Traveling Wave Model Based Simulation of Tunable Multi-Wavelength Diode Laser Systems

Author(s):  
J.-P. Koester ◽  
M. Radziunas ◽  
A. Zeghuzi ◽  
H. Wenzel ◽  
A. Knigge
Author(s):  
Jan-Philipp Koester ◽  
Mindaugas Radziunas ◽  
Anissa Zeghuzi ◽  
Hans Wenzel ◽  
Andrea Knigge

2008 ◽  
Author(s):  
Daniel Bartoschewski ◽  
Jens Meinschien ◽  
Udo Fornahl

2010 ◽  
Author(s):  
Márc T. Kelemen ◽  
Jürgen Gilly ◽  
Rudolf Moritz ◽  
Jeanette Schleife ◽  
Mathias Fatscher ◽  
...  

2015 ◽  
Author(s):  
A. N. Soldatov ◽  
S. Y. Mirza ◽  
Yu. P. Polunin ◽  
A. S. Shumeiko ◽  
I. K. Kostadinov

2010 ◽  
Vol 15 (1) ◽  
pp. 23-38 ◽  
Author(s):  
Aleksandr Dementjev ◽  
Raimondas Čiegis ◽  
Ingrida Laukaitytė ◽  
Nerijus Slavinskis

A detailed theoretical model for the description of generation dynamics of diode laser longitudinally pumped solid‐state lasers with active and/or passive Q‐switching using traveling wave approach is presented. The results of numerical simulations and analysis show that the distribution of generated laser pulse intensity and the other laser parameters along the resonator is very inhomogeneous. Therefore, the widely used point laser model cannot give accurate results when inside the resonator there are active or passive elements which lead to the strong modulation of the generated pulse intensities.


2021 ◽  
Author(s):  
Yi Lu

All-fiber passively Q-switched lasers were demonstrated using ytterbium-doped double cladding fiber (YDF) as an active medium. The laser was pumped by three 25W, 975nm fiber coupled diodes and Q-switching was initiated when the amplified spontaneous emission generated in the core of the gain fiber bleached the saturable absorber (SA). A piece of samarium-doped fiber was used as SA in first configuration and pulses with 68μJ pulse energy and 210ns pulse width were obtained. In second configuration, a piece of ytterbium-doped fiber with much smaller core size was used as SA to produce pulse energy of 86μJ. The last configuration incorporated a 9m-long YDF as gain fiber. The far end from pump was acting as SA in this case and pulses with 82μJ pulse energy and 148ns pulse width were observed. The peak power was estimated at 554W. Traveling wave model was implemented to numerically simulate the output characteristics versus pump power.


2009 ◽  
Vol 71 (2) ◽  
pp. 291-317 ◽  
Author(s):  
Abbey J. Trewenack ◽  
Kerry A. Landman

Author(s):  
Ole Bjarlin Jensen ◽  
Anders Kragh Hansen ◽  
Christian Pedersen ◽  
Peter E. Andersen ◽  
Paul Michael Petersen

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