Thermo-optical modeling of high power operation of 2 μm codoped Tm,Ho solid-state lasers

2008 ◽  
Vol 104 (3) ◽  
pp. 033114 ◽  
Author(s):  
Oleg A. Louchev ◽  
Yoshiharu Urata ◽  
Masaki Yumoto ◽  
Norihito Saito ◽  
Satoshi Wada
Keyword(s):  
Solid State ◽  
High Power ◽  
Solid State Lasers ◽  
Optical Modeling ◽  
High Power Operation ◽  
Power Operation

Coupled thermo-optical modeling of high power operation of Tm, Ho:YLF solid-state lasers

2007 ◽  
Author(s):  
Oleg A. Louchev ◽  
Yoshiharu Urata ◽  
Norihito Saito ◽  
Satoshi Wada
Keyword(s):  
Solid State ◽  
High Power ◽  
Solid State Lasers ◽  
Optical Modeling ◽  
High Power Operation ◽  
Power Operation

High-power operation of AlGaAs SQW-SCH broad-area laser diodes for Nd:YAG solid-state laser pumping

1991 ◽  
Vol 3 (2) ◽  
pp. 97-99 ◽  
Author(s):  
Y. Nagai ◽  
K. Shigihara ◽  
A. Takami ◽  
S. Karakida ◽  
Y. Kokubo ◽  
...  
Keyword(s):  
Solid State ◽  
High Power ◽  
Laser Diodes ◽  
Solid State Laser ◽  
Broad Area ◽  
State Laser ◽  
Laser Pumping ◽  
High Power Operation ◽  
Power Operation

Broadly tunable high-power operation of an all-solid-state titanium-doped sapphire laser system

1991 ◽  
Vol 16 (6) ◽  
pp. 399 ◽  
Author(s):  
T. R. Steele ◽  
D. C. Gerstenberger ◽  
A. Drobshoff ◽  
R. W. Wallace
Keyword(s):  
Solid State ◽  
High Power ◽  
Laser System ◽  
Sapphire Laser ◽  
High Power Operation ◽  
Power Operation ◽  
Sapphire Laser System

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.

High-power operation of 630 nm-band transverse-mode stabilised AlGaInP laser diodes with current-blocking region near facets

1991 ◽  
Vol 27 (8) ◽  
pp. 661 ◽  
Author(s):  
H. Hamada ◽  
M. Shono ◽  
S. Honda ◽  
R. Hiroyama ◽  
K. Matsukawa ◽  
...  
Keyword(s):  
High Power ◽  
Laser Diodes ◽  
Transverse Mode ◽  
High Power Operation ◽  
Power Operation ◽  
Current Blocking

Tapered laser arrays for high power operation (> 1.4 W CW) at 1.59 [micro sign]m for applications in surgery

1998 ◽  
Vol 34 (10) ◽  
pp. 993 ◽  
Author(s):  
P.J. Williams ◽  
J.J. Lewandowski ◽  
D.J. Robbins ◽  
A.K. Wood ◽  
F.O. Robson ◽  
...  
Keyword(s):  
High Power ◽  
Laser Arrays ◽  
High Power Operation ◽  
Power Operation ◽  
Tapered Laser

High-Power Operation of Acoustic-Electric Power Feedthroughs Through Thick Metallic Barriers

2012 ◽  
Author(s):  
K. R. Wilt ◽  
H. A. Scarton ◽  
G. J. Saulnier ◽  
T. J. Lawry ◽  
J. D. Ashdown
Keyword(s):  
Power Density ◽  
High Power ◽  
Electrical Power ◽  
Power Transfer ◽  
Receive Transducer ◽  
High Power Operation ◽  
Linear Effects ◽  
Power Limits ◽  
Power Operation ◽  
Power Testing

Throughout the last few years there has been a significant push to develop a means for the transmission of electrical power through solid metallic walls using ultrasonic means. The bulk of this effort has been focused on using two coaxially aligned piezoelectric transducers on opposite sides of a thick metallic transmission barrier, where one transducer serves as the “transmit” transducer and the other as the “receive” transducer. Previous modeling has predicted reasonably high power transfer efficiencies through the wall using this type of “acoustic-electric channel” to be possible at low power levels, which implies that channel component operates in a linear range with little concern of failure. High-power testing of two acoustic-electric channels has been done in an effort to determine power limits on such channels and to determine levels at which non-linear effects on the piezoelectrics become non-negligible. The tested channels are characterized by the “power density” imposed on the transmit transducer, that is, the power applied per unit area, as the values found for maximum power density are considered to be independent of transducer radii. The constructed channels are shown to be capable of transmitting large amounts of power (over 100 watts) without failure; and further, extrapolation of the results to channels with larger diameter transducers predicts power transfer of 1 kW to be highly feasible.

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