From Phase Transitions to Chaos 1992
DOI: 10.1142/9789814355872_0039
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Thermodynamic Formalism and Quantum Mechanics on the Modular Surface

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Cited by 4 publications
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“…where x φ is an arbitrary point of φ. On the other hand according to Series [2], Adler and Flatto [1] there is an one to one correspondence between P er(r) and the set of primitive periodic orbits ϑ on the unit tangent bundle T 1 M , M = P SL(2, Z)\H, with the period (see [12])…”
Section: Selberg Zeta Function and Transfer Operatormentioning
confidence: 99%
“…where x φ is an arbitrary point of φ. On the other hand according to Series [2], Adler and Flatto [1] there is an one to one correspondence between P er(r) and the set of primitive periodic orbits ϑ on the unit tangent bundle T 1 M , M = P SL(2, Z)\H, with the period (see [12])…”
Section: Selberg Zeta Function and Transfer Operatormentioning
confidence: 99%
“…(Dynamical Fredholm determinants and transfer operators are also useful in quantum chaos, at the triple intersection of number theory, geometry, and group theory. Mayer [73] wrote very readable discussion on the Selberg zeta function and transfer operators applied to quantum chaos on the modular surface. See also [32] and references therein.…”
Section: Dynamical Zeta Functions and Dynamical Fredholm Determinantsmentioning
confidence: 99%
“…In Mayer's theory a transfer operator L s is introduced as a special case of Ruelle's operator for a dynamical system, for instance for the group SL(2, Z) this is the twice iterated Gauss map T = T 2 G acting on the unit interval and the weight function −βlog|T ′ (z)|. Then, as a result of the one-to-one correspondence between the closed geodesics on the modular surface M = H \ SL(2, Z) and the primitive periodic orbits of T the Selberg zeta function can be written as a Fredholm determinant of the transfer operator [3].…”
mentioning
confidence: 99%