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The Hartogs Phenomena — Examples
1 · Prerequisites
- Absolute and Conditional Convergence; Rearrangement; Products
- Analyticity of Holomorphic Functions; Liouville and Morera
- Arc Length and Rectifiable Curves
- Binary Operations, Monoids, Groups and Subgroups
- Bounded Variation and the Riemann–Stieltjes Integral
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Complex Differentiability and the Cauchy–Riemann Equations
- Complex Power Series and Analytic Functions
- Connectedness
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Contour Integration
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Filters and Ultrafilters
- Finite Counting, Factorials and Binomial Coefficients
- Foundations of the Real Numbers for Analysis
- Function Space Topologies and the Exponential Law
- Fundamental Trigonometric Identities
- Goursat's Theorem and Cauchy's Theorem in a Convex Domain
- Holomorphic Functions of Several Complex Variables
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Isolated Singularities and Laurent Series
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Line Integrals and the Gradient Theorem
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Metric Spaces
- Mixed Partials, Taylor Formulae, and Extrema
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Partitions of Unity and Paracompactness
- pi: the Equivalent Characterizations
- Polynomial Rings, the Division Algorithm and Roots
- Power Series and Real-Analytic Functions
- Properties of the Integral and the Working FTC
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Simple Field Extensions and the Construction of the Complex Numbers
- Sine, Cosine, and the Definition of Pi
- Subspaces, Products, and Quotients
- Suprema and Infima
- The Cantor Set, Baire Category, and Measure Zero in ℝ
- The Complex Exponential and Euler's Formula
- The Derivative and the Mean Value Theorems
- The Exponential Function
- The Fundamental Theorems of Calculus
- The Hartogs Phenomena
- The Identity Theorem, the Maximum Principle and the Open Mapping Theorem
- The Logarithm and General Powers
- The Riemann Integral: Definition and Integrability
- The Topology of Euclidean Space
- The Total Derivative in ℝᵐ → ℝⁿ
- The Winding Number and the Global Cauchy Theorem
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Vector Spaces, Linear Subspaces, Span and Direct Sums
2 · Summary
These examples isolate the geometric and algebraic faces of the Hartogs phenomena. The first two make the Hartogs figure concrete and show that the extension theorem is not merely existential: familiar rational functions already extend across the missing core. The next example turns the puncture theorem into a visible computation on the bidisc minus the origin.
The two counterexamples mark the sharp boundary. In one variable, really has a nonremovable puncture, so the dimension hypothesis is essential. And removing a complex hypersurface behaves differently from removing a compact hole: supports the holomorphic obstruction , so it remains a domain of holomorphy.
3 · Logical flowchart
4 · Definitions, theorems and proofs
None yet.
5 · Examples, counterexamples and false statements
The Hartogs figure in (|z1|, |z2|) coordinates
Example
For , the Hartogs figure is the union of a thin inner cylinder and a thick outer shell:
In the -plane this is exactly the region obtained by taking the rectangle together with the vertical strip .
Facts & Assumptions
Given: Real numbers .
The Hartogs figure and its bidisc hull are defined by the displayed modulus conditions in the two coordinates (The Hartogs figure H(r,s) and its bidisc hull).
Verification
By [L1], membership in depends only on the two moduli and , and the two defining pieces are exactly the inequalities listed in the Example.
So the picture in modulus coordinates is the union of the thin horizontal rectangle with the outer vertical strip , while the missing core is .
The function 1 / (1 - z1 z2) extends holomorphically from a Hartogs figure
Example
The function
is holomorphic on the full bidisc and therefore, a fortiori, on every Hartogs figure inside that bidisc.
Facts & Assumptions
Given: The function on the unit bidisc.
Every holomorphic function on a Hartogs figure extends uniquely to the full bidisc hull (A holomorphic function on a Hartogs figure extends to the full bidisc).
Verification
On the unit bidisc one has , so . Hence the reciprocal is holomorphic there.
Restricting to any Hartogs figure produces a concrete instance of [L1], and the extension theorem recovers the same global formula on the whole bidisc.
A holomorphic function on the punctured bidisc extends across the origin
Example
On the punctured bidisc , the function
is holomorphic and extends holomorphically across the origin as the same formula.
Facts & Assumptions
Given: The punctured bidisc and the function .
In complex dimension at least two, a holomorphic function on a punctured domain extends uniquely across the puncture (An isolated puncture is removable in complex dimension at least two).
Verification
On the full bidisc one has , so . Therefore the same formula defines a holomorphic function on the whole bidisc, and its restriction to the punctured bidisc is the displayed .
This explicit extension agrees with the abstract existence statement of [L1] for the missing point .
The bidisc minus the origin is not a domain of holomorphy
Example
The punctured bidisc
is not a domain of holomorphy.
Facts & Assumptions
Given: The punctured bidisc .
A holomorphic function on a punctured several-variable domain extends across the missing point (An isolated puncture is removable in complex dimension at least two).
A domain of holomorphy is one for which no single larger overlap works for every holomorphic function (Holomorphic extension and domains of holomorphy in several variables).
Verification
Let . By [L1], extends holomorphically across the missing origin to the full bidisc. So the same larger domain works for every holomorphic function on .
The fixed overlap can be taken to be any small bidisc around a point of and the larger domain is the whole bidisc. By [L2], this shows that is not a domain of holomorphy.
The one-variable function 1 / z does not extend across the origin
Statement refuted
Refuted claim: the one-variable function extends holomorphically across .
Facts & Assumptions
Given: The holomorphic function on .
A simple pole is a pole of order (Simple poles).
A pole is exactly a nonremovable singularity whose reciprocal has a zero at the singular point (Characterizations of poles).
Counterexample
The function satisfies , so is a pole of order , that is, a simple pole, by [L1].
By [L2], a pole is not removable. Hence does not extend holomorphically across . This is the one-variable contrast to the several-variable puncture theorem.
C^2 minus a complex line is a domain of holomorphy
Statement refuted
Refuted claim: removing a complex line from produces a domain that still cannot be a domain of holomorphy.
Facts & Assumptions
Given: The domain .
A domain of holomorphy is tested by whether every holomorphic function extends through one fixed larger overlap (Holomorphic extension and domains of holomorphy in several variables).
Counterexample
The function is holomorphic on .
If extended holomorphically across any point of the missing hyperplane , then would extend holomorphically there as the constant function , forcing near that point and hence forcing a holomorphic function equal to at , which is impossible. So the missing complex line blocks extension, and is a domain of holomorphy rather than a Hartogs hole.