opti510r: photonics

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OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona [email protected] Meinel building R.626

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Page 1: OPTI510R: Photonics

OPTI510R: Photonics

Khanh Kieu

College of Optical Sciences,

University of Arizona

[email protected]

Meinel building R.626

Page 2: OPTI510R: Photonics

Important announcements

• Homework #2 is assigned, due Feb. 11

• Mid-term exam on Feb 27 (open books/notes)

Page 3: OPTI510R: Photonics

Fabry Pérot Interferometer

Page 4: OPTI510R: Photonics

Fabry Pérot Interferometer

Page 5: OPTI510R: Photonics

Laser Gyroscope

We can easily measure fbeat with <1Hz precision. What would

be the smallest rotation rate that we can measure using a

ring Resonator with 1m radius?

Page 6: OPTI510R: Photonics

Laser Gyroscope

Page 7: OPTI510R: Photonics

There are many other interferometers

• Michelson

• Mach-Zehnder

• Sagnac

• Fabry-Perot

• Fizeau

• Twyman-Green

• Newton

• Nomarski

• …

Page 8: OPTI510R: Photonics

Question for thoughts

Can you come up with a new type of interferometer?

Can we explain interference by a different mechanism other than

waves?

New modulator design for optical communication?

What is the sharpest resonance that we can make?

Can you build a gyroscope that can measure the rotation of the earth

and would still cost <$100?

Can you build a company and then sell it for $100M?

Page 9: OPTI510R: Photonics

Diffraction and Devices

Diffraction

Overcoming the diffraction limit

Diffraction gratings

Ruled grating

Holographic grating

Volume grating

Applications

Tunable laser

Spectroscopy

Laser stabilization

Pulse compression

Volume grating

Page 10: OPTI510R: Photonics

Diffraction

Diffraction relies on the interference of waves emanating from

the same source taking different paths to the same point on a

screen Diffraction can be explained by interference

Diffraction of a laser beam

through a small circular hole

(Airy disk)

Young's double-slit interferometer

Wikipedia

Page 11: OPTI510R: Photonics

Diffraction and nature of light

Arago spot, Fresnel bright spot, or Poisson spot

Need to be in

the near field:

This experiment confirmed the wave nature of light!

Wikipedia

Page 12: OPTI510R: Photonics

Huygens–Fresnel principle

Near field and far-field diffraction

Wikipedia

Page 13: OPTI510R: Photonics

Diffraction limit

How to overcome the diffraction limit?

Page 14: OPTI510R: Photonics

Overcoming the diffraction limit

Page 15: OPTI510R: Photonics

Overcoming the diffraction limit

nobelprize.org

Page 16: OPTI510R: Photonics

STED: Stimulated emission depletion

nobelprize.org

Page 17: OPTI510R: Photonics

STORM: Stochastic Optical

Reconstruction Microscopy

nobelprize.org

Page 18: OPTI510R: Photonics

STORM: Stochastic Optical

Reconstruction Microscopy

nobelprize.org

Page 19: OPTI510R: Photonics

STORM: Stochastic Optical

Reconstruction Microscopy

nobelprize.org

Page 20: OPTI510R: Photonics

Diffraction Grating

A periodic structure that diffracts light into different directions.

Grating can be flat, concave, convex and arbitrary shape

HeNe laser incident on a diffraction grating

showing zero, first and second order beams

Page 21: OPTI510R: Photonics

Diffraction Grating

Page 22: OPTI510R: Photonics

Diffraction Grating

Page 23: OPTI510R: Photonics

Basic equations

Monochromatic source White light

Page 24: OPTI510R: Photonics

Blazed grating

Need: how to concentrate all the lights ------into one order?

Solution: make the grating of right

triangles with a braze angle . By tilting the

slit faces to the normal of incidence of the

desired order, grating efficiencies >90%

can be achieved

Blazed grating

Page 26: OPTI510R: Photonics

Grating fabrication-Ruled grating

Formed by physically writing grooves on a reflective surface

with a diamond blade mounted on a ruling machine:

Ruled grating

Diamond

milling

High throughput and efficiency Maximum groove density of ---3600g/mm Good in IR and far IR Expensive

Page 27: OPTI510R: Photonics

Grating fabrication-Ruled grating

Page 28: OPTI510R: Photonics

Grating fabrication-Ruled grating

Measured at Littrow configuration

Page 29: OPTI510R: Photonics

Holographic grating

Formed by interference lithography and etch

Low stray light and dense groove spacing

Lower reflectivity Maximum groove density of

6000g/mm Availability of non flat substrate Good in UV, short wavelength

Page 30: OPTI510R: Photonics

Holographic grating

Fringe locking controller locks the interference image to moving

substrate by correcting stage error and interferometer phase error

Page 31: OPTI510R: Photonics

Holographic grating

Lightsmith transmission grating

Excellent diffraction efficiency

Page 32: OPTI510R: Photonics

Volume grating

Diffraction efficiency ~99%

Narrow bandwidth

Page 33: OPTI510R: Photonics

Bragg mirrors

22110

0022110

,2

/2,2)(2

dndnn

n

c

ckdndnk

B

Constructive interference

for two layers of a segment

Bragg frequency

Page 34: OPTI510R: Photonics

Fiber Bragg gratings

Fiber laser reflector, filter, dispersion compensator…

Page 35: OPTI510R: Photonics

Fiber Bragg gratings

High Power Fiber Lasers

Page 36: OPTI510R: Photonics

Tunable Grating

Microelectromechanical Systems (MEMS)

spring comb drive actuator

Page 37: OPTI510R: Photonics

Applications-Tunable laser

InAs/GaAs quantum dots laser

Littrow configuration: light of desired

wavelength is diffracted back along

incident beam

Beam rotates as you tune!

Page 38: OPTI510R: Photonics

Applications-Tunable laser

Littman-Metcalf configuration: grating is kept at a fixed angle and a special

mirror is rotated to tune the output wavelength.

Output beam is aligned at grazing incidence

with grating. First order diffracted beam is

sent to retroreflector (mirror) that reflects

beam back to itself.

High efficiency for TM polarization (light

polarized perpendicular to grooves).

Output is the zeroth order reflected beam off

the grating.

Page 39: OPTI510R: Photonics

Applications-Laser stabilization

Page 40: OPTI510R: Photonics

Applications-Spectroscopy

• Czerny-Turner Configuration

– two concave mirrors and planar diffraction grating

– more degrees of freedom, good coma correction at one wavelength

asymmetrical geometry

M1: collimating light sourceM2: focus disperse light from grating

Page 41: OPTI510R: Photonics

Applications-Spectroscopy

Page 42: OPTI510R: Photonics

Applications-Pulse compression

Compressed

pulse

Provide normal dispersion

Page 43: OPTI510R: Photonics

Applications-Pulse compression

Schematic diagram of a chirped pulse amplification system

Page 44: OPTI510R: Photonics

Optics of periodic structures

Photonics crystal!

Page 45: OPTI510R: Photonics

Questions for Thoughts

• Can you come up with a better way to overcome the diffraction limit?

• Can you create a new optics company making diffractive devices?

• Why there is a strong polarization dependence in diffraction

efficiency for metal-coated ruled gratings?

• A compact device providing adjustable GVD with low loss?

• A diffraction grating with 100% diffraction efficiency and broad

operating bandwidth?