Citation: Mohsan Raza, Wasim Ul Haq, Jin-Lin Liu, Saddaf Noreen. Regions of variability for a subclass of analytic functions[J]. AIMS Mathematics, 2020, 5(4): 3365-3377. doi: 10.3934/math.2020217
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Let A be the class of functions f analytic in the open unit disc E={z:|z|<1, z∈C} with the usual normalization f(0)=f′(0)−1=0 and S be the subclass of A consisting of functions which are univalent in E. Consider that A as a topological vector space endowed with the topology of uniform convergence over a compact subsets of E. Also let B denote the class of analytic functions w in E such that |w(z)|<1 and w(0)=0. A function f is said to be subordinate to a function g written as f≺g, if there exists a Schwarz function w∈B such that f(z)=g(w(z)). In particular if g is univalent in E, then f(0)=g(0) and f(E)⊂g(E).
A set D in the complex plane is said to be starlike with respect to a point w0, an interior point of D if the line segment with initial point w0 lies entirely in D. If a function f maps E onto a domain that is starlike with respect to w0, then we say that f is starlike with respect to w0. In the special case that f is starlike function with respect to origin. The class of univalent starlike functions with respect to origin is denoted by S∗. The class of starlike functions with respect to the origin have been studied extensively, for some details [5,6].
In 1933 Spacek [19] extended the idea of starlike functions by using the logarithmic spirals instead of line segment. Let α∈(−π2,π2). The curve γα:t→exp(teiα), t∈R and its rotation eiθγα(t), θ∈R are called α-spirals. A domain D⊂C is said to be α-spirallike with respect to the origin if the spiral with initial point 0 to every point in D lies in D. A function f∈A is spirallike if it maps E onto a domain which is spirallike with respect to 0. The class of spirallike functions is denoted by Sα. In otherwise
Sα={f∈A:Re(eiαzf′(z)f(z))>0, z∈E}. |
Kim and Sugawa [10] introduced the notion of α-argument. Consider that θ=argαw with w∈eiθγα(R). By using the α-argument, it is clear that f∈Sα if and only if
∂∂θ(argαf(reiθ))>0 (θ∈R,0<r<1). |
For some details about the spirallike functions [1,5,6]. A function f with f(0)=f′(0)−1=0 is said to be Robertson functions if
Re{eiα(1+zf′′(z)f′(z))}>0, z∈E. |
The class of Robertson functions is denoted by Cα and defined by Robertson [17]. It is clear that C0=C, usual class of convex functions. In the view of above discussions about the spirallike functions and Robertson functions, we have the following relation. Let f∈A. Then f∈Cα if and only if zf′∈Sα. By using the concept of Janowski [8], Sen et al. [18] studied the class Cα[A,B]. Let A∈C, B∈[−1,0) and α∈(−π2,π2). Then Cα[A,B] denotes the class of analytic functions f in the open unit disc with f(0)=0= f′(0)−1 such that
eiα(1+zf′′(z)f′(z))=cosαp(z)+isinα, |
with
p(z)=1+Aw(z)1+Bw(z). |
The single-valued branch of logarithms for f′(z) when f∈Cα[A,B] is denoted by logf′(z) with logf′(0)=0. Yanagihara [21,22] determined the region of variability for the class of convex functions. Ponnusamy et al. [13] found the region of variability for some subclasses of univalent functions. For some work on region of variability, [7,11,12,13,14,15,16] and references therein.
Using the Herglotz representation for Janowski functions, it can be seen that for f∈Cα[A,B] there exists a unique positive unit measure μ in (−π,π] such that
1+zf′′(z)f′(z)=e−iα[cosαπ∫−π1+Aze−it1+Bze−itdμ(t)+isinα]. | (1.1) |
This shows that
logf′(z)=A−BBe−iαcosαπ∫−πBe−it1+Bze−itdμ(t). | (1.2) |
It follows from (1.2) that for each fixed z0∈E, the region of variability is the set Vλ[z0,A,B] given as
{A−BBe−iαcosαlog(1+Bz):|z|≤|z0|}. |
Let
pf(z)=eiα(1+zf′′(z)f′(z)). |
Then there exists a Schwarz function w∈B, such that
w(z)=pf(z)−eiαAcosα+iBsinα−Bpf(z). | (1.3) |
Let f∈Cα[A,B]. Then by applying Schwarz lemma, that is |w′p(0)|≤1 [4], we get
|f′′(0)|=(A−B)cosα|ω′f(0)|≤(A−B)cosα, |
for some λ∈¯E, Now for λ∈¯E={z∈C:|z|≤1} and z0∈E, we introduce
Cα[λ,A,B]={f∈Cα[A,B]:f′′(0)=λ(A−B)e−iαcosα} |
and
Vλ(z0,A,B)={logf′(z0):f∈Cα[λ,A,B]}. |
The aim of this article is to investigate the region of variability Vλ(z0,A,B) for the class f∈Cα[λ,A,B].
We start our investigations by studying certain general properties of the set Vλ(z0,A,B) such as compactness and convexity.
Proposition 2.1. (i) Vλ(z0,A,B) is a compact subset of C.
(ii) Vλ(z0,A,B) is a convex subset of C.
(iii) If |λ|=1 or z0=0, then Vλ(z0,A,B)={A−BBe−iαcosαlog(1+Bλz0)} and if |λ|<1 and z0≠0, then the set Vλ(z0,A,B) has e−iαcosαlog(1+Bλz0) an interior point.
Proof. (ⅰ) Since Cα[λ,A,B] is a compact subset of C, therefore Vλ(z0,A,B) is also compact.
(ⅱ) Let f1,f2∈Cα[λ,A,B]. Then for 0≤t≤1, the function
f(z)=z∫0(f1(ς))1−t(f2(ς))tdς |
is also in Cα[λ,A,B], therefore Vλ(z0,A,B) is convex because logf′(z)=(1−t)logf′1(z)+tlogf′2(z), t∈[0,1].
(ⅲ)Since |λ|=|w′f(0)|=1, then from Schwarz lemma, we obtain wf(z)=λz, which yields p(z)=1+λAz1+λBz. This implies that
logf′(z)=A−BBe−iαcosαlog(1+Bλz0). |
Therefore
Vλ(z0,A,B)={A−BBe−iαcosαlog(1+Bλz0)}. |
This also trivially holds true when z0=0. For λ∈E and α∈¯E, set
δ(z,λ)=z+λ1+¯λz, |
Fa,λ(z)=z∫0(expς2∫0e−iαcosα(A−B)δ(aς1,λ)1+Bς1δ(aς1,λ))dς1)dς2, z∈E. | (2.1) |
Then Fa,λ(z) is in Cα[λ,A,B] and wf(z)=zδ(az,λ). For fixed λ∈E and z0∈E∖{0} the function
E∋a↦logF′a,λ(z)=z0∫0e−iαcosα(A−B)(aς+λ)1+(a¯λ+Bλ)ς+aBς2dς |
is a non-constant analytic function of a∈E, and therefore is an open mapping. Hence logF′0,λ(z)={A−BBe−iαcosαlog(1+Bλz0)} is an interior point of {logF′a,λ(z):a∈E}⊂Vλ(z0,A,B).
Keeping in view the above proposition, it is sufficient to find Vλ(z0,A,B) for 0≤λ<1 and z0∈E∖{0}.
In this section, we state and prove some results which are needed in the proof of our main theorem.
In the following proposition, we prove that for f∈Cα[λ,A,B], the ratio f′′(z)/f′(z) is contained in a closed disc with center q(z,λ) and radius r(z,λ).
Proposition 3.1. For Cα[λ,A,B], we have
|f′′(z)f′(z)−q(z,λ)|≤r(z,λ), | (3.1) |
where
q(z,λ)=D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1−|z|2|τ(z,λ)|2,r(z,λ)=|z||τ(z,λ)||D(z,λ)+E(z,λ)|1−|z|2|τ(z,λ)|2. | (3.2) |
Proof. Since f∈Cα[λ,A,B]. Then by using Schwarz lemma for wp∈B with w′p(0)=λ such that
|wf(z)z−λ1−¯λwf(z)z|≤|z|. | (3.3) |
Now from (1.3) this can be written equivalently as
|f′′(z)f′(z)−D(z,λ)f′′(z)f′(z)+E(z,λ)|≤|z||τ(z,λ)|, | (3.4) |
where
D(z,λ)=λe−iα(A−B)cosα1+Bλz, E(z,λ)=(B−A)e−iαcosα_λ+Bz, τ(z,λ)=−_λ−Bz1+Bλz. | (3.5) |
This is equivalent to
|f′′(z)f′(z)−D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1−|z|2|τ(z,λ)|2|≤|z||τ(z,λ)||A(z,λ)+B(z,λ)|1−|z|2|τ(z,λ)|2. | (3.6) |
Now after simple calculations, we have
1−|z|2|τ(z,λ)|2=1−B2|z|4+2B(1−|z|2)Reλz+|λ|2|z|2(B2−1)|1+Bλz|2. |
Also
D(z,λ)+E(z,λ)=e−iαcosα(A−B)(|λ|2−1)(1+Bλz)(_λ+Bz) |
and
D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)=e−iα(A−B)cosα{λ(1−|z|2)+B_z(|λ|2−|z|2)}|1+Bλz|2. |
By setting
q(z,λ)=D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1−|z|2|τ(z,λ)|2,r(z,λ)=|z||τ(z,λ)||D(z,λ)+E(z,λ)|1−|z|2|τ(z,λ)|2. |
The relation (3.1) occurs from (3.6) and the above relations. Equality is attained in (3.1) when f=Feiθ,λ(z), for some z∈E. Conversely if equality occurs in (3.1) for some z∈ E∖{0}, then equality must hold in (3.3). Thus by Schwarz lemma there exists θ∈R such that wf(z)=zδ(eiθz,λ) for all z∈E. This implies f=Feiθ,λ.
Geometrically the above proposition means that the functional logf′ lies in the closed disk centred at q(z,λ) with radius r(z,λ).
For λ=0, we have the following special result which gives us bounds on pre-Schwarzian norm of locally univalent functions.
Corollary 3.2. Let f∈Cα[0,A,B]. Then
|f′′(z)f′(z)−−e−iα(A−B)cosα B_z|z|21−B2|z|4|≤|z||A−B|cosα1−B2|z|4. |
Therefore
(1−|B||z|2)|f′′(z)f′(z)|≤|A−B||z|cosα. |
Since |B|≤1, so
(1−|z|2)|f′′(z)f′(z)|≤|A−B||z|cosα. |
The pre-Schwarzian norm for locally univalent functions is defined as
‖f‖=supz∈E(1−|z|2)|f′′(z)f′(z)|. |
It is well-known that ‖f‖≤6, if f is univalent. Becker and Pommerenke [2] proved that if ‖f‖≤1, then f is univalent in E and this bound is sharp. Yamashita [20] proved that if f is convex, then ‖f‖≤1. The norm estimates for some subclasses of univalent functions are studied by many authors. For some details [3,9]. From Corollary 3.2, it is evident that for f′′(0) and A=1,B=−1, we have ‖f‖≤2cosα for Robertson functions. This result was proved by Ponnusamy et al. [15] also for α=0, we have ‖f‖≤2.
In the following result, we prove that the set Vλ(z0,A,B) is contained in a closed disc with centre Q(λ,r) and radius R(λ,r).
Corollary 3.3. Consider the curve γ:z(t), 0≤t≤1 in E with z(0)=0 and z(1)=z0, then
Vλ(z0,A,B)⊂_E(Q(λ,r),R(λ,r))={ω∈C:|ω−Q(λ,r)|≤R(λ,r)}, |
with
Q(λ,r)=1∫0q(z(t),λ)z′(t)dt,R(λ,r)=1∫0r(z(t),λ)z′(t)dt, |
where q(z,λ) and r(z,λ) are given in Proposition 3.1.
Proof. Suppose that f∈Cα[λ,A,B], then from proposition 3.1, we get
|logf′(z0)−Q(λ,r)|=|1∫0{f′′(z)f′(z)−q(z(t),λ)}z′(t)dt|≤1∫0|f′′(z)f′(z)−q(z(t),λ)||z′(t)|dt. |
Now using proposition 3.1, we get
|logf′(z0)−Q(λ,r)|≤1∫0r(z(t),λ)|z′(t)|dt=R(λ,r). |
This shows logf′(z0)∈ ¯D(Q(λ,r),R(λ,r)). Hence the required result.
We need the following lemma which ensures the existence of normalized starlike function which is useful in the proof of next result.
Lemma 3.4. For θ∈R and |λ|<1, the function
G(z)=z∫0eiθζ2(1+(¯λeiθ+Bλ)ζ+Beiθζ2)2dζ, z∈E, |
has zeros of order 2 at the origin and no zero elsewhere in E. Moreover, there exists a starlike normalized univalent function G0 in E such that G=12eiθG20.
The above lemma is due to Ponnusamy et al. [7]. In the below proposition we show that logF′eiθ,λ(z0) lies on the boundary of the set Vλ(z0,A,B).
Proposition 3.5. Let z0∈E∖{0}. Then for θ∈(−π,π], we have logF′eiθ,λ(z0)∈∂Vλ(z0,A,B). Further if logf′(z0)=logF′eiθ,λ(z0) for f∈Cα[λ,A,B], then f=Feiθ,λ.
Proof. Using 2.1, we have
Fa,λ(z)=z∫0(expξ2∫0e−iαcos(A−B)δ(aξ1,λ)1+Bξ1δ(aξ1,λ)dξ1)dξ2. |
Therefore
F′′a,λ(z)F′a,λ(z)=e−iαcos(A−B)δ(az,λ)1+Bzδ(az,λ)=e−iα(A−B)cosα (az+λ)1+(_λa+Bλ)z+Baz2. |
From (3.5), it follows that
F′′a,λ(z)F′a,λ(z)−D(z,λ)=e−iα(A−B)cosα (1−|λ|2)az{1+(_λa+Bλ)z+Baz2}(1+Bzλ)F′′a,λ(z)F′a,λ(z)+E(z,λ)=e−iα(A−B)cosα (|λ|2−1){1+(_λa+Bλ)z+Baz2}(_λ+Bz). |
Therefore
F′′a,λ(z)F′a,λ(z)−q(z,λ)=F′′a,λ(z)F′a,λ(z)−D(z,λ)+|z|2|τ(z,λ)|2E(z,λ)1−|z|2|τ(z,λ)|2=11−|z|2|τ(z,λ)|2{F′′a,λ(z)F′a,λ(z)−D(z,λ)−|z|2|τ(z,λ)|2(F′′a,λ(z)F′a,λ(z)+E(z,λ))}=e−iα(A−B)cosα(1−|λ|2)¯(1+(¯λeiθ+Bλ)z+Beiθz2){1−B2|z|4+2B(1−|z|2)Reλz+|λ|2|z|2(B2−1)}{1+(_λa+Bλ)z+Baz2}. |
Putting a=eiθ, we get
F′′eiθ,λ(z)F′eiθ,λ(z)−q(z,λ)=r(z,λ)eiθe−iαz|z||1+(_λeiθ+Bλ)z+Beiθz2|2(1+(_λeiθ+Bλ)z+Beiθz2)2. |
By using Lemma 3.4, we obtain
F′′eiθ,λ(z)F′eiθ,λ(z)−q(z,λ)=r(z,λ)e−iαG′(z)|G′(z)|. | (3.7) |
Using the argument of Lemma 3.4 that G=2−1eiθG20, where G0 is starlike in E with G0(0)=G′0(0)−1=0, for any z0∈E∖{0} the linear segment joining 0 and G0(z0) lies entirely in G0(E). Let γ0 be the curve defined by
γ0:z(t)=G−10(tG0(z0)), t∈[0,1]. |
Since G(z(t))=2−1eiθ(G0(z(t)))2=2−1eiθ(tG0(z0))2=t2G(z0). Differentiation w.r.t t gives us
G′(z(t))z′(t)=2tG(z0), t∈[0,1]. | (3.8) |
Therefore
{F′′eiθ,λ(z)F′eiθ,λ(z)−q(z(t),λ)}z′(t)=r(z(t),λ)e−iαG(z0)|G(z0)||z′(t)|. |
This relation together with (3.7), we get
logF′eiθ,λ(z)−Q(γ0,λ)=1∫0(F′′eiθ,λ(z)F′eiθ,λ(z)−q(z,λ))z′(t)dt=1∫0r(z(t),λ)e−iαG′(z(t))z′(t)|G′(z(t))z′(t)||z′(t)|dt=e−iαG(z0)|G(z0)|1∫0r(z(t),λ)|z′(t)|dt=e−iαG(z0)|G(z0)|R(λ,γ0). | (3.9) |
This shows that logF′eiθ,λ(z)∈∂E(Q(γ0,λ),R(γ0,r)), where Q(λ,γ0) and R(λ,γ0) are defined as in Corollary 3.3. Also we have logF′eiθ,λ(z0)∈Vλ(z0,A,B), therefore logF′eiθ,λ(z0)∈∂Vλ(z0,A,B).
Now we have to prove logf′(z0)=logF′(z0) for some f∈Cα[λ,A,B], we have
h(t)=e−iα|G(zo)|G(zo){f′′(z(t))f′(z(t))−q(z(t),λ)}z′(t) | (3.10) |
k(t)=eiα|G(zo)|G(zo){F′′(z(t))F′(z(t))−q(z(t),λ)}z′(t), |
where γ0:z(t), 0≤t≤1. Then the function h is continuous and
|h(t)|=|f′′(z(t))f′(z(t))−q(z(t),λ)||z′(t)|. |
Using Proposition 3.1, we have
|h(t)|≤r(z(t),λ)|z′(t)|. |
Now using Proposition 3.1, we get |h(t)|≤r(z(t),λ)|z′(t)|. Further from (3.9), we have From (3.7) and (3.8), this implies that f′′(z)f′(z)=F′′eiθ,λ(z)F′eiθ,λ(z) on γ0. The identity theorem for analytic functions yields us f=Feiθ,λ, z∈E.
In our main result, we give precise description of regions of variability for the class Cα[λ,A,B] and show that the boundary ∂Vλ(z0,A,B) is a Jordan curve.
Theorem 3.6. Let λ∈E and z0∈E∖{0}. Then boundary ∂Vλ(z0,A,B) is the Jordan curve given by
(−π,π]∋θ↦logF′eiθ,λ(z0)=z0∫0e−iαcosα(A−B)δ(aς,λ)1+Bςδ(aς,λ))dς. |
If logf′(z0)=logF′eiθ,λ(z0) for some f∈Cα[λ,A,B] and θ∈(−π,π], then f(z)=Feiθ,λ(z).
Proof. First we have to show that the curve
(−π,π]∋θ↦logF′eiθ,λ(z0) |
is simple. Let us assume that
logF′eiθ1,λ(z0)=logF′eiθ2,λ(z0) |
for some θ1,θ2∈(−π,π] with θ1≠θ2. Then the use of Proposition 3.5 yield us that F′eiθ1,λ(z0)=F′eiθ2,λ(z0), which further gives the following relation
τ(wFeiθ1,λ(z)z,λ)=τ(wFeiθ2,λ(z)z,λ). |
This implies that
B(zeiθ1+λ)+¯λ(1+¯λeiθ1z)1+¯λeiθ1z+λB(zeiθ1+λ)=B(zeiθ2+λ)+¯λ(1+¯λeiθ2z)1+¯λeiθ2z+λB(zeiθ2+λ). |
After some simplification, we obtain zeiθ1=zeiθ2, which leads us to a contradiction. Hence the curve is simple. Since Vλ(z0,A,B) is compact convex subset of C and has non-empty interior, therefore the boundary ∂Vλ(z0,A,B) is a simple closed curve. From Proposition 3.5 the curve ∂Vλ(z0,A,B) contains the curve (−π,π]∋θ↦logFeiθ,λ(z0). Since a simple closed curve cannot contain any simple closed curve other than itself. Thus ∂Vλ(z0,A,B) is given by (−π,π]∋θ↦logF′eiθ,λ(z0).
The following figures show us the geometric view of our main theorem with various choices of involved parameters.
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Authors are thankful to the editor and anonymous referees for their valuable comments and suggestions.
The authors declare no conflicts of interest.
[1] | O. P. Ahuja, H. Silverman, A survey on spiral-like and related function classes, Math. Chronicle, 20 (1991), 39-66. |
[2] | J. Becker, Ch. Pommerenke, Schlichtheitskriterien und Jordangebiete, J. Reine Angew. Math., 354 (1984), 74-94. |
[3] |
J. H. Choi, Y. C. Kim, S. Ponnusamy, et al. Norm estimates for the Alexander transforms of convex functions of order alpha, J. Math. Anal. Appl., 303 (2005), 661-668. doi: 10.1016/j.jmaa.2004.08.066
![]() |
[4] | S. Dineen, The Schwarz lemma, Oxford Math. Monogr., Clarendon Press Oxford, 1989. |
[5] | P. L. Duren, Univalent functions, Grundlehren der Mathematischen Wissenschaften, New York, Berlin, Heidelberg, Tokyo, Springer-Verlag, 1983. |
[6] | A. W. Goodman, Univalent Functions, Vols. I and II, Mariner Publishing Co. Tampa, Florida, 1983. |
[7] |
W. U. Haq, Variability regions for Janowski convex functions, Complex Var. Elliptic Equ., 59 (2014), 355-361. doi: 10.1080/17476933.2012.725164
![]() |
[8] |
J. Janowski, Some extremal problems for certain families of analytic functions I, Ann. Polon. Math., 28 (1973), 297-326. doi: 10.4064/ap-28-3-297-326
![]() |
[9] |
Y. C. Kim, S. Ponnusamy, T. Sugawa, Mapping properties of nonlinear integral operators and pre-Schwarzian derivatives, J. Math. Anal. Appl., 299 (2004), 433-447. doi: 10.1016/j.jmaa.2004.03.081
![]() |
[10] |
Y. C. Kim, T. Sugawa, Correspondence between spirallike functions and starlike functions, Math. Nach., 285 (2012), 322-331. doi: 10.1002/mana.201010020
![]() |
[11] |
S. Ponnusamy, A. Vasudevarao, Regions of variability for functions with positive real part, Ann. Polon. Math., 99 (2010), 225-245. doi: 10.4064/ap99-3-2
![]() |
[12] | S. Ponnusamy, A. Vasudevarao, Region of variability of two subclasses of univalent functions, J. Math. Anal. Appl., 332 (2007) 1323-1334. |
[13] |
S. Ponnusamy, A. Vasudevarao, M. Vuorinen, Region of variability for certain classes of univalent functions satisfying differential inequalities, Complex var. Elliptic Equ., 54 (2009), 899-922. doi: 10.1080/17476930802657616
![]() |
[14] |
S. Ponnusamy, A. Vasudevarao, H. Yanagihara, Region of variability for close-to-convex functions, Complex Var. Elliptic Equ., 53 (2008), 709-716. doi: 10.1080/17476930801996346
![]() |
[15] | S. Ponnusamy, A. Vasudevarao, H. Yanagihara, Region of variability of univalent functions f (z) for which zf'(z) is spirallike, Houston J. Math., 34 (2008), 1037-1048. |
[16] |
M. Raza, W. U. Haq, S. Noreen, Regions of Variability for Janowski Functions, Miskloc Math. Notes, 16 (2015), 1117-1127. doi: 10.18514/MMN.2015.1344
![]() |
[17] | M. S. Robertson, Univalent functions f (z) for which zf'(z) is spirallike, Mich. Math. J., 16 (1969), 97-101. |
[18] | A. Y. Sen, Y. Polatoglu, M. Aydogan, Distortion theorem and the radius of convexity for Janowski-Robertson functions, Stud. Univ. Babeş-Bolyai Math., 57 (2012), 291-294. |
[19] |
L. Spacek, Contribution a la theorie des fonctions univalentes (in Czech), Časopis Pest. Mat., 62 (1933), 12-19. doi: 10.21136/CPMF.1933.121951
![]() |
[20] |
S. Yamashita, Norm estimates for function starlike or convex of order alpha, Hokkaido Math. J., 28 (1999), 217-230. doi: 10.14492/hokmj/1351001086
![]() |
[21] |
H. Yanagihara, Regions of variability for convex function, Math. Nach., 279 (2006), 1723-1730. doi: 10.1002/mana.200310449
![]() |
[22] |
H. Yanagihara, Regions of variability for functions of bounded derivatives, Kodai Math. J., 28 (2005), 452-462. doi: 10.2996/kmj/1123767023
![]() |
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