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4.5. Tensor product and internal Hom\operatorname{Hom}\nolimits

Let us give two applications of the construction of Β§4.3. Let (𝒱1,E1,Ο„1)({\mathcal{V}}_{1},E_{1},\tau_{1}) and (𝒱2,E2,Ο„2)({\mathcal{V}}_{2},E_{2},\tau_{2}) be idempotent-complete strongly pretriangulated 22-representations.

We view 𝒱1βŠ—π’±2{\mathcal{V}}_{1}\otimes{\mathcal{V}}_{2} as endowed with two strictly commuting actions of 𝒰{\mathcal{U}} given by (E1βŠ—1,Ο„1βŠ—1)(E_{1}\otimes 1,\tau_{1}\otimes 1) and (1βŠ—E2,1βŠ—Ο„2)(1\otimes E_{2},1\otimes\tau_{2}): the isomorphism Οƒ:(1βŠ—E2)∘(E1βŠ—1)β†’βˆΌ(E1βŠ—1)∘(1βŠ—E2)\sigma:(1\otimes E_{2})\circ(E_{1}\otimes 1)\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}(E_{1}\otimes 1)\circ(1\otimes E_{2}) is the identity.

We define the tensor product 22-representation

𝒱1βŠ—β—‹π’±2=Δσ(𝒱1βŠ—π’±2).{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}=\Delta_{\sigma}({\mathcal{V}}_{1}\otimes{\mathcal{V}}_{2}).

Given (Ξ¦i,Ο†i):𝒱i→𝒱iβ€²(\Phi_{i},\varphi_{i}):{\mathcal{V}}_{i}\to{\mathcal{V}}^{\prime}_{i} a morphism of 22-representations for i∈{1,2}i\in\{1,2\}, Proposition 4.3.9 provides a morphism of 22-representations 𝒱1βŠ—β—‹π’±2→𝒱′1βŠ—β—‹π’±β€²2{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}\to{\mathcal{V}}^{\prime}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}^{\prime}_{2}.

Given 𝒱1{\mathcal{V}}_{1}, 𝒱2{\mathcal{V}}_{2} and 𝒱3{\mathcal{V}}_{3} 22-representations, Proposition 4.3.12 provides an isomorphism

(𝒱1βŠ—β—‹π’±2)βŠ—β—‹π’±3β†’βˆΌπ’±1βŠ—β—‹(𝒱2βŠ—β—‹π’±3)({\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{2}){\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{3}\mathrel{\mathop{\kern 0.0pt\to}\limits^{\sim}}{\mathcal{V}}_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}({\mathcal{V}}_{2}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}{\mathcal{V}}_{3})

that commutes with forgetful functors Ο‰\omega.

Since the forgetful functors Ο‰\omega are faithful, we deduce that idempotent-complete strongly pretriangulated 22-representations form a monoidal 22-category.

Consider now Hom⁑(𝒱1,𝒱2)\operatorname{Hom}\nolimits({\mathcal{V}}_{1},{\mathcal{V}}_{2}). It is endowed with two strictly commuting structures of 22-representations: the first one is given by ((Ξ¦β†¦Ξ¦βˆ˜E1),Φ​τ1)((\Phi\mapsto\Phi\circ E_{1}),\Phi\tau_{1}) and the second one by ((Φ↦E2∘Φ),Ο„2​Φ)((\Phi\mapsto E_{2}\circ\Phi),\tau_{2}\Phi). The isomorphism Οƒ\sigma is the identity.

We define the internal Hom\operatorname{Hom}\nolimits 22-representation

ℋ​ℋ​o​m​(𝒱1,𝒱2)=Δ​Hom⁑(𝒱1,𝒱2).{\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2})=\Delta\operatorname{Hom}\nolimits({\mathcal{V}}_{1},{\mathcal{V}}_{2}).

The category ℋ​ℋ​o​m​(𝒱1,𝒱2){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) has objects pairs (Ξ¦,Ο€)(\Phi,\pi) where Ξ¦:𝒱1→𝒱2Β―i\Phi:{\mathcal{V}}_{1}\to\overline{{\mathcal{V}}_{2}}^{i} is a differential functor and Ο€:E2​Φ→Φ​E1\pi:E_{2}\Phi\to\Phi E_{1} is a closed natural transformation of functors such that

Ο„1β€‹Ξ¦βˆ˜Ο€β€‹E1∘E2​π=π​E1∘E2β€‹Ο€βˆ˜Ο„2​Φ:E22​Φ→Φ​E12.\tau_{1}\Phi\circ\pi E_{1}\circ E_{2}\pi=\pi E_{1}\circ E_{2}\pi\circ\tau_{2}\Phi:E_{2}^{2}\Phi\to\Phi E_{1}^{2}.

Note that Hom𝒰⁑(𝒱1,𝒱2)\operatorname{Hom}\nolimits_{\mathcal{U}}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) is the full subcategory of ℋ​ℋ​o​m​(𝒱1,𝒱2){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2}) with objects pairs (Ξ¦,Ο€)(\Phi,\pi) where Ξ¦\Phi takes values in 𝒱2{\mathcal{V}}_{2} and Ο€\pi is invertible.

Given (Ξ¦1,Ο†1):𝒱1′→𝒱1(\Phi_{1},\varphi_{1}):{\mathcal{V}}^{\prime}_{1}\to{\mathcal{V}}_{1} and (Ξ¦2,Ο†2):𝒱2→𝒱2β€²(\Phi_{2},\varphi_{2}):{\mathcal{V}}_{2}\to{\mathcal{V}}^{\prime}_{2} two morphisms of 22-representations, Proposition 4.3.9 provides a morphism of 22-representations ℋ​ℋ​o​m​(𝒱1,𝒱2)→ℋ​ℋ​o​m​(𝒱1β€²,𝒱2β€²){\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}_{1},{\mathcal{V}}_{2})\to{\mathcal{H}}\hskip-5.69046pt{\mathcal{H}}{om}({\mathcal{V}}^{\prime}_{1},{\mathcal{V}}^{\prime}_{2}).

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Andrew Manion, Raphael Rouquier

Original source: arXiv:2009.09627v2