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Seven diffraction patterns were collected on a 100 nm Gd-doped ceria layer deposited on a silicon wafer under asymmetric reflection conditions. As the grazing-incidence angle decreases, large shifts (a few tens of degrees) and broadenings (two degrees below the critical angle) of hkl reflections are apparent in the diffraction patterns. The impact of these aberrations on the positions and profiles of the Bragg peaks is studied in detail in this work. On the basis of this analysis, diffraction patterns collected at different angles of incidence could then be refined using a unique structural model. From these refinements, the evolution of the coherent diffracting domains, the strain and the microstrain can clearly be traced as a function of depth.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889811042294/hx5133sup1.cif
Contains datablocks global, ce02-1, ce02-02

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889811042294/hx5133ce02-1sup2.rtv
Contains datablocks ceO2-1, ceO2-1-unknown

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889811042294/hx5133ce02-02sup3.rtv
Contains datablock ceO2-02

Computing details top

For both structures, data collection: no; cell refinement: yes; data reduction: no; program(s) used to solve structure: yes; program(s) used to refine structure: yes; molecular graphics: no; software used to prepare material for publication: no.

ceria (ce02-1) top
Crystal data top
Gd0.1Ce0.9O1.95Cu Kαlpha 1 and 2 radiation
Cubic, FM3MT = 295 K
a = 5.425475 ÅParticle morphology: mesoporous
V = 159.69 Å3black
Z = 4rectangular, 60 × 70 mm
Data collection top
No slits
diffractometer
Data collection mode: reflection
Radiation source: focus line, Godel mirrorScan method: step
Specimen mounting: thin film deposited on a Si(100) wafer2θmin = 10°, 2θmax = 135°, 2θstep = 0.028°
Refinement top
Least-squares matrix: full with fixed elements per cycleExcluded region(s): no
Rp = 0.054Profile function: pseudo voigt
Rwp = 0.04111 parameters
Rexp = 0.015Weighting scheme based on measured s.u.'s
RBragg = 0.037Background function: rational function of sin(theta)
4395 data pointsPreferred orientation correction: no
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Gd0000.8328800.0020833
Ce0000.8328800.01875
O0.250.250.250.8328800.0416667
ceria (ce02-02) top
Crystal data top
Gd0.1Ce0.9O1.95Cu Kαlpha 1 and 2 radiation
Cubic, FM3MT = 295 K
a = 5.412920 ÅParticle morphology: mesoporous
V = 158.59 Å3black
Z = 4rectangular, 60 × 70 mm
Data collection top
No slits
diffractometer
Data collection mode: reflection
Radiation source: focus line, Godel mirrorScan method: step
Specimen mounting: thin film deposited on a Si(100) wafer2θmin = 10°, 2θmax = 133°, 2θstep = 0.056°
Refinement top
Least-squares matrix: full with fixed elements per cycleExcluded region(s): no
Rp = 0.052Profile function: pseudo voigt
Rwp = 0.01511 parameters
Rexp = 0.008Weighting scheme based on measured s.u.'s
RBragg = 0.025Background function: rational function of sin(theta)
2197 data pointsPreferred orientation correction: no
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Gd0001.1027610.0020833
Ce0001.1027610.01875
O0.250.250.251.1027610.0416667
 

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