Generation of continuous-wave ultraviolet light by sum-frequency mixing of diode-laser and argon-ion-laser radiation in β-BaB_2O_4

1991 ◽  
Vol 16 (7) ◽  
pp. 449 ◽  
Author(s):  
Kazuhiko Sugiyama ◽  
Jun Yoda ◽  
Toshio Sakurai
Keyword(s):  
Laser Radiation ◽  
Diode Laser ◽  
Ultraviolet Light ◽  
Continuous Wave ◽  
Sum Frequency ◽  
Argon Ion Laser ◽  
Ion Laser ◽  
Argon Ion ◽  
Frequency Mixing

Diode-laser-pumped continuous-wave doubly linear resonator sum-frequency mixing red laser at 689 nm

Laser Physics ◽  
2011 ◽  
Vol 21 (7) ◽  
pp. 1194-1197 ◽  
Author(s):  
X. M. Fan ◽  
H. Chu ◽  
X. Wang ◽  
Z. Y. Zhang ◽  
W. Liang
Keyword(s):  
Diode Laser ◽  
Continuous Wave ◽  
Sum Frequency ◽  
Frequency Mixing

Fiber Optic Delivery Of Argon Ion Laser Radiation For Open Endarterectamy

1988 ◽  
Author(s):  
John Eugene ◽  
Joseph S. Carey ◽  
Ramon A. Cukingnan ◽  
Marie Hammer-Wilson ◽  
Michael W. Berns
Keyword(s):  
Laser Radiation ◽  
Fiber Optic ◽  
Argon Ion Laser ◽  
Ion Laser ◽  
Argon Ion

Diode-laser-pumped continuous-wave doubly linear resonator sum-frequency mixing orange laser at 600 nm

2010 ◽  
Vol 7 (1) ◽  
pp. 21-24 ◽  
Author(s):  
Y.F. Lü ◽  
X.D. Yin ◽  
J. Xia ◽  
H. Quan ◽  
D. Wang
Keyword(s):  
Diode Laser ◽  
Continuous Wave ◽  
Sum Frequency ◽  
Frequency Mixing

Photolytic and transport effects produced by argon ion laser radiation on hexacyanoferrate(III) solutions

1992 ◽  
Vol 257 (2) ◽  
pp. 217-221 ◽  
Author(s):  
R.M. Villanueva Camañas ◽  
J.M. Sanchis Mallols ◽  
E.F. Simó Alfonso ◽  
G. Ramis Ramos
Keyword(s):  
Laser Radiation ◽  
Argon Ion Laser ◽  
Ion Laser ◽  
Transport Effects ◽  
Argon Ion

Solid Solubility of Sb and Te Implanted GaAs Following Solid Phase Annealing

1983 ◽  
Vol 23 ◽  
Author(s):  
S.T. Johnson ◽  
K.G. Orrman-Rossiter ◽  
J.S. Williams
Keyword(s):  
Solid Solubility ◽  
Continuous Wave ◽  
Solid Phase ◽  
High Dose ◽  
Incoherent Light ◽  
Ion Channeling ◽  
Argon Ion Laser ◽  
Conventional Furnace ◽  
Ion Laser ◽  
Argon Ion

ABSTRACTHigh dose antimony and tellurium implanted (100) GaAs wafers have been annealed in the solid phase under various time/temperature conditions using a conventional furnace, a rapid incoherent light source and a continuous wave CW Argon ion laser. The samples were capped with RF sputtered SiO2 prior to annealing and analysed using 2MeV He++ ion channeling to determine the solid solubility of the implanted ions. Results indicate that the Te is more soluble than Sb; highest solubilities measured were 6 × 1020cm−3 for Te and 1.3 × 1020cm−3 for Sb.

Caractéristiques de la décharge d'un laser à argon multiwatt continu

1985 ◽  
Vol 63 (2) ◽  
pp. 240-245
Author(s):  
J.-L. Breton ◽  
G. Bédard
Keyword(s):  
Magnetic Field ◽  
Continuous Wave ◽  
Axial Magnetic Field ◽  
High Current Density ◽  
High Current ◽  
Argon Ion Laser ◽  
Continuous Current ◽  
Ion Laser ◽  
Discharge Parameters ◽  
Argon Ion

We report on the construction of a 10-mm bore 60-W continuous wave argon ion laser operated at a discharge power of about 64 kW, which provides a continuous current of 200 A. Specially designed high-current-density anodes and cathodes are described. Experimental results on the effects of an axial magnetic field (0–875 G) on discharge parameters are also presented.

scholarly journals Growth Characteristics of Fiber Bragg Gratings Fabricated in High Germania Boron Co-Doped Fiber

1970 ◽  
Vol 3 (2) ◽  
Author(s):  
S. W. Harun , P. Poopalan and H. Ahmad
Keyword(s):  
Continuous Wave ◽  
Uv Light ◽  
Bragg Gratings ◽  
Growth Characteristics ◽  
Phase Mask ◽  
Wavelength Shift ◽  
Argon Ion Laser ◽  
Ion Laser ◽  
Argon Ion ◽  
Co Doped

This paper reports and provides an explanation for the growth characteristics of fibre Bragg gratings (FBGs) fabricated  in high germania boron co-doped optical fiber by using a continuous wave (CW) doubled frequency Argon ion laser as an UV light source. The grating reflectivity and Bragg wavelength shift as a function of exposure time are measured. The index modulation time is observed to have a good fit to a power law of the form n = Ctb (t is the time, C and b are constants), whereas the exponent b of 0.3 is obtained for the FBGs. The UV laser light also causes a shift of the resonant wavelength with fabrication time. The fastest wavelength shift is shown to be 0.53 nm after 524 seconds exposure.Keywords: Fiber Bragg grating, Argon ion laser, Phase mask method, Growth characteristics.

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