TheoremComplete

Derived Functors - Applications

Derived functors have wide-ranging applications across algebraic geometry, topology, and representation theory.

Theorem4.16Čech-to-Derived Spectral Sequence

For a sheaf F\mathcal{F} on a topological space XX with an open cover U={Ui}\mathcal{U} = \{U_i\}, there is a spectral sequence: E2p,q=Hˇp(U,Hq(F))⇒Hp+q(X,F)E_2^{p,q} = \check{H}^p(\mathcal{U}, \mathcal{H}^q(\mathcal{F})) \Rightarrow H^{p+q}(X, \mathcal{F})

where HΛ‡p\check{H}^p is Čech cohomology and Hp+qH^{p+q} is sheaf cohomology.

Remark

This spectral sequence is fundamental in algebraic geometry for computing sheaf cohomology using Čech techniques, which are often more accessible for explicit calculations.

Theorem4.17Local-to-Global Ext

For a Noetherian scheme XX and coherent sheaves F,G\mathcal{F}, \mathcal{G} on XX: Exti(F,G)=sheafificationΒ ofΒ (U↦ExtOX(U)i(F∣U,G∣U))\mathcal{E}xt^i(\mathcal{F}, \mathcal{G}) = \text{sheafification of } (U \mapsto \text{Ext}^i_{\mathcal{O}_X(U)}(\mathcal{F}|_U, \mathcal{G}|_U))

These sheaves measure local extension problems and relate to global Ext via spectral sequences.

ExampleSerre Duality

For a smooth projective variety XX of dimension nn over a field kk, there is a functorial isomorphism: Hi(X,F)βˆ¨β‰…Hnβˆ’i(X,Fβˆ¨βŠ—Ο‰X)H^i(X, \mathcal{F})^\vee \cong H^{n-i}(X, \mathcal{F}^\vee \otimes \omega_X)

where Ο‰X\omega_X is the canonical sheaf. This uses derived functors extensively in its proof.

Theorem4.18Leray Spectral Sequence

For a continuous map f:Xβ†’Yf: X \to Y and sheaf F\mathcal{F} on XX, there is a spectral sequence: E2p,q=Hp(Y,Rqfβˆ—F)β‡’Hp+q(X,F)E_2^{p,q} = H^p(Y, R^qf_*\mathcal{F}) \Rightarrow H^{p+q}(X, \mathcal{F})

where Rqfβˆ—R^qf_* is the right derived functor of the direct image fβˆ—f_*.

Remark

The Leray spectral sequence is essential for computing cohomology of fibrations and understanding how cohomology behaves under continuous maps.

ExampleHochschild Cohomology

For an associative kk-algebra AA, the Hochschild cohomology is: HHn(A,M)=ExtAen(A,M)HH^n(A, M) = \text{Ext}^n_{A^e}(A, M)

where Ae=AβŠ—kAopA^e = A \otimes_k A^{op} is the enveloping algebra and MM is an AA-bimodule. This measures the deformation theory of AA.

Theorem4.19KΓΌnneth Formula for Ext

Over a field kk, for finite-dimensional vector spaces: Extk[x]n(M,N)≅⨁i+j=nExtk[x]i(M,k)βŠ—kExtk[x]j(k,N)\text{Ext}^n_{k[x]}(M, N) \cong \bigoplus_{i+j=n} \text{Ext}^i_{k[x]}(M, k) \otimes_k \text{Ext}^j_{k[x]}(k, N)

This generalizes to more general rings with appropriate flatness conditions.