PHYS 408 Applied Optics (Lecture 8)

Slides:



Advertisements
Similar presentations
One-Dimensional Scattering of Waves 2006 Quantum MechanicsProf. Y. F. Chen One-Dimensional Scattering of Waves.
Advertisements

Today’s summary Polarization Energy / Poynting’s vector
ELEG 648 Plane waves II Mark Mirotznik, Ph.D. Associate Professor The University of Delaware
ENE 428 Microwave Engineering
 Symbolic manipulation with artificial applications …  With little or no connection to the real world…
Wavepackets Outline - Review: Reflection & Refraction - Superposition of Plane Waves - Wavepackets - Δk – Δx Relations.
1 Optical Properties of Materials … reflection … refraction (Snell’s law) … index of refraction Index of refraction Absorption.
Optics of a single Homogeneous and Isotropic Layer
13.6 MATRIX SOLUTION OF A LINEAR SYSTEM.  Examine the matrix equation below.  How would you solve for X?  In order to solve this type of equation,
RS ENE 428 Microwave Engineering Lecture 3 Polarization, Reflection and Transmission at normal incidence 1.
So far, we have considered plane waves in an infinite homogeneous medium. A natural question would arise: what happens if a plane wave hits some object?
Lale T. Ergene Fields and Waves Lesson 5.5 Wave Reflection and Transmission.
Seismology Part V: Surface Waves: Rayleigh John William Strutt (Lord Rayleigh)
PHYS 408 Applied Optics (Lecture 3) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 5)
PHYS 408 Applied Optics (Lecture 10) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 4) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 11) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 9) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 12) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
3.2 Solve Linear Systems Algebraically Algebra II.
PHYS 408 Applied Optics (Lecture 19) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
13.3 Product of a Scalar and a Matrix.  In matrix algebra, a real number is often called a.  To multiply a matrix by a scalar, you multiply each entry.
PHYS 408 Applied Optics (Lecture 6) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
PHYS 408 Applied Optics (Lecture 8)
PHYS 408 Applied Optics (Lecture 7)
PHYS 408 Applied Optics (Lecture 12)
6) x + 2y = 2 x – 4y = 14.
PHYS 408 Applied Optics (Lecture 3)
PHYS 408 Applied Optics (Lecture 15)
Microwave Engineering by David M. Pozar Ch. 4.1 ~ 4 / 4.6
PHYS 408 Applied Optics (Lecture 16)
PHYS 408 Applied Optics (Lecture 21)
Systems of Ordinary Differential Equations Case I: real eigenvalues of multiplicity 1 MAT 275.
PHYS 408 Applied Optics (Lecture 15)
Matrix Operations SpringSemester 2017.
PHYS 408 Applied Optics (Lecture 17)
3.3 Dividing Polynomials.
Announcements 2/3/12 Prayer.
Use Inverse Matrices to Solve Linear Systems
Linear Equations in Linear Algebra
2.6 Factor x2 + bx + c provided ________ = b and ______ = c
ENE 325 Electromagnetic Fields and Waves
PHYS 408 Applied Optics (Lecture 14)
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.
PHYS 408 Applied Optics (Lecture 2)
Linear Algebra Lecture 3.
PHYS 408 Applied Optics (Lecture 7)
PHYS 408 Applied Optics (Lecture 13)
PHYS 408 Applied Optics (Lecture 14)
PHYS 408 Applied Optics (Lecture 17)
PHYS 408 Applied Optics (Lecture 9)
PHYS 408 Applied Optics (Lecture 10)
2.6 Factor x2 + bx + c provided ________ = b and ______ = c
PHYS 408 Applied Optics (Lecture 5)
Thin film constr.,destr. interference
University Physics: Waves and Electricity
PHYS 408 Applied Optics (Lecture 4)
PHYS 408 Applied Optics (Lecture 18)
PHYS 408 Applied Optics (Lecture 2)
PHYS 408 Applied Optics (Lecture 6)
PHYS 408 Applied Optics (Lecture 11)
PHYS 408 Applied Optics (Lecture 20)
PHYS 408 Applied Optics (Lecture 21)
Linear Algebra Lecture 7.
2 Chapter Chapter 2 Equations, Inequalities and Problem Solving.
Matrix Operations SpringSemester 2017.
ENE 428 Microwave Engineering
PHYS 408 Applied Optics (Lecture 19)
Wave BEHAVIOR.
Presentation transcript:

PHYS 408 Applied Optics (Lecture 8) Jan-April 2016 Edition Jeff Young AMPEL Rm 113

Quick review of key points from last lecture One can fairly easily keep track of all multiply reflected wavefronts in a thin-film transmission problem involving incident plane wave, including both their amplitude and phase. Summing the infinite series of interfering waves yields an interesting, non-trivial wavelength dependence to the transmission and reflection properties of the film. The most natural quantities to describe the behaviour include the Fresnel reflection and transmission coefficients associated with both interfaces, and the thickness of the film.

A reminder Infinite series (homework, very intuitive) More powerful approach Remind them of what they did last week at this stage for the single interface problem Write down expressions for the total E field in each region.

The solution Show pdf of handwritten algebra

The solution Condition (equation) for zero reflection? d=600 nm d=600 nm r and t from notes? No, |r|^2 and |t|^2What do you note about these results? 2 pi/lambdo_0 x n x 2d = m (integer) 2 pi, so 1/lambda_0=m/(2 n d), m= 1, 2 Because first reflection has a negative sign, and all remaining ones have positive phase at interfaces Condition (equation) for zero reflection?

Vary e for fixed d=600 nm d=600 nm e=13 d=600 nm e=4 d=600 nm e=2.4

Moving forward Cast our result in the form of a matrix equation that yields the reflected and transmitted wave amplitudes (the out-going wave amplitudes) when the incident wave amplitude from the left hand medium is specified.

Moving forward Cast our result in the form of a matrix equation that yields the reflected and transmitted wave amplitudes (the out-going wave amplitudes) when the incident wave amplitude from the left hand medium is specified.

Moving forward If you had an incident wave from the right hand side, how might you express the corresponding matrix representation of the out-going field amplitudes?

Moving forward Can you combine these to generate a matrix equation that yields the outgoing waves for the general case when you have two in-coming waves, one from each side?

The S and M matricies Would this S matrix help you easily solve for the overall reflected and transmitted fields if you had multiple dielectric layers up against each other? What would the ideal “transfer matrix” be that would allow you to get the overall transmission simply by multiplying matrices for each boundary?

The S and M matricies Can you obtain this desired matrix, call it the M matrix, from the S matrix?

The S and M matricies What is then the algorithm for obtaining the overall transmission and reflection amplitude for plane waves incident on an arbitrary number of dielectric films arranged in a planar stack?

Let’s play! … … n1 d1 n2 d2 n1 d1 n2 d2 n1 d1 n3 d3 n1 d1 n2 d2 n1 d1 nlayers-1 nlayers-1