scholarly journals Large phase shift of (1+1)-dimensional nonlocal spatial solitons in lead glass

2015 ◽  
Vol 338 ◽  
pp. 133-137 ◽  
Author(s):  
Qian Shou ◽  
Miao Wu ◽  
Qi Guo
2011 ◽  
Vol 36 (21) ◽  
pp. 4194 ◽  
Author(s):  
Qian Shou ◽  
Xiang Zhang ◽  
Wei Hu ◽  
Qi Guo

2004 ◽  
Vol 69 (1) ◽  
Author(s):  
Qi Guo ◽  
Boren Luo ◽  
Fahuai Yi ◽  
Sien Chi ◽  
Yiqun Xie

2014 ◽  
Vol 23 (8) ◽  
pp. 084204 ◽  
Author(s):  
Qian Shou ◽  
Dong-Wen Liu ◽  
Xiang Zhang ◽  
Wei Hu ◽  
Qi Guo

2017 ◽  
Vol 28 (38) ◽  
pp. 38LT04 ◽  
Author(s):  
Mircea Dragoman ◽  
Mircea Modreanu ◽  
Ian M Povey ◽  
Sergiu Iordanescu ◽  
Martino Aldrigo ◽  
...  

Nanophotonics ◽  
2018 ◽  
Vol 8 (1) ◽  
pp. 153-170 ◽  
Author(s):  
Yaxin Zhang ◽  
Yuncheng Zhao ◽  
Shixiong Liang ◽  
Bo Zhang ◽  
Lan Wang ◽  
...  

AbstractTerahertz (THz) science and technology promise unique applications in high-speed communications, high-accuracy imaging, and so on. To keep up with the demand for THz systems, THz dynamic devices should feature large phase shift modulation and high speed. To date, however, only a few devices can efficiently manipulate the phase of THz waves. In this paper, we demonstrate that efficient phase modulation of THz waves can be addressed by an active and enhanced resonant metamaterial embedded with a nanostructured 2D electron gas (2DEG) layer of a GaN high electron mobility transistor (HEMT). The enhanced resonant metaunit couples the traditional dipolar and inductance-capacitance resonances together to realize a coupling mode with enhanced resonance. Embedded with the nanostructured 2DEG layer of GaN HEMT, the resonance intensity and surface current circuit of the enhanced resonant mode in the metamaterial unit can be dynamically manipulated by the electrical control of the carrier distribution and depletion of the 3 nm 2DEG, leading to a phase shift greater than 150° in simulation. In the dynamic experiments, a 137° phase shift was achieved with an external controlling voltage of only several volts in the THz transmission mode. This work represents the first realization of a phase shift greater than 100° in a dynamic experiment in transmission mode using an active metamaterial structure with only a single layer. In addition, given the high-speed modulation ability of the HEMT, this concept provides a promising approach for the development of a fast and effective phase modulator in THz application systems.


2012 ◽  
Vol 20 (12) ◽  
pp. 13419 ◽  
Author(s):  
Juan Huo ◽  
Xianfeng Chen
Keyword(s):  

ACS Photonics ◽  
2018 ◽  
Vol 5 (8) ◽  
pp. 3040-3050 ◽  
Author(s):  
Yuncheng Zhao ◽  
Yaxin Zhang ◽  
Qiwu Shi ◽  
Shixiong Liang ◽  
Wanxia Huang ◽  
...  

1973 ◽  
Vol 21 ◽  
pp. 31-34
Author(s):  
L. Detre ◽  
B. Szeidl

AbstractPhotoelectric observations obtained with the 24-in. telescope of the Konkoly Observatory from 1950 to 1972 show that the amplitudes of the changes of the 0.d57 light-curve in the course of the 41-day cycle undergo considerable cyclic variations. The length of the cycles varies between 3.8 and 4.8 yr. A new cycle always begins with a large phase-shift in the 41-day period; afterwards there is generally no further shift during one 4-yr cycle. Following Julia Balázs’ hypothesis, a tentative model is suggested: The 41-day cycle is the rotation period of the star. Magnetic fields concentrated in a limited longitude zone influence the 0.d57 pulsation in such a way that variations in light amplitude and phase arise as aspect effects of the 41-day rotation period. In this way, the 4-yr cycle can be interpreted as the magnetic cycle of the star. The location of the magnetic fields strongly differs in longitude from cycle to cycle causing the observed large phase shifts at the beginning of a new 4-yr cycle.


2015 ◽  
Vol 15 (1) ◽  
Author(s):  
Richard K. Boadi ◽  
John R. Parker

AbstractIn his seminal paper of 1980, Mostow constructed a family of lattices in PU(2, 1), the holomorphic isometry group of complex hyperbolic 2-space. In this paper, we use a description of these lattices given by Thurston in terms of cone metrics on the sphere, which is equivalent to Deligne and Mostow’s description of them using monodromy of hypergeometric functions. We give an explicit fundamental domain for some of Mostow’s lattices, specifically those with large phase shift. Our approach follows Parker’s approach of describing Livné’s lattices in terms of cone metrics on the sphere. The content of this paper is based on Boadi’s PhD thesis.


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