DOCSLIB.ORG

Robust Extended-Range Wireless Power Transfer Using a Higher-Order PT-Symmetric Platform

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Robust Extended-Range Wireless Power Transfer Using a Higher-Order PT-Symmetric Platform PHYSICAL REVIEW RESEARCH 2, 013152 (2020) Robust extended-range wireless power transfer using a higher-order PT-symmetric platform Maryam Sakhdari, Mehdi Hajizadegan, and Pai-Yen Chen * Department of Electrical and Computer Engineering, University of Illinois at Chicago, Chicago, Illinois 60607, USA (Received 4 October 2019; accepted 6 December 2019; published 12 February 2020) A fundamental challenge for the nonradiative wireless power transfer (WPT) resides in maintaining the stable power transmission with a consistently high efficiency under dynamic conditions. Here, we propose and experimentally demonstrate that a frequency-locked WPT system satisfying the higher-order parity-time (PT) symmetry can achieve a near-unity power transfer efficiency that is resilient to effects of distance variation and misalignment between coils, and impedance fluctuations in electric grids. In specific higher-order PT electronic systems, a purely real-valued and coupling-invariant (nonbifurcated) eigenfrequency would enable the robust and efficient wireless charging without frequency hopping or adaptive impedance matching, even for midrange operation. We envision that this WPT technique may provide reliable, fast and efficient power delivery for a variety of consumer electronics, electric vehicles, and medical devices. DOI: 10.1103/PhysRevResearch.2.013152 I. INTRODUCTION when the coupling factor (as a function of distance and alignment between coils) changes, the operating frequency Radio-frequency (RF) wireless power transfer (WPT) has must be adjusted accordingly to maintain a high transfer experienced a rapid and widespread growth in recent years, efficiency [20,21]. Besides, the range of inductive power as driven by the rising demand for wireless charging in transfer remains a principal challenge. In spite of advances in consumer electronics, medical devices, sensors, and automo- various coil designs and the capability to create spatial Bessel tive applications [1–10]. The concept of transferring power beams [22], it remains difficult to overcome the performance without any physical contact was put forward soon after the deterioration due to the poor tolerance in coil misalignment, proposition of Faraday’s law of induction [11]. In late 1890s, especially in the weak-coupling regime [23,24]. Nikola Tesla conducted pioneering experiments with lighting Very recently, a new WPT mechanism based on the concept electric bulbs wirelessly through electrodynamic induction of parity-time (PT) symmetry incorporating a nonlinear gain- (also known as resonant inductive coupling) [12]. Although saturation element has been projected to address this long- his efforts appear to have met with little success, nowadays, existing challenge [7]. Specifically, this system is engineered considerable progress in WPT has been made in the realm to have a subtle balance of energy flowing in (i.e., gain) of nonradiative transfer that employs the near-field magnetic and out (i.e., loss), and in its exact PT-symmetric phase, a coupling to efficiently transmit electrical energy from a power nearly perfect transfer efficiency that is independent of the source to electrical loads [3]. While the WPT technology has coupling strength can be achieved for the short-range oper- motivated considerable research and development in the past ation. Even more importantly, this PT-symmetric nonlinear two decades [13–15], there are still several fundamental issues WPT system does not need the dynamic frequency recon- which need further investigation to maximize the potential figuration. In contrast, when the standard second-order PT of this technology. Traditional WPT systems are not robust system is adopted for wireless powering applications [7], the against alteration of distance and misalignment between coils system requires adaptive frequency tuning (although within [5,16], and variations in the terminating impedance of an a narrow range) and switch-mode amplifiers that cover the electric power grid or battery over time [1]. To date, several full range of operating frequencies. Adjusting the operating techniques have been proposed to optimize the efficiency frequency may increase the design complexity and cost, since of power transfer, which include dynamic adjustment of the system requires tunable filters with high quality factor and operating frequency (resonant-frequency tracking) [17,18], synchronization of convertor/invertor in the transmitter and combination of multiple receivers and repeaters for adaptive receiver. impedance matching [19], and adding nonlinear tuning ele- However, in the standard (second-order) PT-symmetric ments in circuits [7,10]. For these often used WPT schemes, electronic systems [25–34], the exact PT-symmetric phase requires a moderately strong coupling strength [25,28], and this makes the system fail to maintain a satisfactory efficiency *Corresponding author: [email protected] at weak/loose coupling (e.g., midrange power transfer). In addition, perturbing the load resistance of receiver could lead Published by the American Physical Society under the terms of the to a symmetry-breaking phase transition [29,34] and a low Creative Commons Attribution 4.0 International license. Further efficiency is obtained in such broken PT-symmetric phases. distribution of this work must maintain attribution to the author(s) In the following, we will present a new nonradiative WPT and the published article’s title, journal citation, and DOI. system with high-order PT symmetry, as shown in Fig. 1, 2643-1564/2020/2(1)/013152(11) 013152-1 Published by the American Physical Society SAKHDARI, HAJIZADEGAN, AND CHEN PHYSICAL REVIEW RESEARCH 2, 013152 (2020) FIG. 1. (a) Schematics for (i) standard, (ii) third-order, and (iii) generalized higher-order PT-symmetric electronic systems consisting of electronic molecules with gain (red), neutral (gray), and loss (blue) properties. (b) Third-order PT-symmetric wireless power transfer system, where a robot car (loss) is wirelessly charged by a platform consisting of a repeater (neutral) and an active transmitter (gain). The inductive coupling strength between the intermediate and receiver coils (κ) is random, and that between the transmitter and intermediate coils (κ)is tuned by rotating the transmitter coil and a feedback algorithm, such that κ = κ and PT symmetry is preserved. which can further overcome the drawback of the standard cal [36,37], acoustic [38] and electronic [25–34] platforms, PT-symmetric WPT system. Higher-order PT-symmetric elec- and has aroused intense interest for real-life applications, tronic systems in Fig. 1(a) exhibit a unique eigenspectral such as lasers [39–41], sensors [28–32,42–46], cloaks [47,48], feature: a purely real eigenfrequency that is insensitive to and nonreciprocal devices [49]. In electronics, the lumped- variations in the coupling strength and the gain-loss parameter element circuitry could be the simplest possible configuration (related to the receiver’s load impedance). Such a property for observation of exotic physics of PT-symmetric Hamilto- can ensure a transfer efficiency approaching 100% over a nian [30]. In analogy to optical cases, spatially-distributed, wide range of distances and misalignment levels, thereby balanced gain and loss can be readily realized with an active offering an unprecedented robustness and freedom in wireless negative-resistance converter [50,51] and a resistor, which charging. are connected through either capacitive or inductive links, as illustrated in Fig. 1(a). Figure 1(b) presents the proposed third-order (TO) PT-symmetric WPT systems with an equiv- alent circuit model shown in Fig. 1(a) (type ii). In this case, II. HIGHER-ORDER PT-SYMMETRIC the transmitter, repeater, and receiver are represented by the WIRELESS POWERING −RLC, LC, and RLC oscillators, respectively. Here, inductive In 1998, Bender and Boettcher introduced a class of couplings between the neighboring oscillators are identical, non-Hermitian Hamiltonians [35] satisfying PT symmetry. and the coupling between the transmitter and receiver is Counterintuitively, if a quantum system is invariant under the assumed to be ignorable. These coupled the −RLC, LC, combined action of space inversion (P ) and time reversal (T), and RLC oscillators are analogous to “electronic” molecules it exhibits either entirely real eigenspectra or complex conju- with gain, neutral, and loss characteristics, whose relations gate eigenvalue pairs. Although PT-symmetry was originally can be described by a PT -symmetric Hamiltonian. Applying considered as one of interesting theoretical findings in quan- Kirchhoff’s laws to this circuit, the system can be described tum physics, it has been experimentally demonstrated in opti- by Liouvillian formalism: ⎛ ⎞ 000 100 ⎜ ⎟ ⎜ 000 010⎟ ⎜ 000 001⎟ d ⎜ 2 2 2 2 ⎟ L = , L = ⎜− 1−κ κ − κ 1 1−κ 0 − 1 κ ⎟, (1) dτ ⎜ 1−2κ2 1−2κ2 1−2κ2 γ 1−2κ2 γ 1−2κ2 ⎟ ⎜ κ − 1 κ − 1 κ 1 κ ⎟ ⎝ 1−2κ2 1−2κ2 1−2κ2 γ 1−2κ2 0 γ 1−2κ2 ⎠ − κ2 κ − 1−κ2 1 κ2 − 1 1−κ2 1−2κ2 1−2κ2 1−2κ2 γ 1−2κ2 0 γ 1−2κ2 T ω . where ≡ (q1, q2, q3, q˙1, q˙2, q˙3) , qk andq ˙k correspond to measured in units of 0 The effective Hamiltonian can be the charge stored on the capacitor and the displacement cur- written as Heff = iL(Heff = i∂τ ), which is non-Hermitian † = rent in the kth oscillator (the subscripts 1, 2, and 3 denote (Heff Heff ) and symmetric with respect to the PT transfor- , = the active, neutral, and passive tanks, respectively), τ ≡ ω0t, mation, namely [PT Heff ] 0, with the natural frequency of the neutral LC√tank, the gain-loss − parameter (or non-Hermiticity) γ = R 1 L/C, the coupling J 0 I 0 strength characterized by the rescaled mutual inductance = and = , (2) √ P 0 J T 0 −I K κ = M/L, ω0 = 1/ LC, and all (angular) frequencies are 013152-2 ROBUST EXTENDED-RANGE WIRELESS POWER … PHYSICAL REVIEW RESEARCH 2, 013152 (2020) FIG. 2. Evolution of the real (top) and imaginary (bottom) parts of eigenfrequencies as a function the gain-loss parameter γ and the coupling strength κ, for the (a) third-order and (b) standard PT-symmetric electronic systems in Fig. 1(a) (see types i and ii).
Load more

Recommended publications
  • Quantum Optics with Giant Atoms – the First Five Years
    Quantum optics with giant atoms – the first five years Anton Frisk Kockum Abstract In quantum optics, it is common to assume that atoms can be approximated as point-like compared to the wavelength of the light they interact with. However, recent advances in experiments with artificial atoms built from superconducting circuits have shown that this assumption can be violated. Instead, these artificial atoms can couple to an electromagnetic field at multiple points, which are spaced wavelength distances apart. In this chapter, we present a survey of such systems, which we call giant atoms. The main novelty of giant atoms is that the multiple coupling points give rise to interference effects that are not present in quantum optics with ordinary, small atoms. We discuss both theoretical and experimental results for single and multiple giant atoms, and show how the interference effects can be used for interesting applications. We also give an outlook for this emerging field of quantum optics. Key words: Quantum optics, Giant atoms, Waveguide QED, Relaxation rate, Lamb shift, Superconducting qubits, Surface acoustic waves, Cold atoms 1 Introduction Natural atoms are so small (radius r ≈ 10−10 m) that they can be considered point- like when they interact with light at optical frequencies (wavelength λ ≈ 10−6 − 10−7 m)[1]. If the atoms are excited to high Rydberg states, they can reach larger sizes (r ≈ 10−8 − 10−7 m), but quantum-optics experiments with such atoms have them interact with microwave radiation, which has much longer wavelength (λ ≈ arXiv:1912.13012v1 [quant-ph] 30 Dec 2019 10−2 −10−1 m)[2].
    [Show full text]
  • Merging Photonics and Artificial Intelligence at the Nanoscale
    Intelligent Nanophotonics: Merging Photonics and Artificial Intelligence at the Nanoscale Kan Yao1,2, Rohit Unni2 and Yuebing Zheng1,2,* 1Department of Mechanical Engineering, The University of Texas at Austin, Austin, Texas 78712, USA 2Texas Materials Institute, The University of Texas at Austin, Austin, Texas 78712, USA *Corresponding author: [email protected] Abstract: Nanophotonics has been an active research field over the past two decades, triggered by the rising interests in exploring new physics and technologies with light at the nanoscale. As the demands of performance and integration level keep increasing, the design and optimization of nanophotonic devices become computationally expensive and time-inefficient. Advanced computational methods and artificial intelligence, especially its subfield of machine learning, have led to revolutionary development in many applications, such as web searches, computer vision, and speech/image recognition. The complex models and algorithms help to exploit the enormous parameter space in a highly efficient way. In this review, we summarize the recent advances on the emerging field where nanophotonics and machine learning blend. We provide an overview of different computational methods, with the focus on deep learning, for the nanophotonic inverse design. The implementation of deep neural networks with photonic platforms is also discussed. This review aims at sketching an illustration of the nanophotonic design with machine learning and giving a perspective on the future tasks. Keywords: deep learning; (nano)photonic neural networks; inverse design; optimization. 1. Introduction Nanophotonics studies light and its interactions with matters at the nanoscale [1]. Over the past decades, it has received rapidly growing interest and become an active research field that involves both fundamental studies and numerous applications [2,3].
    [Show full text]
  • Up-And-Coming Physical Concepts of Wireless Power Transfer
    Up-And-Coming Physical Concepts of Wireless Power Transfer Mingzhao Song1,2 *, Prasad Jayathurathnage3, Esmaeel Zanganeh1, Mariia Krasikova1, Pavel Smirnov1, Pavel Belov1, Polina Kapitanova1, Constantin Simovski1,3, Sergei Tretyakov3, and Alex Krasnok4 * 1School of Physics and Engineering, ITMO University, 197101, Saint Petersburg, Russia 2College of Information and Communication Engineering, Harbin Engineering University, 150001 Harbin, China 3Department of Electronics and Nanoengineering, Aalto University, P.O. Box 15500, FI-00076 Aalto, Finland 4Photonics Initiative, Advanced Science Research Center, City University of New York, NY 10031, USA *e-mail: [email protected], [email protected] Abstract The rapid development of chargeable devices has caused a great deal of interest in efficient and stable wireless power transfer (WPT) solutions. Most conventional WPT technologies exploit outdated electromagnetic field control methods proposed in the 20th century, wherein some essential parameters are sacrificed in favour of the other ones (efficiency vs. stability), making available WPT systems far from the optimal ones. Over the last few years, the development of novel approaches to electromagnetic field manipulation has enabled many up-and-coming technologies holding great promises for advanced WPT. Examples include coherent perfect absorption, exceptional points in non-Hermitian systems, non-radiating states and anapoles, advanced artificial materials and metastructures. This work overviews the recent achievements in novel physical effects and materials for advanced WPT. We provide a consistent analysis of existing technologies, their pros and cons, and attempt to envision possible perspectives. 1 Wireless power transfer (WPT), i.e., the transmission of electromagnetic energy without physical connectors such as wires or waveguides, is a rapidly developing technology increasingly being introduced into modern life, motivated by the exponential growth in demand for fast and efficient wireless charging of battery-powered devices.
    [Show full text]
  • DNA Nanotechnology Meets Nanophotonics
    DNA nanotechnology meets nanophotonics Na Liu 2nd Physics Institute, University of Stuttgart, Pfaffenwaldring 57, 70569 Stuttgart, Germany Max Planck Institute for Solid State Research, Heisenbergstrasse 1, 70569 Stuttgart, Germany Email: [email protected] Key words: DNA nanotechnology, nanophotonics, DNA origami, light matter interactions Call-out sentence: It will be very constructive, if more research funds become available to support young researchers with bold ideas and meanwhile allow for failures and contingent outcomes. The first time I heard the two terms ‘DNA nanotechnology’ and ‘nanophotonics’ mentioned together was from Paul Alivisatos, who delivered the Max Planck Lecture in Stuttgart, Germany, on a hot summer day in 2008. In his lecture, Paul showed how a plasmon ruler containing two metallic nanoparticles linked by a DNA strand could be used to monitor nanoscale distance changes and even the kinetics of single DNA hybridization events in real time, readily correlating nanoscale motion with optical feedback.1 Until this day, I still vividly remember my astonishment by the power and beauty of these two nanosciences, when rigorously combined together. In the past decades, DNA has been intensely studied and exploited in different research areas of nanoscience and nanotechnology. At first glance, DNA-based nanophotonics seems to deviate quite far from the original goal of Nadrian Seeman, the founder of DNA nanotechnology, who hoped to organize biological entities using DNA in high-resolution crystals. As a matter of fact, DNA-based nanophotonics does closely follow his central spirit. That is, apart from being a genetic material for inheritance, DNA is also an ideal material for building molecular devices.
    [Show full text]
  • Inverse Design for Silicon Photonics: from Iterative Optimization Algorithms to Deep Neural Networks
    applied sciences Review Inverse Design for Silicon Photonics: From Iterative Optimization Algorithms to Deep Neural Networks Simei Mao 1,2, Lirong Cheng 1,2 , Caiyue Zhao 1,2, Faisal Nadeem Khan 2, Qian Li 3 and H. Y. Fu 1,2,* 1 Tsinghua-Berkeley Shenzhen Institute, Tsinghua University, Shenzhen 518055, China; [email protected] (S.M.); [email protected] (L.C.); [email protected] (C.Z.) 2 Tsinghua Shenzhen International Graduate School, Tsinghua University, Shenzhen 518055, China; [email protected] 3 School of Electronic and Computer Engineering, Peking University, Shenzhen 518055, China; [email protected] * Correspondence: [email protected]; Tel.: +86-755-3688-1498 Abstract: Silicon photonics is a low-cost and versatile platform for various applications. For design of silicon photonic devices, the light-material interaction within its complex subwavelength geometry is difficult to investigate analytically and therefore numerical simulations are majorly adopted. To make the design process more time-efficient and to improve the device performance to its physical limits, various methods have been proposed over the past few years to manipulate the geometries of silicon platform for specific applications. In this review paper, we summarize the design methodologies for silicon photonics including iterative optimization algorithms and deep neural networks. In case of iterative optimization methods, we discuss them in different scenarios in the sequence of increased degrees of freedom: empirical structure, QR-code like structure and irregular structure. We also review inverse design approaches assisted by deep neural networks, which generate multiple devices Citation: Mao, S.; Cheng, L.; Zhao, with similar structure much faster than iterative optimization methods and are thus suitable in C.; Khan, F.N.; Li, Q.; Fu, H.Y.
    [Show full text]
  • Wirelessly-Powered Cage Designs for Supporting Long-Term Experiments on Small Freely Behaving Animals in a Large Experimental Arena
    electronics Review Wirelessly-Powered Cage Designs for Supporting Long-Term Experiments on Small Freely Behaving Animals in a Large Experimental Arena Byunghun Lee 1 and Yaoyao Jia 2,* 1 Department of Electrical Engineering, Incheon National University, Incheon 22012, Korea; [email protected] 2 Department of Electrical and Computer Engineering, North Carolina State University, 890 Oval Dr, Raleigh, NC 27606, USA * Correspondence: [email protected]; Tel.: +1-919-515-7350 Received: 22 October 2020; Accepted: 18 November 2020; Published: 25 November 2020 Abstract: In modern implantable medical devices (IMDs), wireless power transmission (WPT) between inside and outside of the animal body is essential to power the IMD. Unlike conventional WPT, which transmits the wireless power only between fixed Tx and Rx coils, the wirelessly-powered cage system can wirelessly power the IMD implanted in a small animal subject while the animal freely moves inside the cage during the experiment. A few wirelessly-powered cage systems have been developed to either directly power the IMD or recharge batteries during the experiment. Since these systems adapted different power carrier frequencies, coil configurations, subject tracking techniques, and wireless powered area, it is important for designers to select suitable wirelessly-powered cage designs, considering the practical limitations in wirelessly powering the IMD, such as power transfer efficiency (PTE), power delivered to load (PDL), closed-loop power control (CLPC), scalability, spatial/angular misalignment, near-field data telemetry, and safety issues against various perturbations during the longitudinal animal experiment. In this article, we review the trend of state-of-the-art wirelessly-powered cage designs and practical considerations of relevant technologies for various IMD applications.
    [Show full text]
  • NANOPHOTONICS a FORWARD LOOK NANOPHOTONICS Association a FORWARD LOOK
    association NANOPHOTONICS A FORWARD LOOK NANOPHOTONICS association A FORWARD LOOK Report Editors Gonçal Badenes, ICFO Stewe Bekk, ICFO Martin Goodwin, 2020 Insights DESIGN Sergio Simón Petreñas D.L. B-29170-2012 (Printed version) B-29171-2012 (Electronic version) © 2012 NEA. The text of this publication may be reproduced provided the source is acknowledged. Reproduction for commercial use without prior permission is prohibited. PICTURES © reserved by original copyright holder. Reproduction of the artistic material contained therein is prohibited The Nanophotonics Europe Association is partially funded by the Spanish Ministry of Economy and Competitiveness through grant ACI-2009-1013 NANOPHOTONICS association A FORWARD LOOK About this Report This document is the report of the Nanophotonics Europe Association workshop held at King's College, London (UK) in July 2012. The purpose was to define a strategy for advancing research and development of nanophotonics. The views, ideas, conclusions and recommendations presented in this report are those of the workshop participants. Nanophotonics Europe Association The Nanophotonics Europe Association (NEA) is a not-for-profit organisation created to promote and advance European science and technology in the emerging area of nanophotonics. The goals of the association are fourfold: 1. To promote research in nanophotonics by coordinating the efforts of the various players involved, and, in particular, by encouraging collaboration between academic institution and industry. 2. To create a common interest group that represents member’s interests with national and transnational scientific government funding agencies, technology platforms, professional associations and the general public. 3. To integrate the resources and strategies of its members. 4. To facilitate the exchange of information, ideas and data.
    [Show full text]
  • Advanced Trends of Nanophotonics
    Part VII Advanced Trends of Nanophotonics Wei Ting Chen and Din Ping Tsai Introduction Nanophotonics is the study of the behavior of light-matter interaction at the nanometer scale. By adding the dimensions of optical devices and components to sub-wavelength scale, nanophotonics provides new opportunities for fundamen- tal science and practical applications. One of the goals of nanophotonics devel- opment is to manipulate light at the nanoscale, which may not be limited by the chemical composition of natural materials and the diffraction limit of electromag- netic wave. Nanophotonics has several advantages with such diffraction-unlimited properties for functional applications: (i) nanoscale footprints-smaller compo- nents and devices; (ii) photon-electron process in nanoscale—faster processing speed, and (iii) nanoscale confinement of optical radiation and electromagnetic fields—enhancing the light-matter interactions and dramatically reducing the optical energy consumption. The characterization of drastic optical localization within such components strongly enhances the typically weak interaction between light and matter, which increases the energy efficiency to obtain desired effects and phenomena. This chapter covers two major parts of the latest trends of nano- photonics, plasmonics, and metamaterials. Several cutting-edge approaches har- vested from the extraordinary properties of nanophotonics, which are conducted to advanced trends relate to: Micro/nano-lasers with the smallest plasmonic nano- laser, theoretical models of the micro/nano-cavity, and semiconductor micro-lasers with tuning functions on a flexible substrate (Chap. 16, 17 and 19), nanostructures light-emitting diode (LED) with better light extraction and reduced piezoelectric field induced by strain (Chap.18 , 24), one-dimensional photonic crystal nanowires with small footprints and ultrahigh Q-factors (Chap.
    [Show full text]
  • Recent Trends in Micro- and Nanophotonics: a Personal Selection
    JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS Vol. 13, No. 9, September 2011, p. 1055 - 1066 Recent trends in micro- and nanophotonics: A personal selection D. MIHALACHE Horia Hulubei National Institute for Physics and Nuclear Engineering, P. O. B. MG-6, 077125 Magurele, Romania I give a brief overview of some recent results in micro- and nanophotonics. Due to the vast amount of research activity in these exploding areas I only concentrate on selected recent advances in (a) silicon photonics, (b) spatial and spatiotemporal optical solitons (alias light bullets) in microwaveguide arrays and in arrays of evanescently-coupled silicon- on-insulator nanowires, (c) spatial solitons in photorefractive materials, (d) nanoplasmonics, (e) photonic crystals, (f) metamaterials for micro- and nanophotonics including optical materials with negative refractive indices, (g) terahertz radiation and its applications, and (h) solid-state single photon sources and nanometric size optical cavities for quantum information processing. (Received August 12, 2011; accepted September 15, 2011) Keywords: Microphotonics, Nanophotonics, Silicon photonics, Plasmonics, Photonic crystals, Spatial optical solitons, Light bullets, Plasmonic lattice solitons, Metamaterials, Terahertz radiation 1. Introduction for biosensing and chemical sensing applications, ability of metal nanoparticles to act as efficient pointlike sources The term “photonics” was coined in 1967 by Pierre of both light and heat, and subwavelength plasmonic Aigrain, a French scientist, who gave the following lattice solitons in arrays of metallic nanowires embedded definition: “Photonics is the science of the harnessing of in nonlinear Kerr media will be briefly discussed. light. Photonics encompasses the generation of light, the Section 4 is devoted to recent advances in the study of detection of light, the management of light through photonic crystals and metamaterial structures (including guidance, manipulation, and amplification, and most engineered media with negative refractive indices).
    [Show full text]
  • From Classical Optics to Nanophotonics
    FEATURES FROM CLASSICAL OPTICS TO NANOPHOTONICS 1 1 1 2 l François Flory , Ludovic Escoubas , Judikael¨ Le Rouzo , Gerard´ Berginc – DOI: https://doi.org/10.1051/ epn/2018503 l IM2NP – Faculte´ des Sciences et Techniques – Avenue Escadrille Normandie Niemen, Service 262 – 13397 Marseille cedex, France l THALES Optronique SA – 2 avenue Gay-Lussac – 78990 Elancourt, France Nanophotonics is a very large and rich young field experienting a very rapid development worldwide. It is based on the study of light/matter interaction at low dimension. Several books are dedicated to different aspects of nanophotonics [1]. FIG 1: long list of philosophers/scientists allowed (1000 A.D.) described light propagation, till 13th cen- (a) SEM image understanding the nature of light and of its tury Italian glassworkers made lenses that were used of Black Silicon surface obtained by interaction with matter, the development for spectacles. Kepler (1604) decribed the propagation cryogenic process. Aof optical instruments and of lasers. We of light through lenses with geometrical optics, and he (b) Cryogenic plasma can briefly cited some of them who are known to bring applied his studies to the eye. Lippershey invented the process black silicon reflectivity compared important steps in these progresses. By trying to explain telescope soon before Galileo (1609) produced his own with unprocessed vision, Greek like Euclid (300 B.C.), Hero (60 A.D.), telescope and started to study planets and moons. Snell, silicon. [10] Ptolemy (120 A. D.) and then the Arab scientist Alhazen Descartes(~1637), Newton (~1704) , Grimaldi (~1665), Huygens (~1690), Euler (1746), Gauss (~1800), Young (1803), Fraunhofer(1814), Fresnel (1819) , Abbe (1887)..
    [Show full text]
  • Review Article Nanophotonics for Molecular Diagnostics and Therapy Applications
    Hindawi Publishing Corporation International Journal of Photoenergy Volume 2012, Article ID 619530, 11 pages doi:10.1155/2012/619530 Review Article Nanophotonics for Molecular Diagnostics and Therapy Applications Joao˜ Conde,1, 2 Joao˜ Rosa,1, 3 Joao˜ C. Lima,3 and Pedro V. Baptista1 1 CIGMH, Departamento de Ciˆencias da Vida, Faculdade de Ciˆencias e Tecnologia, Universidade Nova de Lisboa, Campus de Caparica, 2829-516 Caparica, Portugal 2 Instituto de Nanociencia de Aragon,´ Universidad de Zaragoza, Campus R´ıo Ebro, Edif´ıcio I+D, Mariano Esquillor s/n, 50018 Zaragoza, Spain 3 REQUIMTE, Departamento de Qu´ımica, Faculdade de Ciˆencias e Tecnologia, Universidade Nova de Lisboa, Campus de Caparica, 2829-516 Caparica, Portugal Correspondence should be addressed to Pedro V. Baptista, [email protected] Received 15 June 2011; Accepted 10 July 2011 Academic Editor: Danuta Wrobel Copyright © 2012 Joao˜ Conde et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Light has always fascinated mankind and since the beginning of recorded history it has been both a subject of research and a tool for investigation of other phenomena. Today, with the advent of nanotechnology, the use of light has reached its own dimension where light-matter interactions take place at wavelength and subwavelength scales and where the physical/chemical nature of nanostructures controls the interactions. This is the field of nanophotonics which allows for the exploration and manipulation of light in and around nanostructures, single molecules, and molecular complexes.
    [Show full text]
  • Silicon Nanophotonics: Towards VLSI Photonic Integrated Circuits
    Silicon nanophotonics: towards VLSI photonic integrated circuits G. Roelkens, W. Bogaerts, D. Taillaert, P. Dumon, L. Liu, S. Selvaraja, J. Brouckaert, J. Van Campenhout, K. De Vos, P. Debackere, D. Van Thourhout, R. Baets Ghent University/IMEC – Photonics Research Group, Sint-Pietersnieuwstraat 41, B-9000 Ghent, Belgium www.photonics.intec.ugent.be e-mail: [email protected] Abstract Silicon photonics is emerging as a disruptive technology for passive integrated optical functions and for active optical functions like (electronically controlled) light modulation and switching. In this presentation we will review the work carried out in the Photonics Research Group in the field of silicon photonics. This includes the fabrication of photonic integrated circuits using CMOS deep UV lithography, examples of integrated silicon components for wavelength selective optical functions for use in optical communication and optical sensing, and examples of coupling structures for interfacing the nanophotonic integrated circuits with an optical fiber. 1. Introduction Fabrication techniques with the aim of integrating a set of optical functions on a single optical chip have advanced to the stage of being technically feasible, a discipline which is referred to as integrated photonics. This is comparable to what has been happening in electronics over the last decades, where the number of transistors on state-of- the-art processors doubles approximately every two years. The research in the field of integrated photonics is driven by the advantages seen in integrating electronic functions on electronic integrated circuits, which are ubiquitously used today. Analogous to electronic integrated circuits, integrating photonic functions on a single chip allows realizing cheaper and more compact optical systems with lower power consumption.
    [Show full text]