Scalar and vectorial vortex filtering based on geometric phase modulation with a Q-plate

2019 ◽  
Vol 21 (6) ◽  
pp. 065702 ◽  
Author(s):  
Delin Li ◽  
Shaotong Feng ◽  
Shouping Nie ◽  
Jun Ma ◽  
Caojin Yuan
2021 ◽  
pp. 127847
Author(s):  
Yongmo Lv ◽  
Shaoyun Yin ◽  
Yi Liu ◽  
Zhe Li ◽  
Peng Li ◽  
...  

2020 ◽  
Vol 11 (1) ◽  
Author(s):  
Yueyi Yuan ◽  
Kuang Zhang ◽  
Badreddine Ratni ◽  
Qinghua Song ◽  
Xumin Ding ◽  
...  

ACS Photonics ◽  
2021 ◽  
Author(s):  
Ruonan Ji ◽  
Xin Xie ◽  
Xuyue Guo ◽  
Yang Zhao ◽  
Chuan Jin ◽  
...  

2020 ◽  
Vol 45 (22) ◽  
pp. 6330
Author(s):  
Shiyao Fu ◽  
Xu Han ◽  
Rui Song ◽  
Lei Huang ◽  
Chunqing Gao

2004 ◽  
Vol 237 (1-3) ◽  
pp. 9-15 ◽  
Author(s):  
N. Murakami ◽  
Y. Kato ◽  
N. Baba ◽  
T. Ishigaki

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)).


2014 ◽  
Vol E97.B (10) ◽  
pp. 2102-2109
Author(s):  
Tsubasa TASHIRO ◽  
Kentaro NISHIMORI ◽  
Tsutomu MITSUI ◽  
Nobuyasu TAKEMURA

Sign in / Sign up

Export Citation Format

Share Document