High Pulse Energy and High Peak Power Fiber Amplifiers

Author(s):  
Mark S. Bowers
2006 ◽  
Author(s):  
Matthias Savage-Leuchs ◽  
Eric Eisenberg ◽  
Anping Liu ◽  
Jason Henrie ◽  
Mark Bowers

2014 ◽  
Vol 6 (3) ◽  
pp. 1-8 ◽  
Author(s):  
C. L. Chang ◽  
P. Y. Lai ◽  
Y. Y. Li ◽  
Y. P. Lai ◽  
C. W. Huang ◽  
...  

2019 ◽  
Vol 2 (3) ◽  
pp. 65
Author(s):  
Viktoras Lisicovas ◽  
Bala Murali Krishna Mariserla ◽  
Chakradhar Sahoo ◽  
Reuben T. Harding ◽  
Michael K. L. Man ◽  
...  

Wide-field temporal focused (WF-TeFo) two-photon microscopy allows for the simultaneous imaging of a large planar area, with a potential order of magnitude enhancement in the speed of volumetric imaging. To date, low repetition rate laser sources with over half a millijoule per pulse have been required in order to provide the high peak power densities for effective two-photon excitation over the large area. However, this configuration suffers from reduced signal intensity due to the low repetition rate, saturation effects due to increased excitation fluences, as well as faster photobleaching of the fluorescence probe. In contrast, with the recent advent of high repetition rate, high pulse energy laser systems could potentially provide the advantages of high repetition rate systems that are seen in traditional two-photon microscopes, while minimizing the negatives of high fluences in WF-TeFo setups to date. Here, we use a 100 microjoule/high repetition rate (50–100 kHz) laser system to investigate the performance of a WF-TeFo two-photon microscope. While using micro-beads as a sample, we demonstrate a proportionate increase in signal intensity with repetition rate, at no added cost in photobleaching. By decreasing pulse intensity, via a corresponding increase in repetition rate to maintain fluorescence signal intensity, we find that the photobleaching rate is reduced by ~98.4%. We then image live C. elegans at a high repetition rate for 25 min. as a proof-of-principle. Lastly, we identify the steady state temperature increase as the limiting process in further increasing the repetition rate, and we estimate that repetition rate in the range between 0.5 and 5 MHz is ideal for live imaging with a simple theoretical model. With new generation low-cost fiber laser systems offering high pulse energy/high repetition rates in what is essentially a turn-key solution, we anticipate increased adoption of this microscopy technique by the neuroscience community.


Author(s):  
John Minelly ◽  
Fabio Teodoro ◽  
Matthias Savage-Leuchs ◽  
Deborah Alterman ◽  
Christopher Brooks ◽  
...  

2008 ◽  
Vol 15 (3) ◽  
pp. 136-139 ◽  
Author(s):  
Ryusuke Horiuchi ◽  
Koichi Saiki ◽  
Koji Adachi ◽  
Kazuyoku Tei ◽  
Shigeru Yamaguchi

2010 ◽  
Vol 46 (22) ◽  
pp. 1516 ◽  
Author(s):  
Y. Ding ◽  
D.I. Nikitichev ◽  
I. Krestnikov ◽  
D. Livshits ◽  
M.A. Cataluna ◽  
...  

2008 ◽  
Vol 18 (02) ◽  
pp. 483-492
Author(s):  
JIANWU DING ◽  
BRUCE W. ODOM ◽  
ALLEN R. GEIGER ◽  
RICHARD D. RICHMOND

A compact high peak power eye-safer optical parametric oscillator was constructed by pumping it with a master oscillator power amplifier consisting of a large-mode-area ytterbium doped fiber amplifier and a diode-pumped, passively Q-switched Nd : YAG microchip laser. The master oscillator power amplifier has the maximum output pulse energy of 570 μJ with a 3 nanosecond pulse width and a 3 kHz pulse repetition rate. The compact singly resonating optical parametric oscillator utilized a 50 mm periodically poled Lithium Niobate crystal and generated high peak power 1.5 μm eye-safe laser pulses with more than 140 μJ pulse energy, 3 nanosecond pulse width and 3 kHz repetition rate.


Sign in / Sign up

Export Citation Format

Share Document