Solutions to all six questions of the University of Oxford Part A metric space and complex analysis paper, sat on 12 June 2023. Source: released examination PDF, compilation pages 65–68; paper pages 1–4. The solutions retain the paper's labels. In 2(b)(i), the printed zero case is inconsistent with its one case; the solution explicitly uses the intended . The extra closing parenthesis in the printed definition of the supremum norm metric has no mathematical effect.
A metric space is a bounded set if there is a finite constant such thatFor nonempty , this is equivalent to containment in an open ball of finite radius: the triangle inequality converts a radius bound into a diameter bound, and conversely a diameter bound gives a ball of any slightly larger radius about a chosen point.
It is a complete metric space if every Cauchy sequence in has a limit of a sequence belonging to . Explicitly, the hypothesis on isand completeness requires an with . ThusBoundedness controls distances; completeness ensures that these limiting points remain in the space.
A subset is a closed set in when its complement is an open set in the metric topology. Equivalently,The open ball is taken inside the ambient metric space ; closedness always depends on that ambient space.
First suppose is a closed set. If , the definition in part (ii) gives an open ball disjoint from . Thus every has , and the distance to a set satisfies . Its contrapositive is the required implication.
Conversely, suppose that zero distance to a set forces membership. For we have . Choose . Then , proving is an open set. HenceFor , use the extended-real convention : both assertions hold, with the implication vacuous. Part (b) only uses nonempty sets, so all its distances to a set are ordinary finite real numbers.
Write , so that is the Hausdorff distance. Since is a bounded set, there is a finite with . Nonemptiness of therefore gives , so is finite. Its symmetry and nonnegativity are immediate, as is .
If , then every has zero distance to a set . Since is a closed set, part (a)(iii) gives . Interchanging the sets gives . Thus implies . Closedness is essential here: without it a set and its closure have Hausdorff distance zero.
For the triangle inequality, fix and . The approximation property of an infimum supplies with , and then with . Consequently,Let and take the supremum over to obtain . Applying this inequality in the reverse direction as well yieldsAll metric axioms follow. Boundedness was used to ensure finiteness, and closedness to distinguish different sets; neither was needed for the triangle inequality.
The intersection is a closed set because arbitrary intersections of closed sets are closed. Its nonemptiness needs a construction: bounded closed sets need not be compact sets in this setting.
Fix , , and . Recursively choose , for , using the approximation property of an infimum so thatThis is possible because and . The two bounds form convergent geometric series, so the triangle inequality shows is a Cauchy sequence. By completeness it converges to some .
For each fixed , all sufficiently late lie in , by nesting. Closedness of gives , and hence . In particular, starting with any proves . Moreover,For each starting point , let in this bound on its distance to a set . This does not assert that a nearest point exists. It proves . Since , the other directed Hausdorff distance is zero, andThis is the Summably nested Hausdorff intersection theorem; the summable movement replaces any need for compactness.
Let be a Cauchy sequence for the Hausdorff distance, and putThe bounded set hypothesis makes finite, and the Cauchy sequence property gives . Each is nonempty and a closed set, with .
We need estimates that survive taking the closure. For every nonempty , the distance to a set is Lipschitz continuous with constant one: the triangle inequality gives , and interchanging provesFor every , points of have distance at most from . The same holds throughout their union and its closure, by this continuity. Since ,More generally, if , every point in is within of . Passing to its closure again, and using , givesChoose strictly increasing indices with . Then satisfies part (ii), so it converges in Hausdorff distance to the nonempty closed set , with .
For , the triangle inequality gives the explicit full-sequence boundIt tends to zero as . ThereforeThis proves Completeness of the Hausdorff hyperspace using the proposed tail closures, rather than assuming their diameters shrink.
A metric space is a compact space if every open cover , with all open in , has a finite subcover: finitely many indices cover .
It is a sequentially compact space if every sequence in has a convergent subsequence whose limit of a sequence belongs to . In formulas,A finite subcover is the defining test for compactness; a convergent subsequence is the defining test for sequential compactness.
Let be any sequence in the compact metric space . There must be an such that every open ball about contains for infinitely many indices . Otherwise, for each choose a ball containing only finitely many terms, counted by indices. These balls are an open cover. A finite subcover would imply that only finitely many indices occur anywhere in , a contradiction.
Now choose successively with ; infinitely many available indices make this possible. Then , so is a convergent subsequence. ThusThe proof counts indices rather than distinct points, so it also handles a value repeated infinitely often.
The source prints in the zero case. Since the coordinates are indexed by positive integers, that overlaps its case and does not define a sequence. We use the intended coordinate vectors, with for and for .
Every belongs to , because its entries are bounded by one and its coordinate sequence eventually vanishes. If , their supremum norm distance isIndeed, the difference is at coordinate , at coordinate , and zero elsewhere. No subsequence is a Cauchy sequence, since arbitrarily late distinct terms remain distance one apart. Every convergent sequence is a Cauchy sequence, so no convergent subsequence exists. Therefore .
Yes. Let be any sequence in , where . At coordinate , the values lie in the compact interval . By part (a)(ii) we can successively extract a convergent subsequence for coordinate one, a further one for coordinate two, and so on. Taking the diagonal indices gives a single subsequence for whichThe closed interval bound passes to the limit, so . Hence and .
Coordinate convergence alone would not imply supremum norm convergence. Here the common tail bound supplies the missing estimate. Given , choose with . For ,For the finitely many , coordinate convergence makes all differences less than once is large. Therefore , andThis is an instance of compactness from uniformly vanishing sequence tails. The common bound is exactly what the coordinate vectors in part (i) lack.
By the permitted sequential compactness of the product metric space , the sequence of pairs has a convergent subsequence, and hence a Cauchy subsequence. Choose two of its indices sufficiently late thatThe distance-increasing assumption iterates: . With , use , and then , to obtainBoth summands are nonnegative, soThe use of paired iterates ensures that the same positive return time works for both points.
Choose as in part (i). Since distances between iterates are nondecreasing, the triangle inequality givesLetting and combining with the given reverse bound proves that is an isometry:For surjectivity, fix and use part (i) with and to choose satisfying . Put , interpreting as the identity. By sequential compactness, a convergent subsequence satisfies . The assumed continuity yieldsThus every has a preimage, and . If is empty, both conclusions hold vacuously. This proves the distance-increasing self-map theorem for sequentially compact metric spaces.
At every , the Cauchy-Riemann equations areTo derive them from complex differentiability, approach along real increments . The complex derivative givesApproaching along imaginary increments instead givesThese limits exist because is holomorphic. Equating their real and imaginary parts proves the equations, together with .
A sufficient condition is that is a connected space. Suppose, towards a contradiction, that is the same constant throughout . If , then , contradicting .
If , differentiate in and , and use the Cauchy-Riemann equations from part (a). They giveThe coefficient matrix for has determinant . Hence , so everywhere. A holomorphic function with zero complex derivative is locally constant: within a small disc, differentiate along a straight segment. Local constancy and connectedness imply constancy on , again a contradiction.
Consequently,This is the constant-modulus holomorphic function principle. The extra hypothesis matters: on two disjoint open discs, define on one and on the other. It is holomorphic and nonconstant, yet everywhere.
The function is holomorphic on and hasIts imaginary part is exactly the prescribed . Thus is a real-valued holomorphic function. The Cauchy-Riemann equations force both partial derivatives of its real part to vanish. Since is a connected space, is a single real constant. All possibilities are thereforeConversely every such function has the stated imaginary part. The data determine only up to this real additive constant.
The identity theorem states: if is a nonempty connected open set and are holomorphic functions on , and their equality set has a limit point in , thenThe interior location of the limit point and connectedness are essential hypotheses.
For the proof put . At any , its convergent Taylor series either has every coefficient zero, making zero on a neighbourhood, or has a first nonzero coefficient, of degree . In the latter case,where is holomorphic near . By continuity, is nonzero on a smaller disc. Thus any zero at is isolated unless vanishes on a neighbourhood. An accumulation of distinct zeros at the assumed interior limit point therefore forces the neighbourhood alternative.
Let be the set of points of with a neighbourhood on which . We have just proved , and is an open set. It is also a closed set relative to : a point of its closure outside would be approached by distinct points of , hence by zeros, and the same Taylor series argument would place it in . Since is connected, . Thus on , proving the theorem.
Define . To apply the identity theorem, we first verify that is holomorphic; mere complex conjugation of the values of would not suffice. For ,Thus is an entire function, just as is. At each positive integer , the point is real and is real, so . These distinct points accumulate at . The identity theorem on the connected complex plane givesThis is conjugate reflection of a holomorphic function, with the reality data forcing equality to its reflection.
A function has an isolated singularity at if, for some , it is defined and holomorphic on the punctured disc , while a holomorphic extension through has not been assumed. In particular, its domain omits , or its assigned value there fails to give such an extension. The key local condition isThe convention includes removable singularities, even when a suitable extension would eliminate the missing point.
An isolated singularity at is a removable singularity when there is a holomorphic function on a full disc agreeing with away from . Equivalently,The Riemann removable singularity theorem also characterizes this by boundedness of on a sufficiently small punctured disc. A preassigned incorrect value at is replaced by .
A holomorphic function has a zero of order at when it is holomorphic on a neighbourhood of and factors asEquivalently, and . The order of a zero of a holomorphic function is the degree of the first nonzero term of its Taylor series.
A function has a pole of order at when, on a punctured neighbourhood,Equivalently, has a removable singularity whose extension is nonzero at . After shrinking the neighbourhood so , its reciprocal extends with a zero of order . In particular, at a pole.
We prove the Casorati-Weierstrass theorem by contradiction. Fix an allowed . If the stated image were not a dense set in , there would be a disc disjoint from it. HenceThe holomorphic function is bounded by on that punctured disc. By the permitted Riemann removable singularity theorem, it extends to a holomorphic function on the full disc.
If , then is not identically zero, since is nowhere zero away from . Its Taylor series therefore has a finite first nonzero coefficient: otherwise the identity theorem would make it identically zero. Write with and . Thenhas a pole of order at , since multiplying by gives the nonzero limit .
Both cases contradict an essential singularity. Thus
Use the local factorization for a pole of order :Shrink the disc so that the holomorphic function has no zeros there. Differentiating and dividing gives the logarithmic derivativeThe second term is holomorphic across . Since , the first term cannot cancel. Hence has a simple pole, and the coefficient of in its Laurent series isThis is the pole case of the integer residue of a logarithmic derivative.
Let . It is holomorphic and nowhere zero on a punctured neighbourhood of , and the chain rule givesIf had a pole of order , part (c) would imply . But the derivative of a holomorphic function on a punctured disc has residue zero. Indeed, write its Laurent seriesTermwise differentiation is valid on every smaller closed annulus. The only possible term comes from and has coefficient zero. Thusa contradiction. Therefore . This proves an exponential has no isolated pole, including when has an essential singularity; no choice of a holomorphic logarithm on the entire punctured disc was assumed.
The simple zero assumption gives the local factorizationwhere is holomorphic. In a small disc stays nonzero, so is holomorphic there. Expanding to first order,The residue is thereforeIf , the quotient has a removable singularity rather than a simple pole, and the same formula correctly gives zero. This is the residue formula for a quotient at a simple denominator zero.
The improper integral converges: its integrand is bounded near zero and at most for , which is integrable because .
Set , and . Apply the residue theorem to on the positively oriented sector contour consisting of the segment , the arc for , and the segment , with . No pole lies on the boundary. Exactly one root of is inside this sector, namely ; it is a simple pole. Part (a) givesOn the returning ray, put with decreasing from to zero. Since , the two ray contributions areOn the arc, , so the estimation lemma bounds its contour integral byThe residue theorem and the convergence already established now giveUsing , we concludeThe sector also works for , when it is the upper semicircle. Its angle is chosen so that has the same value on the two rays.
Factor the denominator as and integrateover followed by the upper semicircle, for . The enclosed simple poles are and . The local quotient formula from part (a) givesOn this arc, and , . Thus the estimation lemma givesOn the real line, , so the improper integral is absolutely convergent. Hence the residue theorem yieldsTaking real parts is justified by absolute convergence. ThereforeThe imaginary part vanishes as a further check, since the sine integrand is odd.
A conformal map at a point is a map that preserves oriented angles between regular differentiable curves through . In the differential formulation, it is real differentiable at and its derivative is an orientation-preserving similarity: a rotation followed by multiplication of lengths by a positive constant. The map is conformal on when it has this property at every point:Here is a planar rotation. Conformality is a local property and does not itself require global injectivity. We use the oriented convention standard in complex analysis; a reflection reverses oriented angles.
At , complex differentiability givesWriting , the assumption gives . Its real derivative is therefore the similarity , a rotation through followed by scaling by .
More explicitly, for two differentiable curves with and nonzero tangent vectors, the chain rule givesTaking the complex argument of this ratio shows that the oriented angle is preserved, while nonvanishing ensures both image tangents remain regular. Thus
For , direct calculation givesConversely, solving givesThe denominator cannot vanish inside the unit disc, so these inverse formulas prove . This is the Cayley transform between the half-plane and disk.
For , we also require . In inverse coordinates this becomesThe equivalence holds in both directions, soThus the exterior of the unit semicircle maps to the right half of the unit disc. The circular arc maps to its imaginary diameter, which is excluded because the source inequality is strict.
Let , the right half-disc from part (i). Write with and . Squaring doubles the angle and squares the radius, giving a holomorphic bijectionIts inverse is the unique square root with positive real part, and its derivative is nonzero on . The cut includes zero, because .
Next, the Möbius transformation is a conformal bijection from onto : it is the inverse Cayley transform between the half-plane and disk composed with . For , , it givesConsequently . Since is a bijection on the whole disc, deleting this interval deletes exactly that ray in the image.
The required function composition is thereforeEach component is a conformal bijection between the indicated domains. The only possible denominator zeros of the simplified expression are , outside , andsince is on the excluded semicircle and is outside the upper half-plane. This also checks the local conformality of the conformal map from the exterior half-disc to a slit half-plane.
Suppose were a holomorphic bijection. By the allowed nonvanishing derivative result, throughout . The holomorphic inverse function theorem gives a holomorphic inverse locally at every image point. Since is globally bijective, these local inverses agree with its global inverse .
Thus is an entire function with . The Liouville theorem forces to be constant, contradicting its being an inverse. ThereforeThis is the analytic obstruction behind the fact that the complex plane and unit disc are homeomorphic but not conformally equivalent.
Yes. An explicit holomorphic surjection is the rational functionIts denominator never vanishes inside the unit disc. To prove surjectivity, take any and choose a square root of with ; one of the two opposite roots always has this property. Define . Then andso . Also , and consequently .
This is a holomorphic surjection from the unit disc onto the complex plane. It does not contradict part (i): it is not injective. For example, , with two distinct arguments of modulus .
Solutions to all six questions of the University of Oxford Part A metric space and complex analysis paper, sat on 14 June 2021. Source: released examination PDF, compilation pages 54–58; paper pages 1–5. The examination counted the best four answers; all six are covered here. The printed request in 6(c)(i) is impossible for the stated planar domain: its solution proves this and gives the precise map obtained when the missing point at infinity is accounted for.
A metric space is a complete metric space if every Cauchy sequence in converges to a point of . Explicitly, the hypothesis isand the conclusion is that some satisfies .
It is a sequentially compact space if every sequence in has a convergent subsequence whose limit of a sequence belongs to .
It is a connected space if there are no disjoint nonempty open subsets of with . Here openness refers to the metric topology of .
It is a path-connected space if, for every , there is a continuous map with and . Such a map is a path. Every path-connected space is a connected space: a separation would pull back along a path joining its two sides to a separation of the interval .
The answers, in the order completeness, sequential compactness, connectedness, and path connectedness, areDefine and for . The estimate proves continuity at zero by the squeeze theorem; elsewhere it follows from the usual continuous functions. Thus is the graph of a function on the closed set .
To check closedness directly, if in the Euclidean plane, then and continuity gives . Therefore is a closed subset of the complete metric space , hence is a complete metric space. The sequence has no convergent subsequence, since its first Cartesian coordinates tends to infinity, so sequential compactness fails.
For any two points , the mapis a continuous path in joining them. Thus is path-connected, and consequently connected. The factor is crucial: the oscillations shrink to the single point .
The answers areDistinct natural numbers have . Taking in the Cauchy sequence condition forces every sufficiently late pair of terms to be equal. Every Cauchy sequence is therefore eventually constant and converges in , proving completeness.
The sequence has no convergent subsequence, since convergence would force its sufficiently late terms to lie within distance of its limit of a sequence, hence to equal that limit. Thus sequential compactness fails.
Every singleton is an open ball of radius , so the metric topology is the discrete topology. For example, and form a separation into two nonempty open sets, so is not connected. It is consequently not path-connected either.
The answers areWrite . The given metric describes locally uniform convergence: if and only if for every fixed . Indeed,so convergence in forces . Conversely, split the defining series at : its tail is at most , and its finitely many initial terms tend to zero.
If is a Cauchy sequence in , the same single-term estimate makes it a Cauchy sequence in the supremum norm on every . The completeness of the continuous-map space in the uniform metric gives a continuous function on with uniformly there. Uniqueness of the limit of a sequence gives , so these functions define a single continuous function on . The preceding finite-head and tail argument proves . Thus the space is complete.
The constant functions have whenever . They have no convergent subsequence, so the space is not sequentially compact.
For fixed , set . On ,as . The equivalence with locally uniform convergence proves that is a continuous path for . Hence the space is path-connected and connected.
The inverse tangent is a homeomorphism from the real line with its Euclidean metric onto with its subspace topology: and its inverse are continuous. It is also an isometry from onto , because . Consequently, for ,For a direct open ball interpretation, is -open by continuity of . Conversely, continuity of at supplies a sufficiently small -ball inside any prescribed -ball about . Thus both metrics generate exactly the same open sets.
The arctangent pullback metric is not complete. Take . Since , its transformed sequence is Cauchy, and hence is a Cauchy sequence for . If it converged in to , thenwould force , which is impossible. The missing endpoint of explains the failure of completeness, even though part (i) shows that the metric topologies agree.
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