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Home > Zariski tangent space


 

In algebraic geometry, the Zariski tangent space is a construction that defines a tangent space, at a point P on an algebraic variety V (and more generally). It does not use differential calculus, being based directly on abstract algebra, and in the most concrete cases just the theory of a system of linear equations.

For example, suppose given a plane curve C defined by a polynomial equation

F(X,Y) = 0

and take P to be the origin (0,0). When F is considered only in terms of its first-degree terms, we get a 'linearised' equation reading

L(X,Y) = 0

in which all terms XaYb have been discarded if

a + b > 1.

We have two cases: L may be 0, or it may be the equation of a line. In the first case the (Zariski) tangent space to C at (0,0) is the whole plane, considered as a two-dimensional affine space. In the second case, the tangent space is that line, considered as affine space. (The question of the origin comes up, when we take P as a general point on C; it is better to say 'affine space' and then note that P is a natural origin, rather than insist directly that it is a vector space.)

It is easy to see that over the real field we can obtain L in terms of the first partial derivatives of F. When those both are 0 at P, we have a singular point ( double point , cusp or something more complicated). The general definition is that singular points of C are the cases when the tangent space has dimension 2.

The definition given generalises directly to higher dimensions, in which case a number of equations may be involved in defining a variety V. The non-linear terms are dropped from all of them, giving a system of linear equations that define the tangent space. The definition of singular point is then that the dimension of the tangent space is the dimension of V.

For more abstract theory, one notes that for any commutative local ring R, with maximal ideal M, there is the definition

M/M2

of an R-module, in terms of which the previous definitions can be recovered. For R coming from geometry over a fieldIn abstract algebra, a field is an algebraic structure in which the operations of addition, subtraction, multiplication, and division (except division by zero) may be performed and the associative, commutative, and distributive rules hold, which are famil K, this will be a vector space over K. It therefore serves as an abstract analogue, and is also called the Zariski tangent spaceIn algebraic geometry, the Zariski tangent space is a construction that defines a tangent space, at a point P on an algebraic variety V (and more generally). It does not use differential calculus, being based directly on abstract algebra, and in the most. It has an interpretation in terms of homomorphismThis word should not be confused with homeomorphism. In abstract algebra, a homomorphism is a map from one algebraic structure to another of the same type that preserves all the relevant structure. Some authors use the word homomorphism in a larger contexs to the dual numbersA variety of dualities in mathematics are listed at duality (mathematics). For an article about the dual grammatical number found in some languages see dual grammatical number. In abstract algebra, the dual numbers are a particular two- dimensional commut for K,

K[t]/[t2]

which (thinking about affine schemes) allows one to speak in geometric terms, talking about tangent vectors.

Algebraic geometry Differential algebra

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