Raman spectroscopy: Variants and potentials...Normal coordinate analysis Time-resolved Raman...
Transcript of Raman spectroscopy: Variants and potentials...Normal coordinate analysis Time-resolved Raman...
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2013.10.8
Carl-Zeiss lecture
Jena
Raman spectroscopy: Variants and potentials
Hiro-o Hamaguchi
National Chiao Tung University, Taiwan
The University of Tokyo, Japan
Wseda University, Japan
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Raman spectroscopy: Variants and potentials
○ Raman brothers, Raman, CARS/SRS, and SERS/TERS What do they look at? Hamaguchi’s score sheet for Raman brothers
○ Raman spectroscopy in Japan Discovery of rotational isomerism Normal coordinate analysis
○ Time-resolved Raman spectroscopy Dynamic polarization model of chemical reactions
○ Raman microsepctroscopy of living cells
○ Tailor-made Raman spectroscopy
16
14
12
10
8
6
4
Y /
µm
1612840
X / µm
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Anti-Stokes Raman Rayleigh Stokes Raman
Raman scattering:
Inelastic light scattering discovered by C. V. Raman in 1928
Raman spectroscopy:
Spectroscopy utilizing Raman scattering
Raman Spectroscopy
C. V. Raman (1888-1970)
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Raman
CARS
SERS/
TERS
Raman Brothers: What do they look at?
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Normal Mode of Vibration:
The Totally Symmetric C-C Stretch Mode of
an Acetone Molecule
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Vibrational Motions of Ensembles of Acetone Molecules
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What Does Raman look at?
p = aE
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Raman Looks at a Normal Mode of Vibration.
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http://dailynewsagency.com
Raman Gives a Molecular Fingerprint.
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What Does CARS/SRS Look at?
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CARS/SRS Looks at a Vibrational Coherence
p = cE12E2
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CARS Can Give a Molecular Fingerprint After Some Mathematical Treatments.
Okuno et al. Angewandte Chemie, Angew. Chem. Int. Ed., 49, 6773-6777 (2010).
CARS spectra
Imc3 spectra by
MEM
Imc3 spectra after
SVD
Raman spectra
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Vibrational Motions of Ensembles of Acetone Molecules
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What Does SERS/TERS Look at?
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SERS/TERS is Likely to Look at a Local Molecular Motion (May not be a Normal Mode)
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http://dailynewsagency.com
SERS/TERS May not Give a Full Molecular Fingerprint.
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Raman CARS/SRS SERS/TERS
Selection rule Established Established for homogeneous
systems
Dependence on individual molecular
orientation?
Polarization rule Established
Established for homogeneous
systems High polarization
capabilities
Dependence on individual molecular
orientation?
Information content Molecular Fingerprint
Molecular fingerprint after
mathematics
Molecular Fingerprint?
Sensitivity Ensemble Ensemble Single molecule
Spatial resolution 0.61l/NA (500 nm)
0.61l/NA√3 (300 nm)
Tip size (10 nm)
Time resolution ps ps ps
Experimental difficulty
Fluorescence interference
Phase match/mismatch
Tip/substrate dependence
Hamaguchi’s Score Sheet for Ramans
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○ Raman is HH’s first choice for advanced applications.
○ CARS/SRS surpasses Raman for its polarization capabilities.
○ SERS/TERS excels in sensitivity and spatial resolution. Its information content yet to be clarified.
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Raman Spectroscopy atTokyo
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Discovery of the Rotational Isomerism
Gas
Liquid
Crystal
S. Mizushima (1899-1983)
Trans Gauche
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Raman Spectra are letters from the
molecule
Professor Takehiko Shimanouchi (1916-1980)
Vibrational Ramanspectra are molecular
fingerprints
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T. Shimanouchi, Tables of Molecular Vibrational Frequencies, NSRDS-NBS 39.
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High Resolution Raman Spectrometer (1972)
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Raman Gas Cell in Laser Cavity (1972)
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Raman Spectrum of CH3I (1972)
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Resonance Raman scattering
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Theory of Resonance Raman Scattering
Albrecht’s vibronic theory of resonance Raman Scattering
ars ~ A + B
A term: Franck-Condon term
Totally symmetric modes
High overtones
B term: Vibronic coupling
Non-totally symmetric modes
No high overtones
A. C. Albrecht (1927-2002)
A. C. Albrecht, J. Chem. Phys. 34, 1476 (1961).
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n1 (a1g)
n2 (eg)
n5 (t2g)
r=0.75 r=0.75 r=0
1 0 0 0 1 0 0 0 1
1 0 0 0 -1 0 0 0 0
0 1 0 1 0 0 0 0 0
a1g ~ eg ~ t2g ~
Raman Active Vibrations of MX6 Octahedral Complexes
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Resonance Raman spectrum of PtI62-
Totally symmetric mode (n1, 2n1, 3n1) → A term Non-totally symmetric mode ( n2, 2n2, n1+n2, 2n1+n2 ) → B term
PtI62-
488.0 nm excitation
H. Hamaguchi, I. Harada, T. Shimanouch, J. Raman Spectrosc., 2, 517-528 (1974).
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Polarized Resonance Raman Spectra of PtI62-
PtI62-
488.0 nm excitation
n1, 2n1, 3n1 bands r=0 ; n2 band r=0.75
H. Hamaguchi, J. Chem. Phys., 69, 569-578 (1978).
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IrBr62-
568.2 nm excitation
r=1 for all bands;
H. Hamaguchi, J. Chem. Phys., 66, 5757-5768 (1977); 69, 569-578 (1978).
Polarized Resonance Raman Spectra of IrBr62-
forgot to rotate the analyzer?
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|g(a)> |g(a)> 1 i 0 -i 1 0 0 0 1
0 0 -i 0 0 -1 i 1 0
0 0 -i 0 0 1 i -1 0
1 -i 0 i 1 0 0 0 1
|g(a)> |g(b)>
|g(b)> |g(a)>
|g(b)> |g(b)>
G0=3, Ga=2, Gs=0
G0=0, Ga=4, Gs=0
G0=3, Ga=2, Gs=0
G0=0, Ga=4, Gs=0
G0=6, Ga=12, Gs=0 r=(3Gs+5Ga)/(10G0+4Gs)=1 H. Hamaguchi, J. Chem. Phys., 66, 5757-5768 (1977).
Raman Scattering Tensors and Depolarization ratio of the Totally Symmetric Mode of the IrBr6
2- Ion
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(1985)
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Nanosecond Transient Raman Spectrometer (1983)
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Photoisomerization of Trans-Stilbene
Probe solvent dependent structure and dynamics of S1 trans-stilbene by time-resolved Raman spectroscopy
hn Solvent-dependent isomerization rate
Hexane 70 ps
Dodecane 120 ps
Why, when and how rotation occurs in the excited state?
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Nanosecond Transient Raman Spectrum of S1 Trans-Stilbene (1983)
T. L. Gustafson, D. M. Roberts, and D. A. Chernoff, J. Chem. Phys. 79, 1559 (1983). H. Hamaguchi, C. Kato, M. Tasumi, Chem. Phys. Lett., 100, 3-7 (1983).
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Three Raman Stilbenists on a Bridge near the Noishvanstein Castle (1985)
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(1987)
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Koichi Iwata Volker Deckert
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cw Nd:YAG regenerative amplifier
cw mode-locked Nd:YAG laser
pulse compressor dye laser
SHG
optical delay
sample
multichannel detector (CCD)
pump
probe
SHG
polychromator
sync. pumped
band-reject filter
variable ND
UV cut filter
dichroic mirror
dichroic mirror
SHG
PD
82 MHz 588 nm
amplifier
dye AO
S0
Sn
S1 294 nm 2.2 ps
294 nm 2.2 ps
3.2 ps 588 nm
3.5 cm-1
3.2 ps 588 nm
3.5 cm-1
Trans-Stilbene
Picosecond Time-resolved Raman Spectrometer
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S1 trans-Stilbene in CHCl3
1700 1600 1500 1400 1300 1200 1100
Raman Shift / cm-1
2 ps
20 ps
100 ps
-1 ps
0 ps
10 ps
7 ps
3 ps
30 ps
70 ps
-2 ps
50 ps
5 ps
1 ps
15 ps
40 ps
-10 ps Pump 294 nm Probe 588 nm (0.1 mW)
C=C stretch vibration
1560 cm-1: double bond
Why rotation occurs
around a double bond ?
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1620 1600 1580 1560 1540 1520
Raman Shift / cm-1
Hexane
Decane
Nonane
Octane
Heptane
Hexadecane
Dodecane
Fig. 7 H. Hamaguchi and K. Iwata
The C=C Stretch Raman Band of S1 trans-Stilbene in Alkanes
The peak position shifts to higher wavenumbers and the band width decreases on going from hexane to hexadecane. Why?
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1574
1572
1570
1568
Peak p
ositio
n /
cm
-1
22 21 20 19 18 17
Bandwidth / cm -1
hexane
octane
decane
Peak Position vs Band Width in Alakne Solvents at Different Temperatures
Why does linear Relation hold?
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(c) Continuous Frequency Modulation Model
(b) Many Frequency Exchange Model
(a) Two Frequency Exchange Model
DW = W1t/(1+t2) DG = W1t2/(1+t2)
DG / DW = t
),1/()/(2
1
2
11
tt +=DW =
WWWn
),1/()/(22
1
2
11
tt +=DG =
WWWn
+
=DW0
02
1
)(
)1/()(
tt
tttt
dG
dGW
+
=DG0
022
1
)(
)1/()(
tt
tttt
dG
dGW
DG / DW = t1/2 ; G(t)=exp(-ln2t2/t1/22)
Dynamic Frequency Exchange Model and Vibrational Bandshapes
Hamaguchi Mol. Phys.89, 463 (1997).
W 1
W 2
W 1
W 2
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1574
1572
1570
1568
Peak p
ositio
n /
cm
-1
22 21 20 19 18 17
Bandwidth / cm -1
hexane
octane
decane
Peak Position vs Band Width in Alakne Solvents at Different Temperatures
DW = W1t/(1+t2) DG = W1t
2/(1+t2)
DG / DW = t
t =1.4
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1640 1600 1560 1520 1480
Raman shift / cm-1
Dodecane
Hexane Obs Fit
Fig. 10 H. Hamaguchi and K. Iwata
Fitting of the observed band shapes
Fitting of the C=C Stretch Raman Band of S1 trans-Stilbene by the Two Frequency Exchange Model
W1=2.7x1012 sec-1 (370 (fs)-1)
W1=1.5x1012 sec-1 (670 (fs)-1)
W 1
W 2
W 1
W 2
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0
1
2
3
4
5
DW
/ c
m-1
20x10 9
15 10 5 0 k
iso / s -1
283 K
293 K
298 K
303 K
313 K
Isomerization Rate kiso is Proportional to W1
1x1012
W1
/ s-1
DW = W1t/(1+t2)
t =1.4
DW =0
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Isomeri-zation
W1
W2
Dynamic Polarization Model of Isomerization
Hamaguchi, Iwata, CPL 208, 465 (1993).
Deckert, Iwata, Hamaguchi, J. Photochem. Photobiol. 102, 35 (1996).
Iwata, Ozawa, Hamaguchi, JCP 106, 3614 (2002).
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How Do Chemical Reactions Proceed?
A
A* B
A A* B
Cf. Michaelis-Menten kinetics
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“How can the events in space and time
which take place within the spatial boundary of a living organism be
accounted for by physics and chemistry ?”
In “What is Life”
Erwin Schrödinger
E. Schrödinger (1887-1961)
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1500 1000 500
Wavenumber / cm-1
0min
11min
31min
41min
62min
72min
6min
24min
53min
69min
Raman Spectroscopy of Really Living Cell
Y-S Huang, T. Karashima, M. Yamamoto, H. Hamaguchi, J. Raman Spectrosc., 34, 1-3 (2003).
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Page 54
white blood cell
Thorough interpretation of complicated
spectra is very difficult.
Molecular Component Distribution Imaging (MCDI) of Living Cells with Multivariate Curve Resolution
Analysis
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Multivariate Analysis Matrix factorization by
Singular Value Decomposition (SVD)
A ≈ WSH n
m m
n
n
4
6
810
3
2
4
6
810
4
2
4
6
8
Sin
gu
lar
va
lue
20151050
10
8
6
4
2
0
1086420
10
8
6
4
2
0
1086420
10
8
6
4
2
0
1086420
10
8
6
4
2
0
1086420
10
8
6
4
2
0
1086420
10
8
6
4
2
0
1086420
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4
6
810
3
2
4
6
810
4
2
4
6
8
Sin
gu
lar
va
lue
20151050
Multivariate Curve Resolution (MCR)
Page 56
n
… m
n
m
k
k is determined
Random SVD based
Initial guess
or
Alternating Least-Squares
||A – WH||2
is minimized
SVD
1
2
3
4
5
6
1
2
3
4
5
6
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Multivariate Analyses: Comparison
SVD MCR
W, H ≥ 0 , L1 = 0
MCR
W, H ≥ 0 , L1 = 0.001
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White Blood Cells 5分類
Neutrophil 50-70 % 10-12 μm Phagocytosis
- bacteria, fungi
Eosinophil 2-5 % 10-12 μm Combating parasites
Modulate allergic
inflammatory responses
Basophil < 1 % 12-15 μm release histamine for
inflammatory responses
Lymphocyte 20-40 % 7-8 μm B cells
T cells
NK cells
Monocyte 3-6 % 14-17 μm Differentiate into tissue
resident macrophages
Page 58
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MCR Analysis of White Blood Cells
Neutrophil
Eosinophil
Lymphocyte
Monocyte
Page 59
1500 1000 500
Raman shift / cm-1
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MCDI of White Blood Cells
Neutrophil
Eosinophil
Lymphocyte
Monocyte
Page 60
nucleic acid protein
protein
background
lipid
(unsaturated)
carotenoid
Myeloperoxidase (MPO)
Eosinophil
peroxidase
(EPO)
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Organelle Specific Waters in a Living Cell
(a) (b) (c) (d) (e)
3800360034003200
(a)
(e)
S. Tiwari, M. Andoa and H. Hamaguchi, in preparation
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Broadband Multiplex CARS Microspectroscopy
w2
w1
wCARS
w1
Dw1=20cm-1
n=0
n=1
w1 pulse w2 pulse
w1 100~200pJ w2 ~30pJ
H. Kano and H. Hamaguchi, Anal. Chem., 79, 8967-8973 (2007).
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w1: 10 mW, w2: 10 mW
Expo. time/pixel: 30 msec
Image acquisition time: ~ 12 sec
Vibrational CARS Movies of a Single Budding Yeast Cell
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Multi-focus Confocal Raman Microspectroscopy
M. Okuno and H. Hamaguchi, Opt. Lett., 35, 4096-4098 (2010).
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Budding yeast cells
16
14
12
10
8
6
4
Y /
µm
1612840
X / µm
16
14
12
10
8
6
4Y
/ µ
m
1612840
X / µm
16
14
12
10
8
6
4
Y /
µm
1612840
X / µm
16
14
12
10
8
6
4
Y /
µm
1612840
X / µm
Exposure time: 1 sec
Readout time: ~150 msec
PZT scan 4 x 4 points
2 x 2 mm
Total image acquisition time
(1 sec+ 0.2 sec) x 4 x 4
~20 sec / image !!
Laser power : 1 mW
Total area: 16 x 12 mm
1655 cm-1 1602 cm-1
1584 cm-1 1440 cm-1
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Organ
Cell
Organelle
Liposome
Solvation structure
Complex
Aggregate
Molecule
Atom
Biology
Chemistry
Time Space
109 s
103 s
102 s
10-10 s
10-12 s
10-15 s
10 cm
10 mm
1 mm
10 nm
1 nm
0.1 nm
Ionic liquid
Tim
e/Sp
ace
-res
olv
ed R
aman
Sp
ectr
osc
op
y
Physics
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Raman Measurement of Food in situ
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Raman Application to Food Science
Natural or cultured food resources
Food processing
Food safety & quality control:
Food constituent Functional ingredient Contamination of pathogens or
residual pesticides
Label-free, less invasive and rapid analysis by using Raman spectroscopy
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Raman Spectra of Tuna
Page 69
3000
2500
2000
1500
1000
500
0
Inte
nsi
ty /
a.u
.
3000 2000 1000
Raman shift / cm-1
Quantification of lipids / proteins
⇒ evaluation of food quality and taste
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Lipid Content Analysis of Tuna
Page 70
16
14
12
10
8
6
4
2
0
Inte
nsi
ty r
atio
(lip
id/pr
ote
in)
lean chutoro otoro
16
14
12
10
8
6
4
2
0
Inte
nsi
ty r
atio
(lip
id/pr
ote
in)
Tail (chutoro)
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First Student Summer Camp of Taiwan Association of Raman Spectroscopy (2013.7.6 at Jianshi)