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Derived scheme

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From the functor of points point-of-view, a derived scheme is a sheaf X on the category of simplicial commutative rings which admits an open affine covering {Spec(Ai)→X}.

From the locally ringed space point-of-view, a derived scheme is a pair (X,O) consisting of a topological space X and a sheaf O either of simplicial commutative rings or of commutative ring spectra on X such that (1) the pair (X,π0O) is a scheme and (2) πkO is a quasi-coherent π0O-module.

A derived stack is a stacky generalization of a derived scheme.

Differential graded scheme

Over a field of characteristic zero, the theory is closely related to that of a differential graded scheme. By definition, a differential graded scheme is obtained by gluing affine differential graded schemes, with respect to étale topology. It was introduced by Maxim Kontsevich "as the first approach to derived algebraic geometry" and was developed further by Mikhail Kapranov and Ionut Ciocan-Fontanine.

Connection with differential graded rings and examples

Just as affine algebraic geometry is equivalent (in categorical sense) to the theory of commutative rings (commonly called commutative algebra), affine derived algebraic geometry over characteristic zero is equivalent to the theory of commutative differential graded rings. One of the main example of derived schemes comes from the derived intersection of subschemes of a scheme, giving the Koszul complex. For example, let f1,…,fk∈C[x1,…,xn]=R, then we can get a derived scheme

(X,O∙)=RSpec(R/(f1)⊗RL⋯⊗RLR/(fk))

where

RSpec:(dgaC)op→DerSch

is the étale spectrum. Since we can construct a resolution

0→R→⋅fiR→0↓↓0→0→R/(fi)→0

the derived ring R/(f1)⊗RL⋯⊗RLR/(fk), a derived tensor product, is the Koszul complex KR(f1,…,fk). The truncation of this derived scheme to amplitude [−1,0] provides a classical model motivating derived algebraic geometry. Notice that if we have a projective scheme

Proj⁡(Z[x0,…,xn](f1,…,fk))

where deg⁡(fi)=di we can construct the derived scheme (Pn,E∙,(f1,…,fk)) where

E∙=[O(−d1)⊕⋯⊕O(−dk)→(⋅f1,…,⋅fk)O]

with amplitude [−1,0].

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