Constructions of harmonic maps between Hadamard manifolds
Constructions of harmonic maps between Hadamard manifolds
Constructions of harmonic maps between Hadamard manifolds
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3.1. DAMEK-RICCI SPACES 61<br />
where [ , ] Ò<br />
is the Lie bracket on n defined by (3.1.1). In this way, s becomes a Lie algebra<br />
with an inner product. The simply connected Lie group S associated with s, equipped with<br />
the left invariant metric g S , is called a Damek-Ricci space.<br />
Example. Let v = R 2k , u = R 2 , and µ(z,v) =(−y, x),µ(w, v) =(x, y), where {z,w} is<br />
an orthonormal basis <strong>of</strong> R 2 and v =(x, y) ∈ R k ⊕ R k . Then n is a (classical) Heisenberg<br />
algebra and (S, g S ) is isometric to the complex hyperbolic space whose sectional curvature<br />
K satisfies −4 ≤ K ≤−1. The quaternion hyperbolic space and the Cayley hyperbolic<br />
plane are also Damek-Ricci spaces. These three spaces are called classical (cf. [8]). Thus<br />
Damek-Ricci spaces are generalizations <strong>of</strong> rank one symmetric spaces <strong>of</strong> noncompact type.<br />
Let ∇ be the Levi-Civita connection on (S, g S ). Using the formula<br />
2〈∇ X Y,Z〉 = 〈[X, Y ],Z〉 + 〈[Z, X],Y〉 + 〈[Z, Y ],X〉<br />
for X, Y, Z ∈ s, one obtains<br />
⎧<br />
∇ h X =0, ∇ X h = −[h, X],<br />
⎪⎨ ∇ v v ′ = 〈v, v ′ 〉h + 1 2 [v, v′ ],<br />
∇ v z = ∇ z v = −µ(z,v),<br />
⎪⎩<br />
∇ z z ′ =2〈z,z ′ 〉h,<br />
where X ∈ s,v,v ′ ∈ v,z,z ′ ∈ z and µ is the composition <strong>of</strong> quadratic forms in the definition<br />
<strong>of</strong> n. Then the following results have been proved.<br />
Theorem 3.1.2.<br />
([7], [8]).<br />
(1) A Damek-Ricci space is a symmetric space if and only if it is classical<br />
(2) A Damek-Ricci space has strictly negative sectional curvature if and only if it is classical<br />
([13]).<br />
In fact, Damek constructed a simple example <strong>of</strong> Damek-Ricci space whose sectional<br />
curvature attains zero for some two-dimensional plane. Other examples have been given