Recently: nanocrystalline materials
Lanthanum Aluminate glass
J. Du and L.R. Corales, J. Non-Cryst. Solids (2007)
APPROACH
Slide 9
Raw data
Structure function
APPROACH
Slide 10
How can we get short range structural information?
Pair Distribution Function from total scattering experiments
APPROACH
Slide 11
Strength of the Pair Distribution Function
APPROACH
Slide 12
PDF primer: C60
Pair Distribution Function: info on different lengthscales
APPROACH
Slide 13
APPROACH
Slide 14
Rapid Acquisition PDF (RAPDF) at a synchrotoron:
Measuring PDFs in a few seconds
P. Chupas et al, J. Appl. Cryst. 36, 1342-1347 (2003).
APPROACH
Slide 15
P. Chupas et al, J. Appl. Cryst. 40, 463-470 (2007).
Application of a large-area, high-sensitivity, fast readout,
flat-panel GE detector based on an amorphous silicon
Nickel data, 0.03s collection time, Qmax 28 Å-1
APPROACH
Slide 16
Ni
300K Ni data from GPPD at IPNS, ANL
data
difference
model
PDF Programs
PDFgetX1
PDFgetN1
PDFgui2 (PDFfit)
1 http://nirt.pa.msu.edu
2 http://www.diffpy.org/
APPROACH
Slide 17
Local structural aspects of the metal-insulator transition
in CuIr2S4
- X-ray total scattering study -
Collaboration with: J.F. Mitchell, MSD, Argonne Nat. Lab.
Credits: Y.S. Hor, A.S. Masadeh, H.J. Kim, P. Juhas, S.J.L. Billinge
HIGHLIGHT
Slide 18
HIGHLIGHT
The role of lattice geometry – frustration
Spinel structure: AB2X4 Crystallizes in the cubic (isometric) crystal system B-sublattice – pyrochlore – corner-shared tetrahedra This sublattice promotes frustration, interesting physics arises in spin (AF interactions) and charge (half-integer valence) sectors!