Over a field of characteristic zero, the theory is closely related to that of a differential graded scheme.2 By definition, a differential graded scheme is obtained by gluing affine differential graded schemes, with respect to étale topology.3 It was introduced by Maxim Kontsevich4 "as the first approach to derived algebraic geometry."5 and was developed further by Mikhail Kapranov and Ionut Ciocan-Fontanine.
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 f 1 , … , f k ∈ C [ x 1 , … , x n ] = R {\displaystyle f_{1},\ldots ,f_{k}\in \mathbb {C} [x_{1},\ldots ,x_{n}]=R} , then we can get a derived scheme
where
is the étale spectrum. Since we can construct a resolution
the derived ring R / ( f 1 ) ⊗ R L ⋯ ⊗ R L R / ( f k ) {\displaystyle R/(f_{1})\otimes _{R}^{\mathbf {L} }\cdots \otimes _{R}^{\mathbf {L} }R/(f_{k})} , a derived tensor product, is the koszul complex K R ( f 1 , … , f k ) {\displaystyle K_{R}(f_{1},\ldots ,f_{k})} . The truncation of this derived scheme to amplitude [ − 1 , 0 ] {\displaystyle [-1,0]} provides a classical model motivating derived algebraic geometry. Notice that if we have a projective scheme
where deg ( f i ) = d i {\displaystyle \deg(f_{i})=d_{i}} we can construct the derived scheme ( P n , E ∙ , ( f 1 , … , f k ) ) {\displaystyle (\mathbb {P} ^{n},{\mathcal {E}}^{\bullet },(f_{1},\ldots ,f_{k}))} where
with amplitude [ − 1 , 0 ] {\displaystyle [-1,0]}
Let ( A ∙ , d ) {\displaystyle (A_{\bullet },d)} be a fixed differential graded algebra defined over a field of characteristic 0 {\displaystyle 0} . Then a A ∙ {\displaystyle A_{\bullet }} -differential graded algebra ( R ∙ , d R ) {\displaystyle (R_{\bullet },d_{R})} is called semi-free if the following conditions hold:
It turns out that every A ∙ {\displaystyle A_{\bullet }} differential graded algebra admits a surjective quasi-isomorphism from a semi-free ( A ∙ , d ) {\displaystyle (A_{\bullet },d)} differential graded algebra, called a semi-free resolution. These are unique up to homotopy equivalence in a suitable model category. The (relative) cotangent complex of an ( A ∙ , d ) {\displaystyle (A_{\bullet },d)} -differential graded algebra ( B ∙ , d B ) {\displaystyle (B_{\bullet },d_{B})} can be constructed using a semi-free resolution ( R ∙ , d R ) → ( B ∙ , d B ) {\displaystyle (R_{\bullet },d_{R})\to (B_{\bullet },d_{B})} : it is defined as
Many examples can be constructed by taking the algebra B {\displaystyle B} representing a variety over a field of characteristic 0, finding a presentation of R {\displaystyle R} as a quotient of a polynomial algebra and taking the Koszul complex associated to this presentation. The Koszul complex acts as a semi-free resolution of the differential graded algebra ( B ∙ , 0 ) {\displaystyle (B_{\bullet },0)} where B ∙ {\displaystyle B_{\bullet }} is the graded algebra with the non-trivial graded piece in degree 0.
The cotangent complex of a hypersurface X = V ( f ) ⊂ A C n {\displaystyle X=\mathbb {V} (f)\subset \mathbb {A} _{\mathbb {C} }^{n}} can easily be computed: since we have the dga K R ( f ) {\displaystyle K_{R}(f)} representing the derived enhancement of X {\displaystyle X} , we can compute the cotangent complex as
where Φ ( g d s ) = g ⋅ d f {\displaystyle \Phi (gds)=g\cdot df} and d {\displaystyle d} is the usual universal derivation. If we take a complete intersection, then the koszul complex
is quasi-isomorphic to the complex
This implies we can construct the cotangent complex of the derived ring R ∙ {\displaystyle R^{\bullet }} as the tensor product of the cotangent complex above for each f i {\displaystyle f_{i}} .
Please note that the cotangent complex in the context of derived geometry differs from the cotangent complex of classical schemes. Namely, if there was a singularity in the hypersurface defined by f {\displaystyle f} then the cotangent complex would have infinite amplitude. These observations provide motivation for the hidden smoothness philosophy of derived geometry since we are now working with a complex of finite length.
Given a polynomial function f : A n → A m , {\displaystyle f:\mathbb {A} ^{n}\to \mathbb {A} ^{m},} then consider the (homotopy) pullback diagram
where the bottom arrow is the inclusion of a point at the origin. Then, the derived scheme Z {\displaystyle Z} has tangent complex at x ∈ Z {\displaystyle x\in Z} is given by the morphism
where the complex is of amplitude [ − 1 , 0 ] {\displaystyle [-1,0]} . Notice that the tangent space can be recovered using H 0 {\displaystyle H^{0}} and the H − 1 {\displaystyle H^{-1}} measures how far away x ∈ Z {\displaystyle x\in Z} is from being a smooth point.
Given a stack [ X / G ] {\displaystyle [X/G]} there is a nice description for the tangent complex:
If the morphism is not injective, the H − 1 {\displaystyle H^{-1}} measures again how singular the space is. In addition, the Euler characteristic of this complex yields the correct (virtual) dimension of the quotient stack. In particular, if we look at the moduli stack of principal G {\displaystyle G} -bundles, then the tangent complex is just g [ + 1 ] {\displaystyle {\mathfrak {g}}[+1]} .
Derived schemes can be used for analyzing topological properties of affine varieties. For example, consider a smooth affine variety M ⊂ A n {\displaystyle M\subset \mathbb {A} ^{n}} . If we take a regular function f : M → C {\displaystyle f:M\to \mathbb {C} } and consider the section of Ω M {\displaystyle \Omega _{M}}
Then, we can take the derived pullback diagram
where 0 {\displaystyle 0} is the zero section, constructing a derived critical locus of the regular function f {\displaystyle f} .
Consider the affine variety
and the regular function given by f ( x , y ) = x 2 + y 3 {\displaystyle f(x,y)=x^{2}+y^{3}} . Then,
where we treat the last two coordinates as d x , d y {\displaystyle dx,dy} . The derived critical locus is then the derived scheme
Note that since the left term in the derived intersection is a complete intersection, we can compute a complex representing the derived ring as
where K d x , d y ∙ ( C [ x , y , d x , d y ] ) {\displaystyle K_{dx,dy}^{\bullet }(\mathbb {C} [x,y,dx,dy])} is the koszul complex.
Consider a smooth function f : M → C {\displaystyle f:M\to \mathbb {C} } where M {\displaystyle M} is smooth. The derived enhancement of Crit ( f ) {\displaystyle \operatorname {Crit} (f)} , the derived critical locus, is given by the differential graded scheme ( M , A ∙ , Q ) {\displaystyle (M,{\mathcal {A}}^{\bullet },Q)} where the underlying graded ring are the polyvector fields
and the differential Q {\displaystyle Q} is defined by contraction by d f {\displaystyle df} .
For example, if
we have the complex
representing the derived enhancement of Crit ( f ) {\displaystyle \operatorname {Crit} (f)} .
also often called E ∞ {\displaystyle E_{\infty }} -ring spectra ↩
section 1.2 of Eugster, J.; Pridham, J.P. (2021-10-25). "An introduction to derived (algebraic) geometry". arXiv:2109.14594 [math.AG]. /wiki/ArXiv_(identifier) ↩
Behrend, Kai (2002-12-16). "Differential Graded Schemes I: Perfect Resolving Algebras". arXiv:math/0212225. /wiki/ArXiv_(identifier) ↩
Kontsevich, M. (1994-05-05). "Enumeration of rational curves via torus actions". arXiv:hep-th/9405035. /wiki/ArXiv_(identifier) ↩
"Dg-scheme". http://ncatlab.org/nlab/show/dg-scheme ↩