Abstract

Triangulated derived categories are considered which establish a commutative scheme (triangle) for determine or compute a hypercohomology of motives for the obtaining of solutions of the field equations. The determination of this hypercohomology arises of the derived category $\textup{DM}_{\textup {gm}}(k)$,  which is of the motivic objects whose image is under $\textup {Spec}(k)$  that is to say, an equivalence of the underlying triangulated tensor categories, compatible with respective functors on $\textup{Sm}_{k}^{\textup{Op}}$. The geometrical motives will be risked with the moduli stack to holomorphic bundles. Likewise, is analysed the special case where complexes $C=\mathbb{Q}(q)$,  are obtained when cohomology groups of the isomorphism $H_{\acute{e}t}^{p}(X,F_{\acute{e}t})\cong (X,F_{Nis})$,   can be vanished for  $p>\textup{dim}(Y)$.  We observe also the Beilinson-Soul$\acute{e}$ vanishing  conjectures where we have the vanishing $H^{p}(F,\mathbb{Q}(q))=0, \ \ \textup{if} \ \ p\leq0,$ and $q>0$,   which confirms the before established. Then survives a hypercohomology $\mathbb{H}^{q}(X,\mathbb{Q})$. Then its objects are in $\textup{Spec(Sm}_{k})$.  Likewise, for the complex Riemannian manifold the integrals of this hypercohomology are those whose functors image will be in $\textup{Spec}_{H}\textup{SymT(OP}_{L_{G}}(D))$, which is the variety of opers on the formal disk $D$, or neighborhood of all point in a surface $\Sigma$.  Likewise, will be proved that $\mathrm{H}^{\vee}$,  has the decomposing in components as hyper-cohomology groups which can be characterized as H- states in Vec$_\mathbb{C}$, for field equations $d \textup{da}=0$,  on the general linear group with $k=\mathbb{C}$.  A physics re-interpretation of the superposing, to the dual of the spectrum $\mathrm{H}^{\vee}$,  whose hypercohomology is a quantized version of the cohomology space $H^{q}(Bun_{G},\mathcal{D}^{s})=\mathbb{H}^{q}_{G[[z]]}(\mathrm{G},(\land^{\bullet}[\Sigma^{0}]\otimes \mathbb{V}_{critical},\partial))$ is the corresponding deformed derived category for densities $\mathrm{h} \in \mathrm{H}$, in quantum field theory.

Highlights

  • We have some previous results of PST(k), which is the Universe of all applications, transformations and mappings in Sch, with symmetrizations and triangulations from tensor product structure ⊗tRr, [Mac Lane, 1971] to give the category corresponding of the schemes space on k : Schk = {T ∈ Sch | Ztr(T )(X Y) = HomCork (X Y, T )}, (1)since PST(k), is an additive category

  • Triangulated derived categories are considered which establish a commutative scheme for determine or compute a hypercohomology of motives for the obtaining of solutions of the field equations. The determination of this hypercohomology arises of the derived category DMgm(k), which is of the motivic objects whose image is under Spec(k) that is to say, an equivalence of the underlying triangulated tensor categories, compatible with respective functors on SmOk p

  • For the complex Riemannian manifold the integrals of this hypercohomology are those whose functors image will be in SpecHSymT(OPLG (D)), which is the variety of opers on the formal disk D, or neighborhood of all point in a surface Σ

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Summary

Introduction

If A, is an Abelian group A ⊗ Ztr(Y), for any scheme Y, on k, is a sheaf in the topology of Zariski, and A ⊗ C∗Ztr(Y), is a complex of sheaves. The motivic cohomology groups Hp,q(X, Z), are defined to be the hypercohomology of the motivic complexes Z(q), with respect to the Zariski topology. For the appliying of an adequate pre-sheaves motivic cohomology can be identified the transformation images TotC∗(K), which is a full subcategory of D−(Shet(Cor(k, R))), consisting of complexes with homotopy invariant cohomology sheaves. This space is a motivic Galois group on DMT(k), which is a full subcategory of the Tate category of motives TM(k), its hypercohomology is a corresponding to the cosmic Galois group, and corresponds to the solution for the field equations

Some on Derived Categories in Field Theory
Main Result
Motivic Hypercohomology Solutions to Quantum Field Theory
Conclusions
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