Programmable plasmonic phase modulation of free-space wavefronts at gigahertz rates

2019 ◽  
Vol 13 (6) ◽  
pp. 431-435 ◽  
Author(s):  
Alexei Smolyaninov ◽  
Abdelkrim El Amili ◽  
Felipe Vallini ◽  
Steve Pappert ◽  
Yeshaiahu Fainman
Keyword(s):  
Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Hongxin Zeng ◽  
Sen Gong ◽  
Lan Wang ◽  
Tianchi Zhou ◽  
Yaxin Zhang ◽  
...  

Abstract In the past ten years, terahertz technology has developed rapidly in wireless communications, spectroscopy, and imaging. Various functional devices have been developed, such as filters, absorbers, polarizers, mixers, and modulators. Among these, the terahertz phase modulation is a current research hotspot. It is the core technology to realize flexible control of the terahertz wavefront, beam scanning, focusing deflection. It is indispensable in terahertz wireless communication, high-resolution imaging, and radar systems. This review summarizes the research progress of terahertz phase modulators from the two major types: free space and guided wave integration. Among these, the free space terahertz phase modulator is realized by combining the tunable materials and artificial metasurfaces. Based on different types of tunable materials, the terahertz free space phase modulator combining the semiconductor, liquid crystal, phase change materials, graphene, and other two-dimensional materials are introduced, and the influence of different materials on the phase modulation performance is discussed and analyzed. The monolithic integration and waveguide embedding methods are introduced separately, and the characteristics of different forms of terahertz-guided wave phase modulation are also discussed. Finally, the development trends of terahertz phase modulators, possible new methods, and future application requirements are discussed.


2016 ◽  
Vol 11 (5) ◽  
pp. 367-374
Author(s):  
Huiying Zhang ◽  
Hongzuo Li ◽  
Xiao Dongya ◽  
Cai Chao

2003 ◽  
Vol 81 (4) ◽  
pp. 639-650 ◽  
Author(s):  
T Mikaelian ◽  
M Weel ◽  
A Kumarakrishnan ◽  
P R Battle ◽  
R C Swanson

We demonstrate that an electro-optic phase modulator (EOM) can be used as a constituent of a corner-cube-based modulated high-speed retro-reflector. We performed experiments to investigate the efficiency of the phase modulation produced by an EOM as a function of the angle of a laser beam incident on it. Our experiments demonstrate that the field of view of the EOM is determined by its dimensions and the diameter of the laser beam. This suggests that the device may be suitable for applications involving high-speed (GHz), free-space communication. In these applications, the retro-reflector can be mounted on a moving platform such as a satellite. We find that it is possible to detect the retro-reflected signal with an adequate signal-to-noise ratio using heterodyne detection. We also discuss some practical considerations necessary for the implementation of such a device. PACS Nos.: 42.60.–V, 42.62.Cf, 42.62.Fi, 42.79.Sz, 42.79.Hp


2012 ◽  
Vol 51 (19) ◽  
pp. 4457 ◽  
Author(s):  
Huimin Yue ◽  
Lei Song ◽  
Zexiong Hu ◽  
Hongxiang Liu ◽  
Yong Liu ◽  
...  

2019 ◽  
Vol 37 (2) ◽  
pp. 627-633 ◽  
Author(s):  
Ke Wang ◽  
Christina Lim ◽  
Elaine Wong ◽  
Kamal Alameh ◽  
Sithamparanathan Kandeepan ◽  
...  

Author(s):  
Z.M. Wang ◽  
J.P. Zhang

High resolution electron microscopy reveals that antiphase domain boundaries in β-Ni3Nb have a hexagonal unit cell with lattice parameters ah=aβ and ch=bβ, where aβ and bβ are of the orthogonal β matrix. (See Figure 1.) Some of these boundaries can creep “upstairs” leaving an incoherent area, as shown in region P. When the stepped boundaries meet each other, they do not lose their own character. Our consideration in this work is to estimate the influnce of the natural misfit δ{(ab-aβ)/aβ≠0}. Defining the displacement field at the boundary as a phase modulation Φ(x), following the Frenkel-Kontorova model [2], we consider the boundary area to be made up of a two unit chain, the upper portion of which can move and the lower portion of the β matrix type, assumed to be fixed. (See the schematic pattern in Figure 2(a)).


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