Abstract
For $f\in \mathcal{S}$, the class of normalized functions, analytic and univalent in the unit disk $\mathbb{D}$ and given by $f(z)=z+\sum_{n=2}^{\infty} a_n z^n$ for $z\in \mathbb{D}$, we give an upper bound for the coefficient difference $|a_4|-|a_3|$ when $f\in \mathcal{S}$. This provides an improved bound in the case $n=3$ of Grispan's 1976 general bound $||a_{n+1}|-|a_n||\le 3.61\dots .$ Other coefficients bounds, and bounds for the second and third Hankel determinants when $f\in \mathcal{S}
Results & Lemmas (3)
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Theorem 1 · coeff
Theorem 1. Let and be given by (1) with. Then - - - (iii) - - Proof. (i) The classical inequality for f in S when, gives, which from (8)…
Theorem 1. Let $f \in \mathcal{S}$ and be given by (1) with $a_2 = 0$ . Then
- $(i) |a_3| \leq 1,$
- $(ii) |a_4| \le \frac{2}{3} = 0.666 \dots,$
- (iii) $|a_5| \le \sqrt{\frac{19}{15}} = 1.67666...,$
- $(iv) |H_2(2)| \leq 1,$
- $(v) |H_3(1)| \le \frac{21}{20} = 1.05.$
Proof.
(i) The classical inequality $|a_3 - a_2^2| \le 1$ for f in S when $a_2 = 0$ , gives $|a_3| \le 1$ , which from (8) gives
$$(10) |\omega_{13}| \le \frac{1}{2}.$$
(ii) Next choose $x_1 = 0$ and $x_3 = 1$ in (7), which gives
$$(11) |\omega_{33}| \le \frac{1}{3}.$$
Also, since $\omega_{11} = 0 \ (\Leftrightarrow a_2 = 0)$ , then from (8) and (11) we obtain
<span id="page-2-1"></span><span id="page-2-0"></span>
$$|a_4| = 2|\omega_{33}| \le \frac{2}{3} = 0.666\dots$$
(iii) Again since $\omega_{11} = 0$ , from (8) we obtain
$$|a_5| = |2\omega_{35} + 5\omega_{13}^2|.$$
From (6) with $x_1 = 0$ and $x_3 = 1$ we have $(\omega_{11} = 0)$
<span id="page-3-1"></span><span id="page-3-0"></span>
$$|\omega_{13}|^2 + 3|\omega_{33}|^2 + 5|\omega_{35}|^2 \le \frac{1}{3}$$
and from here
(13)
$$|\omega_{35}| \le \frac{1}{\sqrt{15}} \sqrt{1 - 3|\omega_{13}|^2}.$$
From (12) and (13) we have
$$|a_5| \le 2|\omega_{35}| + 5|\omega_{13}|^2 \le \frac{1}{\sqrt{15}}\sqrt{1 - 3|\omega_{13}|^2} + 5|\omega_{13}|^2 \le \frac{503}{300} = 1.67666\dots$$
- (iv) Since we are assuming $a_2 = 0$ , (i) shows that $|H_2(2)| \le 1$ is trivial.
- (v) When $\omega_{11} = 0$ , from the last relation in (8) we have $\omega_{33} = \omega_{15}$ , and from (9),
<span id="page-3-2"></span>(14)
$$|H_3(1)| = |2\omega_{13}^3 + 4\omega_{13}\omega_{35} - 4\omega_{33}^2| \le 2|\omega_{13}|^3 + 4 + \underbrace{|\omega_{13}\omega_{35} - \omega_{15}^2|}_{E_1}.$$
Now choose $x_1 = -\omega_{15}$ , and $x_3 = \omega_{13}$ , and since $\omega_{33} = \omega_{15}$ , from (6) we obtain
$$|\omega_{13}|^4 + 5E_1^2 \le |\omega_{15}|^2 + \frac{|\omega_{13}|^2}{3} \le \frac{1}{5} - \frac{3}{5}|\omega_{13}|^2 + \frac{1}{3}|\omega_{13}|^2,$$
(since by (6) $3|\omega_{13}|^2 + 5|\omega_{15}|^2 \le 1$ for $x_1 = 1$ , $x_3 = 0$ and $\omega_{11} = 0$ ), which implies $5E_1^2 \le \frac{1}{5} - \frac{4}{15}|\omega_{13}|^2 - |\omega_{13}|^4$ , i.e., $E_1 \le \frac{1}{5}$ .
Finally from (10) and (14), it follows that
$$|H_3(1)| \le 2 \cdot \frac{1}{8} + 4 \cdot \frac{1}{5} = \frac{21}{20} = 1.05.$$
This completes the proof of Theorem 1.
We next prove a similar result, this time assuming that $a_3 = 0$ .
Theorem 2 · coeff
Theorem 2. Let and be given by (1), with. Then - - (iii) Proof. (i) Since and, then, i.e.,. Also, since by, it follows that (15) <span…
Theorem 2. Let $f \in \mathcal{S}$ and be given by (1), with $a_3 = 0$ . Then
- $(i) |a_2| \leq 1,$
- $(ii) |a_4| \le \frac{\sqrt{37} + 13}{12} = 1.59023 \dots,$
(iii)
$$|a_5| \le \frac{1}{4} \sqrt{\frac{757}{15}} + \frac{85}{64} = 3.10412...,$$
$$(iv) |H_2(2)| \le \frac{13+\sqrt{37}}{12} = 1.59023...,$$
$$(v) |H_3(1)| \le \frac{24+\sqrt{645}}{30} = 1.64656\dots$$
Proof.
(i) Since $|a_3 - a_2^2| \le 1$ and $a_3 = 0$ , then $|a_2^2| \le 1$ , i.e., $|a_2| \le 1$ . Also, since by $(8), a_3 = 2\omega_{13} + 3\omega_{11}^2 = 0$ , it follows that
(15)
$$\omega_{13} = -\frac{3}{2}\omega_{11}^2 \quad \left( \Leftrightarrow \ \omega_{11}^2 = -\frac{2}{3}\omega_{13} \right).$$
<span id="page-4-3"></span><span id="page-4-0"></span>Because $|a_2| = |2\omega_{11}| \le 1$ , we have
(16)
$$|\omega_{11}| \le \frac{1}{2}$$
and $|\omega_{13}| \le \frac{3}{8}$ (by (15).
(ii) By using (8) and (15), we obtain
<span id="page-4-1"></span>
$$|a_4| = \left| 2\omega_{33} + 8\omega_{11} \left( -\frac{3}{2}\omega_{11}^2 \right) + \frac{10}{3}\omega_{11}^3 \right|$$
$$= \left| 2\omega_{33} - \frac{26}{3}\omega_{11}^3 \right|$$
$$\leq 2|\omega_{33}| + \frac{26}{3}|\omega_{11}|^3.$$
From (6), using $x_1 = 0$ and $x_3 = 1$ , we have
<span id="page-4-2"></span>
$$|\omega_{13}|^2 + 3|\omega_{33}|^2 \le \frac{1}{3},$$
which implies (with $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ , see (15))
$$|\omega_{33}| \le \sqrt{\frac{1}{9} - \frac{3}{4}|\omega_{11}|^4}.$$
Combining (17) and (18) we obtain
(19)
$$|a_4| \le 2\sqrt{\frac{1}{9} - \frac{3}{4}|\omega_{11}|^4} + \frac{26}{3}|\omega_{11}|^3 =: \varphi(|\omega_{11}|),$$
<span id="page-4-4"></span>where $\varphi(t) = 2\sqrt{\frac{1}{9} - \frac{3}{4}t^4} + \frac{26}{3}t^3$ , $0 \le t = |\omega_{11}| \le \frac{1}{2}$ (by (16)). Since $\varphi$ is increasing function on [0, 1/2],
$$\varphi(t) \le \varphi(1/2) = \frac{\sqrt{37} + 13}{12},$$
which, together with (19), gives the desired result.
(iii) From the last relation in (8), using (15) we have $\omega_{33} = \omega_{15} + \frac{11}{6}\omega_{11}^3$ , which with the expression for $a_5$ in (8), gives
<span id="page-4-5"></span>(20)
$$|a_{5}| = |2\omega_{35} + 8\omega_{11}\omega_{15} + 5\omega_{13}^{2} - 10\omega_{11}^{4}|$$
$$\leq 2\underbrace{|\omega_{35} + 4\omega_{11}\omega_{15}|}_{C_{7}^{}} + \underbrace{5|\omega_{13}|^{2} + 10|\omega_{11}|^{4}}_{C_{7}^{}}.$$
Once again, using (6) choosing $x_1 = 4\omega_{11}$ , $x_3 = 1$ and $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ , we have
$$(C_1^*)^2 = |4\omega_{11}\omega_{15} + \omega_{35}|^2 \le -\frac{5}{4}|\omega_{11}|^4 + \frac{16}{5}|\omega_{11}|^2 + \frac{1}{15} \le \frac{757}{64 \cdot 15},$$
since $|\omega_{11}| \leq \frac{1}{2}$ . Thus
$$C_1^* \le \frac{1}{8} \sqrt{\frac{757}{15}}.$$
Next, since $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ and $|\omega_{11}| \leq \frac{1}{2}$ , we have
$$C_2^* = 5 \cdot \frac{9}{4} \cdot |\omega_{11}|^4 + 10|\omega_{11}|^4 = \frac{85}{4}|\omega_{11}|^4 \le \frac{85}{4} \cdot \frac{1}{16} = \frac{85}{64}$$
since $|\omega_{11}| \leq \frac{1}{2}$ .
Finally from (20) we have
$$|a_5| \le \frac{1}{4} \sqrt{\frac{757}{15}} + \frac{85}{64} = 3.10412\dots$$
(iv) By using (9), (8) and (15), we have
(21)
$$H_2(2) = 4\omega_{11}\omega_{33} + 4\omega_{11}^2\omega_{13} - 4\omega_{13}^2 - \frac{7}{3}\omega_{11}^4$$
$$= 4\omega_{11}\omega_{33} - \frac{52}{3}\omega_{11}^4$$
and from here
<span id="page-5-0"></span>
$$(22) |H_2(2)| \le 4|\omega_{11}||\omega_{33}| + \frac{52}{3}|\omega_{11}|^4.$$
From (18) and (22) we have
$$|H_2(2)| \le 4|\omega_{11}|\sqrt{\frac{1}{9} - \frac{3}{4}|\omega_{11}|^4} + \frac{52}{3}|\omega_{11}|^4 =: \varphi_1(|\omega_{11}|, |\omega_{11}|)$$
where
$$\varphi_1(t) = 4t\sqrt{\frac{1}{9} - \frac{3}{4}t^4} + \frac{52}{3}t^4,$$
with $0 \le t = |\omega_{11}| \le \frac{1}{2}$ . Finally, it can be checked that $\varphi_1$ is an increasing function on the interval (0, 1/2), and so
$$|H_2(2)| \le \varphi_1(1/2) = \frac{13 + \sqrt{37}}{12} = 1.59023....$$
(v) By using the last relation from (8) with $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ , it follows that $\omega_{33} = \omega_{15} + \frac{11}{6}\omega_{11}^3$ , and so using (9), after some calculations we obtain
$$H_3(1) = -12\omega_{11}^2 \left(\omega_{11}\omega_{15} + \frac{2}{3}\omega_{35}\right) - 4\omega_{15}^2 - 30\omega_{11}^6,$$
<span id="page-5-1"></span>which gives
(23)
$$|H_3(1)| \leq \underbrace{12|\omega_{11}|^2 \left|\omega_{11}\omega_{15} + \frac{2}{3}\omega_{35}\right|}_{D_2} + \underbrace{4|\omega_{15}|^2 + 30|\omega_{11}|^6}_{D_2}.$$
Now choose $x_1 = \omega_{11}$ and $x_3 = \frac{2}{3}$ in (6), then (since $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ ),
$$\left|\omega_{11}\omega_{15} + \frac{2}{3}\omega_{35}\right| \le \sqrt{\frac{1}{5}\left(|\omega_{11}|^2 + \frac{4}{27}\right)},$$
and so
<span id="page-6-0"></span>(24)
$$D_{1} \leq 12|\omega_{11}|^{2} \sqrt{\frac{1}{5} \left(|\omega_{11}|^{2} + \frac{4}{27}\right)}$$
$$\leq 12 \cdot \frac{1}{4} \sqrt{\frac{1}{5} \left(\frac{1}{4} + \frac{4}{27}\right)} = \sqrt{\frac{43}{60}} = \frac{\sqrt{645}}{30} = 0.84656 \dots,$$
since $|\omega_{11}| \leq \frac{1}{2}$ .
Also, as in the proof of (iii), we have
$$|5|\omega_{15}|^2 \le 1 - |\omega_{11}|^2 - 3|\omega_{13}|^2 = 1 - |\omega_{11}|^2 - \frac{27}{4}|\omega_{11}|^4$$
where we have once again used $\omega_{13} = -\frac{3}{2}\omega_{11}^2$ . Now
$$D_2 \le \frac{4}{5} - \frac{4}{5}|\omega_{11}|^2 - \frac{27}{5}|\omega_{11}|^4 + 30|\omega_{11}|^6 =: \varphi_2(|\omega_{11}|^2),$$
where
<span id="page-6-1"></span>
$$\varphi_2(t) = \frac{1}{5} \left( 4 - 4t - 27t^2 + 150t^3 \right),\,$$
and $0 \le t = |\omega_{11}|^2 \le \frac{1}{4}$ . Since $\varphi_2$ attains its maximum at $t_0 = 0$ ,
(25)
$$D_2 \le \varphi_2(0) = \frac{4}{5}.$$
Finally, by using (23), (24) and (25) we obtain
$$|H_3(1)| \le D_1 + D_2 \le \frac{24 + \sqrt{645}}{30} = 1.64656...$$
Theorem 3 · coeff
Theorem 3. Let and be given by (1). Then
Theorem 3. Let $f \in \mathcal{S}$ and be given by (1). Then
$$|a_4| - |a_3| < 2.1033299...$$
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