CLT for the trace functional of the IDS of magnetic random Schrödinger operators

We consider the existence of the integrated density of states (IDS) of the magnetic Schrödinger operator with a random potential on the Hilbert space $L^2({\mathbb{R}}^d)$, as an analogue of the law of large numbers (LLN) for trace functionals. In this work, we establish an analogue of the central limit theorem (CLT), which describes the fluctuations of the trace functionals of the IDS, for a class of test functions denoted by $C_{d,0}^1(\mathbb{R})$. This class consists of real-valued, continuously differentiable functions on $\mathbb{R}$ that decay at the rate $O(\mathrm{\mid }x{\mathrm{\mid }}^{-m})$ as $\mathrm{\mid }x\mathrm{\mid }\to \mathrm{\infty }$, where $m>d+1$.