TY - JOUR
T1 - The geodesic flow of a nonpositively curved graph manifold
AU - Croke, C. B.
AU - Kleiner, B.
N1 - Funding Information:
C.B.C. supported by NSF grants DMS-95-05175 DMS-96-26-232 and DMS 99-71749. B.K. supported by a Sloan Foundation Fellowship, and NSF grants DMS-95-05175, DMS-96-26911, DMS-9022140.
PY - 2002
Y1 - 2002
N2 - We consider discrete cocompact isometric actions G right curved arrow signρ X where X is a locally compact Hadamard space (following [B] we will refer to CAT(0) spaces - complete, simply connected length spaces with non-positive curvature in the sense of Alexandrov - as Hadamard spaces) and G belongs to a class of groups ("admissible groups") which includes fundamental groups of 3-dimensional graph manifolds. We identify invariants ("geometric data") of the action p which determine, and are determined by, the equivariant homeomorphism type of the action G right curved arrow sign∂∞ρ ∂∞X of G on the ideal boundary of X. Moreover, if G right curved arrow signρi Xi are two actions with the same geometric data and φ: X1 → X2 is a G-equivariant quasi-isometry, then for every geodesic ray γ1 : [0, ∞) → X1, there is a geodesic ray γ2 : [0, ∞) → X2 (unique up to equivalence) so that limt→∞ 1/tdX2 (Φ O γ1(t), γ2([0, ∞))) = 0. This work was inspired by (and answers) a question of Gromov in [Gr3, p. 136].
AB - We consider discrete cocompact isometric actions G right curved arrow signρ X where X is a locally compact Hadamard space (following [B] we will refer to CAT(0) spaces - complete, simply connected length spaces with non-positive curvature in the sense of Alexandrov - as Hadamard spaces) and G belongs to a class of groups ("admissible groups") which includes fundamental groups of 3-dimensional graph manifolds. We identify invariants ("geometric data") of the action p which determine, and are determined by, the equivariant homeomorphism type of the action G right curved arrow sign∂∞ρ ∂∞X of G on the ideal boundary of X. Moreover, if G right curved arrow signρi Xi are two actions with the same geometric data and φ: X1 → X2 is a G-equivariant quasi-isometry, then for every geodesic ray γ1 : [0, ∞) → X1, there is a geodesic ray γ2 : [0, ∞) → X2 (unique up to equivalence) so that limt→∞ 1/tdX2 (Φ O γ1(t), γ2([0, ∞))) = 0. This work was inspired by (and answers) a question of Gromov in [Gr3, p. 136].
UR - http://www.scopus.com/inward/record.url?scp=0035995734&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0035995734&partnerID=8YFLogxK
U2 - 10.1007/s00039-002-8255-7
DO - 10.1007/s00039-002-8255-7
M3 - Article
AN - SCOPUS:0035995734
SN - 1016-443X
VL - 12
SP - 479
EP - 545
JO - Geometric and Functional Analysis
JF - Geometric and Functional Analysis
IS - 3
ER -