Spectral Theories, II, p. 269
(a) Let n∈N and let f∈S(Rn). The function from R×Rn into C defined by
u(t,x)=∫Rnf(y) exp(2πix⋅y−4π2t∥y∥2)dy
for (t,x)∈R×Rn satisfies
{u(0,x)=f(0,x)
(1)
∂tu=iΔ2u
(“Schrödinger equation”) where
Δ2u=i=1∑n∂xi2u
(b) The function u is the unique solution of (1) such that t↦(x↦u(t,x)) belongs to C∞(R,S(Rn)).
Nothing.
Nothing.