
A special function playing an essential role in the construction of quantum "ax+b"-group is introduced and investigated. The function is denoted by Fℏ(r,ϱ), where ℏ is a constant such that the deformation parameter q2=e-iℏ. The first variable r runs over non-zero real numbers; the range of the second one depends on the sign of r: ϱ=0 for r>0 and ϱ=±1 for r<0. After the holomorphic continuation the function satisfies the functional equation [Formula: see text] The name "exponential function" is justified by the formula: [Formula: see text] where R, S are selfadjoint operators satisfying certain commutation relations and [R+S] is a selfadjoint extension of the sum R+S determined by operators ρ and σ appearing in the formula. This formula will be used in a forthcoming paper to construct a unitary operator W satisfying the pentagonal equation of Baaj and Skandalis.
Linear symmetric and selfadjoint operators (unbounded), selfadjoint extension, quantum \(ax+b\)-group, Applications of operator theory in the physical sciences, exponential function, Quantum groups and related algebraic methods applied to problems in quantum theory, holomorphic continuation
Linear symmetric and selfadjoint operators (unbounded), selfadjoint extension, quantum \(ax+b\)-group, Applications of operator theory in the physical sciences, exponential function, Quantum groups and related algebraic methods applied to problems in quantum theory, holomorphic continuation
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