Raman e Mineralogia, Parma, 12 febbraio 2009 Spettroscopia Raman e Grandi Sorgenti (Synchrotron...
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Transcript of Raman e Mineralogia, Parma, 12 febbraio 2009 Spettroscopia Raman e Grandi Sorgenti (Synchrotron...
Raman e Mineralogia, Parma, 12 febbraio 2009
Spettroscopia Raman e Grandi Sorgenti (Synchrotron Facilities)
Marco Milanesio
Dipartimento Scienze e Tecnologie AvanzateUniversità del Piemonte Orientale, Alessandria, Italy
E-Mail: [email protected]://www.mfn.unipmn.it/~marcomi
Nuove Applicazioni della Spettroscopia Raman nei MineraliParma 12 Febbraio 2009
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 2
Storage ring producing high brilliance X-ray (1000-1000000 more intense than in normal diffractometers)
What is a synchrotron facility?
Raman e Mineralogia, Parma, 12 febbraio 2009
Standard SNBL Beam line at ESRF
Optics A+BHRPD + XAFS PD + Single x-tal
B-Hutch A-Hutch Prep-lab
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 4
The good news: Synchrotron allows X-ray Powder Diffraction (XRPD) in situ studies (down to ms time res.)
Typical business at synchrotron facilities :
When a phase undergoes a phase transition its
diffraction pattern changes
Environmental chambers are used to condition the sample environment: Temperature,
pressure, atmosphere, irradiation, laser in situ
during XRPD
(a)
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 5
1) The availability of 3rd generation synchrotrons allowed the use of XRPD experiments at in situ conditions.
2) The addition of an extra dimension, such as time or temperature allowed the investigation of structural properties during solid-state transformations
IN SITU XRPD synchrotron facilities?
Template Burning inside TS-1 and Fe-MFI Molecular Sieves: An in Situ XRPD Study. Milanesio, M.; Artioli, G.; Gualtieri, A. F.; Palin, L.; Lamberti, C.
J. Am. Chem. Soc.; 2003; 125(47); 14549-14558
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 6
The bad news: the limits of in situ XRPD
amorphous phases
evolved gas
gel phases
liquid phases
nanoparticles
surface reactivity
disordered moieties
light elements (Z < 4)
Why Raman and synchrotron facilities?
Sometime overcame by Raman!!
Raman e Mineralogia, Parma, 12 febbraio 2009
Raman spectroscopy can give complementary information to XRPD, being extremely sensitive to small structural distortions, to changes in the hydration/protonation states, to surface modifications and to changes in the charge/defect distribution and short-range ordering.
Raman information
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 8
• Many non-simultaneous Raman-Xray diffraction/absorption studies have been performed for their complementarities.
• In situ induced sample modifications with multiple external stimuli such as:– Temperature and/or– Pressure and/or– UV or Visible Light, X-ray’s and/or– Oxidizing or reducing environments– ….
• On samples that show kinetic and non-reversible behaviors on one or more of these stimuli
Why Simultaneous RAMAN/XRPD? Because of the perfect space, time and reaction-coordinate correlation between Raman and XRPD and no bias due to different sample holder/conditioning modes
Difficult or impossible to synchronize separate XRPD and Raman experiments
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 9
The first example - Phase transitions of isobutyl-silsesquioxane (SNBL@ESRF, July 2004)
XRPD: phase transition from the triclinic to rhombohedral phase at 323 K
Raman spectroscopy: small variation of the peak at 775 cm-1
related to rotation of the side chain O-Si-C-C torsion angles
This case study allowed i) to test the first Raman/XRPD implementation with a NIR laser (1064 nm) and ii) to design the better setup for the permanent Raman installation at the SNBL
Raman e Mineralogia, Parma, 12 febbraio 2009
SNBL layout with Raman
Optics A+BHRPD + XAFS PD + Single x-tal
B-Hutch A-Hutch Prep-labRam
an
Excitation laserRaman return
Raman e Mineralogia, Parma, 12 febbraio 2009
The Experimental Set-up – Technical detailsReferences on the simultaneous experiments
- More info: E. Boccaleri, F. Carniato, G. Croce, D. Viterbo, W. van Beek, H. Emerich and M. Milanesio, In situ simultaneous Raman/high-resolution X-ray powder diffraction study of transformations occurring in materials at non-ambient conditions, J. Appl. Cryst. (2007). 40, 684-693.
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 12
Possible multi-technique experiments at the SNBL…
Raman/EXAFS
Raman/XRPD/EXAFS
Raman/XRPD/XAFS/Mass Spectroscopy
Raman/Single crystal XRD
Raman/XRPD
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 13
….. accessible non ambient conditions
Helium cryostat down to 5-10 K
Diamond Anvil cell: from 0 to 50 GP
Lamp- and laser- induced excitation: photo-reactivity
Gas blower + Cryostream nitrogen blower: from 80 to 1300 K
Gas pumping system: from vacuum to 30 bars
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 14
Case study 1 - The stearate-hydrotalcite (Mg/Al layered hydroxide) thermal treatment and decomposition (almost no mineralogy!)
Example of application to a low order synthetic
nanocomposite organic-inorganic material –
conformational/chemical sensitivity of Raman
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 15
Case study 1 - XRPD
At 362 K phase transition due to the swelling of the layers
A new peak appeared at 2θ=0.81° (d=42.4 Å). Its intensity increased up to 425 K and its 2θ moved to 0.72° (d=48.2 Å).
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 16
Case study 1 - Raman
The C-H stretching modes (2800-3000 cm-1) and the symmetric and asymmetric C-C stretching modes (at 1044 and 1110 cm-1) are sensitive to the changes in the trans-gauche conformation of the CH2 units and to the packing of the
embedded phase.
Raman e Mineralogia, Parma, 12 febbraio 2009Marco Milanesio 17
31.5 Å(XRPD at RT)
The phase transition characterizationRaman/XRPD the conformational features of the organic moiety and the structural rearrangement of the inorganic moiety
At room temperature: all-trans stearate chains form an inter-digitated bi-layer while (Raman).
45.0 Å (XRPD)
At high temperature: the chains assume folded gauche conformations and inter-digitation is reduced (Raman).
ΔT