KDP Q-switches and second harmonic generator for high-power solid-state lasers

1985 ◽  
Vol 57 (3-4) ◽  
pp. 313-316
Author(s):  
J. Bakos ◽  
T. Juhász ◽  
Cs. Kuti ◽  
L. V. Vannay
Keyword(s):  
Solid State ◽  
High Power ◽  
Second Harmonic ◽  
Solid State Lasers ◽  
Harmonic Generator ◽  
Second Harmonic Generator

KTP second-harmonic generator for high-power lasers

1996 ◽  
Author(s):  
Nina Pavlova ◽  
Oleg E. Sidoryuk ◽  
Valerie A. Astapenko
Keyword(s):  
High Power ◽  
Second Harmonic ◽  
High Power Lasers ◽  
Harmonic Generator ◽  
Second Harmonic Generator

Optimized growth of high length-to-diameter ratio Lu2O3 single crystal fibers by the LHPG method

CrystEngComm ◽  
2021 ◽  
Vol 23 (7) ◽  
pp. 1657-1662
Author(s):  
Na Zhang ◽  
Yuqing Yin ◽  
Jian Zhang ◽  
Tao Wang ◽  
Siyuan Wang ◽  
...  
Keyword(s):  
Solid State ◽  
Single Crystal ◽  
High Power ◽  
Diameter Ratio ◽  
Solid State Lasers ◽  
Crystal Fibers ◽  
High Length ◽  
Length To Diameter Ratio

Lu2O3 crystals have attracted intense attention due to their great potential in the field of high power solid-state lasers.

scholarly journals Stimulated Raman Microscopy Implemented by Three Femtosecond Laser Sources

2021 ◽  
Vol 255 ◽  
pp. 06003
Author(s):  
Rajeev Ranjan ◽  
Maria Antonietta Ferrara ◽  
Luigi Sirleto
Keyword(s):  
Femtosecond Laser ◽  
Stimulated Raman Scattering ◽  
Second Harmonic ◽  
Laser Beams ◽  
Raman Gain ◽  
Harmonic Generator ◽  
Second Harmonic Generator ◽  
Laser Sources ◽  
Fingerprint Region ◽  
Stimulated Raman

In this work, the implementation of a femtosecond Stimulated Raman Scattering microscope, equipped with three femtosecond laser sources: a Titanium-Sapphire (Ti:Sa), an optical parametric oscillator (OPO), and a second harmonic generator (SHG); is presented. Our microscope is designed so that it can cover all the regions of Raman spectra, taking advantage of two possible laser combinations. The first, Ti:Sa and OPO laser beams, which cover the C-H region (>2800 cm-1 ) in stimulated Raman gain (SRG) modality, whereas the second, Ti:Sa and SHG laser beams, covering the C-H region and the fingerprint region in stimulated Raman losses (SRL) modality. The successful realization of the microscope is demonstrated, reporting images of polystyrene beads using both SRL and SRG modalities.

scholarly journals Compact High-Power-VCSEL-Array Pumped Solid-State Lasers

2013 ◽  
Vol 41 (9) ◽  
pp. 679
Author(s):  
Robert VAN LEEUWEN ◽  
Tong CHEN ◽  
Laurence WATKINS ◽  
Jean-Francois SEURIN ◽  
Chuni GHOSH
Keyword(s):  
Solid State ◽  
High Power ◽  
Solid State Lasers
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