Stéphane Petit’s research while affiliated with Université Bordeaux-I and other places

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Publications (93)


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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Figure 1: Experimental Scheme and Concept of Floquet Valleytronics. (a) A polarization-tunable in-
Figure 2: Valley-and Polarization-Resolved Quantum Path Interference Between Floquet-Bloch and
Figure 3: Valley-Polarized Floquet-Bloch States in 2H-WSe 2 . (a) Energy-momentum cut along K-Γ-K ′
Figure 4: XUV Photoemission Circular Dichroism and Orbital Character of Light-Dressed States. (a) Experimentally measured energy-momentum cut along K-Γ-K ′ direction, at pump-probe overlap, using
Floquet-Bloch Valleytronics

December 2024

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82 Reads

Driving quantum materials out-of-equilibrium makes it possible to generate states of matter inaccessible through standard equilibrium tuning methods. Upon time-periodic coherent driving of electrons using electromagnetic fields, the emergence of Floquet-Bloch states enables the creation and control of exotic quantum phases. In transition metal dichalcogenides, broken inversion symmetry within each monolayer results in a non-zero Berry curvature at the K and K^{\prime} valley extrema, giving rise to chiroptical selection rules that are fundamental to valleytronics. Here, we bridge the gap between these two concepts and introduce Floquet-Bloch valleytronics. Using time- and polarization-resolved extreme ultraviolet momentum microscopy combined with state-of-the-art ab initio theory, we demonstrate the formation of valley-polarized Floquet-Bloch states in 2H-WSe2_2 upon below-bandgap coherent electron driving with chiral light pulses. We investigate quantum path interference between Floquet-Bloch and Volkov states, showing that this interferometric process depends on the valley pseudospin and light polarization-state. Conducting extreme ultraviolet photoemission circular dichroism in these nonequilibrium settings reveals the potential for controlling the orbital character of Floquet-engineered states. These findings link Floquet engineering and quantum geometric light-matter coupling in two-dimensional materials. They can serve as a guideline for reaching novel out-of-equilibrium phases of matter by dynamically breaking symmetries through coherent dressing of winding Bloch electrons with tailored light pulses.


Figure 1. Schematic of the experiment. (a) An infrared pump and a polarization-tunable (s-or p-polarized) XUV (21.6 eV) probe pulses are focused onto an MBE-grown 1T-ZrTe 2 sample, in the interaction chamber of a time-of-flight momentum microscope, at an incidence angle of 65°. (b) Constant energy contours for different binding energies, obtained by summing photoemission intensities measured with s-and p-polarized XUV. These measurements were taken at the pump−probe temporal overlap, with an s-polarized IR pump pulse (1.2 eV, 135 fs, 2.95 mJ/cm 2 ). The light scattering plane (orange tilted rectangle overlaid with CEC in (b)) is aligned with the crystal mirror plane , i.e., is along the Γ−M direction.
Figure 2. Linear dichroism in photoexcited 1T-ZrTe 2 . Band structure mapping of 1T-ZrTe 2 along the M−Γ−M direction, at pump−probe overlap (Δt = 0 ps), using an s-polarized pump pulse to avoid the spurious effect of laser-assisted photoemission. (a) Raw signal (unnormalized) obtained by summing photoemission intensities measured using an s-and p-polarized XUV probe pulse. (b) XUV LDAD extracted by subtracting the photoemission intensities measured using p-and s-polarized XUV probe pulses. (c) Normalized photoemission intensity measured using s-polarized XUV probe pulses. (d) Normalized photoemission intensity measured using ppolarized XUV probe pulses. In (c) and (d), each momentumresolved energy slice of the photoemission intensity is normalized by its maximum value.
Figure 3. Excited state band mapping. (a) Normalized energymomentum cut along the M−Γ−M direction at pump−probe overlap (Δt = 0 ps). The IR pump and the XUV probe are s-polarized. (b) Second derivative analysis of the energy-momentum cut along the M−Γ−M direction shown in (a). The second derivative presented in (b) is calculated by summing the second derivatives along the momentum and energy axes. More details about the second derivative procedure can be found in the Supporting Information.
Figure 5. Schematic of ultrafast nonequilibrium carrier dynamics in 1T-ZrTe 2 . The vertical dashed gray lines represent optical transitions leading to initial electron and hole creation. The horizontal light gray arrow represents interband transitions, while the curved black arrows represent intravalley scattering. Shaded red and blue areas represent the accumulation of electrons and holes, above and below the Fermi level.
Excited State Band Mapping and Ultrafast Nonequilibrium Dynamics in Topological Dirac Semimetal 1T-ZrTe2

October 2024

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50 Reads

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1 Citation

Nano Letters

We performed time- and polarization-resolved extreme ultraviolet momentum microscopy on the topological Dirac semimetal candidate 1T-ZrTe2. Excited state band mapping uncovers the previously inaccessible linear dispersion of the Dirac cone above the Fermi level. We study the orbital texture of bands using linear dichroism in photoelectron angular distributions. These observations provide hints about the topological character of 1T-ZrTe2. Time-, energy-, and momentum-resolved nonequilibrium carrier dynamics reveal that intra- and interband scattering processes play a major role in the relaxation mechanism, leading to multivalley electron–hole accumulation near the Fermi level. We also show that electrons’ inverse lifetime has a linear dependence as a function of their excess energy. Our time- and polarization-resolved XUV photoemission results shed light on the excited state electronic structure of 1T-ZrTe2 and provide valuable insights into the relatively unexplored field of quantum-state-resolved ultrafast dynamics in 3D topological Dirac semimetals.


Figure 1: Schematic of the experiment. (a) An infrared pump and a polarizationtunable (s-or p-polarized) XUV (21.6 eV) probe pulses are focused onto an MBE-grown 1T-ZrTe 2 sample, in the interaction chamber of a time-of-flight momentum microscope, at an incidence angle of 65 • . (b) Constant energy contours for different binding energies, obtained by summing photoemission intensities measured with s-and p-polarized XUV. These measurements were taken at the pump-probe temporal overlap, with an s-polarized IR pump pulse (1.2 eV, 135 fs, 2.95 mJ/cm 2 ). The light scattering plane (orange tilted rectangle overlaid with CEC in (b)) is aligned with the crystal mirror plane M, i.e. is along the Γ-M direction.
Figure 2: Linear Dichroism in Photoexcited 1T-ZrTe 2 . Band structure mapping of 1T-ZrTe 2 along M-Γ-M direction, at pump-probe overlap (∆t = 0 ps), using s-polarized pump pulse to avoid spurious effect of laser-assisted photoemission. (a) Raw signal (unnormalized) obtained by summing photoemission intensities measured using s-and p-polarized XUV probe pulse. (b) XUV LDAD extracted by subtracting the photoemission intensities measured using p-and s-polarized XUV probe pulses. (c) Normalized photoemission intensity measured using s-polarized XUV probe pulses. (d) Normalized photoemission intensity measured using p-polarized XUV probe pulses. In (c)-(d), each momentum-resolved energy slice of the photoemission intensity is normalized by its maximum value.
Figure 3: Excited State Band Mapping. (a) Normalized energy-momentum cut along M-Γ-M direction at pump-probe overlap (∆t = 0 ps). The IR pump and the XUV probe are s-polarized. (b) Second derivative analysis of the energy-momentum cut along M-Γ-M direction shown in (a). The second derivative presented in (b) is calculated by summing the second derivatives along the momentum and energy axes. More details about the second derivative procedure can be found in the Supporting Information.
Figure 7: Band structure mapping and 2 nd derivative analysis (a) Normalized energymomentum cut along M-Γ-M direction at pump-probe overlap (∆t = 0 ps). Both the IR pump and the XUV probe ares-polarized. (b) Second derivative analysis of the energymomentum cut along M-Γ-M direction shown in (a). The second derivative presented in (b) is calculated by summing the second derivatives along the momentum (c) and energy axes (d).
Excited States Band Mapping and Ultrafast Nonequilibrium Dynamics in Topological Dirac Semimetal 1T-ZrTe$_2

September 2024

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49 Reads

We performed time- and polarization-resolved extreme ultraviolet momentum microscopy on topological Dirac semimetal candidate 1T-ZrTe2_2. Excited states band mapping uncovers the previously inaccessible linear dispersion of the Dirac cone above the Fermi level. We study the orbital texture of bands using linear dichroism in photoelectron angular distributions. These observations provide hints on the topological character of 1T-ZrTe2_2. Time-, energy- and momentum-resolved nonequilibrium carrier dynamics reveal that intra- and inter-band scattering processes play a capital role in the relaxation mechanism, leading to multivalley electron-hole accumulation near the Fermi level. We also show that electrons' inverse lifetime has a linear dependence on their binding energy. Our time- and polarization-resolved XUV photoemission results shed light on the excited state electronic structure of 1T-ZrTe2_2 and provide valuable insights into the relatively unexplored field of quantum-state-resolved ultrafast dynamics in 3D topological Dirac semimetals.


Mitigating space charge in time-resolved photoelectron spectroscopy to study laser-heated copper dynamics in the high fluence regime

May 2024

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38 Reads

Physical Review B

The performance of time-resolved photoelectron spectroscopy for the study of subpicosecond dynamics of laser-heated solids is often limited by space charge effects. The consequent shift and distortion of the photoelectron spectrum induced by electrons emitted by the ultrashort pump pulse is studied here using a fully coherent approach based on experimental measurements and space charge calculations. The temporal dynamics of the valence band of a copper sample is recorded before and after an 800 nm laser pump excitation at a fluence of 750mJ/cm2. The probe pulse is produced using a laboratory-based high-harmonics source delivering 25 fs pulses up to 100 eV photon energy. We extract the laser-heating contribution by comparing these measurements with space charge calculations based on particle-in-cell simulations of the pump and probe electron clouds mutual interaction on their way to the detector. The deduced picosecond dynamics associated to the electronic density of states shift is attributed to lattice changes with the help of hydrodynamic simulations including the two-temperature model.


Laser-Induced Electron Diffraction in Chiral Molecules

February 2024

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234 Reads

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10 Citations

Physical Review X

Strong laser pulses enable probing molecules with their own electrons. The oscillating electric field tears electrons off a molecule, accelerates them, and drives them back toward their parent ion within a few femtoseconds. The electrons are then diffracted by the molecular potential, encoding its structure and dynamics with angstrom and attosecond resolutions. Using elliptically polarized laser pulses, we show that laser-induced electron diffraction is sensitive to the chirality of the target. The field selectively ionizes molecules of a given orientation and drives the electrons along different sets of trajectories, leading them to recollide from different directions. Depending on the handedness of the molecule, the electrons are preferentially diffracted forward or backward along the light propagation axis. This asymmetry, reaching several percent, can be reversed for electrons recolliding from two ends of the molecule. The chiral sensitivity of laser-induced electron diffraction opens a new path to resolve ultrafast chiral dynamics. Published by the American Physical Society 2024



Fast and precise chiroptical spectroscopy by photoelectron elliptical dichroism

June 2023

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170 Reads

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11 Citations

Physical Chemistry Chemical Physics

The photoionization of chiral molecules by elliptically polarized femtosecond laser pulses produces photoelectron angular distributions which show a strong and enantio-sensitive forward/backward asymmetry along the light propagation direction. We report on high precision measurements of this photoelectron elliptical dichroism (PEELD). Using an optical cavity to recycle the laser pulses and increase the signal-to-noise ratio, we determine enantiomeric excesses with a 0.04% precision with a low-power femtosecond laser (4 W) in a compact scheme. We perform momentum-resolved PEELD measurements in 16 molecules, from volatile terpenes to non-volatile amino acids and large iodoarenes. The results demonstrate the high structural sensitivity of PEELD, confirming the spectroscopic interest of this technique. Last, we show how a convolutional neural network can be used to retrieve the chemical and enantiomeric composition of a sample from the momentum-resolved PEELD maps.


Citations (43)


... The proposed scheme establishes a benchmark for generating well-defined 3D laser fields under realistic experimental conditions and opens a path toward systematic studies of strong-field ionization in 3D light fields a new class of experiments. Beyond fundamental interest, such 3D fields could enable all-optical enantiopurification [24], the generation of chiral bound electronic states [28], advances in laser-induced electron diffraction [44,45], and the investigation of sub-cycle interferences [8,[46][47][48]. Eventually, 3D laser fields may also be combined with pump-probe schemes using non-collinear laser beams [49]. ...

Reference:

Chiral Electron Momentum Distribution upon Strong-Field Ionization of Atoms
Laser-Induced Electron Diffraction in Chiral Molecules

Physical Review X

... A chiral nuclear scaffold gives rise to a chiral potential and imprints a notion of handedness on the system which can be probed and measured via suitable observables. Prominent examples for such observables are microwave three-wave mixing [6-13], circular dichroism (CD) [14][15][16][17][18][19], and photoelectron circular dichroism (PECD) [20][21][22][23][24][25][26][27][28], with the latter allowing for large anisotropies in many molecular species. While it has been shown that PECD in the gas phase is strongly affected by short-range interactions [29], it was recently demonstrated that even in a hydrogen atom, excitations to chiral intermediate states lead to a PECD signal despite the absence of a chiral short-range potential [30]. ...

Fast and precise chiroptical spectroscopy by photoelectron elliptical dichroism

Physical Chemistry Chemical Physics

... 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

... [19,[27][28][29][30] However, when the laser frequency approaches the energy gap between specific ionic states, strong coupling between these states can occur, possibly leaving a distinct fingerprint in the HHS. [31][32][33] Recent work by Shu et al. [31] identified two groups of minimum structure for the short trajectory harmonics. One dip located at lower order is independent of laser intensity and the other at higher order shifts with changing laser intensity. ...

Quantum-Path Resolved Attosecond High-Harmonic Spectroscopy
  • Citing Article
  • February 2023

Physical Review Letters

... In fact, ns laser irradiation at 2.9 μm has already been considered as an attempt to avoid the use of sacrificial layers in nozzle-less LIFT. 29 Another limitation in our approach is the requirement for micromachining commercially available capillaries, as fs-machining equipment can be expensive and not widely available. However, several companies commercially offer fs-machining services, providing a potential solution for those lacking access to the necessary infrastructure. ...

Plasma-free bubble cavitation in water by a 2.9 μ m laser for bioprinting applications

... Ideally, the driving laser maintains the ring shape while the harmonic field exhibits low divergence in the far field, enabling spatial separation of the two fields. 43 This approach has been examined in numerous experiments, including measurements of harmonic efficiency, which demonstrated only a 27% reduction as compared to using a full Gaussian beam, 44 generation of high-flux harmonics, 47,48 and production of attosecond pulse trains covering 30-70 eV with pulse energies up to 51 pJ/shot. 45 Furthermore, Jin et al. 46 systematically investigated the phasematching mechanism and optimal conditions of HHG using a truncated Gaussian annular beam under high laser intensity and gas pressure. ...

Ultrafast polarization-tunable monochromatic extreme ultraviolet source at high-repetition-rate

... Working under such a supposition, VMI data were then processed in an approximate manner using a standard inverse Abel transform. [55][56][57][58][59]66 Through an in-depth tomographic analysis using the HTR method, however, it was shown that symmetry-breaking (i.e., m ≠ 0 spherical harmonic) terms can, in fact, make a significant contribution to the 3D-PEELD distributions, being of similar magnitude to the cylindrically symmetric (i.e., m = 0) terms. An in-depth discussion regarding this may be found in the original publication. ...

Photoelectron elliptical dichroism spectroscopy of resonance-enhanced multiphoton ionization via the 3s, 3p and 3d Rydberg series in Fenchone.
  • Citing Article
  • February 2022

Physical Chemistry Chemical Physics

... Mais cet apport des sources lasers est probablement anecdotique en comparaison de celui qui conduit à la découverte du phénomène de génération d'harmoniques d'ordre élevé (décrit plus en détail dans le chapitre 1), dont le spectre d'émission contient une partie des structures spectroscopiques de l'atome du milieu de génération. Ainsi, le minimum de Cooper de l'argon a été mis en évidence relativement tôt dans des spectres harmoniques (L'Huillier et Wahlström et al., 1993) et étudié plus systématiquement au cours des années 2000 (Minemoto et al., 2008 ;Wörner et al., 2009 ;Higuet et al., 2011). ...

High-order Harmonic Spectroscopy : Experimental and Theoretical study of Cooper Minimum in Argon
  • Citing Article
  • November 2012

... Experiments employing highly intense femtosecond laser fields to trigger tunnel ionization allow one to study PECD with attosecond time resolution [6,7]. Previous works studied chirality with laser fields at comparably low light intensities [6,8] and with an enhanced recollision probability [9][10][11]. The yield of high harmonic generation was studied to reveal differences in the recollision probability for the strong field ionization of chiral molecules [12]. ...

Revealing the Influence of Molecular Chirality on Tunnel-Ionization Dynamics

Physical Review X

... In the context of a large molecule, camphor is a naturally occurring volatile, monoterpene ketone known for its medicinal and other uses [28,29]. This system has long served as a benchmark chiral molecule for asymmetries in angle-resolved photoelectron spectra [30][31][32][33][34][35][36][37]. Although the study does not delve into the chirality of the molecular system, it is important to note that camphor molecules undergo intricate bond rearrangements during fragmentation due to their complexity and numerous functional groups [38,39]. ...

Ultrafast relaxation investigated by Photoelectron Circular Dichroism : an isomeric comparison of Camphor and Fenchone
  • Citing Article
  • November 2021

Physical Chemistry Chemical Physics