Advanced Photonics
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Advanced Photonics 第1卷 第2期

Author Affiliations
Abstract
Université Bourgogne-Franche-Comté—CNRS UMR 6174, Institut FEMTO-ST, Besançon, France
Continued support for research and investment in photonics requires that the public and policy makers are made aware of its significance for societal development. All of us have a role to play in promoting the importance of our field.
Advanced Photonics
2019, 1(2): 020501
Author Affiliations
Abstract
1 University of Technology Sydney, Institute for Biomedical Materials and Devices, Faculty of Science, Ultimo, New South Wales, Australia
2 Southern University of Science and Technology, Department of Biomedical Engineering, Shenzhen, China
A fast off-axis scanning subvoxel light-sheet microscope enables high-throughput image large-volume specimens at cellular resolution.
Advanced Photonics
2019, 1(2): 020502
Author Affiliations
Abstract
1 Chalmers University of Technology, Gothenburg, Sweden
2 Instituto de Estructura de la Materia, Consejo Superior de Investigaciones Científicas, Madrid, Spain
Phonon-polaritons offer an exciting avenue in nanophotonics. We comment on the novel nanofabrication approach presented by Bo Qiang et al. in this issue of Advanced Photonics. Their approach to phononic material allows better radiation manipulation, and high Q-factors.
Advanced Photonics
2019, 1(2): 020503
Author Affiliations
Abstract
1 Harbin Institute of Technology, Department of Physics, Harbin, China
2 National University of Singapore, Department of Electrical and Computer Engineering, Singapore
Usually, an unfocused light beam, such as a paraxial Gaussian beam, can exert a force on an object along the direction of light propagation, which is known as light pressure. Recently, however, it was found that an unfocused light beam can also exert an optical pulling force (OPF) on an object toward the source direction; the beam is accordingly named an optical tractor beam. In recent years, this intriguing force has attracted much attention and a huge amount of progress has been made both in theory and experiment. We briefly review recent progress achieved on this topic. We classify the mechanisms to achieve an OPF into four different kinds according to the dominant factors. The first one is tailoring the incident beam. The second one is engineering the object’s optical parameters. The third one is designing the structured material background, in which the light–matter interaction occurs, and the fourth one is utilizing the indirect photophoretic force, which is related to the thermal effect of light absorption. For all the methods, we analyze the basic principles and review the recent achievements. Finally, we also give a brief conclusion and an outlook on the future development of this field.
optical pulling force optical tractor beam optical manipulation Bessel beam nanophotonic structures photophoresis photophoretic force 
Advanced Photonics
2019, 1(2): 024001
Author Affiliations
Abstract
University of Paderborn, Department of Physics, Paderborn, Germany
Free from phase-matching constraints, plasmonic metasurfaces have contributed significantly to the control of optical nonlinearity and enhancement of nonlinear generation efficiency by engineering subwavelength meta-atoms. However, high dissipative losses and inevitable thermal heating limit their applicability in nonlinear nanophotonics. All-dielectric metasurfaces, supporting both electric and magnetic Mie-type resonances in their nanostructures, have appeared as a promising alternative to nonlinear plasmonics. High-index dielectric nanostructures, allowing additional magnetic resonances, can induce magnetic nonlinear effects, which, along with electric nonlinearities, increase the nonlinear conversion efficiency. In addition, low dissipative losses and high damage thresholds provide an extra degree of freedom for operating at high pump intensities, resulting in a considerable enhancement of the nonlinear processes. We discuss the current state of the art in the intensely developing area of all-dielectric nonlinear nanostructures and metasurfaces, including the role of Mie modes, Fano resonances, and anapole moments for harmonic generation, wave mixing, and ultrafast optical switching. Furthermore, we review the recent progress in the nonlinear phase and wavefront control using all-dielectric metasurfaces. We discuss techniques to realize all-dielectric metasurfaces for multifunctional applications and generation of second-order nonlinear processes from complementary metal–oxide–semiconductor-compatible materials.
nonlinear optics dielectric metasurfaces Mie modes Fano resonances anapole modes harmonic generation 
Advanced Photonics
2019, 1(2): 024002
Shijie Feng 1,2,3Qian Chen 1,2,*Guohua Gu 1,2Tianyang Tao 1,2[ ... ]Chao Zuo 1,2,3,*
Author Affiliations
Abstract
1 Nanjing University of Science and Technology, School of Electronic and Optical Engineering, Nanjing, China
2 Jiangsu Key Laboratory of Spectral Imaging and Intelligent Sense, Nanjing, China
3 Nanjing University of Science and Technology, Smart Computational Imaging Laboratory (SCILab), Nanjing, China
In many optical metrology techniques, fringe pattern analysis is the central algorithm for recovering the underlying phase distribution from the recorded fringe patterns. Despite extensive research efforts for decades, how to extract the desired phase information, with the highest possible accuracy, from the minimum number of fringe patterns remains one of the most challenging open problems. Inspired by recent successes of deep learning techniques for computer vision and other applications, we demonstrate for the first time, to our knowledge, that the deep neural networks can be trained to perform fringe analysis, which substantially enhances the accuracy of phase demodulation from a single fringe pattern. The effectiveness of the proposed method is experimentally verified using carrier fringe patterns under the scenario of fringe projection profilometry. Experimental results demonstrate its superior performance, in terms of high accuracy and edge-preserving, over two representative single-frame techniques: Fourier transform profilometry and windowed Fourier transform profilometry.
fringe analysis phase measurement deep learning 
Advanced Photonics
2019, 1(2): 025001
Author Affiliations
Abstract
1 Nanyang Technological University, Centre for Disruptive Photonic Technologies, The Photonic Institute, School of Physical and Mathematical Sciences, Singapore
2 Nanyang Technological University, Centre for OptoElectronics and Biophotonics, School of Electrical and Electronic Engineering, Singapore
3 Agency for Science, Technology and Research, Institute of Materials Research and Engineering, Singapore
4 Agency for Science, Technology and Research, Institute of Manufacturing Technology, Singapore
Phonon polariton resonances in the mid-infrared spectral range demonstrate properties superior to noble metal-based plasmonics, owing to smaller dissipative loss and better field confinement. However, a conventional way to excite the localized phonon resonance involves ion etching, which reduces the attainable quality factors (Q-factors) of the resonators. We show that by introducing a deep subwavelength layer of dielectric gratings on a phononic substrate, localized dipolar resonance and higher order modes with high Q-factors 96 and 195, respectively, can be excited. We further demonstrate, via experiments and simulations, that the resonant wavelength and field confinement can be controlled by coupling the localized hybrid mode with propagating surface phonon-polaritons. We also observed for the first time the coupling between a localized dipolar mode and a propagating higher-order surface phonon-polariton mode. The results will be useful in designing on-chip, low-loss, and highly integrated phononic devices in the infrared spectral domain.
hybrid resonance high Q-factor phonon resonance mode splitting 
Advanced Photonics
2019, 1(2): 026001
Author Affiliations
Abstract
The article provides information about the image on the cover of Advanced Photonics, Volume 1, Issue 2.
Advanced Photonics
2019, 1(2): 029901

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