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MAE 649 Microscopy and Spectroscopy of Materials
Chapter 5 Fourier Transform Infrared Spectroscopy
What is light ?-- Electromagnetic Radiation Dual nature of light: – Photons as particle: Photons have energy but no mass – Photons as wave: Electric and magnetic fields oscillating in space and time
(FTIR)
Chapter 5- Fourier Transform Infrared Spectroscopy
Electromagnetic Radiation
Contents: • light - electromagnetic wave
• Radiation is absorbed & emitted in photons. The defining characteristic of a photon is that its energy cannot be split into smaller pieces.
• molecular effects of infrared adsorption -- molecular vibration -- dipole change
• Each photon’s energy is defined by its frequency (ν) or wave length (λ) or wave number ( )
• interpretation of IR spectra • Instrumentation and sampling techniques -- transmission spectroscopy -- attenuated total reflection (ATR) -- diffuse reflection -- Polarization modulation infrared reflection adsorption spectroscopy (PM-IRRAS) • Raman spectroscopy
• Ephoton = hν = hc/λ = hc h = Planck’s constant, 6.63 x 10-34 J s c = speed of light, 3.00 x 108 m s-1 (or 3.00 x 1010 cm s-1) Wavenumber, = 1/λ • Energy unit Wavelength (λ): Frequency (ν): Wavenumber:
meter or micron Hz (cycl/s) cm-1
1 eV = 8065.54 cm-1 = 96.4853 kJ/mol = 23.0605 kcal/mol
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Light - Electromagnetic wave spectrum
Electromagnetic spectrum and molecular effects Atoms and molecules can absorb electromagnetic radiation, but only at certain energies (wavelengths).
Adsorption of radiation by molecules
http://www.wag.caltech.edu/home/jang/genchem/infrared.htm
Electromagnetic spectrum and molecular effects
Electromagnetic Radiation-infrared
Infrared (IR) absorbed by organic molecules: – Just below red in the visible region – IR range: 400-4000 cm-1 (wavelengths 25-2.5 m) – Photon energy = 0.8-8.0 x 10-20 J – Molar photon energy = 4.9-49 kJ/mol = 1.2-12 kcal/mol IR photon energy << covalent bond energy. Absorbing IR radiation should not trigger substantial chemical changes. But IR radiation contains more energy than random thermal motion at room temperature (~ 0.6 kcal/mol)
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Infrared Regime
Molecular effects of infrared adsorption
It is useful to divide the infra red region into three sections; near, mid and far infra red
Region
Wavelength range (m)
Wavenumber range (cm-1)
1) IR radiation does not have enough energy to induce electronic transitions as seen with UV. Absorption of IR is restricted to compounds with small energy differences in the possible vibrational states.
Near
0.78 - 2.5
12800 - 4000
2) For a molecule to absorb IR, the vibrations within a molecule must cause a net change in the dipole moment of the molecule.
Middle
2.5 - 25
4000 - 500
3) The alternating electrical field of the radiation interacts with fluctuations in the dipole moment of the molecule.
Far
25 -1000
400 - 10
4) If the frequency of the radiation matches the vibrational frequency of the molecule (resonance), radiation will be absorbed, causing a change in the amplitude of molecular vibration.
Molecular effects of infrared adsorption Molecular rotations Rotational transitions are of little use to the spectroscopist. Rotational levels are quantized, and absorption of IR by gases yields line spectra. However, in liquids or solids, these lines broaden into a continuum due to molecular collisions and other interactions.
Molecular vibration induced by IR adsorption Molecular vibrations The positions of atoms in a molecules are not fixed; they are subject to a number of different vibrations. Vibrations fall into the two main categories of stretching and bending. Stretching: Change in inter-atomic distance along bond axis
Molecular vibrations The positions of atoms in a molecules are not fixed; they are subject to a number of different vibrations. Vibrations fall into the two main categories: stretching and bending.
Asymmetric stretching
Symmetric stretching http://en.wikipedia.org/wiki/Infrared_spectroscopy
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Molecular vibration induced by IR adsorption Bending: Change in angle between two bonds. There are four types of bend: • Rocking • Scissoring • Wagging • Twisting
In-plane scissoring
Molecular vibration induced by IR adsorption The stretching frequency of a bond can be approximated by Hooke’s Law. Two atoms and the connecting bond are treated as a simple harmonic oscillator composed of 2 masses (atoms) joined by a spring: According to Hooke’s law, the vibration frequency of the spring is is expressed by:
In-plane rocking
where k is the force constant, m is the mass, ν is the vibration frequency
out-plane wagging
out-plane twisting
In the classical harmonic oscillator, E = 1/2kx2= hν, where x is the displacement of the spring. Thus, the energy or frequency is dependent on how far one stretches or compresses the spring, which can be any value. If this simple model were true, a molecule could absorb energy of any wavelength.
http://en.wikipedia.org/wiki/Infrared_spectroscopy
Molecular vibration induced by IR adsorption
Molecular vibration induced by IR adsorption
How much movement occurs in the vibration of a C-C bond?
However, vibrational motion is quantized during IR adsorption. It must follow the rules of quantum mechanics to fit the following formula: E = (n + 1/2)hν
154 pm
10 pm
For a C-C bond with a bond length of 154 pm, the variation is about 10 pm.
where ν is the vibration frequency, n is the quantum number (0, 1, 2, 3, . . . ). The lowest energy level is E0 = 1/2 hν, the next highest is E1 = 3/2 hν. According to the selection rule, only transitions to the next energy level are allowed. These correspond to bands called overtones in an IR spectrum.
stretching vibration
4o
10 pm
bending vibration
For C-C-C bond angle a change of 4o is typical. This moves a carbon atom about 10 pm. Energy curve for a vibrating spring (left) and energy constrained to quantum mechanical model (right).
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Molecular vibration induced by IR adsorption
Molecular vibration induced by IR adsorption
A molecule is not just two atoms joined on a spring, of course. A bond can come apart, and it cannot be compressed beyond a certain point. A molecule is actually an anharmonic oscillator. As the interatomic distance increases, the energy reaches a maximum, as seen in Figure. Note how the energy levels become more closely spaced with increasing interatomic distance in the anharmonic oscillator. The allowed transitions, hν, become smaller in energy. Therefore, overtones can be lower in energy than predicted by the harmonic oscillator theory.
Energy curve for an anharmonic oscillator, showing the vibrational levels for a vibrating bond.
• Frequency decreases with increasing atomic weight. • Frequency increases with increasing bond energy • Stretching > Bending > Wagging/Twisting
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
Molecular vibration induced by IR adsorption The following formula has been derived from Hooke’s law. For the case of a diatomic molecule, recall: f m1
m2
Molecular vibration induced by IR adsorption Coupling effects 1) Although a useful approximation, the motion of two atoms in a large molecule cannot be isolated from the motion of the rest of the atoms in the molecule. 2) In a molecule, two oscillating bonds can share a common atom.
where is the wavenumber (cm–1), m1 and m2 are the mass of atoms 1 and 2, respectively, c is the velocity of light (cm/s), f is the force constant of the bond (dyne/cm)
3) When this happens, the vibrations of the two bonds are coupled. 4) As one bond contracts, the other bond can either contract or expand, as in asymmetrical and symmetrical stretching.
Equation shows the relationship of bond strength and atomic mass to the wavenumber (vibration frequency) at which a molecule will absorb IR radiation. As the force constant increases, the wavenumber increases.
5) In general, when coupling occurs, bands at different frequencies are observed
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Correlation of Quantized Absorptions
Dipole movement induced by IR adsorption
Group
Bond
Wavenumber (cm-1)
Alcohol
OH
3200 - 3640 3300 - 3500
Amine
NH
Alkyne
sp CH
3300
Aromatic
aryl CH
3000 - 3100
Alkenes
sp2 CH
3020 - 3080
Alkanes
sp3 CH
2850 - 2960
Aldehydic
Dipole change
O
C
H
2750
Nitriles
CN
Alkyne
CC
2250 2200
Carbonyl
C=O
1650 - 1800
Alkene
C=C
1600
Amino
CN
1200
Ether
CO
1100
Chloro
CCl
550 - 780
Bromo
CBr
510 - 650
Iodo
CI
485 - 600
• Before the IR beam and molecule interact, the H-Cl molecule is at rest. After the interaction, the photon has been absorbed, and its energy deposited into the H-Cl molecule as bond stretching motion. Energy is conserved in the reaction since all the photon’s energy has been transferred to the molecule as vibrational energy. • We detect the absorbance of the photon by a decrease in infrared intensity at the wavenumber of the light absorbed, giving an absorption feature in the IR spectrum of the molecule due to the dipole moment.
http://www.chem.indiana.edu/academics/ugrad/Courses/c343/lecture.asp
Molecular vibration induced by IR adsorption
Molecular effects of infrared adsorption Dipole change
• IR Absorption is quantized Different bonds absorb different units of energy Absorption reported in wavenumbers (cm-1) • Uses infrared light to excite bonds Light is absorbed by functional group and group vibrates
Dipole change
From O. Chiantore
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Molecular effect of IR adsorption
Quantification of Infrared Adsorption
Dipole change • Only vibrational modes that change the dipole moment can interact with light and lead to absorption • CO2 is infrared active, but not all of its modes are
Selection rule for infrared spectroscopy prerequisites for Infrared active That is, the molecules can interact with light and lead to infrared absorption only when all the following requirements are met:
Acquisition of infrared spectra Format of IR spectra Transmission spectrum
1) The frequency of the infrared light must be identical to the frequency of the vibration (resonance). Absorption is quantized, Different bonds absorb different units of E
Wavenumber (cm-1)
2) The dipole of the molecule must change during vibration. 3) The direction of the dipole change must be the same as the direction of the electric filed vector.
Adsorption spectrum
Wavenumber (cm-1)
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Infrared Spectra of materials
Interpretation of infrared spectra
1) Single-bond regime: assign peaks between 3300 and 2800 cm-1 2) Double bond regime (1750-1500 cm-1) 3) Triple bond regime (2300-2100 cm-1) 4) identify major peaks in the finger print region (1500-600 cm-1), each type of compound has characteristic peaks Many bands & many overlaps – Heavy atom stretches. 4) use IR database http://en.wikipedia.org/wiki/Infrared_spectroscopy
Adsorption bands in IR spectra
Interpretation of infrared spectra Where to Begin Interpretation • Find C-H stretches as your starting point • C-H absorb ≈ 2850-3000 cm-1
Stretching and bending vibrational modes for a CH2 group, Leading to the bands (peaks) in the IR spectrum
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Interpretation of infrared spectra Aromatics
* C–H stretch from 3100-3000 cm-1 * overtones, weak, from 2000-1665 cm-1 * C–C stretch (in-ring) from 1600-1585 cm-1 * C–C stretch (in-ring) from 1500-1400 cm-1 * C–H "oop" from 900-675 cm-1
Interpretation of infrared spectra Ether O
C-O absorb ≈ 1100 cm-1
Distinguish Between Alcohol and Ether
C-O absorption weak to medium intensity
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
Interpretation of infrared spectra Alcohols (-OH)
• O–H stretch, hydrogen bonded 3500-3200 cm-1 -- broad lump peak • C–O stretch 1260-1050 cm-1 (s)
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
Interpretation of infrared spectra Ketone: carbonyl band C=O • aliphatic ketones: 1715 cm-1 • α, β-unsaturated ketones: 1685-1666 cm-1
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
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Interpretation of infrared spectra
Interpretation of infrared spectra Nitro compounds: N-O
Ketone: carbonyl band C=O • aliphatic ketones 1715 cm-1 • α, β-unsaturated ketones 1685-1666 cm-1
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
Interpretation of infrared spectra Primary amine: R-NH2 • N–H: two bands from 3400-3300 and 3330-3250 cm-1 • N–H bend from 1650-1580 cm-1 • C–N stretch (aromatic amines) from 1335-1250 cm-1 • C–N stretch (aliphatic amines) from 1250–1020 cm-1 • N–H wag (primary and secondary amines only) from 910-665 cm-1
• N–O asymmetric stretch from 1550-1475 cm-1 • N–O symmetric stretch from 1360-1290 cm-1
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
Interpretation of infrared spectra Halogens are Heavy, thus in the low wavenumber range Cl
C-Cl absorb ≈ 550-780 cm-1
C-Cl absorption weak to medium intensity
http://orgchem.colorado.edu/hndbksupport/irtutor/tutorial.html
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Database of infrared spectra Books • Hummel D.O., Scholl, F Atlas of polymer and plastic additives, vol 1-3 VCH Publisher, Weinheim, 1991 • Pouchert, C.J. The Aldrich Library of IR Spectra, Aldrich Chemical, Milwaukee, 1981 • Merck E, Merk FTIR Atlas, VCH verlagges, Weinheim, 1988 • Simons, W. W,. The Sadtler Collection of IR Spectra Sadtler, Philadelphia, 1978
FTIR quantitative analysis Limitations to Beer’s law
Is the absorbance really linear with respect to the variables? Path Length: Essentially this is always found to be linear. Concentration: Intermolecular interactions Shifting chemical equilibrium
Electronic database Bio-Rad IR Databases, Bio-Rad's Informatics Division NIST database http://webbook.nist.gov/chemistry/
FTIR quantitative analysis
Molar absorptivity: Solution’s index of refraction Also, there are a number of ways that an instrument can itself skew the behavior away from linearity
FTIR quantitative analysis
Beer-Lambert or Beer’s Law: A straightforward study of the absorption process of photons passing through an absorbing medium The intensities of the peaks are directly related to the amount of sample present
intensity
This is a spectroscopic experiment because ε depends upon the wavelength of light employed. Hence, the absorbance is wavelength dependent. Absorbance adds in a multicomponent system – assuming the various components do not interact. Transmittance is the directly measured property but absorbance is directly related to concentration.
concentration
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Summary of FTIR Advantages of FTIR: • FTIR is an ambient technique. The instrument is relatively inexpensive • A universal technique, i.e., solids, liquids, gases, and powders can be routinely analyzed. • IR spectra are information rich; peak positions, intensities, widths, and shapes in a spectrum all give useful information about the analyte. • IR is relatively fast and easy technique. Most samples can be prepared and scanned in less than five minutes. • IR is very sensitive. Micro to nano gram quantities can routinely be detected. Disadvantages of FTIR: • Homonuclear compounds don’t absorb. • Aqueous solutions difficult to analyze because the strong absorbance of water. • Some compounds give broad bands that interfere with other compounds. • Complex mixtures difficult. • Dark (black) compounds often absorb the IR beam completely, i.e., 0% transmittance.
Project timeline • Every student will independently accomplish the report of the project at first. • Every student will turn in the project report on November 16, 11:00am (firm deadline!). • From November 16 to November 27, the students in the same group will work together to make the slides for a common presentation for each group. • On November 28, 11:00am, every group will turn in the electronic file of the presentation. After you turn in the presentation file, you will not be allowed to make any change of your slides. • On November 28 and 30, the groups will make presentation (the duration time for presentation is 18 minutes. Your talk can not be less than 17 minutes, but can not exceed 18 minutes). One student will be selected by each group to make the presentation on behalf of the group.
How to analyze the sample from a car accident
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MAE 649 Microscopy and Spectroscopy of Materials
FTIR instrumentation
Chapter 5 Fourier Transform Infrared Spectroscopy
(FTIR)
Fourier Transform infrared (FTIR) system
Chapter 5- Fourier Transform Infrared Spectroscopy
http://www.forumsci.co.il/HPLC/FTIR_page.html
FTIR instrumentation
Contents: • light - electromagnetic wave • molecular effects of infrared adsorption -- molecular vibration -- dipole change • interpretation of IR spectra • Instrumentation and sampling techniques -- attenuated total reflection (ATR) -- diffuse reflection -- Polarization modulation infrared reflection adsorption spectroscopy (PM-IRRAS) • Raman spectroscopy
Fourier Transform infrared (FTIR) system
http://www.forumsci.co.il/HPLC/FTIR_page.html
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FTIR instrumentation An interferogram is generated because of the unique optics of an FT-IR instrument. The key components are a moveable mirror and beam splitter. The moveable mirror is responsible for the quality of the interferogram, and it is very important to move the mirror at constant speed. The moveable mirror is often the most expensive component of an FT-IR spectrometer.
moving mirror detector
fixed mirror
FTIR instrumentation
beam splitter
IR source
animation of FTIR
A Fourier transform is a mathematical operation used to translate a complex curve into its component curves. The complex curve is an interferogram generated by overlapping light waves, The standard infrared spectrum is calculated from the Fourier-transformed interferogram, giving a spectrum in percent transmittance (%T) vs. light frequency (cm-1) http://www.infrared-analysis.com/info1.htm
FTIR instrumentation
FTIR sampling techniques
1) transmission 2) attenuated total reflection (ATR) 3) Specular reflectance 4) Diffuse reflectance 5) -- DRIFTS (diffuse reflectance Fourier transform spectroscopy) 6) PM-IRRAS (polarization modulation infrared reflection adsorption spectroscopy) 7) portable FTIR (optical fiber)
(ATR)
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FTIR sampling technique -transmission
Powder preparation procedure: (a) The powder sample and KBr must be ground to reduce the particle size to less than 5 mm in diameter. Otherwise, large particles scatter the infrared beam and cause a slope baseline of spectrum. (b) Add a spatula full of KBr into an agate mortar and grind it to fine powder until crystallites can no longer be seen and it becomes somewhat “pasty” and sticks to the mortar. (c), (d) (e) shown in Figure
FTIR sampling technique -ATR Attenuated total reflection (ATR) infrared spectroscopy:
A choice on sampling technique exists for the following types of samples: • solid powder (mixed with KBr) • thin solid films (black samples excluded) • liquid (no water involved) • gas
At each reflection, the light beam penetrates the sample to a depth of a few microns and is absorbed at the characteristic absorption frequencies. Zinc Selenide (ZnSe) crystal is most commonly used for ATR accessory.
FTIR transmission measurement
Evanescent wave: • The defining feature of ATR spectroscopy is the presence of an evanescent wave. The evanescent wave is a special type of electromagnetic radiation • It is present only in the regime of supercritical internal reflection • It propagates parallel to the interface Kit for pressing powder samples
FTIR sampling technique -transmission
• Its intensity decreases exponentially with the distance from the sampling surface of IRE
FTIR sampling technique -ATR
Liquid samples liquid drop
IR transparent disc
liquid or gas samples Penetration depth • Its penetration depth is on the order of wavelength • Intensity of Evanescent wave decreases exponentially with the distance IR
• The penetration depth is a function of experimental parameters, for example, it is dependent upon the sample material
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FTIR sampling technique -ATR The penetration depth d is defined as the distance form the crystal-sample interface where the intensity of the evanescent decays to 1/e (37%) of its original value. It can be given by:
FTIR sampling technique -ATR Attenuated total reflection infrared (ATR-IR) spectroscopy: • for thick films or bulk lump material with smooth surface • for materials which are either too thick or too strong absorbing to be analyzed by transmission spectroscopy. • liquid samples • no sample preparation is required for ATR analysis.
Where is the wavelength of the IR radiation. n1 and n2 are the refractive indices of the ATR crystal and the sample respectively. θ is the angle of incidence. • if the ZnSe crystal (n1=2.4) is used, the penetration depth for a sample with the refractive index of 1.5 at 1000cm-1 is estimated to be 2.0 µm when the angle of incidence is 45°. • If the Ge crystal (n1=4.0) is used, the penetration depth is about 0.664 µm. • The depth of penetration can be controlled either by varying the angle of incidence or by selection of crystals.
FTIR sampling technique -ATR
At each reflection, the light beam penetrates the sample to a depth of a few microns and is absorbed at the characteristic absorption frequencies. Zinc Selenide (ZnSe) crystal is most commonly used for ATR accessory.
ATR/spectroscopic flow cell • It provide real-time chemical information of molecular absorption at the aqueous-solid interface. • It can monitor bacterial attachment and biofilm growth on the surface of ZnSe, Ge, Si or the surface of cellulose acetate. Real time examination of biological • Studies with model compounds, e.g., proteins, molecules with attenuated total polysaccharides, humic and fulvic acids can provide valuable information on the adsorption to polymer surfaces. reflectance (ATR) flow cell
Properties of ATR crystals
2361.62
0.16
2920.23
0.17
Before sulfonation
0.15
0.13
After sulfonation 697.08
0.12
2336.59
2851.59
0.14
0.11
757.22
0.05
3747.42
0.06
3853.31
0.07
1492.82
0.08
1455.94
0.09 2958.44
Log(1/R)
0.10
0.04 0.03 0.02 0.01 -0.00 4000
3500
3000
2500 2000 Wavenumbers (cm-1)
1500
1000
500
ATR characterization of a membrane’s sulfuric acid groups and for the determination of the sulfonation degree of the polymer, sample provided by Hongying Zhou
http://www.piketech.com/technical/crystal-selection-ATR.html
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FTIR sampling technique – diffuse reflectance
FTIR sampling technique – diffuse reflectance • Diffuse Reflectance Infrared Fourier Transform Spectroscopy (DRIFTS) is a technique that collects and analyzes scattered IR energy. • It is used for measurement of fine particles and powders, as well as rough surface (e.g., the interaction of a surfactant with the inner particle, the adsorption of molecules on the particle surface). • Sampling is fast and easy because little or no sample preparation is required.
1) When the IR beam enters the sample, it can either be reflected off the surface of a particle or be transmitted through a particle. 2) The IR energy reflecting off the surface is typically lost. 3) The IR beam that passes through a particle can either reflect off the next particle or be transmitted through the next particle. This transmissionreflectance event can occur many times in the sample, which increases the pathlength. 4) Finally, such scattered IR energy is collected by a spherical mirror that is focused onto the detector. 5) The detected IR light is partially absorbed by particles of the sample, bringing the sample information
FTIR sampling technique – diffuse reflectance Specular reflection versus diffuse reflection • Specular reflection: When an infrared beam is focused on the surface of a particulate sample, it can interact with the sample two ways. First it may simply reflect off the sample surface in the same way visible light reflect off a mirror. This phenomenon, called “ specular reflection”, is a function of the refractive index of the sample. • Specular reflection is suitable for smooth surface that can strongly reflect IR beam.
• Diffuse reflection collects infrared radiation from the IR beam that passes through a particle can either reflect off the next particle or be transmitted through the next particle. This transmission-reflectance event can occur many times in the sample, which increases the pathlength. • Diffuse reflection collects scattered IR energy, • Diffuse reflection is used for rough sample and particle assembly.
There are three ways to prepare samples for DRIFTS measurement: 1) Fill the micro-cup with the powder (or the mixture of the powder and KBr). The diffuse reflectance accessory uses a focusing mirror to focus the beam on the sample surface and collect the IR energy. The micro-cup needs to be filled consistently in order to keep the focus. 2) Scratch the sample surface with a piece of abrasive (SiC) paper and then measuring the particles adhering to the paper. 3) Place drops of solution on a substrate. If colloids or powders are dissolved or suspended in a volatile solvent, you can place a few drops of the solution on a substrate, and then evaporate the solvent, subsequently analyze the remaining particles on the substrate.
FTIR sampling technique: PM-IRRAS PM-IRRAS: Polarization modulation infrared reflection adsorption spectroscopy S-polarized: Electric field lies in the plane formed by incident and reflected waves. For p-polarized light, the electric field has a component perpendicular to the surface and a component parallel to the surface
P-polarized: Electric field lies perpendicular to the plane formed by incident and reflected waves. For s-polarized light, the electric field is parallel to the surface plane
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FTIR sampling technique: PM-IRRAS
PM-IRRAS analysis organic monolayer on inorganic substrate Si-CH2
C=O
-NH Si-O-Si
1) The IRRAS is dependent upon the optical constants of the thin film and substrate, the angle of incidence, as well as the polarization of the incident IR radiation. 2) The phase shift of the perpendicular component, s, exhibits no significant dependence upon the variation of the angle of incidence. 3) Because the phase shift of the perpendicular component, s, is nearly 180° for all the angles of incidence, the net amplitude of the IR radiation parallel to the substrate surface is zero. 4) The phase shift of the parallel component, p, strongly depends upon the angle of incidence. The p-polarized component goes through a maximum at 88°. At such grazing incidence, the p-polarized radiation sums up of Ep and Ep’, leading to a net combined amplitude that is almost twice that of the incident radiation.
PM-IRRAS PM-IRRAS has a surface-enhanced effect; and it is used for characterization of very thin films or monolayer It can determines molecular orientation and conformation in organic/biological polymer films. It can be use to analyze films (e,g,. Lipid film) on water-solid interface.
wavenumber (cm-1)
PM-IRRAS spectrum of organic monolayer on the ITO glass substrate, sample provided by HyungEui Lee
Application of PM-IRRAS in biology
virus
(virus)
PM-IRRAS spectrum of poly-Llysine on gold substrate
PM-IRRAS spectrum of arachidic acid monolayer at the air/water interface
PM-IRRAS spectrum obtained from virus on Au substrate, by courtesy Rafael Vega and C. Mirkin
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FTIR sampling techniques
PM-IRRAS analysis of monolayers PM-IRRAS mode of FTIR showing the lipid transferred from a Langmuir-Blodgett trough under a variety of subphase conditions, such as the presence of Chromium (III) ions, TAP, or both, by courtesy of N. Catron
The monolayer is a double C18 tailed lipid, with a dual-purpose headgroup. The headgroup can chelate metals, dimerizing given a metal with high enough coordination number. The headgroup also has a portion designed to bind 2,4,6-Triaminopyrimidine (TAP). This lipid was studied by transferring a monolayer onto a gold substrate and using the Polarization modulation-infrared reflection-adsorption spectroscopy (PMIRRAS) mode of FTIR.
FTIR sampling technique: PM-IRRAS
This table is meant to serve as a general guide for method selection based on the physical form of a sample. Upon assessment of a specific sample it is possible that none of the listed techniques will be suitable. ATR
Specular reflectance
monolithic solid
x
x
particle
x
coating
x
Sample Form
x
PMIRRAS
x
DRIFTS
Transmission
x
x
x
x
x
monolayer fiber
x
microtome cut
x
x
x
Thick film (mm)
x
X ??
thin films (micron)
x
x
paper
x
x x
x
x x
FTIR Imaging • FTIR microscope - Provide FT-IR spectra for samples down to about 10 μm in size - Two primary modes of FT-IR microscopy: reflectance and transmission - More advanced mode: ATR
From Maltseva Elena
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FTIR Imaging
FTIR Imaging
Fingerprint analysis Closer examination in right figure reveals that the spectrum at one of the spots has CH3, CH2, NH and OH absorptions typical of proteins, while neighbouring spectra just show finger grease
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MAE 649 Microscopy and Spectroscopy of Materials
Chapter 5 Raman Spectroscopy
Principle of Raman spectroscopy interaction between light (electromagnetic radiation) and molecules 1) Electromagnetic radiation consists of oscillating electric and magnetic fields. 2) Both of these fields have the potential to interact with molecules, however the magnetic interaction is much less likely to cause transitions to occur, and so the electric effect dominates. 3) Usually in rotational and vibrational spectroscopy, the transitions of interest are those involving the interaction between the electric dipole moment of the molecule ( µ ) and the electric field of the radiation ( E ).
Energy of interaction = µ E µ can be considered as: µ = ∑qiri where q is a charge and r is its distance from the centre of the molecule.
Chapter 5- Fourier Transform Infrared Spectroscopy Contents: • light - electromagnetic wave • molecular effects of infrared adsorption -- molecular vibration -- dipole change • interpretation of IR spectra • Instrumentation and sampling techniques -- attenuated total reflection (ATR) -- diffuse reflection -- Polarization modulation infrared reflection adsorption spectroscopy (PM-IRRAS)
Principle of Raman spectroscopy interaction between light (electromagnetic radiation) and molecules µ varies as the molecule moves. For a strong interaction between the molecule and the radiation, µ must oscillate at the same frequency ( ν ) as the electric field. In other words, the energy held by a photon of the radiation must be equal to the gap in energy between two states, either rotational or vibrational, of the molecule: h ν = E2 - E1 In absorption spectroscopy, the photon transfers its energy to the molecule, resulting in its transition to a higher energy state. In emission spectroscopy, the molecule drops from a higher energy state to a lower one, and the energy lost in this process is emitted as a photon. When a beam of radiation with a frequency which will lead to a transition is passed through a sample, the chances of absorption or emission being induced are equal. Whether net absorption or emission is seen depends on the population of the energy levels.
• Raman spectroscopy
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Principle of Raman spectroscopy interaction between light (electromagnetic radiation) and molecules 1) Usually in rotational and vibrational spectroscopy, the transitions of interest are those involving the interaction between the electric dipole moment of the molecule ( µ ) and the electric field of the radiation ( E ).
Energy of interaction = µ E µ can be considered as: µ = ∑qiri where q is a charge and r is its distance from the centre of the molecule.
Principle of Raman spectroscopy Selection rule for Raman active-- polarizability IR i. vibrational modes
Raman vibrational modes
ii. change in dipole
change in polarizability
Need a permanent dipole moment iii. excitation of molecule to excited vibrational state
No need momentary distortion of the electrons distributed around the bond
Principle of Raman spectroscopy
Principle of Raman spectroscopy
Selection rule for Raman active-- polarizability For IR spectroscopy, it is necessary for the molecule to have a permanent electric dipole. This is not the case for Raman spectroscopy, rather it is the polarizability (α) of the molecule which is important.
Selection rule for Raman active-- polarizability
The oscillating electric field of a photon causes charged particles (electrons and, to a lesser extent, nuclei) in the molecule to oscillate. This leads to an induced electric dipole moment, µind, where µind = α E This induced dipole moment then emits a photon, leading to either Raman or Raleigh scattering. The energy of this interaction is also dependent on the polarizability: Energy of interaction = -1/2α E 2 The energies of Raman transitions are relatively weak. To counter this, a higher intensity of the exciting radiation is used. For Raman scattering to occur, the polarizability of the molecule must vary with its orientation. One of the strengths of Raman spectroscopy is that this will be true for both heteronuclear and homonuclear diatomic molecules.
Comparison between Raman and IR Spectroscopy They are complementary, both measure the vibrational energies of molecules Raman IR • The photon causes a • To be active, the momentary distortion of the edistribution around a bond, dipole moment of the followed by re-emission of molecule must radiation as the bond returns to its normal state. (the dipole change then disappears) • To be active, the polarizability of the molecule must change with the vibrational motion
(Dipole = a molecule with a charge difference)
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Principle of Raman spectroscopy
Principle of Raman spectroscopy
Selection rule for Raman active-- polarizability
Selection rule for Raman active-- polarizability Raman spectroscopy: IR spectroscopy: • scattered emission: • Adsorption: (radiation at a certain frequency (radiation at a certain frequency is is scattered by the molecule with adsorbed due to the resonance of shifts in the wavelength of the molecular vibration) incident beam) • observed peak is due to • observed frequency shifts are molecular vibration related to vibrational changes in the molecule
Must be change in polarizability Non-Polar groups such as C-S, S-S, C=C, C=C (triple bond), N=N and heavy atoms (I, Br, Hg) strong scatterers Symmetric stretching vibrations are much stronger scatterers than asymmetric stretching vibrations
hv 1
hv 1
Principle of Raman spectroscopy
Principle of Raman spectroscopy
The basic set-up of a Raman spectrometer is shown below. Note that the detector is orthogonal to the direction of the incident radiation, so as to observe only the scattered light. The source needs to provide intense monochromatic radiation, and so is usually a laser.
Types of scattering Consider a light wave as a stream of photons each with energy hν. When each photon collides with a molecule, two type of photon emission of which are considered below: Elastic, or Raleigh scattering: This is when the photon simply 'bounces' off the molecule, with no exchange in energy.
1) Raman spectroscopy collect scattered radiation. 2) The criteria for a molecule to be Raman active are also different to other types of spectroscopy. Raman active does NOT require a permanent dipole moment.
Inelastic, or Raman scattering: This is when there is an exchange of energy between the photon and the molecule, leading to the emission of another photon with a different frequency to the incident photon
From Kiera Jones
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Principle of Raman spectroscopy
Principle of Raman spectroscopy
Selection rule for Raman active- energy quantitized Rotational To find allowed rotational transitions, the total angular momentum quantum number for rotational energy states, J, must be considered. Raman spectroscopy involves a 2 photon process, each of which obeys: ΔJ = ±1 Therefore, for the overall transition, ΔJ = 0, ±2 where ΔJ = 0 corresponds to Raleigh scattering, ΔJ = +2 corresponds to a Stokes transition, and ΔJ = -2 corresponds to an anti-Stokes transition. Vibrational To find allowed transitions the vibrational quantum number, υ, must be considered. For the overall transition, Δυ = ±1 Transitions where Δυ = ±2 are also possible, but these are of weaker intensity.
Principle of Raman spectroscopy
Selection rule for Raman active The molecule is originally at the E2 energy state. The photon interacts with the molecule, exciting it with an energy hνi. However, there is no stationary state of the molecule corresponding to this energy, and so the molecule relaxes down to the energy levels E1 or E3 . This process emits a photon in two ways: Anti-Stokes transition: If the molecule relaxes to energy state E1, it will have lost energy, and so the photon emitted will have energy hνr1, where hνr1 > hνi Stokes transitions: If the molecule relaxes to energy state E3, it will have gained energy, and so the photon emitted will have energy hνr2, where hνr2 < hνi
From Clayton Butler
Principle of Raman spectroscopy Summary of the selection rules for Raman active 1) For Raman scattering to occur, the polarizability of the molecule must vary with its orientation. (However, Raman active does NOT require a permanent dipole moment). 2) For vibrational or rotational transitions, the total angular momentum quantum number for rotational energy states must be met. 3) For rotational spectroscopy, both Stokes and anti-Stokes transitions are seen. For vibrational spectroscopy, Stokes transitions are far more common, and so anti-Stokes transitions can effectively be ignored.
For rotational spectroscopy, both Stokes and anti-Stokes transitions are seen. For vibrational spectroscopy, Stokes transitions are far more common, and so anti-Stokes transitions can effectively be ignored.
raleigh scatter
http://www.chemsoc.org/ExemplarChem/entries/2004/birmingham_jones/raman.html#Spectra
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Application of Raman spectroscopy How does it work?
Comparing Infrared with Raman spectroscopy 3.) Active Raman Vibrations: - need change in polarizability of molecule during vibration - polarizability related to electron cloud distribution
Proprietary Raman Ink
Material Identification through Raman spectroscopy.
example:
Libraries of Raman Barcodes
Brand Security
O=C=O
IR inactive Raman active
O=C=O
IR active Raman inactive
IR & Raman are complimentary. Can be cases where vibration is both IR & Raman active (eg. SO2 – non-linear molecule) O
500
Anti-counterfeiting
1000
1500
2000
Wavenumbers
Comparing Infrared with Raman spectroscopy
2500
In general: C IR tends to emphasize polar functional groups (R-OH, , etc.) Raman emphasizes aromatic & carbon backbone (C=C, -CH2-, etc.) - Raman does not “see” many common polar solvents can use with aqueous samples – advantage over IR Raman frequency range: 4000 -50 cm-1(Stokes and antistokes)
Infrared and Raman Spectra of Benzene
Raman
IR
Infrared
Raman
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Application of Raman spectroscopy
Application of Raman spectroscopy Raman peak is sensitive to stress in materials
Initial Phase of CdS Deposition on InP(100) at 200°C
broad shoulder on low frequency side of CdS phonon peak indicates an Interfacial reaction leading to an In-S rich layer The Raman shift of diamond 1332 cm-1 band increases with compressive stress. Calibration of this shift to stress is very complicated for non-hydrostatic stress fields; but we expect it to be of similar magnitude to the hydrostatic value, a shift of 2.4 cm1 GPa-1. If a compressive stress is applied to a sample, the binding distance of the atoms is reduced resulting in a higher vibrational frequency. The Raman line of this vibration is shifted to higher frequencies. Accordingly, a tensile strain shifts the Raman lines to lower wavenumbers. http://www.renishaw.com/UserFiles/acrobat/UKEnglish/SPD-PO-080.pdf
Application of Raman spectroscopy Confocal Raman microscopy for three-dimensional imaging
www.renishaw.com
Application of Raman spectroscopy Confocal Raman microscopy for imaging of food
(a) Raman image of instant gravy thickener particles. (Scan range: 50 50 m, 150 150 pixels, 22,500 spectra, 70 ms/spectrum, excitation: 532 nm Nd:Yag.) (b) corresponding Raman spectra.
http://www.kosi.com/raman/resources/technotes/1350.pdf
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Advantages of Raman spectroscopy Raman spectroscopy is useful for analyzing molecules without a permanent dipole moment which would not show up on an IR spectrum. It can be used to determine bond lengths in non-polar molecules. Water compatible– water is a weak Raman scatter. It is useful for determining the identity of organic and inorganic species in solution, as the Raman transitions for these species are more characteristic than for IR, where the transitions are much more affected by the other species present in the solution. Raman spectroscopy is sensitive the stress in materials, and it is also used for detection of crystal orientation. No sample preparation
Analytical Capabilities of IR and Raman Analytical Capabilities
XPS
FTIR
• Primary beam
X-ray
infrared light
• secondary beam
electrons
infrared light
• spatial resolution
10 µm
10 µm
• sampling depth
1-10nm
micron- mm
• Elemental identification All except H, He • Molecular Information
chemical shift
• Quantification
Excellent without standard
• Detection Limit
0.1%
• organic/inorganic
both
No Functional Groups limited 0.1% both
• No one analytical technique provides all the answers.
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