Analytic Continuation
Can a holomorphic function defined only on a small disk secretly determine its own values elsewhere? This question sounds absurd for smooth real functions. Those can be modified arbitrarily far from any given point. For holomorphic functions, though, the answer is a resounding yes. The rigidity behind the Identity Theorem and Zeros makes this possible. A holomorphic function is pinned down by its values on any set with an accumulation point. This forces every local piece of a holomorphic function to carry a seed. That seed points to a unique, often much larger, global object. This phenomenon, called analytic continuation, is one of the most striking manifestations of complex rigidity. It explains why the Riemann zeta function has a fully determined extension. The function was originally defined only for by a convergent series. Yet it extends to nearly the whole plane. It also explains why the "multivalued" square root or logarithm functions aren't really functions on the plane. Instead, they are functions on a more subtle geometric object called a Riemann surface. The big picture is that holomorphy is a local condition with global consequences. Overlapping consistent local descriptions glue together in an essentially forced way. When they fail to glue consistently around a loop, new geometry is born. This includes branch points, monodromy, and multivaluedness. This article builds analytic continuation from the ground up. We cover continuation along a chain of disks, and continuation along a path. We introduce the Monodromy Theorem, which controls when path-continuations agree. We also examine the emergence of multivalued functions and their natural domains, called Riemann surfaces. These ideas are shown through worked examples with and . Throughout, we use Mobius Transformations as recurring test objects. We contrast their single-valued rigidity with the genuinely multivalued behavior of roots and logarithms. We aim for full rigor. Every continuation step is justified by the Identity Theorem. The Monodromy Theorem is proved in complete detail. This proof uses a compactness/connectedness argument on the unit interval. Subtleties are pinned down precisely, especially continuation along homotopic versus merely different paths.
- Analytic continuation extends a holomorphic function beyond its original domain by chaining together overlapping power series that must agree on overlaps by the Identity Theorem.
- Continuation along a path is well-defined step by step, but the final germ obtained can depend on which path was chosen.
- The Monodromy Theorem says: if the domain is simply connected (or more precisely, if two paths are homotopic rel endpoints within the domain of continuability), continuation along them yields the same result.
- Functions like and cannot be continued consistently around the origin — continuing all the way around a loop returns a different branch, revealing genuine multivaluedness.
- The set of all germs obtained by continuation, glued together correctly, forms a Riemann surface on which the "multivalued function" becomes single-valued and holomorphic.
- Key idea: local holomorphic data plus overlap-consistency forces a unique (but possibly path-dependent, possibly multivalued) global extension.
Where this lives today
Analytic continuation is the mechanism behind the Riemann zeta function's extension to , which underlies the Riemann Hypothesis and much of analytic number theory; the functional equation and continuation of and -functions are indispensable in the distribution of primes. In physics, analytic continuation in the complex time or coupling-constant variable — Wick rotation between Minkowski and Euclidean quantum field theory, or continuation of scattering amplitudes and partition functions — relies on exactly the path-continuation and monodromy framework developed here. In algebraic geometry and complex geometry, the passage from local holomorphic germs to global multivalued functions on Riemann surfaces is the seed of the theory of covering spaces, uniformization, and the modern sheaf-theoretic viewpoint on complex manifolds. In applied contexts, analytic continuation underlies Borel summation and resurgence techniques for divergent perturbative series in mathematical physics, and in numerical and engineering contexts (e.g. conformal mapping, control theory, signal processing) continuation arguments justify extending transfer functions or Green's functions beyond their original region of convergence.
Ask the tutor: How does the construction of the "complete analytic function" as a Riemann surface make precise the idea that √z or log z are single-valued once we change the domain?
A function element is a pair where is a domain (open, connected) and is holomorphic. Two function elements and are direct analytic continuations of one another if and on some connected component of . A chain of continuation is a finite sequence of function elements such that and are direct analytic continuations of each other for . We say is obtained from by analytic continuation. Given a path and a function element with , a continuation of along is a family of function elements such that: 1. for every ; 2. for every there is such that for all with , and on a neighborhood of (equivalently, is the germ of at ). By a germ of a holomorphic function at a point we mean an equivalence class of function elements with , where iff on some neighborhood of contained in . The germ at determined by the continuation is denoted .
Intuition
Picture a holomorphic function as a puddle of certainty spreading from its power series at a point, radius equal to the distance to the nearest true singularity. The Identity Theorem says this puddle's shape and values are completely non-negotiable: any two holomorphic functions that agree on an open subset of overlap must agree throughout the overlap's connected component, since their difference is a holomorphic function vanishing on a set with an accumulation point, hence identically zero. This is the mechanism, and only this mechanism, that lets us walk a chain of overlapping disks and know that "the same function" (as a germ) is propagating, not a new arbitrary redefinition. Now imagine walking around a small loop encircling while carrying a branch of . Locally, at each point of the loop, is perfectly well-defined and holomorphic — it is the puddle-spreading process itself that is unambiguous at every step. But after a full trip around the loop, the value has silently increased by . The obstruction is not a failure of local rigidity; it is global topology: the loop is not contractible in , so there is room for the continued germ to differ from the starting germ even though every local step was forced. This is the origin of the branch cut and, more deeply, of Riemann surfaces: instead of forcing to live on (where it cannot be single-valued), we build a new domain — an infinite spiral staircase covering — on which is single-valued.
(A) Uniqueness along a fixed path. Let be a function element and a path with . If and are both continuations of along , then for every ; that is, the germ obtained by continuing along a given path is unique.
(B) Monodromy Theorem. Let be a domain, a function element with , and suppose can be analytically continued along every path in starting at a fixed basepoint . Let be two paths from to a common endpoint , and suppose and are homotopic in rel endpoints (i.e. through a continuous family of paths in from to ). Then the continuation of along and along produce the same germ at . In particular, if is simply connected and can be continued along every path in from , then continuation produces a single well-defined holomorphic function on all of extending .
Let be a domain and holomorphic on . If on a nonempty open subset , then on all of .
This is precisely the Identity Theorem and Zeros: let , holomorphic on the connected open set . Since on the open set , every point of is a non-isolated zero of (in fact an accumulation point of zeros, being an interior point). The Identity Theorem states that a holomorphic function on a domain with a zero set having an accumulation point in the domain is identically zero on the domain. Hence on , i.e. on .
∎Technique: connectedness of via the "closed and open" argument. Let . We show is nonempty, open, and closed in ; since is connected, this forces . Nonempty. By hypothesis as the initial element (both continuations start from the same germ at ), so . Open. Let , so , meaning on some open neighborhood of contained in . By definition of continuation along a path (condition 2), there is such that for : , near , and near (shrinking if necessary to satisfy both continuation conditions simultaneously — possible since each condition individually supplies such an , and we take the minimum). Since throughout the neighborhood (by definition of ), and both agree with respectively near , shrinking further to lie inside gives near . Hence for all with (intersected with ), so is open in . Closed. Let be a limit point of ; we show . By the continuation condition applied at , there is such that for , and , near . Since is a limit point of , choose with , . Then , i.e. on a neighborhood of . But also and near (by the choice of applied to ). So on a common neighborhood of contained in (all these domains being open sets containing , their intersection is open and nonempty). Since are domains (connected open sets) and agree on a nonempty open subset of 's component containing , and lies in the same domain — we now apply the Local persistence of equality Lemma on the connected component of containing : on all of . Since continuation requires for near and by continuity of , and lie in the same connected component (as is continuous and connects them through nearby values of , all mapping into by the openness condition — more directly, trivially and is in the same component as because both are limits along the connected path-image for between , which lies in by the -condition). Hence near , i.e. . So is closed. Since is nonempty, open, and closed in the connected space , . This proves part (A).
∎Technique: compactness of and a grid subdivision argument, combined with part (A). Let be a homotopy rel endpoints with , wait — we set conventions: let , for all , , , and continuous on with values in . For each , let , a path from to in . By hypothesis, continues along every path in from ; in particular it continues along each . By part (A), for each fixed the germ at the endpoint is unambiguous — the notation is well defined. We must show is locally constant in , hence constant on the connected interval (again by connectedness), giving , i.e. continuation along and agree. Claim: for each , there is such that . Fix . Let denote a continuation of along . For each , is an open set containing ; let be such that the open disk . Since is compact and is continuous, and since the continuation family also satisfies a local-persistence property, we may — by compactness of — choose a finite partition
and radii so that:
- for each ;
- for all (i.e. the disk covers the path segment) — such a partition exists because covers and Lebesgue's number lemma applied to the compact metric space with the open cover by preimages of the disks gives a uniform partition mesh.
By continuity of on the compact square , is uniformly continuous. Hence there is such that implies
and moreover whenever (shrinking further using uniform continuity of so that nearby-in- paths stay within the same chain of disks — this is possible since uniform continuity controls for all simultaneously once ). Now fix such with . We claim the continuation of along can be carried out using the same chain of function elements (restricted appropriately), because the path restricted to stays inside the disk , on which the germ is already . Concretely: define a continuation along by setting, for , the function element to be the germ of at (well-defined since ). At the junction points , both the element inherited from the -th disk and from the -th disk are restrictions of the original continuation-along- chain, which are consistent by construction of a valid continuation (they were direct analytic continuations of each other along , and since also lies in the overlap of the two disks — using that the disks have radius large enough to contain a neighborhood of both and the nearby — the same equality on overlap propagates). Hence this defines a valid continuation of along , terminating at with the germ — the same germ as the continuation along , because and the last function element in the chain is literally (unchanged, since is a fixed endpoint of the homotopy, for all ). By part (A) (uniqueness of continuation along a fixed path ), any continuation of along — in particular the one we are given by hypothesis — must yield the same terminal germ as this explicitly constructed one. Therefore . This proves the claim: is locally constant on . A locally constant function on the connected space is constant, so , i.e. continuation along and continuation along produce the same germ at . This proves part (B). For the final statement: if is simply connected, any two paths in from to any point are homotopic rel endpoints (definition of simple connectivity), so depends only on the endpoint , not on the path. Defining (as a germ, hence a well-defined holomorphic function value near ) gives a well-defined function on , holomorphic since it agrees locally with each continued function element, and it extends since restricted to the constant path at recovers .
∎Worked examples
Example 1: Continuing around the singularity at , staying single-valued. The power series converges on to . We continue this along the path for — the circle of radius about the origin, which stays well inside and avoids the singularity at . Since already contains the entire trace of , the trivial continuation for all works, and by uniqueness (Part A) this is the continuation. The germ at (back at ) is exactly the original germ: no monodromy, as expected since is a loop contractible in actually here we didn't even need to leave . Now let's do a genuinely nontrivial continuation. Take instead with , and continue along the straight path for heading from toward the point , which lies outside the unit disk (in fact ). We build the chain explicitly. Since is holomorphic on all of , and our path never touches (it heads off at angle , never reaching the positive real axis except at ), we may re-expand at each point along the way. Concretely, expand about the point for any fixed :
convergent for , the distance from to the singularity . Since never equals for (as is real only at , giving ), the radius of convergence is a continuous, strictly positive function of on the compact set , hence bounded below by some . Taking and the above series, one checks directly (matching Taylor coefficients, or just recognizing all these series as restrictions of the single global meromorphic function on ) that consecutive elements agree on overlaps. This is a valid continuation, and since restricted to a neighborhood of the path is simply connected around this particular path (the path doesn't wind around ), the terminal germ at is simply the Taylor expansion of centered there:
Numerically, , so , and
This illustrates the general principle: a meromorphic function on continues consistently along any path avoiding the poles, precisely because is the natural single-valued domain and continuation just re-expands the same global object — no monodromy arises for rational or meromorphic functions, only for functions with branch points (as in Example 2).
Example 2: The multivaluedness of around , with an explicit non-symmetric loop. Let (a disk centered at , avoiding ), and define
using the branch of argument continuous near (where ). Concretely (check: ✓.) Now continue along the path
a circle of radius centered at the origin, starting and ending at , traversed once counterclockwise starting from angle . At each parameter , expand near using the branch of argument that continuously varies as (a continuously increasing real number, not reduced mod ), so that
This is a valid continuation: consecutive elements agree on overlaps since varies continuously and each is a genuine branch of on a small disk around not containing . At : again, but now the germ is with . So
This is manifestly different from . So continuation of once around the origin returns the negative of the original branch: as germs (their values already disagree at the single point ). Continuing a second time around the loop, one recovers again (since increases by total, and ), confirming is exactly 2-valued and its continuation has monodromy of order 2. This is entirely consistent with the Monodromy Theorem: it does not apply here because (the domain avoiding the branch point) is not simply connected, and indeed our loop is not null-homotopic in — precisely the situation the theorem's hypothesis excludes.
The Monodromy Theorem requires that the two paths be homotopic within the region where continuation is possible along every path. Drop this and continuation genuinely fails to be well-defined as a function on , even though it remains well-defined as a germ along each individual path. Take , which is connected but not simply connected. Let be the germ of at as in Example 2 above, i.e. . This germ can be continued along every path in (since , or more precisely a continuously-varying choice of argument, can always be locally defined away from ) — so the hypothesis " continues along every path in from " genuinely holds. Now take two paths from to itself (a loop):
- , the constant path.
- , the full counterclockwise loop of Example 2.
Both are paths in from to . Continuation along trivially returns the same germ , giving value . Continuation along returns, as computed above, the germ with value at . These two terminal germs are different, even though and share the same start and end point. The reason the Monodromy Theorem's conclusion fails here is exactly that its hypothesis fails: and are not homotopic rel endpoints in , because has fundamental group (generated by loops winding around ), and winds once around while winds zero times — they represent different, non-trivial elements of , so no continuous homotopy through loops in based at can deform one into the other. If we had instead required to be simply connected (e.g. a slit plane ), no such discrepancy could arise, exactly as the theorem promises: all loops in a simply connected domain are null-homotopic, so continuation around any loop returns to the same germ, ruling out this construction. This is the precise mechanism by which "multivalued functions" arise: they are single-valued germs whose continuation is path-independent locally, but whose continuation around non-contractible loops in a punctured or otherwise non-simply-connected domain produces a strictly different germ at the same point.
Scope, edge cases & common traps
| Situation | What holds | What can fail |
|---|---|---|
| simply connected, continuation possible along all paths from | Global single-valued holomorphic extension on (Monodromy Thm) | — |
| not simply connected (e.g. punctured disk) | Continuation along each fixed path is still unique | Different (non-homotopic) paths can give different germs at the same endpoint |
| Meromorphic functions (, rational functions) | No monodromy: continuation around poles avoided entirely reproduces the same global meromorphic function | Continuation is not possible through the poles themselves (domain of continuability excludes poles) |
| Branch-point functions (, , , etc.) | Continuation well-defined locally; loops around branch points change the germ | Naively writing " is a function on " is false — it is a function on a Riemann surface covering |
| Continuation along a path that leaves and re-enters the original domain of definition without ever crossing a singularity | Reproduces the original function element again upon return, by Part (A) uniqueness | — |
| Attempting continuation across a natural boundary (e.g. on ) | Continuation is impossible past any boundary arc: no function element continues across any boundary point | Common trap: assuming every power series boundary is "just a singularity to route around" |
The mathematician behind it
Origins · 1 minKarl Weierstrass and how this was discovered
Weierstrass developed the theory of analytic continuation via convergent power series and "elements" precisely to give complex analysis an arithmetically rigorous foundation, free from the more geometric (and at the time less airtight) approach of Riemann. His notion of a function as an equivalence class of overlapping power series — exactly the "function element" and "germ" formalism used above — became the standard rigorous language for continuation, monodromy, and eventually the modern theory of Riemann surfaces and analytic sheaves.
Why does the Identity Theorem force continuation to be "essentially unique" locally?
Because two direct analytic continuations of the same germ that overlap on an open set must, by the Identity Theorem, agree on the entire connected component of the overlap — a holomorphic function vanishing on an open set has an accumulation point of zeros, hence (on a connected domain) is identically zero. So there is no freedom to "redefine" the function differently on the overlap; any valid continuation step is completely determined by matching the germ, not chosen freely. This is what makes the "chain of disks" construction well-posed: consecutive elements are forced to agree wherever they overlap, so gluing produces one coherent object, not an arbitrary patchwork. Uniqueness along a fixed path (Part A above) is a direct consequence of this rigidity together with a connectedness argument on the parameter interval .
Is every "multivalued function" really a single-valued function on some larger space?
Yes, in the precise sense developed by Weyl: given a germ that continues along every path in a domain , one constructs the complete analytic function by gluing together all germs obtained via all possible continuations, topologized so that continuation along paths corresponds to lifting paths. This produces a genuine Riemann surface with a covering map (or more general holomorphic map) , and the original multivalued expression becomes an honest single-valued holomorphic function on . For this is the double cover of branched at ; for it is the universal (infinite-sheeted) cover.
Does analytic continuation always succeed if the function is bounded near the boundary?
No — boundedness is not sufficient; the obstruction is whether any function element extends across a boundary point, which is a purely local question about the behavior of the germ there, not a global boundedness statement. A function can be bounded on a disk and yet have every boundary point be a genuine obstruction to continuation, the extreme case being a natural boundary, as in the lacunary series , which is bounded on compact subsets of (locally uniformly convergent there) but admits no analytic continuation across any arc of the unit circle. Conversely, unbounded functions like continue perfectly well past most of their "singular-looking" boundary, since is an isolated obstruction, not a natural boundary.
How does the Monodromy Theorem relate continuation to the fundamental group?
It shows that continuation of a germ along loops based at , when it always succeeds, defines a map from to the set of germs at obtainable by continuation (the "monodromy action"). The Monodromy Theorem is the statement that this map factors through homotopy classes of loops — i.e., it only depends on the class in , not the specific loop. When is simply connected, is trivial, so the monodromy action is trivial and continuation gives one single-valued extension. For and , the monodromy action of the generator of is "add ," an infinite-order action reflecting the infinitely many branches of the logarithm.
Can two completely different-looking power series be analytic continuations of one another?
Yes, and this is common and important: the same underlying global holomorphic (or meromorphic) function can look utterly different when expanded around different centers, yet be connected by an explicit chain of continuations. The classic example is on versus its re-expansion around ; both are Taylor series of but with different coefficients and different radii of convergence ( versus ). Recognizing two power series as continuations of each other typically requires either identifying a common closed-form function (as here) or explicitly verifying agreement on an overlap region via the Identity Theorem, since matching coefficients directly is usually infeasible.
What goes wrong if we try to apply the Monodromy Theorem without checking that continuation is possible along every path, not just the two given ones?
The theorem's hypothesis is global: must continue along every path in starting at , not merely along and . This matters because the proof constructs the homotopy as an entire family of intermediate paths , and continuation must succeed along each of these intermediate paths for the compactness argument (Lebesgue number / uniform continuity step) to go through. If continuation is only known to be possible along the two endpoint paths but fails along some intermediate path in the homotopy — for instance if that intermediate path passes through a singularity avoided by themselves — the theorem simply does not apply, and no conclusion about agreement of the two germs can be drawn.
Why is √z only 2-valued while log z has infinitely many branches?
This reflects the order of the monodromy action of the generator of : continuing once around multiplies the germ by , and repeating this twice gives , returning to the start — so the monodromy has order exactly , giving exactly two branches. For itself, continuing once around adds to the value, and no finite number of repetitions ever returns to the original value (adding is never for ), so the monodromy has infinite order, producing infinitely many distinct branches indexed by . In general has monodromy of order exactly around .