Spectral Theories, IV, p. 351
We resume the notation of the preceding exercise.
a) There exist functions f1 and f2 in C2([a,b]) such that −fi′′+qfi=0 and
f1(0)=0,f1′(0)=1
f2(1)=0,f2′(1)=−1
These functions are the unique solutions of these equations and the function w= f1f2′−f1′f2 is constant.
b) Let g∈C([0,1]). There exists a unique function φ∈C2([0,1]) such that
−φ′′+qφ=g
and one has φ=c1f1+c2f2, where
c1(x)=−w1∫x1g(y)f2(y)dμ(y),c2(x)=−w1∫0xg(y)f1(y)dμ(y)
for every x∈[0,1]. c) The partial operator SLq is surjective; its inverse is the mapping g↦φ and there exists a function G∈C([0,1]2) such that
SLq−1(g)(x)=∫01G(x,y)g(y)dμ(y)
for every g∈C([0,1]) and almost every x∈[0,1]. One has G(x,y)=G(y,x) for every (x,y)∈[0,1]2.
d) The operator SLq−1 is compact and injective on L2([0,1],μ).
e) The functions (φn) form an orthonormal basis of L2([0,1]), and the spectrum of SLq coincides with the set of its eigenvalues.
Nothing.
Nothing.