NRC Publications Archive (NPArC) Archives des publications du CNRC (NPArC) Mineralogical adventures of a powder diffractionist Whitfield, Pamela; Roberts, Andy; Mitchell, Lyndon; Le Page, Yvon; Mills, Stuart; Kern, Arnt; Tait, Kim Web page / page Web http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/ctrl?action=rtdoc&an=16240055&lang=en http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/ctrl?action=rtdoc&an=16240055&lang=fr Access and use of this website and the material on it are subject to the Terms and Conditions set forth at http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/jsp/nparc_cp.jsp?lang=en READ THESE TERMS AND CONDITIONS CAREFULLY BEFORE USING THIS WEBSITE. L’accès à ce site Web et l’utilisation de son contenu sont assujettis aux conditions présentées dans le site http://nparc.cisti-icist.nrc-cnrc.gc.ca/npsi/jsp/nparc_cp.jsp?lang=fr LISEZ CES CONDITIONS ATTENTIVEMENT AVANT D’UTILISER CE SITE WEB. Contact us / Contactez nous: [email protected]. Mineralogical Adventures of a Powder Diffractionist Pamela Whitfielda, Andy Robertsb, Lyndon Mitchella, Yvon Le Pagea, Stuart Millsc, Arnt Kernd and Kim Taite a NRC, b Geological Survey of Canada, c University of British Columbia, d Bruker-AXS, e Royal Ontario Museum My background in diffraction? • My background is inorganic solid-state chemistry – functional oxides such as lithium battery materials • Have unique equipment/capabilities for powder diffraction. – 3 instruments of different configurations (tube anodes Cr Ag) – custom-built attachments for non-ambient capillary and in-situ gas pressure work – beta test software for Bruker-AXS • Never done single-crystal diffraction and have enough work that I may never have to! • Done most powder diffraction techniques up to and including structure solution from powder diffraction. – jack of all trades and master of none? – currently chair of the IUCr Commission for Powder Diffraction Why is a chemist playing with minerals? • Structure determination from lab powder diffraction data not a common technique in Canada. • A colleague of a colleague of a colleague in Canada sent me a sample of a very boring-looking new mineral – needed capillary geometry - LiNaB3SiO7(OH) – very fine grained <5 m – wanted the structure in a couple of weeks for IMA submission! Bright-field optical image of new mineral - not very exciting And? Crystal structure of jadarite • Successfully solved the structure using simulated annealing • The mineral was jadarite, aka kryptonite (chemical formula as per Superman 3) as reported by the BBC and others – and the rest is history… Kryptonite? Jadarite - dull reality! What came next? • Funnily enough some weird and wonderful fine-grained minerals from Canadian labs have come my way since then…. • The list includes – stichtite, woodallite, barbertonite, angastonite, widgiemoolthalite, dypingite, strontiodresserite, montroyalite, F-altered gibbsite and so on…. • The rest of the presentation consists of a survey of new techniques and instrumentation to solve the challenges posed by different mineral samples that have come my way…. Angastonite CaMgAl2(PO4)2(OH)4.7H2O • • Australian mineral described in 2008. Lab data triclinic 2150Å3 unit cell – new indexing algorithm Unusual in that lab data much better than synchrotron – unstable over time and in beam? 50000 0.5mm capillary Focusing mirror – CuK Vantec PSD 40000 Intensity (counts) • 30000 298 K time 20000 10000 0 5 10 15 20 25 30 35 40 45 50 55 60 65 Two theta (degrees) Le Bail fit of triclinic cell to lab data 2 3 4 5 6 7 2 (degrees - 0.697 Å) Synchrotron data from angastonite Stichtite Mg6Cr2(OH)16CO3.4H2O • Stichtite has the hydrotalcite structure – simple R-3m symmetry but multiple occupancies and vacancies – also shows hkl-dependent peak broadening (very unpleasant!) 006 012/ 009 015 Le Bail fit to data 018 110 113 116 Stichtite • Seen broadening in R-3m layered battery materials before – no peak shifts so probably twin faulting in stichtite Monte-Carlo simulation of effect of 5% stacking faults ( ) and twin faults ( ) – previously developed reciprocal-space relationship to model broadening in R-3m with 1 variable vs 6 spherical harmonics variables If H-K 3n = constant lc* cos(c* ^ R*) l = Miller index, c* = c reciprocal space vector, R* = reciprocal space vector Stichtite • Structure refinement without the broadening correction.. and with…. 1,100,000 1,100,000 1,050,000 1,050,000 1,000,000 1,000,000 950,000 950,000 900,000 stitchtite-3R1 79.18 % Lizardite 1T 0.56 % stitchtite-2H1 20.25 % stitchtite-3R1 87.92 % Lizardite 1T 0.81 % stitchtite-2H1 11.27 % 900,000 850,000 850,000 800,000 800,000 750,000 750,000 700,000 700,000 650,000 650,000 600,000 550,000 600,000 500,000 550,000 450,000 500,000 400,000 450,000 350,000 400,000 300,000 350,000 250,000 300,000 200,000 250,000 150,000 200,000 100,000 150,000 50,000 100,000 0 50,000 -50,000 0 -100,000 -50,000 -150,000 10 20 30 40 50 10 60 20 70 30 80 2Th Degrees 40 90 50 100 60 110 70 120 80 2Th Degrees 130 90 100 110 120 130 F-modified gibbsite (Francon quarry, Montreal) • Multi-phase (F-gibbsite, corundum, mica, lizardite) • Gibbsite is layered anisotropic broadening back again • Difficult one to fit and potential correlations are horrendous 280 F-Gibbsite Corundum Biotite-mica lizardite-1T capillary background 260 240 220 88.16 % 0.50 % 3.96 % 7.38 % 0.00 % 200 Sqrt(Counts) 180 160 140 120 100 80 60 40 20 0 -20 5 • • • • 10 15 20 25 30 35 40 45 50 55 60 65 2Th Degrees 70 75 80 Al(1)-O average bond length = 1.95 Å , Al(2)-O average bond length = 1.82 Å, Al-O6 from bond valence = 1.91 Å, Al-F6 from bond valence = 1.80 Å, 85 90 95 100 105 110 Fourier difference plot reveals significant residual electron density between the layers. Significant H2O content? Fluorocronite very recent IMA submission • • capillary geometry -1 Cu of 1525 cm ! Had very little material and multi-phase However mineral of interest is PbF2; has – CuK a non-starter but wanted to solve with lab equipment – was going to be named after Lachlan Cranswick but Ron Peterson beat us to it 35,000 20000 30,000 25,000 16000 20,000 14000 Counts Intensity (counts) 18000 12000 10000 26.22962 5.046336 7.539469 8.805516 10.11759 11.38644 14.45781 15.05726 17.54717 cassiterite 40.07 % fluorocronite 59.93 % 15,000 10,000 8000 5,000 6000 0 4000 2000 10 20 30 40 2 (MoK - 0.7Å) Debye-Scherrer data with MoK . Likely R with 0.3mm cap still >5 -5,000 6 8 10 12 14 16 18 20 22 24 2Th Degrees 26 28 30 32 34 36 38 Data from AgK (0.56Å) with focusing mirror. Likely R with 0.3mm cap <3 40 Carbonation of CaSiO3 under pressure • Custom pressure stage built to study crystallization of polymers under CO2 • Proof of concept study carried out for sequestration-related work using wollastonite as a model 60°C 56 bar CO2 In-situ carbonation with 56 bar CO2 of damp CaSiO3 Arrhenius plot for carbonation of CaSiO3 Strontiodresserite SrAl2(CO3)2(OH)4.H2O • This sample was supposed to be montroyalite but turned out to be something else….. • The data was very good quality to low d-spacings - the ‘heavy’ Sr atom made it a good candidate for charge flipping Log Intensity 1e+5 4 hemispheres 0.5mm capillary Focusing mirror 1e+4 1e+3 1e+2 20 1mm hemisphere embedded in sill rock (Francon Quarry, Montreal) 40 60 80 100 2 (degrees CuK ) Raw data up to 140°2 120 Charge flipping • Charge-flipping can be extremely fast – often get solution in less than 3 mins • Sr, Al and many of the oxygens located • Info used to constrain simulated annealing run to get rest of the structure Al Sr Atom picking from electron density map generated from charge-flipping using the tangent formula Strontiodresserite structure • • • • • Irregular 9-coordinate Sr-O polyhedra Octahedral AlO6 Blocks tied together by carbonate anions Water molecules in a channel along the b-direction Isostructural with dundasite, PbAl2(CO3)2(OH)4.H2O • Hydroxides located with bond valence sums • DFT calculations to verify structure and localize H-bond network Polyhedral representation of strontiodresserite structure Conclusions • Laboratory powder diffraction equipment and techniques have improved considerably in recent years – Detectors, optics, software, new algorithms, etc • Information can now be extracted in the lab from samples that may previously have been intractable or only possible using a synchrotron beamline • The continuing evolution of powder diffraction guarantees it will play an increasingly important role in the analysis of both new minerals and in revisiting some old ones… Acknowledgements • Chris Stanley and co for the kryptonite adventure – and everyone in the powder diffraction community who will never let me forget it! • Peter Stephens (SUNY/Brookhaven) for valiantly trying to get some decent data from the angastonite on his beamline • Hugues Guerault of Bruker-AXS for collecting the AgK data Questions?
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