The Dirac operator for the pair of Ruelle and Koopman operators, and a generalized Boson formalism
Abstract
Denote by μ the maximal entropy measure for the shift map σ acting on = \0, 1\N, by L the associated Ruelle operator and by K = L the Koopman operator, both acting on L2(μ). The Ruelle-Koopman pair can determine a generalized boson system in the sense of Kuo. Here 2-12 K plays the role of the creation operator and 2-12 L is the annihilation operator. We show that [L,K] is the projection on the kernel of L. In C*-algebras the Dirac operator D represents derivative. Akin to this point of view we introduce a dynamically defined Dirac operator D associated with the Ruelle-Koopman pair and a representation π. Given a continuous function f, denote by Mf the operator g Mf(g)=f\, g. Among other dynamical relations we get \|[ D , π (Mf) ]\| = x ∈ |f(x) - f(0x)|22 + |f(x) - f(1x)|22 = |L |K f - f|2|∞ which concerns a form of discrete-time mean backward derivative. We also derive an inequality for the discrete-time forward derivative f σ -f: |f σ -f |∞ = |K f - f|∞ ≥ \|[ D , π (Mf) ]\| ≥ |f - L f|∞. Moreover, we get \|\, [D ,π(K L)] \,\|=1. The Number operator is 12K 12 L. The Connes distance requires to ask when an operator A satisfies the inequality \|\, [D ,π(A)] \,\|≤ 1; the Lipschtiz constant of A smaller than 1.
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