5.3.4. Tensor product case
Let A 1 A_{1} and A 2 A_{2} be two differential algebras equipped with
structures of 2 2 -representations ( E i , τ i ) (E_{i},\tau_{i}) , i = 1 , 2 i=1,2 .
Let B = A 1 ⊗ A 2 B=A_{1}\otimes A_{2} . It is endowed with commuting
2 2 -representations ( E 1 ⊗ A 2 , τ 1 ⊗ 1 ) (E_{1}\otimes A_{2},\tau_{1}\otimes 1) and
( A 1 ⊗ E 2 , 1 ⊗ τ 2 ) (A_{1}\otimes E_{2},1\otimes\tau_{2}) : the isomorphism σ \sigma is
induced by the swap map E 2 ⊗ E 1 → ∼ E 1 ⊗ E 2 , a 2 ⊗ a 1 ↦ a 1 ⊗ a 2 E_{2}\otimes E_{1}\xrightarrow{\sim}E_{1}\otimes E_{2},\ a_{2}\otimes a_{1}\mapsto a_{1}\otimes a_{2} .
The tensor product identifies ( A 1 − diff ) ⊗ ( A 2 − diff ) (A_{1}\operatorname{\!-diff}\nolimits)\otimes(A_{2}\operatorname{\!-diff}\nolimits) with a full
subcategory of B − diff B\operatorname{\!-diff}\nolimits .
Assume E 1 E_{1} is right finite. The map λ \lambda is an isomorphism.
We put A 1 ⊗ ○ A 2 = Δ λ ′ ( B ) A_{1}{\hskip 1.9919pt\otimes\hskip-10.81218pt\bigcirc}A_{2}=\Delta^{\prime}_{\lambda}(B) . It is
the quotient
of the tensor algebra T A 1 ⊗ A 2 ( E 1 ∨ ⊗ E 2 ) T_{A_{1}\otimes A_{2}}(E_{1}^{\vee}\otimes E_{2}) by
the ideal generated by p τ 2 ( q ) − τ 1 ( p ) q p\tau_{2}(q)-\tau_{1}(p)q for p ∈ ( E 1 ∨ ) ⊗ 2 p\in(E_{1}^{\vee})^{\otimes 2}
and q ∈ ( E 2 ) ⊗ 2 q\in(E_{2})^{\otimes 2} .
The underlying differential module is
A = ⨁ i ≥ 0 ( E 1 ∨ ) i ⊗ H i E 2 i . A=\bigoplus_{i\geq 0}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}^{i}.
The multiplication is defined by
( ( E 1 i ) ∨ ⊗ H i E 2 i ) ⊗ ( ( E 1 j ) ∨ ⊗ H j E 2 j ) → ( E 1 i + j ) ∨ ⊗ H i + j E 2 i + j , ( a 1 ⊗ a 2 ) ⊗ ( b 1 ⊗ b 2 ) ↦ ( a 1 b 1 ) ⊗ ( a 2 b 2 ) . \bigl((E_{1}^{i})^{\vee}\otimes_{H_{i}}E_{2}^{i}\bigr)\otimes\bigl((E_{1}^{j})^{\vee}\otimes_{H_{j}}E_{2}^{j}\bigr)\to(E_{1}^{i+j})^{\vee}\otimes_{H_{i+j}}E_{2}^{i+j},\ (a_{1}\otimes a_{2})\otimes(b_{1}\otimes b_{2})\mapsto(a_{1}b_{1})\otimes(a_{2}b_{2}).
We have
E = ( ⨁ i ≥ 0 ( E 1 ∨ ) i ⊗ H i E 2 E 2 i ) ⊕ ( ⨁ i ≥ 0 E 1 ( E 1 ∨ ) i ⊗ H i E 2 i ) η 1 ⊗ 1 . E={\lx@xy@svg{\hbox{\raise 2.5pt\hbox{\kern 106.07784pt\hbox{{\hbox{\kern-106.07784pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.50006pt\hbox{$\textstyle{\bigl(\bigoplus_{i\geq 0}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}E_{2}^{i}\bigr)\oplus\bigl(\bigoplus_{i\geq 0}E_{1}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}^{i}\bigr)}$}}}}}\ignorespaces{}{}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{}{}{{}}{}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces{}{}{}{{}{}}\ignorespaces\ignorespaces{\hbox{\kern-17.8201pt\raise 23.31715pt\hbox{{}\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\hbox{\hbox{\kern 0.0pt\raise-1.57501pt\hbox{$\scriptstyle{\eta_{1}\otimes 1}$}}}\kern 3.0pt}}}}}}\ignorespaces{}{}{}{{}}{\hbox{\kern 68.28625pt\raise 11.38104pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}\ignorespaces\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{}{{}{}{}\lx@xy@spline@}{}}}}\ignorespaces{}\ignorespaces\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{{}{}{}{{}{}{}}{}}}}\ignorespaces{}\ignorespaces}}}}}.
The right action of A A on E E is given by right multiplication, while the left action of
E 1 ∨ ⊗ E 2 E_{1}^{\vee}\otimes E_{2} on A 1 ⊗ E 2 ⊕ E 1 ⊗ A 2 ⊂ E A_{1}\otimes E_{2}\oplus E_{1}\otimes A_{2}\subset E is given by
( E 1 ∨ ⊗ E 2 ) ⊗ A 1 ⊗ A 2 ( A 1 ⊗ E 2 ) → ∼ can E 1 ∨ ⊗ E 2 2 → 1 ⊗ τ 2 E 1 ∨ ⊗ E 2 2 (E_{1}^{\vee}\otimes E_{2})\otimes_{A_{1}\otimes A_{2}}(A_{1}\otimes E_{2})\xrightarrow[\sim]{{\mathrm{can}}}E_{1}^{\vee}\otimes E_{2}^{2}\xrightarrow{1\otimes\tau_{2}}E_{1}^{\vee}\otimes E_{2}^{2}
( E 1 ∨ ⊗ E 2 ) ⊗ A 1 ⊗ A 2 ( E 1 ⊗ A 2 ) → ∼ can E 1 ∨ E 1 ⊗ E 2 → ( ε 1 , ρ 1 ) A 1 ⊗ E 2 ⊕ E 1 E 1 ∨ ⊗ E 2 . (E_{1}^{\vee}\otimes E_{2})\otimes_{A_{1}\otimes A_{2}}(E_{1}\otimes A_{2})\xrightarrow[\sim]{{\mathrm{can}}}E_{1}^{\vee}E_{1}\otimes E_{2}\xrightarrow{(\varepsilon_{1},\rho_{1})}A_{1}\otimes E_{2}\oplus E_{1}E_{1}^{\vee}\otimes E_{2}.
We have
E 2 = ( ⨁ ( E 1 ∨ ) i ⊗ H i E 2 2 E 2 i ) ⊕ ( ⨁ E 1 ( E 1 ∨ ) i ⊗ H i E 2 E 2 i ) ⊕ ( ⨁ E 1 ( E 1 ∨ ) i ⊗ H i E 2 E 2 i ) ⊕ ( ⨁ E 1 2 ( E 1 ∨ ) i ⊗ H i E 2 i ) η 1 ( E 1 ∨ ) i ⊗ E 2 2 + i η 1 ( E 1 ∨ ) i ⊗ τ 2 E 2 i E 1 η 1 ( E 1 ∨ ) i ⊗ E 2 1 + i ( E 1 ρ 1 ∘ η 1 E 1 ) ( E 1 ∨ ) i ⊗ E 2 1 + i 1 . 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The endomorphism τ \tau of E 2 E^{2} is given on
( ( E 1 ∨ ) i ⊗ H i E 2 2 E 2 i ) ⊕ ( E 1 ( E 1 ∨ ) i ⊗ H i E 2 E 2 i ) ⊕ ( E 1 ( E 1 ∨ ) i ⊗ H i E 2 E 2 i ) ⊕ ( E 1 2 ( E 1 ∨ ) i ⊗ H i E 2 i ) \bigl((E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}^{2}E_{2}^{i}\bigr)\oplus\bigl(E_{1}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}E_{2}^{i}\bigr)\oplus\bigl(E_{1}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}E_{2}^{i}\bigr)\oplus\bigl(E_{1}^{2}(E_{1}^{\vee})^{i}\otimes_{H_{i}}E_{2}^{i}\bigr)
by
τ = ( 1 ⊗ τ 2 E 2 i 0 0 0 0 0 1 0 0 0 0 0 0 0 0 τ 1 ( E 1 ∨ ) i ⊗ 1 ) . \tau=\left(\begin{matrix}1\otimes\tau_{2}E_{2}^{i}&0&0&0\\
0&0&1&0\\
0&0&0&0\\
0&0&0&\tau_{1}(E_{1}^{\vee})^{i}\otimes 1\end{matrix}\right).
This construction provides the differential 2 2 -category of right finite 2 2 -representations
on differential algebras with a monoidal structure.