We present a Renormalization Group (RG) framework based on a nonlocal effective action ansatz to analyze the strong coupling dynamics of the three-dimensional relativistic theory. By implementing a Hubbard-Stratonovich transformation, we decouple the quartic interaction into the primary field and an auxiliary field , allowing both exponents and to act as independent, unconstrained variables rather than fixed scaling dimensions. Within this nonlocal propagator framework, both the field self-energies and vertex corrections are evaluated at the one-loop order. The resulting one-loop logarithmic derivatives determine the renormalization group flows of the couplings and the scaling exponents. For and , the self-consistent equations yield a physical fixed point at and . These exponents result in a kinematic anomalous dimension , an energy operator dimension , and a thermal correlation length exponent . For , the self-consistent equations yield another fixed point at , , and , corresponding to and . Although these leading-order results show deviations from high-precision Quantum Monte Carlo (QMC) and conformal bootstrap benchmarks, they characterize the baseline scaling behavior of the Wilson-Fisher universality class.

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