Slide 1
Atomic structure at the nanoscale: a 21st century materials challenge
Emil S. Bozin
Applied Physics and Applied Mathematics Department, Columbia University
Condensed Matter Physics and Material Science Department, BNL
Workshop on Characterization of Advanced Materials under Extreme Environments for Next Generation Energy Systems
September 25-26, 2009
Slide 2
Images: Igor Levin/Tom Pinnavaia/Sandra Rosenthal
Nanoporous (mesoporous) materials
Nanoparticles
Nanostructured bulk crystals
INTRO
- Complex bulk systems with interesting physical properties are often inhomogeneous on a nanometer lengthscale
high-temperature superconductors, colossal magnetoresistive materials,
high performance thermoelectric materials …
- Nano-particles, nano-tubes, nano-wires etc. important for applications optoelectronics, nanosensors, programmed release drug delivery systems…
Physical properties often critically depend on the nano-scale structure, rather than the long-range structure!
Slide 3
ROUTINE
Figures: J.S.O. Evans et al.
and M. Tucker et al.
Bragg peak info ONLY
Rietveld method
in powders
Slide 4
Example: Ho2(Ti2‑xHox)O7-x/2 ”stuffed spin ice”
300K neutron diffraction patterns (GPPD, IPNS, Argonne)
CHALLENGE
Rietveld approach assumption: crystals are perfectly periodic…
…but this is not always the case!
Slide 5
CHALLENGE
Figures: J.S.O. Evans et al.
and M. Tucker et al.
Bragg peak info ONLY
Rietveld method
in powders
Slide 6
FUTURE
Add complementary information
Extra experimental data
Theoretical constraints
Science, 316, 561 (2007).
Slide 7
Pair distribution function (PDF) gives the probability of finding an atom at a distance “r” from a given atom.
APPROACH
Slide 8
Originally: short range order in liquids and glasses
Since late 1980’s: disorder in crystalline materials