Enhanced coherent transition radiation from midinfrared-laser-driven microplasmas

Abstract

AbstractWe present a particle-in-cell (PIC) analysis of terahertz (THz) radiation by ultrafast plasma currents driven by relativistic-intensity laser pulses. We show that, while the I0$${\lambda }_{0}^{2}$$ λ 0 2 product of the laser intensity I0 and the laser wavelength λ0 plays the key role in the energy scaling of strong-field laser-plasma THz generation, the THz output energy, WTHz, does not follow the I0$${\lambda }_{0}^{2}$$ λ 0 2 scaling. Its behavior as a function of I0 and λ0 is instead much more complex. Our two- and three-dimensional PIC analysis shows that, for moderate, subrelativistic and weakly relativistic fields, WTHz(I0$${\lambda }_{0}^{2}$$ λ 0 2 ) can be approximated as (I0λ02)α, with a suitable exponent α, as a clear signature of vacuum electron acceleration as a predominant physical mechanism whereby the energy of the laser driver is transferred to THz radiation. For strongly relativistic laser fields, on the other hand, WTHz(I0$${\lambda }_{0}^{2}$$ λ 0 2 ) closely follows the scaling dictated by the relativistic electron laser ponderomotive potential $${\mathscr{F}}_{{\text{e}}}$$ F e , converging to WTHz ∝ $${I}_{0}^{1/2}{\lambda }_{0}$$ I 0 1 / 2 λ 0 for very high I0, thus indicating the decisive role of relativistic ponderomotive charge acceleration as a mechanism behind laser-to-THz energy conversion. Analysis of the electron distribution function shows that the temperature Te of hot laser-driven electrons bouncing back and forth between the plasma boundaries displays the same behavior as a function of I0 and λ0, altering its scaling from (I0λ02)α to that of $${\mathscr{F}}_{{\text{e}}}$$ F e , converging to WTHz ∝ $${I}_{0}^{1/2}{\lambda }_{0}$$ I 0 1 / 2 λ 0 for very high I0. These findings provide a clear physical picture of THz generation in relativistic and subrelativistic laser plasmas, suggesting the THz yield WTHz resolved as a function of I0 and λ0 as a meaningful measurable that can serve as a probe for the temperature Te of hot electrons in a vast class of laser–plasma interactions. Specifically, the α exponent of the best (I0λ02)α fit of the THz yield suggests a meaningful probe that can help identify the dominant physical mechanisms whereby the energy of the laser field is converted to the energy of plasma electrons.