Spectral Theories, IV, p. 368
Let n∈N. We denote by Δ the Laplacian on L2(Rn).
a) For every t∈R∗, the endomorphism eitΔ of L2(Rn) is given by
eitΔf(x)=(2it)n/21∫Rnf(y)ei∣x−y∣2/(4t)dy
if f∈L1(Rn)∩L2(Rn). (Use the Fourier transform.)
b) Let C be the unitary mapping on L2(Rn) deduced by passing to the quotient from the mapping f↦C(f) defined for f∈L2(Rn) by
C(f)(x)=(2it)n/21e4tix2Ff(2tx)
for x∈Rn.
One has eitΔ→C when t→+∞ in the space L(L2(Rn)) endowed with the topology of simple convergence.
c) Suppose that 1⩽n⩽3. Let g∈L∞(Rn)+L2(Rn) be real-valued. Let us denote by u the partial operator u=Δ+mg; it is self-adjoint on L2(Rn) (exercise 14). For f∈L1(Rn)∩L2(Rn) and t∈R∗, one has
eituf(x)= limk→+∞(2it/k)kn/21∫Rnkf(yk) exp(kit∑i=1k(4(t/k)2∣yi−yi−1∣2−g(yi))dy
where one writes y=(y1,...,yk) with yi∈Rn.
d) Interpretation of the preceding formula.
Nothing.
Nothing.