Brauer-Manin obstruction for Erd\H{o}s-Straus surfaces
Martin Bright, Daniel Loughran

TL;DR
This paper investigates why certain solutions to the Erdős–Straus conjecture fail the integral Hasse principle and strong approximation, using the Brauer-Manin obstruction as a key tool.
Contribution
It applies the Brauer-Manin obstruction to analyze failures of the integral Hasse principle for Erdős–Straus surfaces, providing new insights into their arithmetic properties.
Findings
Identifies cases where the Brauer-Manin obstruction explains failures
Provides criteria for the failure of strong approximation
Enhances understanding of the arithmetic structure of Erdős–Straus surfaces
Abstract
We study the failure of the integral Hasse principle and strong approximation for the Erd\H{o}s-Straus conjecture using the Brauer-Manin obstruction.
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Brauer–Manin obstruction for Erdős–Straus surfaces
Martin Bright
Mathematisch Instituut
Niels Bohrweg 1
2333 CA Leiden
Netherlands
and
Daniel Loughran
Department of Mathematical Sciences
University of Bath
Claverton Down
Bath
BA2 7AY
UK https://sites.google.com/site/danielloughran/
Abstract.
We study the failure of the integral Hasse principle and strong approximation for the Erdős–Straus conjecture using the Brauer–Manin obstruction.
2010 Mathematics Subject Classification:
14G05 (primary), 11D68, 11D25, 14F22 (secondary)
Contents
- 1 Introduction
- 2 Geometry of Erdős–Straus surfaces
- 3 Brauer–Manin obstruction
- A Comparison with previous results
1. Introduction
1.1. The Erdős–Straus conjecture
The Erdős–Straus conjecture states that for every the equation
[TABLE]
always has a solution with . Note that there is always a solution with [14], and to prove the conjecture it suffices to consider the case where is a prime. Moreover for any fixed , it is straightforward to see that there can be only finitely many solutions, and that they may be easily enumerated (see Lemma 3.10). We refer to Mordell’s book [19, Ch. 30] and the more recent paper [8] for further background and history on this problem.
In this paper we investigate what modern techniques from arithmetic geometry can say about this conjecture and more generally the structure of the solutions to (1.1). At a first glance, it is not clear how to use tools from modern algebraic geometry to tackle the problem, as is not a ring. However, this conjecture does indeed have a natural interpretation as a question of strong approximation, stipulating that integer solutions with certain real conditions exist. Our first main result states that there is no Brauer–Manin obstruction in this case (see §1.2 for a more precise statement and background on the Brauer–Manin obstruction).
Theorem 1.1**.**
Let . Then there is no Brauer–Manin obstruction to the existence of natural number solutions of the equation (1.1).
Despite there being no Brauer–Manin obstruction to the conjecture, it turns out that there is in fact an obstruction to strong approximation at the -adic places. This obstruction has the following completely explicit description. (In the statement denotes the Hilbert symbol.)
Theorem 1.2**.**
Let be odd and a solution to (1.1). Then
[TABLE]
Despite the apparent asymmetry, the given Hilbert symbols are actually invariant under the natural action of the symmetric group on the variables (see Proposition 2.6). In the stated generality, Theorem 1.2 does not seem to have been known and gives new conditions which natural number solutions must satisfy. Theorem 1.2 allows one to recover various known results in a more systematic and conceptual way, as special cases of a Brauer–Manin obstruction. For example if is an odd prime, we have the following.
Corollary 1.3**.**
Let be an odd prime and a solution to (1.1). Then there exists such that . For such a solution we have
[TABLE]
where the symbol is the Legendre symbol.
Corollary 1.3 unifies various quadratic reciprocity conditions found by Yamamoto [24] for . We are also able to recover the following result of Elsholtz and Tao ([8, Prop. 1.6]).
Corollary 1.4**.**
If is an odd square, then there are no natural number solutions with
[TABLE]
Corollary 1.4 is really a condition on natural number solutions which is not present for integer solutions (e.g. for consider the solutions and ). Similarly, the congruence condition in Corollary 1.3 is also not present for integer solutions in general. For example, consider and the solution , where the corresponding Legendre symbol is . In fact, for integer solutions which are not natural number solutions, the exact opposite of Theorem 1.2 holds.
Theorem 1.5**.**
Let be an odd integer and a solution to (1.1) which is not a natural number solution. Then
[TABLE]
1.2. Geometric interpretation
We now explain in more detail how to interpret our results geometrically using the Brauer–Manin obstruction. Consider the corresponding algebraic surface derived from (1.1)
[TABLE]
This is an affine cubic surface, and geometrically a so-called log K surface. Many interesting classical Diophantine equations turn out to concern log K3 surfaces, and their integer points are an active area of research [5, 6, 11, 12, 13, 17]. Note that is singular, with the unique singular point lying at the origin.
We let denote the natural model for given by the same equation in . Note that over for all , by simply rescaling the . The Erdős–Straus conjecture therefore concerns existence of certain integer points on different models over of the same surface over ; in particular this nicely highlights the fact that different models of the same surface can give rise to very different problems in general.
Let be the set of connected components of and the ring of finite adeles. One says that satisfies strong approximation if has dense image in equivalently, if
[TABLE]
for all non-empty open subsets . We work with since is discrete as is affine, hence clearly not dense. We let
[TABLE]
We will show that is a connected component of , and its complement is also a connected component. We define . The Erdős–Straus conjecture is equivalent to (1.3) for , hence stipulates that a special case of strong approximation holds. One can even formulate the conjecture as a problem of strong approximation for ; here it is equivalent to (1.3) for and for all , where
[TABLE]
We now recall how one can use the Brauer group to study this problem (see [20, §8.2] for further background on the Brauer–Manin obstruction). Recall that there is a right continuous pairing
[TABLE]
given by pairing with an element of and taking the sum of local invariants. For an open subset , we define to be the right kernel of this pairing restricted to . We have ; in particular, if then and one says that there is a Brauer–Manin obstruction to strong approximation (cf. (1.3)). We first calculate the Brauer group.
Theorem 1.6**.**
We have
[TABLE]
generated by the quaternion algebra .
The algebra in Theorem 1.6 is transcendental, meaning that it does not become trivial after base change to an algebraic closure of , so we will obtain new cases of a transcendental Brauer–Manin obstruction on log K3 surfaces. One novel feature is that there are few examples in the literature where Brauer groups of singular varieties have been computed, as Brauer group computations usually use Grothendieck’s purity theorem which requires regularity (or at least a singular locus of large codimension). We prove Theorem 1.6 by first calculating the Brauer group of a desingularisation, then showing that every such Brauer group element comes from the singular surface.
This latter property is a special case of a more general result about Brauer groups of singular surfaces, which may be of independent interest and does not seem to have been noticed before. Recall that a normal variety is said to have only rational singularities if there exists a desingularisation for which all the higher direct images of are trivial.
Theorem 1.7**.**
Let be a normal surface over a field of characteristic [math] with rational singularities and a desingularisation. Then the induced map is surjective.
One could hope to use the Brauer group element from Theorem 1.6 to disprove the Erdős–Straus conjecture by showing that ; our next result says that this does not happen.
Theorem 1.8**.**
For all we have
[TABLE]
The first equation (1.4) is a more precise version of Theorem 1.1. The second equation (1.5) says that nonetheless there is always a Brauer–Manin obstruction to strong approximation for natural number solutions (as manifested by Theorems 1.2 and 1.5).
Despite there being a Brauer–Manin obstruction to strong approximation, it turns out that not every failure of strong approximation is explained by the Brauer–Manin obstruction.
Theorem 1.9**.**
For all , the map
[TABLE]
does not have dense image.
We prove this by showing that is not Zariski dense using real considerations. The conclusion then follows from the fact that is finite.
Remark 1.10**.**
In this paper we focus on the original conjecture of Erdős–Straus concerning the equation (1.1). A more general conjecture, due to Schinzel [22], states that given , for all there exists such that
[TABLE]
These surfaces are again -isomorphic, hence Theorem 1.6 still holds here. A minor adaptation of our method shows the following analogue of Theorem 1.2: for all solutions with we have
[TABLE]
Moreover versions of Theorems 1.5, 1.8, and 1.9 also hold in this case.
Outline of the paper
In §2 we study the geometry of Erdős-Straus surfaces over a field of characteristic zero. We calculate the desingularisation, the Picard group, and the Brauer group (Theorem 1.6). In §3 we apply our knowledge of the Brauer group to prove the remaining results from the introduction. The appendix explains in more detail how Corollary 1.3 relates to results of Yamamoto [24].
Notation
For a field , we denote by the group of roots of unity in . For a scheme , we denote by its (cohomological) Brauer group.
Acknowledgements
We thank Yang Cao, Jean-Louis Colliot-Thélène, and Christian Elsholtz for useful comments and references. This work was undertaken at the Institut Henri Poincaré during the trimester “Reinventing rational points”. The authors thank the organisers and staff for ideal working conditions. We are grateful to the referee for numerous helpful comments. The second-named author is supported by EPSRC grant EP/R021422/2.
2. Geometry of Erdős–Straus surfaces
In this section we study the geometry of the surfaces from (1.2). We work over a field of characteristic [math] with algebraic closure . The primary aim of this section is to prove Theorem 1.6. We also prove a result of independent interest on Brauer groups of rational surface singularities (Theorem 1.7).
2.1. The Cayley cubic and its lines
We let
[TABLE]
be the closure of in , with being the affine patch with variables . For , this projective surface is known as Cayley’s (nodal) cubic surface; every is isomorphic over to the Cayley cubic surface. The surface has singularities, each of type , given by setting all but one coordinate equal to [math]; we let be the singularity in . The Cayley cubic has lines over . This induces lines on , of which we are interested in the following lines
[TABLE]
2.2. Desingularisation
Let be the desingularisation of given by blowing up once, with exceptional curve . By abuse of notation, we denote by the strict transform of the relevant lines in . We have the equation
[TABLE]
where are coordinates on , and are homogeneous coordinates on . With respect to this equation, the curves of interest to us are
[TABLE]
One checks that
[TABLE]
2.3. Parametrisation
Any cubic surface with a rational singularity is rational, with a birational parametrisation given by projecting away for the singular point. Applying this to the singularity , we obtain the birational map to . On the desingularisation, this becomes the birational morphism
[TABLE]
We let
[TABLE]
Note that the boundary is the disjoint union of the lines
[TABLE]
The following important observation will be used numerous times.
Lemma 2.1**.**
We have and , with the factor generated by and .
Proof.
That follows from the fact that the map (2.2) becomes an isomorphism onto its image when restricted to . The second part follows from the fact that the invertible regular functions on are generated by characters and non-zero constants. ∎
Lemma 2.2**.**
**
Proof.
By Lemma 2.1 any invertible regular function must be a non-trivial product of powers of and , modulo constants. However, such a function cannot be invertible on since its divisor is always non-trivial by (2.1). ∎
2.4. Picard group
Lemma 2.3**.**
We have generated by .
Proof.
By Lemma 2.1 and (2.1) we have the exact sequence
[TABLE]
where the second map associates to a rational function its divisor and the third map associates to a divisor its class. But by Lemma 2.1. The result now follows from (2.1). ∎
2.5. Brauer group
2.5.1. Brauer group of
We denote by the algebraic Brauer group of a variety .
Lemma 2.4**.**
**
Proof.
Lemma 2.2 and the Hochschild–Serre spectral sequence give an injection . But with trivial Galois action by Lemma 2.3, hence this Galois cohomology group is trivial. ∎
We now find the Galois action on the Brauer group. We denote by , and refer to [10, §2.5] for background on cyclic algebras.
Proposition 2.5**.**
The natural map induced by the inclusion , is an isomorphism. In particular as a Galois module, and its elements are represented by the cyclic algebras
[TABLE]
Proof.
The explicit description of follows from Lemma 2.1 and the fact that , given by the stated cyclic algebras (see [4, §8.1] – note that for we have , but for an th root of unity and we have ).
So let . It suffices to show that is unramified along the boundary (2.4). The are regular and disjoint, hence Grothendieck’s purity theorem [9, Cor. 6.2] yields the exact sequence
[TABLE]
where the last map is the residues along the . (Note that the hypothesis that the boundary divisor be regular is missing from Grothendieck’s statement, but it holds in our case.) However is simply connected, so the corresponding residues are trivial. The result follows. ∎
We next show that every Galois-invariant element of in fact descends to the ground field . To do this, we make use of the relation
[TABLE]
derived from (1.1). (This relation will also appear in other parts of the paper).
Proposition 2.6**.**
The natural map is surjective. A complete set of representatives for the elements of is given by the cyclic algebras
[TABLE]
These algebras have the following equivalent representations:
[TABLE]
Proof.
By Proposition 2.5, we have , and this is (non-canonically) isomorphic to [6, Lem. 2.4]. By Proposition 2.5, the cyclic algebras therefore give a complete set of representatives for the Galois-invariant elements. It thus suffices to show that these descend to .
The different representations are easily checked to hold in the Brauer group of the function field of , using (2.1) and the relation . To show that is unramified along the , we use (2.1). By symmetry, it suffices to show that is unramified along . However, by (2.1) and standard formulae for residues [10, Prop. 7.5.1, Ex. 7.1.5], the residue of along is
[TABLE]
where is the order of . But using the relation (2.5), we have
[TABLE]
so that the residue is in fact equal to along as here. This shows that , as required. ∎
Note that Proposition 2.6 shows that is finite if is a number field; something which is not a priori obvious.
Corollary 2.7**.**
If , then is isomorphic to generated by the class of the quaternion algebra
[TABLE]
Remark 2.8**.**
Note that the “obvious” Galois-invariant element does not descend to . Despite being unramified over , it ramifies over the lines with constant (non-trivial) residue. We have multiplied this element by some ramified algebraic Brauer group elements to kill these constant residues.
2.5.2. Brauer group of
We calculated the Brauer group of the desingularisation using Grothendieck’s purity theorem. This method uses that is smooth and does not apply directly to . To calculate we shall use Theorem 1.7, which we now prove.
Proof of Theorem 1.7.
We compute the higher direct images with respect to the étale topology and use the Leray spectral sequence for the morphism and the sheaf ; the necessary material can be found in [16, §III, §IV].
Let be the closed points at which is singular, with residue fields , and let be the exceptional divisor above . Let be a geometric point above , and let the fibre above . By [1, Prop. 1], is a tree of s. By [16, Prop. 11.1], is isomorphic to , where is the number of irreducible components of , with the absolute Galois group of permuting the factors as it permutes the irreducible components.
Let be a strict Henselisation of the local ring of at . The standard calculation of the stalks of higher direct images shows that is isomorphic to . The natural map is injective by [16, Thm. 12.1] and surjective by [16, Lem. 14.3], so is an isomorphism. We deduce that and are isomorphic as Galois modules over . Let be the inclusion. Given that is supported at the points , we have computed
[TABLE]
It follows that
[TABLE]
since is an induced module.
We now show that the stalks are torsion-free. The Kummer sequence on gives, for any , an exact sequence
[TABLE]
Proper base change [18, Cor. VI.2.7] shows
[TABLE]
where the last isomorphism follows from the Kummer sequence of , as by [9, Cor. 1.2]. Therefore surjects onto by (2.6), showing that has no non-trivial -torsion.
Using (2.6) and (2.7), the Leray spectral sequence for the morphism and the sheaf now gives an exact sequence
[TABLE]
Since is regular, is a subgroup of and is therefore torsion. Thus the rightmost arrow is zero. This proves that is surjective. ∎
In the case of Erdős–Straus surfaces, we obtain the following stronger result.
Corollary 2.9**.**
The natural map is an isomorphism.
Proof.
By Theorem 1.7, it suffices to show that the stated map is injective. The exact sequence (2.8) here reads
[TABLE]
But is surjective as the strict transform of has intersection number with the exceptional divisor . This completes the proof. ∎
Corollaries 2.7 and 2.9 in particular prove Theorem 1.6.
Remark 2.10**.**
The map in Theorem 1.7 need not be an isomorphism in general. If is the Cayley cubic surface in , then [2, Tab. 2], but the Brauer group of the desingularisation is clearly trivial.
Remark 2.11**.**
We have calculated for completeness; however, we could just have chosen to work on the desingularisation instead. Namely, consider the Brauer group element . Restricting to the exceptional divisor , we find that is constant along as (in fact our choice of is even trivial along ). Therefore, we could have chosen to instead define
[TABLE]
as pairing with is independent of the choice of lift of adelic point from to . This is essentially the approach advocated in [7, §8] for dealing with the Brauer–Manin obstruction on singular varieties. (Note that in our case the smooth points are dense in for all , so in the notation of loc. cit.)
3. Brauer–Manin obstruction
We now study the integral Brauer–Manin obstruction in our case over . Let .
3.1. Local invariants
We begin by calculating the local invariants of the element , which we view as an element of . We take the convention that the local invariants lie in , rather than . Thus for a place of the local invariant map is given by the Hilbert symbol
[TABLE]
The stated expression is only well-defined if ; for other points, one can reduce to the above case as the local invariant is continuous [20, Prop. 8.2.9]. Indeed, it follows from the implicit function theorem that the -points of any dense Zariski-open subset are dense in the smooth points of ; and, as noted in Remark 2.11, the smooth points are dense in .
3.2. Real points
Lemma 3.1**.**
Let
[TABLE]
Then the and are both connected and
[TABLE]
Proof.
We first show that has two connected components. Consider
[TABLE]
This map is not surjective; indeed, we rearrange the equation (2.5) to obtain
[TABLE]
So the image misses every point on the hyperbola , except the origin which is the image of the line . The hyperbola splits the plane into components, but one branch passes through the origin and hence the image of (3.2) has components. The fibres of (3.2) are connected, being a single point or over the origin. Hence has connected components. These are easily checked to be the two components stated in the lemma. The local invariants are then calculated by standard formulae for Hilbert symbols. ∎
3.3. -adic points
3.3.1. Preliminaries
Lemma 3.2**.**
Let be an odd prime with and with . Then there exists such that .
Proof.
Write and where . The equation (1.2) becomes
[TABLE]
Without loss of generality . If , then the result is clear. So assume for a contradiction that . But as , we then have
[TABLE]
Thus , which contradicts the fact that the are units, as required. ∎
Remark 3.3**.**
Note that Lemma 3.2 fails in general if has a prime divisor with valuation at least . For example, for we have the solution .
Lemma 3.4**.**
Let be an odd prime and let be such that . Then
[TABLE]
Proof.
As , this follows immediately from (3.1) and standard formulae for Hilbert symbols [21, Thm. III.1]. ∎
3.3.2. Good primes
Lemma 3.5**.**
For all we have .
Proof.
By continuity, we may assume that . (The continuity argument above was stated for -points, but the -points form an open set in the -points so the argument also holds for -points.) Up to permuting coordinates, Lemma 3.2 gives . If , then the invariant is by Lemma 3.4. So assume , so that . But from the equation (1.2), it is clear that cannot divide only one of the since . As we find that . From (2.5) we have
[TABLE]
As , , and the left hand side is a -adic unit, we must have . Thus and so the local invariant is again trivial by Lemma 3.4. ∎
3.3.3. Bad odd primes
Lemma 3.6**.**
Let be an odd prime. Then the map
[TABLE]
is surjective.
Proof.
We first consider the case where . Write where and substitute . The equation (1.2) becomes
[TABLE]
Modulo this is
[TABLE]
As is odd, there exists a solution with and arbitrary modulo . Geometrically, the equation (3.3) defines the union of three planes which is non-singular away from the common points of intersection. Providing that , we may therefore use Hensel’s lemma to lift to a -adic solution. Thus, we have shown that we may choose -adic solutions such that and both possibilities
[TABLE]
may be realised. The result in this case therefore follows from Lemma 3.4.
We now consider the general case. Let where and . We take a -adic solution as constructed in the previous case, and consider the solution . The quotients are unchanged, hence the result follows from the previous case and (3.1). ∎
3.3.4. The prime
Lemma 3.7**.**
Suppose that is even. Then the map
[TABLE]
is surjective.
Proof.
It suffices to prove the result for , since then we can just obtain the result for all even by rescaling, as in the proof of Lemma 3.6. Here our equation is
[TABLE]
There is the natural number solution which is easily seen to have local invariant . Next, one verifies that the solution
[TABLE]
lifts by Hensel’s lemma to a -point with local invariant . ∎
Surprisingly, for odd the local invariant is always trivial at .
Lemma 3.8**.**
Suppose that is odd. Then .
Proof.
By continuity it is enough to prove
[TABLE]
when . Write with and . Without loss of generality, we may assume that . Looking at valuations in the equation
[TABLE]
shows that . Taking out a factor of gives
[TABLE]
Looking modulo shows . We therefore have
[TABLE]
Using the formula of [21, Thm. III.1], the Hilbert symbol above is given by
[TABLE]
where and . Note that is an even function. We define
[TABLE]
If , then (3.4) gives , and so . If , then (3.4) gives , and so ; and because is even.
The remaining case is . In this case, (3.4) gives , which implies
[TABLE]
and therefore
[TABLE]
Now looking at the possible values for gives the following.
[TABLE]
Thus, in all cases, , completing the proof. ∎
3.4. Proof of Theorem 1.2
Hilbert’s reciprocity law [21, Thm. III.3] gives
[TABLE]
For a natural number solution the local invariant at is by Lemma 3.1. Moreover, the local invariant at is by Lemmas 3.5 and 3.8. ∎
3.5. Proof of Theorem 1.5
Similar to the proof of Theorem 1.2, but if one of the is negative then the local invariant at is , by Lemma 3.1. ∎
3.6. Proof of Corollary 1.3
The first part of the statement follows from Lemma 3.2. For the second part, without loss of generality we assume that . Then by Theorem 1.2 and Lemma 3.4, we deduce that
[TABLE]
whence the Legendre symbol must be , as required. ∎
3.7. Proof of Corollary 1.4
By Theorem 1.2, to prove Corollary 1.4 it suffices to show the following purely local statement (applied to each ).
Lemma 3.9**.**
Let be an odd prime and , where and . Let be such that
[TABLE]
Then .
Proof.
We first consider type 1 solutions. Here the Hilbert symbol is
[TABLE]
However it follows easily from the equation (1.2) that , so that is even and the result follows.
Now consider type 2 solutions. The equation (1.2) implies that , so the Hilbert symbol is
[TABLE]
If , then is even by assumption, and the result follows. Otherwise, suppose that . From (2.5) we have
[TABLE]
since . The result follows. ∎
3.8. Proof of Theorem 1.8
First note that as and , we have
[TABLE]
It follows from Lemmas 3.6 and 3.7 that there is some prime for which the local invariant is surjective on . Therefore, there are elements of (3.5) whose product of local invariants is and , respectively. ∎
3.9. Proof of Theorem 1.9
The set of real points is non-compact. Still, it follows easily from the equation (1.1) that
[TABLE]
These real conditions impose strong arithmetic conditions. (In the terminology of [13, §2] our surface is “not weakly obstructed” but is “strongly obstructed” at infinity.) This observation gives the following.
Lemma 3.10**.**
The set
[TABLE]
is finite. In particular, is not Zariski dense and is finite.
Proof.
Without loss of generality, we have . Then by (3.6) we have so there are only finitely many choices for . If , then we obtain the solution , which is being excluded. Hence we have
[TABLE]
and the left hand size is non-zero and takes only finitely many values. But then as in (3.6), one finds that and take only finitely many values, as required. ∎
Lemma 3.11**.**
For all but finitely many primes , the map is not surjective.
Proof.
Follows from Lemma 3.10 and the Lang–Weil estimates [15] ∎
We now complete the proof of Theorem 1.9. If the map had dense image then, as is finite (Theorem 1.6), it would follow from [6, Lem. 6.5] (applied to ) that the map has dense image for all finitely many primes ; however this clearly contradicts Lemma 3.11, and shows Theorem 1.9. ∎
Remark 3.12**.**
Let be a smooth variety over which contains a dense torus with and torsion free. If the action of on itself extends to , i.e. is a toric variety, then in [3, 23] it is shown that the Brauer–Manin obstruction is the only one to strong approximation away from . However this result need not hold if the action of does not extend to the whole variety. Here contains but does not satisfy this result by Theorem 1.9.
Appendix A Comparison with previous results
In [24] (see also [19, p. 290]), Yamamoto shows numerous quadratic reciprocity requirements for solutions to (1.1) when is prime, with various hypotheses. In this appendix we explain how these are all special cases of Corollary 1.3.
There are two types of solutions to (1.1) (see [19, Ch. 30] and [8, Prop. 2.11]). Type 1 is when exactly divides one of the to valuation , and Type 2 is when divides exactly two of the to valuation .
We first deal with Type solutions. Let and suppose that , , . Then one can write (see [19, p. 289])
[TABLE]
with positive integers satisfying , and
[TABLE]
Yamamoto [24, Lem. 2] defines and then shows [24, Lem. 4] that the Kronecker symbol
[TABLE]
This follows from Corollary 1.3. Indeed, using we have
[TABLE]
For Type solutions, let with , , . Write
[TABLE]
with positive integers satisfying and (again see [19, p. 289]). Then we have
[TABLE]
In [24, Lem. 2] Yamamoto defines , assumes (see the proof of [24, Lem. 4]) and shows that the Kronecker symbol
[TABLE]
By Corollary 1.3 we deduce this as follows. As we have
[TABLE]
Yamamoto also proves two further conditions [24, Lem. 3, Lem. 4] in the case which, in either the Type or Type case, reduce to
[TABLE]
where are as defined above for Type or Type solutions, respectively. These also follow from Corollary 1.3, as follows:
[TABLE]
The reference list from the paper itself. Each links out to its DOI / PubMed record.
- 1[1] M. Artin, On isolated rational singularities of surfaces, Amer. J. Math. 88 (1966), no. 1, 129–136.
- 2[2] M. Bright, Brauer groups of singular del Pezzo surfaces, Michigan Math. J. , 62 (3) (2013), 657–664.
- 3[3] Y. Cao, F. Xu, Strong approximation with Brauer-Manin obstruction for toric varieties, Ann. Inst. Fourier , 68 (5) (2018), 1879–1908.
- 4[4] J.-L. Colliot-Thélène, A. Skorobogatov, The Brauer–Grothendieck group , http://wwwf.imperial.ac.uk/~anskor/brauer.pdf .
- 5[5] J.-L. Colliot-Thélène, O. Wittenberg, Groupe de Brauer et points entiers de deux familles de surfaces cubiques affines, Amer. J. Math. 134 (2012), no. 5, 1303–1327.
- 6[6] J.-L. Colliot-Thélène, D. Wei, F. Xu, Brauer–Manin obstruction for Markoff surfaces, Annali della Scuola Normale di Pisa , to appear.
- 7[7] J.-L. Colliot-Thélène, F. Xu, Strong approximation for the total space of certain quadric fibrations, Acta Arith. 157 (2013), 169–199.
- 8[8] C. Elsholtz, T. Tao, Counting the number of solutions to the Erdős–Straus equation on unit fractions, J. Aust. Math. Soc. 94 (2013), no. 1, 50–105.
