A)B2m;
a3 = 8a2 (a� 2) + 8a (1� a)AB � a2 (A�B)2m2;
a4 = 2a (2a� 3) (A�B)m;
106
and
� = 2 (2a� 1)� a (A�B)mr + 2�B2 � a (A+B)B
�r2:
We have T (0) > 0 and T (1) < 0: Therefore D�f(z) maps jzj < r0 onto a convex domain;
where r0 is the least positive root of the equation T (r) = 0; lying in (0; 1).
For D�f1 (z) such thatD�+1f1 (z)
D�f1 (z)=b (pm (z)� 1) + 2
2;
where pm (z) =2+(A�B)mz�2ABz2
2(1�B2z2) ; we have
�z�D�f1(z)
�0�0(D�f1(z))
0 =a1r
4 + a2r3 + a3r
2 + a4r + 4 (2a� 1)(2 + (A�B)mr � 2ABr2) � = 0;
for z = r0. Hence this radius r0 is sharp.
By choosing the parameters A = 1; B = �1; m = 2; b = 2 and � = 0; we obtain the
following known result [24].
Corollary 6.3.5 Let f (z) 2 S�. Then f (z) maps jzj < r0 onto a convex domain; where
r0 is the least positive root of the equation
r4 � 2r3 � 6r2 � 2r + 1 = 0 with 0 � r < 1;
which is r0 = 2�p3: This is also sharp.
6.4 Conclusion
We generalized the class Vm (�; b; �) with the concept of Janowski functions and intro-
duced the class V�m [A;B; �; b] : This generalized class contains many known classes and
we included them as special cases. The coe¢ cient bound, inclusion result and a radius
problem are investigated. Several known results are deducted from our main results as
special cases by assigning particular values to di¤erent parameters.
107
Chapter 7
On Janowski Functions Associated with Conic
Domains
108
In the study of analytic functions, geometry of image domain has undoubtedly a great
importance. Analytic functions are classi�ed into many classes and then into subclasses
depending upon the shape of image domain and other geometrical properties. It has been
a matter of discussion that there always exist analytic functions with di¤erent geometrical
structures as their image domains. Since Goodman [22, 23] introduced parabolic region as
image domain and de�ned the function which gives exactly parabolic region as its image
domain. After that Kanas and Wisniowska [36, 35] contributed in form of hyperbolic and
elliptic regions along with their extremal functions. For details, see section 2.6.1. Before
all this, Janowski introduced circular regions and their extremal functions as discussed
in section 2.6.2.
In this chapter, we will introduce new geometrical structures of oval and petal type
shape as image domain and de�ne the classes of functions which give these types of map-
pings. The concepts of Janowski functions and conic domains are combined together to
de�ne a new domain k [A;B] which represents the oval and petal type regions. Di¤erent
graphical views of this new domain for speci�c values of parameters will be shown in or-
der to have better understanding of the behaviour of this domain k [A;B] : This domain
gives both conic and circular domains as special cases which is the main motivation of
this chapter. Moreover, two new classes k�UCV [A;B] of k-uniformly Janowski convex
and k � ST [A;B] of k- Janowski starlike functions will be de�ned and our main results
will be based on their properties.
A number of already known classes of analytic functions can easily be obtained from
our new classes as special cases. The class SD (k; �) discussed in section 2.6.1 is also a
special case of our new class k�ST [A;B] : The coe¢ cient bound for the class SD (k; �),
proved by Owa et al. [83] is improved, that is, the coe¢ cient bound for class SD (k; �)
obtained from our main results as special case gives much better result as compared to
that one, proved by Owa et al. [83].
It is to be mentioned here that some of the contents of this chapter have been pub-
lished in a well reputed journal "Computers and Mathematics with Applications, Vol
109
62; 2011; Pages 2209� 2217", for detail, see[73].
7.1 Introduction
The classes S� (�) and C (�) are the well-known classes of starlike and convex univalent
functions of order � (0 � � < 1) respectively, discussed in section 2.4. The class P [A;B]
represents the class of Janowski functions which we have de�ned in section 2.6.2 and its
connection with the class P of functions with positive real part is also shown there by
(2:6:9) : The circular domain [A;B] from which Janowski functions take values is given
by (2:6:8) :
Kanas and Wisniowska [36, 35] introduced and studied the class k � UCV of k-
uniformly convex functions and the corresponding class k � ST of k-starlike functions.
These classes were de�ned subject to the conic domain k; k � 0 which is de�ned by
(2:6:1) : These classes were then generalized to KD (k; �) and SD (k; �) respectively by
Shams et.al [101] subject to the conic domain G (k; �) ; k � 0; 0 � � < 1; which is
de�ned by (2:6:7) :
Now using the concepts of Janowski functions and the conic domain, we de�ne the
following.
De�nition 7.1.1 A function p (z) is said to be in the class k � P [A;B] ; if and only if,
p (z) � (A+ 1) pk(z)� (A� 1)(B + 1) pk(z)� (B � 1)
; k � 0; (7.1.1)
where pk(z) is de�ned by (2:6:2) and �1 � B < A � 1: Geometrically, the function
p (z) 2 k�P [A;B] takes all values from the domain k [A;B] ; �1 � B < A � 1; k � 0
which is de�ned as:
k [A;B] =
�w : Re
�(B � 1)w(z)� (A� 1)(B + 1)w(z)� (A+ 1)
�> k
����(B � 1)w(z)� (A� 1)(B + 1)w(z)� (A+ 1) � 1�����(7.1.2)
110
or equivalently
k [A;B] =nu+ iv :
��B2 � 1
� �u2 + v2
�� 2 (AB � 1)u+
�A2 � 1
��2> k2
h��2 (B + 1)
�u2 + v2
�+ 2 (A+B + 2)u� 2 (A+ 1)
�2+4 (A�B)2 v2
�:
The domain k [A;B] represents the conic type regions as shown in the �gures below.
Figure 7.1: Boundary of domain k [0:5;�0:5]
Figure 7.2: Boundary of domain k [0:8; 0:2]
111
The domain k [A;B] retains the conic domain k inside the circular region de�ned by
[A;B] : The impact of [A;B] on the conic domain k changes the original shape of
the conic regions. The ends of hyperbola and parabola get closer to each other but never
meet anywhere and the ellipse gets the shape of oval as shown in �gures 7.1, 7.2 above.
When A �! 1; B �! �1; the radius of the circular disk de�ned by [A;B] tends to
in�nity, consequently the arms of hyperbola and parabola expand and the oval turns into
ellipse as shown in �gures below.
Figure 7.3: View of k [A;B] when A! 1; B ! �1:
Figure 7.4: Close view of Fig. 7.3.
It can be seen that k [1;�1] = k; the conic domain de�ned by Kanas and Wisniowska
[36]. Here are some basic facts about the class k � P [A;B] :
112
Remark 7.1.1 1. k � P [A;B] � P�2k+1�A2k+1�B
�; the class of functions with real part
greater than 2k+1�A2k+1�B :
2. k � P [1;�1] = P (pk) ; the well-known class introduced by Kanas and Wisniowska
[36].
3. 0� P [A;B] = P [A;B] ; the well-known class introduced by Janowski [30].
Now we de�ne the classes k � UCV [A;B] of k-uniformly Janowski functions and
k � ST [A;B] of k-Janowski starlike functions as follows.
De�nition 7.1.2 A function f (z) 2 A is said to be in the class k�UCV [A;B] ; k � 0;
�1 � B < A � 1; if and only if ,
Re
0@(B � 1) (zf 0(z))0f 0(z) � (A� 1)
(B + 1) (zf0(z))0
f 0(z) � (A+ 1)
1A > k
������(B � 1)(zf 0(z))0
f 0(z) � (A� 1)
(B + 1) (zf0(z))0
f 0(z) � (A+ 1)� 1
������ ;or equivalently,
(zf 0(z))0
f 0 (z)2 k � P [A;B] : (7.1.3)
De�nition 7.1.3 A function f (z) 2 A is said to be in the class k � ST [A;B] ; k � 0;
�1 � B < A � 1; if and only if ,
Re
(B � 1) zf
0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)
!> k
�����(B � 1)zf 0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)� 1����� ;
or equivalently,zf 0(z)
f (z)2 k � P [A;B] : (7.1.4)
It can be easily seen that
f (z) 2 k � UCV [A;B] () zf 0 (z) 2 k � ST [A;B] : (7.1.5)
113
Special Cases
(i) k � ST [1;�1] = k � ST; k � UCV [1;�1] = k � UCV; the well-known classes of
k-uniformly convex and k-starlike functions respectively, introduced by Kanas and
Wisniowska [36, 35].
(ii) k � ST [1� 2�;�1] = SD (k; �) ; k � UCV [1� 2�;�1] = KD (k; �) ; the classes,
introduced by Shams et.al in [101].
(iii) 0 � ST [A;B] = S� [A;B] ; 0 � UCV [A;B] = C [A;B] ; the well-known classes
of Janowski starlike and Janowski convex functions respectively, introduced by
Janowski [30].
Now we discuss some results concerning above classes.
7.2 Main results
Our �rst result is a su¢ cient condition for a function f (z) 2 A to be from k�ST [A;B] :
It gives many known results as special cases as discussed after this result.
Theorem 7.2.1 A function f (z) 2 A and of the form (2:1:1) is in the class k �
ST [A;B] ; if it satis�es the condition
1Xn=2
f2 (k + 1) (n� 1) + jn (B + 1)� (A+ 1)jg janj < jB � Aj ; (7.2.1)
where �1 � B < A � 1 and k � 0:
Proof. Assuming that (7:2:1) holds, then it su¢ ces to show that
k
�����(B � 1)zf 0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)� 1������ Re
"(B � 1) zf
0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)� 1#< 1:
114
We have
k
�����(B � 1)zf 0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)� 1������ Re
"(B � 1) zf
0(z)f(z)
� (A� 1)
(B + 1) zf0(z)f(z)
� (A+ 1)� 1#
� (k + 1)����(B � 1) zf 0 (z)� (A� 1) f (z)(B + 1) zf 0 (z)� (A+ 1) f (z) � 1
����= 2 (k + 1)
���� f (z)� zf 0 (z)
(B + 1) zf 0 (z)� (A+ 1) f (z)
����
= 2 (k + 1)
��������1Pn=2
(1� n) anzn
(B � A) z +1Pn=2
fn (B + 1)� (A+ 1)g anzn
��������
� 2 (k + 1)
1Pn=2
j1� nj janj
jB � Aj �1Pn=2
jn (B + 1)� (A+ 1)j janj:
The last expression is bounded above by 1 if
1Xn=2
f2 (k + 1) (n� 1) + jn (B + 1)� (A+ 1)jg janj < jB � Aj
and this completes the proof.
When A = 1; B = �1 in above theorem, then we have the following known result,
proved by Kanas and Wisniowska in [35].
Corollary 7.2.1 A function f (z) 2 A and of the form (2:1:1) is in the class k � ST; if
115
it satis�es the condition
1Xn=2
fn+ k (n� 1)g janj < 1; k � 0:
When A = 1 � 2�; B = �1 with 0 � � < 1 in Theorem 7.2.1, then we have the
following known result, proved by Shams et.al in [101].
Corollary 7.2.2 A function f (z) 2 A and of the form (2:1:1) is in the class SD (k; �) ;
if it satis�es the condition
1Xn=2
fn (k + 1)� (k + �)g janj < 1� �;
where 0 � � < 1 and k � 0:
When A = 1 � 2�; B = �1 with 0 � � < 1 and k = 0 in Theorem 7.2.1, then we
have the following known result, proved by Selverman in [100].
Corollary 7.2.3 A function f (z) 2 A and of the form (2:1:1) is in the class S� (�) ; if
it satis�es the condition
1Xn=2
(n� �) janj < 1� �; 0 � � < 1:
Theorem 7.2.2 A function f (z) 2 A and of the form (2:1:1) is in the class k �
UCV [A;B] ; if it satis�es the condition
1Xn=2
n f2 (k + 1) (n� 1) + jn (B + 1)� (A+ 1)jg janj < jB � Aj ;
where �1 � B < A � 1 and k � 0:
Proof follows immediately by using Theorem 7.2.1 and (7:1:5) :
Now we �nd the coe¢ cient bound for functions of k�ST [A;B] : It gives many known
results as special cases. Also it gives a re�nement in one already known result.
116
Theorem 7.2.3 Let f (z) 2 k � ST [A;B] and is of the form (2:1:1) : Then, for n � 2;
janj �n�2Yj=0
j�k (A�B)� 2jBj2 (j + 1)
; (7.2.2)
where �k is de�ned by (2:6:3) :
Proof. By de�nition, for f (z) 2 k � ST [A;B] ; we have
zf 0 (z)
f (z)= p (z) ; (7.2.3)
where
p (z) � (A+ 1) pk(z)� (A� 1)(B + 1) pk(z)� (B � 1)
= [(A+ 1) pk(z)� (A� 1)] [(B + 1) pk(z)� (B � 1)]�1
=
�A� 1B � 1 �
A+ 1
B � 1pk(z)�"1 +
1Xn=1
�B + 1
B � 1pk(z)�n#
=A� 1B � 1 �
A+ 1
B � 1pk(z) +A� 1B � 1
1Xn=1
�B + 1
B � 1pk(z)�n
�A+ 1B � 1pk(z)
1Xn=1
�B + 1
B � 1pk(z)�n
=A� 1B � 1 +
�(A� 1) (B + 1)(B � 1)2
� A+ 1
B � 1
�pk(z)
+
(A� 1) (B + 1)2
(B � 1)3� (A+ 1) (B + 1)
(B � 1)2
!(pk(z))
2
+
(A� 1) (B + 1)3
(B � 1)4� (A+ 1) (B + 1)
2
(B � 1)3
!(pk(z))
3 + � � � :
117
If pk(z) = 1 + �kz + � � � ; then we have
p (z) � A� 1B � 1 +
�(A� 1) (B + 1)(B � 1)2
� A+ 1
B � 1
�(1 + �kz + � � � )
+
(A� 1) (B + 1)2
(B � 1)3� (A+ 1) (B + 1)
(B � 1)2
!(1 + �kz + � � � )2
+
(A� 1) (B + 1)3
(B � 1)4� (A+ 1) (B + 1)
2
(B � 1)3
!(1 + �kz + � � � )3 + � � �
=
(A� 1B � 1 +
(A� 1) (B + 1)(B � 1)2
� A+ 1
B � 1 +(A� 1) (B + 1)2
(B � 1)3
�(A+ 1) (B + 1)(B � 1)2
+ :::
�+
�(A� 1) (B + 1)(B � 1)2
� A+ 1
B � 1
+2
(A� 1) (B + 1)2
(B � 1)3� (A+ 1) (B + 1)
(B � 1)2
!
+3
(A� 1) (B + 1)3
(B � 1)4� (A+ 1) (B + 1)
2
(B � 1)3
!)�kz + :::
=
(�2B � 1 �
2 (B + 1)
(B � 1)2� 2 (B + 1)
2
(B � 1)3� :::
)
+
�(A� 1) (B + 1)� (A+ 1) (B � 1)
(B � 1)2
+2 (B + 1)
�(A� 1) (B + 1)� (A+ 1) (B � 1)
(B � 1)3�
+3 (B + 1)2�(A� 1) (B + 1)� (A+ 1) (B � 1)
(B � 1)4��
�kz + :::
=
1Xn=1
�2 (B + 1)n�1
(B � 1)n +
( 1Xn=1
2n (A�B) (B + 1)n�1
(B � 1)n+1
)�kz + � � � :
Now we see that the series1Pn=1
�2(B+1)n�1(B�1)n and
1Pn=1
2n(A�B)(B+1)n�1
(B�1)n+1 are convergent and
converge to 1 and A�B2respectively. Therefore,
p (z) � 1 + 12(A�B) �kz + � � � :
118
Now if p(z) = 1 +1Pn=1
cnzn; then by Lemma 2.10.5, we have
jcnj �1
2(A�B) j�kj ; n � 1: (7.2.4)
Now from (7:2:3) ; we have
zf 0 (z) = f (z) p (z) ;
which implies that
z +1Xn=2
nan zn =
z +
1Xn=2
an zn
! 1 +
1Xn=1
cn zn
!:
Equating coe¢ cients of zn on both sides, we have
(n� 1) an =n�1Xj=1
an�jcj; a1 = 1:
This implies that
janj �1
n� 1
n�1Xj=1
jan�jj jcjj ; a1 = 1:
Using (7:2:4) ; we have
janj �j�kj (A�B)
2 (n� 1)
n�1Xj=1
jajj ; a1 = 1: (7.2.5)
Now we prove that
j�kj (A�B)
2 (n� 1)
n�1Xj=1
jajj �n�2Yj=0
j�k (A�B)� 2jBj2 (j + 1)
: (7.2.6)
For this, we use induction method.
For n = 2;
119
From (7:2:5) ; we have
ja2j �j�kj (A�B)
2:
From (7:2:2) ; we have
ja2j �j�kj (A�B)
2:
For n = 3;
From (7:2:5) ; we have
ja3j �j�kj (A�B)
4(1 + ja2j)
� j�kj (A�B)
4
�1 +
j�kj (A�B)
2
�:
From (7:2:2) ; we have
ja3j �j�kj (A�B)
2
j�k (A�B)� 2Bj4
� j�kj (A�B)
2
j�kj (A�B) + 2 jBj4
� j�kj (A�B)
2
�j�kj (A�B)
2+ 1
�:
Let the hypothesis be true for n = m:
From (7:2:5) ; we have
jamj �j�kj (A�B)
2 (m� 1)
m�1Xj=1
jajj ; a1 = 1:
120
From (7:2:2) ; we have
jamj �m�2Yj=0
j�k (A�B)� 2jBj2 (j + 1)
�m�2Yj=0
j�kj (A�B) + 2j
2 (j + 1):
By induction hypothesis, we have
j�kj (A�B)
2 (m� 1)
m�1Xj=1
jajj �m�2Yj=0
j�kj (A�B) + 2j
2 (j + 1):
Multiplying both sides by j�kj(A�B)+2(m�1)2m
; we have
m�1Yj=0
j�kj (A�B) + 2j
2 (j + 1)� j�kj (A�B)
2 (m� 1)j�kj (A�B) + 2 (m� 1)
2m
m�1Xj=1
jajj
=j�kj (A�B)
2m
(j�kj (A�B)
2 (m� 1)
m�1Xj=1
jajj+m�1Xj=1
jajj)
� j�kj (A�B)
2m
(jamj+
m�1Xj=1
jajj)
=j�kj (A�B)
2m
mXj=1
jajj :
That is,j�kj (A�B)
2m
mXj=1
jajj �m�1Yj=0
j�kj (A�B) + 2j
2 (j + 1);
which shows that the inequality (7:2:6) is true for n = m+ 1: Hence the required result.
121
Corollary 7.2.4 When A = 1; B = �1; then (7:2:2) reduces to
janj �n�2Yj=0
j�k + jjj + 1
; n � 2;
which is the coe¢ cient inequality of the class k�ST; introduced by Kanas and Wisniowska
[35].
Corollary 7.2.5 When A = 1� 2�; B = �1 with 0 � � < 1; then (7:2:2) reduces to
janj �n�2Yj=0
j�k (1� �) + jjj + 1
; n � 2; (7.2.7)
which is the coe¢ cient inequality of the class SD (k; �) ; introduced by Shams et.al [101].
The inequality (7:2:7) gives the better result as compared with that, proved by Owa
et al. [83]. Owa et al. [83] gave the following coe¢ cient bound of SD (k; �) ;
ja2j � 2(1��)j1�kj ;
janj � 2(1��)(n�1)j1�kj
n�2Qj=1
�1 + 2(1��)
jj1�kj
�; n � 3:
9>=>; (7.2.8)
According to (7:2:8) ; for k = 12; � = 1
2; we have ja2j � 2 but from (7:2:7) we have
ja2j � 0:5926 which clearly shows that our result is far better than that of Owa et al.
[83].
When k = 0; then �k = 2 and from Theorem 7.2.3 we get the following known result,
proved in [30].
Corollary 7.2.6 Let f (z) 2 S� [A;B] and is of the form (2:1:1) : Then, for n � 2;
janj �n�2Yj=0
j(A�B)� jBjj + 1
; �1 � B < A � 1:
When A = 1 � 2�; B = �1 with 0 � � < 1 and k = 0 in Theorem 7.2.3, then we
have the following known result, see [24].
122
Corollary 7.2.7 Let f (z) 2 S� (�) and is of the form (2:1:1) : Then, for n � 2;
janj �
nQj=2
(j � 2�)
(n� 1)! ; 0 � � < 1:
Theorem 7.2.4 Let f (z) 2 k�UCV [A;B] and is of the form (2:1:1) : Then, for n � 2;
janj �1
n
n�2Yj=0
j�k (A�B)� 2jBj2 (j + 1)
; (7.2.9)
where �k is de�ned by (2:6:3) :
Proof follows immediately by using Theorem 7.2.3 and (7:1:5) :
Theorem 7.2.5 Let f (z) 2 S: Then f (z) 2 k � UCV [A;B] for jzj < r0 < 1 with
r0 =2�
p3 + �2
1 + �;
where
� =2k + 1� A
2k + 1�B: (7.2.10)
Proof can be done by using similar technique as used in Theorem 4.2.3.
When A = 1; B = �1 and k = 0 in Theorem 7.2.5, then we have the following result,
proved in [24].
Corollary 7.2.8 Let f (z) 2 S: Then f (z) 2 C for jzj < r0 < 1 with r0 = 2�p3:
When A = 1; B = �1 and k = 1 in Theorem 7.2.5, then we have the following result,
proved in [96].
Corollary 7.2.9 Let f (z) 2 S: Then f (z) 2 UCV for jzj < r0 < 1 with
r0 =4�
p13
3:
123
When A = 1 and B = �1 in Theorem 7.2.5, then we have the following result, proved
by Kanas and Wisniowska [36].
Corollary 7.2.10 Let f (z) 2 S: Then f (z) 2 k � UCV for jzj < r0 < 1 with
r0 =2 (k + 1)�
p4k2 + 6k + 3
2k + 1:
Now we have an extension of the Lemma 2.10.1 proved in [33].
Lemma 7.2.1 Let 0 � k <1: Also, let �; 2 C be such that � 6= 0 and Re (�� + ) >
0; where � is de�ned by (7:2:10) : If p (z) is analytic in E; p (0) = 1; p (z) satis�es
p (z) +zp0 (z)
�p (z) + � pk (A;B; z) ; (7.2.11)
where
pk (A;B; z) =(A+ 1) pk(z)� (A� 1)(B + 1) pk(z)� (B � 1)
and if q (z) is analytic solution of
q (z) +zq0 (z)
�q (z) + = pk (A;B; z) ;
then q (z) is univalent, p (z) � q (z) � pk (A;B; z) and q (z) is the best dominant of
(7:2:11) :
Proof follows similarly as given in [33].
Moreover, the solution q (z) is given by
q (z) =
��
Z 1
0
�t�+ �1 exp
Z tz
z
pk (A;B;u)� 1u
du
��dt
��1�
�:
For more details of best dominant, we refer to [33, 53].
124
As a special case, when � = 1 and = 0; we have the function q (z) as
q (z) =
24 1Z0
0@exp tzZz
pk (A;B;u)� 1u
du
1A dt
35�1 : (7.2.12)
Now we see a few applications of the Lemma 7.2.1.
When k > 1; the domain k [A;B] may be characterized by the circular domain
having its diameter end points as the vertices of the oval (or ellipse). As we see that the
vertices of oval (or ellipse) are (�; 0) and (�1; 0) ; where � is de�ned by (7:2:10) and
�1 =2k + A� 12k +B � 1 :
The circle K (X;R) having diameter end points (�; 0), (�1; 0) has its center at
X�4k2�(A�1)(B�1)4k2�(B�1)2 ; 0
�and radius R as
R =2k (A�B)
4k2 � (B � 1)2:
The point z = 1 is contained inside the circleK (X;R) and then the function �k (A;B; z) :
E �! K (X;R) has the form
�k (A;B; z) =2k + (A� 1) z2k + (B � 1) z :
Theorem 7.2.6 Let k 2 (1;1) : Also, let p (z) be analytic in E with p (0) = 1 and p (z)
satis�es (7:2:11) : Then
p (z) �
8>>>>><>>>>>:(1�A)z2k
��1 + (B�1)z
2k
�B�AB�1 �
�1 + (B�1)z
2k
���1; �1 < B < A < 1;
z
(z�k) log(1� zk); A = 1; B = �1;
125
and
Re p (z) >
8>>>><>>>>:A�12k
h�1� B�1
2k
�B�AB�1 �
�1� B�1
2k
�i�1; �1 < B < A < 1;
1
(k+1) log(1+ 1k); A = 1; B = �1:
Proof. Since p satis�es (7:2:11) and for each �xed k; pk (A;B; z) � �k (A;B; z) ; so
p (z) � �k (A;B; z) : This implies from (7:2:12) ;
q (z) =
24 1Z0
0@exp tzZz
�k (A;B;u)� 1u
du
1A dt
35�1
=
24 1Z0
0@exp tzZz
2k+(A�1)u2k+(B�1)u � 1
udu
1A dt
35�1
=
24 1Z0
0@exp tzZz
A�B
2k + (B � 1)udu
1A dt
35�1
=
24 1Z0
�exp
��A�B
B � 1
�log
2k + (B � 1) tz2k + (B � 1) z
��dt
35�1
=
24 1Z0
�2k + (B � 1) tz2k + (B � 1) z
�A�BB�1
dt
35�1
=
24� 1
2k + (B � 1) z
�A�BB�1
1Z0
(2k + (B � 1) tz)A�BB�1 dt
35�1
=(A� 1) z
(2k + (B � 1) z)B�AB�1
�(2k + (B � 1) z)
A�1B�1 � (2k)
A�1B�1��1
=(1� A) z
2k
(2k + (B � 1) z)A�BB�1
(2k)A�BB�1
241� �1 + (B � 1) z2k
�A�1B�135�1
126
=(1� A) z
2k
�1 +
(B � 1) z2k
�A�BB�1
241� �1 + (B � 1) z2k
�A�BB�1 +1
35�1
=(1� A) z
2k
"�1 +
(B � 1) z2k
�B�AB�1
��1 +
(B � 1) z2k
�#�1:
Also we have
Re p (z) > q (�1) =
8>>>><>>>>:A�12k
h�1� B�1
2k
�B�AB�1 �
�1� B�1
2k
�i�1; �1 < B < A < 1;
1
(k+1) log(1+ 1k); A = 1; B = �1;
for z 2 E:
The above Lemma 7.2.1 and Theorem 7.2.6 have been proved only for A = 1; B = �1
by Kanas [33].
Theorem 7.2.7 If f (z) 2 A satis�es the inequality
Re
( zf 00(z)f 0(z)
zf 0(z)f(z)
� 1
)<3� �
2� �;
where � is de�ned by (7:2:10) ; then f (z) 2 k � ST [A;B] ; k � 0; with �1 � B < 0 and
B < A � 1:
Proof can be done by using similar technique as used in Theorem 4.2.1.
From the Theorem 7.2.7, we see that when A = 1; B = �1 and k = 1; we have the
following result which is the special case (when p = 1) of the result proved by Al-Kharsani
et.al [6].
Corollary 7.2.11 If f (z) 2 A satis�es the inequality
Re
( zf 00(z)f 0(z)
zf 0(z)f(z)
� 1
)<5
3;
127
then f (z) is uniformly starlike in E (that is f (z) 2 1� ST ).
7.3 Conclusion
We introduced new geometrical structures of oval and petal type shaped as image domain
and de�ned the classes of functions which give these types of mappings. We introduced
the domain k [A;B] which represents the oval and petal type regions. Di¤erent graphical
views of this new domain for speci�c values of parameters are shown in order to have
better understanding of the behaviour of this domain k [A;B] : Moreover, two new
classes k�UCV [A;B] of k-uniformly Janowski convex and k�ST [A;B] of k- Janowski
starlike functions are de�ned and a number of already known classes of analytic functions
are obtained from these classes as special cases. We investigated certain properties of
these classes. We improved the coe¢ cient bound of the class SD (k; �) which was proved
by Owa et al. [83].
128
Chapter 8
Conclusion
129
This research is carried out on analytic functions associated with conic domains. In this
thesis, we generalized the conic domains and circular domains. We removed the de�ciency
in already known conic domains and made it able to magnify as well as contract. We also
introduced new petal and oval type domains by combining conic and circular domains.
We de�ned certain classes of analytic functions which give these types of mappings. Many
of our results are re�nement of already known results. The concept of our new introduced
domains and their respective classes of analytic functions will open a new direction of
future research. Various di¤erential and integral operators can be applied to introduce
and study new classes of analytic functions and many other geometrical properties can
also be studied.
It is worthy to mention that most of this work has been published in well reputed
journals as listed below.
1. Khalida Inayat Noor and Sarfraz Nawaz Malik (2012). On generalized bounded
Mocanu variation associated with conic domain, Math. Comput. Modell. 55,
844-852.
2. Khalida Inayat Noor and Sarfraz Nawaz Malik (2011). On a new class of analytic
functions associated with conic domain, Comput.Math. Appl. 62, 367�375.
3. Khalida Inayat Noor, Sarfraz Nawaz Malik, Muhammad Arif and Mohsan Raza
(2011). On Bounded Boundary and Bounded Radius Rotation Related with Janowski
Function, World Appl. Sci. J. 12 (6), 895-902.
4. Khalida Inayat Noor and Sarfraz NawazMalik (2011). On coe¢ cient inequalities
of functions associated with conic domains, Comput.Math. Appl. 62, 2209�2217.
Although, writing up this thesis was not an easy task, but the scholarly, perceptive
and insightful guidance of Prof. Dr. Khalida Inayat Noor made it possible for me. This
work is rich with new ideas and can motivate many researchers working in this �eld.
130
Chapter 9
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