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V. Vaičaitis

Publications and source records attributed to V. Vaičaitis.

3 recordsLinked to original sources

Four-wave mixing and secondary radiations generated by nonharmonic two-color filaments in air: Influence of the Kerr and plasma nonlinearities

Four-wave mixing (FWM) is an efficient source of light waves emitted at various frequencies, usually associated with third-order optical nonlinearities. Whereas attention has mostly been paid in the past to the generation of Stokes (e.g., visible) modes by mixing two nonharmonic frequencies in degenerate FWM, the present work aims to analyze the weaker components, i.e., the anti-Stokes (resp. mid-IR) radiation and cascaded satellites, and characterize their conversion efficiency and tunability. Here we report the production of tunable mid-infrared radiation around 3.3 $μ$m delivered by two-color femtosecond filaments in air combining $\sim 800$ nm fundamental and $\sim 1.3$ $μ$m seed waves. Although the Kerr response of air plays a key role in creating both visible and mid-IR radiations, we show that plasma nonlinearities also contribute by broadening and mixing the pump frequencies. Two experimental setups are exploited to focus, separately, on the production of FWM modes and cascaded satellites - called secondary radiations. A first filamentation setup employing different focal lengths for the two colors displays an ionization-induced broadening of the mid-IR radiation during the plasma stage. A second setup focusing the two pump components over equal propagation distances allows us to unveil the secondary radiations emerging at lower intensity levels when plasma occurs. We examine which player, among the plasma- or Kerr-induced FWM, is the most active in the conversion process. Numerical simulations based on a local-current model and a unidirectional solver highlight the role of the Kerr stage in amplifying the FWM radiations prior to the development of the weaker satellites in plasma regime. Their results, agreeing well with the experimental data, demonstrate that a broad visible emission is needed to trigger secondary radiations.

physics.optics↗

All-optical attoclock for imaging tunnelling wavepackets

Recent experiments on measuring time-delays during tunnelling of cold atoms through an optically created potential barrier are reinvigorating the controversial debate regarding possible time-delays during light-induced tunnelling of an electron from an atom. Compelling theoretical and experimental arguments have been put forward to advocate opposite views, confirming or refuting the existence of finite tunnelling time delays. Yet, such a delay, whether present or not, is but a single quantity characterizing the tunnelling wavepacket; the underlying dynamics are richer. Here we propose to augment photo-electron detection in laser-induced tunnelling with detection of light emitted by the tunnelling electron -- the so-called Brunel radiation. Using a combination of single-color and two-color driving fields, we identify the all-optical signatures of the re-shaping of the tunnelling wavepacket as it emerges from the tunnelling barrier and moves away from the core. This reshaping includes not only an effective time-delay but also time-reversal asymmetry of the ionization process, which we describe theoretically and observe experimentally. We show how both delay and reshaping are mapped on the polarization properties of the Brunel radiation, with different harmonics behaving as different hands of a clock moving at different speeds. The all-optical detection paves the way to time-resolving optical tunnelling in condensed matter systems, e.g. tunnelling across bandgaps in solids, on the attosecond time-scale.

physics.optics↗

Terahertz pulse generation by two-color laser fields with circular polarization

We study the influence of the polarization states of femtosecond two-color pulses ionizing gases on the emitted terahertz radiation. A local-current model and plane-wave evaluations justify the previously-reported impact on the THz energy yield and an (almost) linearly-polarized THz field when using circularly-polarized laser harmonics. For such pump pulses, the THz yield is independent on the relative phase between the two colors. When the pump pulses have same helicity, the increase in the THz yield is associated to longer ionization sequences and higher electron transverse momenta acquired in the driving field. Reversely, for two color pulses with opposite helicity, the dramatic loss of THz power comes from destructive interferences driven by the highly symmetric response of the photocurrents lined up on the third harmonic of the fundamental pulse. While our experiments confirm an increased THz yield for circularly polarized pumps of same helicity, surprisingly, the emitted THz radiation is not linearly-polarized. This effect is explained by means of comprehensive 3D numerical simulations highlighting the role of the spatial alignment and non-collinear propagation of the two colors.

physics.optics↗