We review a number of instruments employed in a high-intensity J-KAREN-P laser-solid interaction experiment and discuss the applicability of the diagnostics to the best target position determination with a ~10 μm accuracy, while the focal spot size was ~1 μm and peak intensity was up to 7×1021 W/cm2. We discuss both front- and back-side diagnostics, some of them operated in the infrared, visible and ultraviolet ranges, while others in the extreme ultraviolet, soft X-ray and gamma-ray ranges. We found that the applicability of some of the instruments to the best at-focus target position determination depends on the thickness of the target.
The spatio-temporal and polarisation properties of intense light is important in wide-ranging topics at the forefront of intense light-matter interactions, including laser-driven particle acceleration. In the context of experiments to optimize transparency-enhanced ion acceleration in expanding ultrathin foils, we investigate the polarisation and temporal properties of intense light measured at the rear of the target. An effective change in the angle of linear polarisation of the light results from a superposition of coherent radiation, generated by a directly accelerated bipolar electron distribution, and the light transmitted due to the onset of relativistic self-induced transparency. Simulations show that the generated light has a high-order transverse electromagnetic mode structure in both the first and second laser harmonics that can evolve on intra-pulse time-scales. The mode structure and polarisation state vary with the interaction parameters, opening up the possibility of developing this approach to achieve dynamic control of structured light fields at ultrahigh intensities [1].
We also report on frequency-resolved optical gating measurements of the light which demonstrate a novel and simple approach to diagnose the time during the interaction at which the foil becomes transparent to the laser light. This is a key parameter for optimising ion acceleration in expanding ultrathin foils. Coherent transition radiation produced at the foil rear interferes with laser light transmitted through the foil producing spectral fringes. The fringe spacing enables the relative timing of the onset of transmission with respect to the transition radiation generation to be determined. This self-referencing approach to spectral interferometry provides a route to optically controlling and optimising ion acceleration from ultrathin foils undergoing transparency [2].
[1] M.J. Duff et al., Scientific Reports 10, 105 (2020)
[2] S.D.R. Williamson et al., Phys. Rev. Applied 14, 034018 (2020)
In this work, a theoretical and model study of the temperature effects on threshold current, as tuning technique, and the
comparison with experimental results of quantum dot (QD) diode lasers is presented. It is well known the dependence of
output wavelength with temperature in semiconductor lasers. This property can be highly useful in order to obtain stable
and easy tuning lasers getting two different specific wavelengths to achieve signals in the millimetre (mmW) and
terahertz (THz) ranges by photomixing. Our model and study over QD lasers allow us to understand the behaviour of
temperature inside the device and thus, we can estimate the best characteristics to obtain the desired results.
In this work, we study and investigate the thermally effects on the compact continuous wave (CW) distributed feedback
(DFB) laser as a tuning method using an external platinum μ-heater film in a vertical and lateral configurations. A low
injection current into platinum heater produces the variation temperature inside the active and grating regions to shift the
lasing wavelength. The frequency is continuously tuned up to 3 THz at operation wavelength of 937 nm, by controlling
the temperature of the laser to achieve sub-millimetre (sub-mmW) and terahertz (THz) signals generation by
photomixing.
In this paper, a theoretical investigation of the coupling phenomena of two laterally coupled diode lasers is
presented. The analysis is centered in a new dynamic modeling of laterally coupled diode lasers where the modulation
response shows additional resonance that is beyond the normal relaxation oscillation frequency. This additional
resonance is attributed to the coupling effect between the two coupled diode lasers. We present results obtained with this
new model and we compare them with previous experimental results in order to demonstrate the good agreement
between them.
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