Investigation and analysis of leaf reflective structures in the field of plasmonics for the application of passive components

Number of pages: 180 File Format: word File Code: 32186
Year: 2013 University Degree: Master's degree Category: Electrical Engineering
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  • Summary of Investigation and analysis of leaf reflective structures in the field of plasmonics for the application of passive components

    Master thesis in the field of electrical engineering - field telecommunications

    Abstract

    Investigation and analysis of leaf reflector structures in the field of plasmonics for the use of passive components

    by effort

    Omidreza Daneshmandi

     

    In optical integrated circuit design, the diffraction limit limits the miniaturization of optical elements. Surface plasmon polaritons that propagate at the interface of metal and dielectric overcome this limitation. One of the subjects that is studied in this thesis is the laboratory investigation of dielectric-metal-dielectric plasmonic plate and channel waveguides with polymer-silver-prism structure. The plasmonic wave was excited by the well-known coupling method by a prism. A simple laboratory method was also introduced to measure the propagation length of the plasmonic wave. An interesting phenomenon that was observed in the experiments was the scattering effects of surface plasmonic waves at the end of the silver strip, which creates a discontinuity. This phenomenon can be used for coupling between conventional 3D waveguides and plasmonic waveguides. Currently, this topic is under investigation for the design of hybrid plasmonic couplers. In addition, in this thesis, alternating leaf structures that are used as reflectors and filters in optical circuits are studied. Plasmonic hybrid structures were used to design and simulate leaf reflectors. Plasmonic hybrid reflectors based on sinusoidal and toothed gratings were investigated and compared with the previously introduced rectangular grating. It is shown that the sawtooth grating shows better characteristics compared to the three gratings, and this grating has less passband distortion and a narrower cutoff bandwidth compared to rectangular and sinusoidal gratings. It is also shown that the sinusoidal grating, which can be easily made with holographic techniques, has less passband distortion and narrower cutoff bandwidth compared to the rectangular grating. In addition, the apodization operation of plasmonic hybrid arrays was investigated and it was found that by using this technique, the distortion in the passband and cutoff bandwidth can be further reduced.

    Keywords: plasmonics, surface plasmon, waveguide, filter, leaf reflector

    1-1 Introduction and importance of the topic

    Optics is one of the branches of science that had made a lot of progress before defining light as photon packets. Defining light in the form of electromagnetic waves with specific wavelengths has greatly contributed to the expansion of this science. Photonics was another name for this science that came with the definition of light particles. In this definition, light was expressed as a package of massless particles with a specific momentum. Therefore, the wave and particle properties of light both led to the development of the science of light or optics. The advancement of technology has widened the use of light in the fields of telecommunications, material identification, biosensors, and circuits with nanometer dimensions.

    Optical integrated circuits are among the discussions that have received much attention from researchers with the advancement of optics. Of course, fundamental limitations were observed in the miniaturization of optical devices. The most important of these limitations stated that light cannot be replaced in space or space in dimensions smaller than wavelength. Scientists have specified a minimum limit for this substitution in their physical tests. This minimum limit was named the diffraction limit [3] to reduce the dimensions of the parts and the accuracy [2] of observing objects.

    Surface plasmons (the theoretical discussions of which are expressed in the following chapters), which are defined by the full name of surface plasmon polaritons [4] (SSP), are surface electromagnetic waves that propagate parallel to the metal-dielectric interface. The full definition of these waves was first introduced in 1957 AD (years mentioned in the text are all in AD) by Mr. Ritcher [5] completely with optical application. In recent decades, these waves have become candidates for reducing the dimensions of optics to two dimensions, so that they have the ability to exceed the diffraction limit (which will be explained later) [1].

    The advantages of manufacturing optical devices with micrometer and nanometer dimensions along with the development of display technologies such as optical near-field display [6] (SNOM) have caused more attention to research in this field of photonics. This field is called nanophotonics and plasmonics because of the nanometer dimensions of its elements. Information transmission in this area is done with much higher frequencies compared to electronics, and much more bandwidth is accessible. Optics requires larger waveguide lines compared to nano dimensions, which is difficult due to the limitation of the diffraction limit of the miniaturization of waveguide parts. In addition, in electronic circuits, there is a delay in the exchange of data between the source and the destination, and the speed of the circuits is greatly reduced. In optical circuits, this speed increases in addition to the capacity of the transmission line.  But still the problem of diffraction limit is the main obstacle in the miniaturization of circuits. Therefore, it can miniaturize optics and its elements with much larger bandwidth and very small waveguides. So it combines all the advantages and properties of electronic and optical circuits. This technology needs further development because it has disadvantages such as the short propagation length of surface plasmon waves. In recent years, many researches have been started to reduce the disadvantages of these waves by using material properties to amplify waves and hybrid structures[7]. Measurements have also become very complicated in plasmonic science. For this reason, part of the research is spent on simplifying the measurements through the inherent characteristics of these waves in observing plasmons and measuring their propagation length. Therefore, in this thesis, after reviewing the history of plasmonic science and the brief definition of surface plasmon polaritons, we will introduce the diffraction limit and break it by plasmonic science. In the second chapter, the theory related to surface plasmons in different structures is expressed. Of course, according to the purpose of this thesis, which was to investigate the construction of IMI filters [8], and due to the time limit until the construction stage of the IMI waveguide for the first time in the country, and the introduction of a new method of measuring the propagation length, progress was achieved. In the third chapter, the experiments performed on the excitation of plasmons and the idea of ??a new method for measuring their propagation length are mentioned. In the fourth chapter, the simulation of hybrid plasmonic leaf filters is explained.

    1-2 History overview

    Electromagnetic surface waves, which are a special type of this thesis, can move along the interface of two dissimilar environments. These waves have been investigated in the last century.

    Zennik[9] encountered the propagation of these waves in 1909 during the discussions of radio communication around the globe when he assumed the upper half of space to be a dielectric and the earth to be a conductor[2]. Such a similar wave can be propagated at the metal-dielectric interface by coupling the electromagnetic beam to the oscillating charge density in metals. Of course, some researchers introduced this mode as a sound wave that propagates in the free electron gas model of the electron sea of ??metals [3].

    Fano[10] recognized in 1941 that the surface waves that propagate at the interface of metal and dielectric are similar to the waves that were introduced years ago by Zennick and later by Summerfield[11] in 1909. Fano's theory was fully proved with laboratory methods in 1967 by Richer and later by Bieglehl[12]. They separately and with coherent experiments expressed the excitation of surface plasmons by electronic and optical methods. Richer was able to obtain surface plasmons with the help of the scattering relation experiment [13]. He had done this for an incident beam with parallel polarization [14] while Bieglehl did it for both parallel and vertical polarization [15] [1].

  • Contents & References of Investigation and analysis of leaf reflective structures in the field of plasmonics for the application of passive components

    List:

    Chapter One: Introduction..2

    1-1 Introduction and importance of the topic.2

    1-2 An overview of history.5

    1-3 Polariton and surface polariton plasmon.7

    1-4 Plasmonics and the uncertainty principle (diffraction limit). 9

    Chapter Two: Theoretical foundations of surface plasmon polariton structures.14

    2-1 Maxwell's equations and electromagnetic wave propagation.14

    2-2 Dielectric function of free electron gas model of metals.19

    2-3 Comparison of dielectric function of real metals with dielectric function of plasma model.23

    2-4          Review of plasmon polaritons surface at the metal-insulator boundary.27

    2-4-1 Wave equation.27

    Title

    Page

           2-5           Relation of surface plasmon scattering of polaritons. 32

    2-6           Spatial expansion of SPPs waves.

    2-6-1          Depth of penetration of plasmons surface. 40

    2-6-2            The propagation length of surface plasmons. 41

    2-7             Investigating the properties of SPPs in multi-layer systems.

    2-8-2 Coupling using grating.58

    2-8-3 Excitation using highly focused beams.61

    2-8-4 Excitation by near field.63

    2-8-5 Proper coupling methods of plasmons for integrated circuits of plasmonic and photonic devices.65

    2-9 Plasmonic hybrid structures. 67 2-9-1 Hybrid plasmonic waveguides: a combination of dielectric and plasmonic waveguides.

    2-9-2-2 Analysis of two-dimensional hybrid plasmonic waveguide. 78

    2-9-2-3 Analysis method and some important definitions. 81

    Title

    Page

    2-9-2-4               Effect of changes of some parameters on the degree of improvement of hybrid plasmonic waveguide. 82

    2-10          Reflector or filter Leaves in plasmonic applications. 86

    2-10-1 Structure of IMI leaf filters. 89

    2-10-2 Structure of MIM leaf filters. 94

    2-10-3 Structure of hybrid plasmonic leaf filters. 97

    Chapter 3: Fabrication of plasmonic waveguides and ideas for measuring the propagation length of plasmons. 107

    3-1 Planar IMI waveguide structure simulation. 101

    3-2 Construction of IMI planar waveguide (air-silver-silica). 106

    3-2-1 Excitation of surface plasmons in planar waveguide. 107

    3-3 Construction of channel waveguide and excitation of surface plasmons in 111

    3-3-1 Construction of surface plasmon channel waveguide (silica-silver-air). 112

    3-3-2 Exciting plasmons on the channel waveguide and observing the coupling angle.

    3-4-1                                                                                                                                                                                                                                                                                                   address). 127

    3-4-4 Discussion and review of data and test results. 130

    3-4-5 138

    4-2 Simulation of plasmonic hybrid leaf reflector with sinusoidal profile. 140

    4-3 Simulation of plasmonic hybrid leaf reflector with serrated profile. 145

    4-4 Simulation of distortion reduction in plasmonic hybrid leaf reflector145

    4-4 nanophotonic devices using the Finite Element Method," University of Nottingham, 2010.

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Investigation and analysis of leaf reflective structures in the field of plasmonics for the application of passive components