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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1.1. LOCAL EXISTENCE OF SOLUTIONS TO (1.1.1) WITH (1.1.2) 23<br />
Since the solutions depend continuously on initial values, it follows that for the above δ>0,<br />
there exists an ¯ε >0 such that if | ¯s 0 − s 0 | < ¯ε, then<br />
∣ sup |ρ(τ) − r(τ)| + sup<br />
dρ dr ∣∣∣<br />
∣ (τ) −<br />
τ∈I<br />
τ∈I dτ dτ (τ) <br />
dτ dτ (τ) − δ>η>0 on [τ 1 − ε, τ 0 ],<br />
ρ(τ 1 − ε) 0. Suppose that inf A(r 0 )=0. For s 0 ∈A(r 0 ), let r = r(τ)<br />
be a solution to the equation (1.1.4) with the initial condition (1.1.5). Then<br />
d 2 r<br />
dτ (τ 0)=−P (τ 2 0 )s 0 + Q(τ 0 ,r 0 ).<br />
Since Q(τ 0 ,r 0 ) > 0, for sufficiently small δ>0, one can take s 0 > 0 so that<br />
d 2 r<br />
dτ (τ 0) > 2δ.<br />
2<br />
Hence there exists an ε = ε(s 0 ) > 0 such that<br />
d 2 r dr<br />
(τ) >δ,<br />
dτ<br />
2<br />
dτ (τ) > 0 and r(τ) > 0 on (τ 0 − 2ε, τ 0 +2ε).<br />
For ¯s 0 ∈A(r 0 ) such that ¯s 0 r(τ) and<br />
Thus we obtain<br />
dρ dr<br />
(τ) <<br />
dτ dτ (τ).<br />
d 2 ρ<br />
(τ) =−P (τ)dρ<br />
dτ<br />
2<br />
dτ (τ)+Q(τ,ρ(τ))<br />
≥−P (τ) dr<br />
dτ (τ)+Q(τ,r(τ)) = d2 r<br />
(τ) >δ<br />
dτ<br />
2