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Lecture 2 Andrei Sirenko, NJIT 1 Welcome to Phys 774: Principles of Spectroscopy Fall 2007 Lecture 2 Andrei Sirenko, NJIT 2 Instructor: Andrei Sirenko Associate Professor at the Dept. of Physics, NJIT http://web.njit.edu/~sirenko 476 Tiernan Office hours: After the classes on We.’s or by appointment 973-596-5342 Class Schedule: Wednesday 11:30am - 12:55pm | FMH 106 Friday 1:00pm - 2:25pm | FMH 203 Lecture 2 Andrei Sirenko, NJIT 3 Spectrum of Electromagnetic Radiation and Light Lecture 2 Andrei Sirenko, NJIT 4 How can we produce EM waves ?
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Page 1: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 1

Welcome to

Phys 774: Principles of Spectroscopy

Fall 2007

Lecture 2 Andrei Sirenko, NJIT 2

Instructor:Andrei SirenkoAssociate Professor at the Dept. of Physics, NJIT

http://web.njit.edu/~sirenko

476 Tiernan

Office hours: After the classes on We.’s or by appointment973-596-5342

Class Schedule:Wednesday 11:30am - 12:55pm | FMH 106Friday 1:00pm - 2:25pm | FMH 203

Lecture 2 Andrei Sirenko, NJIT 3

Spectrum of Electromagnetic Radiation and Light

Lecture 2 Andrei Sirenko, NJIT 4

How can we produce EM waves ?

Page 2: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 5

How can we analyze EM waves ?

Position Wavelength

Resolution

Prism vs. Grating

Lecture 2 Andrei Sirenko, NJIT 6

Resolution depends on d – number of groves per mm

How can we analyze EM waves ?

Lecture 2 Andrei Sirenko, NJIT 7

Energy Dispersive Principlehttp://www4.nau.edu/microanalysis/Microprobe/Course%20Overview.html

How can we analyze EM waves ?

Lecture 2 Andrei Sirenko, NJIT 8

Interferometry Principle

How can we analyze EM waves ?

Page 3: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 9

Light and Atoms

Lecture 2 Andrei Sirenko, NJIT 10

Light and Atoms

Lecture 2 Andrei Sirenko, NJIT 11

Light and Atoms

Lecture 2 Andrei Sirenko, NJIT 12

Light and Atoms

Page 4: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 13

Light and Atoms

Lecture 2 Andrei Sirenko, NJIT 14

Light and Atoms: Photoelectric Effect

Lecture 2 Andrei Sirenko, NJIT 15

Light and Atoms: Photoelectric Effect

Lecture 2 Andrei Sirenko, NJIT 16

Wave-Particle Duality

Page 5: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 17

Wave-Particle Duality

Lecture 2 Andrei Sirenko, NJIT 18

The interaction of radiation with matter

Lecture 2 Andrei Sirenko, NJIT 19

The interaction of radiation with matter

Lecture 2 Andrei Sirenko, NJIT 20

Application of Lasers

TELECOMMUNICATIONLaser Dreams

Page 6: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 21

Types of LasersThe laser medium can be a solid, gas, liquid or semiconductor.

Solid-state lasers have lasing material distributed in a solid matrix (such as the ruby or neodymium:yttrium-aluminum garnet "YAG" lasers). The neodymium-YAG laser emits infrared light at 1064 nanometers (nm).

Gas lasers (helium and helium-neon, HeNe, are the most common gas lasers) have a primary output of visible red light. CO2 lasers emit energy in the far-infrared, and are used for cutting hard materials.

Excimer lasers (the name is derived from the terms excited and dimers) use reactive gases, such as chlorine and fluorine, mixed with inert gases such as argon, krypton or xenon. When electrically stimulated, a pseudo molecule (dimer) is produced. When lased, the dimer produces light in the ultraviolet range.

Dye lasers use complex organic dyes, such as rhodamine 6G, in liquid solution or suspension as lasing media. They are tunable over a broad range of wavelengths.

Semiconductor lasers, sometimes called diode lasers, are not solid-state lasers. These electronic devices are generally very small and use low power. They may be built into larger arrays, such as the writing source in some laser printers or CD players.

And more: Ring lasers, Disk lasers, Free electron lasers, …Lecture 2 Andrei Sirenko, NJIT 22

Regular Light

Laser Light

What is the difference ?

Properties of laser radiation:

•Monochromatic•Coherent•Directional

•Stimulated emission and gain

Lecture 2 Andrei Sirenko, NJIT 23

Laser Wavelength

Properties of laser radiation:

•Monochromatic•Coherent•Directional

•Stimulated emission and gain

Lecture 2 Andrei Sirenko, NJIT 24

Regular Light

Laser Light

Like rain

Page 7: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 25

Regular Light

Laser Light

Like rain

go !

COHERENCE:

Lecture 2 Andrei Sirenko, NJIT 26

Regular Light

Laser Light

go !

COHERENCE:

Lecture 2 Andrei Sirenko, NJIT 27

Red Laser

Orange Laser

Yellow Laser

Green Laser

Blue Laser

Indigo Laser

Violet LaserAnything else ?

Visible Lasers:

Lecture 2 Andrei Sirenko, NJIT 28

Typical Laser Wavelengths:

1060010600Carbon dioxide (FIR)Carbon dioxide (FIR)

10641064Nd:YagNd:Yag (NIR)(NIR)

694Ruby (CrAlO3) (red)

570-650Rhodamine 6G dye (tunable)

633Helium neon (red)

543Helium neon (green)

514Argon (green)

488Argon (blue)

337Nitrogen (UV)

308Xenon chloride (UV)

248248Krypton fluoride (UV)Krypton fluoride (UV)

193193Argon fluoride (UV)Argon fluoride (UV)

Wavelength (nm)Laser Type

Page 8: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 29

Optical Transmission System

LaserTransmitter(s) Receiver(s)

Optical Fiber

30 - 100 miles

Up to 10,000 miles

Amp Amp

DetectorA

mpl

ifie

r

Lecture 2 Andrei Sirenko, NJIT 30

I/O Fibers

Imaging LensesReflector

MEMS 2-axis Tilt Mirrors

MEMS OXC-- 2N Mirror Design

Beam scanning during connection setup.

2N MEMS mirrors in an NxN single-mode fiber optical crossconnect.

Lecture 2 Andrei Sirenko, NJIT 31

Principles of Laser Radiation

Lecture 2 Andrei Sirenko, NJIT 32

Principles of 3-level laser operation

Page 9: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 33

Principles of the Solid State Laser operation

Lecture 2 Andrei Sirenko, NJIT 34

Semiconductor Lasers

Lecture 2 Andrei Sirenko, NJIT 35

Three level energy diagram of the He-Ne laser transition

Helium

1S

2S

Neon

1S

2P

3S

electron impact

interatomic collision

Laser transition 632 nm

diffusion to wall

1E-8 sec

1E-7 sec

The laser process in a HeNe laser starts with collision of electrons from the electrical discharge with the helium atoms in the gas. This excites helium from the ground state to the long-lived, metastable excited states. Collision of the excited helium atoms with the ground-state neon atoms results in transfer of energy to the neon atoms. This is due to a coincidence of energy levels between the helium and neon atoms.

This process is given by the reaction equation:He* + Ne → He + Ne* + ∆E

Lecture 2 Andrei Sirenko, NJIT 36

Fundamentals of Laser OperationIf the atom is in the excited state, it may decay into the ground state by the process of spontaneous emission:

E2 − E1 = hν

the rate of which stimulated emission, where ρ(ν) is the radiation density of photons :

Stimulated emission cross section

where g1 and g2 are the degeneracies of energy levels 1 and 2, respectively

Optical amplification

General gain equation

Gain:

Saturation intensity:

Large signal:

The intensity of the stimulated emission [W/m2]Saleh, Bahaa E. A. and Teich, Malvin Carl (1991). Fundamentals of Photonics. New York: John Wiley & Sons. ISBN 0-471-83965-5.

Page 10: Welcome to Phys 774: Principles of SpectroscopySirenko/Phys-774/Lecture2-2007.pdfLecture 2 Andrei Sirenko, NJIT 21 Types of Lasers The laser medium can be a solid, gas, liquid or semiconductor.

Lecture 2 Andrei Sirenko, NJIT 37 Lecture 2 Andrei Sirenko, NJIT 38

Examples of transverse Gaussian laser modes

Examples of longitudinal laser modes


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