Abstract
We study the generalized transfer operator ℒ β f(z)=\(\sum\limits_{n = 1}^\infty {\left( {\frac{1}{{z + n}}} \right)^{2\beta } \times f\left( {1/\left( {z + n} \right)} \right)} \) of the Gauss mapTx=(1/x) mod 1 on the unit interval. This operator, which for β=1 is the familiar Perron-Frobenius operator ofT, can be defined for Re β>1/2 as a nuclear operator either on the Banach spaceA ∞(D) of holomorphic functions over a certain discD or on the Hilbert space ℋ (2)Reβ (H -1/2 of functions belonging to some Hardy class of functions over the half planeH −1/2. The spectra of − β on the two spaces are identical. On the space ℋ (2)Reβ (H -1/2 ℒ β is isomorphic to an integral operatorK β with kernel the Bessel function\(\mathfrak{F}_{2\beta - 1} (2\sqrt {st} )\) and hence to some generalized Hankel transform. This shows that ℒ β has real spectrum for real β>1/2. On the spaceA ∞(D) the operator ℒ β can be analytically continued to the entire β-plane with simple poles atβ=β k =(1-k)/2,k=0, 1, 2,..., and residue the rank 1 operatorN (k) f=1/2(1/K!)f (k)(0) . From this similar analyticity properties for the Fredholm determinant det (1-ℒ β ) of ℒ β and hence also for Ruelle's zeta function follow. Another application is to the function\(\zeta _{\rm M} (\beta ) = \sum\limits_{n = 1}^\infty {\left[ n \right]^\beta } \), where [n] denotes the irradional [n]=(n+(n 2+4)1/2)/2.ζ M (β) extends to a meromorphic function in the β-plane with the only poles at β=±1 both with residue 1.
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Communicated by J.-P. Eckmann
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Mayer, D.H. On the thermodynamic formalism for the gauss map. Commun.Math. Phys. 130, 311–333 (1990). https://doi.org/10.1007/BF02473355
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DOI: https://doi.org/10.1007/BF02473355