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Lecture 31 Lecture 31

Lecture 31 - PowerPoint Presentation

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Lecture 31 - PPT Presentation

General issues of spectroscopies I c So Hirata Department of Chemistry University of Illinois at UrbanaChampaign This material has been developed and made available online by work supported jointly by University of Illinois the National Science Foundation under Grant CHE1118616 CAREE ID: 268559

spectroscopy emission spectroscopies stimulated emission spectroscopy stimulated spectroscopies optical absorption electronic elements modes transitions dispersing spontaneous wave radiation

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Slide1

Lecture 31General issues of spectroscopies. I

(c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign.

This material has

been developed and made available online by work supported jointly by University of Illinois, the National Science Foundation under Grant CHE-1118616 (CAREER), and the Camille & Henry Dreyfus Foundation, Inc. through the Camille Dreyfus Teacher-Scholar program. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the sponsoring agencies

.Slide2

General issues of spectroscopiesIn this lecture, we have an overview of spectroscopies:

Photon energies and dynamical degrees of freedom and spectroscopies

Three elements of spectroscopy

Three modes of optical transitions

Lasers

Spectral

linewidthsSlide3

Important physical quantitiesλ

(wave length) (typically in nm)

v

(frequency) (typically in Hz = s

–1

) = c / λ (wave number) (in cm–1) = 1 / λ = v / cVisible light : 400 – 700 nm1 eV = 8065 cm–1 298 K = 207 cm–1 10000000 / 400 nm = 25000 cm–1 = 3.1 eVSlide4

Photon energies and spectroscopies

Radio-wave

Micro-wave

IR

Visible

UVX-rayγ-ray>30 cm30 cm – 3 mm33–13000 cm–1 700–400 nm3.1–124 eV100 eV –100 keV

>100 keVNuclear spinRotation

VibrationElectronicElectronicCore

electronicNuclearSlide5

Electronic, vibration, and rotation

Born-Oppenheimer approximation

Exact separation

Rigid rotor approximationSlide6

Electronic, vibration, and rotation

kT

Vibrational spectroscopy

IR/Raman spectroscopies

Electronic spectroscopy

UV/

vis spectroscopyRotational spectroscopy

Microwave spectroscopySlide7

Three elements of

spectroscopy

1. Source

Sample

Reference

2. Dispersing element3. DetectorSlide8

Sources of radiation

The sun and stars

Various conventional lamps

Newer radiation

sources:

LasersSynchrotron radiationPublic domain image created by U.S. Department of EnergyAdvanced Light Source at Argonne National LaboratorySlide9

The dispersing elements: prism

air

glassSlide10

The dispersing

elements: diffraction gratingSlide11

The dispersing

elements: Fourier transform technique

M

ovable mirror

Mirror

Laser Interferometer Gravitational Observatory (LIGO) at Hanford, WA Copyrighted image in courtesy of LIGO LaboratoryHalf mirrorSlide12

Detectors

CCD

CCD

Digital camera

Photodiode

Photodiode

Pyroelectric

Pyroelectric

Remote control

Optical mouse

Barcode reader

Heat sensing missile

Night vision goggle Slide13

Stimulated

absorption

Stimulated

emission

Spontaneous

emissionEinstein’s theory of three modes of optical transitionsAbsorption always needs the help of photon – stimulated absorption.Emission occurs in two ways – stimulated or spontaneous emission.Slide14

Three modes of optical transitions

Stimulated

absorption

Stimulated

emission

Spontaneous

emission

A

B

B

'

ρ

ρ

N

N

'Slide15

Three modes of optical transitions

Equilibrium: no net excitation or deexcitation

Blackbody radiationSlide16

Three modes of optical transitions

Same effects on both states. If it were not for

A

,

N

= N'

Einstein

A coeff

Stimulated

absorptionStimulated emission

Spontaneousemission

A

B

B

'

ρ

ρ

N

N

'

Einstein

B

coeff

The

greater the

frequency, the

the greater the rate of the spontaneous

emission, causing Boltzmann distribution Slide17

Lasers

High power

Monochromatic and polarized

Coherent

Low divergence and long

path lengthsSlide18

Population inversion

Thermal equilibrium

Pumping

Laser actionSlide19

Applications of laserHigh power

Nonlinear/

multiphoton

spectroscopy (including Raman)

High sensitivity

MonochromaticState-to-state reaction dynamics; Laser isotope separationHigh resolutionSlide20

Linewidths

: lifetime broadening

Collisional deactivation

Natural

linewidthSlide21

Linewidths: Doppler broadeningSlide22

Summary

We have discussed photon energies, molecular dynamical degrees of freedom, and spectroscopies.

We have surveyed three elements (light source, dispersing element, and detector) of spectroscopy.

We have characterized three modes of optical transitions (stimulated absorption and emission as well as spontaneous emission).

We have learned the origins of line widths.