scholarly journals Adaptive aberration compensation for three-dimensional micro-fabrication of photonic crystals in lithium niobate

2011 ◽  
Vol 19 (10) ◽  
pp. 9419 ◽  
Author(s):  
Benjamin P. Cumming ◽  
Alexander Jesacher ◽  
Martin J. Booth ◽  
Tony Wilson ◽  
Min Gu
2009 ◽  
Vol 21 (34) ◽  
pp. 3526-3530 ◽  
Author(s):  
Airán Ródenas ◽  
Guangyong Zhou ◽  
Daniel Jaque ◽  
Min Gu

2019 ◽  
Vol 10 (1) ◽  
Author(s):  
Dunzhao Wei ◽  
Chaowei Wang ◽  
Xiaoyi Xu ◽  
Huijun Wang ◽  
Yanlei Hu ◽  
...  

Abstract Nonlinear beam shaping refers to spatial reconfiguration of a light beam at a new frequency, which can be achieved by using nonlinear photonic crystals (NPCs). Direct nonlinear beam shaping has been achieved to convert second-harmonic waves into focusing spots, vortex beams, and diffraction-free beams. However, previous nonlinear beam shaping configurations in one-dimensional and two-dimensional (2D) NPCs generally suffer from low efficiency because of unfulfilled phase-matching condition. Here, we present efficient generations of second-harmonic vortex and Hermite-Gaussian beams in the recently-developed three-dimensional (3D) lithium niobate NPCs fabricated by using a femtosecond-laser-engineering technique. Since 3D χ(2) modulations can be designed to simultaneously fulfill the requirements of nonlinear wave-front shaping and quasi-phase-matching, the conversion efficiency is enhanced up to two orders of magnitude in a tens-of-microns-long 3D NPC in comparison to the 2D case. Efficient nonlinear beam shaping paves a way for its applications in optical communication, super-resolution imaging, high-dimensional entangled source, etc.


Author(s):  
Ted Janssen ◽  
Gervais Chapuis ◽  
Marc de Boissieu

The law of rational indices to describe crystal faces was one of the most fundamental law of crystallography and is strongly linked to the three-dimensional periodicity of solids. This chapter describes how this fundamental law has to be revised and generalized in order to include the structures of aperiodic crystals. The generalization consists in using for each face a number of integers, with the number corresponding to the rank of the structure, that is, the number of integer indices necessary to characterize each of the diffracted intensities generated by the aperiodic system. A series of examples including incommensurate multiferroics, icosahedral crystals, and decagonal quaiscrystals illustrates this topic. Aperiodicity is also encountered in surfaces where the same generalization can be applied. The chapter discusses aperiodic crystal morphology, including icosahedral quasicrystal morphology, decagonal quasicrystal morphology, and aperiodic crystal surfaces; magnetic quasiperiodic systems; aperiodic photonic crystals; mesoscopic quasicrystals, and the mineral calaverite.


2005 ◽  
Vol 13 (7) ◽  
pp. 2370 ◽  
Author(s):  
Peng Yao ◽  
Garrett J. Schneider ◽  
Dennis W. Prather ◽  
Eric D. Wetzel ◽  
Daniel J. O'Brien

2005 ◽  
Vol 87 (9) ◽  
pp. 091117 ◽  
Author(s):  
Dennis McPhail ◽  
Martin Straub ◽  
Min Gu

Sign in / Sign up

Export Citation Format

Share Document