Literature DB >> 25844240

Crystal structure of 2-hydroxy-N-(2-hydroxyethyl)-N-{2-hydroxy-3-[(E)-N-hydroxyethanimidoyl]-5-methylbenzyl}ethanaminium acetate monohydrate.

Gary S Nichol1, Jamie M Frost1, Sergio Sanz1, Euan K Brechin1.   

Abstract

The structure of the title hydrated mol-ecular salt, C14H23N2O4 (+)·C2H3O2 (-)·H2O, was determined as part of a wider study on the use of the mol-ecule as a polydentate ligand in the synthesis of Mn(III) clusters with magnetic properties. The cation features intra-molecular O-H⋯N and N-H⋯O hydrogen-bond inter-actions. The crystal structure features a range of inter-molecular hydrogen-bonding inter-actions, principally O-H⋯O inter-actions between all three species in the asymmetric unit. An R (2) 4(8) graph-set hydrogen-bonding motif between the anion and water mol-ecules serves as a unit which links to the cation via the di-ethano-lamine group. Each O atom of the acetate anion accepts two hydrogen bonds.

Entities:  

Keywords:  crystal structure; hydrate; hydrogen bonding; magnetism; organic salt

Year:  2015        PMID: 25844240      PMCID: PMC4350734          DOI: 10.1107/S2056989015002418

Source DB:  PubMed          Journal:  Acta Crystallogr E Crystallogr Commun


Related literature

For background literature on Mn-containing single mol­ecule magnets, see: Inglis et al. (2012 ▸); Milios et al. (2007 ▸); Tasiopoulos & Perlepes (2008 ▸). For examples of the use of 3-{[bis­(2-hy­droxy­eth­yl)amino]­meth­yl}-2-hy­droxy-5-methyl­benzaldehyde in the synthesis of magnetic Mn cluster compounds, see: Sanz et al. (2014a ▸,b ▸) – mol­ecular wheels; Frost et al. (2014 ▸) – tetra­hedron cage. For examples of other magnentic oxime-containing clusters, see: Vlahopoulou et al. (2009 ▸); Stamatatos et al. (2007 ▸). For a review of pyrid­yl–oxime coordination chemistry, see: Milios et al. (2006 ▸). For the synthesis of 3-{[bis­(2-hy­droxy­eth­yl)amino]­meth­yl}-2-hy­droxy-5-methylbenzaldehyde, see: Wang et al. (2006 ▸).

Experimental

Crystal data

C14H23N2O4 +·C2H3O2 −·H2O M = 360.40 Monoclinic, a = 14.4338 (5) Å b = 10.4786 (3) Å c = 12.4045 (4) Å β = 101.593 (3)° V = 1837.86 (10) Å3 Z = 4 Mo Kα radiation μ = 0.10 mm−1 T = 120 K 0.48 × 0.38 × 0.18 mm

Data collection

Agilent SuperNova diffractometer Absorption correction: gaussian (CrysAlis PRO; Agilent, 2014 ▸) T min = 0.942, T max = 0.975 38067 measured reflections 5542 independent reflections 4362 reflections with I > 2σ(I) R int = 0.054

Refinement

R[F 2 > 2σ(F 2)] = 0.054 wR(F 2) = 0.129 S = 1.09 5542 reflections 338 parameters All H-atom parameters refined Δρmax = 0.33 e Å−3 Δρmin = −0.24 e Å−3

Data collection: CrysAlis PRO (Agilent, 2014 ▸); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▸); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015 ▸); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▸); software used to prepare material for publication: OLEX2. Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989015002418/hb7350sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015002418/hb7350Isup2.hkl Click here for additional data file. Supporting information file. DOI: 10.1107/S2056989015002418/hb7350Isup3.cdx Click here for additional data file. Supporting information file. DOI: 10.1107/S2056989015002418/hb7350Isup4.cml Click here for additional data file. 4 L . DOI: 10.1107/S2056989015002418/hb7350fig1.tif The asymmetric unit of H4 L. Displacement ellipsoids are at the 50% probability level and C-bound H atoms have been omitted. Click here for additional data file. 4 L x y z x y z x y z . DOI: 10.1107/S2056989015002418/hb7350fig2.tif Hydrogen-bonding inter­actions, indicated by dashed lines, in the crystal structure of H4 L. Symmetry operations for equivalent atoms: $1, 1 − x, −y, 2 − z; $2, x,  − y,  + z; $3, 1 − x, − + y,  − z. CCDC reference: 1047385 Additional supporting information: crystallographic information; 3D view; checkCIF report
C14H23N2O4+·C2H3O2·H2OF(000) = 776
Mr = 360.40Dx = 1.303 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 14.4338 (5) ÅCell parameters from 10187 reflections
b = 10.4786 (3) Åθ = 3.5–30.2°
c = 12.4045 (4) ŵ = 0.10 mm1
β = 101.593 (3)°T = 120 K
V = 1837.86 (10) Å3Block, colourless
Z = 40.48 × 0.38 × 0.18 mm
Agilent SuperNova diffractometer5542 independent reflections
Radiation source: SuperNova (Mo) X-ray Source4362 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.054
Detector resolution: 5.1574 pixels mm-1θmax = 31.1°, θmin = 3.1°
ω scansh = −20→20
Absorption correction: gaussian (CrysAlis PRO; Agilent, 2014)k = −15→13
Tmin = 0.942, Tmax = 0.975l = −18→17
38067 measured reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054All H-atom parameters refined
wR(F2) = 0.129w = 1/[σ2(Fo2) + (0.0431P)2 + 0.9291P] where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max < 0.001
5542 reflectionsΔρmax = 0.33 e Å3
338 parametersΔρmin = −0.24 e Å3
0 restraints
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. All H atoms were located in a difference Fourier map and refined freely.
xyzUiso*/Ueq
O10.25286 (7)−0.10957 (10)0.65849 (9)0.0229 (2)
H10.2395 (15)−0.050 (2)0.6990 (18)0.046 (6)*
O20.14106 (9)0.14279 (11)0.81376 (9)0.0320 (3)
H20.2011 (17)0.160 (2)0.8484 (19)0.054 (7)*
O30.24215 (8)0.03539 (12)0.40801 (10)0.0304 (3)
H30.2659 (18)0.107 (3)0.418 (2)0.060 (7)*
O40.45674 (8)−0.04092 (11)0.61916 (10)0.0300 (3)
H40.4552 (16)−0.026 (2)0.686 (2)0.055 (7)*
N10.15152 (9)0.03976 (12)0.74689 (10)0.0232 (3)
N20.32127 (9)−0.19342 (12)0.47375 (10)0.0220 (3)
H2A0.3117 (13)−0.1223 (18)0.5112 (15)0.028 (5)*
C10.16920 (10)−0.16143 (13)0.60648 (11)0.0202 (3)
C20.17518 (10)−0.26194 (13)0.53438 (12)0.0223 (3)
C30.09294 (11)−0.32024 (14)0.47871 (12)0.0246 (3)
H3A0.0993 (13)−0.3890 (18)0.4276 (15)0.029 (5)*
C40.00394 (11)−0.27997 (14)0.49290 (12)0.0243 (3)
C5−0.00027 (10)−0.17826 (14)0.56389 (11)0.0213 (3)
H5−0.0609 (13)−0.1492 (17)0.5733 (14)0.024 (4)*
C60.08079 (10)−0.11679 (13)0.62184 (11)0.0192 (3)
C70.07274 (10)−0.00789 (14)0.69504 (11)0.0203 (3)
C8−0.02208 (11)0.04239 (17)0.70539 (14)0.0264 (3)
H8A−0.0567 (16)0.073 (2)0.638 (2)0.053 (6)*
H8B−0.0153 (17)0.104 (2)0.757 (2)0.058 (7)*
H8C−0.0601 (16)−0.026 (2)0.7244 (18)0.052 (6)*
C9−0.08552 (13)−0.34031 (18)0.43012 (14)0.0323 (4)
H9A−0.1036 (15)−0.305 (2)0.3569 (18)0.042 (6)*
H9B−0.1359 (18)−0.334 (2)0.474 (2)0.063 (7)*
H9C−0.0770 (15)−0.429 (2)0.4181 (18)0.048 (6)*
C100.27174 (11)−0.30209 (14)0.51927 (14)0.0261 (3)
H10A0.2691 (13)−0.3701 (19)0.4675 (16)0.032 (5)*
H10B0.3144 (13)−0.3244 (17)0.5908 (15)0.027 (5)*
C110.27852 (12)−0.16896 (15)0.35473 (12)0.0259 (3)
H11A0.2117 (13)−0.1940 (17)0.3425 (14)0.024 (4)*
H11B0.3108 (13)−0.2206 (19)0.3119 (15)0.032 (5)*
C120.28636 (12)−0.02870 (16)0.33149 (13)0.0294 (3)
H12A0.3503 (14)−0.0019 (18)0.3386 (15)0.032 (5)*
H12B0.2514 (13)−0.0128 (18)0.2536 (15)0.030 (5)*
C130.42648 (11)−0.21255 (17)0.49313 (14)0.0288 (3)
H13A0.4494 (12)−0.1530 (17)0.4413 (14)0.025 (4)*
H13B0.4385 (12)−0.3021 (18)0.4792 (14)0.027 (4)*
C140.47242 (12)−0.17376 (17)0.60884 (14)0.0298 (3)
H14A0.5399 (14)−0.1927 (18)0.6200 (15)0.034 (5)*
H14B0.4445 (13)−0.2225 (18)0.6635 (15)0.030 (5)*
O50.30047 (8)0.22604 (11)0.92796 (9)0.0297 (3)
O60.38120 (9)0.06607 (11)1.01687 (10)0.0349 (3)
C150.34399 (10)0.17389 (14)1.01535 (13)0.0242 (3)
C160.35169 (15)0.24691 (19)1.12192 (15)0.0347 (4)
H16A0.409 (2)0.234 (3)1.167 (3)0.098 (11)*
H16B0.348 (2)0.337 (3)1.110 (3)0.101 (11)*
H16C0.307 (2)0.221 (3)1.162 (3)0.108 (12)*
O70.46060 (14)0.00383 (17)0.83335 (12)0.0569 (5)
H7A0.4274 (18)0.028 (3)0.873 (2)0.059 (8)*
H7B0.5160 (19)−0.016 (3)0.875 (2)0.064 (8)*
U11U22U33U12U13U23
O10.0198 (5)0.0238 (5)0.0247 (5)0.0018 (4)0.0037 (4)−0.0027 (4)
O20.0276 (6)0.0354 (6)0.0320 (6)0.0025 (5)0.0035 (5)−0.0167 (5)
O30.0300 (6)0.0243 (6)0.0361 (6)−0.0018 (5)0.0048 (5)−0.0022 (5)
O40.0306 (6)0.0328 (6)0.0282 (6)0.0025 (5)0.0099 (5)−0.0019 (5)
N10.0251 (6)0.0229 (6)0.0216 (6)0.0016 (5)0.0051 (5)−0.0044 (5)
N20.0225 (6)0.0208 (6)0.0233 (6)0.0035 (5)0.0062 (5)−0.0030 (5)
C10.0223 (7)0.0177 (6)0.0208 (6)0.0002 (5)0.0046 (5)0.0031 (5)
C20.0268 (7)0.0167 (6)0.0251 (7)0.0020 (5)0.0096 (6)0.0036 (5)
C30.0343 (8)0.0166 (6)0.0247 (7)−0.0023 (6)0.0098 (6)0.0001 (5)
C40.0291 (8)0.0232 (7)0.0218 (6)−0.0063 (6)0.0077 (6)0.0005 (5)
C50.0214 (7)0.0226 (7)0.0208 (6)−0.0016 (5)0.0070 (5)0.0025 (5)
C60.0223 (7)0.0180 (6)0.0178 (6)−0.0002 (5)0.0053 (5)0.0029 (5)
C70.0223 (7)0.0218 (7)0.0177 (6)0.0008 (5)0.0061 (5)0.0017 (5)
C80.0227 (8)0.0304 (8)0.0271 (7)0.0018 (6)0.0075 (6)−0.0024 (6)
C90.0333 (9)0.0343 (9)0.0303 (8)−0.0124 (7)0.0085 (7)−0.0093 (7)
C100.0301 (8)0.0185 (7)0.0312 (8)0.0048 (6)0.0097 (6)0.0005 (6)
C110.0294 (8)0.0282 (8)0.0204 (6)−0.0018 (6)0.0057 (6)−0.0049 (6)
C120.0313 (9)0.0310 (8)0.0251 (7)−0.0038 (6)0.0039 (6)0.0016 (6)
C130.0217 (8)0.0337 (9)0.0326 (8)0.0081 (6)0.0091 (6)−0.0046 (7)
C140.0224 (8)0.0337 (9)0.0331 (8)0.0074 (6)0.0050 (6)−0.0006 (7)
O50.0302 (6)0.0252 (6)0.0310 (6)−0.0027 (4)−0.0003 (5)0.0003 (4)
O60.0394 (7)0.0216 (6)0.0417 (7)0.0006 (5)0.0032 (5)−0.0002 (5)
C150.0192 (7)0.0219 (7)0.0311 (7)−0.0064 (5)0.0043 (6)−0.0005 (6)
C160.0391 (10)0.0332 (9)0.0309 (8)−0.0034 (7)0.0044 (7)−0.0042 (7)
O70.0679 (11)0.0706 (11)0.0285 (7)0.0369 (9)0.0011 (7)−0.0062 (7)
O1—H10.85 (2)C8—H8B0.91 (3)
O1—C11.3625 (17)C8—H8C0.96 (2)
O2—H20.91 (2)C9—H9A0.97 (2)
O2—N11.3880 (16)C9—H9B0.99 (3)
O3—H30.82 (3)C9—H9C0.96 (2)
O3—C121.415 (2)C10—H10A0.95 (2)
O4—H40.85 (2)C10—H10B1.001 (18)
O4—C141.420 (2)C11—H11A0.982 (18)
N1—C71.2891 (19)C11—H11B0.94 (2)
N2—H2A0.903 (19)C11—C121.506 (2)
N2—C101.513 (2)C12—H12A0.952 (19)
N2—C111.5034 (19)C12—H12B1.009 (18)
N2—C131.503 (2)C13—H13A0.999 (18)
C1—C21.396 (2)C13—H13B0.976 (19)
C1—C61.408 (2)C13—C141.511 (2)
C2—C31.389 (2)C14—H14A0.98 (2)
C2—C101.503 (2)C14—H14B0.996 (19)
C3—H3A0.976 (19)O5—C151.2628 (18)
C3—C41.396 (2)O6—C151.2495 (19)
C4—C51.392 (2)C15—C161.512 (2)
C4—C91.506 (2)C16—H16A0.91 (3)
C5—H50.955 (18)C16—H16B0.96 (4)
C5—C61.401 (2)C16—H16C0.92 (4)
C6—C71.4773 (19)O7—H7A0.79 (3)
C7—C81.496 (2)O7—H7B0.89 (3)
C8—H8A0.95 (2)
C1—O1—H1106.8 (15)H9A—C9—H9C104.1 (18)
N1—O2—H2103.4 (15)H9B—C9—H9C106 (2)
C12—O3—H3107.3 (18)N2—C10—H10A105.6 (11)
C14—O4—H4107.4 (17)N2—C10—H10B104.7 (10)
C7—N1—O2114.11 (12)C2—C10—N2110.81 (12)
C10—N2—H2A107.2 (12)C2—C10—H10A112.3 (11)
C11—N2—H2A106.8 (11)C2—C10—H10B112.1 (10)
C11—N2—C10111.31 (12)H10A—C10—H10B110.8 (15)
C13—N2—H2A106.4 (11)N2—C11—H11A107.6 (10)
C13—N2—C10112.21 (12)N2—C11—H11B107.6 (11)
C13—N2—C11112.46 (12)N2—C11—C12108.81 (12)
O1—C1—C2116.19 (13)H11A—C11—H11B109.9 (15)
O1—C1—C6123.00 (13)C12—C11—H11A109.9 (10)
C2—C1—C6120.80 (13)C12—C11—H11B112.7 (12)
C1—C2—C10118.00 (13)O3—C12—C11105.86 (13)
C3—C2—C1119.59 (14)O3—C12—H12A111.0 (11)
C3—C2—C10122.41 (13)O3—C12—H12B111.0 (10)
C2—C3—H3A117.7 (11)C11—C12—H12A112.2 (12)
C2—C3—C4121.35 (14)C11—C12—H12B107.6 (11)
C4—C3—H3A120.9 (11)H12A—C12—H12B109.2 (15)
C3—C4—C9121.51 (14)N2—C13—H13A105.6 (10)
C5—C4—C3118.00 (14)N2—C13—H13B108.1 (10)
C5—C4—C9120.44 (15)N2—C13—C14110.65 (12)
C4—C5—H5118.6 (11)H13A—C13—H13B113.1 (15)
C4—C5—C6122.59 (14)C14—C13—H13A107.7 (10)
C6—C5—H5118.8 (11)C14—C13—H13B111.5 (10)
C1—C6—C7121.69 (13)O4—C14—C13107.57 (13)
C5—C6—C1117.66 (13)O4—C14—H14A111.1 (12)
C5—C6—C7120.65 (13)O4—C14—H14B110.4 (11)
N1—C7—C6115.82 (13)C13—C14—H14A108.3 (11)
N1—C7—C8123.45 (13)C13—C14—H14B110.4 (11)
C6—C7—C8120.73 (13)H14A—C14—H14B109.1 (15)
C7—C8—H8A112.0 (14)O5—C15—C16117.90 (14)
C7—C8—H8B110.1 (15)O6—C15—O5122.85 (15)
C7—C8—H8C109.7 (14)O6—C15—C16119.25 (15)
H8A—C8—H8B110 (2)C15—C16—H16A111 (2)
H8A—C8—H8C104.4 (19)C15—C16—H16B112 (2)
H8B—C8—H8C110 (2)C15—C16—H16C113 (2)
C4—C9—H9A111.6 (13)H16A—C16—H16B105 (3)
C4—C9—H9B109.7 (14)H16A—C16—H16C106 (3)
C4—C9—H9C111.5 (13)H16B—C16—H16C111 (3)
H9A—C9—H9B113.5 (19)H7A—O7—H7B107 (2)
O1—C1—C2—C3179.65 (12)C3—C2—C10—N2118.43 (15)
O1—C1—C2—C10−0.96 (19)C3—C4—C5—C6−0.8 (2)
O1—C1—C6—C5−179.83 (12)C4—C5—C6—C1−0.1 (2)
O1—C1—C6—C71.0 (2)C4—C5—C6—C7179.07 (13)
O2—N1—C7—C6179.25 (11)C5—C6—C7—N1178.18 (13)
O2—N1—C7—C8−0.1 (2)C5—C6—C7—C8−2.5 (2)
N2—C11—C12—O3−55.59 (16)C6—C1—C2—C3−1.3 (2)
N2—C13—C14—O4−63.57 (17)C6—C1—C2—C10178.13 (13)
C1—C2—C3—C40.3 (2)C9—C4—C5—C6−178.27 (14)
C1—C2—C10—N2−60.94 (17)C10—N2—C11—C12148.01 (13)
C1—C6—C7—N1−2.68 (19)C10—N2—C13—C14−81.01 (16)
C1—C6—C7—C8176.67 (13)C10—C2—C3—C4−179.04 (14)
C2—C1—C6—C51.1 (2)C11—N2—C10—C2−72.47 (15)
C2—C1—C6—C7−178.03 (12)C11—N2—C13—C14152.57 (14)
C2—C3—C4—C50.7 (2)C13—N2—C10—C2160.50 (12)
C2—C3—C4—C9178.13 (14)C13—N2—C11—C12−85.09 (16)
D—H···AD—HH···AD···AD—H···A
O1—H1···N10.85 (2)1.78 (2)2.5368 (16)148 (2)
O2—H2···O50.91 (2)1.71 (2)2.5985 (16)165 (2)
O3—H3···O5i0.82 (3)1.82 (3)2.6335 (17)171 (3)
O4—H4···O70.85 (2)1.84 (2)2.6875 (19)176 (2)
N2—H2A···O10.903 (19)2.168 (18)2.8121 (16)127.6 (15)
O7—H7A···O60.79 (3)2.07 (3)2.823 (2)159 (3)
O7—H7B···O6ii0.89 (3)1.86 (3)2.738 (2)169 (2)
Table 1

Hydrogen-bond geometry (, )

DHA DHHA D A DHA
O1H1N10.85(2)1.78(2)2.5368(16)148(2)
O2H2O50.91(2)1.71(2)2.5985(16)165(2)
O3H3O5i 0.82(3)1.82(3)2.6335(17)171(3)
O4H4O70.85(2)1.84(2)2.6875(19)176(2)
N2H2AO10.903(19)2.168(18)2.8121(16)127.6(15)
O7H7AO60.79(3)2.07(3)2.823(2)159(3)
O7H7BO6ii 0.89(3)1.86(3)2.738(2)169(2)

Symmetry codes: (i) ; (ii) .

  9 in total

1.  A record anisotropy barrier for a single-molecule magnet.

Authors:  Constantinos J Milios; Alina Vinslava; Wolfgang Wernsdorfer; Stephen Moggach; Simon Parsons; Spyros P Perlepes; George Christou; Euan K Brechin
Journal:  J Am Chem Soc       Date:  2007-02-20       Impact factor: 15.419

2.  A short history of SHELX.

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

3.  Initial employment of alpha-benzoin oxime as a route to high-nuclearity metal clusters: decanuclear CuII complexes with a wheel topology.

Authors:  Gina C Vlahopoulou; Theocharis C Stamatatos; Vassilis Psycharis; Spyros P Perlepes; George Christou
Journal:  Dalton Trans       Date:  2009-03-17       Impact factor: 4.390

4.  Twisted molecular magnets.

Authors:  Ross Inglis; Constantinos J Milios; Leigh F Jones; Stergios Piligkos; Euan K Brechin
Journal:  Chem Commun (Camb)       Date:  2011-09-05       Impact factor: 6.222

5.  Combining complementary ligands into one framework for the construction of a ferromagnetically coupled [Mn(III)12] wheel.

Authors:  Sergio Sanz; Jamie M Frost; Thayalan Rajeshkumar; Scott J Dalgarno; Gopalan Rajaraman; Wolfgang Wernsdorfer; Jürgen Schnack; Paul J Lusby; Euan K Brechin
Journal:  Chemistry       Date:  2014-01-27       Impact factor: 5.236

6.  Diol-type ligands as central 'players' in the chemistry of high-spin molecules and single-molecule magnets.

Authors:  Anastasios J Tasiopoulos; Spyros P Perlepes
Journal:  Dalton Trans       Date:  2008-07-31       Impact factor: 4.390

7.  The highest nuclearity metal oxime clusters: Ni14 and Ni12Na2 complexes from the use of 2-pyridinealdoximate and azide ligands.

Authors:  Theocharis C Stamatatos; Khalil A Abboud; Spyros P Perlepes; George Christou
Journal:  Dalton Trans       Date:  2007-07-30       Impact factor: 4.390

8.  A truncated [Mn(III)₁₂] tetrahedron from oxime-based [Mn(III)₃O] building blocks.

Authors:  J M Frost; S Sanz; T Rajeshkumar; M B Pitak; S J Coles; G Rajaraman; W Wernsdorfer; J Schnack; P J Lusby; E K Brechin
Journal:  Dalton Trans       Date:  2014-07-28       Impact factor: 4.390

9.  Crystal structure refinement with SHELXL.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr C Struct Chem       Date:  2015-01-01       Impact factor: 1.172

  9 in total

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