Title: 16.711 Lecture 1 Review of Wave optics
116.711 Lecture 1 Review of Wave optics
Today
- Introduction to this course
- Light waves in homogeneous medium
- Monochromatic Waves in inhomogeneous medium
- Polychromatic waves
- Multiple interference and optical resonator
- Diffraction principle and diffraction grating
216.711 Lecture 1 Review of Wave optics
Syllabus and policy of the course
- Syllabus, course materials, schedules are
available on the course website - http//faculty.uml.edu/xlu/16.711
Course contents
- Introduction of the course, reviews of Wave
Optics - Dielectric waveguides and optical fibers, mode
and effective index - Optical Fiber modal and wavdguide dispersions,
dispersion management - Mode-coupling theory, Mach-zehnder
interferometer, Directional coupler, taps and WDM
coupler - Electro-optics, polarization and modulation of
lights - Optical Amplifiers. noise figure, gain profile,
ASE noise. Gain equalization, optical
filter, bit error rate, amplifier cascade - DWDM technology, Gratings, AWG, Fiber Bragg
grating - Photonic switches and all optical switches
- Nonlinear Fiber optics
316.711 Lecture 1 Review of Wave optics
Light waves in homogeneous medium
Helmholtz equation
- Plane electromagnetic wave
416.711 Lecture 1 Review of Wave optics
Light waves in homogeneous medium
516.711 Lecture 1 Review of Wave optics
616.711 Lecture 1 Review of Wave optics
Total Power
The ratio of the power carried within a circle
of radius
The power contained within a circle of radius
86 of the total power.
99 of the total power is contained within a
circle of radius .
716.711 Lecture 1 Review of Wave optics
- Beam radius of a Gaussian beam
is the spot size.
is the waist radius.
when
86 energy is confined in the cone.
816.711 Lecture 1 Review of Wave optics
is the spot size.
is the waist radius.
The gaussian has minimum width at .
The axial distance for the beam width
is called depth of focus.
916.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
1016.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
The Fresnels equations is derived from the
boundary conditions.
when
At normal incidence, no phase shift if n1gtn2, 180
phase shift if n2gtn1.
1116.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
- polarization angle or Brewsters angle
At
The reflected wave is linear polarized.
1216.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
- Total internal reflection
The amplitude of the reflected wave is 1.
At
The phase of the reflected wave changes with the
incident angle.
1316.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
- Total internal reflection and evanescent wave
1416.711 Lecture 1 Review of Wave optics
Monochromatic waves in inhomogeneous medium
- Reflectance and Transmittance
1516.711 Lecture 1 Review of Wave optics
Polychromatic waves
wave packet speed
is called group index.
Exercise the difference between phase velocity
and group velocity?
1616.711 Lecture 1 Review of Wave optics
Polychromatic waves
- absorption and dispersion
is the absorption or attenuation coefficient.
a wave packet broadening for a length of L is
dispersion parameter
1716.711 Lecture 1 Review of Wave optics
Polychromatic waves
- classical picture of the susceptibility
classical electron moving equation
1816.711 Lecture 1 Review of Wave optics
Multiple interference and optical resonator
- interference of monochromatic waves
Mach-zehnder
Sagnac
Michelson
1916.711 Lecture 1 Review of Wave optics
Multiple interference and optical resonator
- interference of two oblique plane waves
interference of a plane wave and spherical wave
2016.711 Lecture 1 Review of Wave optics
Multiple interference and optical resonator
- interference of two monochromatic waves light
beating
2116.711 Lecture 1 Review of Wave optics
Multiple interference and optical resonator
Diffraction principle and diffraction grating
2216.711 Lecture 1 Review of Wave optics
Diffraction principle
- The Fourier optics view of Fraunhofer diffraction
In far fields, the spatial frequency is
transferred to position.
2316.711 Lecture 1 Review of Wave optics
Diffraction grating