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The applicability of the one-parameter scaling hypothesis to nonreciprocal high-dimensional disordered systems, specifically, those in dimensions higher than the critical dimension d₂=2, as predicted by the standard one-parameter scaling theory of Anderson localization, remains unresolved. In this work, we propose that the size dependence of the reduced participation ratio Y₋ in nonreciprocal d-dimensional systems of size L^d follows a universal one-parameter scaling form. This feature is encapsulated by the one-parameter function Y₋=dlnY₋/dlnL, which describes the critical properties of Anderson localization transitions, including the critical exponent, the fractal dimension D, and the critical reduced participation ratio Y₋^*. We demonstrate the applicability of our one-parameter scaling theory across the AI, A, and AII classes of three-dimensional nonreciprocal systems under periodic boundary conditions and further extend our analysis to higher dimensions in the presence of nonreciprocity, specifically d=4, 5, and 6. Our one-parameter scaling theory also applies to nonreciprocal systems with open boundary conditions, where all states are non-Hermitian skin modes. The scaling analysis indicates that open nonreciprocal systems do not exhibit genuine extended states extending throughout the system in the thermodynamic limit.
Wang et al. (Wed,) studied this question.