The crossed-product factorization conjecture for Orlicz spaces

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

Sψ={a∈A~:θs(aφ~ψ∗(h)1/2χ[0,δ](h))=e−s/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={a∈A~:θs(aφψ∗(h)1/2χ[0,δ](h))=e−s/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⁡‾{a∗b:a,b∈Sψ}andLψ(M)=span⁡‾{a∗b:a,b∈Sψ}.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.

References

Primary source

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

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