Non-equilibrium properties of trapped ions under sudden application of a laser

Coherent quantum-state manipulation of trapped ions using classical laser fields is a trademark of modern quantum technologies. In this work, we study aspects of work statistics and irreversibility in a single trapped ion due to sudden interaction with the impinging laser. This is clearly an out-of-equilibrium process where work is performed through illumination of an ion by the laser. Starting with the explicit evaluation of the first moments of the work distribution, we proceed to a careful analysis of irreversibility as quantified by the nonequilibrium lag. The treatment employed here is not restricted to the Lamb-Dicke limit, what allows us to investigate the interplay between nonlinearities and irreversibility. We show, for instance, that in the resolved carrier and sideband regimes, variation of the Lamb-Dicke parameter may cause a non-monotonic behavior of the irreversibility indicator. Counterintuitively, we find a working point where nonlinearity helps reversibility, making the sudden quench of the Hamiltonian closer to what would have been obtained quasistatically and isothermally.

Efficient and Selectable Production of Reactive Species Using a Nanosecond Pulsed Discharge in Gas Bubbles in Liquid

A plasma gas bubble-in-liquid method for high production of selectable reactive species using a nanosecond pulse generator has been developed. The gas of choice is fed through a hollow needle in a point-to-plate bubble discharge, enabling improved selection of reactive species. The increased interface reactions, between the gas-plasma and water through bubbles, give higher productivity. H_{le="margin: 0px; padding: 0px; border: 0px; outline: 0px; font-size: 0.8em; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial; white-space: nowrap; line-height: 0.7em; font-family: Arial, "Lucida Grande", Geneva, Verdana, Helvetica, "Lucida Sans Unicode", sans-serif;">2}O_{le="margin: 0px; padding: 0px; border: 0px; outline: 0px; font-size: 0.8em; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial; white-space: nowrap; line-height: 0.7em; font-family: Arial, "Lucida Grande", Geneva, Verdana, Helvetica, "Lucida Sans Unicode", sans-serif;">2} was the predominant species produced using Ar plasma, while predominantly  and NO_{le="margin: 0px; padding: 0px; border: 0px; outline: 0px; font-size: 0.8em; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial; white-space: nowrap; line-height: 0.7em; font-family: Arial, "Lucida Grande", Geneva, Verdana, Helvetica, "Lucida Sans Unicode", sans-serif;">2} were generated using air plasma, in good agreement with the observed emission spectra. This method has nearly 100% selectivity for H_{le="margin: 0px; padding: 0px; border: 0px; outline: 0px; font-size: 0.8em; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial; white-space: nowrap; line-height: 0.7em; font-family: Arial, "Lucida Grande", Geneva, Verdana, Helvetica, "Lucida Sans Unicode", sans-serif;">2}O_{le="margin: 0px; padding: 0px; border: 0px; outline: 0px; font-size: 0.8em; background-image: initial; background-position: initial; background-size: initial; background-repeat: initial; background-attachment: initial; background-origin: initial; background-clip: initial; white-space: nowrap; line-height: 0.7em; font-family: Arial, "Lucida Grande", Geneva, Verdana, Helvetica, "Lucida Sans Unicode", sans-serif;">2}, with seven times higher production, and 92% selectivity for , with nearly twice the production, compared with a plasma above the water.