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Abstract

It is well-known that the condition ${\operatorname{Re}} \left[1+\frac{zf''(z)}{f'(z)}\right]>0$, $z\in{\mathbb D}$, implies that $f$ is starlike function (i.e. convexity implies starlikeness). If the previous condition is not satisfied for every $z\in {\mathbb D}$, then it is possible to get new criteria for starlikeness by using $\left|\arg\left[α+\frac{zf''(z)}{f'(z)}\right]\right|$, $z\in{\mathbb D}$, where $α>1.$

Results & Lemmas (9)

Each result is auto-extracted from the paper via OCR - the math is shown verbatim and may carry occasional transcription artifacts. Click to expand the full statement.

Theorem 1 Theorem 1. Let,, and let (1) Then.
Theorem 1. Let $f \in \mathcal{A}$ , $\alpha > 1$ , and let (1) $$\left| \arg \left[ \alpha + \frac{zf''(z)}{f'(z)} \right] \right| < \arctan \frac{\sqrt{3}}{\alpha - 1} \quad (z \in \mathbb{D}).$$ Then $f \in \mathcal{S}^*$ .
Corollary 1 · radius Corollary 1. Let and Then. Further, it is easy to verify that the disc with center and radius is contained in the angle, and so by using…
Corollary 1. Let $f \in A$ and $$\left| \arg \left[ \frac{zf''(z)}{f'(z)} + 1 \right] \right| < \frac{\pi}{2} \quad (z \in \mathbb{D})$$ Then $f \in \mathcal{S}^*$ . Further, it is easy to verify that the disc with center $\alpha$ and radius $\frac{\alpha\sqrt{3}}{\sqrt{3+(\alpha-1)^2}}$ is contained in the angle $|\arg z| < \arctan\frac{\sqrt{3}}{\alpha-1}$ , and so by using the result of Theorem 1, we have that $$\left| \frac{zf''(z)}{f'(z)} \right| = \left| \left( \frac{zf''(z)}{f'(z)} + \alpha \right) - \alpha \right| < \frac{\alpha\sqrt{3}}{\sqrt{3 + (\alpha - 1)^2}} \quad (z \in \mathbb{D})$$ implies $f \in \mathcal{S}^*$ . Since the function $\varphi(\alpha) =: \frac{\alpha\sqrt{3}}{\sqrt{3+(\alpha-1)^2}}$ , $\alpha \geq 1$ , attains its maximal value 2 for $\alpha = 4$ , we get
Corollary 2 Corollary 2. Let and Then. In a similar way as in Theorem 1, we can consider starlikeness problem in connection with the class defined by…
Corollary 2. Let $f \in A$ and $$\left| \frac{zf''(z)}{f'(z)} \right| < 2 \quad (z \in \mathbb{D})$$ Then $f \in \mathcal{S}^*$ . In a similar way as in Theorem 1, we can consider starlikeness problem in connection with the class defined by $$\mathcal{G} = \left[ f \in \mathcal{A} : \operatorname{Re} \left[ 1 + \frac{zf''(z)}{f'(z)} \right] < \frac{3}{2}, z \in \mathbb{D} \right].$$ Ozaki in [4] proved that if $f \in \mathcal{G}$ , then f is univalent in $\mathbb{D}$ . Later, Umezava in [6] showed the functions from $\mathcal{G}$ are convex in one direction. Also, it is shown in the papers [2] and [5] that $\mathcal{G}$ is subclass of $\mathcal{S}^*$ . If Re $\left[1 + \frac{zf''(z)}{f'(z)}\right] < \frac{3}{2}$ is not satisfied for every $z \in \mathbb{D}$ , then we can pose a question if for some $\beta < 1$ , such that (4) $$\operatorname{Re}\left[\beta + \frac{zf''(z)}{f'(z)}\right] < \frac{3}{2} \quad (z \in \mathbb{D}),$$ is it possible obtain sufficient condition for starlikeness, in a similar way as in Theorem 1. The condition (4) is equivalent to $$\operatorname{Re}\left[\frac{3-2\beta}{2} - \frac{zf''(z)}{f'(z)}\right] > 0 \quad (z \in \mathbb{D}),$$ and we can use similar technique. This lead so
Theorem 2 Theorem 2. Let,, and let Then.
Theorem 2. Let $f \in \mathcal{A}$ , $\beta < 1$ , and let $$\left| \arg \left[ \frac{3 - 2\beta}{2} - \frac{zf''(z)}{f'(z)} \right] \right| < \arctan \frac{2\sqrt{3}}{5 - 2\beta} \quad (z \in \mathbb{D}).$$ Then $f \in \mathcal{S}^*$ .
Corollary 3 · radius Corollary 3. Let and Then. As in the case of Theorem 1, we can show that the disc with center and radius is containing in the angle arctg.…
Corollary 3. Let $f \in A$ and $$\left| \arg \left[ \frac{1}{2} - \frac{zf''(z)}{f'(z)} \right] \right| < \operatorname{arctg} \frac{2}{\sqrt{3}} \approx 49.1^{\circ} \quad (z \in \mathbb{D}).$$ Then $f \in \mathcal{S}^*$ . As in the case of Theorem 1, we can show that the disc with center $\frac{3-2\beta}{2}$ and radius $\frac{(3-2\beta)\sqrt{3}}{\sqrt{12+(5-2\beta)^2}}$ is containing in the angle $|\arg z| \le$ arctg $\frac{2\sqrt{3}}{5-2\beta}$ . So, if $$\left| \frac{zf''(z)}{f'(z)} \right| = \left| \left( \frac{3 - 2\beta}{2} - \frac{zf''(z)}{f'(z)} \right) - \frac{3 - 2\beta}{2} \right| < \frac{(3 - 2\beta)\sqrt{3}}{\sqrt{12 + (5 - 2\beta)^2}},$$ for all $z \in \mathbb{D}$ , then Theorem 2 brings that $f \in \mathcal{S}^*$ . Since the function $\psi(\beta) =: \frac{(3-2\beta)\sqrt{3}}{\sqrt{12+(5-2\beta)^2}}$ is decreasing on the interval $(-\infty, 1]$ , and $\psi(\beta) \to \sqrt{3}$ , when $\beta \to -\infty$ , we get
Corollary 4 Corollary 4. Let and Then. For a starlike function f it is not necessary that,. For example, for Koebe function we have and this also holds…
Corollary 4. Let $f \in A$ and $$\left| \frac{zf''(z)}{f'(z)} \right| < \sqrt{3} \quad (z \in \mathbb{D}).$$ Then $f \in \mathcal{S}^*$ . For a starlike function f it is not necessary that $Re\frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ . For example, for Koebe function $k(z) = \frac{z}{(1-z)^2}$ we have $$\operatorname{Re} \frac{k(z)}{z} \bigg|_{z=(1+i)/\sqrt{2}} = -(\sqrt{2}+1) < 0,$$ and this also holds for points in $\mathbb{D}$ close enought to $\frac{1+i}{\sqrt{2}}$ . In the next theorem we give a condition which provides $\operatorname{Re} \frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ .
Theorem 3 Theorem 3. Let, and let Then Re,.
Theorem 3. Let $f \in \mathcal{A}, \gamma \geq 0$ , and let $$\left| \arg \left[ \frac{zf'(z)}{f(z)} + \gamma \right] \right| < \arctan \frac{1}{1+\gamma} \quad (z \in \mathbb{D}).$$ Then Re $\frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ .
Corollary 5 · radius Corollary 5. Let and Then Re,. In Theorem 3 the function f from need not be starlike as the next example shows. Example 2. Let is defined…
Corollary 5. Let $f \in A$ and $$\left|\arg \frac{zf'(z)}{f(z)}\right| < \frac{\pi}{4} \quad (z \in \mathbb{D}).$$ Then Re $\frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ . In Theorem 3 the function f from $\mathcal{A}$ need not be starlike as the next example shows. Example 2. Let $f \in \mathcal{A}$ is defined by (7) $$\frac{zf'(z)}{f(z)} = \sqrt{3} \left(\frac{1+z}{1-z}\right)^{\frac{1}{3}} + 1 - \sqrt{3},$$ where we use the principal value for square root. For real z close to -1 we have that $\operatorname{Re}\left[\frac{zf'(z)}{f(z)}\right] < 0$ , which means that f is not starlike. But from (7) we have $$\frac{zf'(z)}{f(z)} + (\sqrt{3} - 1) = \sqrt{3} \left(\frac{1+z}{1-z}\right)^{\frac{1}{3}},$$ and from here $$\left| \arg \left[ \frac{zf'(z)}{f(z)} + (\sqrt{3} - 1) \right] \right| \le \frac{1}{3} \left| \arg \left( \frac{1+z}{1-z} \right) \right|$$ $$< \frac{\pi}{6} = \operatorname{arctg} \frac{1}{(\sqrt{3} - 1) + 1},$$ which by Theorem 3 (with $\gamma = \sqrt{3} - 1$ ) implies that $\operatorname{Re} \frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ . It is possible to show that the disc with center $1 + \gamma$ and radius $\frac{1+\gamma}{\sqrt{1+(1+\gamma)^2}}$ lies in the angle $|\arg z| \leq \arctan\frac{1}{1+\gamma}$ , and so, by using the result of Theorem 3 we have that $$\left| \frac{zf'(z)}{f(z)} - 1 \right| = \left| \left( \frac{zf'(z)}{f(z)} + \gamma \right) - (1+\gamma) \right| < \frac{1+\gamma}{\sqrt{1+(1+\gamma)^2}} \quad (z \in \mathbb{D})$$ implies Re $\frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ . When $\gamma \to +\infty$ we receive
Corollary 6 Corollary 6. Let and Then Re,.
Corollary 6. Let $f \in A$ and $$\left| \frac{zf'(z)}{f(z)} - 1 \right| < 1 \quad (z \in \mathbb{D}).$$ Then Re $\frac{f(z)}{z} > 0$ , $z \in \mathbb{D}$ .

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