
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
![]() | Crystallographic Information File (CIF) https://doi.org/10.1107/S0021889811042294/hx5133sup1.cif |
![]() | Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889811042294/hx5133ce02-1sup2.rtv |
![]() | Rietveld powder data file (CIF format) https://doi.org/10.1107/S0021889811042294/hx5133ce02-02sup3.rtv |
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
Gd0.1Ce0.9O1.95 | Cu Kαlpha 1 and 2 radiation |
Cubic, FM3M | T = 295 K |
a = 5.425475 Å | Particle morphology: mesoporous |
V = 159.69 Å3 | black |
Z = 4 | rectangular, 60 × 70 mm |
Data collection top
No slits diffractometer | Data collection mode: reflection |
Radiation source: focus line, Godel mirror | Scan method: step |
Specimen mounting: thin film deposited on a Si(100) wafer | 2θmin = 10°, 2θmax = 135°, 2θstep = 0.028° |
Refinement top
Least-squares matrix: full with fixed elements per cycle | Excluded region(s): no |
Rp = 0.054 | Profile function: pseudo voigt |
Rwp = 0.041 | 11 parameters |
Rexp = 0.015 | Weighting scheme based on measured s.u.'s |
RBragg = 0.037 | Background function: rational function of sin(theta) |
4395 data points | Preferred orientation correction: no |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Gd | 0 | 0 | 0 | 0.832880 | 0.0020833 |
Ce | 0 | 0 | 0 | 0.832880 | 0.01875 |
O | 0.25 | 0.25 | 0.25 | 0.832880 | 0.0416667 |
ceria (ce02-02) top
Crystal data top
Gd0.1Ce0.9O1.95 | Cu Kαlpha 1 and 2 radiation |
Cubic, FM3M | T = 295 K |
a = 5.412920 Å | Particle morphology: mesoporous |
V = 158.59 Å3 | black |
Z = 4 | rectangular, 60 × 70 mm |
Data collection top
No slits diffractometer | Data collection mode: reflection |
Radiation source: focus line, Godel mirror | Scan method: step |
Specimen mounting: thin film deposited on a Si(100) wafer | 2θmin = 10°, 2θmax = 133°, 2θstep = 0.056° |
Refinement top
Least-squares matrix: full with fixed elements per cycle | Excluded region(s): no |
Rp = 0.052 | Profile function: pseudo voigt |
Rwp = 0.015 | 11 parameters |
Rexp = 0.008 | Weighting scheme based on measured s.u.'s |
RBragg = 0.025 | Background function: rational function of sin(theta) |
2197 data points | Preferred orientation correction: no |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Gd | 0 | 0 | 0 | 1.102761 | 0.0020833 |
Ce | 0 | 0 | 0 | 1.102761 | 0.01875 |
O | 0.25 | 0.25 | 0.25 | 1.102761 | 0.0416667 |