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In mathematics, specifically harmonic analysis and probability theory, the Furstenberg boundary is a notion of boundary associated with a group. It is named for Harry Furstenberg, who introduced it in a series of papers beginning in 1963 (in the case of semisimple Lie groups). The Furstenberg boundary can be characterized as a universal boundary space for harmonic analysis on the group, in the sense that bounded harmonic functions can be represented by their boundary values via a Poisson-type integral.

For example, when , the Furstenberg boundary is the real projective line , which may be identified with the boundary circle of the hyperbolic plane, and the Poisson-like integral is the usual Poisson kernel for the upper half-plane.

Semisimple Lie groups

Let be a connected semisimple Lie group. The Furstenberg boundary of is the homogeneous space

where is a minimal parabolic subgroup of .

This space is compact and homogeneous under the action of . More generally, quotients by parabolic subgroups are generalized flag manifolds, and the Furstenberg boundary is the maximal one among these in the sense that every quotient by a parabolic subgroup is a factor of .

For example, if , then the Furstenberg boundary is the manifold of complete flags in . For , it is .

Relation to Poisson boundaries

Let be a probability measure on . A function on is called -harmonic if

The Poisson boundary of the measured group is a measure space that represents bounded -harmonic functions by boundary integrals. Unlike the Furstenberg boundary, the Poisson boundary depends on the choice of the measure .

For semisimple Lie groups, Furstenberg showed that for broad classes of measures the Poisson boundary can be realized on a homogeneous boundary of the form , where is a parabolic subgroup. In particular situations the maximal boundary plays the role of a universal homogeneous boundary from which the others are obtained as quotients.

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