The crossed-product factorization conjecture for Orlicz spaces

Let ψ\psi be an Orlicz function. The spaces SψS^\psi and SψS_\psi consist of the elements defined by the scaling conditions

Sψ={aA~:θs(aφ~ψ(h)1/2χ[0,δ](h))=es/2aφ~ψ(h)1/2χ[0,esδ](h) for all 0<δ}S^\psi = \{a\in\widetilde{\mathcal{A}}: \theta_s(a\widetilde{\varphi}_{\psi^*}(h)^{1/2}\chi_{[0,\delta]}(h)) = e^{-s/2}a\widetilde{\varphi}_{\psi^*}(h)^{1/2}\chi_{[0,e^s\delta]}(h) \text{ for all } 0<\delta\}

and

Sψ={aA~:θs(aφψ(h)1/2χ[0,δ](h))=es/2aφψ(h)1/2χ[0,esδ](h) for all 0<δ}.S_\psi = \{a\in\widetilde{\mathcal{A}}: \theta_s(a{\varphi}_{\psi^*}(h)^{1/2}\chi_{[0,\delta]}(h)) = e^{-s/2}a{\varphi}_{\psi^*}(h)^{1/2}\chi_{[0,e^s\delta]}(h) \text{ for all } 0<\delta\}.

The crossed-product factorization conjecture. For any Orlicz function ψ\psi,

Lψ(M)=span{ab:a,bSψ}andLψ(M)=span{ab:a,bSψ}.L^\psi(\mathcal{M}) = \overline{\operatorname{span}}\{a^*b: a, b \in S^\psi\} \qquad\text{and}\qquad L_\psi(\mathcal{M}) = \overline{\operatorname{span}}\{a^*b: a, b \in S_\psi\}.

The author presents this relationship as currently unproved because of technical difficulties in establishing the asserted descriptions of the Orlicz spaces.

Sources & referencesView supporting material

Primary source

Louis Labuschagne, “A crossed product approach to Orlicz spaces”, arXiv:1205.2192 (2013).

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