Geometric invariant theory

In mathematics, geometric invariant theory (or GIT) is a method for constructing quotients by group actions in algebraic geometry, used to construct moduli spaces. It was developed by David Mumford in 1965, using ideas from the paper in classical invariant theory.
Geometric invariant theory studies an action of a group "G" on an algebraic variety (or scheme) "X" and provides techniques for forming the 'quotient' of "X" by "G" as a scheme with reasonable properties. One motivation was to construct moduli spaces in algebraic geometry as quotients of schemes parametrizing marked objects. In the 1970s and 1980s the theory developed interactions with symplectic geometry and equivariant topology, and was used to construct moduli spaces of objects in differential geometry, such as instantons and monopoles.
Background.
Invariant theory is concerned with a group action of a group "G" on an algebraic variety (or a scheme) "X". Classical invariant theory addresses the situation when "X" = "V" is a vector space and "G" is either a finite group, or one of the classical Lie groups that acts linearly on "V". This action induces a linear action of "G" on the space of polynomial functions "R"("V") on "V" by the formula
The polynomial invariants of the "G"-action on "V" are those polynomial functions "f" on "V" which are fixed under the 'change of variables' due to the action of the group, so that "g"·"f" = "f" for all "g" in "G". They form a commutative algebra "A" = "R"("V")"G", and this algebra is interpreted as the algebra of functions on the 'invariant theory quotient' "V" //"G" because any one of these functions gives the same value for all points that are equivalent (that is, formula_2 for all ). In the language of modern algebraic geometry,
Several difficulties emerge from this description. The first one, successfully tackled by Hilbert in the case of a general linear group, is to prove that the algebra "A" is finitely generated. This is necessary if one wanted the quotient to be an affine algebraic variety. Whether a similar fact holds for arbitrary groups "G" was the subject of Hilbert's fourteenth problem, and Nagata demonstrated that the answer was negative in general. On the other hand, in the course of development of representation theory in the first half of the twentieth century, a large class of groups for which the answer is positive was identified; these are called reductive groups and include all finite groups and all classical groups.
The finite generation of the algebra "A" is but the first step towards the complete description of "A", and progress in resolving this more delicate question was rather modest. The invariants had classically been described only in a restricted range of situations, and the complexity of this description beyond the first few cases held out little hope for full understanding of the algebras of invariants in general. Furthermore, it may happen that any polynomial invariant "f" takes the same value on a given pair of points "u" and "v" in "V", yet these points are in different orbits of the "G"-action. A simple example is provided by the multiplicative group C* of non-zero complex numbers that acts on an "n"-dimensional complex vector space C"n" by scalar multiplication. In this case, every polynomial invariant is a constant, but there are many different orbits of the action. The zero vector forms an orbit by itself, and the non-zero multiples of any non-zero vector form an orbit, so that non-zero orbits are parametrized by the points of the complex projective space CP"n"−1. If this happens (different orbits having the same function values), one says that "invariants do not separate the orbits", and the algebra "A" reflects the topological quotient space "X" /"G" rather imperfectly. Indeed, the latter space, with the quotient topology, is frequently non-separated (non-Hausdorff). (This is the case in our example – the null orbit is not open because any neighborhood of the null vector contains points in all other orbits, so in the quotient topology any neighborhood of the null orbit contains all other orbits.) In 1893 Hilbert formulated and proved a criterion for determining those orbits which are not separated from the zero orbit by invariant polynomials. Rather remarkably, unlike his earlier work in invariant theory, which led to the rapid development of abstract algebra, this result of Hilbert remained little known and little used for the next 70 years. Much of the development of invariant theory in the first half of the twentieth century concerned explicit computations with invariants, and at any rate, followed the logic of algebra rather than geometry.
Mumford's book.
Geometric invariant theory was founded and developed by Mumford in a monograph, first published in 1965, that applied ideas of nineteenth century invariant theory, including some results of Hilbert, to modern algebraic geometry questions. (The book was greatly expanded in two later editions, with extra appendices by Fogarty and Mumford, and a chapter on symplectic quotients by Kirwan.) The book uses both scheme theory and computational techniques available in examples. 
The abstract setting used is that of a group action on a scheme "X".
The simple-minded idea of an orbit space
i.e. the quotient space of "X" by the group action, runs into difficulties in algebraic geometry, for reasons that are explicable in abstract terms. There is in fact no general reason why equivalence relations should interact well with the (rather rigid) regular functions (polynomial functions), which are at the heart of algebraic geometry. The functions on the orbit space "G"\"X" that should be considered are those on "X" that are invariant under the action of "G". The direct approach can be made, by means of the function field of a variety (i.e. rational functions): take the "G"-invariant rational functions on it, as the function field of the quotient variety. Unfortunately this — the point of view of birational geometry — can only give a first approximation to the answer. As Mumford put it in the Preface to the book:
In Chapter 5 he isolates further the specific technical problem addressed, in a moduli problem of quite classical type — classify the big 'set' of all algebraic varieties subject only to being non-singular (and a requisite condition on polarization). The moduli are supposed to describe the parameter space. For example, for algebraic curves it has been known from the time of Riemann that there should be connected components of dimensions
according to the genus "g" =0, 1, 2, 3, 4, …, and the moduli are functions on each component. In the coarse moduli problem Mumford considers the obstructions to be:
It is the third point that motivated the whole theory. As Mumford puts it, if the first two difficulties are resolved
To deal with this he introduced a notion (in fact three) of stability. This enabled him to open up the previously treacherous area — much had been written, in particular by Francesco Severi, but the methods of the literature had limitations. The birational point of view can afford to be careless about subsets of codimension 1. To have a moduli space as a scheme is on one side a question about characterising schemes as representable functors (as the Grothendieck school would see it); but geometrically it is more like a compactification question, as the stability criteria revealed. The restriction to non-singular varieties will not lead to a compact space in any sense as moduli space: varieties can degenerate to having singularities. On the other hand, the points that would correspond to highly singular varieties are definitely too 'bad' to include in the answer. The correct middle ground, of points stable enough to be admitted, was isolated by Mumford's work. The concept was not entirely new, since certain aspects of it were to be found in David Hilbert's final ideas on invariant theory, before he moved on to other fields.
The book's Preface also enunciated the Mumford conjecture, later proved by William Haboush.
Stability.
If a reductive group "G" acts linearly on a vector space "V", then a non-zero point of "V" is called
There are equivalent ways to state these (this criterion is known as the Hilbert–Mumford criterion):
A point of the corresponding projective space of "V" is called unstable, semi-stable, or stable if it is the 
image of a point in "V" with the same property. "Unstable" is the opposite of "semistable" (not "stable"). The unstable points form a Zariski closed set of projective space, while the semistable and stable points both form Zariski open sets (possibly empty). These definitions are from and are not equivalent to the ones in the first edition of Mumford's book.
Many moduli spaces can be constructed as the quotients of the space of stable points of some subset of projective space by some group action. These spaces can often be compactified by adding certain equivalence classes of semistable points. Different stable orbits correspond to different points in the quotient, but two different semistable orbits may correspond to the same point in the quotient if their closures intersect. 
Example: 
A stable curve is a reduced connected curve of genus ≥2 such that its only singularities are ordinary double points and every non-singular rational component meets the other components in at least 3 points. The moduli space of stable curves of genus "g" is the quotient of a subset of the Hilbert scheme of curves in P5"g"-6 with Hilbert polynomial (6"n"−1)("g"−1) by the group PGL5"g"−5.
Example:
A vector bundle "W" over an algebraic curve (or over a Riemann surface) is a stable vector bundle 
if and only if
for all proper non-zero subbundles "V" of "W" 
and is semistable if this condition holds with < replaced by ≤.