Literature DB >> 23723790

Poly[tetra-aqua-(5-hy-droxy-pyridin-1-ium-3-carboxyl-ato-κO (3))tris-(μ-oxalato-κ(4) O (1),O (2):O (1'),O (2'))dieuropium(III)].

Shan-Shan Xu1, Jun-Long Mi, Hong-Ji Chen.   

Abstract

In the title compound, [Eu2(C6H5NO3)2(C2O4)3(H2O)4] n , the Eu(III) atom is bonded to one O atom from a monodentate 5-hy-droxy-pyridin-1-ium-3-carboxyl-ate ligand, six O atoms from three oxalate ligands and two water mol-ecules, exhibiting a highly distorted tricapped trigonal geometry. Three independent oxalate ligands, each lying on an inversion center, bridge the Eu(III) atoms, forming a brickwall-like layer parallel to (001), which is stabilized by intra-layer O-H⋯O hydrogen bonds. The layers are further linked through inter-layer O-H⋯O and N-H⋯O hydrogen bonds and π-π inter-actions between the pyridine rings [centroid-centroid distance = 3.5741 (14) Å] into a three-dimensional supra-molecular network.

Entities:  

Year:  2013        PMID: 23723790      PMCID: PMC3647824          DOI: 10.1107/S1600536813011057

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


Related literature

For background to metal complexes of pyridine-carb­oxy­lic derivatives, see: Black et al. (2009 ▶); Cañadillas-Delgado et al. (2010 ▶); Hu et al. (2007 ▶); Sun et al. (2010 ▶); Wen et al. (2007 ▶); Xu et al. (2008 ▶). For structures and properties of coordination polymers derived from 5-hy­droxy­nicotinic acid, see: Bunzli (2010 ▶); Decadt et al. (2012 ▶); Gai et al. (2012 ▶); Ramya et al. (2012 ▶); Yang et al. (2011 ▶); Zhang et al. (2012 ▶).

Experimental

Crystal data

[Eu2(C6H5NO3)2(C2O4)3(H2O)4] M = 918.26 Triclinic, a = 7.5912 (2) Å b = 8.0973 (3) Å c = 10.6706 (3) Å α = 103.493 (3)° β = 98.589 (3)° γ = 92.240 (3)° V = 628.78 (3) Å3 Z = 1 Mo Kα radiation μ = 5.05 mm−1 T = 153 K 0.24 × 0.17 × 0.08 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.377, T max = 0.688 12455 measured reflections 3135 independent reflections 2965 reflections with I > 2σ(I) R int = 0.037

Refinement

R[F 2 > 2σ(F 2)] = 0.018 wR(F 2) = 0.038 S = 1.09 3135 reflections 221 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.55 e Å−3 Δρmin = −0.54 e Å−3 Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: SHELXTL. Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813011057/hy2623sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813011057/hy2623Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Eu2(C6H5NO3)2(C2O4)3(H2O)4]Z = 1
Mr = 918.26F(000) = 442
Triclinic, P1Dx = 2.425 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.5912 (2) ÅCell parameters from 3135 reflections
b = 8.0973 (3) Åθ = 2.6–29.4°
c = 10.6706 (3) ŵ = 5.05 mm1
α = 103.493 (3)°T = 153 K
β = 98.589 (3)°Block, colorless
γ = 92.240 (3)°0.24 × 0.17 × 0.08 mm
V = 628.78 (3) Å3
Bruker APEXII CCD diffractometer3135 independent reflections
Radiation source: fine-focus sealed tube2965 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.037
φ and ω scansθmax = 29.5°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −9→9
Tmin = 0.377, Tmax = 0.688k = −11→10
12455 measured reflectionsl = −13→14
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.018H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.038w = 1/[σ2(Fo2) + (0.0087P)2 + 0.3669P] where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.002
3135 reflectionsΔρmax = 0.55 e Å3
221 parametersΔρmin = −0.54 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0094 (4)
Experimental. IR (cm-1, KBr): 3495(s), 3380(s), 3103(m), 3076(w), 3047(w), 2929(w), 2461(m), 2146(m), 1968(w), 1893(w), 1695(s), 1655(s), 1621(s), 1602(s), 1575(s), 1379(s), 1320(s), 1256(m), 1147(w), 1114(w), 1010(w), 935(w), 880(m), 806(s), 784(s), 667(m), 620(w), 565(w), 531(w), 484(m).
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*/Ueq
C10.7687 (3)0.8846 (3)0.9610 (2)0.0095 (5)
C20.7420 (3)0.7295 (3)1.0146 (2)0.0094 (5)
C30.7733 (3)0.5691 (3)0.9454 (2)0.0116 (5)
H30.80820.55520.86390.014*
C40.7525 (4)0.4283 (3)0.9978 (2)0.0127 (5)
C50.7046 (4)0.4541 (3)1.1205 (2)0.0132 (5)
H50.69340.36311.15900.016*
C60.6887 (3)0.7479 (3)1.1353 (2)0.0110 (5)
H60.66310.85401.18180.013*
C70.5536 (3)1.0035 (3)0.4431 (2)0.0099 (5)
C81.0255 (3)0.5479 (3)0.4489 (2)0.0084 (5)
C90.4854 (3)0.4971 (3)0.5697 (2)0.0101 (5)
Eu10.797021 (16)0.810935 (14)0.626500 (11)0.00700 (5)
N10.6745 (3)0.6119 (3)1.1836 (2)0.0112 (4)
O10.8197 (2)0.8624 (2)0.85299 (16)0.0118 (4)
O20.7395 (3)1.0258 (2)1.03073 (16)0.0141 (4)
O30.7803 (3)0.2743 (2)0.92694 (18)0.0225 (5)
H3A0.77130.20350.96980.034*
O40.7120 (2)0.9644 (2)0.45635 (16)0.0117 (4)
O50.5274 (2)0.9519 (2)0.65247 (17)0.0138 (4)
O60.9752 (2)0.6961 (2)0.45804 (16)0.0103 (3)
O70.8889 (2)0.5283 (2)0.63432 (17)0.0120 (4)
O80.5549 (2)0.6147 (2)0.66268 (16)0.0117 (4)
O90.6111 (2)0.6314 (2)0.42511 (16)0.0138 (4)
O101.1269 (2)0.8348 (2)0.70926 (19)0.0138 (4)
O110.9123 (3)1.1139 (2)0.7043 (2)0.0161 (4)
H10.645 (4)0.622 (4)1.257 (3)0.025 (9)*
H71.179 (5)0.876 (4)0.667 (4)0.032 (11)*
H81.168 (5)0.893 (4)0.794 (4)0.038 (10)*
H90.937 (5)1.181 (5)0.654 (4)0.050 (12)*
H100.874 (5)1.164 (4)0.760 (4)0.027 (10)*
U11U22U33U12U13U23
C10.0109 (12)0.0101 (11)0.0078 (12)−0.0005 (9)0.0008 (9)0.0036 (9)
C20.0096 (12)0.0113 (11)0.0076 (12)−0.0008 (9)0.0007 (9)0.0037 (9)
C30.0162 (13)0.0124 (12)0.0073 (12)0.0010 (10)0.0041 (9)0.0035 (9)
C40.0177 (13)0.0096 (12)0.0118 (13)0.0024 (10)0.0037 (10)0.0034 (9)
C50.0191 (14)0.0104 (12)0.0127 (13)0.0025 (10)0.0051 (10)0.0060 (9)
C60.0151 (13)0.0080 (11)0.0101 (12)−0.0007 (10)0.0036 (9)0.0015 (9)
C70.0127 (12)0.0076 (11)0.0106 (12)0.0009 (9)0.0053 (9)0.0025 (9)
C80.0074 (12)0.0105 (11)0.0078 (11)0.0007 (9)0.0009 (9)0.0030 (9)
C90.0080 (12)0.0138 (12)0.0103 (13)0.0028 (10)0.0037 (9)0.0045 (9)
Eu10.00918 (8)0.00665 (7)0.00609 (7)0.00141 (4)0.00295 (4)0.00217 (4)
N10.0159 (11)0.0124 (10)0.0056 (10)−0.0002 (9)0.0039 (8)0.0014 (8)
O10.0162 (9)0.0119 (8)0.0077 (9)−0.0008 (7)0.0031 (7)0.0027 (6)
O20.0256 (10)0.0077 (8)0.0102 (9)0.0014 (7)0.0067 (7)0.0019 (7)
O30.0487 (14)0.0073 (9)0.0173 (10)0.0068 (9)0.0196 (9)0.0049 (7)
O40.0101 (9)0.0144 (9)0.0126 (9)0.0033 (7)0.0047 (7)0.0052 (7)
O50.0154 (9)0.0194 (9)0.0107 (9)0.0078 (7)0.0051 (7)0.0088 (7)
O60.0128 (9)0.0080 (8)0.0129 (9)0.0032 (7)0.0067 (7)0.0049 (6)
O70.0170 (9)0.0095 (8)0.0131 (9)0.0045 (7)0.0096 (7)0.0047 (7)
O80.0125 (9)0.0142 (9)0.0082 (9)−0.0020 (7)0.0027 (7)0.0020 (7)
O90.0173 (10)0.0148 (9)0.0098 (9)−0.0066 (7)0.0049 (7)0.0038 (7)
O100.0118 (9)0.0165 (9)0.0123 (10)−0.0015 (8)0.0031 (7)0.0016 (8)
O110.0274 (12)0.0109 (9)0.0122 (10)0.0002 (8)0.0090 (8)0.0035 (8)
C1—O11.246 (3)C9—O9iii1.266 (3)
C1—O21.258 (3)C9—C9iii1.546 (5)
C1—C21.515 (3)Eu1—O12.3333 (16)
C2—C61.384 (3)Eu1—O52.4025 (18)
C2—C31.385 (3)Eu1—O72.4348 (16)
C3—C41.395 (3)Eu1—O62.4433 (17)
C3—H30.9300Eu1—O42.4539 (17)
C4—O31.341 (3)Eu1—O112.4776 (18)
C4—C51.383 (3)Eu1—O92.4899 (17)
C5—N11.344 (3)Eu1—O102.5118 (19)
C5—H50.9300Eu1—O82.5142 (16)
C6—N11.328 (3)N1—H10.83 (3)
C6—H60.9300O3—H3A0.8200
C7—O5i1.246 (3)O5—C7i1.246 (3)
C7—O41.252 (3)O7—C8ii1.241 (3)
C7—C7i1.569 (5)O9—C9iii1.266 (3)
C8—O7ii1.241 (3)O10—H70.76 (4)
C8—O61.260 (3)O10—H80.92 (4)
C8—C8ii1.562 (5)O11—H90.89 (4)
C9—O81.238 (3)O11—H100.74 (4)
O1—C1—O2125.5 (2)O1—Eu1—O875.12 (6)
O1—C1—C2117.7 (2)O5—Eu1—O868.60 (6)
O2—C1—C2116.8 (2)O7—Eu1—O866.05 (6)
C6—C2—C3119.3 (2)O6—Eu1—O8117.53 (5)
C6—C2—C1119.8 (2)O4—Eu1—O8115.81 (6)
C3—C2—C1120.9 (2)O11—Eu1—O8138.86 (6)
C2—C3—C4120.1 (2)O9—Eu1—O864.36 (5)
C2—C3—H3119.9O10—Eu1—O8129.19 (6)
C4—C3—H3119.9O1—Eu1—C7i100.78 (6)
O3—C4—C5123.0 (2)O5—Eu1—C7i20.20 (6)
O3—C4—C3118.5 (2)O7—Eu1—C7i140.16 (6)
C5—C4—C3118.5 (2)O6—Eu1—C7i120.37 (6)
N1—C5—C4119.3 (2)O4—Eu1—C7i48.67 (6)
N1—C5—H5120.4O11—Eu1—C7i78.99 (6)
C4—C5—H5120.4O9—Eu1—C7i70.91 (6)
N1—C6—C2119.0 (2)O10—Eu1—C7i148.31 (6)
N1—C6—H6120.5O8—Eu1—C7i77.75 (6)
C2—C6—H6120.5O1—Eu1—C7125.61 (6)
O5i—C7—O4125.9 (2)O5—Eu1—C748.20 (6)
O5i—C7—C7i116.6 (3)O7—Eu1—C7141.25 (6)
O4—C7—C7i117.5 (3)O6—Eu1—C793.32 (6)
O7ii—C8—O6125.7 (2)O4—Eu1—C720.65 (6)
O7ii—C8—C8ii117.4 (3)O11—Eu1—C775.30 (6)
O6—C8—C8ii116.9 (3)O9—Eu1—C762.82 (6)
O8—C9—O9iii126.9 (2)O10—Eu1—C7132.68 (6)
O8—C9—C9iii118.7 (3)O8—Eu1—C798.11 (6)
O9iii—C9—C9iii114.4 (3)C7i—Eu1—C728.45 (8)
O1—Eu1—O580.96 (6)O1—Eu1—C8ii102.84 (6)
O1—Eu1—O785.97 (6)O5—Eu1—C8ii146.68 (6)
O5—Eu1—O7134.62 (6)O7—Eu1—C8ii19.51 (6)
O1—Eu1—O6138.32 (6)O6—Eu1—C8ii47.81 (6)
O5—Eu1—O6140.49 (6)O4—Eu1—C8ii119.19 (6)
O7—Eu1—O667.29 (5)O11—Eu1—C8ii135.25 (6)
O1—Eu1—O4137.52 (6)O9—Eu1—C8ii71.90 (6)
O5—Eu1—O467.69 (6)O10—Eu1—C8ii67.29 (6)
O7—Eu1—O4136.49 (6)O8—Eu1—C8ii80.29 (6)
O6—Eu1—O475.83 (6)C7i—Eu1—C8ii142.17 (6)
O1—Eu1—O1176.53 (6)C7—Eu1—C8ii129.65 (6)
O5—Eu1—O1178.03 (7)C6—N1—C5123.8 (2)
O7—Eu1—O11140.07 (7)C6—N1—H1120 (2)
O6—Eu1—O11103.48 (6)C5—N1—H1116 (2)
O4—Eu1—O1169.67 (6)C1—O1—Eu1158.00 (17)
O1—Eu1—O9139.48 (6)C4—O3—H3A109.5
O5—Eu1—O983.77 (6)C7—O4—Eu1115.60 (15)
O7—Eu1—O978.60 (6)C7i—O5—Eu1118.04 (15)
O6—Eu1—O967.69 (6)C8—O6—Eu1118.79 (14)
O4—Eu1—O966.30 (6)C8ii—O7—Eu1119.54 (15)
O11—Eu1—O9135.93 (6)C9—O8—Eu1118.26 (15)
O1—Eu1—O1075.35 (6)C9iii—O9—Eu1120.53 (15)
O5—Eu1—O10143.27 (6)Eu1—O10—H7111 (3)
O7—Eu1—O1071.49 (6)Eu1—O10—H8119 (2)
O6—Eu1—O1066.30 (6)H7—O10—H8105 (3)
O4—Eu1—O10113.98 (6)Eu1—O11—H9125 (3)
O11—Eu1—O1069.47 (7)Eu1—O11—H10116 (3)
O9—Eu1—O10131.87 (6)H9—O11—H10109 (4)
D—H···AD—HH···AD···AD—H···A
N1—H1···O9iv0.83 (3)1.84 (3)2.662 (3)172 (3)
O3—H3A···O2v0.821.732.543 (2)169
O10—H7···O4vi0.76 (4)2.26 (4)3.016 (2)168 (4)
O10—H8···O2vii0.92 (4)1.85 (4)2.759 (3)170 (3)
O11—H9···O6vi0.88 (4)1.90 (4)2.771 (3)170 (4)
O11—H10···O3viii0.74 (4)2.04 (4)2.776 (3)172 (4)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
N1—H1⋯O9i 0.83 (3)1.84 (3)2.662 (3)172 (3)
O3—H3A⋯O2ii 0.821.732.543 (2)169
O10—H7⋯O4iii 0.76 (4)2.26 (4)3.016 (2)168 (4)
O10—H8⋯O2iv 0.92 (4)1.85 (4)2.759 (3)170 (3)
O11—H9⋯O6iii 0.88 (4)1.90 (4)2.771 (3)170 (4)
O11—H10⋯O3v 0.74 (4)2.04 (4)2.776 (3)172 (4)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) .

  8 in total

1.  A short history of SHELX.

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

2.  3-D lanthanide metal-organic frameworks: structure, photoluminescence, and magnetism.

Authors:  Cory A Black; José Sánchez Costa; Wen Tian Fu; Chiara Massera; Olivier Roubeau; Simon J Teat; Guillem Aromí; Patrick Gamez; Jan Reedijk
Journal:  Inorg Chem       Date:  2009-02-02       Impact factor: 5.165

Review 3.  Lanthanide luminescence for biomedical analyses and imaging.

Authors:  Jean-Claude G Bünzli
Journal:  Chem Rev       Date:  2010-05-12       Impact factor: 60.622

4.  Intramolecular ferro- and antiferromagnetic interactions in oxo-carboxylate bridged digadolinium(III) complexes.

Authors:  Laura Cañadillas-Delgado; Oscar Fabelo; Jorge Pasán; Fernando S Delgado; Francesc Lloret; Miguel Julve; Catalina Ruiz-Pérez
Journal:  Dalton Trans       Date:  2010-06-30       Impact factor: 4.390

5.  Synthesis, crystal structures, and luminescence properties of carboxylate based rare-earth coordination polymers.

Authors:  Roel Decadt; Kristof Van Hecke; Diederik Depla; Karen Leus; David Weinberger; Isabel Van Driessche; Pascal Van Der Voort; Rik Van Deun
Journal:  Inorg Chem       Date:  2012-10-18       Impact factor: 5.165

6.  Visible and NIR photoluminescence properties of a series of novel lanthanide-organic coordination polymers based on hydroxyquinoline-carboxylate ligands.

Authors:  Yan-Li Gai; Ke-Cai Xiong; Lian Chen; Yang Bu; Xing-Jun Li; Fei-Long Jiang; Mao-Chun Hong
Journal:  Inorg Chem       Date:  2012-12-03       Impact factor: 5.165

7.  Highly luminescent and thermally stable lanthanide coordination polymers designed from 4-(dipyridin-2-yl)aminobenzoate: efficient energy transfer from Tb3+ to Eu3+ in a mixed lanthanide coordination compound.

Authors:  A R Ramya; Debajit Sharma; Srinivasan Natarajan; M L P Reddy
Journal:  Inorg Chem       Date:  2012-08-03       Impact factor: 5.165

8.  Template synthesis of lanthanide (Pr, Nd, Gd) coordination polymers with 2-hydroxynicotinic acid exhibiting ferro-/antiferromagnetic interaction.

Authors:  Na Xu; Wei Shi; Dai-Zheng Liao; Shi-Ping Yan; Peng Cheng
Journal:  Inorg Chem       Date:  2008-08-23       Impact factor: 5.165

  8 in total
  1 in total

1.  Crystal structure of poly[bis-(μ2-5-hydroxy-nicotinato-κ(2) N:O (3))zinc].

Authors:  Wen-Bing Wang; Shan-Shan Xu; Hong-Ji Chen
Journal:  Acta Crystallogr E Crystallogr Commun       Date:  2015-01-14
  1 in total

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