Nanophotonics with Surface Plasmons 0444528385
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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]. -
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]. -
Surface Plasmons and Gain Media
Chapter 5 Surface plasmons and gain media by M.A. Noginov, G. Zhu Center for Materials Research, Norfolk State University, Norfolk, VA, 23504 V.P. Drachev, V.M. Shalaev School of Electrical & Computer Engineering and Birck Nanotechnology Center, Purdue University, West Lafayette, IN 47907 Nanophotonics with Surface Plasmons V.M. Shalaev & S. Kawata (Editors) Advances in Nano-Optics and Nano-Photonics r 2007 Published by Elsevier B.V. ISSN: 1871-0018 DOI: 10.1016/S1871-0018(06)02005-X 141 Contents Page y 1. Introduction . ...................................143 y 2. Estimation of the critical gain ........................148 y 3. Experimental samples and setups . ....................149 y 4. Experimental results and discussion....................149 y 5. Summary . ...................................164 Acknowledgments ................................... 165 References . ....................................... 165 142 § 1. Introduction The technique of coloring stain glasses by gold and silver nanoparticles was known to Romans. The British Museum has a famous Lycurgus Cup (4th Century A.D.), which changes its color depending on the illumination (fig. 1). When viewed in reflected light, for example, in daylight, it appears green. However, when a light is shone into the cup and transmitted through the glass, it appears red. Nowadays it is known that the colora- tion of the Cup is determined by the frequency of localized surface plasmon (SP) resonance in metallic nanoparticles embedded into the glass. Localized SP is the oscillation of free electrons in a metallic particle (driven by an external electromagnetic wave), whose resonance frequency is the plasma frequency adjusted by the size and, mainly, the shape of the particle. A phenomenon relevant to localized SPs is a surface plasmon polariton (SPP) or a surface electromagnetic wave propagating along the interface between two media possessing permittivities with opposite signs, such as metal–dielectric interface. -
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. -
Electronic Ferroelectricity in Carbon Based Materials
Electronic ferroelectricity in carbon based materials Natasha Kirova1,3* and Serguei Brazovskii2,3 1LPS, CNRS, Univ Paris-Sud, Université Paris-Saclay, 91405 Orsay Cedex, France 2LPTMS, CNRS, Univ Paris-Sud, Université Paris-Saclay, 91405 Orsay Cedex, France 3Moscow Institute for Steel and Alloys, Leninskii av. 4, 119049 Moscow, Russia. We review existing manifestations and prospects for ferroelectricity in electronically and optically active carbon-based materials. The focus point is the proposal for the electronic ferroelectricity in conjugated polymers from the family of substituted polyacetylenes. The attractive feature of synthetic organic ferroelectrics is a very high polarizability coming from redistribution of the electronic density, rather than from conventional displacements of ions. Next fortunate peculiarity is the symmetry determined predictable design of perspective materials. The macroscopic electric polarization follows ultimately from combination of two types of a microscopic symmetry breaking which are ubiquitous to qusi-1D electronic systems. The state supports anomalous quasi-particles - microscopic solitons, carrying non-integer electric charges, which here play the role of nano-scale nucleus of ferroelectric domain walls. Their spectroscopic features in optics can interfere with low-frequency ferroelectric repolarization providing new accesses and applications. In addition to already existing electronic ferroelectricity in organic crystals and donor-acceptor chains, we point to a class of conducting polymers and may be also to nano-ribbons of the graphene where such a state can be found. These proposals may lead to potential applications in modern intensive searches of carbon ferroelectrics. Keywords: ferroelectricity, organic conductor, conjugated polymers, polyacetylene, graphene, soliton, non- integer charge, domain wall 1. Introduction Ferroelectricity is a phenomenon of spontaneous controllable electric polarizations in some, usually crystalline, solids [1]. -
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. -
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. -
Ferroelectricity and Piezoelectricity Batio3
Ferroelectricity and Piezoelectricity BaTiO3 cubic (contains i = > no spontaneous P) Can be used to make nonvolatile memory BaTiO3 r 1 Can be used to make ultracapacitors Paraelectric state Above Tc, BaTiO3 is paraelectric. The susceptibility (and dielectric constant) diverge like a Curie-Weiss law. 1 1 0 TT c This causes a big peak in the dielectric constant at Tc. Ferroelectric Paraelectric PbTiO3 Dielectric constant 1 TT c Pyroelectric constant Polarization Specific heat Antiferroelectricity PbZrO3 Polarization aligns antiparallel. Associated with a structural phase transition. Large susceptibility and dielectric constant near the transition. Phase transition is observed in the specific heat, x-ray diffraction. Applied field T > Tc T < Tc T < Tc Piezoelectricity Many piezoelectric materials are ferroelectric. Electric field couples to polarization, polarization couples to structure. lead zirconate titanate (Pb[ZrxTi1−x]O3 0<x<1) —more commonly known as PZT barium titanate (BaTiO3) Tc = 408 K lead titanate (PbTiO3) Tc = 765 K potassium niobate (KNbO3) Tc = 708 K lithium niobate (LiNbO3) Tc = 1480 K lithium tantalate (LiTaO3) Tc = 938 K quartz (SiO2), GaAs, GaN Gallium Orthophosphate (GaPO4) Tc = 970 K Third rank tensor, No inversion symmetry Piezoelectric crystal classes: 1, 2, m, 222, mm2, 4, -4, 422, 4mm, -42m, 3, 32, 3m, 6, -6, 622, 6mm, -62m, 23, -43m Piezoelectricity When you apply a voltage across certain crystals, they get longer. AFM's, STM's Quartz crystal oscillators Surface acoustic wave generators Pressure sensors - Epcos Fuel injectors - Bosch Inkjet printers PZT (Pb[ZrxTi1−x]O3 0<x<1) Antiferroelectric Large piezoelectric response near the rhombohedral-tetragonal transition. Electric field induces a structural phase transition. -
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. -
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. -
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. -
Coupled Electricity and Magnetism: Multiferroics and Beyond
Coupled electricity and magnetism: multiferroics and beyond Daniel Khomskii Cologne University, Germany JMMM 306, 1 (2006) Physics (Trends) 2, 20 (2009) Degrees of freedom charge Charge ordering Ferroelectricity Qαβ ρ(r) (monopole) P or D (dipole) (quadrupole) Spin Orbital ordering Magnetic ordering Lattice Maxwell's equations Magnetoelectric effect In Cr2O3 inversion is broken --- it is linear magnetoelectric In Fe2O3 – inversion is not broken, it is not ME (but it has weak ferromagnetism) Magnetoelectric coefficient αij can have both symmetric and antisymmetric parts Pi = αij Hi ; Symmetric: Then along main axes P║H , M║E For antisymmetric tensor αij one can introduce a dual vector T is the toroidal moment (both P and T-odd). Then P ┴ H, M ┴ E, P = [T x H], M = - [T x E] For localized spins For example, toroidal moment exists in magnetic vortex Coupling of electric polarization to magnetism Time reversal symmetry P → +P t → −t M → −M Inversion symmetry E ∝ αHE P → −P r → −r M → +M MULTIFERROICS Materials combining ferroelectricity, (ferro)magnetism and (ferro)elasticity If successful – a lot of possible applications (e.g. electrically controlling magnetic memory, etc) Field active in 60-th – 70-th, mostly in the Soviet Union Revival of the interest starting from ~2000 • Perovskites: either – or; why? • The ways out: Type-I multiferroics: Independent FE and magnetic subsystems 1) “Mixed” systems 2) Lone pairs 3) “Geometric” FE 4) FE due to charge ordering Type-II multiferroics:FE due to magnetic ordering 1) Magnetic spirals (spin-orbit interaction) 2) Exchange striction mechanism 3) Electronic mechanism Two general sets of problems: Phenomenological treatment of coupling of M and P; symmetry requirements, etc.