Electro‐optic amplitude modulation using three‐dimensional LiNbO3waveguide fabricated by TiO2diffusion

1975 ◽  
Vol 27 (1) ◽  
pp. 19-21 ◽  
Author(s):  
Juichi Noda ◽  
Naoya Uchida ◽  
Shoichi Saito ◽  
Tadashi Saku ◽  
Makoto Minakata
2011 ◽  
Vol 36 (2) ◽  
pp. 238 ◽  
Author(s):  
Noriaki Ohmae ◽  
Shigenori Moriwaki ◽  
Norikatsu Mio

2004 ◽  
Vol 846 ◽  
Author(s):  
Jessica Sinness ◽  
Olivier Clot ◽  
Scott R. Hammond ◽  
Nishant Bhatambrekar ◽  
Harrison L. Rommel ◽  
...  

ABSTRACTPrevious research in organic electro-optics has shown dramatic increases in the hyperpolarizablity of NLO chromophores. However, this large microscopic activity has not been translated to the macroscopic domain. The polymeric electro-optic (E-O) materials continue to lack the high noncentrosymmetric order of the poled chromophores within the matrix necessary for high E-O response (r33). This deficiency of order represents one major obstacle that must be overcome before E-O device commercialization can be achieved. This lack of order is partially due to the large dipole moments of high μβ chromophores, which cause the chromophores to align in a centrosymmetric fashion through intermolecular electrostatic interactions. However, quantum calculations show that when the aspect ratio between the width and length of the chromophore system is adjusted to be greater than 1.4:1 by adding bulky side groups around the center of the chromophore, it would prevent side on pairing of the chromophores. This would cause a decrease in the large areas of centrosymmetric aggregation and thus allow for easier poling of the system. Here we report the synthesis of a nanoscale NLO architecture in which dendritic moieties have been incorporated around the center of the chromophore to give a three dimensional structure in order to achieve the 1.4:1 aspect ratio and maximize the macroscopic order of the system.


Symmetry ◽  
2020 ◽  
Vol 12 (5) ◽  
pp. 748
Author(s):  
Yulong An ◽  
Yanmei Zhang ◽  
Haichao Guo ◽  
Jing Wang

Low-cost Laser Detection and Ranging (LiDAR) is crucial to three-dimensional (3D) imaging in applications such as remote sensing, target detection, and machine vision. In conventional nonscanning time-of-flight (TOF) LiDAR, the intensity map is obtained by a detector array and the depth map is measured in the time domain which requires costly sensors and short laser pulses. To overcome such limitations, this paper presents a nonscanning 3D laser imaging method that combines compressive sensing (CS) techniques and electro-optic modulation. In this novel scheme, electro-optic modulation is applied to map the range information into the intensity of echo pulses symmetrically and the measurements of pattern projection with symmetrical structure are received by the low bandwidth detector. The 3D imaging can be extracted from two gain modulated images that are recovered by solving underdetermined inverse problems. An integrated regularization model is proposed for the recovery problems and the minimization functional model is solved by a proposed algorithm applying the alternating direction method of multiplier (ADMM) technique. The simulation results on various subrates for 3D imaging indicate that our proposed method is feasible and achieves performance improvement over conventional methods in systems with hardware limitations. This novel method will be highly valuable for practical applications with advantages of low cost and flexible structure at wavelengths beyond visible spectrum.


2014 ◽  
Vol 25 (33) ◽  
pp. 335703 ◽  
Author(s):  
Christoph Marutschke ◽  
Deron Walters ◽  
Jason Cleveland ◽  
Ilka Hermes ◽  
Ralf Bechstein ◽  
...  

2013 ◽  
Vol 378 ◽  
pp. 322-326
Author(s):  
Zhi Yuan Zhou ◽  
Qing Xin Meng ◽  
Hao Tian ◽  
Zhong Xiang Zhou

The Terahertz modulator based on polymer electro-optic modulation is designed by Macher-Zehnder structure. The ridge waveguide is used to realize TM00 mode transmission, and the Y-branch with double circular arch type is to decrease the loss of transmission in modulator. The transmission of THz is analyzed by the beam propagate method (BPM). The structure parameters of the M-Z modulator, such as the size of ridge waveguide, the type of Y-branch and the optical offset structure for phase, are optimized to realize THz amplitude modulation. The depth of modulation is 83.8% when the applied field is 31.5V.


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