The printed uniqueness claim omits nondegeneracy of the limit. The zero process is a Lévy process, and every yields that limit. We first classify all possibilities under the stated assumptions, then identify the unique nonzero one.
For , part (b) gives
for each fixed . If , the characteristic functions tend to zero for every nonzero parameter and remain one at zero. This discontinuous function cannot be the characteristic function of a probability law. The characteristic-function convergence theorem therefore rules out even one-dimensional weak convergence of random variables at a positive time.
For joint convergence, take and write . Independent increments give
At , this tends to . These are exactly the joint laws of standard Brownian motion: increments are independent centred normals with variances . The assumed limiting Lévy process thus has the Brownian law.
For , the same joint characteristic functions tend to one. Every limiting vector is zero. The càdlàg path convention then makes the limiting process identically zero almost surely: first intersect the zero-value events at rational times, then use right continuity. The complete scaling classification of a continuous-time symmetric simple random walk is
In particular, if a nonzero limiting Lévy process is intended, the unique exponent is , and
The finite-dimensional Brownian law, together with the Lévy càdlàg convention, determines the process law and its continuous version. No assertion of path-space convergence of the approximating walks is needed here.
The characteristic function of is
Thus every already has the standard Cauchy law, and convergence in law follows from characteristic-function convergence theorem.
Characteristic-function convergence theorem says iff for all , where the limiting function is continuous at zero.