We study the quenching dynamics of a one-dimensional spin-1/2 model in a transverse field when the transverse field is quenched repeatedly between and . A single passage from to $h \to +\infty$ or the other way around is referred to as a half-period of quenching. For an even number of half-periods, the transverse field is brought back to the initial value of ; in the case of an odd number of half-periods, the dynamics is stopped at . The density of defects produced due to the non-adiabatic transitions is calculated by mapping the many-particle system to an equivalent Landau-Zener problem and is generally found to vary as for large ; however, the magnitude is found to depend on the number of half-periods of quenching. For two successive half-periods, the defect density is found to decrease in comparison to a single half-period, suggesting the existence of a corrective mechanism in the reverse path. A similar behavior of the density of defects and the local entropy is observed for repeated quenching. The defect density decays as for large for any number of half-periods, and shows a increase in kink density for small for an even number; the entropy shows qualitatively the same behavior for any number of half-periods. The probability of non-adiabatic transitions and the local entropy saturate to 1/2 and , respectively, for a large number of repeated quenching.

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