Continuous-wave anti-Stokes Raman laser based on phase-matched nondegenerate four-wave mixing

2014 ◽  
Vol 40 (1) ◽  
pp. 73 ◽  
Author(s):  
Shin-ichi Zaitsu ◽  
Totaro Imasaka
Keyword(s):  
Continuous Wave ◽  
Raman Laser ◽  
Four Wave Mixing ◽  
Wave Mixing ◽  
Anti Stokes

scholarly journals High-phase-conjugate reflectivity (>800%) obtained by degenerate four-wave mixing in a continuous-wave diode-side-pumped Nd:YVO_4 amplifier

1999 ◽  
Vol 24 (14) ◽  
pp. 972 ◽  
Author(s):  
S. Mailis ◽  
J. Hendricks ◽  
D. P. Shepherd ◽  
A. C. Tropper ◽  
N. Moore ◽  
...  
Keyword(s):  
Continuous Wave ◽  
Four Wave Mixing ◽  
Wave Mixing ◽  
Phase Conjugate ◽  
Degenerate Four Wave Mixing ◽  
High Phase

Total Stokes or Anti-Stokes Conversion from Four-Wave Mixing Process (FWMP) in Para-H 2

1986 ◽  
Vol 2 (9) ◽  
pp. 695-699 ◽  
Author(s):  
M Bernardini ◽  
M Giorgi ◽  
A Palucci ◽  
S Ribezzo ◽  
S Marchetti
Keyword(s):  
Four Wave Mixing ◽  
Wave Mixing ◽  
Mixing Process ◽  
Anti Stokes

Four-wave mixing effect on high-power continuous-wave all-fiber lasers

2018 ◽  
Vol 32 (23) ◽  
pp. 1850275
Author(s):  
Jinkun Zheng ◽  
Wei Zhao ◽  
Baoyin Zhao ◽  
Zhe Li ◽  
Gang Li ◽  
...  
Keyword(s):  
High Power ◽  
Fiber Lasers ◽  
Continuous Wave ◽  
Beam Quality ◽  
Matching Condition ◽  
Four Wave Mixing ◽  
Theoretical Description ◽  
Phase Matching ◽  
Wave Mixing ◽  
Mixing Effect

A four-wave mixing effect on high-power continuous-wave fiber lasers has been demonstrated theoretically and experimentally. Detailed theoretical description of phase matching is presented and we found that the phase matching condition is satisfied at the frequency shift of 5.16 THz. While the intensity in fiber core region is more than about 394 MW/cm2, the four-wave mixing products of 1100 nm and 1060 nm were also observed in high-power all-fiber laser. The comparison shows that the experiment result is in good agreement with the simulation result. In addition, the beam quality deterioration for the laser is caused by the four-wave mixing effect and the mode instability. The [Formula: see text] factor measured at maximal intensity of 478 MW/cm2 is 2.80.

Continuous-Wave Phase-Conjugate Self-Oscillation Induced by Na-Vapour Degenerate Four-Wave Mixing with Gain

1986 ◽  
Vol 2 (10) ◽  
pp. 747-753 ◽  
Author(s):  
J. R. R Leite ◽  
P Simoneau ◽  
D Bloch ◽  
S. Le Boiteux ◽  
M Ducloy
Keyword(s):  
Continuous Wave ◽  
Four Wave Mixing ◽  
Wave Mixing ◽  
Phase Conjugate ◽  
Wave Phase ◽  
Degenerate Four Wave Mixing

Modulating the correlation and squeezing of phase-conjugate four-wave mixing via the polarizable dressing states

2015 ◽  
Vol 17 (20) ◽  
pp. 13442-13450 ◽  
Author(s):  
Ruimin Wang ◽  
Yao Guo ◽  
Zheng Liu ◽  
Jiaqi Ma ◽  
Ming Yin ◽  
...  
Keyword(s):  
Experimental Observation ◽  
Four Wave Mixing ◽  
Noise Correlation ◽  
Wave Mixing ◽  
Intensity Noise ◽  
Phase Conjugate ◽  
Anti Stokes

We report the experimental observation of the intensity noise correlation and squeezing between counter propagating Stokes and anti-Stokes signals in Pr3+:Y2SiO5 crystals.

ULTRASLOW SOLITONS VIA FOUR-WAVE MIXING IN A CRYSTAL OF MOLECULAR MAGNETS

2009 ◽  
Vol 23 (07) ◽  
pp. 989-1004
Author(s):  
LIUGANG SI ◽  
XINYOU LÜ ◽  
PEIJUN SONG ◽  
JIBING LIU
Keyword(s):  
Magnetic Field ◽  
Electromagnetic Field ◽  
Group Velocity ◽  
Electromagnetic Fields ◽  
Continuous Wave ◽  
Four Wave Mixing ◽  
Molecular Magnets ◽  
Wave Mixing ◽  
Bright Solitons ◽  
Rotating Wave

The authors theoretically investigate the formation of ultraslow dark and bright solitons via four-wave mixing (FWM) in a crystal of molecular magnets in the presence of a uniform d.c. magnetic field, where two strong continuous wave pump electromagnetic fields and a weak-pulsed probe electromagnetic field produce a pulsed FWM electromagnetic field. By solving the Maxwell–Schrödinger equations under the slowly varying envelope approximation and rotating-wave approximations, we demonstrate that both the weak-pulsed probe and FWM electromagnetic fields can evolve into dark and bright solitons with the same shape and the same ultraslow group velocity.

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