Continuous-wave mode-locked solid-state lasers with enhanced spatial hole burning

1995 ◽  
Vol 61 (6) ◽  
pp. 569-579 ◽  
Author(s):  
F. X. K�rtner ◽  
B. Braun ◽  
U. Keller
Keyword(s):  
Solid State ◽  
Continuous Wave ◽  
Wave Mode ◽  
Hole Burning ◽  
Solid State Lasers ◽  
Spatial Hole Burning ◽  
Continuous Wave Mode

Continuous-wave mode-locked solid-state lasers with enhanced spatial hole burning

1995 ◽  
Vol 61 (5) ◽  
pp. 429-437 ◽  
Author(s):  
B. Braun ◽  
K. J. Weingarten ◽  
F. X. K�rtner ◽  
U. Keller
Keyword(s):  
Solid State ◽  
Continuous Wave ◽  
Wave Mode ◽  
Hole Burning ◽  
Solid State Lasers ◽  
Spatial Hole Burning ◽  
Continuous Wave Mode

Stable continuous-wave mode-locked laser from a 1645 nm Er:YAG ceramic oscillator

2022 ◽  
Author(s):  
Yangyu Liu ◽  
Xue Cao ◽  
AnHua Xian ◽  
Guangmiao Liu ◽  
Wei zhou ◽  
...  
Keyword(s):  
Solid State ◽  
Pulse Width ◽  
Peak Power ◽  
Continuous Wave ◽  
Modulation Depth ◽  
Average Power ◽  
Mode Locking ◽  
Wave Mode ◽  
Semiconductor Saturable Absorber ◽  
Continuous Wave Mode

Abstract We demonstrate stable continuous-wave mode-locking (CWML) pulses around 1645nm by employing the home-made Er:YAG ceramic. By using a fiber laser and semiconductor saturable absorber mirror (SESAM) with modulation depth of 1.2%, we get ML pulses with the output average power up to 815 mW, the pulse width shortened as ~4 ps, and the peak power of 1.8 kW. With the SESAM of modulation depth of 2.4%, the second-order harmonic ML pulses were also obtained. As far as we know, this is the first report of CWML from Er3+-doped ceramics and also the shortest pulse duration in Er3+-doped solid-state oscillators.

scholarly journals Multi-wavelength, all-solid-state, continuous wave mode locked picosecond Raman laser

2010 ◽  
Vol 18 (5) ◽  
pp. 5289 ◽  
Author(s):  
Eduardo Granados ◽  
Helen M. Pask ◽  
Elric Esposito ◽  
Gail McConnell ◽  
David J. Spence
Keyword(s):  
Solid State ◽  
Continuous Wave ◽  
Raman Laser ◽  
Wave Mode ◽  
Multi Wavelength ◽  
Continuous Wave Mode

Elimination of spatial hole burning in solid-state lasers using nanostructured thin films

2019 ◽  
Vol 59 (5) ◽  
pp. A83 ◽  
Author(s):  
Jean-François Bisson ◽  
Koffi Novignon Amouzou
Keyword(s):  
Thin Films ◽  
Solid State ◽  
Hole Burning ◽  
Solid State Lasers ◽  
Spatial Hole Burning ◽  
Nanostructured Thin Films

Selective pumping and spatial hole burning for generation of photon wave packets with ray-wave duality in solid-state lasers

2015 ◽  
Vol 13 (2) ◽  
pp. 025001 ◽  
Author(s):  
J C Tung ◽  
H C Liang ◽  
P H Tuan ◽  
F L Chang ◽  
K F Huang ◽  
...  
Keyword(s):  
Solid State ◽  
Wave Packets ◽  
Hole Burning ◽  
Solid State Lasers ◽  
Spatial Hole Burning

Standoff Detection of Oil and Powder Mixtures at 12 Meters Using a Tunable Quantum Cascade Laser-Based System with a Close Focus Telescope and Uncooled Infrared Detector

2021 ◽  
pp. 000370282110603
Author(s):  
J. Chance Carter ◽  
Phillip H. Paul ◽  
Joshua M. Ottaway ◽  
Peter Haugen ◽  
Anastacia M. Manuel
Keyword(s):  
Quantum Cascade Laser ◽  
Continuous Wave ◽  
Infrared Detector ◽  
Wave Mode ◽  
Infrared Source ◽  
Powder Mixtures ◽  
Quantum Cascade ◽  
System A ◽  
Continuous Wave Mode ◽  
Lock In

We have designed and demonstrated a quantum cascade laser (QCL) based standoff system that utilizes an uncooled mercury cadmium telluride (MCT) detector with lock-in signal processing for chemical identification at a distance of 12.5 meters in indoor ambient light conditions. In the system, a tunable quad-QCL operating (1 MHz) in quasi-continuous wave mode between 8.45 and 10.03 μm (∼1182 to 1000 cm−1) serves as the active mid-infrared source for remotely interrogating mineral, powder, and thin film oil samples including powder mixtures (6, 12.5, 25, and 50%) of crystalline quartz (SiO2) in KBr. Light as reflected from a given sample is collected using a 10-inch (25.4 cm) Dall Kirkham telescope and coupled with ZnSe optics to an uncooled MCT detector. The mixture dependence of the highly transparent KBr and strongly absorbing quartz was found to fit a modified version of the Schatz reflectance model for compacted powder mixtures. All reflectance spectra reported are relative to an Au-coated diffuse reflector. A NIST traceable polystyrene standard reflector was also used to determine the QCL wavelength tuning range and calibration.

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