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Mineralogical adventures of a powder diffractionist
Whitfield, Pamela; Roberts, Andy; Mitchell, Lyndon; Le Page, Yvon; Mills, Stuart; Kern, Arnt; Tait, Kim
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
Mineralogical Adventures of a Powder
Diffractionist
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?
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?
• 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…
Crystal structure of jadarite
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
CaMgAl
2(PO
4)
2(OH)
4.7H
2O
• 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?
Le Bail fit of triclinic cell to lab data
2 (degrees - 0.697 Å)
2 3 4 5 6 7
time
Synchrotron data from angastonite
Two theta (degrees)
5 10 15 20 25 30 35 40 45 50 55 60 65 Intensity (counts ) 0 10000 20000 30000 40000 50000 298 K 0.5mm capillary
Focusing mirror – CuK
Stichtite
Mg
6Cr
2(OH)
16CO
3.4H
2O
• Stichtite has the hydrotalcite structure
– simple R-3m symmetry but multiple occupancies and vacancies – also shows hkl-dependent peak broadening (very unpleasant!)
018 110 113 116
006
015 012/
009 Le Bail fit to data
Stichtite
• Seen broadening in R-3m layered battery materials before
– no peak shifts so probably twin faulting in stichtite
– previously developed reciprocal-space relationship to model broadening in R-3m with 1 variable vs 6 spherical harmonics variables
Monte-Carlo simulation of effect of 5% stacking faults ( ) and twin faults ( )
If H-K 3n = constant lc* cos(c* ^ R*)
Stichtite
• Structure refinement without the broadening correction..
and with….
2Th Degrees70 80 90 100 110 120 130 60 50 40 30 20 10 1,100,000 1,050,000 1,000,000 950,000 900,000 850,000 800,000 750,000 700,000 650,000 600,000 550,000 500,000 450,000 400,000 350,000 300,000 250,000 200,000 150,000 100,000 50,000 0 -50,000 -100,000 -150,000 stitchtite-3R1 87.92 % Lizardite 1T 0.81 % stitchtite-2H1 11.27 % 2Th Degrees70 80 90 100 110 120 130 60 50 40 30 20 10 1,100,000 1,050,000 1,000,000 950,000 900,000 850,000 800,000 750,000 700,000 650,000 600,000 550,000 500,000 450,000 400,000 350,000 300,000 250,000 200,000 150,000 100,000 50,000 0 -50,000 stitchtite-3R1 79.18 % Lizardite 1T 0.56 % stitchtite-2H1 20.25 %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
• 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,
2Th Degrees55 60 65 70 75 80 85 90 95 100 105 110 50 45 40 35 30 25 20 15 10 5 S qr t( C ou nts) 280 260 240 220 200 180 160 140 120 100 80 60 40 20 0 -20 F-Gibbsite 88.16 % Corundum 0.50 % Biotite-mica 3.96 % lizardite-1T 7.38 % capillary background 0.00 %
Fourier difference plot reveals significant residual electron density between the layers.
Fluorocronite
very recent IMA submission
• Had very little material and multi-phase → capillary geometry • However mineral of interest is PbF2; has Cu of 1525 cm-1 !
– 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 2 (MoK - 0.7Å) 10 20 30 40 Inten sity (co un ts) 2000 4000 6000 8000 10000 12000 14000 16000 18000 20000
Debye-Scherrer data with MoK .
Likely R with 0.3mm cap still >5 mirror. Likely R with 0.3mm cap <3 Data from AgK (0.56Å) with focusing
2Th Degrees20 22 24 26 28 30 32 34 36 38 40 18 16 14 12 10 8 6 C o u n ts 35,000 30,000 25,000 20,000 15,000 10,000 5,000 0 -5,000 5.046336 7.539469 8.805516 10.11759 11.38644 14.45781 15.05726 17.54717 26.22962 cassiterite 40.07 % fluorocronite 59.93 %
Carbonation of CaSiO
3under 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
In-situ carbonation with 56 bar CO2 of damp CaSiO3
60°C
56 bar CO2
Strontiodresserite
SrAl
2(CO
3)
2(OH)
4.H
2O
• 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
1mm hemisphere embedded in sill rock
(Francon Quarry, Montreal) Raw data up to 140° 2
2 (degrees CuK ) 20 40 60 80 100 120 Log Intens ity 1e+2 1e+3 1e+4 1e+5 4 hemispheres 0.5mm capillary Focusing mirror
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
Sr Al
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
Polyhedral representation of strontiodresserite structure • Hydroxides located with
bond valence sums • DFT calculations to
verify structure and
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