Among the various materials used for supercontinuum generation, Nd:YAG ceramics and crystals exhibit exceptional efficiency and potential for use in, for instance, nonlinear imaging [1], [2]. In this work, we study wave collapse due to the intriguing spatiotemporal propagation effects possible in Nd:YAG. Beam collapse in nonlinear bulk media can be stabilized by several mechanisms, including conical emission, colinear and non-colinear supercontinuum generation, and plasma defocusing [3], [4]. As the beam propagates, plasma effects occur in nonuniformly-spaced focusing-defocusing cycles [2], [5], [6], in which a particular parameter plays a significant role: the electron collision time (proportional to conductivity) [2]. Supercontinuum generation accompanies beam collapse after only a millimeter-scale propagation distance, preventing the different wavepackets from dispersing significantly. Therefore, such light sources support interesting applications in nonlinear spectroscopy such as multiplex-CARS, as we have recently shown in Refs. [1], [2].
Dynamics of Supercontinuum Generation from Light Filaments in Ceramic Nd:YAG Polycrystals / Bagley, N.; Wehbi, S.; Mansuryan, T.; Boulesteix, R.; Maître, A.; Arosa, Y.; Ferraro, M.; Mangini, F.; Sun, Y.; Krupa, K.; Wetzel, B.; Wabnitz, S.; Aceves, A.; Tonello, A.; Couderc, V.. - (2025), pp. 1-1. ( 2025 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC) Munich, Germany ) [10.1109/cleo/europe-eqec65582.2025.11110618].
Dynamics of Supercontinuum Generation from Light Filaments in Ceramic Nd:YAG Polycrystals
Ferraro, M.;Mangini, F.;Sun, Y.;Krupa, K.;Wabnitz, S.;Couderc, V.
2025
Abstract
Among the various materials used for supercontinuum generation, Nd:YAG ceramics and crystals exhibit exceptional efficiency and potential for use in, for instance, nonlinear imaging [1], [2]. In this work, we study wave collapse due to the intriguing spatiotemporal propagation effects possible in Nd:YAG. Beam collapse in nonlinear bulk media can be stabilized by several mechanisms, including conical emission, colinear and non-colinear supercontinuum generation, and plasma defocusing [3], [4]. As the beam propagates, plasma effects occur in nonuniformly-spaced focusing-defocusing cycles [2], [5], [6], in which a particular parameter plays a significant role: the electron collision time (proportional to conductivity) [2]. Supercontinuum generation accompanies beam collapse after only a millimeter-scale propagation distance, preventing the different wavepackets from dispersing significantly. Therefore, such light sources support interesting applications in nonlinear spectroscopy such as multiplex-CARS, as we have recently shown in Refs. [1], [2].I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.


