<p>We investigate the <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\hbox {C}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>C</mtext> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-algebra inclusions <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(B \subset A \mathop {\rtimes _{\textrm{r}}}\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>B</mi> <mo>⊂</mo> <mi>A</mi> <msub> <mo>⋊</mo> <mtext>r</mtext> </msub> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation> arising from inclusions <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(B \subset A\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>B</mi> <mo>⊂</mo> <mi>A</mi> </mrow> </math></EquationSource> </InlineEquation> of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>-<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\hbox {C}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>C</mtext> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-algebras. The main result shows that, when <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(B \subset A\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>B</mi> <mo>⊂</mo> <mi>A</mi> </mrow> </math></EquationSource> </InlineEquation> is <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\hbox {C}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>C</mtext> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-irreducible in the sense of Rørdam, and is centrally <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Γ</mi> </math></EquationSource> </InlineEquation>-free in the sense of the author, then after tensoring with the Cuntz algebra <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({\mathcal {O}}_2,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> all intermediate <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\hbox {C}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>C</mtext> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-algebras <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(B \subset C\subset A \mathop {\rtimes _{\textrm{r}}}\Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>B</mi> <mo>⊂</mo> <mi>C</mi> <mo>⊂</mo> <mi>A</mi> <msub> <mo>⋊</mo> <mtext>r</mtext> </msub> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation> enjoy a natural crossed product splitting <Equation ID="Equ1"> <EquationSource Format="TEX">\(\begin{aligned} {\mathcal {O}}_2\otimes C=({\mathcal {O}}_2 \otimes D) \mathop {\rtimes _{{\textrm{r}}, \gamma , \mathfrak {w}}} \Lambda \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> <mo>⊗</mo> <mi>C</mi> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> <mo>⊗</mo> <mi>D</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mo>⋊</mo> <mrow> <mtext>r</mtext> <mo>,</mo> <mi>γ</mi> <mo>,</mo> <mi mathvariant="fraktur">w</mi> </mrow> </msub> <mi mathvariant="normal">Λ</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>for <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(D:= C \cap A,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>D</mi> <mo>:</mo> <mo>=</mo> <mi>C</mi> <mo>∩</mo> <mi>A</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> some <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\Lambda &lt;\Gamma ,\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>&lt;</mo> <mi mathvariant="normal">Γ</mi> <mo>,</mo> </mrow> </math></EquationSource> </InlineEquation> and a subsystem <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\((\gamma , \mathfrak {w})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <mi>γ</mi> <mo>,</mo> <mi mathvariant="fraktur">w</mi> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> of a unitary perturbed cocycle action <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\Lambda \curvearrowright {\mathcal {O}}_2\otimes A.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Λ</mi> <mo>↷</mo> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> <mo>⊗</mo> <mi>A</mi> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation> As an application, we give a new Galois’s type theorem for the Bisch–Haagerup type inclusions <Equation ID="Equ2"> <EquationSource Format="TEX">\(\begin{aligned} A^K \subset A\mathop {\rtimes _{\textrm{r}}}\Gamma \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msup> <mi>A</mi> <mi>K</mi> </msup> <mo>⊂</mo> <mi>A</mi> <msub> <mo>⋊</mo> <mtext>r</mtext> </msub> <mi mathvariant="normal">Γ</mi> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>for actions of compact-by-discrete groups <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(K \rtimes \Gamma \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>K</mi> <mo>⋊</mo> <mi mathvariant="normal">Γ</mi> </mrow> </math></EquationSource> </InlineEquation> on simple <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\hbox {C}^*\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mtext>C</mtext> <mo>∗</mo> </msup> </math></EquationSource> </InlineEquation>-algebras. Due to a K-theoretical obstruction, the operation <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\({\mathcal {O}}_2\otimes -\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> <mo>⊗</mo> <mo>-</mo> </mrow> </math></EquationSource> </InlineEquation> is necessary to obtain the clean splitting. Also, in general 2-cocycles <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\mathfrak {w}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="fraktur">w</mi> </math></EquationSource> </InlineEquation> appearing in the splitting cannot be removed even further tensoring with any unital (cocycle) action. We show them by examples, which further show that <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\({\mathcal {O}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> is a minimal possible choice. We also establish a von Neumann algebra analogue, where <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\({\mathcal {O}}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">O</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> is replaced by the type I factor <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\mathbb {B}(\ell ^2(\mathbb {N})).\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">B</mi> <mo stretchy="false">(</mo> <msup> <mi>ℓ</mi> <mn>2</mn> </msup> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">N</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Crossed product splitting of intermediate operator algebras via 2-cocycles

  • Yuhei Suzuki

摘要

We investigate the \(\hbox {C}^*\) C -algebra inclusions \(B \subset A \mathop {\rtimes _{\textrm{r}}}\Gamma \) B A r Γ arising from inclusions \(B \subset A\) B A of \(\Gamma \) Γ - \(\hbox {C}^*\) C -algebras. The main result shows that, when \(B \subset A\) B A is \(\hbox {C}^*\) C -irreducible in the sense of Rørdam, and is centrally \(\Gamma \) Γ -free in the sense of the author, then after tensoring with the Cuntz algebra \({\mathcal {O}}_2,\) O 2 , all intermediate \(\hbox {C}^*\) C -algebras \(B \subset C\subset A \mathop {\rtimes _{\textrm{r}}}\Gamma \) B C A r Γ enjoy a natural crossed product splitting \(\begin{aligned} {\mathcal {O}}_2\otimes C=({\mathcal {O}}_2 \otimes D) \mathop {\rtimes _{{\textrm{r}}, \gamma , \mathfrak {w}}} \Lambda \end{aligned}\) O 2 C = ( O 2 D ) r , γ , w Λ for \(D:= C \cap A,\) D : = C A , some \(\Lambda <\Gamma ,\) Λ < Γ , and a subsystem \((\gamma , \mathfrak {w})\) ( γ , w ) of a unitary perturbed cocycle action \(\Lambda \curvearrowright {\mathcal {O}}_2\otimes A.\) Λ O 2 A . As an application, we give a new Galois’s type theorem for the Bisch–Haagerup type inclusions \(\begin{aligned} A^K \subset A\mathop {\rtimes _{\textrm{r}}}\Gamma \end{aligned}\) A K A r Γ for actions of compact-by-discrete groups \(K \rtimes \Gamma \) K Γ on simple \(\hbox {C}^*\) C -algebras. Due to a K-theoretical obstruction, the operation \({\mathcal {O}}_2\otimes -\) O 2 - is necessary to obtain the clean splitting. Also, in general 2-cocycles \(\mathfrak {w}\) w appearing in the splitting cannot be removed even further tensoring with any unital (cocycle) action. We show them by examples, which further show that \({\mathcal {O}}_2\) O 2 is a minimal possible choice. We also establish a von Neumann algebra analogue, where \({\mathcal {O}}_2\) O 2 is replaced by the type I factor \(\mathbb {B}(\ell ^2(\mathbb {N})).\) B ( 2 ( N ) ) .