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On the thermodynamic formalism for the Gauss map
Authors:Dieter H Mayer
Institution:(1) Max-Planck-Institut für Mathematik, Gottfried-Claren-Straße 26, D-5300 Bonn 3, Federal Republic of Germany
Abstract:We study the generalized transfer operatorMediaObjects/220_2005_BF02102958_f2.jpg of the Gauss mapTx=(1/x) mod 1 on the unit interval. This operator, which for beta=1 is the familiar Perron-Frobenius operator ofT, can be defined for Re beta>1/2 as a nuclear operator either on the Banach spaceA infin(D) of holomorphic functions over a certain discD or on the Hilbert spaceMediaObjects/220_2005_BF02102958_f3.jpg of functions belonging to some Hardy class of functions over the half planeH –1/2. The spectra ofMediaObjects/220_2005_BF02102958_f4.jpg on the two spaces are identical. On the spaceMediaObjects/220_2005_BF02102958_f5.jpg is isomorphic to an integral operatorMediaObjects/220_2005_BF02102958_f6.jpg with kernel the Bessel function 
$$\mathfrak{F}_{2\beta  - 1} (2\sqrt {st} )$$
and hence to some generalized Hankel transform. This shows thatMediaObjects/220_2005_BF02102958_f7.jpg has real spectrum for real beta>1/2. On the spaceA infin(D) the operatorMediaObjects/220_2005_BF02102958_f8.jpg can be analytically continued to the entire beta-plane with simple poles at 
$$\beta  = \beta _k  = (1 - k)/2,k = 0,1,2,...$$
and residue the rank 1 operator 
$$\mathcal{N}^{(k)} f = \tfrac{1}{2}(1/k!)f^{(k)} (0)$$
. From this similar analyticity properties for the Fredholm determinantMediaObjects/220_2005_BF02102958_f9.jpg ofMediaObjects/220_2005_BF02102958_f10.jpg and hence also for Ruelle's zeta function follow. Another application is to the function 
$$\zeta _M (\beta ) = \sum\limits_{n = 1}^\infty  {n]^\beta  } $$
, where n] denotes the irrationaln]=(n+(n 2+4)1/2)/2. zetaM(beta) extends to a meromorphic function in the beta-plane with the only poles at beta=±1 both with residue 1.
Keywords:
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