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A holomorphic function on a Hartogs figure extends to the full bidisc
Statement
Fix . Every holomorphic function on the Hartogs figure admits a unique holomorphic extension to the bidisc .
Facts & Assumptions
Given: A holomorphic function on .
The Hartogs figure and its bidisc hull are the sets defined on the page's opening definition (The Hartogs figure H(r,s) and its bidisc hull).
For any with , define for and .
If , then the slice is holomorphic on the whole unit disc, so the one-variable Cauchy formula recovers it from the circle whenever (Cauchy's integral formula on a circle compactly contained in a disc of holomorphy).
A holomorphic function on a connected open set is determined by its values on any nonempty open subset (A holomorphic function vanishing on a nonempty open subset of a domain vanishes identically).
The negative Laurent coefficients of the -slices vanish identically on the parameter disc (Negative Laurent coefficients vanish on a Hartogs figure), and the coefficient functions themselves are holomorphic in the parameter (Laurent coefficients on Hartogs slices depend holomorphically on the remaining variables).
A separately holomorphic function that is locally bounded is jointly holomorphic (Locally bounded and separately holomorphic implies holomorphic).
Proof
Fix with and define by the Cauchy integral in [L2]. Since and place inside by [L1], the integral is well defined. For fixed with , [L2] applied to the one complex parameter makes holomorphic on . For fixed , the same theorem applied to the one complex parameter makes holomorphic on . The ML estimate gives local bounds on compact subsets, so [L6] upgrades to a jointly holomorphic function on .
If , then the slice is holomorphic on . Therefore [L3] gives whenever and . So extends across the missing core over that open overlap.
If , then both and are holomorphic on by step 1.1, and step 2.1 shows that they agree on the nonempty open subset . Hence [L4] forces on the whole connected domain .
For each point choose any with , and set . Step 3.1 shows that this does not depend on the chosen , so is well defined and holomorphic locally, hence holomorphic on all of .
Step 2.1 gives on the open set , so is a holomorphic extension of to the bidisc. If is another such extension, then and are holomorphic on the connected bidisc and agree on the same nonempty open overlap with ; [L4] gives . Thus the extension is unique.
The Laurent-coefficient view in [L5] is compatible with the integral construction above: the Cauchy kernel removes the vanished negative part and rebuilds the same holomorphic continuation.
Depends on
- Holomorphic extension and domains of holomorphy in several variables
- The Hartogs figure H(r,s) and its bidisc hull
- Laurent coefficients on Hartogs slices depend holomorphically on the remaining variables
- Negative Laurent coefficients vanish on a Hartogs figure
- A contour integral of a jointly continuous, parameter-holomorphic integrand is holomorphic
- Cauchy's integral formula on a circle compactly contained in a disc of holomorphy
- A holomorphic function vanishing on a nonempty open subset of a domain vanishes identically
- Locally bounded and separately holomorphic implies holomorphic
Used by
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Sources
- J. Lebl, Tasty Bits of Several Complex Variables, §2.1 (standard reference, not scraped)