In this study, we investigate the bifurcation of limit cycles from a class of uniform isochronous cubic centers in the plane under small continuous perturbations. Such systems provide classic yet challenging examples in nonlinear differential equations, offering valuable insight into the dynamics of planar polynomial systems and the emergence of small-amplitude periodic solutions. Understanding these bifurcations is fundamental for advancing the qualitative theory of planar systems and their applications in modeling oscillatory phenomena.

The differential system under consideration is given by:

\dot{x}=-y+x^{2}y+xy^{2}+\sum\limits_{i=1}^{6}\epsilon^{i}P_{i}(x,y),\quad

\dot{y}=x+xy^{2}-x^{2}y+\sum\limits_{i=1}^{6}\epsilon^{i}Q_{i}(x,y),​

where P_{i}(x,y) and Q_{i}(x,y) are cubic polynomials, and ε is a small perturbation parameter. Introducing polar coordinates, the system is transformed into a form suitable for the averaging method. Applying the sixth-order averaging theory, we derive sufficient conditions for the existence of limit cycles through the analysis of the averaged functions. This higher-order approach enables the detection of subtle bifurcation phenomena that may be missed in lower-order analyses.

Our analysis demonstrates that at most three small-amplitude limit cycles can bifurcate from the uniform isochronous cubic center under small continuous perturbations. The use of higher-order averaging reveals complex dynamics and interactions between the perturbation terms that are otherwise undetectable.

These findings enrich the qualitative theory of planar polynomial differential systems and showcase the effectiveness of sixth-order averaging methods in studying limit cycle bifurcations. The results highlight the intricate behavior of cubic systems and provide a robust framework for future investigations in nonlinear dynamics, with potential applications for modeling oscillatory behaviors in applied mathematics, physics, and engineering.