Spectral Theories, IV, p. 351
We retain the notation of the preceding exercise. We denote by φn the unique eigenfunction of SLq corresponding to the eigenvalue λn such that φn′(0)=λn.
a) Let M = sup{q(x)}. For every n∈N, one has
π2(n+1)2⩽λn⩽π2(n+1)2+M
and moreover
λn=π2(n+1)2(1+O(n21))
when n→+∞.
b) Let s>0. Let f∈C2([0,1]) be such that
−f′′+s2f=−qf,f(0)=0,f′(0)=s
Then one has (1−s−1us)f=gs, where gs(x)= sin(sx) and us is the integral operator on C([0,1]) given by
us(f)(x)=∫0x sin(s(x−y))q(y)f(y)dμ(y).
c) For s sufficiently large, one has s∈/ Sp(us).
d) For every fixed x, one has
φn(x)= sin((n+1)x) +O(n−1)
when n→+∞.
Nothing.
Nothing.