Although there is a growing consensus as to the universality of domain growth kinetics in quenched systems, discrepancies remain among theory, experiments, and simulations. We identify a major discrepancy between the three-the time dependence of mass transfer kinetics. We show that this discrepancy can be resolved in Monte Carlo simulations of domain growth. Our results strengthen the emerging consensus that systems having a nonconserved order parameter obey Lifschitz-Allen-Cahn growth kinetics in the asymptotic scaling limit.PACS numbers: 68.35.Fx, 61.70.NgGrowth and ordering processes are abundant in nature, underlying phenomena as diverse as snowflake and soot formation, crystal growth, and the evolution of the Universe. The search for universality and possible subclassifications in these apparently wide and varied phenomena is a significant fundamental problem in nonequilibrium statistical mechanics [1]. In thermally quenched systems, the development of long-range order is accomplished by the growth of ordered domains. It is becoming increasingly evident that domain growth in these systems exhibits universal behavior. That is, many systems which conserve the order parameter conform to the Lifschitz-Slyozov (LS) theory [2] of domain growth, while systems having a nonconserved order parameter generally exhibit Lifschitz-Allen-Cahn (LAC) [3] growth kinetics. Ordering kinetics in these theories are described by a power-law expression of the form (l(t)) -(At) x , where (lit)) is a characteristic length of a domain at time /, A is a proportionality factor, and x is a growth exponent. In the LAC theory, x -j, while x = y in the LS theory. Although the current understanding of domain growth has emerged with considerable controversy, these theories remain the most widely accepted descriptions of domain growth.