Jérôme Lhermite’s research while affiliated with Centre Lasers Intenses et Applications and other places

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Publications (14)


Compression of a repetition-rate tunable electro-optic laser in the multiGHz regime
  • Conference Paper

June 2025

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10 Reads

Duncan Sarton

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Jérôme Lhermite

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Jean-Christophe Delagnes

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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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81 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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Schematic of the experimental setup used for the experiments described in this Letter. EOM stands for electro-optic modulator; AOM for acousto-optic modulator; PBS for polarizing beam splitter; CVBG for chirped volume Bragg grating; PDH for Pound–Drever–Hall; and PD for photodiode; and CCD is a beam profiler.
Average power stacked in the OEC versus the input average power.
Beam radius (at $1/e^2$ of intensity profile), measured on a camera 67 cm downstream from the output mirror, as a function of the average power in the OEC. Points in red (squares) and blue (diamonds) show measurements made during the first and second run showing excellent consistency. The black solid line is the expected beam radius on the camera, only accounting for the change of ROC of the mirrors due to thermal loading of the OEC. The dashed line further accounts for thermal lensing in the bulk of M $_2$ assuming a coating absorption of $0.36$ ppm, as explained in the text. The gray band represents a variation of the coating absorption by about 10%.
(Left) Beam profile as measured on the camera at 650 kW. (Right) Corresponding projections in the horizontal (up) and vertical (down) axes are given with colored dots. The black line is a Gaussian fit of these data. The beam remains circular with no obvious presence of high-order mode degeneracy.
Simulation of the optimum waist size versus the optimum waist position of the input laser beam relative to the input mirror, accounting for thermal lensing in M $_1$ (solid black line and dots). Encircled regions corresponding to the coupling coefficient related to transverse mode-matching in excess of 90% for 100 kW, 200 kW, 500 kW, and 1 MW in this plane, with their optimum shown with a marker. The M $_1$ mirror absorption is assumed to be of $a_1=0.56$ ppm.
710 kW stable average power in a 45,000 finesse two-mirror optical cavity

November 2024

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73 Reads

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6 Citations

Very high-average optical enhancement cavities (OECs) are being used both in fundamental and applied research. The most demanding applications require stable megawatt level average power of infrared picosecond pulses with repetition rates of several tens of MHz. Toward reaching this goal, we report on the achievement of 710 kW of stable average power in a two-mirror hemispherical optical enhancement cavity. This result further improves the state of the art. So far, in compact high-power systems, cavity geometry optimization has been driven by the need to limit the deformation of radii of curvatures due to thermal effects. Here we explicitly demonstrate that thermal lensing must be accounted for, too, and that it can be used to assess the absorption of coatings. Experimental observations are matched with a simple model of thermal effects in the mirror’s coatings. These results set a further stage for designing an optimized optical system for several applications where very high-average power enhancement cavities are expected to be operated.


First production of X-rays at the ThomX high-intensity Compton source

May 2024

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134 Reads

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6 Citations

The European Physical Journal Plus

With the increase in laser power and finesse of optical cavities over the last decade, laboratory-size Compton sources are very promising. These sources produce X-rays through interactions between relativistic electrons and laser photons and, in term of brightness, fall between large synchrotron facilities and classical laboratory X-ray sources. The ThomX source is the French project in this field. This article first presents a state of the art of high-intensity Compton sources, then the ThomX source is briefly described, and the first results are detailed, in particular the production of the first X-rays, the acquisition of the first spectrum and the first image of the beam. Finally, the next objectives are discussed.


Fabrication and characterization of tapered photonic crystal fiber for broadband 2 µm: four-wave mixing-based fibered OPCPA

April 2023

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153 Reads

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1 Citation

Applied Physics B

We present the simulation, fabrication, and characterization of large area microstructured fiber tapers which enables broadband phasematching conditions of the four wave-mixing process. These silica-based tapers are intended to serve as a nonlinear gain medium for intense and high average power Fiber Optical Parametric Chirped Pulse Amplifier emitting at 2 μm\upmu \hbox {m} and strongly pumped at Yb wavelength. Different geometries (tapered/untapered, aspect ratio, etc.) are fabricated, analyzed and their broadening properties—key for supporting ultrashort pulses amplification—are compared and discussed. The characterization of nonlinear gain bandwidth of the tapers relies on a tunable source of stochastic pulses based on tunable amplified spontaneous emission in Yb-doped amplifiers. The strong overshoots of this source allows degenerate four-wave mixing process to occur thus generating broadband incoherent visible signal and mid-infrared idler waves at much lower average power than usually needed with coherent pumping. The idler centered around 1.85 μμ\mum is broadened due to zero-dispersion wavelength shift along the taper.





Citations (5)


... A standard watt-level laser with a pulse repetition rate in the range from 40 MHz to several GHz can be coupled to an external EC that boosts the pulse energy by coherently summing multiple pulses, and, depending on the finesse of the cavity, passive gains of the order of thousands can be reached. [29][30][31][32] However, cavity-enhanced THz generation has experienced only limited progress, in contrast to the success of ECs in frequency upconversion. [33][34][35] To the best of our knowledge, only one attempt at using femtosecond EC for THz generation was made in 2008 by Theuer et al. 36 This experiment was based on cavityenhanced OR inside bulk lithium niobate in Cherenkov-radiation type geometry. ...

Reference:

Ytterbium-laser-driven THz generation in thin lithium niobate at 1.9 kW average power in a passive enhancement cavity
710 kW stable average power in a 45,000 finesse two-mirror optical cavity

... In summer 2023, the first x-rays were detected [68]. X-ray production was done in a nonsynchronized mode between electron bunches and laser pulses from a locked Fabry-Perot cavity, and with the storage ring nominal optics working at 500.38 MHz (see Sec. III B). ...

First production of X-rays at the ThomX high-intensity Compton source
  • Citing Article
  • May 2024

The European Physical Journal Plus

... Une possibilité intéressante seraitégalement dŠutiliser une Ąbre ' a cristaux photoniqueś etirée (taper). Dans uneétude publiée par Ahmedou et al. [149], les auteurs ont utilisé ce type de Ąbre aĄn de modiĄer la longueur dŠonde de zéro de dispersion le long de la Ąbre, permettant ainsi de générer un continuum par mélange ' a quatre ondes, et donc des impulsions plus courtes que celle générées dans une Ąbre similaire mais nonétirée. LŠutilisation de ce type de Ąbre en cavité permettrait de développer des sources ultracourtes présentant des spectres plus important que des lasers classiques, ou encore ' a des longueur dŠondes exotiques. ...

Fabrication and characterization of tapered photonic crystal fiber for broadband 2 µm: four-wave mixing-based fibered OPCPA

Applied Physics B

... Another approach consists in generating Fourier-transform-limited pulses with durations of tens of picoseconds starting from a single-frequency continuous-wave (CW) seed laser gated by a high-speed electro-optic intensity modulator (EOM), which offers more flexibility and better quality pulses with an adjustable repetition rate [8]. Using this method, Renard et al. [9] developed an ultrashort laser source derived from a CW seed emitting at 1030 nm. The picosecond pulses carved by the EOM were then spectrally broadened through self-phase modulation (SPM) within a long passive fiber. ...

Agile femtosecond synchronizable laser source from a gated CW laser
  • Citing Article
  • July 2022

Laser Physics Letters

... The amplifier cell was qualified at different repetition rates from one shot per few minutes to one shot per minute. Emphasis is herein placed on assessment of mid spatial scale [1 mm -10 mm] distortions in amplified wavefronts commonly observed in fluid-cooled amplifiers [25,26]. Such wavefront defects in large-aperture multi-slabs laser systems are likely to degrade the focal point quality and, in the worst case, damage optical materials due to Kerr effects and/or amplitude modulation during laser beam propagation [17,27]. ...

Index-leveling for forced-flow turbulent face-cooling of laser amplifiers