Literature DB >> 23633981

Redetermination of Nd2Ti2O7: a non-centrosymmetric structure with perovskite-type slabs.

Nobuo Ishizawa1, Keisuke Ninomiya, Terutoshi Sakakura, Jun Wang.   

Abstract

Single crystals of dineodymium(III) dititanium(IV) hepta-oxide, Nd2Ti2O7, were synthesized by the flux method and found to belong to the family of compounds with perovskite-type structural motifs. The asymmetric unit contains four Nd, four Ti and 14 O-atom sites. The perovskite-type slabs are stacked parallel to (010) with a thickness corresponding to four corner-sharing TiO6 octa-hedra. The Nd and Ti ions are displaced from the geometrical centres of respective coordin-ation polyhedra so that the net polarization occurs along the c axis. The investigated crystals were all twinned and have a halved monoclinic unit cell in comparison with the first structure determination of this compound [Scheunemann & Müller-Buschbaum (1975 ▶). J. Inorg. Nucl. Chem. 37, 2261-2263].

Entities:  

Year:  2013        PMID: 23633981      PMCID: PMC3629463          DOI: 10.1107/S1600536813005497

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For previous determinations of Nd2Ti2O7, see: Scheunemann & Müller-Buschbaum (1975 ▶); Harvey et al. (2005 ▶). For related compounds, see: Gasperin (1975 ▶); Ishizawa et al. (1980 ▶); Schmalle et al. (1993 ▶). For the extinction method, see: Becker & Coppens (1974 ▶).

Experimental

Crystal data

Nd2Ti2O7 M = 496.2 Monoclinic, a = 7.6747 (1) Å b = 13.0025 (2) Å c = 5.4640 (1) Å γ = 98.5165 (5)° V = 539.24 (2) Å3 Z = 4 Mo Kα radiation μ = 21.77 mm−1 T = 293 K 0.11 × 0.08 × 0.07 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (TWINABS; Bruker, 2008 ▶) T min = 0.134, T max = 0.206 25187 measured reflections 6608 independent reflections 6200 reflections with I > 3σ(I) R int = 0.049

Refinement

R[F 2 > 2σ(F 2)] = 0.024 wR(F 2) = 0.027 S = 1.37 6608 reflections 133 parameters Δρmax = 2.44 e Å−3 Δρmin = −1.57 e Å−3 Absolute structure: Flack (1983 ▶), 3019 Friedel pairs Flack parameter: 0.220 (12) Data collection: APEX2 (Bruker, 2008 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT; program(s) used to solve structure: SUPERFLIP (Palatinus & Chapuis, 2007 ▶); program(s) used to refine structure: JANA2006 (Petříček et al., 2006 ▶); molecular graphics: ATOMS (Dowty, 2006 ▶) and DIAMOND (Brandenburg & Putz, 2005 ▶); software used to prepare material for publication: PLATON (Spek, 2009 ▶) and publCIF (Westrip, 2010 ▶). Click here for additional data file. Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813005497/wm2720sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813005497/wm2720Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Nd2Ti2O7F(000) = 880
Mr = 496.2Dx = 6.110 Mg m3
Monoclinic, P1121Mo Kα radiation, λ = 0.71069 Å
Hall symbol: P 2zcCell parameters from 12720 reflections
a = 7.6747 (1) Åθ = 3.2–40.2°
b = 13.0025 (2) ŵ = 21.77 mm1
c = 5.4640 (1) ÅT = 293 K
β = 90°Block, purple
V = 539.24 (2) Å30.11 × 0.08 × 0.07 mm
Z = 4
Bruker APEXII CCD diffractometer6200 reflections with I > 3σ(I)
Radiation source: X-ray tubeRint = 0.049
φ and ω scansθmax = 40.3°, θmin = 1.6°
Absorption correction: multi-scan (TWINABS; Bruker, 2008)h = −13→13
Tmin = 0.134, Tmax = 0.206k = −23→23
25187 measured reflectionsl = −9→9
6608 independent reflections
Refinement on FWeighting scheme based on measured s.u.'s w = 1/(σ2(F) + 0.0001F2)
R[F2 > 2σ(F2)] = 0.024(Δ/σ)max = 0.016
wR(F2) = 0.027Δρmax = 2.44 e Å3
S = 1.37Δρmin = −1.57 e Å3
6608 reflectionsExtinction correction: B-C type 1 Gaussian isotropic (Becker & Coppens, 1974)
133 parametersExtinction coefficient: 349 (12)
0 restraintsAbsolute structure: Flack (1983), 3019 Friedel pairs
1 constraintFlack parameter: 0.220 (12)
xyzUiso*/Ueq
Nd10.22817 (5)0.906931 (15)0.75507 (4)0.00599 (5)
Nd20.14522 (4)0.574954 (15)0.34489 (4)0.00563 (5)
Nd30.71953 (5)0.881350 (15)0.74678 (4)0.00533 (5)
Nd40.64866 (4)0.612953 (17)0.28408 (4)0.00796 (5)
Ti10.47020 (19)0.87935 (5)0.25800 (16)0.00463 (15)
Ti20.41480 (19)0.67491 (5)0.78904 (13)0.00476 (16)
Ti30.96662 (19)0.88160 (5)0.25934 (16)0.00437 (15)
Ti40.92426 (19)0.67911 (5)0.78238 (14)0.00521 (16)
O10.5306 (4)0.9810 (2)0.5246 (6)0.0050 (6)*
O20.5001 (5)0.7695 (3)0.4494 (7)0.0081 (6)*
O30.4073 (5)0.5586 (2)0.5773 (6)0.0064 (5)*
O40.2248 (6)0.8923 (2)0.3081 (6)0.0099 (5)*
O50.1746 (6)0.6954 (2)0.6923 (6)0.0072 (5)*
O60.4338 (5)0.8188 (2)0.9387 (6)0.0044 (5)*
O70.3756 (5)0.6078 (3)0.0680 (7)0.0114 (7)*
O80.9591 (5)0.9796 (3)0.5265 (6)0.0079 (6)*
O90.8867 (5)0.7715 (3)0.4553 (7)0.0073 (6)*
O100.8731 (5)0.5702 (2)0.5633 (6)0.0065 (5)*
O110.7275 (6)0.9089 (2)0.1730 (6)0.0062 (5)*
O120.6740 (6)0.6933 (2)0.8421 (6)0.0084 (5)*
O130.9747 (5)0.8155 (2)0.9432 (6)0.0072 (6)*
O140.9226 (5)0.5940 (2)0.0518 (6)0.0063 (6)*
U11U22U33U12U13U23
Nd10.00488 (8)0.00601 (7)0.00701 (8)0.00062 (9)−0.00008 (13)0.00075 (7)
Nd20.00502 (8)0.00630 (7)0.00558 (8)0.00087 (10)−0.00014 (11)−0.00051 (6)
Nd30.00446 (8)0.00581 (7)0.00580 (8)0.00100 (9)−0.00004 (12)0.00079 (6)
Nd40.00543 (9)0.01077 (8)0.00800 (9)0.00231 (10)−0.00042 (12)−0.00119 (6)
Ti10.0050 (3)0.0047 (2)0.0043 (2)0.0010 (4)0.0009 (7)0.0001 (2)
Ti20.0042 (3)0.0046 (2)0.0052 (3)−0.0002 (3)0.0013 (6)−0.00020 (18)
Ti30.0041 (3)0.0049 (2)0.0044 (2)0.0014 (3)0.0011 (7)0.0000 (2)
Ti40.0055 (3)0.0045 (2)0.0056 (3)0.0003 (4)0.0013 (7)−0.0005 (2)
Nd1—O12.691 (3)Nd4—O92.710 (3)
Nd1—O1i2.631 (3)Nd4—O102.426 (4)
Nd1—O42.450 (3)Nd4—O12vi2.627 (3)
Nd1—O52.742 (3)Nd4—O142.499 (4)
Nd1—O62.312 (4)Ti1—O11.975 (3)
Nd1—O8ii2.701 (4)Ti1—O1vii2.220 (3)
Nd1—O8i2.659 (4)Ti1—O21.812 (4)
Nd1—O11i2.411 (3)Ti1—O41.935 (5)
Nd1—O13ii2.360 (4)Ti1—O6vi1.917 (3)
Nd2—O32.415 (4)Ti1—O112.010 (4)
Nd2—O52.450 (3)Ti2—O22.269 (4)
Nd2—O72.318 (4)Ti2—O31.898 (3)
Nd2—O10ii2.398 (4)Ti2—O51.973 (4)
Nd2—O10iii2.423 (3)Ti2—O62.028 (3)
Nd2—O14ii2.381 (4)Ti2—O7v1.760 (4)
Nd2—O14iv2.457 (3)Ti2—O121.989 (5)
Nd3—O12.410 (3)Ti3—O4viii1.984 (5)
Nd3—O22.621 (3)Ti3—O81.944 (4)
Nd3—O4i2.931 (3)Ti3—O8ix2.213 (3)
Nd3—O62.458 (4)Ti3—O91.820 (4)
Nd3—O82.401 (3)Ti3—O111.977 (4)
Nd3—O92.601 (4)Ti3—O13vi1.935 (3)
Nd3—O11v2.355 (3)Ti4—O5viii1.964 (4)
Nd3—O122.474 (3)Ti4—O92.196 (4)
Nd3—O132.494 (4)Ti4—O101.851 (3)
Nd4—O22.636 (4)Ti4—O121.984 (5)
Nd4—O32.472 (4)Ti4—O131.965 (3)
Nd4—O3iii2.481 (3)Ti4—O14v1.841 (3)
Nd4—O72.398 (4)
O1—Ti1—O1vii84.56 (13)O4viii—Ti3—O888.84 (15)
O1—Ti1—O293.27 (15)O4viii—Ti3—O8ix83.46 (13)
O1—Ti1—O488.45 (14)O4viii—Ti3—O9101.10 (15)
O1—Ti1—O6vi162.01 (13)O4viii—Ti3—O11164.50 (12)
O1—Ti1—O1185.18 (13)O4viii—Ti3—O13vi93.06 (16)
O1vii—Ti1—O2172.96 (16)O8—Ti3—O8ix85.77 (14)
O1vii—Ti1—O483.65 (13)O8—Ti3—O991.99 (16)
O1vii—Ti1—O6vi78.18 (12)O8—Ti3—O1186.75 (14)
O1vii—Ti1—O1180.38 (13)O8—Ti3—O13vi165.40 (14)
O2—Ti1—O4103.01 (15)O8ix—Ti3—O9174.89 (17)
O2—Ti1—O6vi103.26 (15)O8ix—Ti3—O1181.40 (13)
O2—Ti1—O1192.78 (15)O8ix—Ti3—O13vi80.08 (13)
O4—Ti1—O6vi94.59 (16)O9—Ti3—O1193.89 (15)
O4—Ti1—O11163.29 (13)O9—Ti3—O13vi101.82 (15)
O6vi—Ti1—O1186.97 (15)O11—Ti3—O13vi87.61 (16)
O2—Ti2—O384.58 (13)O5viii—Ti4—O986.72 (14)
O2—Ti2—O584.71 (13)O5viii—Ti4—O1090.78 (16)
O2—Ti2—O681.60 (13)O5viii—Ti4—O12167.53 (13)
O2—Ti2—O7v172.61 (17)O5viii—Ti4—O1387.47 (15)
O2—Ti2—O1281.44 (14)O5viii—Ti4—O14v100.64 (16)
O3—Ti2—O591.46 (16)O9—Ti4—O1082.06 (14)
O3—Ti2—O6166.09 (13)O9—Ti4—O1282.86 (14)
O3—Ti2—O7v98.63 (15)O9—Ti4—O1383.96 (14)
O3—Ti2—O1295.54 (16)O9—Ti4—O14v171.88 (16)
O5—Ti2—O685.68 (14)O10—Ti4—O1294.53 (16)
O5—Ti2—O7v101.79 (17)O10—Ti4—O13165.99 (15)
O5—Ti2—O12163.81 (12)O10—Ti4—O14v94.32 (14)
O6—Ti2—O7v95.28 (15)O12—Ti4—O1384.64 (15)
O6—Ti2—O1284.04 (14)O12—Ti4—O14v90.22 (16)
O7v—Ti2—O1291.59 (17)O13—Ti4—O14v99.66 (14)
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