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applications of Synchrotron FourierTransform Infrared (FT-IR) - - PowerPoint PPT Presentation

Diagnostic techniques for cultural heritage: applications of Synchrotron FourierTransform Infrared (FT-IR) spectroscopy Mariangela Cestelli Guidi Sinbad IR beamline @ Da F ne INFN-International Masterclass 2015 Layout The scientific


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Diagnostic techniques for cultural heritage: applications of Synchrotron FourierTransform Infrared (FT-IR) spectroscopy

Mariangela Cestelli Guidi Sinbad IR beamline @ DaFne INFN-International Masterclass 2015

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 The scientific approach to conservation  Principles of FT-IR spectroscopy  Sampling techniques: transmission, reflection, Attenuated total reflection (ATR) and Diffuse reflection (DRIFT)  Infrared imaging and microscopy: chemical images  FT-IR Analysis of a painting cross section

Layout

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FOURIER TRANSFORM INFRARED SPECTROSCOPY (FT-IR): physical principles

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Electromagnetic spectrum and IR

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 Tecniche invasive e distruttive

The EM field

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 Visible and IR light are both EM radiation, differing only for the

  • wavelegth. They both propagate in vacuum at the light speed c.

 Wavelength l (mm)  Frequency n (Hz: n=c/l)  Energy E (eV: E=hn)  Wavenumber 𝜉 (cm-1)

𝝃 (cm-1)= 1/l (cm)

IR Units

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What happens when «light» interacts with matter

E total = E translational + E rotational + E vibrational

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 In the simple case of two point charges, one with charge +q and the other one with charge −q, the electric dipole moment p is:  d is the displacement vector pointing from the negative charge to the positive

  • charge. Thus, the electric dipole moment vector p points from the negative

charge to the positive charge.

Every molecule interacts with the IR EM field?

Electric field of an electric dipole. The dipole consists of two point electric charges of opposite polarity located close together

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Polar molecules

A molecule of water is polar because of the unequal sharing of its electrons in a "bent"

  • structure. A separation of charge is present

with negative charge in the middle (red shade), and positive charge at the ends (blue shade). Examples of polar molecules of materials that are gases under standard conditions are: Ammonia (NH3) Sulfur Dioxide (SO2) Hydrogen Sulfide (H2S).

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Common examples of non-polar gases are the noble or inert gases, including:  Helium (He)  Neon (Ne)  Krypton (Kr)  Xenon (Xe) Other non-polar gases include:  Hydrogen (H2)  Nitrogen (N2)  Oxygen (O2)  Carbon Dioxide (CO2)  Methane (CH4)  Ethylene (C2H4) 

Non polar molecules

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 O2, H2, Cl2, N2 are not IR active!

IR active modes

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M1 M2 𝜉 = 𝑙 𝑛 vibration frequency 𝑛 =

𝑁1∙𝑁2 𝑁1+𝑁2 (reduced mass)

Increasing k (bond strength) the frequency increases Decreasing m, the frequency increases.

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Single bonds: C-C, C-O, C-N  800 - 1300 cm-1 Double bonds: C=C, C=O, C=N  1700-1900 cm-1 Triple bonds: C≡C, C ≡O, C ≡N  2000-2300 cm-1 C-H, N-H, O-H  2700-3800 cm-1

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𝐹 = (𝑜 + 1

2) hn

(quantized energy levels)

 3N-6 (non linear molecule)  3N -5 (linear molecule)

Normal modes of vibration

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Every molecule has its unique IR spectrum

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Also very complex molecules...

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Fourier Transform Infrared Spectroscopy (FT-IR)

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Detector Detector Reflection Transmission IR source Sample

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IR sources

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Synchrotron radiation

LNF, February 16 2015

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Every moving electric charge emits EM radiation. Classic (v<<c) Relativistic (v≈c) 1/𝛿 𝛿 = 1 1 − 𝛾2 𝛾 = 𝑤/𝑑

Per b=0.99 1/g= 10 mrad

Critical energy

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The beamlines

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The IR SINBAD beamline

Infrared domain from 10 to 103 cm-1 1.24meV to 1.24 eV

DAFNE

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Michelson interferometer

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Mobile mirror M1 Fixed mirror M1 IR source Detector beamsplitter

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The interferogram depends on the optical path difference (OPD) between the two beams The OPD is twice the mirror excursion x. Since the mirror speed v is constant:

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OPD= 2n

𝜇 2 (𝑜 = 0, ±1, ±2, … )

OPD= (2n+1) 𝜇

2 (𝑜 = 0, ±1, ±2, … )

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Origin of the interferogram: the momocromatic wave

Detector signal OPD

The Fourier transform

Spectrum Frequency FOURIER TRANSFORM

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Origin of the interferogram: the policromatic wave (disccrete frequencies)

Detector signal Spectrum

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Origin of the interferogram: the policromatic wave (continuous frequencies)

Detector signal

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Measuring an IR spectrum

TRANSMITTANCE

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ABSORBANCE

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Sampling techniques

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 Depending on the sample form (solid, liquid, powder, film) and which characteristics you want to mantain, it is possible to use different sampling techniques, distructive or non distructive:  Transmission (liquids, powders, thin sections)  Specular reflection (crystals, polished sections)  Diffuse reflectance (powders)  Attenuated Total Reflection (ATR) (thick samples, non reflecting surfaces)

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Transmission KBr powder pellets

  • Invasive
  • Destructive
  • Time consuming
  • Very precise (absolute measurement)
  • Spectral database
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Sample

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Beer-Lambert law A = log I0/I= e C b Absorbance is proportional to the concentration

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Reflection spectroscopy

Preparation of the surface – polishing Thick samples

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Attenuated Total Reflection (ATR)

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Crystal n1 Sample n2 Snell’s law: n1 x sini = n2 x sinr Critical angle: r = 90° sinc = n2 / n1 (es. 38° for ZnSe for a sample with n=1.5)

Principles of Attenuated Total Reflection spectroscopy (ATR)

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Penetration depth

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dP prop l

ATR = AB * n [cm-1] / 1000 [cm-1]

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 Quick  Non invasive  (semi)destructive

Kazarian et al, Vibrational Spectroscopy 53 (2010) 274–278

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CaSO4·2H2O CaSO4.0.5H2O CaSO4

ATR spectrum of gypsum

n3 Stretching antisymmetric of SO4 tetrahedra n1 Stretching symmetric of SO4 tetrahedra Water molecule: Stretching symmetric and antisymmetric of H2O

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CaSO4·2H2O CaCO3

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What if the sample is VERY small?

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Microscopy and Imaging

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The microscope is essentially a beam condenser The IR microscope is essentially a beam condenser

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FTIR imaging

Vincent Mazel et al, (2007). Analytical Chemistry. DOI : 10.1021/ac070993k

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Mapping vs imaging

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APPLICATION TO THE STUDY OF PAINTING CROSS SECTIONS

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Figura 1. Sezione stratigrafica di un frammento prelevato dalla veste verde di un dipinto raffigurante la Madonna col Bambino: a) sezione stratigrafia al microscopio ottico in luce visibile; b) immagine ottenuta al microscopio elettronico (SEM); c) mappatura dell’elemento rame (Cu) eseguita mediante spettrometro a raggi X al microscopio elettronico (SEM-EDS); d) distribuzione della resina poliestere ottenuta mediante FTIR FPA-imaging; e) distribuzione del pigmento verde malachite, ottenuta mediante FTIR FPA-imaging; f) distribuzione di legante proteico,

  • ttenuta mediante FTIR FPA-imaging; g) distribuzione di olio siccativo ottenuta mediante FTIR FPA-imaging; h) spettro di assorbenza della

particella verde e del riferimento della malachite; i) spettro della componente proteica e del riferimento del rosso d’uovo; j) spettro ottenuto da una zona contenente olio siccativo e lo spettro di riferimento di una “sapone” formatosi per reazione tra rame e olio siccativo – immagine tratta dal testo citato – nota 3

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LED lights may be bad for Van Gogh Paintings

http://www.vangogh.ua.ac.be/

The darkening of chrome yellow is a phenomenon widely observed on several paintings by Vincent van Gogh such as the famous versions of the Sunflowers. Analysis of artificially aged model samples of lead chromate using the combined use of various synchrotron radiation based analytical techniques (μ-XRD, μ-XANES and µ-FTIR), established that darkening of chrome yellow is caused by reduction of PbCrO4 to Cr2O3.2H2O (viridian green). This is likely accompanied by the presence

  • f another Cr(III) compound, such as either Cr2(SO4)3.H2O or

(CH3CO2)7Cr3(OH)2 [chromium(III) acetate hydroxide].

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Image courtesy of http://www.vangogh.ua.ac.be/

Phosphor-based white LED light

To avoid photo induced darkening of the susceptible variants of the lead chromate-based pigments, it is advisable to minimize their exposure to light with wavelengths shorter than about 525 nm

PbCr1−xSxO4 PbCrO4

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What is the alteration mechanism of the chrome yellow pigments?

Micro-X-ray Fluorescence Micro-X-ray Diffraction Micro-Fourier Transform Infrared Spectroscopy Micro-X-ray Absorption Near-Edge

Combined use of Synchrotron Radiation Based Techniques for Revealing an Alternative Degradation Pathway of the Pigment Cadmium Yellow in a Painting by Van Gogh

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Fourier Transform Infrared Spectroscopy (FT-IR) @ LNF

Sulphate [SO 4 2- ] content

monoclinic

  • rthorombic
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Septimius Severus’s Arch degradation products

200x600 mm

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MICRO FT-IR chemical imaging

FPA detector Ossalato 20 mm

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Multivariate analysis combined with FT-IR

Cluster Analysis Principal Component Analysis RGB map of the sample composition

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Alcuni spettri di riferimento

Courtesy of Centro Conservazione e Restauro La Venaria Reale

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Il carbonile

Solventi Leganti Vernici Fibre Ma anche in alcuni pigmenti inorganici

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Gli esteri

Olii siccativi Resine naturali Cere Resine sintetiche Additivi Plastiche

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Le ammidi

Struttura generale di un'ammide. Se R' e R" sono idrogeni l'ammide si dice primaria, se solo uno fra R' ed R" è un H, si dice secondaria, se R' ed R" non sono idrogeni, l'ammide si dice terziaria Tempere all’uovo Tempera grassa Lana e seta Colle animali Cuoio e pelle Caseina Plastica

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I polisaccaridi

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 Carbonati  Silicati  Solfati  Pigmenti organici

I pigmenti

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 Solfati  Ossalati  Nitrati  Saponi

Prodotti di degrado comuni

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https://web2.infn.it/Dafne_Light/ cestelli@lnf.infn.it