The Quest for the Superlens
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Far-Field Optical Imaging of Viruses Using Surface Plasmon Polariton
Magnifying superlens in the visible frequency range. I.I. Smolyaninov, Y.J.Hung , and C.C. Davis Department of Electrical and Computer Engineering, University of Maryland, College Park, MD 20742, USA Optical microscopy is an invaluable tool for studies of materials and biological entities. With the current progress in nanotechnology and microbiology imaging tools with ever increasing spatial resolution are required. However, the spatial resolution of the conventional microscopy is limited by the diffraction of light waves to a value of the order of 200 nm. Thus, viruses, proteins, DNA molecules and many other samples are impossible to visualize using a regular microscope. The new ways to overcome this limitation may be based on the concept of superlens introduced by J. Pendry [1]. This concept relies on the use of materials which have negative refractive index in the visible frequency range. Even though superlens imaging has been demonstrated in recent experiments [2], this technique is still limited by the fact that magnification of the planar superlens is equal to 1. In this communication we introduce a new design of the magnifying superlens and demonstrate it in the experiment. Our design has some common features with the recently proposed “optical hyperlens” [3], “metamaterial crystal lens” [4], and the plasmon-assisted microscopy technique [5]. The internal structure of the magnifying superlens is shown in Fig.1(a). It consists of the concentric rings of polymethyl methacrylate (PMMA) deposited on the gold film surface. Due to periodicity of the structure in the radial direction surface plasmon polaritons (SPP) [5] are excited on the lens surface when the lens is illuminated from the bottom with an external laser. -
Optical Negative-Index Metamaterials
REVIEW ARTICLE Optical negative-index metamaterials Artifi cially engineered metamaterials are now demonstrating unprecedented electromagnetic properties that cannot be obtained with naturally occurring materials. In particular, they provide a route to creating materials that possess a negative refractive index and offer exciting new prospects for manipulating light. This review describes the recent progress made in creating nanostructured metamaterials with a negative index at optical wavelengths, and discusses some of the devices that could result from these new materials. VLADIMIR M. SHALAEV designed and placed at desired locations to achieve new functionality. One of the most exciting opportunities for metamaterials is the School of Electrical and Computer Engineering and Birck Nanotechnology development of negative-index materials (NIMs). Th ese NIMs bring Center, Purdue University, West Lafayette, Indiana 47907, USA. the concept of refractive index into a new domain of exploration and e-mail: [email protected] thus promise to create entirely new prospects for manipulating light, with revolutionary impacts on present-day optical technologies. Light is the ultimate means of sending information to and from Th e arrival of NIMs provides a rather unique opportunity for the interior structure of materials — it packages data in a signal researchers to reconsider and possibly even revise the interpretation of zero mass and unmatched speed. However, light is, in a sense, of very basic laws. Th e notion of a negative refractive index is one ‘one-handed’ when interacting with atoms of conventional such case. Th is is because the index of refraction enters into the basic materials. Th is is because from the two fi eld components of light formulae for optics. -
Phase Reversal Diffraction in Incoherent Light
Phase Reversal Diffraction in incoherent light Su-Heng Zhang1, Shu Gan1, De-Zhong Cao2, Jun Xiong1, Xiangdong Zhang1 and Kaige Wang1∗ 1.Department of Physics, Applied Optics Beijing Area Major Laboratory, Beijing Normal University, Beijing 100875, China 2.Department of Physics, Yantai University, Yantai 264005, China Abstract Phase reversal occurs in the propagation of an electromagnetic wave in a negatively refracting medium or a phase-conjugate interface. Here we report the experimental observation of phase reversal diffraction without the above devices. Our experimental results and theoretical analysis demonstrate that phase reversal diffraction can be formed through the first-order field correlation of chaotic light. The experimental realization is similar to phase reversal behavior in negatively refracting media. PACS numbers: 42.87.Bg, 42.30.Rx, 42.30.Wb arXiv:0908.1522v1 [quant-ph] 11 Aug 2009 ∗ Corresponding author: [email protected] 1 Diffraction changes the wavefront of a travelling wave. A lens is a key device that can modify the wavefront and perform imaging. The complete recovery of the wavefront is possible if its phase evolves backward in time in which case an object can be imaged to give an exact copy. A phase-conjugate mirror formed by a four-wave mixing process is able to generate the conjugate wave with respect to an incident wave and thus achieve lensless imaging[1]. A slab of negative refractive-index material can play a role similar to a lens in performing imaging[2, 3, 4, 5, 6, 7]. Pendry in a recent paper[8] explored the similarity between a phase-conjugate interface and negative refraction, and pointed out their intimate link to time reversal. -
ARTIFICIAL MATERIALS for NOVEL WAVE PHENOMENA Metamaterials 2019
ROME, 16-21 SEPTEMBER 2019 META MATE RIALS 13TH INTERNATIONAL CONGRESS ON ARTIFICIAL MATERIALS FOR NOVEL WAVE PHENOMENA Metamaterials 2019 Proceedings In this edition, there are no USB sticks for the distribution of the proceedings. The proceedings can be downloaded as part of a zip file using the following link: 02 President Message 03 Preface congress2019.metamorphose-vi.org/proceedings2019 04 Welcome Message To browse the Metamaterials’19 proceedings, please open “Booklet.pdf” that will open the main file of the 06 Program at a Glance proceedings. By clicking the papers titles you will be forwarded to the specified .pdf file of the papers. Please 08 Monday note that, although all the submitted contributions 34 Tuesday are listed in the proceedings, only the ones satisfying requirements in terms of paper template and copyright 58 Wednesday form have a direct link to the corresponding full papers. 82 Thursday 108 Student paper competition 109 European School on Metamaterials Quick download for tablets and other mobile devices (370 MB) 110 Social Events 112 Workshop 114 Organizers 116 Map: Crowne Plaza - St. Peter’s 118 Map to the Metro 16- 21 September 2019 in Rome, Italy 1 President Message Preface It is a great honor and pleasure for me to serve the Virtual On behalf of the Technical Program Committee (TPC), Institute for Artificial Electromagnetic Materials and it is my great pleasure to welcome you to the 2019 edition Metamaterials (METAMORPHOSE VI) as the new President. of the Metamaterials Congress and to outline its technical Our institute spun off several years ago, when I was still a program. -
State-Of-The-Art of Metamaterials: Characterization, Realization and Applications
Technological University Dublin ARROW@TU Dublin Articles Antenna & High Frequency Research Centre 2014-7 State-of-the-Art of Metamaterials: Characterization, Realization and Applications Giuseppe Ruvio Technological University Dublin, [email protected] Giovanni Leone Second University of Naples, [email protected] Follow this and additional works at: https://arrow.tudublin.ie/ahfrcart Part of the Electromagnetics and Photonics Commons Recommended Citation G. Ruvio & G. Leone,(2014) State-of-the-art of Metamaterials: Characterization, Realization and Applications, Studies in Engineering and Technology, vol. 1, issue 2. doi:10.11114/set.v1i2.456 This Article is brought to you for free and open access by the Antenna & High Frequency Research Centre at ARROW@TU Dublin. It has been accepted for inclusion in Articles by an authorized administrator of ARROW@TU Dublin. For more information, please contact [email protected], [email protected]. This work is licensed under a Creative Commons Attribution-Noncommercial-Share Alike 4.0 License Redfame Publish ing State-of-the-art of metamaterials: characterization, realization and applications Giuseppe Ruvio 1, 2 & Giovanni Leone 1 1Seconda Università di Napoli, Dipartimento di Ingegneria Industriale e dell’Informazione, Via Roma 29, 81031 Aversa (CE), Italy 2Dublin Institute of Technology, Antenna & High Frequency Research Centre, Kevin Street, Dublin 8, Ireland Abstract Metamaterials is a large family of microwave structures that produces interesting ε and µ conditions with huge implications for numerous electromagnetic applications. Following a description of modern techniques to realize epsilon-negative, mu-negative and double-negative metamaterials, this paper explores recent literature on the use of metamaterials in hot research areas such as metamaterial-inspired microwave components, antenna applications and imaging. -
Advanced Metamaterials for High Resolution Focusing and Invisibility Cloaks
Doctoral thesis submitted for the degree of Doctor of Philosophy in Telecommunication Engineering Postgraduate programme: Communication Technology Advanced metamaterials for high resolution focusing and invisibility cloaks Presented by: Bakhtiyar Orazbayev Director: Dr. Miguel Beruete Díaz Pamplona, November 2016 Abstract Metamaterials, the descendants of the artificial dielectrics, have unusual electromagnetic parameters and provide more abilities than naturally available dielectrics for the control of light propagation. Being able to control both permittivity and permeability, metamaterials have opened a way to obtain a double negative medium. The first experimental realization of such medium gave an enormous impulse for research in the field of electromagnetism. As result, many fascinating electromagnetic devices have been developed since then, including metamaterial lenses, beam steerers and even invisibility cloaks. The possible applications of metamaterials are not limited to these devices and can be applied in many fields, such as telecommunications, security systems, biological and chemical sensing, spectroscopy, integrated nano-optics, nanotechnology, medical imaging systems, etc. The aim of this doctoral thesis, performed at the Public University of Navarre in collaboration with the University of Texas at Austin, the Valencia Nanophotonics Technology Center in the UPV and King’s College London, is to contribute to the development of metamaterial based devices, including their fabrication and, when possible, experimental verification. The thesis is not focused on a single application or device, but instead tries to provide an extensive exploration of the different metamaterial devices. These results include the following: Three different lens designs based on a fishnet metamaterial are presented: a broadband zoned fishnet metamaterial lens, a Soret fishnet metamaterial lens and a Wood zone plate fishnet metamaterial. -
Super-Resolution Imaging by Dielectric Superlenses: Tio2 Metamaterial Superlens Versus Batio3 Superlens
hv photonics Article Super-Resolution Imaging by Dielectric Superlenses: TiO2 Metamaterial Superlens versus BaTiO3 Superlens Rakesh Dhama, Bing Yan, Cristiano Palego and Zengbo Wang * School of Computer Science and Electronic Engineering, Bangor University, Bangor LL57 1UT, UK; [email protected] (R.D.); [email protected] (B.Y.); [email protected] (C.P.) * Correspondence: [email protected] Abstract: All-dielectric superlens made from micro and nano particles has emerged as a simple yet effective solution to label-free, super-resolution imaging. High-index BaTiO3 Glass (BTG) mi- crospheres are among the most widely used dielectric superlenses today but could potentially be replaced by a new class of TiO2 metamaterial (meta-TiO2) superlens made of TiO2 nanoparticles. In this work, we designed and fabricated TiO2 metamaterial superlens in full-sphere shape for the first time, which resembles BTG microsphere in terms of the physical shape, size, and effective refractive index. Super-resolution imaging performances were compared using the same sample, lighting, and imaging settings. The results show that TiO2 meta-superlens performs consistently better over BTG superlens in terms of imaging contrast, clarity, field of view, and resolution, which was further supported by theoretical simulation. This opens new possibilities in developing more powerful, robust, and reliable super-resolution lens and imaging systems. Keywords: super-resolution imaging; dielectric superlens; label-free imaging; titanium dioxide Citation: Dhama, R.; Yan, B.; Palego, 1. Introduction C.; Wang, Z. Super-Resolution The optical microscope is the most common imaging tool known for its simple de- Imaging by Dielectric Superlenses: sign, low cost, and great flexibility. -
All-Angle Negative Refraction Without Negative Effective Index
RAPID COMMUNICATIONS PHYSICAL REVIEW B, VOLUME 65, 201104͑R͒ All-angle negative refraction without negative effective index Chiyan Luo, Steven G. Johnson, and J. D. Joannopoulos* Department of Physics and Center for Materials Science and Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 J. B. Pendry Condensed Matter Theory Group, The Blackett Laboratory, Imperial College, London SW7 2BZ, United Kingdom ͑Received 22 January 2002; published 13 May 2002͒ We describe an all-angle negative refraction effect that does not employ a negative effective index of refraction and involves photonic crystals. A few simple criteria sufficient to achieve this behavior are presented. To illustrate this phenomenon, a microsuperlens is designed and numerically demonstrated. DOI: 10.1103/PhysRevB.65.201104 PACS number͑s͒: 78.20.Ci, 42.70.Qs, 42.30.Wb Negative refraction of electromagnetic waves in ‘‘left- We observe from Fig. 1 that due to the negative-definite ץ ץ 2ץ handed materials’’ has become of interest recently because it photonic effective mass / ki k j at the M point, the fre- is the foundation for a variety of novel phenomena.1–6 In quency contours are convex in the vicinity of M and have particular, it has been suggested that negative refraction leads inward-pointing group velocities. For frequencies that corre- to a superlensing effect that can potentially overcome the spond to all-convex contours, negative refraction occurs as diffraction limit inherent in conventional lenses.2 These phe- illustrated in Fig. 2. The distinct refracted propagating modes nomena have been described in the context of an effective- are determined by the conservation of the frequency and the medium theory with negative index of refraction, and at the wave-vector component parallel to the air/photonic-crystal moment only appear possible in the microwave regime. -
Physics and Applications of Negatively Refracting Electromagnetic Materials Steven M
Physics and Applications of Negatively Refracting Electromagnetic Materials Steven M. Anlage, Michael Ricci, Nathan Orloff Work Funded by NSF/ECS-0322844 1 Outline What are Negative Index of Refraction Metamaterials? What novel properties do they have? How are they made? What new RF/microwave applications are emerging? Superconducting Metamaterials Caveats / Prospects for the future 2 Why Negative Refraction? n > 0 n >< 0 1 2 r r Hr refractedH H ray normalθ r Snell’s Law 2 k normalθ θ1 r 2 refracted r n1 sin(θ1) = n2 sin(θ2) k ray k incident r r r ray E EE PositiveNegative Index Index of of Refraction Refraction (PIR) (NIR) = =Right Left Handed Medium (RHM)(LHM) n1>0 n2<0>0 n n11>0>0 Two images! NIRPIR // RHMLHM source No real image Flat“Lens” Lens 3 How can we make refractive index n < 0? ”Use “Metamaterials ng materials withArtificially prepared dielectric and conducti negative values of both ε and μ r r r r DE= ε BH= μ ÎonNegative index of refracti! Many optical properties are reversed! Propagating Waves μ RHM Vac RHM Vac LHM n=εμ >0 ε n=εμ <0 Ordinary Negative Propagating Waves!Non-propagating Waves Refraction Refraction LHM 4 Negative Refraction: Consequences Left-Handed or Negative Index of Refraction Metamaterials ε < 0 AND μ < 0 Veselago, 1967 Propagating waves have index of refraction n < 0 ⇒ Phase velocity is opposite to Poynting vector direction Negative refraction in Snell’s Law: n1 sinθ1 = n2 sinθ2 Flat lens with no optical axis Converging Lens → Diverging Lens “Perfect” Lens (Pendry, 2000) and vice-versa Reverse Doppler Effect Reversed Čerenkov Effect Radiation Tension RHM LHM RHM Flat Lens Imaging Point source “perfect image” V. -
Crphysique-Meta-Preface-Gralak
Foreword Boris Gralak, Sebastien Guenneau To cite this version: Boris Gralak, Sebastien Guenneau. Foreword. Comptes Rendus Physique, Centre Mersenne, 2020, 21 (4-5), pp.311-341. 10.5802/crphys.36. hal-03087380 HAL Id: hal-03087380 https://hal.archives-ouvertes.fr/hal-03087380 Submitted on 23 Dec 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Foreword Boris Gralak and Sébastien Guenneau a CNRS, Aix Marseille Univ, CentraleMarseille, Institut Fresnel,Marseille, France b UMI 2004 Abraham deMoivre-CNRS, Imperial College London, London SW7 2AZ,UK E-mails: [email protected] (B. Gralak), [email protected] (S. Guenneau) Manuscript received 14th October 2020, accepted 22nd October 2020. Metamaterial is a word that seems both familiar and mysterious to the layman: on the one hand, this research area born twenty years ago at the interface between physical and engineering sciences requires a high level of expertise to be investigated with advanced theoretical and experimental methods; and on the other hand electromagnetic paradigms such as negative refraction, super lenses and invisibility cloaks have attracted attention of mass media. Even the origin and meaning of the word metamaterial (formed of the Greek prefix μετά meaning beyond or self and the Latin suffix materia, meaning material) remains elusive. -
EEE17 Negative Refraction in Metamaterials
EEE 17 Negative Refraction in Metamaterials EEE17 Negative Refraction in Metamaterials Cheng Zixiang Raffles Institution Lian Kay Sean Temasek JC NRP Supervisor: Prof. Luo Yu NTU EEE 17 Negative Refraction in Metamaterials Research Plan Artificially engineered metamaterials have unique properties that cannot be obtained with natural materials. Negative Index Metamaterials or NIMs, as they are commonly known, have a negative refractive index, thus light rays are refracted on the same side of the normal on entering the material. Our project focuses on two ways of achieving NIMs. One would be constructing dielectric metamaterials created with a periodic array of subwavelength unit cells, the other would be creating a hyperbolic metamaterial by alternating layers of mediums of different refractive index. The aim of our project is to investigate the materials that can be used to construct the hyperbolic and dielectric method of realising negative refraction and the efficacy of the material used. Both approaches achieved negative refraction in the mid infra-red frequency. The simulation would be done with COMSOL software. EEE 17 Negative Refraction in Metamaterials Abstract A metamaterial is a material engineered to have a property not found in nature. Metamaterials usually gain their properties from structure rather than composition, offering a great freedom in material design. Recently, well designed metamaterials have received much interest because their atypical interaction with electromagnetic waves that can be used for subwavelength imaging and designing cloaking devices. In my project, that property is to be able to realise negative refraction in certain frequencies of the electromagnetic spectrum. The metamaterial concept was proposed in 1999 by John Pendry, who detailed in a paper in 2000 applying the concept of negative refraction to create a lens that can focus light onto a sub-wavelength area. -
Negative Refraction at Deep-Ultraviolet Frequency in Monocrystalline Graphite
Negative refraction at deep-ultraviolet frequency in monocrystalline graphite Jingbo Sun, Ji Zhou*, Lei Kang, Rui Wang, Xianguo Meng, Bo Li, Feiyu Kang and Longtu Li State Kay Lab of New Ceramics and Fine Processing, Department of Materials Science and Engineering, Tsinghua University, Beijing 100084, China Abstract: Negative refraction is such a prominent electromagnetic phenomenon that most researchers believe it can only occur in artificially engineered metamaterials. In this article, we report negative refraction for all incident angles for the first time in a naturally existing material. Using ellipsometry measurement of the equifrequency contour in the deep-ultraviolet frequency region (typically 254 nm), obvious negative refraction was demonstrated in monocrystalline graphite for incident angles ranging from 20o to 70o. This negative refraction is attributed to extremely strong anisotropy in the crystal structure of graphite, which gives the crystal indefinite permeability. This result not only explores a new route to identifying natural negative-index materials, but it also holds promise for the development of an ultraviolet hyperlens, which may lead to a breakthrough in nanolithography, the most critical technology necessary for the next generation of electronics. Since the concept of negative-index materials (NIMs) was first proposed by Veselago1, it has been realised by various mechanisms such as left-handed materials2-4, photonic crystals5, 6, and artificially indefinite media7, 8. A well-established route for constructing NIM structures is based on Veselago’s theory of left-handed materials (LHM), simultaneous negative permittivity (ε), and magnetic permeability (μ) with different types of metamaterials9−12. Recent experimental13 and theoretical14 results have also shown negative refraction phenomena in photonic crystals in regimes of negative group velocity and negative effective index above the first band near the Brillouin zone centre (Γ), without the requirement of an overlap in negative permittivity and permeability.