research papers
The deformation electron density of ferroelectric sodium nitrite has been determined from X-ray diffraction data at 30 K, using Hirshfeld deformation functions. Owing to the strong correlation between odd terms of the deformation coefficients, constraints were imposed in the refinement. The net charges for Na, N and O atoms were estimated to be 0.27, 0.20 and -0.24 e, respectively. The calculated spontaneous polarization using these net charges and atomic dipole terms, 7.8 µC cm-2, is much closer to the recently measured value, 12 µC cm-2, as compared with the value calculated from the formal point charges (74 µC cm-2).
Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S010876819901054X/os0030sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S010876819901054X/os0030sup2.hkl |
Computing details top
Data collection: DIF4; cell refinement: LATCON (Lundgren, 1983); data reduction: STOEDATRED (Lundgren, 1983); program(s) used to refine structure: DUPALS (Lundgren, 1983).
Sodium Nitrite top
Crystal data top
NNaO2 | F(000) = 68 |
Mr = 69.0 | Dx = 2.203 Mg m−3 |
Orthorhombic, Im2m | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: I -2 -2 | Cell parameters from 15 reflections |
a = 3.5024 (6) Å | θ = 26.4–27.4° |
b = 5.5209 (5) Å | µ = 0.39 mm−1 |
c = 5.3789 (9) Å | T = 30 K |
V = 104.01 (2) Å3 | Hexagonal prism, colourless |
Z = 2 | 0.22 × 0.18 × 0.08 mm |
Data collection top
HUBER/STOE/ARACOR diffractometer | 384 reflections with I > −3σ(I) |
Radiation source: fine focus Philips Mo tube | Rint = 0.012 |
Graphite monochromator | θmax = 53.0°, θmin = 5.3° |
ω/2θ scans | h = −7→7 |
Absorption correction: integration ABSSTOE (Lundgren, 1983) | k = −12→12 |
Tmin = 0.923, Tmax = 0.948 | l = −12→0 |
1396 measured reflections | 5 standard reflections every 240 min |
384 independent reflections | intensity decay: 0.1% |
Refinement top
Refinement on F2 | Weighting scheme based on measured s.u.'s w = 1/σ2(F2) |
Least-squares matrix: full | (Δ/σ)max = 0.031 |
R[F2 > 2σ(F2)] = 0.014 | Δρmax = 0.11 e Å−3 |
wR(F2) = 0.022 | Δρmin = −0.12 e Å−3 |
S = 1.79 | Extinction correction: Becker & Coppens (1975) type 1 Lorentzian isotropic |
1390 reflections | Extinction coefficient: '0.177E4 (7) |
68 parameters |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Na | 0 | 0.58833 (4) | 0 | 0.00573 (3) | .25 |
N | 0 | 0.12277 (4) | 0 | 0.00595 (4) | .25 |
O | 0 | 0 | 0.19646 (3) | 0.00685 (4) | .5 |
Atomic displacement parameters (Å2) top
U11 | U22 | U33 | U12 | U13 | U23 | |
Na | 0.00623 (3) | 0.00538 (3) | 0.00559 (3) | 0 | 0 | 0 |
N | 0.00836 (4) | 0.00461 (5) | 0.00490 (4) | 0 | 0 | 0 |
O | 0.00886 (4) | 0.00706 (5) | 0.00462 (4) | 0 | 0 | 0.00076 (4) |
Geometric parameters (Å, º) top
Na—N | 2.5703 (3) | Na—Oii | 2.4434 (3) |
Na—Oi | 2.5064 (2) | N—O | 1.2554 (1) |
O—N—Oiii | 114.65 (1) |
Symmetry codes: (i) x, y+1, z; (ii) x−1/2, y+1/2, z−1/2; (iii) x, y, −z. |