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Abstract
The Bost-Connes system [BC95] is a C ∗ -dynamical system whose partition function, KMS states, and symmetries are related to the explicit class field theory of Q. In particular, its zero-temperature KMS states, when evaluated on certain points in an arithmetic sub-algebra, yield the generators of Qcycl. The Bost-Connes system can be viewed in terms of a geometric picture of 1-dimensional Q-lattices. The GL2- system [CM04] is an extension of this idea to the setting of 2-dimensional Q-lattices. A specialization of the GL2-system introduced in [CMR06] is related in a similar way to the explicit class field theory of imaginary quadratic extensions.
Inspired by the philosophy of Manin’s real multiplication program, we define a boundary version of the GL2-system. In this viewpoint we see P 1 (R) under a certain PGL2(Z) action (which is related to the shift of the continued fraction expansion) as a moduli space characterizing degenerate elliptic curves. These degenerate elliptic curves can be realized as non-commutative 2-tori. This moduli space of the noncommutative tori is interpreted as an “invisible” boundary of the moduli space of elliptic curves. In fact, we define a family of such boundary GL2 systems indexed by a choice of continued fraction algorithm. We analyze their partition functions, KMS states, and ground states. We also define an arithmetic algebra of unbounded multipliers in analogy with the GL2case. We show that the ground states when evaluated on points in the arithmetic algebra give pairings of the limiting modular symbols of [MM02] with weight-2 cusp forms.
We also begin the project of extending this picture to the higher weight setting by defining a higher-weight limiting modular symbol. We use as a starting point the Shokurov modular symbols [Sho81a], which are constructed using Kuga varieties over the modular curves. We subject these modular symbols to a limiting procedure. We then show, using the coding space setting of [KS07b], that these limiting modular symbols can be written as a Birkhoff ergodic average everywhere.
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