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Constructions of harmonic maps between Hadamard manifolds

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1.2. GLOBAL PROPERTIES OF SOLUTIONS 37<br />

Lemma 1.2.7. The function φ(r 0 ,t 0 ) is well-defined for r 0 > 0 and t 0 > 0, and<br />

lim φ(r 0,t 0 )=0.<br />

r 0 →∞<br />

Pro<strong>of</strong>. It follows from (H-3) that (h 2 i ) ′ (s) ≥ (h 2 i ) ′ (s − r 0 ) for s>r 0 . Integrating both<br />

sides with respect to s from r 0 to s, we get<br />

Therefore, it holds that for K>0<br />

∫ ∞<br />

r 0 +K<br />

h i (s) 2 − h i (r 0 ) 2 ≥ h i (s − r 0 ) 2 .<br />

[γ 1 (t 0 ) 2 {h 1 (s) 2 − h 1 (r 0 ) 2 } + γ 2 (t 0 ) 2 {h 2 (s) 2 − h 2 (r 0 ) 2 } + β(r 0 ,t 0 ) 2 ] −1/2 ds<br />

≤ C(t 0 )<br />

≤ C(t 0 )<br />

∫ ∞<br />

r 0 +K<br />

∫ ∞<br />

K<br />

[h 1 (s − r 0 ) 2 + h 2 (s − r 0 ) 2 ] −1/2 ds<br />

ds<br />

h(s) .<br />

Note that it follows from the condition (1.2.5) that for any ε>0<br />

for sufficiently large K.<br />

∫ ∞<br />

K<br />

ds<br />

h(s) r 0<br />

where ρ i ∈ (r 0 ,s). It follows from (H-3) that<br />

Therefore it holds that<br />

∫ r0 +K<br />

r 0<br />

h i (s) 2 − h i (r 0 ) 2 =2h i (ρ i )h ′ i (ρ i)(s − r 0 ),<br />

h i (s) 2 − h i (r 0 ) 2 ≥ 2h i (r 0 )h ′ i(r 0 )(s − r 0 ) > 0.<br />

[γ 1 (t 0 ) 2 {h 1 (s) 2 − h 1 (r 0 ) 2 } + γ 2 (t 0 ) 2 {h 2 (s) 2 − h 2 (r 0 ) 2 } + β(r 0 ,t 0 ) 2 ] −1/2 ds<br />

≤ [2(γ 1 (t 0 ) 2 h 1 (r 0 )h ′ 1(r 0 )+γ 2 (t 0 ) 2 h 2 (r 0 )h ′ 2(r 0 ))] −1/2 ∫ r0 +K<br />

≤ C(t 0 ) √ K min { [h 1 (r 0 )h ′ 1 (r 0)] −1/2 , [h 2 (r 0 )h ′ 2 (r 0)] −1/2} .<br />

r 0<br />

ds<br />

√ s − r0

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