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Physical & Electromagnetic Optics: Basic Principles & Interference Optical Engineering Prof. Elias N. Glytsis School of Electrical & Computer Engineering National Technical University of Athens 29/05/2017

Physical & Electromagnetic Optics: Basic Principles ...users.ntua.gr/eglytsis/OptEng/Interference_p.pdf · Physical & Electromagnetic Optics: Basic Principles & ... • Interference

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  • Physical & Electromagnetic Optics: Basic Principles &

    Interference

    Optical Engineering Prof. Elias N. Glytsis

    School of Electrical & Computer Engineering National Technical University of Athens

    29/05/2017

  • Prof. Elias N. Glytsis, School of ECE, NTUA 2

    Quantum Optics

    Electromagnetic Optics Wave (Physical) Optics

    Geometrical Optics

    Wave and Electromagnetic Optics

  • Prof. Elias N. Glytsis, School of ECE, NTUA 3

    Electromagnetic Spectrum

    https://en.wikipedia.org/wiki/File:EM_Spectrum_Properties_edit.svg

  • Maxwells Equations Differential Form

    Integral Form

    4 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Boundary Conditions

    S

    Region +

    Region -

    5 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Maxwells Equations Time Harmonic Form

    Constitutive Relations

    6 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 7

    1D-Wave Equation

    c c A A A

    z ct ct

    t = 0 t = t t = t

    General Solution

  • z

    x y

    E

    H

    |k| = k0n

    Maxwells Equations Plane Wave Solutions Isotropic Case

    8 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Polarization of Electromagnetic Waves

    Polarization is the phenomenon in which electromagnetic waves are restricted in direction of vibration

    Polarization is a property of waves that describes the orientation of their oscillations

    9 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Two beams, otherwise identical, may interact differently with matter if their polarization states are different.

    Interference only occurs when EM waves have the same frequency and polarization (i.e., they are coherent)

    Polarization of Electromagnetic Waves

    Linear

    Circular

    Elliptical

    Random or unpolarized

    Polarization Types

    10 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Linear Polarization

    Plane EM wave linearly polarized Trace of electric field vector is linear Also called plane-polarized light Convention is to refer to the electric field vector

    http://www.univie.ac.at/mikroskopie/1_grundlagen/optik/wellenoptik/6_polarisation.htm

    http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polclas.html

    11 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://en.wikipedia.org/wiki/Image:Linear_polarization_schematic.png

  • Linear Polarization (Animation)

    http://bestanimations.com/Science/Physics/45degree-polarized-light-wave.gif https://userscontent2.emaze.com/images/cac94365-b9dc-4762-9121-96c69882485b/458fc46b-b8bd-43e1-b3db-f7ae1667d4e0image20.gif

    Linear Polarization (Horizontal) Linear Polarization (45 degrees)

    12 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Circular Polarization

    Two perpendicular electric field components of equal amplitude with 90 difference in phase Electric vector rotates counterclockwise right-hand circular polarization Electric vector rotates clockwise left-hand circular polarization

    http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polclas.html

    http://www.univie.ac.at/mikroskopie/1_grundlagen/optik/wellenoptik/6_polarisation.htm

    13 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://en.wikipedia.org/wiki/Image:Circular_polarization_schematic.png

  • Circular Polarization (Animation)

    http://i.imgur.com/3bjXjMd.gif

    Left Handed Circular Polarization (LHC)

    14 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Elliptical Polarization

    Two perpendicular eletric field components not in phase, either with different amplitudes and/or not 90 out of phase Electric vector rotates counterclockwise right-hand elliptical polarization Electric vector rotates clockwise left-hand elliptical polarization The most general state of complete polarization is elliptical

    http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polclas.html

    http://www.univie.ac.at/mikroskopie/1_grundlagen/optik/wellenoptik/6_polarisation.htm

    15 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://en.wikipedia.org/wiki/Image:Elliptical_polarization_schematic.png

  • Animation showing four different polarization states and two orthogonal projections.

    By de:Benutzer:Averse - http://www.radartutorial.eu/06.antennas/pic/zirkulanim.gif via de.wikipedia.org, CC BY-SA 2.0, https://commons.wikimedia.org/w/index.php?curid=4849061

    A circularly polarized wave as a sum of two linearly polarized components 90 out of phase

    By Davidjessop - Own work, CC BY-SA 4.0, https://commons.wikimedia.org/w/index.php?curid=48021939

    Polarization Animation

    16 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Scattering by molecules Reflection and transmission

    at interfaces

    Polarization States Occurring Naturally

    By DrBob Bob Mellish - English Wikipedia repository., CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=724505

    17 Prof. Elias N. Glytsis, School of ECE, NTUA

  • http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polabs.html

    Polarization Applications

    Dichroism Polarizing Glasses

    18 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Photographic Filters When light reflects off water it becomes polarized. Such light is often called glare and can make it harder to see what's behind it. Photographers often use filters to cut out glare and get better pictures.

    3 D films When you watch a 3D film you are actually watching two films shot with different cameras, looking at the same thing but from slightly different angles. When the films are projected the light is polarised and polaroid filters, worn as glasses, can let just one of the films into each eye.

    Liquid Crystal (LCD) Displays There are some crystals that become aligned when an electric field is put across them. When this happens they act as polarising filters.

    Stress Analysis When light passes through some materials its plane of polarisation is rotated. The thicker the material the more it is rotated and different colours are rotated by different amounts. To investigate the stresses in an engineering part you could make a model of it in plastic, pass light through and then put it under stress. The patterns produced which may give an indication of where the material has been deformed.

    Polarization Applications

    http://www.stokesleyscience.org/A%20level%20Physics/EM%20Waves/applications.htm

    19 Prof. Elias N. Glytsis, School of ECE, NTUA

  • At places where the internal stresses are greatest, the colored bands change more rapidly (with distance). Engineers wishing to predict where a mechanical component might fail, when placed under stress, can make a model of the component out of, for example, Perspex and observe the stress patterns (the colored bands are more concentrated where the stresses are greatest. The design of the model can then be modified accordingly before the actual component is manufactured.

    Certain plastics rotate the plane of polarization of light passing through them. The angle through which the plane of polarization is rotated is found to vary when the sample is placed under stress, for example by bending it. The angle also depends on the wavelength of the light. The photograph on the right shows a small part of a plastic set square viewed under normal conditions

    Stress Analysis using Polarization

    20 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Stress Analysis using Polarization

    By Spigget - Own work, CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=9587846

    Stress in plastic glasses

    21 Prof. Elias N. Glytsis, School of ECE, NTUA

  • By PiccoloNamek at the English language Wikipedia, CC BY-SA 3.0, https://commons.wikimedia.org/w/index.php?curid=1103795

    The effects of a polarizing filter (right image) on the sky in a photograph.

    Polarizing Filters

    22 Prof. Elias N. Glytsis, School of ECE, NTUA

  • http://plc.cwru.edu/tutorial/enhanced/files/lc/biref/graphics/birefringence.JPG

    Birefringent Crystals

    23 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://www.olympusmicro.com/primer/images/birefringence/crystalpencil.jpg

  • Measuring the concentration of solutions using Polarization

    Certain solutions rotate the plane of polarization of light passing through them. The angle through which the plane of polarization is rotated depends on the concentration of the solution.

    24 Prof. Elias N. Glytsis, School of ECE, NTUA

  • On the under-side of the top plate of the liquid crystal container, A, are fine lines etched parallel to the plane of polarization of the top Polaroid. Similarly there are lines etched into face B parallel to the plane of the lower Polaroid. The liquid crystals line up with these fine lines but also tend to line up with each other so there is a gradual change in the alignment of the crystals from A to B. The crystals change the plane of polarization of the light so that the light can pass through the lower polarizer and be reflected by the mirror. The display appears light. When a voltage is applied, the crystals line up along the direction of the electric field and they therefore no longer allow light to pass through. The display appears dark.

    Liquid crystal displays

    http://www.connessioni.biz/website/categoria-tecnologie/tecnologia-lcd-inorganici-guida-alla-tecnologia-parte-1.html?lang=en

    25 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Inclusion of a fly in Baltic amber. Although amber is an amorphous substance and in theory optically isotropic, the flow structures of the resin due to internal strain as well as the strain caused by the inclusions can be visualized in polarized light. The use of polarized light and the first-order red compensator lead to intensive colors in the otherwise golden amber . Courtesy of Michael Hgi, Swiss Gemological Society, Bern, Switzerland.

    Cobalt, cold-rolled, Beraha etch, polarization. The examination of microstructure morphology plays a decisive role in materials science and failure analysis. Color contrast and specific microstructure formations can frequently be enhanced by optical polarization of the etched samples under the polarizing microscope. Courtesy of Ursula Christian, University of Pforzheim, Germany.

    Polarizing Microscopy

    http://www.leica-microsystems.com/science-lab/polarization-contrast/

    26 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Fresnel Equations

    1, 0

    1

    2, 0

    x

    z 2

    TE polarization

    TM polarization

    Ei

    Er Et

    Power Conservation

    27 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 28

    Fresnel Equations

    Brewster Angles

    Critical Angle

  • Planar Interface - Wavevector Diagrams

    1, 0

    1

    2, 0

    x

    z 2

    TE polarization TM polarization

    Ei

    Er Et

    29 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Example of Fresnel Equations

    n1 = 1, n2 = 1.5

    30 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1, n2 = 1.5

    Example of Fresnel Equations

    31 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1, n2 = 1.5

    Example of Fresnel Equations

    32 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.5, n2 = 1

    Example of Fresnel Equations

    33 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.5, n2 = 1

    Example of Fresnel Equations

    34 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Example of Evanescent Field n1 = 1.5, n2 = 1

    35 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.5, n2 = 1

    Example of Fresnel Equations

    36 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.0, n2 = 0.855 - j1.8955 (Gold at 0 =0.5m)

    Example of Fresnel Equations

    37 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.0, n2 = 0.855 - j1.8955 (Gold at 0 =0.5m)

    Example of Fresnel Equations

    38 Prof. Elias N. Glytsis, School of ECE, NTUA

  • n1 = 1.0, n2 = 0.855 - j1.8955 (Gold at 0 =0.5m)

    Example of Fresnel Equations

    39 Prof. Elias N. Glytsis, School of ECE, NTUA

  • + =

    Constructive interference (In phase)

    + =

    ( out of phase)

    (Waves cancel)

    Destructive interference

    Wave Interference

    40 Prof. Elias N. Glytsis, School of ECE, NTUA

  • + =

    Constructive interference results when light paths differ by an integer multiple of the wavelength: r = m

    Mirror

    1

    2 *

    When light waves travel different paths, and are then recombined, they interfere.

    Wave Interference

    41 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Destructive interference results when light paths differ by an odd multiple of the half wavelength: r = (2m+1) /2

    Mirror

    1

    2 *

    When light waves travel different paths, and are then recombined, they interfere.

    + =

    Wave Interference

    42 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 43

    Two Plane Wave Interference x

    z 1

    2

    k1

    k2

    n

    Special Case: 1= - 2 =

  • Prof. Elias N. Glytsis, School of ECE, NTUA 44

    Special Case: 1= 60deg and 2= 0deg

    Two Plane Wave Interference

  • Double-Slit Experiment (Youngs Experiment)

    45 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Double-Slit Experiment (Youngs Experiment)

    46 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 47

    Double-Slit Experiment (Youngs Experiment)

  • https://upload.wikimedia.org/wikipedia/commons/1/18/%D0%97%D0%B5%D1%80%D0%BA%D0%B0%D0%BB%D0%BE_%D0%9B%D0%BB%D0%BE%D0%B9%D0%B4%D0%B0.png

    Lloyds Mirror

    48 Prof. Elias N. Glytsis, School of ECE, NTUA

    z

    x

    L

    D

    mirror

    Lloyds Mirror

    S

    A

  • Prof. Elias N. Glytsis, School of ECE, NTUA 49

    i

    t

    i

    A

    B

    C

    D

    E

    t nf

    n0

    n0

    Transmitted Waves

    Reflected Waves

    Fabry-Perot Interferometer

  • Prof. Elias N. Glytsis, School of ECE, NTUA 50

    Fabry-Perot Interferometer

  • Prof. Elias N. Glytsis, School of ECE, NTUA 51

    Asymmetric Fabry-Perot Interferometer with Gain or Loss

    G = et

    Gain Loss

  • Prof. Elias N. Glytsis, School of ECE, NTUA 52

    Symmetric Fabry-Perot Interferometer

    m m+1 m-1

    FSR

    Resonant Frequencies

  • Prof. Elias N. Glytsis, School of ECE, NTUA 53

    Symmetric Fabry-Perot Interferometer

    Coefficient of Finesse

  • Prof. Elias N. Glytsis, School of ECE, NTUA 54

    Symmetric Fabry-Perot Interferometer

    /k0 m01 m02

    2m 2m

    1

    1/2

    Minimum Wavelength Separation

  • Prof. Elias N. Glytsis, School of ECE, NTUA 55

    m m+1 m-1

    FSR

    Symmetric Fabry-Perot Interferometer

    Resolving Power

    Finesse

  • Fabry-Perot Interferometer

    56 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Thin Film Interference Examples

    http://www.explainthatstuff.com/thin-film-interference.html

    Soap Bubbles Oil Thin Films

    R. A. Serway and J. W. Jewett, Physics for Scientists and Engineers, Thomson Brooks/Cole, 6th Ed. 2004

    Oil film

    Incident Sunlight

    Multiple Colors

    Red Orange Green Blue

    Internal Reflection

    External Reflection

    57 Prof. Elias N. Glytsis, School of ECE, NTUA

  • http://en.wikipedia.org/wiki/Morpho

    Morpho butterflies

    Thin Film Interference Examples

    Peacock Feathers

    http://www.microscopyu.com/articles/polarized/interferenceintro.html http://www.rowland.harvard.edu/organization/past_research/optics/default.html

    58 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Michelson Interferometer

    http://www.britannica.com/EBchecked/topic/380060/Michelson-interferometer

    http://skullsinthestars.com/2008/10/16/fabry-perot-and-their-wonderful-interferometer-1897-1899/

    59 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 60

    Michelson Interferometer

    http://cnx.org/contents/APKEiCUR@3/The-Michelson-Interferometer

    With Compensators

  • Michelson Interferometer Sample Patterns

    61 Prof. Elias N. Glytsis, School of ECE, NTUA

  • http://physics.aps.org/articles/v9/17

    Gravitational Waves Measurement LIGO (Light Interferometer Gravitational-Wave Observatory)

    Observation of Gravitational Waves from a Binary Black Hole Merger B.P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration) Phys. Rev. Lett. 116, 061102 (2016)

    Video: A schematic depiction of LIGOs interferometric gravitational wave detector. Light from a laser is split in two by a beam splitter; one half travels down the vertical arm of the interferometer, the other half travels down the horizontal arm. The detector is designed so that in the absence of gravitational waves (top left) the light takes the same time to travel back and forth along the two arms and interferes destructively at the photodetector, producing no signal. As the wave passes (moving clockwise from top right) the travel times for the lasers change, and a signal appears in the photodetector. (The actual distortions are extremely small, but are exaggerated here for easier viewing.) Inset: The elongations in a ring of particles show the effects of a gravitational wave on spacetime.

    62 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102

  • Observation of Gravitational Waves from a Binary Black Hole Merger B.P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration) Phys. Rev. Lett. 116, 061102 (2016)

    First Experimental Measurement of Gravitational Waves on September 14, 2015 at 09:50:45 UTC (coordinated universal time)

    Gravitational Waves Measurement LIGO (Light Interferometer Gravitational-Wave Observatory)

    63 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102

  • Observation of Gravitational Waves from a Binary Black Hole Merger B.P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration) Phys. Rev. Lett. 116, 061102 (2016)

    http://blogs.scientificamerican.com/sa-visual/ligo-and-gravitational-waves-a-graphic-explanation/

    Gravitational Waves Measurement LIGO (Light Interferometer Gravitational-Wave Observatory)

    64 Prof. Elias N. Glytsis, School of ECE, NTUA

    http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102http://link.aps.org/doi/10.1103/PhysRevLett.116.061102

  • Evolved Laser Interferometer Space Antenna (eLISA)

    eLISA would be the first dedicated space-based gravitational wave detector. It aims to measure gravitational waves directly by using laser interferometry. The LISA concept has a constellation of three spacecraft, arranged in an equilateral triangle with million-kilometre arms (5 million km for classic LISA, 1 million km for eLISA) flying along an Earth-like heliocentric orbit.

    Proposed for launch in 2034

    https://en.wikipedia.org/wiki/Evolved_Laser_Interferometer_Space_Antenna

    65 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Antireflection Layer

    n1 n2 nc

    dc

    1

    x

    z antirelection

    layer

    http://www.pveducation.org/pvcdrom/anti-reflection-coatings

    Comparison of surface reflection from a silicon solar cell, with and without a typical anti-reflection coating.

    66 Prof. Elias N. Glytsis, School of ECE, NTUA

  • Prof. Elias N. Glytsis, School of ECE, NTUA 67

    Antireflection Layer Amorphous Silicon (Solar Cells)

    0 = 0.6m, = 0 deg

    http://www.filmetrics.com/refractive-index-database/Si/Silicon Amorphous Silicon Data 2

    Amorphous Silicon Data 1 https://refractiveindex.info/?shelf=main&book=Si&page=Pierce

    D. T. Pierce and W. E. Spicer, Electronic structure of amorphous Si from photoemission and optical studies, Phys. Rev. B 5, 3017-3029 (1972)

    Amorphous Silicon Data 1 Amorphous Silicon Data 2

    https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017https://doi.org/10.1103/PhysRevB.5.3017

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