Macalester Oct 2014

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Noisy Light Spectroscopy

A science story

Darin J. Ulness

Department of Chemistry

Concordia College, Moorhead, MN

Spectroscopy

Using light to gain information about matter

Information

• Spectra

• Transition frequencies

• Time dynamics

• Absorptivities

• Susceptibilities

Uses of information

• In Chemistry

• In Biology

• In Engineering

Modern Spectroscopy

Frequency Domain

• Measure Spectra

• Examples

• IR, UV-VIS, Raman

• Material response

• Spectrally narrow

• Temporally slow

Time Domain

• Response to light pulse

• Examples

• PE, transient abs.

• Material response

• Spectrally broad

• Temporally fast

Modern Spectroscopy

Frequency Domain

• Measure Spectra

• Examples

• IR, UV-VIS, Raman

• Material response

• Spectrally narrow

• Temporally slow

Time Domain

• Response to light pulse

• Examples

• PE, transient abs.

• Material response

• Spectrally broad

• Temporally fast

Time Domain Spectroscopy

Ultrashort pulses are used to excite a molecule

Time Domain Spectroscopy

Ultrashort pulses are used to excite a molecule

Creating Ultrashort Pulses

Fourier Transforms!

• Things that happen fast in time require a broad frequency spectrum

• To make a short pulse you need a lot of colors

Phase Locking

Synchronize the phase of the electric field

• Many colors conspire to create a short pulse

• The phases of the different colors need to be “locked”

Noisy light Spectroscopy

Unlock the phase!

• The phases of the different colors have a random relation to one another

• Many colors conspire to create a short pulse coherence time

Frequency

Time

Noisy light Spectroscopy

Interacting with molecules

• The noisy light is “always on” …it is quasi-continuous wave

• The field may interact with the molecule at any time

Foundations of Noisy Light

Noisy Light Spectroscopy

Optical coherence theory

Perturbation theory:

Density operator

Nonlinear Spectroscopy

Signal

Material

P= c

E Light field

Perturbation series approximation

P(t) = P (1) + P (2) + P (3) …

P (1) =

P (3) = c

(1) E, P (2) = c

(2) EE, c

(3) EEE

CARS

C oherent A ntiS tokes R aman S cattering w

R w

1 w

2 w

1 w

CARS w

1

w

2

= w

R w

CARS

= w

1

+ w

R

Bichromophoric Model

(3)

P

( t ) a

Noisy light b

(3) *

P ( s )

< >

Theoretical Challenges

• Complicated Mathematics

• Complicated Physical Interpretation

Difficulty

• The cw nature requires all field action permutations. The light is always on.

• The proper treatment of the noise cross-correlates chromophores.

New Viewpoint: The c

(5) Story

Theoretical Challenges

• Complicated Mathematics

• Complicated Physical Interpretation

Difficulty

• The cw nature requires all field action permutations. The light is always on.

• The proper treatment of the noise cross-correlates chromophores.

FTC Diagram Analysis

Messy integration and algebra

Set of intensity level terms

(pre-evaluated)

Construction

Rules

Set of FTC diagrams

Evaluation

Rules Set of evaluated intensity level terms easy hard hard

Physics

FTC Diagram Analysis a b

P ( t ,{ t i

})

P ( s ,{ s i

}) arrow segments : t

-dependent line segments : correlation t

-independent correlation

I (2) CARS

Computer

Monochromator

CCD

Sample

Interferometer t

B’

B

I (2) CARS

Lens

M

Narrowband

Source

Broadband

Source

• Signal is dispersed onto the CCD

• Entire Spectrum is taken at each delay

• 2D data set: the Spectrogram

-1

-2

2

1

0

18000

0.8

I (2) CARS: Data Processing

BenzeneT22

BenzeneT22

150

18100 18200 18300 18400

200

125

Fourier

100

Transformation

50

75

25

0

0 200 400 600 800 1000 1200

300 400 100

0.6

0.4

0.2

X-Marginal

-200

-400

400

200

0

I (2) CARS: Hydrogen Bonding

Pyridine Pyridine

Neat

Pyridine

400

200

0

FT

-200

-400

17300 17400 17500 17600 17300 17400 17500 ave x .45 pyr_water

400

Pyridine/

Water

X w

= 0.55

200

-200

0

-400

17300 17400 17500 17600

17600

I (2) CARS: Hydrogen Bonding

I (2) CARS: Halogen Bonding

2.5

3

3.5

4

1.5

0.5

1

2

0

900 920 940 960

Pyridine and C3F7I

980 1000

Frequency (cm-1)

1020 1040 1060 1080 1100

0.9

Neat

0.3

0.4

0.5

0.6

0.1

0.2

0.7

0.8

C6F13I and Pyridine

3.5

4

2.5

3

1.5

2

0.5

1

0

900 920 940 960 980 1000

Frequency (cm-1)

1020 1040 1060 1080 1100

0.6

0.7

0.4

0.5

.8

0.9

0.2

0.3

Neat

0.1

Halogen Bonding

Electropositve s

-hole

Test Charge

Electronegative

“belt”

Electroneutral

“ring”

Photosynthesis

Acknowledgements

Students

Theory

Jahan Dawlaty

Dan Biebighauser

John Gregiore

Duffy Turner

Kurt Haag

Issac Heath

Carena Daniels

Method Development

Pye Phyo Aung

Tanner Schulz

Lindsay Weisel

Krista Cosert

Perrie Cole

Alex Harsh

Britt Berger

Zach Johnson

Thao Ta Funding

NSF CAREER Grant CHE-0341087

Henry Dreyfus Teacher/Scholar program

Concordia Chemistry Research Fund

Hydrogen/Halogen bonding

Eric Berg

Jeff Eliason

Diane Moliva

Jason Olson

Scott Flancher

Danny Green

Photosynthesis

Becca Hendrickson

Meghan Knudtzon

Dylan Howie

Bobby Spoja

Other Group Members

Dr. Mark Gealy, Department of Physics

Dr. Eric Booth, Post-doctoral researcher

Dr. Haiyan Fan, Post-doctoral researcher

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