The interaction of intense ultrashort laser pulses with cryogenic He jets

TL;DR

This study uses advanced simulations to explore how intense ultrashort laser pulses interact with cryogenic helium jets, revealing ionization dynamics, extreme plasma conditions, and potential experimental diagnostics relevant for high-energy density physics.

Contribution

It provides new insights into ionization propagation, transient fields, and plasma states in cryogenic helium jets under intense laser irradiation, with implications for high-energy density experiments.

Findings

Ionization front propagates along the jet at a fraction of the speed of light.

Ionized regions reach solid-like densities and high temperatures.

Plasmon and non-collective modes are generated, proportional to ionized volume.

Abstract

We study the interaction of intense ultrashort laser pulses with cryogenic He jets using 2d/3v relativistic Particle-in-Cell simulations (XOOPIC). Of particular interest are laser intensities $(10^{15}-10^{20})$ W/cm$^2$, pulse lengths $\le 100$ fs, and the frequency regime $\sim 800$ nm for which the jets are initially transparent and subsequently not homogeneously ionized. Pulses $\ge 10^{16}$ W/cm$^2$ are found to drive ionization along the jet and outside the laser spot, the ionization-front propagates along the jet at a fraction of the speed of light. Within the ionized region, there is a highly transient field, which may be interpreted as two-surface wave decay and as a result of the charge-neutralizing disturbance at the jet-vacuum interface. The ionized region has solid-like densities and temperatures of few to hundreds of eV, i.e., warm and hot dense matter regimes. Such extreme conditions are relevant for high-energy densities as found, e.g., in shock-wave experiments and inertial confinement fusion studies. The temporal evolution of the ionization is studied considering theoretically a pump-probe x-ray Thomson scattering (XRTS) scheme. We observe plasmon and non-collective modes that are generated in the jet, and their amplitude is proportional to the ionized volume. Our theoretical findings could be tested at free-electron laser facilities such as FLASH and the European XFEL (Hamburg) and the LCLS (Stanford).