Marie-Christine Nadeau’s research while affiliated with French National Centre for Scientific Research and other places

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Publications (10)


Physics and technology of liquid face-cooling for multi-kiloWatt Yb-YAG laser amplifiers
  • Conference Paper

June 2025

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10 Reads

Philippe Balcou

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Christophe Féral

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Stéphane Petit

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[...]

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Commissioning of ThomX Compton source subsystems and demonstration of 10 10 x-rays/s
  • Article
  • Full-text available

February 2025

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80 Reads

Physical Review Accelerators and Beams

ThomX is a compact x-ray source based on Compton scattering, installed at IJCLab (Laboratoire de physique des 2 infinis-Irène Joliot-Curie) in Orsay. The machine uses a small electron storage ring and an intense laser pulse stored in a high-finesse optical cavity. This article describes the various subsystems of the machine and their initial results of the commissioning, which began in mid-2021. This first commissioning phase led to the production of 10 10 x-rays/s with an on-axis energy of 45 keV. The main steps to be taken to reach the nominal flux are outlined at the end. Published by the American Physical Society 2025

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Noise performances of a high-power picosecond Nd:YVO4 oscillator

February 2011

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15 Reads

Proceedings of SPIE - The International Society for Optical Engineering

We report on an experimental investigation of the noise properties of an free-running, high-power, picosecond Nd:YVO4 oscillator pumped by a 100 W laser diode. The amplitude noise has been measured with a photodiode and an electronic spectrum analyser, and then compared with other mode-locked oscillator's noise spectrum. We show that in terms of noise properties, our powerful oscillator is comparable with low-power oscillators such like low-noise Ti:Sapphire oscillators. We also show that the frequency doubling does not affect the amplitude noise of the oscillator. High power diode pumping is then not an issue to get low-noise high-power oscillators.



Oscillator setup: M 1 , concave mirror, ROC 0.5   m ; M 2 , M 5 , plane mirror; M 3 , M 4 , convex mirror, ROC − 1.25   m ; OC, output coupler. For a cavity length of 1.64   m , the laser crystal is placed at 31   cm from the OC.
Average output power versus absorbed pump power for two different OCs. Limits between QML and CML regimes are also shown for each OC. In insets, M 2 measurement and far-field beam profile at full pump power with OC = 8 % .
Pulse duration versus output coupler transmission and associated average output power. Dots represent the experimental data, and the solid curve is the simulation predicted by Haus’s theory (Eq. 4.11 with FWHM in [18]). In insets, the autocorrelation traces and their sech 2 fit for 5% and 38% OC.
Average output power versus pulse duration. Square dots represent our experimental data from changing only the OC. The other points show a non-exhaustive but representative set of results for several Nd : Y V O 4 oscillators found in the literature (the number attached to the data is the reference). From the analysis of each article, + represent oscillators with SHB and − without SHB.
Picosecond pulses of variable duration from a high-power passively mode-locked Nd : Y V O 4 laser free of spatial hole burning

May 2010

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24 Reads

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10 Citations

We report on a high-power passively mode-locked TEM 00 Nd : Y V O 4 oscillator, 888 nm diode-pumped, with pulse durations adjustable between 46 ps and 12 ps . The duration tunability was obtained by varying the output coupler (OC) transmission while avoiding resorting to spatial hole burning (SHB) for pulse shortening. At a repetition rate of 91 MHz and for an output power ranging from 15 W to 45 W , we produced SHB-free 12 - ps - to 32 - ps -long pulses. Within this range of power, these are the shortest pulse durations obtained directly from Nd : Y V O 4 oscillators.


High-power passively mode-locked Nd:YVO4 oscillator with adjustable pulse duration between 46 ps and 12 ps

April 2010

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29 Reads

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2 Citations

Proceedings of SPIE - The International Society for Optical Engineering

We report on a high-power, passively mode-locked, TEM00 Nd:YVO4 oscillator with adjustable pulse duration between 46 and 12ps. The laser is end-pumped by an 888nm laser diode and mode-locking is achieved with a semiconductor saturable absorber mirror (SESAM). The laser has a repetition rate of 91MHz and the M2 beam quality factor is better than 1.2 at 15ps. At the optimum output coupler, it provides a maximum average output power of 45W with 32ps pulse duration. In literature, the presence of spatial hole burning (SHB) often helps to shorten the pulse length down to few picoseconds. However, SHB might be an issue for some specific application requiring e.g. low noise picosecond oscillators. In this contribution, we demonstrate that it is possible to shorten the pulse duration by lowering the intracavity losses without SHB. Pulse tunability from 46 to 12ps is achieved by changing the output coupler of the cavity while staying in the continuous-wave mode-locked regime. Pulse duration is almost linear with the output coupler transmission and increases from 12 to 32ps with average output power ranging from 15 to 45W. In this range of output power, we demonstrate the shortest pulses directly from a Nd:YVO4 oscillator.

Citations (1)


... Nd:YVO 4 enjoys large absorption and stimulated emission cross sections that may easily lead to high gain but weak thermal property due to the low thermal conductivity and high energy transfer upconversion (ETU) coefficient. In addition, an 888 nm pumping scheme is an effective way to compensate thermal effect for output properties upgrading in Nd:YVO 4 laser, which has been widely used in Q-switched [3], mode-locked [4,5] oscillators, pulse amplifiers [6,7] and optical parametric technology [8]. In particular, high-power Q-switched neodymium pulse lasers are widely used in laser machining manufacture [9] and the thermal effect is a key factor. ...

Reference:

Four-Dimensional Thermal Analysis of 888 nm Pumped Nd:YVO4 Dual-Rod Acousto-Optic Q-Switched Laser
Picosecond pulses of variable duration from a high-power passively mode-locked Nd : Y V O 4 laser free of spatial hole burning