time-resolved fourier transform infrared spectroscopy ... · 2 outline physical processes in the ir...

papadopoulos@physik.uni-leipzig.de

Periklis Papadopoulos

Universität Leipzig, Fakultät für Physik und Geowissenschaften

Institut für Experimentelle Physik I, Abteilung "Molekülphysik“

Time-resolved Fourier Transform Infrared Spectroscopy (FTIR) in Soft Matter research

2

Outline

Physical processes in the IR spectral range

IR spectrometry

Fourier Transform Infrared Spectroscopy (FTIR)

Quantitative information from IR spectra

Effects of external fields on the molecular level

Time resolved FTIR

Chemical reactions

Conformational changes

...

3

Example: CO2 gas

Rotational – vibrational transitions

IR spectral range

-11[cm ]

4

IR spectra of condensed matter

Gases show complex vibrational-rotational spectra

In soft matter absorption bands are significantly broader

Martin Chaplin, www.physics.umd.edu

IR spectral range

H2O

CO2

5

IR spectroscopy as analytical tool

Widely used as analytical tool

Easier preparation than NMR, less quantitative

Underestimated!

IR and Raman spectroscopy are very powerful techniques

IR spectral range

6

Grating IR spectrometer

Requirements:

Well collimated beam

Monochromator

Largest part of light intensity is not used

Calibration is necessary

IR spectrometry

7

FTIR spectroscopy

Michelson interferometer

Interferogram: intensity vs optical path difference

Intensity at all wavelengths is measured simultaneously

-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)

0 0

det

0

ig

, cos 42 2

1 cos 42

I II

II d

IR spectrometry

Optical path difference for each wavelength

8

FTIR spectroscopy

Spectrum is easily obtained from the Fourier transform of the interferogram

IR spectrometry

ig 0

0

0 : 0I I d

ig

ig 0

0

ig

0

ig

0 ig

0 1cos 4

2 2

0Re

2 2

02Re

2

II I d

IF I

II F I

4000 3500 3000 2500 2000 1500 1000

0.0

0.2

0.4

0.6

0.8

1.0

Inte

nsity (

arb

. u

nits)

wavenumber (cm-1)

no sample silk

3500 3000 2500 2000 1500 1000

0

1

2

3

Ab

so

rba

nce

wavenumber (cm-1)

-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)

Fourier

transform

Division

solvent solvent

„white light“ position

9

Resolution – Apodization

Problem: impossible to integrate interferogram from - to +

Equivalent to multiplying “ideal” interferogram with a “box” function

FT of a product is the convolution of FT‘s

Resolution depends on maximum mirror path ~ Δ-1

Artefacts!

Multiplying with other functions improves quantitative accuracy, but reduces resolution

Apodization=”removing feet”

Apodizationfunction

Fourier transform of Iig(γ)

Shape ofinfinitely thin lines

IR spectrometry

( ) ( )F f g F f F g

Fourier Transform Infrared Spectrometry,P. R. Griffiths, J.A. de Haseth, Wiley

10

Advantages of FTIR

Jacquinot advantage

FTIR not as sensitive to beam misalignment, allowing for larger aperture – throughput

Fellget advantage (“multiplex”)

All frequencies measured together

Connes advantage

Built-in calibration, mirror position determined by He-Ne laser

FTIR is exclusively used nowadays

11

Transmission – reflection modes

Simplified: no interference, etc.

Transmission - absorption Specular reflection

Absorbance

Absorption coefficient α

Molar absorption coefficient ε=α/c

Lambert-Beer law:

1

0

logI

AI

1 0 0e el clI I I

ln10 ln10

l clA

Reflectivityref

0

IR

I

Normal incidence in air2

1

1

nR

n

12

Complex refractive index

The imaginary part is proportional to the absorption coefficient

Dielectric function

Real and imaginary parts are related through Kramers-Kronig relations

Example:polycarbonate

n n in

0

0

exp 2

exp 4 exp 4

4

t

t

E x E i n x

I I i n x n x

n

2

n

Fourier Transform Infrared Spectrometry,P. R. Griffiths, J.A. de Haseth, Wiley

13

Oscillations – selection rules

Covalent bonds can be described by Morse or LJ potential curves

Quantum harmonic oscillator is a good approximation

Both stretching and bending modes

Single photon is absorbed by interaction with oscillating dipole –transition dipole moment

Absorption coefficient:

No absorption normal to the transition dipole moment

IR spectral range

nmp m n d

Δn=±1Others weakly allowed, due to anharmonicity

i iq rd : dipole operator

p E

14

Polarization dependence

Example: salol crystal

All transition dipoles (for a certain transition) are perfectly aligned

Intensity of absorption bands depends greatly on crystal orientation

Dichroism: difference of absorption coefficient between two axes

Biaxiality (all three axes different)

IR spectral range

salol

Vibrational Spectroscopy in Life Science, F. Siebert, P. HildebrandtJ. Hanuza et al. / Vib. Spectrosc. 34 (2004) 253–268

15

Order parameter

Non-crystalline solids: molecules (and transition dipole moments) are not (perfectly) aligned

Rotational symmetry is common

Different absorbance A|| and A

Dichroic ratio R= A|| / A

Molecular order parameter

IR spectral range

Reference axis

Molecular segment

Transition dipole

||

2

2

3 cos 1

2

molS P

10 :

2

mol RS

R

1: 2

2 2

mol RS

R

“parallel” vibration

“perpendicular” vibration

2

2

1 2cot 2

2 2cot 1

mol RS

R

16

1050 1000 950

0.1

0.2

0.3

0.4

Po

ly(a

lanin

e)

(Ala

Gly

) n

Po

ly(g

lycin

e)

I

Ab

so

rba

nce

wavenumber (cm-1)

Po

ly(g

lycin

e)

II

Po

ly(a

lanin

e)

0°

polarization

90°

0,0

0,2

0,4

0,6

0

30

60

90

120

150

180

210

240

270

300

330

0,0

0,2

0,4

0,6

Ab

so

rba

nce

Smol

=0.25

0,0

0,2

0,4

0,6

0

30

60

90

120

150

180

210

240

270

300

330

0,0

0,2

0,4

0,6

Smol

=0.50

Ab

so

rba

nce

0,0

0,2

0,4

0,6

0

30

60

90

120

150

180

210

240

270

300

330

0,0

0,2

0,4

0,6

Smol

=0.80A

bso

rba

nce

0

2

4

0

30

60

90

120

150

180

210

240

270

300

330

0

2

4

Smol

=0.93

Ab

so

rba

nce

High order of alanine-rich crystalsLow order of glycine-rich amorphous chains

Order of crystals and amorphous phase in spider silk

Experimental

2

p E

p: transition dipole moment

Papadopoulos et al., Eur. Phys. J. E, 24, 193 (2007)Glisovic et al. Macromolecules 41, 390 (2008)

17

Examples of structural changes in soft matter

Phase transitions

liquid crystals

Conformational changes

Protein secondary structure

In many cases these processes take place very fast (< s)

Cannot be probed by X-rays or NMR

Lemieux, R. P. Acc. Chem. Res. 2001, 34, 845-853

18

Time-resolved measurements

Two possibilities:

Collect interferogram as fast as possible (“rapid scan”)

Synchronize spectrometer with external event (“step scan”)

19

Rapid scan - kinetics

Interferograms are collected successively

Time resolution down to a few ms (depending on spectral resolution)

Non-repetitive processes

Cannot average scans

noise0 1 2 3 4 5

0.0

0.2

0.4

0.6

0.8

1.0

Inte

nsity (

arb

. u

nits)

time (min)

trigger

-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)

Time-resolved FTIR

20

Irreversible processes

Rapid scan is useful for studying chemical reactions and phase transitions

Crystallization of a liquid crystal by T-jump

Synthesis of polyurethane

For faster processes:Static measurements at different spots of a flow cell

1t

2tReaction time

Time-resolved FTIR

de Haseth et al., Appl. Spectrosc., 47, 173 (1993)Takahashi et al. J. Biol. Chem. 270, 8405 (1995)

amorphous

crystal

90°C

36°C

21

Step scan

Differences from rapid scan kinetics:

Interferograms are not measured successively

Triggered event is repeated for every mirror step

Allows study of very fast processes

down to ns, ps -> chemical reactions

Lower noise than kinetics

Disadvantages:

Limited to repetitive processes

Sensitive to system instabilities

Time-resolved FTIR

22

-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)

-0.01 0.00 0.01

-0.2

-0.1

0.0

0.1

0.2

Inte

nsity (

arb

. u

nits)

Optical retardation (cm)

Step scan

Stroboscopic technique

Mirror moves stepwise

All measurements after a certain dtfrom trigger are assembled to make a single interferogram

All interferograms are collected in a single scan

One scan takes longer than rapid scan, but much higher time resolution

Time-resolved FTIR

23

Step scan

Mirror position in rapid scan and step scan

0 200 400 600 800 1000

0.0

0.2

0.4

0.6

0.8

1.0

1.2 rapid scan step scan

optical path

diffe

rence (

arb

. units)

time (arb. units)

Time-resolved FTIR

24

4000 3500 3000 2500 2000 1500 1000

0.0

0.2

0.4

0.6

0.8

1.0

Inte

nsity (

arb

. u

nits)

wavenumber (cm-1)

no sample silk (0 ms) silk (20 ms)

3500 3000 2500 2000 1500 1000

0

1

2

3

Ab

so

rba

nce

wavenumber (cm-1)

0 ms 20 ms

1000 950

0.3

0.4

0.5

0.6

Ab

so

rba

nce

wavenumber (cm-1)

0 ms 20 ms

Step scan example: spider silk

Time-resolved FTIR

25

Combined IR and mechanical spectroscopy

polarizer

IR beam

Piezo crystals –DC motors

Force sensor

IR detector

sample

Tracing microscopic effects of strain

Possible to extract order parameter dependence on external fields

Dynamic Infrared Linear Dichroism (DIRLD)

Transmission mode using microscope

Experimental

26

Preparation of Step Scan measurement

Process studied with Step Scan FTIR should be reproducible

Several cycles should be run before actual measurement

Measurement should start at this point to ensure reproducibility

Time-resolved FTIR

27

DIRLD in polymers

Dichroic ratio depends on strain

Polymer chains become better oriented

Different trend for dipole moments parallel and normal to the chain

S. Toki et al. / Polymer 41 (2000) 5423–5429I. Noda et al. / Appl. Spectrosc. 42 (1988) 203–216

Natural rubber (polyisoprene)

polystyrene

Time-resolved FTIR

28

External – crystal stress comparison: Phase

The step-scan technique allows IR measurements with high time resolution

Crystal stress can be measured as a function of time under sinusoidal external field

Phase shift < 2°

R. Ene et al. / Soft Matter, 2009, 5, 4568–4574

Time-resolved FTIR

29

What is the origin of frequency shifts?

Vibrational frequency depends on:

Atom mass

Bond force constant

Number of atoms involved in vibration

Perturbations

H-bonding

Conformation

Anharmonicity

Thermal expansion

External fields

30

C

CH3H

C

O

N

H

N

H

C

O

-1 -18 cm GPad d

pertV F r

1,4 1,6

-4,8

-4,6

Energ

y (

10

-19 J

)

r (Å)

-4,68

-4,66

hc

Quantum Perturbation Theory

The shift is ~ 0.3 %

QPT is applicable

The bond anharmonicity gives rise to the shift of energy levels

0( ) 2

0 0(1 )a r r

U U U e

0 1 2 3 4-6

-4

-2

0

2

4

En

erg

y (

10

-19 J

)

r (Å)

Morse potential

Morse potential

+

perturbation

N-C

3 eV

0.12 eV

F r 0.17 eV

dis

N CE

P. Papadopoulos et al. Eur. Phys. J. E 24, 193 (2007)

Theoretical value

31

Microscopic – macroscopic stress in silk

Crystal stress is equal to the externally applied

At time scales from µs to hours

Independent of sample history

Serial connection of crystals

0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4

961

962

963

964

965

stress (GPa)

wa

ve

nu

mb

er

(cm

-1)

Static

-2.6 cm- 1 GPa

- 1

Kinetics

Step Scan

PP, J. Sölter, F. Kremer Eur. Phys. J. E 24, 193 (2007)

32

Photoinduced protein folding

Bacteriorhodopsin structure changes after visible photon absorption

IR photons do not have enough energy to change structure, just probe vibrations!

Pulsed laser is synchronized with spectrometer

Retinal conformational changes during the complete cycle (~ms) are observed

retin

al

R. Rammelsberg et al. Appl. Spectrosc. 51, 558 (1997)

Time-resolved FTIR

33

Folding kinetics of peptides after T-jumps

Alanine-based peptide

Secondary structure depends on temperature (coil at higher T)

Reaction rate “constants“ can be studied by T-jumps

IR laser pulses synchronized with spectrometer heat the sample by ~ 10°C

The sum ku+kf is determined by kinetics, ratio ku/kf by equilibriumu

f

folded unfolded

k

k

exp u fk k t

T. Wang et al. J. Phys. Chem. B 108, 15301 (2004)

Time-resolved FTIR

34

Summary

Fourier Transform IR spectroscopy is an ideal tool to study fast processes

High sensitivity

Information for different molecular groups

High time resolution

Time resolved measurements

Rapid scan

Step scan

Effects of external perturbations in various systems:

Polymers

Proteins

Liquid crystals, ...

http://www.uni-leipzig.de/~mop/lectures

Thank you for your attention!

35

N-term. C-term.

GGXGAAAAAAAA

Repetitive pattern

GGXGGX GGX GGX GGX

n

AAAAAAA GPGXX GPGXX GPGXX GPGXX GPGXX

n

MaSp2

MaSp1

Hydrophobic Slightly hydrophilic

Chemical structure of dragline silk and PA6

Block copolymer

Two high-MW proteins (MaSp1 and MaSp2)

Semi-crystalline

High Ala- and Gly- content

PA6 (Nylon):

Spider silk

36

Normal vibrational modes

Simple relations only in diatomic molecules!

Vibrations involve more than two atoms

Especially at low frequencies

Example: amide bondC

O

N H

C

k

Amide I Amide II

Amide III Amide IV

37

Absorption spectrum of silk

Typical protein spectrum

Amide vibrations dominate, but ...

They cannot give aminoacid-specific information

The region 1100 – 900 cm-1

can be used instead

4000 3500 3000 2500 2000 1500 1000

0.0

0.5

1.0

1.5

Am

ide I

IIAm

ide I

I

Am

ide I

Ab

so

rba

nce

wavenumber (cm-1)

Am

ide A

1050 1000 950

0.2

0.3

0.4

Po

ly(a

lan

ine

)

(Ala

Gly

) n

Po

ly(g

lycin

e)

I

Ab

so

rba

nce

wavenumber (cm-1)

Po

ly(g

lycin

e)

II

Experimental

38

Poly(alanine) segment

Rotondi, K. S.; Gierasch, L. M. Biopolymers 2005, 84, 13-22.

Simmons, A.; Ray, E.; Jelinski, L. W. Macromolecules 1994, 27, 5235-5237.

C-terminus

N-terminus

N-terminus

C-terminus

N-terminus

N-terminus

C-terminus

C-terminus

N C

NC

N C

N C

Antiparallel and parallel b-sheet structure

39

3500 3250 3000 2750 2500 2250 2000 1750 1500 1250 1000 750

0,0

0,3

0,6

0,9

1,2

0,0

0,5

1,0

1,5

b-polyalanine

wavenumber (cm-1)

Abso

rba

nce

Am

ide III

Am

ide II

Am

ide I

Am

ide B MA silk

||

Abso

rptio

n c

oe

ffic

ien

t

(m

-1) A

mid

e A

Polyaminoacid IR spectra

Dragline silk and b-polyalanine

A. M. Dwivedi, S. Krimm Macromolecules 15, 186 (1982)

40

Similar findings in PA6

Similar to silk, orientation beforecrystallization induces the high order

3500 3000 2500 2000 1500 1000

0.000

0.005

0.010

0.015C-N

C=O

CH2

Absorb

an

ce

wavenumber / cm-1

//

N-H

Crystal vibration responds

linearly to applied stress

Both spider silk and PA6 are

glassy at room temperature