Politecnico Di Bari

Total Page:16

File Type:pdf, Size:1020Kb

Politecnico Di Bari POLITECNICO DI BARI RESEARCH DOCTORATE IN INFORMATION ENGINEERING XXV CYCLE 2010-2012 SSD: ING-INF/01 DOCTORAL THESIS OPTICAL BIOCHEMICAL PLATFORMS FOR NANOPARTICLES DETECTION Supervisor: Prof. C. CIMINELLI Coordinator of the Ph.D. Course: Prof. B. TURCHIANO Ph.D. Candidate: Clarissa M. CAMPANELLA Per aspera sic itur ad astra. Thanks to all the minds and hearts I met in the past three years And to those pure souls I’ll never forget. LIST OF ABBREVIATIONS: CW Clockwise CCW Counter-Clockwise CMT Coupled Mode Theory ER Extinction Ratio FDTD Finite Difference Time Domain FWHM Full Width at Half Maximum IO Integrated Optics LOD Limit Of Detection NA Numerical Aperture NAIL Numerical Aperture Increasing Lens NP Nanoparticle Q Quality Factor RI Refractive Index RIU Refractive Index Unit SIL Solid Immersion Lens SPR Surface Plasmon Resonance WGM Whispering Gallery Mode TABLE OF CONTENTS Chapter 1 INTRODUCTION ............................................................................................... - 1 - 1.1 DISSERTATION OVERVIEW ................................................................ - 5 - 1.2 REFERENCES .......................................................................................... - 7 - Chapter 2 BIOCHEMICAL SENSORS ................................................................................ - 9 - 2.1 DEFINITION ............................................................................................ - 9 - 2.2 BIO-SENSORS PROPERTIES ............................................................... - 11 - 2.3 SENSITIVE LAYER .............................................................................. - 12 - 2.3.1 RECEPTORS IMMOBILIZATION ON THE SUBSTRATE ......... - 14 - 2.3.2 MOLECULAR RECOGNITION ELEMENTS ............................... - 16 - 2.4 SENSING MECHANISMS AND TRANSDUCING METHODS: OPTICAL DEVICES .................................................................................... - 18 - 2.4.1 ELECTRONIC ABSORPTION SPECTROSCOPY ........................ - 20 - 2.4.2 ELECTRONIC LUMINESCENCE SPECTROSCOPY .................. - 22 - 2.4.3 VIBRATIONAL SPECTROSCOPY ................................................ - 22 - 2.4.4 REFRACTIVE INDEX CHANGE ................................................... - 22 - 2.6 GEOMETRIES OF INTEGRATED OPTICS BIOSENSORS ............... - 25 - 2.6.1 PLANAR WAVEGUIDES ............................................................... - 25 - 2.6.2 PHOTONIC CRYSTAL DEVICES ................................................. - 30 - 2.6.3 FIBER OPTIC BIOSENSORS ......................................................... - 30 - 2.6.4 OPTICAL RESONATORS .............................................................. - 31 - 2.7 CONCLUSIONS ..................................................................................... - 34 - 2.8 REFERENCES ........................................................................................ - 35 - Chapter 3 WHISPERING GALLERY MODE BASED BIO-CHEMICAL SENSORS ......... - 37 - 3.1 OPTICAL RING RESONATOR CONFIGURATIONS AND PERFORMANCES OVERVIEW ................................................................. - 39 - 3.1.1 PLANAR RING RESONATORS .................................................... - 39 - 3.1.2 OPTO-FLUIDIC RING RESONATORS ......................................... - 42 - 3.1.3 MICROSPHERE RING RESONATORS ........................................ - 45 - 3.2 CAVITY DESIGN: DISCUSSION ......................................................... - 51 - 3.2.1 GUIDING STRUCTURE ................................................................. - 51 - 3.2.2 COUPLER SECTION ...................................................................... - 53 - 3.2.2.1.1 RESONATOR-WAVEGUIDE COUPLING ..................... - 59 - 3.2.2.1.2 INTERNAL MODAL COUPLING ................................... - 61 - 3.2.3 LOSS SOURCES .............................................................................. - 65 - 3.2.3.1 INTERNAL LOSS .................................................................... - 65 - 3.2.3.2 BENDING OR RADIATION LOSS ........................................ - 66 - 3.2.3.3 MODAL MISMATCH LOSS ................................................... - 67 - 3.2.4 NOISE SOURCES ............................................................................ - 67 - 3.3 CONCLUSIONS ..................................................................................... - 68 - 3.4 REFERENCES ........................................................................................ - 69 - Chapter 4 NANOPARTICLES DETECTION ..................................................................... - 77 - 4.1 MECHANICAL DETECTION ............................................................... - 79 - 4.2 ELECTRICAL DETECTION ................................................................. - 80 - 4.3 OPTICAL DETECTION ......................................................................... - 81 - 4.3.1 WGM BASED NP DETECTION .................................................... - 81 - 4.3.2 MICROSCOPY BASED NP DETECTION ..................................... - 84 - 4.4 CONCLUSIONS ..................................................................................... - 89 - 4.5 REFERENCES ........................................................................................ - 90 - Chapter 5 WISPERING GALLERY MODEs BASED SINGLE NANOPARTICLE DETECTION ..................................................................................................... - 95 - 5.1 THE HARMONIC OSCILLATOR ......................................................... - 96 - 5.2 NANOPARTICLE SIZING: MATHEMATICAL MODEL .................. - 98 - 5.2.1 DETECTION LIMIT ENHANCEMENT ...................................... - 109 - 5.3 CAVITY DESIGN: HYBRID RING RESONATOR ........................... - 116 - 5.3.1 SINGLE NANOPARTICLE DETECTION AND SIZING ........... - 127 - 5.4 DISCUSSION ....................................................................................... - 134 - 5.4.1 HYBRID RING RESONATORS ADVANTAGES ....................... - 136 - 5.4.2 BIOLOGICAL SENSING: GLUCOSE CONCENTRATION ...... - 138 - 5.4.3 CHALLENGES: ON CHIP PLATFORM ...................................... - 142 - 5.5 CONCLUSIONS ................................................................................... - 144 - 5.6 REFERENCES ...................................................................................... - 145 - Chapter 6 INTERFEROMETRIC REFLECTANCE IMAGING SENSOR BASED NANOPARTICLE DETECTION ..................................................................... - 149 - 6.1 BASICS OF INTERFEROMETRIC MICROSCOPY FOR NANOPARTICLE DETECTION ............................................................... - 150 - 6.2 ANGULAR SPECTRUM REPRESENTATION ................................. - 154 - 6.3 ANGULAR SPECTRUM REPRESENTATION OF A FAR FIELD .. - 156 - 6.4 FIELD FOCUSED BY AN APLANATIC LENS ................................ - 158 - 6.5 FIELD FOCUSED NEAR A PLANAR INTERFACE ......................... - 161 - 6.6 FIELD IN THE IMAGE SPACE .......................................................... - 166 - 6.7 BACK-SIDE ILLUMINATION MODELING ..................................... - 170 - 6.7.1 DIPOLE EXCITATION FIELD ..................................................... - 172 - 6.7.2 DIPOLE SCATTERED FIELD ...................................................... - 173 - 6.7.3 DIPOLE FIELD IN THE IMAGE SPACE .................................... - 174 - 6.7.4 TOTAL FIELD IN THE IMAGE SPACE ..................................... - 175 - 6.8 RESULTS .............................................................................................. - 175 - 6.8.1 DIELECTRIC NPs ......................................................................... - 176 - 6.9 CONCLUSIONS ................................................................................... - 184 - 6.10 REFERENCES .................................................................................... - 185 - Chapter 7 CONCLUSION ................................................................................................ - 187 - 7.1 REFERENCES ...................................................................................... - 190 - APPENDIX 1: RING RESONATORS THEORY .................................................. 191 APPENDIX 2: MICROSCOPY THEORY ............................................................ 198 List of publications Chapter 1. INTRODUCTION Preserving, monitoring, or anyway dealing with the human and environmental health state should be one of the major goals to be pursued in a world always more dominated by a strong correlation between industrial processes and technological advances. Due to their enormous potential, biosensors are widely used for detecting a wide range of analytes in the health care and food industries and in the environmental monitoring. Mainly, the widespread employment of these devices is attributed to the enormous demands of diseases diagnosis and control, as well as to the property of biosensors of offering a convenient, hygienic, rapid, and compact method for personal monitoring [1]. In recent years, indeed, the sensors market has been dominated by an increasing demand in the field of medical diagnostics relying on the individuation of disposable, reliable, user-friendly, cost-efficient devices that also demonstrate fast response times and that are suitable for mass production. All these criteria are potentially fulfilled by biosensor technologies that combine interdisciplinary approaches coming from nanotechnology,
Recommended publications
  • Crystalline Whispering Gallery Mode Resonators in Optics and Photonics
    3 Crystalline Whispering Gallery Mode Resonators in Optics and Photonics Lute Maleki, Vladimir S. Ilchenko, Anatoliy A. Savchenkov, and Andrey B. Matsko OEwaves Inc. Contents 3.1 Introduction ........................................................................................................................134 3.2 Fabrication Technique ....................................................................................................... 135 3.3 Coupling Techniques ......................................................................................................... 137 3.3.1 Critical Coupling .................................................................................................... 137 3.3.2 Prism ........................................................................................................................ 139 3.3.3 Angle-Cut Fiber ...................................................................................................... 142 3.3.4 Fiber Taper .............................................................................................................. 142 3.3.5 Planar Coupling ..................................................................................................... 143 3.4 Modal Structure and Spectrum Engineering ................................................................ 144 3.4.1 The Spectrum and the Shape of the Resonator ................................................. 145 3.4.2 White Light Resonators ........................................................................................
    [Show full text]
  • A Short Review of Plasmonic Graphene-Based Resonators: Recent Advances and Prospects
    A Short Review of Plasmonic Graphene-Based Resonators: Recent Advances and Prospects Mohammad Bagher Heydari 1,*, Mohammad Hashem Vadjed Samiei 1 1 School of Electrical Engineering, Iran University of Science and Technology (IUST), Tehran, Iran *Corresponding author: [email protected] Abstract: This article aims to study graphene-based resonators published in the literature. Graphene resonators are designed based on graphene conductivity, a variable parameter that can be changed by either electrostatic or magnetostatic gating. A historical review of plasmonic graphene resonators is presented in this paper, which can give physical insight to the researchers to be familiarized with four types of graphene-based resonators: 1-Ring resonators, 2- planar, 3- Fabry-Perot, and 4-other resonators which are not categorized in any of the other three groups. Key-words: Graphene, Plasmonic, Ring resonator, Planar resonator, Fabry-Perot resonator 1. Introduction In recent years, plasmonics is a new emerging science, which exhibits novel features in the THz region [1, 2]. Both metals and two-dimensional (2D) materials can support surface plasmon polaritons (SPPs). In metals, SPPs often are excited in the visible and near-infrared regions [3, 4]. Graphene is a 2D sheet that offers fascinating properties. One of these properties is optical conductivity, which can be tuned by either electrostatic or magnetostatic gating or via chemical doping. This fascinating feature makes graphene a good candidate for designing innovative THz components such as waveguides [5-11], filters [12], couplers [13], Radar Cross-Section (RCS) reduction-based devices [14-16], and graphene-based medical components [17-23]. Moreover, the hybridization of graphene with anisotropic materials such as ferrites, which have many features [24, 25], can enhance the performance of the graphene-based devices [6].
    [Show full text]
  • Whispering Gallery Mode Microresonators: Fundamentals and Applications
    RIVISTA DEL NUOVO CIMENTO Vol. 34, N. 7 2011 DOI 10.1393/ncr/i2011-10067-2 Whispering gallery mode microresonators: Fundamentals and applications G. C. Righini(1),Y.Dumeige(2),P.Feron´ (2), M. Ferrari(3), G. Nunzi Conti(1), D. Ristic(3)andS. Soria(1) (1) CNR, Istituto di Fisica Applicata “Nello Carrara”, MDF Lab 50019, Sesto Fiorentino, Italy (2) UMR Foton, ENSSAT - 22305 Lannion, France (3) CNR, Istituto di Fotonica e Nanotecnologie - 38123 Trento, Italy (ricevuto il 30 Marzo 2011) Summary. — Confinement of light into small volumes has become an essential requirement for photonic devices; examples of this trend are provided by optical fibers, integrated optical circuits, semiconductor lasers, and photonic crystals. Op- tical dielectric resonators supporting Whispering Gallery Modes (WGMs) represent another class of cavity devices with exceptional properties, like extremely small mode volume, very high power density, and very narrow spectral linewidth. WGMs are now known since more than 100 years, after the papers published by John William Strutt (Lord Rayleigh), but their importance as unique tools to study nonlinear optical phenomena or quantum electrodynamics, and for application to very low- threshold microlasers as well as very sensitive microsensors, has been recognized only in recent years. This paper presents a review of the field of WGM resonators, which exist in several geometrical structures like cylindrical optical fibers, microspheres, microfiber coils, microdisks, microtoroids, photonic crystal cavities, etc. up to the most exotic structures, such as bottle and bubble microresonators. For the sake of simplicity, the fundaments of WGM propagation and most of the applications will be described only with reference to the most common structure, i.e.
    [Show full text]
  • Label-Free Detection with High-Q Microcavities: a Review of Biosensing Mechanisms for Integrated Devices
    Nanophotonics 1 (2012): 267–291 © 2012 Science Wise Publishing & De Gruyter • Berlin • Boston. DOI 10.1515/nanoph-2012-0021 Review Label-free detection with high-Q microcavities: a review of biosensing mechanisms for integrated devices Frank Vollmer1,* and Lan Yang2 selective detection of biomolecular markers – even against the 1Max Planck Institute for the Science of Light, Laboratory of background of a multitude of other molecular species. Here, it Nanophotonics and Biosensing, G.Scharowsky Str. 1, 91058 is essential to achieve single molecule detection capabi lity in Erlangen, Germany, e-mail: [email protected] an aqueous environment since clinical samples are water based 2Electrical and Systems Engineering Department, and rapid detection relies on transduction of single molecular Washington University, St. Louis, MO 63130, USA interaction events. Although there are many approaches to label-free bio- *Corresponding author sensing only few technologies promise single mole cule Edited by Shaya Fainman, UC San Diego, La Jolla, CA, USA detection capability potentially integrated on a chip-scale platform. Figure 1 shows what we identify as the most Abstract prominent approaches: high-Q optical resonators, plasmon resonance sensors, nanomechanical resonators and nano- Optical microcavities that confi ne light in high-Q resonance wire sensors. In this review we will focus on high-Q optical promise all of the capabilities required for a successful next- resonator-based biosensors and discuss their various mech- generation microsystem biodetection technology. Label-free anisms for biodetection, possibly down to single molecules. detection down to single molecules as well as operation in Similar to the nanomechanical [6, 7], electrical [8, 9] and aqueous environments can be integrated cost-effectively on plasmonic [1] counterparts shown in Figure 1 and Table 1, microchips, together with other photonic components, as well the sensitivity of optical resonators scales inversely with as electronic ones.
    [Show full text]
  • A Model for an Optical Ring Microresonator Towards Nanoparticle Detection
    A Model for an Optical Ring Microresonator towards Nanoparticle Detection A thesis submitted to the Graduate School of Natural and Applied Sciences by Faruk ahmeti in partial fulfillment for the degree of Master of Science in Electronics and Computer Engineering A Model for an Optical Ring Microresonator towards Nanoparticle Detection Faruk ahmeti Abstract High-Q optical resonators are very prominent bio-sensing technologies that confines light inside a microsize system. Due to their small size and dielectric fabrication materials, these systems can be integrated cost-effectively on integrated chips along with other optical and electrical components. Measurement of the resonance shift proceeded by the transmission spectrum enables observation of binding events in real time, and can also be used to characterize particle size and type. Combination of small size and high Q factor empowers these devices with excellent detection capability. In this thesis, an optical microring resonator has been developed through a multiphysics model using finite element method to solve the relevant equations. All the platform was built in COMSOL Multyphisics software tool. The general framework of this sensor is based on a laser light source, a straight-shape waveguide, a ring-based waveguide, and a photodector at the end of the straight waveguide. A communication laser was used to generate the light at a wavelength of 1.55 µm. In this thesis, it is important to achieve single particle detection inside an aqueous en- vironment since most of the clinical samples are water based. The exact position of the resonance wavelength is located and the transmission spectrum is recorded.
    [Show full text]
  • Optimization of Whispering Gallery Mode Microsphere Resonators and Their Application in Biomolecule Sensing
    Optimization of Whispering Gallery Mode Microsphere Resonators and Their Application in Biomolecule Sensing By Lin Zeng Submitted to the graduate degree program in Chemistry and the Graduate Faculty of the University of Kansas in partial fulfillment of the requirements for the degree of Master of Science. Chairperson: Dr. Robert C. Dunn Dr. Cindy Berrie Dr. Michael Johnson Date Defended: December 15th, 2016 The Thesis Committee for Lin Zeng certifies that this is the approved version of the following thesis: Optimization of Whispering Gallery Mode Microsphere Resonators and Their Application in Biomolecule Sensing Chairperson: Dr. Robert C. Dunn Date approved: December 15th, 2016 ii Abstract Optical Whispering gallery mode (WGM) resonators have attracted attention due to their label-free and sensitive detection capabilities for sensing. Light is confined and continuously recirculated within the cavity via total internal reflection at the resonant wavelength. The long recirculation time significantly enhances the interaction of light with sample, enabling improved sensitivity. Among various WGM resonators with different geometries, microsphere resonators fabricated with heating via surface tension can achieve ultrahigh quality factors and small mode volumes, making them good candidates for WGM sensing applications. The sensing performance of a microsphere resonator is greatly related to its size. Therefore, the fabrication method is optimized to form silica microspheres with smooth surfaces and different sizes (15휇푚~165휇푚 in diameter). The size effects on their sensitivities and quality factors are studied. Silica microspheres with optimal sizes (~45휇푚 in diameter), which achieve high sensitivities and large quality factors, are selected for sensing applications. In addition, the thermal effect on WGM resonators is also explored for silica microspheres and barium titanate microspheres.
    [Show full text]
  • Optical Biosensors Based on Silicon-On-Insulator Ring Resonators: a Review
    molecules Review Optical Biosensors Based on Silicon-On-Insulator Ring Resonators: A Review Patrick Steglich 1,2,* , Marcel Hülsemann 3, Birgit Dietzel 2 and Andreas Mai 1,2 1 IHP—Leibniz-Institut für Innovative Mikroelektronik, Im Technologiepark 25, 15236 Frankfurt (Oder), Germany; [email protected] 2 Technische Hochschule Wildau, Hochschulring 1, 15745 Wildau, Germany; [email protected] 3 First Sensor AG, Peter-Behrens-Straße 15, 12459 Berlin, Germany; marcel.huelsemann@first-sensor.com * Correspondence: [email protected] Academic Editors: Giorgia Oliviero and Nicola Borbone Received: 31 December 2018; Accepted: 25 January 2019; Published: 31 January 2019 Abstract: Recent developments in optical biosensors based on integrated photonic devices are reviewed with a special emphasis on silicon-on-insulator ring resonators. The review is mainly devoted to the following aspects: (1) Principles of sensing mechanism, (2) sensor design, (3) biofunctionalization procedures for specific molecule detection and (4) system integration and measurement set-ups. The inherent challenges of implementing photonics-based biosensors to meet specific requirements of applications in medicine, food analysis, and environmental monitoring are discussed. Keywords: biosensors; biophotonics; integrated optical sensors; aptamers; biomaterials; optical sensor; silicon photonics; ring resonators; lab-on-a-chip 1. Introduction Silicon-based photonic biosensors integrated into a semiconductor chip technology can lead to major advances in point-of-care applications, food diagnostics, and environmental monitoring through the rapid and precise analysis of various substances. In recent years, there has been an increasing interest in sensors based on photonic integrated circuits (PIC) because they give rise to cost effective, scalable and reliable on-chip biosensors for a broad market [1,2].
    [Show full text]
  • Silicon Nitride in Silicon Photonics
    Silicon Nitride in Silicon Photonics By DANIEL J. BLUMENTHAL , Fellow IEEE,RENÉ HEIDEMAN,DOUWE GEUZEBROEK,ARNE LEINSE, AND CHRIS ROELOFFZEN | ABSTRACT The silicon nitride (Si3N4) planar waveguide plat- history of low-loss Si3N4 waveguide technology and a survey of form has enabled a broad class of low-loss planar-integrated worldwide research in a variety of device and applications as devices and chip-scale solutions that benefit from trans- well as the status of Si3N4 foundries. parency over a wide wavelength range (400–2350 nm) and KEYWORDS | Biophotonics; lasers; microwave photonics; fabrication using wafer-scale processes. As a complimentary optical device fabrication; optical fiber devices; optical fil- platform to silicon-on-insulator (SOI) and III–V photonics, Si N 3 4 ters; optical resonators; optical sensors; optical waveguides; waveguide technology opens up a new generation of system- photonic-integrated circuits; quantum entanglement; silicon on-chip applications not achievable with the other platforms nitride; silicon photonics; spectroscopy alone. The availability of low-loss waveguides (<1dB/m)that can handle high optical power can be engineered for linear and nonlinear optical functions, and that support a variety of pas- I. INTRODUCTION sive and active building blocks opens new avenues for system- Photonic-integrated circuits (PICs) are poised to enable an on-chip implementations. As signal bandwidth and data rates increasing number of applications including data commu- continue to increase, the optical circuit functions and com- nications and telecommunications [1], [2], biosensing [3], plexity made possible with Si3N4 has expanded the practical positioning and navigation [4], low noise microwave application of optical signal processing functions that can synthesizers [5], spectroscopy [6], radio-frequency (RF) reduce energy consumption, size and cost over today’s digital signal processing [7], quantum communication [8], and electronic solutions.
    [Show full text]
  • Sensing Nitrous Oxide with QCL-Coupled Silicon-On-Sapphire Ring Resonators
    Sensing nitrous oxide with QCL-coupled silicon-on-sapphire ring resonators Clinton J. Smith,1;∗ Raji Shankar,2 Matthew Laderer,1 Michael B. Frish,1 Marko Loncar,˘ 2 and Mark G. Allen1 1Physical Sciences, Inc., 20 New England Business Center, Andover, MA 01810, USA 2School of Engineering and Applied Sciences, Harvard University, Cambridge, MA 02138, USA ∗[email protected] Abstract: We report the initial evaluation of a mid-infrared QCL-coupled silicon-on-sapphire ring resonator gas sensor. The device probes the N2O −1 2241.79 cm optical transition (R23 line) in the n3 vibrational band. N2O concentration is deduced using a non-linear least squares fit, based on coupled-mode theory, of the change in ring resonator Q due to gas absorption losses in the evanescent portion of the waveguide optical mode. These early experiments demonstrated response to 5000 ppmv N2O. © 2015 Optical Society of America OCIS codes: (130.6010) Integrated Optics: Sensors; (300.1020) Spectroscopy: Absorption; (300.6340) Spectroscopy, infrared; (300.6360) Spectroscopy, laser. References and links 1. M. Frish, R. Shankar, I. Bulu, I. W. Frank, M. C. Laderer, R. T. Wainner, M. G. Allen, and M. Loncar,ˇ “Progress Toward Mid-IR Chip-Scale Integrated-Optic TDLAS Gas Sensors,” Proc. SPIE 9101, 8631–8639 (2014). 2. X. Fan, I. M. White, S. I. Shopova, H. Zhu, J. D. Suter, and Y. Sun, “Sensitive optical biosensors for unlabeled targets: A review,” Anal. Chim. Acta 620, 8–26 (2008). 3. Y. Sun and X. Fan, “Optical ring resonators for biochemical and chemical sensing.” Anal. Bioanal. Chem. 399, 205–211 (2011).
    [Show full text]
  • Silicon Photonic Resonator Sensors and Devices
    Invited Paper Silicon photonic resonator sensors and devices Lukas Chrostowskia, Samantha Grista, Jonas Flueckigera, Wei Shia, Xu Wanga, Eric Ouelletb, Han Yuna, Mitch Webba, Ben Niea, Zhen Lianga, Karen C. Cheunga, Shon A. Schmidtc, Daniel M. Ratnerc, and Nicolas A. F. Jaegera aDepartment of Electrical and Computer Engineering, and bDepartment of Chemical and Biological Engineering, University of British Columbia, Vancouver, British Columbia, Canada cDepartment of Bioengineering, University of Washington, Seattle, Washington, USA ABSTRACT Silicon photonic resonators, implemented using silicon-on-insulator substrates, are promising for numerous applications. The most commonly studied resonators are ring/racetrack resonators. We have fabricated these and other resonators in- cluding disk resonators, waveguide-grating resonators, ring resonator reflectors, contra-directional grating-coupler ring resonators, and racetrack-based multiplexer/demultiplexers. While numerous resonators have been demonstrated for sensing purposes, it remains unclear as to which structures provide the highest sensitivity and best limit of detection; for example, disc resonators and slot-waveguide-based ring resonators have been conjectured to provide an improved limit of detection. Here, we compare various resonators in terms of sensor metrics for label-free bio-sensing in a micro-fluidic environment. We have integrated resonator arrays with PDMS micro-fluidics for real-time detection of biomolecules in experiments such as antigen-antibody binding reaction experiments using Human Factor IX proteins. Numerous resonators are fabricated on the same wafer and experimentally compared. We identify that, while evanescent-field sensors all operate on the principle that the analyte’s refractive index shifts the resonant frequency, there are important differences between implementations that lie in the relationship between the optical field overlap with the analyte and the relative contributions of the various loss mechanisms.
    [Show full text]
  • Whispering Gallery Microsensors: a Review
    Whispering gallery microsensors: a review Xuefeng Jiang, Abraham J. Qavi, Steven H. Huang, and Lan Yang* Department of Electrical and System Engineering, Washington University in St. Louis, St. Louis, Missouri 63130, USA *Corresponding author: [email protected] Abstract: Optical whispering gallery mode (WGM) microresonators, confining resonant photons in a microscale resonator for long periods of time, could strongly enhance light-matter interaction, making it an ideal platform for all kinds of sensors. In this paper, an overview of optical sensors based on WGM microresonators is comprehensively summarized. First, the fundamental sensing mechanisms as well as several recently developed enhanced sensing techniques are introduced. Then, different types of WGM structures for sensing as well as microfluidics techniques are summarized. Furthermore, several important sensing parameters are discussed. Most importantly, a variety of WGM sensing applications are reviewed, including both traditional matter sensing and field sensing. Last, we give a brief summary and perspective of the WGM sensors and their role in future applications. I. Introduction Optical sensors have become one of the elementary building blocks of modern society, in which we rely on them to facilitate our everyday lives by monitoring the intensity, phase, polarization, frequency or speed of the light. A prominent example is fiber optic sensor [1]–[3], which have been well developed to measure strain, temperature, pressure, voltage or other physical quantities in an optical fiber as well as fiber-based devices, and particularly to provide distributed sensing capabilities over a very long distance. For single-pass fiber optic sensors, to improve the sensitivity as well as the detection limit, one typically needs to increase the physical length of the fiber to enhance the interaction between the light and target matter/field.
    [Show full text]
  • On-Chip High-Finesse Fabry-Perot Microcavities for Optical Sensing and Quantum Information
    sensors Review On-Chip High-Finesse Fabry-Perot Microcavities for Optical Sensing and Quantum Information Mohammad H. Bitarafan * and Ray G. DeCorby * ECE department, University of Alberta, 9107-116 St. NW, Edmonton, AB T6G 2V4, Canada * Correspondence: [email protected] (M.H.B.); [email protected] (R.G.D.) Received: 15 June 2017; Accepted: 21 July 2017; Published: 31 July 2017 Abstract: For applications in sensing and cavity-based quantum computing and metrology, open-access Fabry-Perot cavities—with an air or vacuum gap between a pair of high reflectance mirrors—offer important advantages compared to other types of microcavities. For example, they are inherently tunable using MEMS-based actuation strategies, and they enable atomic emitters or target analytes to be located at high field regions of the optical mode. Integration of curved-mirror Fabry-Perot cavities on chips containing electronic, optoelectronic, and optomechanical elements is a topic of emerging importance. Micro-fabrication techniques can be used to create mirrors with small radius-of-curvature, which is a prerequisite for cavities to support stable, small-volume modes. We review recent progress towards chip-based implementation of such cavities, and highlight their potential to address applications in sensing and cavity quantum electrodynamics. Keywords: Fabry-Perot; integrated optics devices; microcavities 1. Introduction In its simplest form, the Fabry-Perot cavity (FPC) confines light between two planar and parallel mirrors. Its historical importance to optics and photonics (and in fact physics) is difficult to overstate. Owing to its higher resolving power and light throughput compared to diffraction grating instruments [1], the FPC played a central role in early studies of the fine structure of spectral lines [2].
    [Show full text]