Two-photon correlated–spontaneous-emission laser: Quantum noise quenching and squeezing

1988 ◽  
Vol 60 (18) ◽  
pp. 1832-1835 ◽  
Author(s):  
Marlan O. Scully ◽  
K. Wódkiewicz ◽  
M. S. Zubairy ◽  
J. Bergou ◽  
Ning Lu ◽  
...  
ChemPhysChem ◽  
2010 ◽  
pp. n/a-n/a
Author(s):  
Hong Xia ◽  
Jie Yang ◽  
Hong-Hua Fang ◽  
Qi-Dai Chen ◽  
Hai-Yu Wang ◽  
...  

RSC Advances ◽  
2017 ◽  
Vol 7 (32) ◽  
pp. 19737-19741 ◽  
Author(s):  
Feng Jin ◽  
Liang Xu ◽  
Mei-Ling Zheng ◽  
Jing-Xia Wang ◽  
Xian-Zi Dong ◽  
...  

We demonstrate inhibition and enhancement of fluorescence of embedded fluorescent defects in colloidal crystals incorporated by two-photon polymerization.


2002 ◽  
Vol 202 (1-3) ◽  
pp. 221-225 ◽  
Author(s):  
Guangyong Zhou ◽  
Dong Wang ◽  
Xiaomei Wang ◽  
Xinguang Xu ◽  
Zongshu Shao ◽  
...  

2017 ◽  
Vol 34 (12) ◽  
pp. 2478 ◽  
Author(s):  
Alexander M. Akulshin ◽  
Nafia Rahaman ◽  
Sergey A. Suslov ◽  
Russell J. McLean

1989 ◽  
Vol 73 (1) ◽  
pp. 57-61 ◽  
Author(s):  
J. Bergou ◽  
Ning Lu ◽  
Marlan O. Scully

2003 ◽  
Vol 17 (22n24) ◽  
pp. 4123-4138 ◽  
Author(s):  
Wing-Shun Lam ◽  
Parvez N. Guzdar ◽  
Rajarshi Roy

The dynamical behavior of power dropouts in a semiconductor laser with optical feedback, pumped near threshold current, is strongly influenced by quantum noise. This is clearly demonstrated by experiments with modulations on the pumping current or the feedback strength. For the cases without modulation and with only current modulation, the dropouts occur randomly. However the feedback strength modulation locks the dropout events periodically. By numerically modeling these three cases using the Lang–Kobayashi equations with a stochastic term to take into account spontaneous emission noise, it is shown that the observed behavior of the dropouts can be readily reproduced for all three cases. Noise plays a signifcant role in explaining the observed dropout events. A simple explanation of the observed dropout phenomenon is presented, based on the adiabatic motion of the ellipse formed by the steady state solutions of the rate equations due to slow time modulations of the injection current or the feedback strength.


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