Posts filed under ‘algebraic geometry’

Elliptic curves for high school students

I had to give a talk to high school students about some mathematical notion: I decided to tell them something about elliptic curves, but not the usual speech about cryptography, finite fields and the group law on a cubic curve…

Instead, I talked about the perhaps less known appearances of elliptic functions as solutions of classical ODEs (even if I don’t really know much about these myself). The simplest mechanical system whose motion is governed by an elliptic curve is the pendulum: the reason for this is that the ODE \ddot{x} + \sin x = 0 which classically describes the time evolution of the angle of the pendulum is best rewritten in terms of the altitude of the pendulum: the law of energy conservation is then written as
p^2 = q(q-q_0)(q-2l) = P(q)
where 0 and 2l are the extremal values of the altitude q, q_0 is the highest altitude which can be reached with a given energy (even if q_0 > 2l, which corresponds to the pendulum make full rotations around its axis), and p is the vertical momentum of the pendulum.

In this setting, there are classical Hamilton relations dq = p dt, dp = P'(q) dt, so the differential form dt = dq/p turns out to be the canonical non-vanishing abelian differential on the elliptic curve. This explains why the period of the pendulum is an elliptic integral, which can be calculed by an arithmetic-geometric mean, and why the position of the pendulum at t = t_1 + t_2 can be deduced from its position at times t_1 and t_2 by the classical secant-tangent law.

The notes for the talk (in French) are available here.

11 May 2009 at 8:08 pm Leave a comment

Computing Gröbner bases in Haskell

I wrote a small package to compute Gröbner bases in Haskell with the Buchberger algorithm (with applications to variable elimination). Performance is quite bad compared to specialised software like Macaulay, but it seems to work ! I put a Cabal package here. Maybe I’ll add several functions afterwards.

A testcase :
import Data.Polynomial
import Data.Ring
import Algebra.GroebnerBasis
import Algebra.Elimination
type R = Polynom QQ VarXYZ
[x,y,z,t,u,v] = map returnp [X,Y,Z,T,U,V] :: [R]
-- projection from a point on the intersection of quadrics
main = do
print $ step_eliminate [T] $ MakeIdeal
[x^2 - 3*y*z + z*t + 2*x*t,
z^2 + 5*y^2 + z*x - 2*t*z]

The output should be :
[x*y^2+2/5*x^2*z+1/2*y^2*z+3/10*x*z^2+-3/5*y*z^2+1/10*z^3]

20 March 2009 at 7:47 pm Leave a comment

Schemes in algebraic geometry 3 : glued schemes and sheaves

André Weil was among the first ones to point out the importance of having a local description of varieties, especially projective spaces, which can always locally be described as an affine space with completion by a hyperplane at infinity, and projective varieties, which similarly look like varieties in affine space. The use of sheaves in local description of spaces was magnified by Cartan and Serre, in the context of complex analytic spaces, and generalised to the algebraic setting by Serre in Faisceaux algébriques cohérents.

The projective space is the simplest example of an algebro-geometric object which cannot be described by the prime spectrum or the functor of points of a ring. For example, there is no obvious ring whose ideals describe varieties in projective space, which come from homogeneous equations. We would like to give a correct definition of gluing affine lines (with coordinates z and 1/z) to define the projective line \mathbb P^1 as the gluing of \mathbb A^1 with \mathbb A^1 \to \mathbb P^1 given by z \mapsto 1/z. For functors of points, the latest article by Alain Connes and Caterina Consani, gives a definition. For prime spectra, one has to be aware that gluing only topological spaces do not give meaningful information on algebraic properties. This is illustrated by the case of differentiable manifolds, which are not the same as topological manifolds: gluing differentiable manifolds has to induce a correspondance between differentiable functions (this is equivalent to the requirement that gluing maps between charts be differentiable).
(more…)

17 March 2009 at 12:35 am Leave a comment

Schemes in algebraic geometry 2 : prime spectra and generic points

I just explained how the affine plane could be described by the ring \mathbb Z[x,y]. A point M of the affine plane whose coordinate ring is R is a morphism \mathbb Z[x,y] \to R defined by the assignment P \mapsto P(a,b) \in R, where (a,b) are the coordinates of M. In the case of points corresponding to morphisms \mathbb Z[x,y] \to \mathbb Z, there is a natural way of recovering the point from the ring morphism by looking at his equations, which are elements of the kernel of the morphism. If M satisfies the equations x=a and y=b, then M has the form (a,b). This motivates the abstract definition of point of the affine plane as a morphism \mathbb Z[x,y] \to R to some ring.

Conversely, the set of equations of M defines a canonically associated point p_M, which is the morphism \mathbb Z[x,y] \to \mathbb Z[x,y]/I, where I is the ideal generated by the equations. But this morphism has no reason to totally recover M if it wasn’t a point with integral coordinates. For example, the point (2,3) is a special point, satisfying a lot of equations, which characterize it. But (\log 2, \pi) do not satisfy any polynomial equations with integral coefficients, so the set of its equations is empty, and cannot be used to recover it. Moreover, the point (e, \log 3) does not satisfy equations either: their algebraic properties are exactly the same. These points are called generic.

The prime spectrum of a ring is a convenient way of describing equivalence classes of points of a given ring.
Definition. The prime spectrum of A = \mathbb Z[x,y] is the set of points p_I: A \to A/I for prime ideals I. If M: A \to R is any point of the affine plane with coordinates in an integral domain R, then Mis canonically associated to some p_M := p_I, where I is the kernel of the map A \to R.
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10 March 2009 at 10:07 pm 2 comments

Schemes in algebraic geometry I : the affine plane

I think most people blogging around algebraic geometry eventually write about schemes, (as in Rigorous trivialities or algebraic stacks (in the Secret Blogging Seminar), which are traditionnally seen as the main reason (not) to study algebraic geometry today. My turn now. I recommend Igor Dolgacev’s lectures which is one of my favorite ways of speaking of schemes.

Interesting mathematics come up when algebraic varieties (things defined by several polynomial equations) are no longer defined as mere sets (sets of tuples of numbers satisfying the equation) but mope complex mathematical objects. Differential geometry, for example, gives the structure of a complex manifold to algebraic varieties in \mathbb C^n, which is still an efficient way of proving theorems. However, during the 20th century, a lot of mathematicians tried to develop a new structure which would avoid the use of analysis to concentrate on the algebraic aspects (I don’t know exaclty who, but expect Hilbert, Zariski, Chevalley, Grothendieck to have played a role). Grothendieck approach using category theory and functors of points is now widely used and is a very impressive way of tying together intuition, commutative algebra, and geometry.

There are many ways of reverse engineering Grothendieck’s definition of a scheme (see EGA1 if you want to know how this is related to Chevalley’s definition of a scheme). The first thing to say is probably what properties and notions are needed for schemes:
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8 March 2009 at 12:49 pm 2 comments

Ten constructions of the cohomology of varieties

When talking about “the” cohomology of mathematical objects, we do not always explicitly mention which cohomology is used, because it is obvious (in cases there is only one possible definition), or because we really don’t care (since as we will see, it is frequent that different definitions lead to equivalent results). The case of differentiable manifolds or algebraic varieties is particularly impressive, since there were a lot of equivalent cohomology theories defined during last century in order to simplify proofs or allow generalisations. Most cohomology theories, if not all, are defined as the cohomology of a complex : i.e. a sequence of vector spaces or modules (V_n) with a boundary map d. The kernel of d is called the set of cycles, while the images by d are called boundaries : the cohomology H^n is then the quotient of cycles in V_n by the subspace of boundaries.

Classical topologists, for example, will use preferably (see MacLane, Homology or the book of Allen Hatcher) :

  • simplicial (co)homology : it is defined for a triangulated space, i.e. the manifold is cut by curves, surfaces, etc. which make it isomorphic to a sort of polyhedron (a complex); simplicial homology describe non-triviality (holes) in the combinatorial structure of this polyhedron; here the boundary map is really the boundary map.
  • singular (co)homology : a more abstract version of simplicial homology; now we consider the set of all possible simplexes (curves, polygons, polyhedra, and their generalisations…) drawn on the manifold; this definition was given by Eilenberg; I don’t know who first defined simplicial homology, but MacLane mentions that Poincaré and Noether gaves important contributions to this theory.

Then come sheaves, which were explicitly defined by Leray (tales for young mathematicians help remember that Leray made considerable efforts as a prisoner in concentration camps to focus his work on especially “useless” subjects to avoid helping Nazis). (more…)

14 February 2009 at 11:50 pm 4 comments

Experimental algebraic geometry I : the grassmannian

I just began playing with Macaulay 2 to see how it could help doing algebraic geometry without manual tedious computations. Let’s try with the grassmannian: fortunately, the program comes with lots of pre-written functions, including the generation of Grassmanians.

Macaulay provides a command-line interface using the readline library (like many other command-line programs) : here is what input/output looks like

i1 : V = Grassmannian(1,3)
o1 = ideal(p   p    - p   p    + p   p   )
            1,2 0,3    0,2 1,3    0,1 2,3
o1 : Ideal of ZZ[p   , p   , p   , p   , p   , p   ]
                  0,1   0,2   1,2   0,3   1,3   2,3

When I type a command at i1, I get an output o1 with a value \mathrm{ideal}(p_{1,2} p_{0,3} - p_{0,2} p_{1,3} + p_{0,1} p_{2,3}) and a type: this output is an ideal of the ring \mathbb{Z}[p_{0,1}, p_{0,2}, p_{1,2}, p_{0,3}, p_{1,3}, p_{2,3}]. Many features of the Grassmannian as an algebraic variety are available: first define

i1 : V = Grassmannian(1,3,CoefficientRing => QQ);
o1 : Ideal of QQ[p   , p   , p   , p   , p   , p   ]
                  0,1   0,2   1,2   0,3   1,3   2,3
i2 : X = Proj(ring V / V)
o2 = X
o2 : ProjectiveVariety

the projective variety X over \mathbb Q defined by the homogeneous ideal V : here ring V denotes the ambient ring of V. We see that V is a non-singular quadric in 5-dimensional projective space, and check several well-known facts (more…)

7 February 2009 at 11:17 pm Leave a comment

Lines in space and the Grassmann variety

This is an English version of my previous post. Schubert calculus is a collection of techniques and formulae used for computations of enumerative, numerical properties of common objects in linear algebra (there are very nice books by William Fulton covering the subject). The example of the set of lines in three-dimensional space is commonly chosen to illustrate the kind of results which are obtained by Schubert calculus: the reason is probably that it is the simplest non trivial situation.

A line in affine space would usually by defined by its direction (which is a line in a vector space, and depends on two parameters: imagine parameterising it by a vector on a sphere), and its position, depending on two more parameters, for a given direction (think of the possible translations of a given line). Thus the set of lines might be parameterised by four parameters, and more precisely one can show that it has dimension four. Even more interestingly, two parallel planes define for almost every line a unique pair of intersection points (one on each plane) which enables us to recover the line. This means lines are (almost all) parameterised by four coordinates, by means of rational functions (well, we still have to explain what is parameterised: for example, we could say that the slope, direction of the line and its position are rational functions of the coordinates on the two planes). The resulting parameterisation is somewhat bijective, but a few lines are missing (for example, lines parallel to the plane): however, we say the set of lines is a rational variety: which means the parameterisation is essentially bijective, and the missing elements can be obtained by taking limits.

The Plücker embedding

To avoid tiring case disjunctions, it is very nice to extend the theory to the set of lines in projective space. They can be defined by their Plücker coordinates : given a line in space, we choose two points, given by projective (a.k.a. barycentric) coordinates {M = [a_1:a_2:a_3:a_4]} and {N = [b_1:b_2:b_3:b_4]}. Then we define the Plücker coordinates of the line MN by the six numbers x_{ij} = (a_i b_j - a_j b_i). The fundamental properties of these coordinates is their invariance under changing the choice of points. Any other pair of points would be given by barycentres of M and N (with weights (\lambda,\mu) and (\nu,\pi)), giving new coordinates
(\lambda a_i + \mu b_i)(\nu a_j + \pi b_j) - (\lambda a_j + \mu b_j)(\nu a_i + \pi b_i)
= (\lambda \pi - \mu \nu)(a_i b_j - a_j b_i)
which are actually proportional to the old coordinates. These coordinates, as projective coordinates, are thus uniquely defined (and even allow to recover the line). The set of lines now appears as a subvariety of a projective space called the Grassmann variety of lines in 3-space.

(more…)

5 February 2009 at 11:52 am 1 comment

Les droites de l’espace et la grassmannienne

Le calcul de Schubert désigne un ensemble de techniques destinées à calculer les propriétés énumératives, ou numériques, d’objets communs de l’algèbre linéaire (voir notamment les excellents ouvrages de William Fulton à ce propos). L’exemple traditionnellement choisi, et probablement le plus simple, concerne l’ensemble des droites de l’espace (à 3 dimensions).

Une droite de l’espace est habituellement repérée par sa direction (qui est une droite vectorielle, et dépend donc de deux paramètres, et sa position, qui dépend de deux paramètres supplémentaires (à direction fixée). L’ensemble des droites peut donc être paramétré par quatre paramètres, on peut montrer qu’il est de dimension quatre. Plus intéressant encore, si on place dans l’espace deux plans parallèles, presque toutes les droites peuvent être décrites (de manière unique) par leurs points d’intersection avec ces plans : on obtient ainsi une description par 4 fractions rationnelles (à supposer qu’on sache ce qu’on est en train de paramétrer, ce qui sera plus clair dans une seconde). Ce paramétrage est à peu de chose près bijectif (il manque les droites un peu particulières) : on dit que l’ensemble des droites forme une variété rationnelle.

Le plongement de Plücker

Pour éviter de fastidieuses études de cas, on s’intéresse également aux droites de l’espace projectif : on peut les repérer par les coordonnées de Plücker. Étant donnée une droite de l’espace, considérons deux points sur cette droite de coordonnées projectives {M = [a_1:a_2:a_3:a_4]} et {N = [b_1:b_2:b_3:b_4]}. Les coordonnées de Plücker de la droite sont, par définition, les 6 nombres x_{ij} = (a_i b_j - a_j b_i). Si on avait choisi d’autres points (qui seraient donc des barycentres de M et N), on aurait obtenu des nombres de la forme

(\lambda a_i + \mu b_i)(\nu a_j + \pi b_j) - (\lambda a_j + \mu b_j)(\nu a_i + \pi b_i)
= (\lambda \pi - \mu \nu)(a_i b_j - a_j b_i)

qui sont en fait proportionnels à ceux calculés avec M et N. Les droites sont donc naturellement paramétrées par des coordonnées projectives et forment la variété grassmannienne des droites de l’espace.

(more…)

30 January 2009 at 8:33 am 1 comment

Extensions of sheaves and the local-global spectral sequence

GIven a topological space X, algebraic topologists would sometimes be interested in sheaves over this space. In most cases, these sheaves are sheaves of functions with some special property, or sheaves of modules over these rings. We could casually say thet the notion of sheaf is some mix of topology and algebra (more generally, categories), which allows to remember where are localized objects. For example, the set of continuous functions over a compact space can sometimes allow to recover an isomorphic space, but its mere normed algebra structure does not immediately say things like: “i am greater here than there”, “i am positive here and negative there”…

So a sheaf is not only determined by a set of fonctions (the commonly used term is section) defined over the whole space, but also by sections over open sets, and by the restriction maps between these various sets of sections. A sheaf has also a gluing theory : if we choose sections over open sets with equal restrictions on the intersections, they must glue to a section over the union of the open sets (if not, our object does not deserve to be a sheaf, so it is only a presheaf).

Virtually anything which can be restricted to open sets and defined locally defines a sheaf: continuous functions form a sheaf, but functions with ||f||_{\infty} = 1 do not usually form a sheaf (this property is not local). A sheaf of abelian groups is a sheaf of things which can be (locally) added and substracted, a sheaf of rings has sections which can be multiplied, and we can also define sheaves of modules over a sheaf of rings.

A morphism of sheaves f: F \to G is a map which is determined by the image of localized sections. In the case of abelian groups, the kernel sheaf is the sheaf of sections of F which are locally in the kernel of f, while the quotient sheaf (cokernel) is something looking like G where sections are identified if locally it should be so. A morphism is thus injective or surjective if locally it is so. Sheaves of abelian groups (or sheaves of modules over some sheaf of rings) form an abelian category, and it makes sense to speak of the extension group \mathrm{Ext}^1(F,G) for two such sheaves F and G. Suppose we are working with sheaves of modules (especially coherent sheaves) over a sheaf of rings \mathcal O_X. How should we compute this group ?

(more…)

10 January 2009 at 5:02 pm Leave a comment


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