Literature DB >> 21201028

Tricaesium tris-(pyridine-2,6-dicarboxyl-ato-κO,N,O)lutetium(III) octa-hydrate.

Vincent Legrand, Flavien Aubert, Anthony D'Aléo, Philippe Rabiller, Olivier Maury.   

Abstract

Colourless block crystals of the title compound, Cs(3)[Lun class="Chemical">(dipic)(3)]·8H(2)O [dipic is dipicolinate or pyridine-2,6-dicarboxyl-ate, C(7)H(3)NO(4)] were synthesized by slow evaporation of the solvent. The crystal structure of this Lu(III)-complex, isostructural with the Dy(III) and Eu(III) complexes, was determined from a crystal twinned by inversion and consists of discrete [Lu(dipic)(3)](3-) anions, Cs(+) cations and water mol-ecules involving hydrogen bonding. The Lu atom lies on a twofold rotation axis and is coordinated by six O atoms and three N atoms of three dipicolinate ligands. One Cs atom is also on a twofold axis. The unit cell can be regarded as successive layers along the crystallographic c-axis formed by [Lu(dipic)(3)](3-) anionic planes and [Cs(+), H(2)O] cationic planes. In the crystal structure, although the H atoms attached to water mol-ecules could not be located, short O-O contacts clearly indicate the occurrence of an intricate hydrogen-bonded network through contacts with other water mol-ecules, Cs cations or with the O atoms of the dipicolinate ligands.

Entities:  

Year:  2008        PMID: 21201028      PMCID: PMC2959249          DOI: 10.1107/S1600536808029243

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


Related literature

For potential applications of lanthanide complexes as second-order non-linear optical materials, see: Tancrez et al. (2005 ▶); Sénéchal et al. (2004 ▶). For the isostructural EuIII complex, see: Brayshaw et al. (1995 ▶). For other related complexes, see: Murray et al. (1990 ▶). For related literature, see: Flack & Bernardinelli (1999 ▶, 2000 ▶).

Experimental

Crystal data

Cs3[Lu(C7H3NO4)3]·8H2O M = 1213.14 Orthorhombic, a = 10.0406 (2) Å b = 17.8109 (6) Å c = 18.4221 (5) Å V = 3294.46 (16) Å3 Z = 4 Mo Kα radiation μ = 6.36 mm−1 T = 100 (2) K 0.20 × 0.19 × 0.19 mm

Data collection

Oxford Diffraction Xcalibur–Sapphire3 diffractometer Absorption correction: Gaussian (ABSORB; DeTitta, 1985 ▶) T min = 0.307, T max = 0.425 51066 measured reflections 3520 independent reflections 3491 reflections with I > 2σ(I) R int = 0.045

Refinement

R[F 2 > 2σ(F 2)] = 0.025 wR(F 2) = 0.063 S = 1.46 3520 reflections 208 parameters H-atom parameters constrained Δρmax = 3.00 e Å−3 Δρmin = −0.94 e Å−3 Absolute structure: Flack (1983 ▶), 1501 Friedel pairs Flack parameter: 0.270 (12) Data collection: CrysAlis CCD (Oxford Diffraction 2006 ▶); cell refinement: CrysAlis n class="Disease">RED (Oxford Diffraction 2006 ▶); data reduction: SORTAV (Blessing, 1989 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808029243/dn2357sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808029243/dn2357Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Cs3[Lu(C7H3NO4)3]·8H2OF(000) = 2312
Mr = 1213.14Dx = 2.446 Mg m3
Orthorhombic, C2221Mo Kα radiation, λ = 0.71073 Å
Hall symbol: C 2c 2Cell parameters from 17659 reflections
a = 10.0406 (2) Åθ = 3.2–59.9°
b = 17.8109 (6) ŵ = 6.36 mm1
c = 18.4221 (5) ÅT = 100 K
V = 3294.46 (16) Å3Block, colourless
Z = 40.20 × 0.19 × 0.19 mm
Oxford Diffraction Xcalibur-Sapphire3 diffractometer3520 independent reflections
Radiation source: fine-focus sealed tube3491 reflections with I > 2σ(I)
graphiteRint = 0.045
ω scansθmax = 27.0°, θmin = 3.2°
Absorption correction: gaussian (ABSORB; DeTitta, 1985)h = −12→12
Tmin = 0.308, Tmax = 0.425k = −22→22
51066 measured reflectionsl = −23→23
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025H-atom parameters constrained
wR(F2) = 0.063w = 1/[σ2(Fo2) + (0.0149P)2 + 27.044P] where P = (Fo2 + 2Fc2)/3
S = 1.46(Δ/σ)max < 0.001
3520 reflectionsΔρmax = 3.00 e Å3
208 parametersΔρmin = −0.94 e Å3
0 restraintsAbsolute structure: Flack (1983),1501 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.270 (12)
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/UeqOcc. (<1)
Lu10.75054 (5)0.00000.00000.00950 (7)
Cs10.74407 (4)0.021678 (17)−0.24335 (2)0.01702 (8)
Cs20.5000−0.26389 (3)−0.25000.01796 (11)
N110.8713 (4)−0.1197 (2)−0.0042 (3)0.0107 (8)
O110.6846 (4)−0.0835 (2)−0.0950 (2)0.0149 (8)
O120.7226 (5)−0.1846 (3)−0.1649 (2)0.0228 (12)
O131.0389 (5)−0.0907 (3)0.1601 (2)0.0174 (11)
O140.9174 (4)−0.01382 (19)0.0906 (2)0.0124 (8)
C120.9612 (6)−0.1355 (3)0.0466 (3)0.0131 (12)
C131.0349 (6)−0.2016 (3)0.0468 (3)0.0187 (13)
H131.1001−0.20890.08190.022*
C141.0140 (14)−0.2518 (3)−0.0006 (8)0.040 (2)
H141.0567−0.29800.00260.048*
C150.9185 (7)−0.2357 (4)−0.0624 (3)0.0199 (13)
H150.9073−0.2688−0.10100.024*
C160.8496 (6)−0.1693 (3)−0.0580 (3)0.0132 (11)
C170.7438 (8)−0.1440 (3)−0.1112 (3)0.0146 (6)
C180.9756 (6)−0.0754 (3)0.1041 (4)0.0146 (6)
N210.5071 (8)0.00000.00000.0173 (12)
O210.4794 (7)−0.1104 (3)0.1573 (3)0.0323 (15)
O220.6543 (5)−0.0785 (2)0.0880 (2)0.0168 (9)
C220.4415 (7)−0.0390 (4)0.0490 (3)0.0242 (9)
C230.3047 (7)−0.0426 (4)0.0509 (3)0.0242 (9)
H230.2584−0.07190.08430.029*
C240.2430 (13)0.00000.00000.0242 (9)
H240.15030.00000.00000.029*
C250.5310 (6)−0.0805 (4)0.1040 (4)0.0146 (6)
O1W0.7467 (9)−0.1739 (4)−0.3818 (4)0.0584 (17)
O2W0.9514 (7)−0.0907 (4)−0.3228 (4)0.0424 (18)
O3W0.5456 (5)−0.0888 (3)−0.3207 (3)0.0240 (12)
O4WA0.6970 (8)0.2031 (4)−0.2207 (6)0.032 (3)0.69 (2)
O4WB0.7228 (15)0.1956 (8)−0.1715 (11)0.023 (6)0.31 (2)
U11U22U33U12U13U23
Lu10.00740 (14)0.01013 (12)0.01097 (13)0.0000.000−0.00081 (10)
Cs10.01540 (16)0.02237 (15)0.01327 (15)−0.00244 (13)0.00109 (19)−0.00051 (11)
Cs20.0245 (3)0.01430 (19)0.0151 (2)0.000−0.0028 (2)0.000
N110.008 (2)0.0127 (18)0.011 (2)−0.0017 (15)0.0012 (18)0.0004 (17)
O110.013 (2)0.013 (2)0.018 (2)−0.0015 (16)−0.0019 (16)−0.0004 (16)
O120.023 (4)0.023 (2)0.022 (2)0.0013 (18)−0.0084 (19)−0.0097 (17)
O130.019 (3)0.023 (3)0.010 (2)0.0014 (18)−0.0035 (16)0.0022 (17)
O140.010 (2)0.008 (2)0.018 (2)0.0010 (14)−0.0021 (15)−0.0017 (14)
C120.015 (3)0.011 (2)0.014 (3)−0.0009 (19)0.001 (2)0.002 (2)
C130.018 (4)0.017 (3)0.021 (3)0.004 (2)−0.004 (2)0.001 (2)
C140.033 (6)0.023 (3)0.066 (5)−0.003 (3)−0.040 (5)0.009 (3)
C150.026 (4)0.018 (3)0.016 (3)0.007 (3)−0.002 (2)−0.005 (2)
C160.015 (3)0.012 (3)0.012 (3)−0.002 (2)0.003 (2)0.001 (2)
C170.0135 (16)0.0138 (13)0.0166 (13)−0.0096 (16)0.0027 (15)−0.0028 (10)
C180.0135 (16)0.0138 (13)0.0166 (13)−0.0096 (16)0.0027 (15)−0.0028 (10)
N210.009 (3)0.027 (3)0.016 (3)0.0000.000−0.010 (3)
O210.038 (4)0.039 (3)0.021 (2)−0.021 (3)0.014 (2)−0.009 (2)
O220.020 (3)0.013 (2)0.0168 (19)−0.0027 (17)0.0040 (17)−0.0020 (15)
C220.0106 (19)0.048 (2)0.0143 (17)−0.007 (2)0.0024 (15)−0.0146 (17)
C230.0106 (19)0.048 (2)0.0143 (17)−0.007 (2)0.0024 (15)−0.0146 (17)
C240.0106 (19)0.048 (2)0.0143 (17)−0.007 (2)0.0024 (15)−0.0146 (17)
C250.0135 (16)0.0138 (13)0.0166 (13)−0.0096 (16)0.0027 (15)−0.0028 (10)
O1W0.046 (4)0.079 (5)0.051 (3)0.016 (5)−0.002 (4)−0.012 (3)
O2W0.047 (4)0.021 (3)0.059 (4)0.003 (3)0.028 (3)0.001 (3)
O3W0.018 (3)0.032 (3)0.022 (3)−0.004 (2)−0.005 (2)0.004 (2)
O4WA0.028 (4)0.030 (4)0.039 (6)−0.002 (3)−0.003 (3)0.007 (3)
O4WB0.012 (11)0.018 (7)0.038 (13)0.005 (5)0.011 (7)0.015 (6)
Lu1—O22i2.348 (4)O11—C171.267 (8)
Lu1—O222.348 (4)O12—C171.244 (7)
Lu1—O142.377 (4)O13—C181.242 (9)
Lu1—O14i2.377 (4)O13—Cs1ix3.070 (5)
Lu1—O112.390 (4)O13—Cs2x3.100 (5)
Lu1—O11i2.390 (4)O13—Cs1i3.553 (5)
Lu1—N212.445 (8)O14—C181.267 (8)
Lu1—N11i2.454 (4)O14—Cs1i3.312 (4)
Lu1—N112.454 (4)C12—C131.390 (8)
Lu1—Cs14.5002 (4)C12—C181.513 (8)
Lu1—Cs1i4.5002 (4)C13—C141.267 (13)
Cs1—O13ii3.070 (5)C13—Cs2x3.810 (6)
Cs1—O3W3.142 (5)C13—H130.9300
Cs1—O22i3.167 (4)C14—C151.517 (12)
Cs1—O2W3.237 (6)C14—H140.9300
Cs1—O4WA3.293 (8)C15—C161.373 (9)
Cs1—O21iii3.299 (6)C15—H150.9300
Cs1—O14i3.312 (4)C16—C171.514 (9)
Cs1—O113.367 (4)C18—Cs1i3.592 (6)
Cs1—O4WB3.375 (16)N21—C22i1.315 (8)
Cs1—O21i3.474 (6)N21—C221.315 (8)
Cs1—C25i3.502 (6)O21—C251.230 (9)
Cs1—O13i3.553 (5)O21—Cs1xi3.299 (6)
Cs2—O123.073 (5)O21—Cs1i3.474 (6)
Cs2—O12iv3.073 (5)O22—C251.273 (8)
Cs2—O13v3.100 (5)O22—Cs1i3.167 (4)
Cs2—O13vi3.100 (5)C22—C231.376 (10)
Cs2—O4WAvii3.145 (8)C22—C251.544 (10)
Cs2—O4WAviii3.145 (8)C23—C241.356 (9)
Cs2—O4WBvii3.219 (14)C23—Cs1xi3.840 (6)
Cs2—O4WBviii3.219 (14)C23—H230.9300
Cs2—O3W3.410 (6)C24—C23i1.356 (9)
Cs2—O3Wiv3.410 (6)C24—H240.9300
Cs2—C13v3.810 (6)C25—Cs1i3.502 (6)
Cs2—C13vi3.810 (6)O3W—Cs1iv3.705 (6)
N11—C121.330 (7)O4WA—Cs2xii3.145 (8)
N11—C161.345 (7)O4WB—Cs2xii3.219 (14)
O22i—Lu1—O22131.4 (2)O13v—Cs2—O4WAviii82.77 (19)
O22i—Lu1—O14146.72 (14)O13vi—Cs2—O4WAviii79.26 (18)
O22—Lu1—O1475.16 (15)O4WAvii—Cs2—O4WAviii158.5 (3)
O22i—Lu1—O14i75.16 (15)O12—Cs2—O4WBvii120.2 (4)
O22—Lu1—O14i146.72 (14)O12iv—Cs2—O4WBvii72.8 (3)
O14—Lu1—O14i90.4 (2)O13v—Cs2—O4WBvii86.8 (3)
O22i—Lu1—O1175.58 (13)O13vi—Cs2—O4WBvii71.4 (3)
O22—Lu1—O1191.20 (14)O4WAvii—Cs2—O4WBvii17.2 (3)
O14—Lu1—O11130.16 (14)O4WAviii—Cs2—O4WBvii150.6 (3)
O14i—Lu1—O1175.28 (14)O12—Cs2—O4WBviii72.8 (3)
O22i—Lu1—O11i91.20 (14)O12iv—Cs2—O4WBviii120.2 (4)
O22—Lu1—O11i75.58 (13)O13v—Cs2—O4WBviii71.4 (3)
O14—Lu1—O11i75.28 (14)O13vi—Cs2—O4WBviii86.8 (3)
O14i—Lu1—O11i130.16 (14)O4WAvii—Cs2—O4WBviii150.6 (3)
O11—Lu1—O11i147.8 (2)O4WAviii—Cs2—O4WBviii17.2 (3)
O22i—Lu1—N2165.71 (12)O4WBvii—Cs2—O4WBviii154.1 (5)
O22—Lu1—N2165.71 (12)O12—Cs2—O3W71.14 (12)
O14—Lu1—N21134.81 (10)O12iv—Cs2—O3W58.84 (12)
O14i—Lu1—N21134.81 (10)O13v—Cs2—O3W125.24 (14)
O11—Lu1—N2173.90 (11)O13vi—Cs2—O3W162.07 (13)
O11i—Lu1—N2173.90 (11)O4WAvii—Cs2—O3W111.48 (18)
O22i—Lu1—N11i73.00 (16)O4WAviii—Cs2—O3W88.59 (17)
O22—Lu1—N11i134.33 (16)O4WBvii—Cs2—O3W119.5 (3)
O14—Lu1—N11i73.72 (14)O4WBviii—Cs2—O3W85.3 (3)
O14i—Lu1—N11i65.42 (14)O12—Cs2—O3Wiv58.84 (12)
O11—Lu1—N11i134.47 (16)O12iv—Cs2—O3Wiv71.14 (12)
O11i—Lu1—N11i64.75 (15)O13v—Cs2—O3Wiv162.07 (13)
N21—Lu1—N11i119.60 (10)O13vi—Cs2—O3Wiv125.24 (14)
O22i—Lu1—N11134.33 (16)O4WAvii—Cs2—O3Wiv88.59 (17)
O22—Lu1—N1173.00 (16)O4WAviii—Cs2—O3Wiv111.48 (19)
O14—Lu1—N1165.42 (14)O4WBvii—Cs2—O3Wiv85.3 (3)
O14i—Lu1—N1173.72 (14)O4WBviii—Cs2—O3Wiv119.5 (3)
O11—Lu1—N1164.75 (15)O3W—Cs2—O3Wiv47.76 (19)
O11i—Lu1—N11134.47 (16)O12—Cs2—C13v129.96 (13)
N21—Lu1—N11119.60 (10)O12iv—Cs2—C13v60.42 (13)
N11i—Lu1—N11120.8 (2)O13v—Cs2—C13v47.80 (13)
O22i—Lu1—Cs141.88 (11)O13vi—Cs2—C13v113.68 (13)
O22—Lu1—Cs1137.11 (11)O4WAvii—Cs2—C13v92.8 (2)
O14—Lu1—Cs1135.91 (10)O4WAviii—Cs2—C13v83.7 (2)
O14i—Lu1—Cs145.74 (10)O4WBvii—Cs2—C13v109.0 (4)
O11—Lu1—Cs147.15 (10)O4WBviii—Cs2—C13v66.5 (4)
O11i—Lu1—Cs1132.23 (10)O3W—Cs2—C13v77.57 (13)
N21—Lu1—Cs189.173 (8)O3Wiv—Cs2—C13v120.70 (13)
N11i—Lu1—Cs187.94 (12)O12—Cs2—C13vi60.42 (13)
N11—Lu1—Cs192.88 (12)O12iv—Cs2—C13vi129.96 (13)
O22i—Lu1—Cs1i137.11 (11)O13v—Cs2—C13vi113.68 (13)
O22—Lu1—Cs1i41.88 (11)O13vi—Cs2—C13vi47.80 (13)
O14—Lu1—Cs1i45.74 (10)O4WAvii—Cs2—C13vi83.7 (2)
O14i—Lu1—Cs1i135.91 (10)O4WAviii—Cs2—C13vi92.8 (2)
O11—Lu1—Cs1i132.23 (10)O4WBvii—Cs2—C13vi66.5 (4)
O11i—Lu1—Cs1i47.15 (10)O4WBviii—Cs2—C13vi109.0 (4)
N21—Lu1—Cs1i89.173 (8)O3W—Cs2—C13vi120.70 (13)
N11i—Lu1—Cs1i92.88 (12)O3Wiv—Cs2—C13vi77.57 (13)
N11—Lu1—Cs1i87.94 (12)C13v—Cs2—C13vi161.41 (18)
Cs1—Lu1—Cs1i178.347 (17)C12—N11—C16119.3 (5)
O13ii—Cs1—O3W115.98 (14)C12—N11—Lu1119.8 (4)
O13ii—Cs1—O22i126.72 (12)C16—N11—Lu1120.9 (4)
O3W—Cs1—O22i115.44 (13)C17—O11—Lu1124.9 (4)
O13ii—Cs1—O2W61.89 (12)C17—O11—Cs1101.4 (3)
O3W—Cs1—O2W79.37 (13)Lu1—O11—Cs1101.50 (14)
O22i—Cs1—O2W142.10 (16)C17—O12—Cs2142.9 (5)
O13ii—Cs1—O4WA77.43 (18)C18—O13—Cs1ix139.2 (4)
O3W—Cs1—O4WA125.53 (19)C18—O13—Cs2x124.2 (4)
O22i—Cs1—O4WA62.0 (2)Cs1ix—O13—Cs2x96.56 (13)
O2W—Cs1—O4WA139.14 (19)C18—O13—Cs1i81.8 (4)
O13ii—Cs1—O21iii88.27 (12)Cs1ix—O13—Cs1i101.70 (14)
O3W—Cs1—O21iii67.47 (13)Cs2x—O13—Cs1i87.33 (12)
O22i—Cs1—O21iii98.92 (14)C18—O14—Lu1123.5 (4)
O2W—Cs1—O21iii118.85 (19)C18—O14—Cs1i92.2 (4)
O4WA—Cs1—O21iii60.2 (2)Lu1—O14—Cs1i103.33 (13)
O13ii—Cs1—O14i97.84 (11)N11—C12—C13122.8 (5)
O3W—Cs1—O14i133.79 (12)N11—C12—C18114.0 (5)
O22i—Cs1—O14i52.77 (10)C13—C12—C18123.1 (5)
O2W—Cs1—O14i91.16 (16)C14—C13—C12120.5 (7)
O4WA—Cs1—O14i90.54 (19)C14—C13—Cs2x123.1 (7)
O21iii—Cs1—O14i148.13 (12)C12—C13—Cs2x95.2 (4)
O13ii—Cs1—O11144.99 (12)C14—C13—H13119.7
O3W—Cs1—O1184.68 (12)C12—C13—H13119.7
O22i—Cs1—O1152.66 (10)Cs2x—C13—H1350.1
O2W—Cs1—O1197.89 (14)C13—C14—C15119.3 (7)
O4WA—Cs1—O11114.7 (2)C13—C14—H14120.4
O21iii—Cs1—O11126.59 (13)C15—C14—H14120.4
O14i—Cs1—O1151.67 (10)C16—C15—C14115.9 (6)
O13ii—Cs1—O4WB84.6 (3)C16—C15—H15122.1
O3W—Cs1—O4WB135.4 (3)C14—C15—H15122.1
O22i—Cs1—O4WB48.2 (3)N11—C16—C15121.9 (5)
O2W—Cs1—O4WB141.8 (3)N11—C16—C17113.3 (5)
O4WA—Cs1—O4WB16.4 (3)C15—C16—C17124.8 (5)
O21iii—Cs1—O4WB74.7 (4)O12—C17—O11127.0 (7)
O14i—Cs1—O4WB74.8 (4)O12—C17—C16117.5 (6)
O11—Cs1—O4WB100.4 (3)O11—C17—C16115.5 (5)
O13ii—Cs1—O21i128.72 (14)O12—C17—Cs186.7 (3)
O3W—Cs1—O21i90.39 (15)O11—C17—Cs159.6 (3)
O22i—Cs1—O21i39.15 (12)C16—C17—Cs1129.9 (4)
O2W—Cs1—O21i168.30 (16)O13—C18—O14126.1 (6)
O4WA—Cs1—O21i52.14 (18)O13—C18—C12118.4 (6)
O21iii—Cs1—O21i61.01 (17)O14—C18—C12115.5 (5)
O14i—Cs1—O21i91.90 (11)O13—C18—Cs1i78.2 (4)
O11—Cs1—O21i75.32 (12)O14—C18—Cs1i67.2 (3)
O4WB—Cs1—O21i49.9 (3)C12—C18—Cs1i128.8 (4)
O13ii—Cs1—C25i137.62 (15)C22i—N21—C22119.9 (9)
O3W—Cs1—C25i97.62 (14)C22i—N21—Lu1120.0 (4)
O22i—Cs1—C25i21.25 (13)C22—N21—Lu1120.0 (4)
O2W—Cs1—C25i155.39 (16)C25—O21—Cs1xi121.5 (5)
O4WA—Cs1—C25i61.7 (2)C25—O21—Cs1i81.1 (4)
O21iii—Cs1—C25i81.26 (15)Cs1xi—O21—Cs1i92.82 (13)
O14i—Cs1—C25i73.18 (12)C25—O22—Lu1125.2 (4)
O11—Cs1—C25i57.51 (13)C25—O22—Cs1i94.4 (4)
O4WB—Cs1—C25i53.1 (3)Lu1—O22—Cs1i108.45 (15)
O21i—Cs1—C25i20.31 (14)N21—C22—C23122.8 (7)
O13ii—Cs1—O13i61.34 (14)N21—C22—C25114.3 (6)
O3W—Cs1—O13i160.15 (13)C23—C22—C25122.8 (6)
O22i—Cs1—O13i74.71 (11)C24—C23—C22114.3 (8)
O2W—Cs1—O13i82.72 (16)C24—C23—Cs1xi124.7 (4)
O4WA—Cs1—O13i74.07 (18)C22—C23—Cs1xi98.5 (4)
O21iii—Cs1—O13i129.85 (12)C24—C23—H23122.8
O14i—Cs1—O13i37.82 (10)C22—C23—H23122.8
O11—Cs1—O13i89.41 (11)Cs1xi—C23—H2348.6
O4WB—Cs1—O13i64.3 (3)C23i—C24—C23125.6 (11)
O21i—Cs1—O13i106.43 (12)C23i—C24—H24117.2
C25i—Cs1—O13i95.10 (14)C23—C24—H24117.2
O12—Cs2—O12iv125.26 (18)O21—C25—O22127.3 (7)
O12—Cs2—O13v138.44 (13)O21—C25—C22119.0 (6)
O12iv—Cs2—O13v91.16 (13)O22—C25—C22113.6 (5)
O12—Cs2—O13vi91.16 (13)O21—C25—Cs1i78.6 (4)
O12iv—Cs2—O13vi138.44 (13)O22—C25—Cs1i64.4 (3)
O13v—Cs2—O13vi66.60 (18)C22—C25—Cs1i133.9 (4)
O12—Cs2—O4WAvii134.6 (2)Cs1—O3W—Cs2119.00 (16)
O12iv—Cs2—O4WAvii58.0 (2)Cs1—O3W—Cs1iv91.19 (14)
O13v—Cs2—O4WAvii79.26 (18)Cs2—O3W—Cs1iv104.99 (14)
O13vi—Cs2—O4WAvii82.77 (19)Cs2xii—O4WA—Cs191.3 (2)
O12—Cs2—O4WAviii58.0 (2)Cs2xii—O4WB—Cs188.6 (4)
O12iv—Cs2—O4WAviii134.6 (2)
  4 in total

1.  Absolute structure and absolute configuration.

Authors: 
Journal:  Acta Crystallogr A       Date:  1999-09-01       Impact factor: 2.290

2.  First lanthanide dipolar complexes for second-order nonlinear optics.

Authors:  Katell Sénéchal; Loïc Toupet; Isabelle Ledoux; Joseph Zyss; Hubert Le Bozec; Olivier Maury
Journal:  Chem Commun (Camb)       Date:  2004-09-08       Impact factor: 6.222

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

4.  Lanthanide complexes for second order nonlinear optics: evidence for the direct contribution of f electrons to the quadratic hyperpolarizability.

Authors:  Nicolas Tancrez; Christophe Feuvrie; Isabelle Ledoux; Joseph Zyss; Loïc Toupet; Hubert Le Bozec; Olivier Maury
Journal:  J Am Chem Soc       Date:  2005-10-05       Impact factor: 15.419

  4 in total

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