Prospect of Applying Controlling Chaotic Vibration in the Waterborne-Noise Confrontation

Author(s):  
Rong-Jun Jiang ◽  
Shi-Jian Zhu ◽  
Lin He ◽  
Wei-Jian Qian

Abstract This paper taking the Duffing system with nonlinear soft stiffness as an example, discusses the possibility of applying the chaotic phenomenon to get a broadband frequency output for a single frequency input. Thereby proves the application value of controlling chaos in the waterborne-noise confrontation.

2013 ◽  
Vol 25 (10) ◽  
pp. 955-957 ◽  
Author(s):  
Ran Wang ◽  
Chunqing Gao ◽  
Yan Zheng ◽  
Mingwei Gao ◽  
Qing Ye

Author(s):  
I. Freitag ◽  
R. Henking ◽  
F. von Alvensleben ◽  
A. Tünnermann

2008 ◽  
Vol 33 (18) ◽  
pp. 2161 ◽  
Author(s):  
Bao-Quan Yao ◽  
Xiao-Ming Duan ◽  
Dan Fang ◽  
Yun-Jun Zhang ◽  
Liang Ke ◽  
...  

2013 ◽  
Vol 11 (4) ◽  
pp. 041406-41408 ◽  
Author(s):  
Mingwei Gao Mingwei Gao ◽  
Yu Zhao Yu Zhao ◽  
Luyan Zhang Luyan Zhang ◽  
Lei Wang Lei Wang ◽  
Chunqing Gao Chunqing Gao

2014 ◽  
Vol 989-994 ◽  
pp. 356-359
Author(s):  
Yong Ming Nie ◽  
Ya Kun Guo ◽  
Xin Ding ◽  
Min Min Guo

Single-frequency microchip lasers have been widely used in differential absorption radars, pulse coherent Doppler radars, pumping optical parametric oscillators, and etc. So theoretical analysis and experimental researches on the LD-pumped 2.09 μm microchip laser have important realistic meaning. According to quasi-three-level Cr, Tm, Ho: YAG(CTH:YAG) laser crystal working characteristics, the theoretical expression and relationship curve between the output optical power and 785nm LD-pumped power are obtained by theoretical calculating based on the pumping rate equation. The CTH:YAG crystal with 4mm diameter and 1 mm thickness is used to do experimental test. The corresponding three kinds of particle concentration are 0.85%, 5.9% and 0.36% respectively. When the crystal temperature is controlled at 10 °C, microchip laser beam output characteristic curve is obtained under different pump spots. The results show that when the pump spot diameter is 75um the maximum single-frequency output power is 32mW and when the pump beam is 100um the maximum single-frequency output power is 30mW. The corresponding optical to optical conversion slope efficiencies are 6.8% and 6% respectively.


2010 ◽  
Vol 18 (12) ◽  
pp. 12161 ◽  
Author(s):  
Jing Li ◽  
SuHui Yang ◽  
ChangMing Zhao ◽  
HaiYang Zhang ◽  
Wen Xie

1995 ◽  
Vol 20 (24) ◽  
pp. 2499 ◽  
Author(s):  
I. Freitag ◽  
R. Henking ◽  
A. Tünnermann ◽  
H. Welling

2003 ◽  
Vol 39 (24) ◽  
pp. 1717 ◽  
Author(s):  
Y. Jeong ◽  
J.K. Sahu ◽  
D.J. Richardson ◽  
J. Nilsson

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