In complex analysis, a branch of mathematics, Bloch's theorem describes the behaviour of holomorphic functions defined on the unit disk. It gives a lower bound on the size of a disk in which an inverse to a holomorphic function exists. It is named after André Bloch.
Statement
Let f be a holomorphic function in the unit disk |z| ≤ 1 for which
-
|
f
′
(
0
)
|
=
1
{\displaystyle |f'(0)|=1}
Bloch's theorem states that there is a disk S ⊂ D on which f is biholomorphic and f(S) contains a disk with radius 1/72.
Landau's theorem
If f is a holomorphic function in the unit disk with the property |f′(0)| = 1, then let Lf be the radius of the largest disk contained in the image of f.
Landau's theorem states that there is a constant L defined as the infimum of Lf over all such functions f, and that L is greater than Bloch's constant L ≥ B.
This theorem is named after Edmund Landau.
Valiron's theorem
Bloch's theorem was inspired by the following theorem of Georges Valiron:
Theorem. If f is a non-constant entire function then there exist disks D of arbitrarily large radius and analytic functions φ in D such that f(φ(z)) = z for z in D.
Bloch's theorem corresponds to Valiron's theorem via the Bloch's principle.
Proof
Landau's theorem
We first prove the case when f(0) = 0, f′(0) = 1, and |f′(z)| ≤ 2 in the unit disk.
By Cauchy's integral formula, we have a bound
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f
″
(
z
)
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=
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1
2
π
i
∮
γ
f
′
(
w
)
(
w
−
z
)
2
d
w
|
≤
1
2
π
⋅
2
π
r
sup
w
=
γ
(
t
)
|
f
′
(
w
)
|
|
w
−
z
|
2
≤
2
r
,
{\displaystyle |f''(z)|=\left|{\frac {1}{2\pi i}}\oint _{\gamma }{\frac {f'(w)}{(w-z)^{2}}}\,\mathrm {d} w\right|\leq {\frac {1}{2\pi }}\cdot 2\pi r\sup _{w=\gamma (t)}{\frac {|f'(w)|}{|w-z|^{2}}}\leq {\frac {2}{r}},}
-
|
f
″
(
z
)
|
=
|
1
2
π
i
∮
γ
f
′
(
w
)
(
w
−
z
)
2
d
w
|
≤
1
2
π
⋅
2
π
r
sup
w
=
γ
(
t
)
|
f
′
(
w
)
|
|
w
−
z
|
2
≤
2
r
,
{\displaystyle |f''(z)|=\left|{\frac {1}{2\pi i}}\oint _{\gamma }{\frac {f'(w)}{(w-z)^{2}}}\,\mathrm {d} w\right|\leq {\frac {1}{2\pi }}\cdot 2\pi r\sup _{w=\gamma (t)}{\frac {|f'(w)|}{|w-z|^{2}}}\leq {\frac {2}{r}},}
where γ is the counterclockwise circle of radius r around z, and 0 < r < 1 − |z|.
By Taylor's theorem, for each z in the unit disk, there exists 0 ≤ t ≤ 1 such that f(z) = z + z2f″(tz) / 2.
Thus, if |z| = 1/3 and |w| < 1/6, we have
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(
f
(
z
)
−
w
)
−
(
z
−
w
)
|
=
1
2
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z
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2
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f
″
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t
z
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≤
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z
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2
1
−
t
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z
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≤
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z
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2
1
−
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z
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=
1
6
<
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z
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−
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w
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≤
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z
−
w
|
.
{\displaystyle |(f(z)-w)-(z-w)|={\frac {1}{2}}|z|^{2}|f''(tz)|\leq {\frac {|z|^{2}}{1-t|z|}}\leq {\frac {|z|^{2}}{1-|z|}}={\frac {1}{6}}<|z|-|w|\leq |z-w|.}
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(
f
(
z
)
−
w
)
−
(
z
−
w
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=
1
2
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z
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2
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f
″
(
t
z
)
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≤
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z
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2
1
−
t
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z
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≤
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z
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2
1
−
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z
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=
1
6
<
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z
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−
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w
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≤
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z
−
w
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.
{\displaystyle |(f(z)-w)-(z-w)|={\frac {1}{2}}|z|^{2}|f''(tz)|\leq {\frac {|z|^{2}}{1-t|z|}}\leq {\frac {|z|^{2}}{1-|z|}}={\frac {1}{6}}<|z|-|w|\leq |z-w|.}
By Rouché's theorem, the range of f contains the disk of radius 1/6 around 0.
Let D(z0, r) denote the open disk of radius r around z0. For an analytic function g : D(z0, r) → C such that g(z0) ≠ 0, the case above applied to (g(z0 + rz) − g(z0)) / (rg′(0)) implies that the range of g contains D(g(z0), |g′(0)|r / 6).
For the general case, let f be an analytic function in the unit disk such that |f′(0)| = 1, and z0 = 0.
- If |f′(z)| ≤ 2|f′(z0)| for |z − z0| < 1/4, then by the first case, the range of f contains a disk of radius |f′(z0)| / 24 = 1/24.
- Otherwise, there exists z1 such that |z1 − z0| < 1/4 and |f′(z1)| > 2|f′(z0)|.
- If |f′(z)| ≤ 2|f′(z1)| for |z − z1| < 1/8, then by the first case, the range of f contains a disk of radius |f′(z1)| / 48 > |f′(z0)| / 24 = 1/24.
- Otherwise, there exists z2 such that |z2 − z1| < 1/8 and |f′(z2)| > 2|f′(z1)|.
Repeating this argument, we either find a disk of radius at least 1/24 in the range of f, proving the theorem, or find an infinite sequence (zn) such that |zn − zn−1| < 1/2n+1 and |f′(zn)| > 2|f′(zn−1)|.
In the latter case the sequence is in D(0, 1/2), so f′ is unbounded in D(0, 1/2), a contradiction.
Bloch's theorem
In the proof of Landau's Theorem above, Rouché's theorem implies that not only can we find a disk D of radius at least 1/24 in the range of f, but there is also a small disk D0 inside the unit disk such that for every w ∈ D there is a unique z ∈ D0 with f(z) = w. Thus, f is a bijective analytic function from D0 ∩ f−1(D) to D, so its inverse φ is also analytic by the inverse function theorem.
Bloch's and Landau's constants
The number B is called Bloch's constant. The lower bound 1/72 in Bloch's theorem is not the best possible. Bloch's theorem tells us B ≥ 1/72, but the exact value of B is still unknown.
The best known bounds for B at present are
-
0.4332
≈
3
4
+
2
×
10
−
4
≤
B
≤
3
−
1
2
⋅
Γ
(
1
3
)
Γ
(
11
12
)
Γ
(
1
4
)
≈
0.47186
,
{\displaystyle 0.4332\approx {\frac {\sqrt {3}}{4}}+2\times 10^{-4}\leq B\leq {\sqrt {\frac {{\sqrt {3}}-1}{2}}}\cdot {\frac {\Gamma ({\frac {1}{3}})\Gamma ({\frac {11}{12}})}{\Gamma ({\frac {1}{4}})}}\approx 0.47186,}
where Γ is the Gamma function. The lower bound was proved by Chen and Gauthier, and the upper bound dates back to Ahlfors and Grunsky.
The similarly defined optimal constant L in Landau's theorem is called Landau's constant. Its exact value is also unknown, but it is known that
-
0.5
<
L
≤
Γ
(
1
3
)
Γ
(
5
6
)
Γ
(
1
6
)
=
0.543258965342...
{\displaystyle 0.5<L\leq {\frac {\Gamma ({\frac {1}{3}})\Gamma ({\frac {5}{6}})}{\Gamma ({\frac {1}{6}})}}=0.543258965342...\,\!}
(sequence A081760 in the OEIS)
In their paper, Ahlfors and Grunsky conjectured that their upper bounds are actually the true values of B and L.
For injective holomorphic functions on the unit disk, a constant A can similarly be defined. It is known that
-
0.5
<
A
≤
0.7853
{\displaystyle 0.5<A\leq 0.7853}
See also
References
- Ahlfors, Lars Valerian; Grunsky, Helmut (1937). "Über die Blochsche Konstante". Mathematische Zeitschrift. 42 (1): 671–673. doi:10.1007/BF01160101. S2CID 122925005.
- Baernstein, Albert II; Vinson, Jade P. (1998). "Local minimality results related to the Bloch and Landau constants". Quasiconformal mappings and analysis. Ann Arbor: Springer, New York. pp. 55–89.
- Bloch, André (1925). "Les théorèmes de M.Valiron sur les fonctions entières et la théorie de l'uniformisation" (PDF). Annales de la Faculté des Sciences de Toulouse. 17 (3): 1–22. doi:10.5802/afst.335. ISSN 0240-2963.
- Chen, Huaihui; Gauthier, Paul M. (1996). "On Bloch's constant". Journal d'Analyse Mathématique. 69 (1): 275–291. doi:10.1007/BF02787110. S2CID 123739239.
- Landau, Edmund (1929), "Über die Blochsche Konstante und zwei verwandte Weltkonstanten", Mathematische Zeitschrift, 30 (1): 608–634, doi:10.1007/BF01187791, S2CID 120877278