Complex numbers/phasors and amplitudes Student question: since the Re part of a complex field is the physical one, why do we need the full phasor length.

Slides:



Advertisements
Similar presentations
Light.
Advertisements

Chris A. Mack, Fundamental Principles of Optical Lithography, (c) 2007
AQA Science © Nelson Thornes Ltd P3 2 Summary Light and sound Jim Reed/Digital Vision WW (NT)
Which of the two photographs appears to be the sharpest to your eyes? The image on the left has relatively low resolution with high contrast, while the.
White n t Wavelength (nm) R t = 400 nm, n = 1.515,  = 0.
Rf 1) 2) 3) p.a. Which ray is NOT correct? R f 1) 3) p.a. Ray through center should reflect back on self. Which ray is NOT correct?
Chapter 35 The concept of optical interference is critical to understanding many natural phenomena, ranging from color shifting in butterfly wings to intensity.
Today 1/27  HW: 1/27 Handout “Anti-Reflection Coating” due Thursday 1/30  Today: Reflections at Boundaries 27.3  Thin Film Interference 27.3  Labs.
Electromagnetic waves Transverse wave Oscillating quantities: electric and magnetic fields, in phase, perpendicular to each other and direction of propagation.
Suppose that you hold the transparency in the photograph below in front of a mirror. How will its reflection appear? Is the image: (1) inverted top-to-bottom?
Today 1/29  Lab Questions?  Air wedges, soap films, coatings  HW:1/29 “Air Wedge” handout Due Friday 1/31  Thursday:Begin Ch 26 Refraction  Peer guidance.
Light Chapter 19.
Behavior of Light.
Interactions of Light With Matter Science: Chapter 3 Mrs. Milliken.
W. Sautter Normal Line Normal Line ii rr ii rr Glass n = 1.5 Air n =1.0  r = angle of refraction  i = angle of incidence Light travels.
Ray Diagrams.
Optics. Spherical Mirrors Spherical mirror – a section of a sphere of radius R and with a center of curvature C R C Mirror.
All visible objects emit or reflect light rays in all directions.
Physics for Scientists and Engineers, 6e
Interference Applications Physics 202 Professor Lee Carkner Lecture 25.
Announcements 11/14/11 Prayer HW 29 problem Labs 8 & 9 due Saturday Progress Reports… Review: Rubes.
Properties of Multilayer Optics An Investigation of Methods of Polarization Analysis for the ICS Experiment at UCLA 8/4/04 Oliver Williams.
sections 26-3 – 26-5 Physics 1161: Pre-Lecture 22 Reflection and Refraction of Light.
ConcepTest #37: An electromagnetic wave travels from region 1 with index of refraction n 1 into region 2 with index of refraction n 2. The index of refraction.
Design Realization lecture 25 John Canny 11/20/03.
6. Interference by thin films t No phase shift (if n 2 < n 1 ) Phase shift -_____ (if n 2 > n 1 ) If there is a very thin film of material – a few wavelengths.
Interference Applications Physics 202 Professor Lee Carkner Lecture 25.
Review: Laws of Reflection and Refraction
Modern Optics IV-coherence Special topics course in IAMS Lecture speaker: Wang-Yau Cheng 2006/4.
Chapter 18 Mirrors and Lenses Mirrors A. Objects and Images in Plane Mirrors. A. Objects and Images in Plane Mirrors. B. Concave Mirrors. B. Concave.
Introduction to Mirrors Light incident on an object Absorption Everything true for wavelengths
Defining and Evaluating Multilayer Coatings in FRED Marko Swoboda.
GHSGT Review Day 2 – Describe the Properties of a Wave.
Light through a Converging lens. Lesson Objectives. Know how converging lenses refract light. Describe how to draw light diagrams from convex lenses.
Curved Mirrors: Locating Images in Concave & Convex Mirrors.
Chapter 20 Mirrors and Lenses. Objectives 20.1 Explain how an image is formed in three types of mirrors 20.1 Identify examples and uses of plane, concave,
PHENOMENA OF LIGHT Chapters 27, 29, & 31. Easy to get mixed up… Polarization (Light)Ch 27 Reflection (Water & Light)Ch 29 Refraction (Light)Ch 29 Dispersion.
Fa ‘04 Hopkins Chapter 19: Models of Light Particle Model of Light – Isaac Newton, in the mid 1600’s Wave Model of Light – mid to late 1800’s – lots of.
1 Electromagnetic waves: Multiple beam Interference Friday November 8, 2002.
Interference Applications Physics 202 Professor Lee Carkner Lecture 25.
1 Electromagnetic waves: Interference Wednesday November 6, 2002.
Complex numbers/phasors and amplitudes There was a question last time: since the Re part of a complex field is the physical one, why do we need the full.
Electromagnetic Waves
Newton’s rings between two curved surfaces
1 Electromagnetic waves: Reflection, Transmission and Interference Monday October 28, 2002.
1 Electromagnetic waves: Interference Wednesday October 30, 2002.
6.2 Two slit interference Coherence Two-Slit Interference Thin film Interference.
Dispersion The spreading of light into its color components is called dispersion. When light enters a prism, the refracted ray is bent towards the normal,
Today’s agenda: Thin Film Interference.
Science 8: Unit C – Light and Optical Systems Topic 3: Refraction.
Today’s Lecture will cover textbook sections 26-3 – 26-5, 26-8 Physics 1161: Lecture 17 Reflection and Refraction of Light.
STScI Calibration Workshop1 Fringing in the WFC3/UVIS detector Mike Wong UC Berkeley.
Multiple Beam Interference at Dielectric Interfaces n1n1 n2n2 n3n3 If the reflectivity is high, multiple reflections can not be ignored Things can get.
Non-reflective coating Good quality lenses in a camera reflect very little light and appear dark or slightly purple. A thin coating of a fluoride salt.
Physics 102: Lecture 16, Slide 1 Physics 102: Lecture 16 Introduction to Mirrors.
Chapter Four: Chemistry and Physics Connections 4.1 Elements, Compounds, and Reactions 4.2 Carbon Compounds and Cells 4.3 Light and Living Things.
Final Exam (chapters since Exam#2). time: Friday 05/03 3:30 pm- 5:30 pm. Location: room 114 of physics building. If you can not make it, please let me.
Light and Optics Part Three: Optics and Reflection.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. Schematic diagram for second-harmonic generation using quadrature configuration.
Review: Laws of Reflection and Refraction
Polarization of Electromagnetic Waves
1 Electromagnetic waves: Interference Wednesday October 30, 2002.
Announcements 2/3/12 Prayer.
Reading Quiz In the text’s treatment of the double boundary problem, in the middle region all of the reflections that end up traveling to the right are.
Soap film illuminated by bright white light
Complex numbers/phasors and amplitudes
Thin Films.
Thin film constr.,destr. interference
Unit 4 - Energy Learning Target 4.4 – Be able to describe wave interactions (reflection, refraction, diffraction, and absorption),
Air-Water (n=1.3)-Air film (soap film) Normal incidence
Presentation transcript:

Complex numbers/phasors and amplitudes Student question: since the Re part of a complex field is the physical one, why do we need the full phasor length as the physical field magnitude? The physical field is the Re part of E at each time. At some time the phasor will rotate across the real axis, and the amplitude will peak. So the phasor magnitude is the physical field amplitude.

Absorption filters (colored glass) Transmission vs :

short-pass filter Multilayer filters and Multilayer mirrors--- based on interference: much sharper and specialized features possible. Notch filter 3-notch filter long-pass filter

Multilayer method summary

P. If we choose a layer of effective thickness “  /2”, the matrix M will ______: a) have zeros for its diagonal elements b) have zeros for its off-diagonal elements (Note: in multilayer technology, layers described as “  /2” or “  /4”, etc,  is that in the material, not vacuum. The effective thickness is.)

Physics 123 ideas If we choose the thickness to be “  /4”, the phases of these reflecting rays (due to thickness alone) are ________. a)All in phase b)Alternating phase

If we choose the thickness to be “  /4”, and we want a high R, we better choose the n’s to be ___________. Look at the phase of the first three reflections. a)(1.4, 1.5, 1.8) b)(1.5, 1.4, 1.8) Physics 123 ideas

Reflectance and coatings Air-Glass (multilayer theory works for zero layers, too!): Normal incidence Normal incidence R≈4% across visible for n G =1.5.

Anti-reflectance coatings Single /4 layer, Normal incidence Air-L-Glass (H) : Normal incidence R≈1% across visible for n G =1.5.

Anti-reflectance coatings Two /4 layers, normal incidence Air-L-H-Glass : More freedom to chose n’s, so usually better at some design, but but not so good at ’s away from the design. LH

Single /4 Anti-Reflectance Coating: AL Glass(H) light still bounces among lenses in camera, spreading glare Triple /4 coating : ALHLGlass(H)

High reflectance multilayers Air-(HL) N -Glass(H) /4 layers Better: Air-(HL) N -H-Glass

Computer design can optimize for any application, with different d’s, n’s and ordering One complication n: depends on.