Patrick Georges
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View article: High-energy soliton frequency shifting in a nitrogen-filled multipass cell
High-energy soliton frequency shifting in a nitrogen-filled multipass cell Open
We report an experimental demonstration of soliton self-frequency shift in a nitrogen-filled multipass cell. The use of a molecular gas combined with the flexible geometry of the multipass platform enables efficient wavelength conversion f…
View article: Indirectly LED-pumped Nd:glass regenerative amplifier
Indirectly LED-pumped Nd:glass regenerative amplifier Open
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View article: Cr:ZnSe as a luminescent concentrator
Cr:ZnSe as a luminescent concentrator Open
We demonstrate the first Cr:ZnSe luminescent concentrator. Enhanced by amplified spontaneous emission, it has the best efficiency ever reported for luminescent concentrators emitting in the SWIR band. It emits an output power of 1.6 W and …
View article: Numerical and experimental study of self-seeded stimulated Brillouin scattering in active fibers injected by a sinusoidally phase modulated signal
Numerical and experimental study of self-seeded stimulated Brillouin scattering in active fibers injected by a sinusoidally phase modulated signal Open
Sinusoidal phase modulation is a simple technique for increasing the SBS threshold by an enhancement factor (EF) of 3 to 10 in fiber-based laser systems. However, this EF can be reduced by a factor of ∼2 if modulation settings are not care…
View article: LED pumped alexandrite multipass amplifier designed for acousto-optic imaging
LED pumped alexandrite multipass amplifier designed for acousto-optic imaging Open
In this paper we present an alexandrite (Cr 3+ :BeAl 2 O 4 ) multipass amplifier pumped by blue LEDs via a luminescent concentrator (LC). This emerging pump technology provides up to 2.6 kW optical pump power during 400 µs at 10 Hz in the …
View article: Accurate pulse-to-pulse stability measurement for femtosecond lasers
Accurate pulse-to-pulse stability measurement for femtosecond lasers Open
Short-term energy stability metrology of pulsed lasers is the source of widespread misleading comparisons. The most used value for this characterization in commercial products and laboratory applications is the rms pulse-to-pulse stability…
View article: Temporal pulse shaping technique for nonlinear frequency shifting
Temporal pulse shaping technique for nonlinear frequency shifting Open
We present a spectral phase-only shaping technique allowing to generate arbitrary temporal shapes and demonstrate its use for ultrafast ytterbium-based laser sources. This technique is based on the introduction of a nonlinear chirp that is…
View article: Off-resonance intracavity up-conversion pumping architecture enabling multi-watt operation of a 2.3-µm Tm:YLF laser
Off-resonance intracavity up-conversion pumping architecture enabling multi-watt operation of a 2.3-µm Tm:YLF laser Open
We present an intra-cavity upconversion pumping scheme for Thulium lasers operating on the 3 H 4 → 3 H 5 transition. It is based on detuning the pump wavelength from the resonance of excited-state absorption, 3 F 4 → 3 F 2,3 , around 1 µm.…
View article: Indirectly LED-pumped Nd:glass: potential for high energy laser facilities
Indirectly LED-pumped Nd:glass: potential for high energy laser facilities Open
Flashlamp-pumped Nd:glass is used as a power amplifier in many high energy laser facilities. Despite the problems of this old technology, flashlamps are still being considered for the next generation of lasers as diode laser pumping is far…
View article: Higher-order- and multimode properties of nonlinear multipass cells for temporal compression
Higher-order- and multimode properties of nonlinear multipass cells for temporal compression Open
Over the last few years, temporal compression in nonlinear multipass cells (MPCs) has been proven to be a very promising method for future ultrafast laser sources. Although the majority of the work has been done with Gaussian beams, a few …
View article: Type-I intermittency route to the chaos in passively Q-switched Tm:YLF laser emitting at 2.3 μm
Type-I intermittency route to the chaos in passively Q-switched Tm:YLF laser emitting at 2.3 μm Open
We report on an original chaotic dynamic behavior of a Tm-doped Q-switched laser operating on the 3 H 4 → 3 H 5 transition emitting at 2.3 μm using a Tm:YLF crystal, with optional co-lasing at 1.9 μm via the ³F₄ → ³H₆ transition. This stud…
View article: Real-time acousto-optic imaging using high-peak-power long-pulsed illumination
Real-time acousto-optic imaging using high-peak-power long-pulsed illumination Open
Acousto-optic imaging (AOI) of absorbing objects embedded in highly scattering media remains challenging, since the detectable signal suitable for image reconstruction is weak. To increase the detected signals to a level required by live b…
View article: Chaotic dynamics in passively Q-switched Tm:LiYF4 laser operating at 2.3 <i>μ</i>m on the 3H4 → 3H5 transition
Chaotic dynamics in passively Q-switched Tm:LiYF4 laser operating at 2.3 <i>μ</i>m on the 3H4 → 3H5 transition Open
We report on the chaotic dynamics in a passively Q-switched 2.3-μm thulium laser operating on the 3H4 → 3H5 transition. The experiment exploits a Tm:LiYF4 crystal and various laser cavity configurations, involving an optional cascade laser…
View article: High-power 2.3 µm Tm:YLF laser with intracavity upconversion pumping by a Nd:ASL laser at 1051 nm
High-power 2.3 µm Tm:YLF laser with intracavity upconversion pumping by a Nd:ASL laser at 1051 nm Open
A Tm:LiYF 4 laser operating on the 3 H 4 → 3 H 5 transition is embedded in a high-power diode-pumped Nd:ASL laser for intracavity upconversion pumping at 1.05 µm. This leads to a record-high output power at 2.3 µm for any bulk thulium lase…
View article: CTH:YAG : from laser medium to luminescent concentrator
CTH:YAG : from laser medium to luminescent concentrator Open
This work presents what we believe is a new way to use a CTH:YAG crystal for spontaneous emission instead of laser emission. The spontaneous emission is collected in one main direction thanks to a luminescent concentrator configuration. Th…
View article: Chirped pulse upconversion for femtosecond mid-infrared spectroscopy at 100 kHz
Chirped pulse upconversion for femtosecond mid-infrared spectroscopy at 100 kHz Open
We demonstrate that chirped pulse up-conversion (CPU), a method routinely used with systems based on 1-kHz Titanium:Sapphire lasers, can be extended to a repetition rate of 100 kHz with an Ytterbium diode-pumped femtosecond amplifier. Indi…
View article: Maximizing the efficiency of intrapulse difference frequency generation by pulse shaping and recycling
Maximizing the efficiency of intrapulse difference frequency generation by pulse shaping and recycling Open
View article: Type-I intermittency route to chaos in passively Q-switched Tm:YLF laser emitting at 2.3 μm
Type-I intermittency route to chaos in passively Q-switched Tm:YLF laser emitting at 2.3 μm Open
We report on an original chaotic dynamic behaviour of a passively Q-switched 2.3-μm Thulium laser operating on the 3 H 4 → 3 H 5 transition. The experiment employs a Tm:LiYF 4 laser crystal within various laser cavity configurations, invol…
View article: Experimental demonstration of a temporal pulse shaping method based on nonlinear chirp
Experimental demonstration of a temporal pulse shaping method based on nonlinear chirp Open
We present a general temporal shaping method based on spectral phase-only modulation for ultrafast laser sources. We explain the working principle of this technique and use it experimentally to generate a ramp-shaped pulse at the output of…
View article: High-power intracavity upconversion pumped Tm:YLF laser emitting at 2.3 μm
High-power intracavity upconversion pumped Tm:YLF laser emitting at 2.3 μm Open
A Tm:LiYF4 laser operating on the 3 H 4 → 3 H 5 transition is integrated into a high-power diode-pumped Nd:ASL laser for intracavity upconversion pumping at 1.05 μm. This architecture leads to a record-high output power at 2.3 μm ever extr…
View article: Power scaling of LED-pumped alexandrite: The road to high gain multipass amplifiers
Power scaling of LED-pumped alexandrite: The road to high gain multipass amplifiers Open
Our experiment demonstrates that LED-pumping through luminescent concentrator enables sufficient pump power for viable alexandrite amplifier gain. In 10 passes we obtain a gain of 19 with 10 W output power, for 50 µs pulses at 20 Hz and 76…
View article: Nonlinear post-compression of a hybrid vortex mode in a gas-filled capillary
Nonlinear post-compression of a hybrid vortex mode in a gas-filled capillary Open
We demonstrate nonlinear temporal compression of a vortex beam by propagation in a gas-filled capillary. Starting from an ytterbium-based laser delivering 700 μ J 640 fs pulses at a 100 kHz repetition rate, the vortex beam is generated usi…
View article: On the efficiency of Intrapulse Difference Frequency Generation MIR systems
On the efficiency of Intrapulse Difference Frequency Generation MIR systems Open
Intrapulse Difference Frequency Generation (iDFG) is an interesting technique for generating femtosecond pulses in the Mid-Infrared (MIR) range with unique properties such as robust Carrier-Envelope Phase (CEP) stability. However, its effi…
View article: Cascade laser optimization for <sup>3</sup>H<sub>4</sub> → <sup>3</sup>H<sub>5</sub> and <sup>3</sup>F<sub>4</sub> → <sup>3</sup>H<sub>6</sub> sequent transitions in Tm<sup>3+</sup>-doped materials
Cascade laser optimization for <sup>3</sup>H<sub>4</sub> → <sup>3</sup>H<sub>5</sub> and <sup>3</sup>F<sub>4</sub> → <sup>3</sup>H<sub>6</sub> sequent transitions in Tm<sup>3+</sup>-doped materials Open
We study a cascade laser scheme involving the 3 H 4 → 3 H 5 and 3 F 4 → 3 H 6 consecutive transitions in Tm 3+ -doped materials as a promising technique to favor laser emission at 2.3 µm. We examine the conditions in terms of the Tm 3+ dop…
View article: Pulsewidth-switchable ultrafast source at 114 nm
Pulsewidth-switchable ultrafast source at 114 nm Open
Femtosecond laser sources with high repetition rate in the ultraviolet (UV) and vacuum UV (VUV) are fundamental tools enabling tabletop time-resolved and angle-resolved photoemission spectroscopy in solids. We describe a VUV source at 114 …
View article: Pump tunable mirrorless OPO: an innovative concept for future space IPDA emitters
Pump tunable mirrorless OPO: an innovative concept for future space IPDA emitters Open
A highly efficient mirrorless OPO tunable in the mid-infrared around 2 µm has been developed and characterized in an original pumping configuration comprising a tunable high power hybrid Ytterbium laser MOPA (Master Oscillator Power Amplif…
View article: LED-pumped Er:Cr:YSGG light sources
LED-pumped Er:Cr:YSGG light sources Open
For, what we believe is, the first time, an Er:Cr:YSGG crystal is pumped by LEDs through a Ce:YAG luminescent concentrator. We demonstrate both laser emission at 2.79 µm and strong spontaneous emission at 1.6 µm. The luminescent concentrat…
View article: Ce:LYSO, from scintillator to solid-state lighting as a blue luminescent concentrator
Ce:LYSO, from scintillator to solid-state lighting as a blue luminescent concentrator Open
Cerium-doped lutetium-yttrium oxyorthosilicate (Ce:LYSO) is a well-known single crystal scintillator used in medical imaging and security scanners. Recent development of high power UV LED, matching its absorption band, questions the possib…
View article: Tm:CALGO lasers at 2.32 µm: cascade lasing and upconversion pumping
Tm:CALGO lasers at 2.32 µm: cascade lasing and upconversion pumping Open
We report on the first laser operation of a disordered Tm:CaGdAlO 4 crystal on the 3 H 4 → 3 H 5 transition. Under direct pumping at 0.79 µm, it generates 264 mW at 2.32 µm with a slope efficiency of 13.9% and 22.5% vs. incident and absorb…
View article: Intensity noise in difference frequency generation-based tunable femtosecond MIR sources
Intensity noise in difference frequency generation-based tunable femtosecond MIR sources Open
We characterize the intensity noise of two mid-infrared (MIR) ultrafast tunable (3.5-11 μ m) sources based on difference frequency generation (DFG). While both sources are pumped by a high repetition rate Yb-doped amplifier delivering 200 …