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Four new praseodymium(III) metal–organic compounds varying in dimensionality from 0D to 3D have been designed and synthesized based on N-heterocyclic polycarb­ox­ylic acids, including pyridine-2,6-di­carb­ox­ylic acid (H2pydc) and pyrazine-2,3-di­carb­ox­ylic acid (H2pzdc). Altering the concentration of piperazine (pip, ancillary ligand) enables control over the dimensionality of the compound by switching between the 0D [H2pip][Hpip][Pr(pydc)3]·4H2O (I) and the 1D {[Pr(pydc)(Hpydc)(H2O)2]·4H2O}n (II) coordination polymer (CP). Upon replacing H2pydc with H2pzdc, CP II is converted to the 2D CP [Pr(pzdc)(Hpzdc)(H2O)3]n (III) and using the metalloligand [Zn(Hpzdc)2(H2O)2]2−, the 3D heterometallic CP {[Pr2Zn(pzdc)4(H2O)6]·2H2O}n (IV) is formed. Com­pound IV shows high stability in the absence of uncoordinated solvent molecules and is stable up to 400°C, even in the presence of humidity. Therefore, IV was utilized for iodine adsorption in the vapour phase and in the presence of humidity. The results confirm the remarkable potential of IV for reversible adsorption of iodine vapour.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520620009336/bm5130sup1.cif
Contains datablocks II, I, III, IV

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620009336/bm5130Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620009336/bm5130IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620009336/bm5130IIIsup4.hkl
Contains datablock III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520620009336/bm5130IVsup5.hkl
Contains datablock IV

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520620009336/bm5130sup6.pdf
Details of crystal structure of I. Tables of H-bond geometry for I-IV. The FT-IR Spectra of I-IV. The PXRD pattern of I-IV. TGA diagrams of I, II, III.

CCDC references: 1994544; 1994545; 1994546; 1994547; 1994544; 1994545; 1994546; 1994547

Computing details top

Data collection: CrysAlis CCD 1.171.38.41 (Rigaku Oxford Diffraction, 2015 for (II); CrysAlis CCD 1.171.38.43 (Rigaku Oxford Diffraction, 2015) for (I), (III), (IV). Cell refinement: CrysAlis RED 1.171.38.41 (Rigaku Oxford Diffraction, 2015) for (II); CrysAlis PRO 1.171.38.43 (Rigaku Oxford Diffraction, 2015) for (I), (III), (IV). Data reduction: CrysAlis RED 1.171.38.41 (Rigaku Oxford Diffraction, 2015) for (II); CrysAlis PRO 1.171.38.43 (Rigaku Oxford Diffraction, 2015) for (I), (III), (IV). Program(s) used to solve structure: SHELXT (Sheldrick, 2014) for (II); SHELXT-2014/7 (Sheldrick, 2014) for (I), (III), (IV). Program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014) for (II); SHELXL2018/3 (Sheldrick, 2018) for (I), (III), (IV). For all structures, molecular graphics: Brandenburg & Putz (2006). Diamond 3.0. Crystal and Molecular Structure Visualisation, University of Bonn, Germany. Software used to prepare material for publication: SHELXL2014/7 (Sheldrick, 2014) for (II); SHELXL2018/3 (Sheldrick, 2018) for (I), (III), (IV).

(II) top
Crystal data top
C14H13N2O11Pr·3(H2O)F(000) = 1152
Mr = 580.22Dx = 1.952 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.9898 (3) ÅCell parameters from 19570 reflections
b = 11.2016 (2) Åθ = 3.0–29.6°
c = 12.9061 (3) ŵ = 2.55 mm1
β = 102.499 (2)°T = 100 K
V = 1974.56 (7) Å3Parallelepiped, light purple
Z = 40.25 × 0.23 × 0.12 mm
Data collection top
KUMA KM-4 with CCD detector
diffractometer
5139 independent reflections
Radiation source: fine-focus sealed X-ray tube4530 reflections with I > 2σ(I)
Detector resolution: 10.6249 pixels mm-1Rint = 0.034
ω–scanθmax = 29.7°, θmin = 2.4°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.41 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1819
Tmin = 0.797, Tmax = 1.000k = 1515
37026 measured reflectionsl = 1717
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: mixed
wR(F2) = 0.054H atoms treated by a mixture of independent and constrained refinement
S = 1.00 w = 1/[σ2(Fo2) + (0.0262P)2 + 2.8293P]
where P = (Fo2 + 2Fc2)/3
5139 reflections(Δ/σ)max = 0.003
297 parametersΔρmax = 0.83 e Å3
0 restraintsΔρmin = 0.66 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pr0.73237 (2)0.70456 (2)0.84946 (2)0.00644 (4)
N110.54939 (14)0.70735 (17)0.86605 (15)0.0114 (4)
C120.50321 (18)0.8110 (2)0.8691 (2)0.0168 (5)
C130.4048 (2)0.8173 (3)0.8696 (3)0.0337 (8)
H130.3737330.8922550.8728300.040*
C140.3523 (2)0.7117 (3)0.8655 (4)0.0484 (11)
H140.2841350.7136150.8639790.058*
C150.3995 (2)0.6040 (3)0.8635 (3)0.0346 (7)
H150.3649880.5306610.8613110.042*
C160.49851 (18)0.6057 (2)0.8648 (2)0.0174 (5)
C170.56755 (17)0.9196 (2)0.87167 (19)0.0135 (5)
O110.65638 (11)0.90127 (14)0.86827 (13)0.0121 (3)
O120.52943 (13)1.01944 (16)0.87675 (15)0.0215 (4)
C180.56032 (18)0.4960 (2)0.86578 (19)0.0153 (5)
O130.64659 (12)0.50579 (14)0.86184 (13)0.0127 (3)
O140.51622 (14)0.39584 (16)0.87173 (16)0.0256 (4)
H14A0.563 (3)0.319 (3)0.871 (3)0.038*
N210.83501 (13)0.94937 (16)0.48072 (14)0.0074 (3)
C220.82904 (15)0.95285 (19)0.58277 (17)0.0080 (4)
C230.86426 (16)1.0478 (2)0.64901 (17)0.0105 (4)
H230.8615201.0467130.7219130.013*
C240.90350 (17)1.1440 (2)0.60561 (18)0.0118 (4)
H240.9261461.2117170.6482300.014*
C250.90984 (16)1.1418 (2)0.49963 (17)0.0109 (4)
H250.9364441.2075060.4687870.013*
C260.87634 (16)1.04127 (19)0.44007 (17)0.0090 (4)
C270.77706 (16)0.84760 (19)0.61813 (17)0.0089 (4)
O210.78411 (12)0.83371 (14)0.71566 (12)0.0110 (3)
O220.72902 (12)0.78198 (13)0.54523 (12)0.0102 (3)
C280.88354 (16)1.0260 (2)0.32526 (17)0.0094 (4)
O230.84894 (12)0.92945 (14)0.28121 (12)0.0111 (3)
O240.92303 (12)1.10709 (14)0.28357 (12)0.0140 (3)
O10.87691 (12)0.81719 (15)0.93787 (13)0.0131 (3)
H1A0.9248690.8007610.9089680.020*
H1B0.8957390.7926781.0019900.020*
O20.63504 (13)0.65305 (16)0.67061 (13)0.0181 (4)
H2A0.6252040.5779600.6662130.027*
H2B0.6687020.6676330.6243150.027*
O30.95883 (12)0.81047 (14)1.14848 (13)0.0117 (3)
H3A0.9946510.7511221.1734310.018*
H3B0.9243630.8311301.1924000.018*
O40.96669 (13)1.05707 (15)0.09487 (13)0.0147 (3)
H4A0.9506841.0735400.1532900.022*
H4B0.9828650.9838430.0946500.022*
O50.80055 (16)0.09574 (18)0.91051 (19)0.0350 (5)
H5A0.8311710.0917690.9753310.052*
H5B0.7631730.0352480.8953780.052*
O60.62634 (19)0.22155 (19)0.8839 (3)0.0599 (9)
H6A0.6884440.2171710.8935220.090*
H6B0.6076660.1494030.8857450.090*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pr0.00711 (7)0.00665 (6)0.00570 (6)0.00042 (4)0.00165 (4)0.00058 (4)
N110.0101 (9)0.0136 (10)0.0110 (9)0.0015 (7)0.0033 (8)0.0008 (7)
C120.0125 (12)0.0152 (12)0.0230 (13)0.0013 (9)0.0043 (10)0.0004 (9)
C130.0144 (14)0.0184 (14)0.072 (2)0.0002 (10)0.0170 (15)0.0051 (14)
C140.0168 (15)0.0276 (17)0.108 (3)0.0023 (12)0.0283 (19)0.0064 (18)
C150.0163 (14)0.0231 (15)0.069 (2)0.0067 (11)0.0182 (14)0.0017 (15)
C160.0157 (12)0.0160 (12)0.0219 (12)0.0046 (9)0.0071 (10)0.0002 (10)
C170.0128 (11)0.0121 (11)0.0156 (11)0.0006 (9)0.0031 (9)0.0009 (9)
O110.0098 (8)0.0112 (8)0.0156 (8)0.0009 (6)0.0035 (6)0.0008 (6)
O120.0144 (9)0.0150 (9)0.0349 (11)0.0057 (7)0.0044 (8)0.0021 (8)
C180.0180 (12)0.0145 (12)0.0134 (11)0.0034 (9)0.0030 (9)0.0012 (9)
O130.0126 (8)0.0101 (8)0.0152 (8)0.0018 (6)0.0025 (7)0.0008 (6)
O140.0223 (10)0.0124 (9)0.0427 (12)0.0064 (7)0.0085 (9)0.0036 (8)
N210.0059 (9)0.0089 (9)0.0073 (8)0.0003 (7)0.0010 (7)0.0006 (7)
C220.0070 (10)0.0073 (10)0.0100 (10)0.0016 (8)0.0022 (8)0.0017 (8)
C230.0128 (11)0.0117 (11)0.0070 (10)0.0009 (8)0.0018 (8)0.0002 (8)
C240.0142 (11)0.0092 (11)0.0118 (11)0.0017 (8)0.0024 (9)0.0027 (8)
C250.0121 (11)0.0090 (11)0.0115 (11)0.0006 (8)0.0023 (9)0.0016 (8)
C260.0072 (10)0.0097 (10)0.0099 (10)0.0015 (8)0.0014 (8)0.0006 (8)
C270.0087 (10)0.0071 (10)0.0117 (10)0.0021 (8)0.0040 (8)0.0002 (8)
O210.0151 (8)0.0119 (8)0.0058 (7)0.0015 (6)0.0023 (6)0.0010 (6)
O220.0115 (8)0.0115 (8)0.0076 (7)0.0035 (6)0.0022 (6)0.0016 (6)
C280.0088 (10)0.0096 (10)0.0097 (10)0.0005 (8)0.0019 (8)0.0007 (8)
O230.0154 (8)0.0101 (7)0.0085 (7)0.0032 (6)0.0044 (6)0.0024 (6)
O240.0203 (9)0.0118 (8)0.0119 (8)0.0047 (7)0.0081 (7)0.0010 (6)
O10.0115 (8)0.0188 (9)0.0088 (8)0.0020 (6)0.0015 (6)0.0008 (6)
O20.0211 (9)0.0226 (9)0.0108 (8)0.0108 (7)0.0038 (7)0.0015 (7)
O30.0144 (8)0.0117 (8)0.0099 (8)0.0030 (6)0.0046 (6)0.0001 (6)
O40.0211 (9)0.0120 (8)0.0136 (8)0.0030 (7)0.0095 (7)0.0022 (6)
O50.0288 (12)0.0167 (10)0.0523 (14)0.0066 (8)0.0071 (10)0.0030 (9)
O60.0290 (13)0.0141 (11)0.136 (3)0.0004 (9)0.0169 (16)0.0014 (14)
Geometric parameters (Å, º) top
Pr—O12.4462 (16)C22—C231.386 (3)
Pr—O212.4779 (15)C22—C271.507 (3)
Pr—O22.4808 (16)C23—C241.382 (3)
Pr—O112.4811 (16)C23—H230.9500
Pr—O23i2.5122 (15)C24—C251.390 (3)
Pr—O22i2.5416 (15)C24—H240.9500
Pr—O132.5507 (16)C25—C261.387 (3)
Pr—N112.615 (2)C25—H250.9500
Pr—N21i2.6176 (18)C26—C281.516 (3)
N11—C121.334 (3)C27—O211.251 (3)
N11—C161.341 (3)C27—O221.266 (3)
C12—C131.380 (4)C28—O241.244 (3)
C12—C171.509 (3)C28—O231.268 (3)
C13—C141.388 (4)O1—H1A0.8553
C13—H130.9500O1—H1B0.8574
C14—C151.379 (4)O2—H2A0.8522
C14—H140.9500O2—H2B0.8528
C15—C161.382 (4)O3—H3A0.8526
C15—H150.9500O3—H3B0.8518
C16—C181.501 (3)O4—H4A0.8520
C17—O121.247 (3)O4—H4B0.8511
C17—O111.270 (3)O5—H5A0.8546
C18—O131.224 (3)O5—H5B0.8524
C18—O141.291 (3)O6—H14A1.40 (4)
O14—H14A1.08 (4)O6—H6A0.8521
N21—C221.338 (3)O6—H6B0.8512
N21—C261.342 (3)
O1—Pr—O2171.78 (5)N11—C16—C15122.7 (2)
O1—Pr—O2141.79 (5)N11—C16—C18113.1 (2)
O21—Pr—O270.83 (5)C15—C16—C18124.2 (2)
O1—Pr—O1179.91 (5)O12—C17—O11125.4 (2)
O21—Pr—O1175.27 (5)O12—C17—C12117.7 (2)
O2—Pr—O1197.88 (6)O11—C17—C12116.9 (2)
O1—Pr—O23i86.44 (5)C17—O11—Pr126.18 (14)
O21—Pr—O23i78.16 (5)O13—C18—O14124.6 (2)
O2—Pr—O23i78.58 (6)O13—C18—C16119.9 (2)
O11—Pr—O23i152.80 (5)O14—C18—C16115.5 (2)
O1—Pr—O22i72.36 (5)C18—O13—Pr124.21 (15)
O21—Pr—O22i136.82 (5)C18—O14—H14A113.3 (19)
O2—Pr—O22i144.51 (5)C22—N21—C26119.10 (19)
O11—Pr—O22i75.50 (5)C22—N21—Prii120.92 (14)
O23i—Pr—O22i122.48 (5)C26—N21—Prii118.35 (14)
O1—Pr—O13140.68 (5)N21—C22—C23122.7 (2)
O21—Pr—O13139.96 (5)N21—C22—C27114.34 (18)
O2—Pr—O1371.60 (5)C23—C22—C27122.94 (19)
O11—Pr—O13123.49 (5)C24—C23—C22117.9 (2)
O23i—Pr—O1381.39 (5)C24—C23—H23121.1
O22i—Pr—O1383.07 (5)C22—C23—H23121.1
O1—Pr—N11132.90 (6)C23—C24—C25120.0 (2)
O21—Pr—N11119.27 (6)C23—C24—H24120.0
O2—Pr—N1174.28 (6)C25—C24—H24120.0
O11—Pr—N1162.20 (6)C26—C25—C24118.3 (2)
O23i—Pr—N11139.22 (6)C26—C25—H25120.9
O22i—Pr—N1171.87 (6)C24—C25—H25120.9
O13—Pr—N1161.52 (6)N21—C26—C25121.9 (2)
O1—Pr—N21i75.85 (5)N21—C26—C28114.90 (19)
O21—Pr—N21i129.31 (5)C25—C26—C28123.2 (2)
O2—Pr—N21i124.24 (6)O21—C27—O22126.1 (2)
O11—Pr—N21i135.10 (5)O21—C27—C22117.64 (19)
O23i—Pr—N21i61.74 (5)O22—C27—C22116.27 (19)
O22i—Pr—N21i61.40 (5)C27—O21—Pr143.38 (14)
O13—Pr—N21i65.42 (5)C27—O22—Prii125.67 (14)
N11—Pr—N21i111.38 (6)O24—C28—O23126.2 (2)
C12—N11—C16118.7 (2)O24—C28—C26118.03 (19)
C12—N11—Pr120.12 (15)O23—C28—C26115.75 (19)
C16—N11—Pr121.02 (15)C28—O23—Prii124.49 (13)
N11—C12—C13122.3 (2)Pr—O1—H1A109.4
N11—C12—C17114.3 (2)Pr—O1—H1B109.6
C13—C12—C17123.3 (2)H1A—O1—H1B104.2
C12—C13—C14118.4 (3)Pr—O2—H2A109.9
C12—C13—H13120.8Pr—O2—H2B109.4
C14—C13—H13120.8H2A—O2—H2B104.4
C15—C14—C13119.7 (3)H3A—O3—H3B109.4
C15—C14—H14120.1H4A—O4—H4B109.4
C13—C14—H14120.1H5A—O5—H5B109.6
C14—C15—C16118.1 (3)H14A—O6—H6A131.8
C14—C15—H15121.0H14A—O6—H6B123.6
C16—C15—H15121.0H6A—O6—H6B104.5
Symmetry codes: (i) x, y+3/2, z+1/2; (ii) x, y+3/2, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O14—H14A···O61.08 (4)1.40 (4)2.471 (3)173 (3)
O6—H14A···O131.40 (4)2.41 (3)3.215 (3)112.3 (19)
C25—H25···O3iii0.952.593.481 (3)156
O1—H1A···O4iv0.862.212.711 (2)118
O1—H1B···O30.861.922.713 (2)154
O2—H2A···O12v0.852.212.702 (2)116
O2—H2B···O220.851.942.712 (2)150
O3—H3A···O24vi0.851.992.840 (2)174
O3—H3B···O23vii0.852.042.866 (2)163
O4—H4A···O240.851.842.695 (2)177
O4—H4B···O3viii0.852.112.856 (2)145
O5—H5A···O4ix0.852.202.976 (3)150
O5—H5B···O11x0.852.092.939 (3)171
O6—H6A···O50.852.052.772 (3)142
O6—H6B···O12x0.851.812.630 (3)161
Symmetry codes: (iii) x+2, y+1/2, z+3/2; (iv) x+2, y+2, z+1; (v) x+1, y1/2, z+3/2; (vi) x+2, y1/2, z+3/2; (vii) x, y, z+1; (viii) x, y, z1; (ix) x, y1, z+1; (x) x, y1, z.
(I) top
Crystal data top
C21H9N3O12Pr·C4H12N2·C4H11N2·4(H2O)[+solvent]Z = 1
Mr = 1767.18F(000) = 900
Triclinic, P1Dx = 1.572 Mg m3
a = 10.1302 (5) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.4807 (6) ÅCell parameters from 5618 reflections
c = 17.8828 (11) Åθ = 2.8–25.9°
α = 86.979 (4)°µ = 1.38 mm1
β = 80.143 (5)°T = 100 K
γ = 87.451 (4)°Parallelepiped, light-yellow
V = 1866.81 (18) Å30.21 × 0.18 × 0.15 mm
Data collection top
KUMA KM-4 with CCD detector
diffractometer
7325 independent reflections
Radiation source: fine-focus sealed X-ray tube5816 reflections with I > 2σ(I)
Detector resolution: 10.6249 pixels mm-1Rint = 0.081
ω–scanθmax = 26.0°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1212
Tmin = 0.887, Tmax = 1.000k = 1212
28543 measured reflectionsl = 2222
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.061Hydrogen site location: mixed
wR(F2) = 0.164H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.093P)2 + 1.2435P]
where P = (Fo2 + 2Fc2)/3
7325 reflections(Δ/σ)max = 0.001
490 parametersΔρmax = 4.87 e Å3
0 restraintsΔρmin = 1.58 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pr0.50206 (3)0.48944 (3)0.24776 (2)0.01043 (13)
N10.4932 (5)0.7406 (4)0.2430 (3)0.0084 (10)
O10.6835 (4)0.6031 (4)0.1613 (3)0.0148 (10)
O20.3382 (4)0.3172 (4)0.2770 (3)0.0176 (10)
O30.6799 (4)0.3130 (4)0.2245 (3)0.0156 (10)
O40.3121 (4)0.6000 (4)0.3299 (3)0.0158 (10)
O50.6628 (4)0.5427 (4)0.3313 (3)0.0170 (10)
O60.3459 (4)0.5568 (4)0.1571 (3)0.0158 (10)
O70.1827 (4)0.7715 (4)0.3675 (3)0.0186 (10)
O80.8017 (5)0.7751 (4)0.1218 (3)0.0195 (11)
N20.5216 (5)0.3669 (4)0.1216 (3)0.0132 (11)
O90.2517 (4)0.5284 (4)0.0547 (3)0.0191 (10)
O100.2071 (5)0.1873 (4)0.3585 (3)0.0211 (11)
N30.4864 (5)0.3641 (4)0.3784 (3)0.0125 (11)
O110.8043 (4)0.1732 (4)0.1503 (3)0.0192 (10)
O120.7532 (5)0.5144 (5)0.4375 (3)0.0219 (11)
N41.0071 (5)0.5852 (4)0.4341 (3)0.0134 (11)
H4A1.0537280.6402870.3994030.016*
H4B0.9237910.5797730.4221260.016*
N50.0152 (5)0.5872 (5)0.0605 (3)0.0152 (12)
H5A0.0686410.5848840.0724750.018*
H5B0.0675380.6422040.0916040.018*
C10.7022 (6)0.7227 (6)0.1575 (4)0.0110 (13)
C20.7091 (6)0.2519 (5)0.1640 (4)0.0116 (13)
C30.5895 (6)0.8044 (5)0.1995 (4)0.0114 (13)
C40.3870 (6)0.8027 (5)0.2831 (4)0.0120 (13)
C50.2841 (6)0.7194 (5)0.3307 (4)0.0109 (13)
C60.3348 (6)0.5010 (6)0.0968 (3)0.0106 (12)
C70.6172 (6)0.2735 (5)0.1057 (4)0.0137 (13)
C80.5704 (6)0.3917 (6)0.4263 (4)0.0159 (14)
C90.3030 (6)0.2567 (5)0.3405 (4)0.0150 (14)
O130.1033 (5)0.3443 (5)0.2139 (3)0.0268 (12)
H13A0.0817430.4224050.2096710.040*
H13B0.1713790.3414020.2358740.040*
C100.6694 (6)0.4916 (6)0.3972 (4)0.0142 (13)
C110.4376 (6)0.3931 (6)0.0739 (3)0.0140 (13)
C120.3948 (6)0.2753 (5)0.3991 (4)0.0149 (14)
O140.0469 (5)0.5596 (5)0.2728 (3)0.0293 (12)
H14A0.1113940.6016300.2968620.044*
H14B0.0273770.6027170.2312040.044*
N60.0557 (5)0.1425 (5)0.2724 (3)0.0177 (12)
H6A0.0137180.1962600.2608660.021*
H6B0.1040450.1497980.2338020.021*
C131.0761 (7)0.4566 (6)0.4292 (4)0.0178 (14)
H1311.1701740.4635930.4365910.021*
H1321.0772050.4239710.3781670.021*
C140.4734 (7)1.0045 (6)0.2329 (4)0.0223 (16)
H140.4659121.0950710.2273630.027*
C150.3762 (7)0.9365 (6)0.2795 (4)0.0200 (15)
H150.3025330.9798800.3089760.024*
C160.9947 (6)0.6366 (6)0.5107 (4)0.0136 (13)
H1610.9435040.7193460.5121580.016*
H1621.0850690.6517910.5217840.016*
C170.5838 (7)0.9365 (6)0.1937 (4)0.0205 (15)
H170.6547930.9811710.1631920.025*
O150.1220 (5)0.7269 (5)0.1836 (4)0.0334 (13)
H15A0.1988060.6904190.1796840.050*
H15B0.1346420.7978090.1584260.050*
C180.0704 (7)0.4579 (6)0.0733 (4)0.0159 (14)
H1810.1649370.4620660.0654040.019*
H1820.0686980.4273120.1264660.019*
C190.4401 (7)0.3263 (6)0.0076 (4)0.0200 (15)
H190.3759460.3458060.0247040.024*
C200.0091 (6)0.6349 (5)0.0201 (4)0.0164 (14)
H2010.0331160.7190130.0275740.020*
H2020.1011450.6462860.0316970.020*
C210.6286 (7)0.2050 (6)0.0406 (4)0.0185 (14)
H210.6972100.1404850.0300060.022*
C220.3822 (7)0.2096 (6)0.4694 (4)0.0214 (15)
H220.3167540.1466080.4833650.026*
C230.5374 (8)0.2322 (6)0.0092 (4)0.0252 (17)
H230.5429100.1861170.0540890.030*
C240.5637 (7)0.3303 (7)0.4977 (4)0.0239 (16)
H240.6228920.3508190.5307960.029*
C250.4685 (7)0.2385 (7)0.5192 (4)0.0256 (17)
H250.4616450.1952100.5676060.031*
C260.0018 (7)0.0075 (6)0.2795 (4)0.0238 (16)
H2610.0513370.0172190.2303110.029*
H2620.0579490.0009670.3180680.029*
C270.1424 (8)0.1802 (7)0.3441 (4)0.0287 (18)
H2710.1801550.2680350.3376970.034*
H2720.0889790.1785310.3856460.034*
N70.2086 (8)0.0436 (6)0.3716 (4)0.045 (2)
H7A0.2460740.1039970.3908470.054*
C280.1142 (8)0.0801 (6)0.3022 (5)0.0305 (18)
H2810.0768340.1673590.3110350.037*
H2820.1648850.0825570.2596520.037*
O160.1386 (8)0.0283 (7)0.4728 (5)0.066 (2)
H16A0.1436870.0502190.4607430.098*
H16B0.1211150.0324330.5212370.098*
C290.2564 (8)0.0854 (7)0.3639 (5)0.0341 (19)
H2910.3137440.1090480.4120980.041*
H2920.3125090.0924200.3235630.041*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pr0.0088 (2)0.01219 (19)0.0107 (2)0.00075 (13)0.00297 (13)0.00020 (12)
N10.004 (2)0.014 (2)0.008 (3)0.003 (2)0.003 (2)0.0008 (19)
O10.020 (2)0.0033 (19)0.019 (3)0.0007 (17)0.0014 (19)0.0002 (16)
O20.020 (3)0.014 (2)0.019 (3)0.0004 (19)0.002 (2)0.0034 (18)
O30.020 (2)0.009 (2)0.019 (3)0.0048 (18)0.006 (2)0.0051 (18)
O40.021 (3)0.009 (2)0.018 (3)0.0016 (18)0.003 (2)0.0030 (17)
O50.016 (2)0.015 (2)0.019 (3)0.0026 (18)0.001 (2)0.0029 (18)
O60.017 (2)0.013 (2)0.019 (3)0.0053 (18)0.0058 (19)0.0034 (18)
O70.012 (2)0.017 (2)0.023 (3)0.0021 (18)0.007 (2)0.0035 (19)
O80.016 (3)0.011 (2)0.027 (3)0.0063 (19)0.008 (2)0.0003 (19)
N20.013 (3)0.011 (2)0.015 (3)0.004 (2)0.001 (2)0.000 (2)
O90.012 (2)0.029 (3)0.018 (3)0.0008 (19)0.005 (2)0.005 (2)
O100.021 (3)0.011 (2)0.029 (3)0.0077 (19)0.004 (2)0.0023 (19)
N30.015 (3)0.008 (2)0.015 (3)0.004 (2)0.002 (2)0.002 (2)
O110.017 (2)0.015 (2)0.026 (3)0.0075 (19)0.001 (2)0.0068 (19)
O120.014 (2)0.039 (3)0.015 (3)0.001 (2)0.008 (2)0.005 (2)
N40.013 (3)0.013 (3)0.014 (3)0.002 (2)0.002 (2)0.003 (2)
N50.017 (3)0.012 (2)0.017 (3)0.001 (2)0.002 (2)0.004 (2)
C10.008 (3)0.015 (3)0.010 (3)0.003 (2)0.003 (3)0.000 (2)
C20.012 (3)0.006 (3)0.015 (4)0.001 (2)0.002 (3)0.003 (2)
C30.012 (3)0.010 (3)0.013 (3)0.004 (2)0.003 (3)0.002 (2)
C40.007 (3)0.012 (3)0.018 (4)0.001 (2)0.004 (3)0.002 (2)
C50.012 (3)0.010 (3)0.012 (3)0.001 (2)0.002 (3)0.001 (2)
C60.006 (3)0.018 (3)0.009 (3)0.006 (2)0.002 (2)0.001 (2)
C70.015 (3)0.008 (3)0.016 (4)0.005 (2)0.002 (3)0.002 (2)
C80.011 (3)0.019 (3)0.017 (4)0.004 (3)0.002 (3)0.003 (3)
C90.012 (3)0.006 (3)0.022 (4)0.003 (2)0.011 (3)0.003 (2)
O130.024 (3)0.028 (3)0.030 (3)0.007 (2)0.010 (2)0.002 (2)
C100.009 (3)0.019 (3)0.014 (4)0.010 (3)0.001 (3)0.006 (3)
C110.018 (4)0.018 (3)0.006 (3)0.004 (3)0.002 (3)0.002 (2)
C120.016 (3)0.011 (3)0.016 (4)0.006 (3)0.001 (3)0.000 (2)
O140.022 (3)0.032 (3)0.032 (3)0.001 (2)0.000 (2)0.006 (2)
N60.016 (3)0.013 (3)0.023 (3)0.001 (2)0.002 (2)0.004 (2)
C130.021 (4)0.015 (3)0.015 (4)0.002 (3)0.003 (3)0.007 (3)
C140.020 (4)0.014 (3)0.031 (4)0.004 (3)0.001 (3)0.003 (3)
C150.009 (3)0.022 (3)0.029 (4)0.001 (3)0.000 (3)0.009 (3)
C160.013 (3)0.014 (3)0.013 (4)0.002 (2)0.001 (3)0.005 (2)
C170.020 (4)0.016 (3)0.022 (4)0.003 (3)0.005 (3)0.000 (3)
O150.018 (3)0.028 (3)0.053 (4)0.008 (2)0.003 (3)0.002 (3)
C180.017 (4)0.017 (3)0.014 (4)0.004 (3)0.002 (3)0.002 (2)
C190.021 (4)0.024 (3)0.015 (4)0.005 (3)0.001 (3)0.003 (3)
C200.013 (3)0.009 (3)0.026 (4)0.002 (2)0.001 (3)0.001 (3)
C210.015 (3)0.018 (3)0.021 (4)0.002 (3)0.002 (3)0.005 (3)
C220.021 (4)0.019 (3)0.018 (4)0.002 (3)0.009 (3)0.008 (3)
C230.040 (5)0.024 (4)0.014 (4)0.001 (3)0.007 (3)0.012 (3)
C240.021 (4)0.032 (4)0.019 (4)0.015 (3)0.003 (3)0.009 (3)
C250.022 (4)0.034 (4)0.017 (4)0.008 (3)0.003 (3)0.009 (3)
C260.030 (4)0.023 (4)0.018 (4)0.009 (3)0.003 (3)0.005 (3)
C270.034 (5)0.025 (4)0.027 (4)0.001 (3)0.000 (3)0.015 (3)
N70.058 (5)0.020 (3)0.047 (5)0.009 (3)0.022 (4)0.007 (3)
C280.031 (4)0.017 (3)0.042 (5)0.002 (3)0.002 (4)0.001 (3)
O160.059 (5)0.072 (5)0.068 (5)0.014 (4)0.004 (4)0.030 (4)
C290.034 (5)0.034 (4)0.030 (5)0.004 (4)0.007 (4)0.003 (3)
Geometric parameters (Å, º) top
Pr—O22.481 (4)O14—H14A0.8396
Pr—O52.489 (4)O14—H14B0.8472
Pr—O42.493 (4)N6—C271.486 (9)
Pr—O12.493 (4)N6—C261.501 (8)
Pr—O62.508 (4)N6—H6A0.9100
Pr—O32.523 (4)N6—H6B0.9100
Pr—N32.602 (5)C13—C16i1.519 (9)
Pr—N12.627 (5)C13—H1310.9900
Pr—N22.629 (5)C13—H1320.9900
N1—C31.321 (8)C14—C151.375 (9)
N1—C41.349 (7)C14—C171.401 (9)
O1—C11.273 (7)C14—H140.9500
O2—C91.275 (8)C15—H150.9500
O3—C21.270 (7)C16—H1610.9900
O4—C51.272 (7)C16—H1620.9900
O5—C101.279 (8)C17—H170.9500
O6—C61.278 (7)O15—H15A0.8449
O7—C51.242 (7)O15—H15B0.8510
O8—C11.232 (7)C18—C20ii1.505 (8)
N2—C111.315 (8)C18—H1810.9900
N2—C71.352 (8)C18—H1820.9900
O9—C61.237 (7)C19—C231.371 (10)
O10—C91.228 (7)C19—H190.9500
N3—C121.337 (8)C20—H2010.9900
N3—C81.356 (8)C20—H2020.9900
O11—C21.241 (7)C21—C231.401 (10)
O12—C101.242 (8)C21—H210.9500
N4—C161.483 (8)C22—C251.402 (10)
N4—C131.491 (7)C22—H220.9500
N4—H4A0.9100C23—H230.9500
N4—H4B0.9100C24—C251.386 (10)
N5—C181.481 (7)C24—H240.9500
N5—C201.492 (8)C25—H250.9500
N5—H5A0.9100C26—C281.483 (10)
N5—H5B0.9100C26—H2610.9900
C1—C31.512 (8)C26—H2620.9900
C2—C71.515 (9)C27—C291.540 (10)
C3—C171.383 (8)C27—H2710.9900
C4—C151.400 (8)C27—H2720.9900
C4—C51.508 (8)N7—C291.423 (9)
C6—C111.526 (8)N7—C281.487 (10)
C7—C211.385 (9)N7—H7A0.7854
C8—C241.391 (9)C28—H2810.9900
C8—C101.493 (9)C28—H2820.9900
C9—C121.540 (9)O16—H16A0.8408
O13—H13A0.8408O16—H16B0.8534
O13—H13B0.8482C29—H2910.9900
C11—C191.404 (9)C29—H2920.9900
C12—C221.390 (9)
O2—Pr—O5124.60 (15)N2—C11—C19123.0 (6)
O2—Pr—O478.41 (14)N2—C11—C6114.7 (5)
O5—Pr—O491.89 (14)C19—C11—C6122.2 (6)
O2—Pr—O1151.99 (15)N3—C12—C22121.7 (6)
O5—Pr—O175.36 (15)N3—C12—C9114.6 (5)
O4—Pr—O1123.89 (13)C22—C12—C9123.7 (6)
O2—Pr—O680.08 (14)H14A—O14—H14B103.7
O5—Pr—O6150.65 (14)C27—N6—C26111.1 (5)
O4—Pr—O676.76 (14)C27—N6—H6A109.4
O1—Pr—O688.51 (14)C26—N6—H6A109.4
O2—Pr—O386.43 (14)C27—N6—H6B109.4
O5—Pr—O377.34 (14)C26—N6—H6B109.4
O4—Pr—O3151.87 (15)H6A—N6—H6B108.0
O1—Pr—O378.88 (14)N4—C13—C16i110.7 (5)
O6—Pr—O3124.01 (14)N4—C13—H131109.5
O2—Pr—N362.05 (15)C16i—C13—H131109.5
O5—Pr—N362.66 (15)N4—C13—H132109.5
O4—Pr—N376.18 (15)C16i—C13—H132109.5
O1—Pr—N3134.54 (15)H131—C13—H132108.1
O6—Pr—N3136.90 (15)C15—C14—C17118.1 (6)
O3—Pr—N375.79 (15)C15—C14—H14120.9
O2—Pr—N1136.61 (14)C17—C14—H14120.9
O5—Pr—N176.36 (14)C14—C15—C4119.4 (6)
O4—Pr—N162.05 (14)C14—C15—H15120.3
O1—Pr—N161.84 (14)C4—C15—H15120.3
O6—Pr—N174.41 (14)N4—C16—C13i110.6 (5)
O3—Pr—N1136.96 (14)N4—C16—H161109.5
N3—Pr—N1119.42 (15)C13i—C16—H161109.5
O2—Pr—N274.64 (15)N4—C16—H162109.5
O5—Pr—N2134.66 (15)C13i—C16—H162109.5
O4—Pr—N2133.44 (15)H161—C16—H162108.1
O1—Pr—N277.42 (14)C3—C17—C14120.0 (6)
O6—Pr—N261.78 (15)C3—C17—H17120.0
O3—Pr—N262.24 (15)C14—C17—H17120.0
N3—Pr—N2120.57 (15)H15A—O15—H15B104.9
N1—Pr—N2120.00 (15)N5—C18—C20ii111.1 (5)
C3—N1—C4120.9 (5)N5—C18—H181109.4
C3—N1—Pr120.0 (4)C20ii—C18—H181109.4
C4—N1—Pr119.1 (4)N5—C18—H182109.4
C1—O1—Pr126.3 (4)C20ii—C18—H182109.4
C9—O2—Pr127.5 (4)H181—C18—H182108.0
C2—O3—Pr125.4 (4)C23—C19—C11118.3 (6)
C5—O4—Pr127.2 (4)C23—C19—H19120.8
C10—O5—Pr126.0 (4)C11—C19—H19120.8
C6—O6—Pr126.0 (4)N5—C20—C18ii110.6 (5)
C11—N2—C7119.0 (5)N5—C20—H201109.5
C11—N2—Pr121.0 (4)C18ii—C20—H201109.5
C7—N2—Pr120.0 (4)N5—C20—H202109.5
C12—N3—C8120.0 (6)C18ii—C20—H202109.5
C12—N3—Pr120.7 (4)H201—C20—H202108.1
C8—N3—Pr119.3 (4)C7—C21—C23119.0 (6)
C16—N4—C13112.4 (5)C7—C21—H21120.5
C16—N4—H4A109.1C23—C21—H21120.5
C13—N4—H4A109.1C12—C22—C25118.4 (6)
C16—N4—H4B109.1C12—C22—H22120.8
C13—N4—H4B109.1C25—C22—H22120.8
H4A—N4—H4B107.9C19—C23—C21119.0 (6)
C18—N5—C20111.5 (5)C19—C23—H23120.5
C18—N5—H5A109.3C21—C23—H23120.5
C20—N5—H5A109.3C25—C24—C8118.2 (7)
C18—N5—H5B109.3C25—C24—H24120.9
C20—N5—H5B109.3C8—C24—H24120.9
H5A—N5—H5B108.0C24—C25—C22120.0 (7)
O8—C1—O1125.3 (6)C24—C25—H25120.0
O8—C1—C3119.0 (5)C22—C25—H25120.0
O1—C1—C3115.7 (5)C28—C26—N6109.8 (6)
O11—C2—O3125.1 (6)C28—C26—H261109.7
O11—C2—C7117.7 (6)N6—C26—H261109.7
O3—C2—C7117.1 (5)C28—C26—H262109.7
N1—C3—C17120.9 (6)N6—C26—H262109.7
N1—C3—C1115.3 (5)H261—C26—H262108.2
C17—C3—C1123.8 (5)N6—C27—C29108.5 (5)
N1—C4—C15120.7 (6)N6—C27—H271110.0
N1—C4—C5115.9 (5)C29—C27—H271110.0
C15—C4—C5123.5 (5)N6—C27—H272110.0
O7—C5—O4126.0 (6)C29—C27—H272110.0
O7—C5—C4118.6 (5)H271—C27—H272108.4
O4—C5—C4115.3 (5)C29—N7—C28110.7 (6)
O9—C6—O6126.3 (6)C29—N7—H7A130.1
O9—C6—C11117.6 (5)C28—N7—H7A109.9
O6—C6—C11116.1 (5)C26—C28—N7114.1 (6)
N2—C7—C21121.6 (6)C26—C28—H281108.7
N2—C7—C2114.7 (5)N7—C28—H281108.7
C21—C7—C2123.7 (6)C26—C28—H282108.7
N3—C8—C24121.7 (6)N7—C28—H282108.7
N3—C8—C10115.5 (6)H281—C28—H282107.6
C24—C8—C10122.7 (6)H16A—O16—H16B105.0
O10—C9—O2127.4 (7)N7—C29—C27112.8 (7)
O10—C9—C12118.6 (6)N7—C29—H291109.0
O2—C9—C12114.0 (5)C27—C29—H291109.0
H13A—O13—H13B105.2N7—C29—H292109.0
O12—C10—O5125.9 (6)C27—C29—H292109.0
O12—C10—C8117.6 (6)H291—C29—H292107.8
O5—C10—C8116.5 (6)
Symmetry codes: (i) x+2, y+1, z+1; (ii) x, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H4A···O7iii0.911.942.781 (7)154
N4—H4B···O120.911.862.698 (7)152
N5—H5A···O90.911.902.732 (7)151
N5—H5B···O1iv0.912.653.270 (7)126
N5—H5B···O8iv0.911.912.780 (7)159
N6—H6A···O130.911.912.767 (7)155
N6—H6B···O11iv0.911.892.798 (8)176
C13—H131···O4iii0.992.593.117 (8)113
C13—H131···O12i0.992.533.209 (8)126
C15—H15···O10v0.952.483.317 (8)146
C16—H162···O12i0.992.503.190 (8)126
C17—H17···O11v0.952.553.383 (8)147
C18—H181···O1iv0.992.583.095 (8)112
C18—H181···O9ii0.992.453.164 (8)129
C18—H182···O130.992.633.443 (8)140
C19—H19···O1vi0.952.643.496 (8)151
C20—H202···O9ii0.992.533.218 (8)127
Symmetry codes: (i) x+2, y+1, z+1; (ii) x, y+1, z; (iii) x+1, y, z; (iv) x1, y, z; (v) x, y+1, z; (vi) x+1, y+1, z.
(III) top
Crystal data top
C12H11N4O11PrDx = 2.183 Mg m3
Mr = 528.16Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcaCell parameters from 7873 reflections
a = 7.9007 (4) Åθ = 2.8–26.2°
b = 14.6884 (5) ŵ = 3.11 mm1
c = 27.6980 (13) ÅT = 100 K
V = 3214.3 (2) Å3Parallelepiped, colourless
Z = 80.25 × 0.14 × 0.10 mm
F(000) = 2064
Data collection top
KUMA KM-4 with CCD detector
diffractometer
3801 independent reflections
Radiation source: fine-focus sealed X-ray tube2752 reflections with I > 2σ(I)
Detector resolution: 10.6249 pixels mm-1Rint = 0.076
ω–scanθmax = 27.8°, θmin = 2.8°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 1010
Tmin = 0.763, Tmax = 1.000k = 1919
52105 measured reflectionsl = 3636
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.051Hydrogen site location: mixed
wR(F2) = 0.111H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.044P)2 + 7.8115P]
where P = (Fo2 + 2Fc2)/3
3801 reflections(Δ/σ)max = 0.002
256 parametersΔρmax = 2.86 e Å3
0 restraintsΔρmin = 1.12 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pr0.48728 (4)0.61073 (2)0.62835 (2)0.00916 (11)
N10.3517 (6)0.6093 (3)0.53425 (19)0.0136 (11)
C20.3036 (7)0.5256 (4)0.5191 (2)0.0113 (12)
C30.2290 (8)0.5104 (4)0.4746 (2)0.0133 (13)
N40.2029 (6)0.5844 (3)0.44616 (19)0.0138 (11)
H4N0.1505270.5770850.4183830.017*
C50.2541 (7)0.6685 (4)0.4588 (2)0.0164 (13)
H50.2398330.7186700.4376210.020*
C60.3280 (7)0.6795 (4)0.5036 (2)0.0122 (12)
H60.3635360.7386200.5130990.015*
C70.3340 (7)0.4488 (4)0.5545 (2)0.0128 (12)
O10.4351 (5)0.4669 (3)0.58857 (15)0.0132 (9)
O20.2620 (5)0.3763 (3)0.54671 (16)0.0161 (9)
C80.1789 (7)0.4195 (3)0.4527 (2)0.0108 (12)
O30.0271 (5)0.4013 (2)0.45289 (16)0.0146 (9)
O40.3026 (5)0.3745 (2)0.43566 (15)0.0107 (9)
N110.8329 (6)0.3538 (3)0.7313 (2)0.0158 (11)
C120.8571 (7)0.4430 (4)0.7223 (2)0.0139 (13)
C130.8914 (7)0.5044 (4)0.7595 (2)0.0098 (12)
N140.8920 (6)0.4787 (3)0.80534 (19)0.0149 (11)
C150.8652 (8)0.3887 (4)0.8146 (2)0.0175 (14)
H140.8648910.3676010.8470060.021*
C160.8382 (8)0.3272 (4)0.7770 (2)0.0175 (14)
H160.8232080.2645910.7843370.021*
C170.8373 (7)0.4689 (4)0.6701 (2)0.0124 (12)
O110.7227 (5)0.5241 (3)0.65889 (16)0.0174 (10)
O120.9294 (6)0.4264 (3)0.63951 (16)0.0160 (10)
C180.9353 (7)0.6044 (4)0.7516 (2)0.0109 (12)
O130.9766 (5)0.6280 (2)0.70995 (15)0.0132 (9)
O140.9285 (5)0.6540 (3)0.78803 (15)0.0137 (9)
O1W0.1724 (5)0.6122 (3)0.62895 (16)0.0133 (9)
H1A0.1331410.6587540.6122910.020*
H1B0.1340050.6226830.6582660.020*
O2W0.4080 (5)0.7723 (3)0.61148 (16)0.0139 (9)
H2A0.3980330.7831400.5794690.021*
H2B0.4917670.8109390.6200630.021*
O3W0.7172 (5)0.7219 (3)0.65719 (15)0.0152 (9)
H3A0.8081620.6922480.6672660.023*
H3B0.6840050.7514960.6833240.023*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pr0.00849 (17)0.00732 (17)0.01167 (19)0.00026 (13)0.00022 (12)0.00031 (12)
N10.010 (3)0.013 (2)0.017 (3)0.0008 (19)0.001 (2)0.002 (2)
C20.004 (3)0.012 (3)0.018 (3)0.005 (2)0.001 (2)0.003 (2)
C30.014 (3)0.011 (3)0.015 (3)0.003 (2)0.003 (2)0.003 (2)
N40.014 (3)0.013 (2)0.015 (3)0.000 (2)0.003 (2)0.001 (2)
C50.013 (3)0.015 (3)0.022 (4)0.001 (2)0.003 (3)0.004 (3)
C60.012 (3)0.008 (3)0.017 (3)0.002 (2)0.003 (2)0.001 (2)
C70.011 (3)0.014 (3)0.013 (3)0.004 (2)0.003 (2)0.002 (3)
O10.011 (2)0.0138 (18)0.015 (2)0.0001 (16)0.0007 (17)0.0015 (18)
O20.016 (2)0.015 (2)0.017 (3)0.0047 (17)0.0022 (18)0.0000 (18)
C80.009 (3)0.009 (3)0.014 (3)0.000 (2)0.000 (2)0.002 (2)
O30.008 (2)0.0144 (17)0.022 (2)0.0034 (16)0.0001 (17)0.0052 (17)
O40.008 (2)0.0078 (16)0.017 (2)0.0000 (15)0.0021 (16)0.0016 (17)
N110.007 (2)0.017 (3)0.023 (3)0.003 (2)0.002 (2)0.001 (2)
C120.010 (3)0.011 (3)0.021 (4)0.007 (2)0.000 (2)0.003 (3)
C130.007 (3)0.010 (2)0.012 (3)0.001 (2)0.002 (2)0.000 (2)
N140.008 (3)0.013 (2)0.024 (3)0.000 (2)0.005 (2)0.000 (2)
C150.022 (3)0.013 (3)0.018 (4)0.005 (2)0.002 (3)0.002 (3)
C160.018 (3)0.008 (3)0.026 (4)0.005 (2)0.002 (3)0.001 (3)
C170.008 (3)0.010 (3)0.019 (4)0.007 (2)0.003 (2)0.000 (2)
O110.016 (2)0.0140 (19)0.022 (3)0.0011 (18)0.0030 (19)0.0006 (18)
O120.017 (2)0.012 (2)0.018 (3)0.0057 (17)0.0028 (18)0.0015 (18)
C180.007 (3)0.014 (3)0.012 (3)0.003 (2)0.006 (2)0.001 (3)
O130.011 (2)0.0136 (17)0.015 (2)0.0002 (16)0.0014 (17)0.0003 (17)
O140.014 (2)0.0132 (18)0.014 (2)0.0009 (16)0.0049 (18)0.0004 (18)
O1W0.007 (2)0.018 (2)0.015 (2)0.0022 (17)0.0010 (16)0.0018 (19)
O2W0.011 (2)0.0119 (19)0.018 (2)0.0017 (16)0.0050 (18)0.0024 (18)
O3W0.011 (2)0.0117 (18)0.023 (3)0.0009 (16)0.0046 (18)0.0036 (18)
Geometric parameters (Å, º) top
Pr—O112.407 (4)C8—O31.229 (7)
Pr—O12.418 (4)C8—O41.270 (7)
Pr—O4i2.439 (4)N11—C161.324 (8)
Pr—O14ii2.446 (4)N11—C121.348 (7)
Pr—O1W2.488 (4)C12—C131.398 (8)
Pr—O2W2.499 (4)C12—C171.502 (9)
Pr—O3W2.570 (4)C13—N141.323 (8)
Pr—N14ii2.775 (5)C13—C181.525 (7)
Pr—N12.818 (5)N14—C151.363 (7)
N1—C61.350 (7)C15—C161.395 (8)
N1—C21.354 (7)C15—H140.9500
C2—C31.383 (8)C16—H160.9500
C2—C71.514 (8)C17—O111.254 (7)
C3—N41.358 (7)C17—O121.279 (7)
C3—C81.520 (7)C18—O141.246 (7)
N4—C51.346 (7)C18—O131.247 (7)
N4—H4N0.8800O1W—H1A0.8809
C5—C61.379 (9)O1W—H1B0.8801
C5—H50.9500O2W—H2A0.9042
C6—H60.9500O2W—H2B0.9032
C7—O21.227 (7)O3W—H3A0.8852
C7—O11.265 (7)O3W—H3B0.8843
O11—Pr—O180.21 (14)N4—C5—C6118.0 (6)
O11—Pr—O4i77.09 (14)N4—C5—H5121.0
O1—Pr—O4i82.09 (13)C6—C5—H5121.0
O11—Pr—O14ii87.22 (14)N1—C6—C5122.3 (5)
O1—Pr—O14ii128.75 (13)N1—C6—H6118.9
O4i—Pr—O14ii142.63 (14)C5—C6—H6118.9
O11—Pr—O1W140.80 (14)O2—C7—O1127.3 (5)
O1—Pr—O1W80.81 (13)O2—C7—C2117.4 (5)
O4i—Pr—O1W133.21 (14)O1—C7—C2115.3 (5)
O14ii—Pr—O1W78.54 (14)C7—O1—Pr129.1 (4)
O11—Pr—O2W139.60 (14)O3—C8—O4129.8 (5)
O1—Pr—O2W134.58 (14)O3—C8—C3116.3 (5)
O4i—Pr—O2W87.14 (13)O4—C8—C3113.9 (5)
O14ii—Pr—O2W83.27 (13)C8—O4—Pri138.4 (4)
O1W—Pr—O2W75.07 (13)C16—N11—C12117.4 (5)
O11—Pr—O3W71.36 (13)N11—C12—C13121.2 (6)
O1—Pr—O3W144.81 (14)N11—C12—C17114.3 (5)
O4i—Pr—O3W71.84 (13)C13—C12—C17124.6 (5)
O14ii—Pr—O3W71.04 (14)N14—C13—C12121.6 (5)
O1W—Pr—O3W134.36 (13)N14—C13—C18114.4 (5)
O2W—Pr—O3W68.39 (13)C12—C13—C18124.0 (5)
O11—Pr—N14ii66.90 (14)C13—N14—C15117.1 (5)
O1—Pr—N14ii69.20 (14)C13—N14—Priii115.8 (3)
O4i—Pr—N14ii136.72 (13)C15—N14—Priii126.6 (4)
O14ii—Pr—N14ii60.21 (13)N14—C15—C16120.7 (6)
O1W—Pr—N14ii74.37 (14)N14—C15—H14119.6
O2W—Pr—N14ii136.02 (14)C16—C15—H14119.6
O3W—Pr—N14ii115.47 (14)N11—C16—C15121.8 (5)
O11—Pr—N1127.92 (14)N11—C16—H16119.1
O1—Pr—N160.46 (13)C15—C16—H16119.1
O4i—Pr—N165.60 (14)O11—C17—O12124.2 (6)
O14ii—Pr—N1143.66 (14)O11—C17—C12118.5 (6)
O1W—Pr—N168.05 (14)O12—C17—C12117.0 (5)
O2W—Pr—N174.88 (13)C17—O11—Pr170.5 (4)
O3W—Pr—N1124.13 (14)O14—C18—O13126.8 (5)
N14ii—Pr—N1120.24 (14)O14—C18—C13115.8 (5)
C6—N1—C2117.3 (5)O13—C18—C13117.4 (5)
C6—N1—Pr129.0 (4)C18—O14—Priii127.4 (3)
C2—N1—Pr113.7 (4)Pr—O1W—H1A110.8
N1—C2—C3122.9 (5)Pr—O1W—H1B110.6
N1—C2—C7115.5 (5)H1A—O1W—H1B103.1
C3—C2—C7121.7 (5)Pr—O2W—H2A111.8
N4—C3—C2116.9 (5)Pr—O2W—H2B111.3
N4—C3—C8115.6 (5)H2A—O2W—H2B102.2
C2—C3—C8127.4 (5)Pr—O3W—H3A111.1
C5—N4—C3122.4 (5)Pr—O3W—H3B110.9
C5—N4—H4N118.8H3A—O3W—H3B103.0
C3—N4—H4N118.8
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1/2, y, z+3/2; (iii) x+1/2, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N4—H4N···O12i0.881.722.597 (7)171
C5—H5···O4iv0.952.313.127 (7)143
C6—H6···O2iv0.952.443.207 (7)138
C15—H14···O1iii0.952.372.970 (8)121
C16—H16···O13v0.952.563.292 (7)134
C16—H16···O14vi0.952.573.318 (7)136
O1W—H1B···O13vii0.881.902.735 (6)158
O2W—H2A···O2iv0.902.072.712 (6)127
O2W—H2B···O12viii0.901.892.716 (6)152
O3W—H3A···O130.892.022.870 (6)162
O3W—H3B···N11viii0.882.012.851 (7)158
Symmetry codes: (i) x+1, y+1, z+1; (iii) x+1/2, y, z+3/2; (iv) x+1/2, y+1/2, z; (v) x+2, y1/2, z+3/2; (vi) x+3/2, y1/2, z; (vii) x1, y, z; (viii) x+3/2, y+1/2, z.
(IV) top
Crystal data top
C24H20N8O22Pr2Zn·2(H2O)F(000) = 1128
Mr = 1155.70Dx = 2.298 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 6.1336 (2) ÅCell parameters from 5676 reflections
b = 22.6987 (8) Åθ = 3.2–31.1°
c = 11.9981 (4) ŵ = 3.70 mm1
β = 91.196 (3)°T = 100 K
V = 1670.07 (10) Å3Parallelepiped, colourless
Z = 20.22 × 0.09 × 0.08 mm
Data collection top
KUMA KM-4 with CCD detector
diffractometer
5542 independent reflections
Radiation source: fine-focus sealed X-ray tube4195 reflections with I > 2σ(I)
Detector resolution: 10.6249 pixels mm-1Rint = 0.060
ω–scanθmax = 32.6°, θmin = 2.5°
Absorption correction: multi-scan
CrysAlisPro 1.171.38.43 (Rigaku Oxford Diffraction, 2015) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
h = 98
Tmin = 0.918, Tmax = 1.000k = 3329
20894 measured reflectionsl = 1818
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038Hydrogen site location: mixed
wR(F2) = 0.070H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.0198P)2 + 1.1093P]
where P = (Fo2 + 2Fc2)/3
5542 reflections(Δ/σ)max = 0.001
274 parametersΔρmax = 1.41 e Å3
0 restraintsΔρmin = 0.96 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pr0.43969 (3)0.64572 (2)0.44235 (2)0.00534 (5)
Zn1.0000000.5000000.0000000.00879 (12)
N10.6444 (5)0.70098 (13)0.2628 (2)0.0080 (6)
C20.5250 (5)0.74357 (15)0.2134 (3)0.0066 (7)
C30.5961 (5)0.77310 (15)0.1186 (3)0.0072 (7)
N40.8010 (5)0.76470 (13)0.0834 (2)0.0081 (6)
C50.9187 (5)0.72203 (16)0.1322 (3)0.0087 (7)
H51.0617020.7143210.1070160.010*
C60.8372 (5)0.68870 (16)0.2189 (3)0.0088 (7)
H60.9202360.6565510.2474890.011*
C70.3219 (6)0.76196 (16)0.2756 (3)0.0085 (7)
O10.2588 (4)0.72606 (11)0.34865 (19)0.0095 (5)
O20.2438 (4)0.81059 (11)0.2544 (2)0.0116 (5)
C80.4618 (6)0.81407 (16)0.0450 (3)0.0086 (7)
O30.2701 (4)0.80021 (11)0.01956 (19)0.0090 (5)
O40.5619 (4)0.85859 (11)0.0083 (2)0.0115 (5)
N110.7518 (5)0.56232 (13)0.0085 (2)0.0088 (6)
C120.6110 (5)0.54902 (16)0.0891 (3)0.0079 (7)
C130.4370 (6)0.58657 (16)0.1083 (3)0.0091 (7)
N140.4045 (5)0.63667 (13)0.0506 (2)0.0109 (6)
C150.5465 (6)0.64801 (17)0.0288 (3)0.0106 (7)
H150.5279890.6827570.0721220.013*
C160.7201 (6)0.61117 (16)0.0508 (3)0.0096 (7)
H160.8173240.6208450.1086720.012*
C170.6572 (6)0.49241 (16)0.1530 (3)0.0094 (7)
O110.7926 (4)0.45782 (11)0.1104 (2)0.0103 (5)
O120.5578 (4)0.48544 (12)0.2405 (2)0.0155 (6)
C180.2623 (6)0.57313 (16)0.1910 (3)0.0081 (7)
O130.2660 (4)0.60033 (11)0.2814 (2)0.0117 (5)
O140.1140 (4)0.53817 (11)0.1597 (2)0.0119 (5)
O1W0.3275 (5)0.53961 (11)0.4838 (2)0.0187 (6)
H1A0.2504250.5249240.4276490.028*
H1B0.2362280.5382180.5394570.028*
O2W0.7460 (4)0.58334 (11)0.3848 (2)0.0147 (6)
H2A0.7167280.5462730.3959310.022*
H2B0.8597870.5896620.4277400.022*
O3W0.5262 (5)0.61214 (12)0.6343 (2)0.0227 (7)
H3A0.4184670.5915000.6602520.034*
H3B0.5340060.6422570.6793360.034*
O4W0.0320 (5)0.47626 (14)0.3579 (2)0.0254 (7)
H4A0.0920990.4426900.3651760.038*
H4B0.0337720.4830840.2882710.038*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pr0.00536 (8)0.00519 (9)0.00548 (8)0.00021 (8)0.00003 (6)0.00010 (7)
Zn0.0073 (3)0.0097 (3)0.0094 (3)0.0006 (2)0.0020 (2)0.0002 (2)
N10.0080 (13)0.0080 (15)0.0078 (13)0.0000 (12)0.0009 (11)0.0012 (11)
C20.0081 (16)0.0029 (16)0.0088 (16)0.0020 (13)0.0010 (13)0.0010 (12)
C30.0060 (15)0.0070 (17)0.0085 (16)0.0015 (13)0.0013 (13)0.0023 (13)
N40.0091 (14)0.0070 (15)0.0081 (14)0.0007 (12)0.0004 (11)0.0002 (11)
C50.0042 (15)0.0099 (18)0.0121 (17)0.0010 (13)0.0005 (13)0.0007 (13)
C60.0064 (15)0.0069 (17)0.0130 (17)0.0003 (14)0.0019 (13)0.0007 (14)
C70.0086 (16)0.0089 (18)0.0079 (16)0.0011 (14)0.0016 (13)0.0034 (13)
O10.0087 (12)0.0132 (14)0.0065 (12)0.0022 (10)0.0023 (9)0.0023 (10)
O20.0172 (13)0.0087 (13)0.0089 (12)0.0068 (11)0.0002 (10)0.0000 (10)
C80.0072 (16)0.0113 (18)0.0073 (16)0.0022 (14)0.0025 (13)0.0010 (13)
O30.0054 (11)0.0114 (14)0.0100 (12)0.0015 (10)0.0003 (9)0.0011 (10)
O40.0072 (11)0.0118 (14)0.0157 (12)0.0007 (11)0.0048 (10)0.0063 (11)
N110.0110 (14)0.0090 (15)0.0064 (13)0.0016 (12)0.0002 (11)0.0019 (11)
C120.0063 (15)0.0096 (18)0.0077 (15)0.0000 (14)0.0018 (12)0.0037 (13)
C130.0124 (17)0.0078 (18)0.0070 (15)0.0023 (14)0.0017 (13)0.0025 (13)
N140.0118 (15)0.0097 (17)0.0110 (14)0.0005 (12)0.0020 (12)0.0025 (12)
C150.0133 (17)0.0085 (18)0.0100 (16)0.0012 (15)0.0023 (13)0.0003 (14)
C160.0092 (16)0.0083 (18)0.0115 (17)0.0037 (14)0.0029 (13)0.0005 (13)
C170.0082 (16)0.0100 (18)0.0098 (16)0.0015 (14)0.0019 (13)0.0058 (14)
O110.0099 (12)0.0072 (13)0.0138 (12)0.0008 (10)0.0031 (10)0.0012 (10)
O120.0206 (14)0.0162 (15)0.0100 (12)0.0072 (12)0.0062 (11)0.0042 (10)
C180.0087 (16)0.0068 (17)0.0088 (16)0.0059 (14)0.0033 (13)0.0003 (13)
O130.0106 (12)0.0128 (14)0.0115 (12)0.0015 (11)0.0003 (10)0.0057 (10)
O140.0119 (12)0.0152 (14)0.0085 (12)0.0015 (11)0.0004 (10)0.0030 (10)
O1W0.0286 (16)0.0096 (14)0.0175 (14)0.0049 (12)0.0128 (12)0.0014 (11)
O2W0.0100 (13)0.0073 (13)0.0269 (15)0.0012 (11)0.0034 (11)0.0015 (11)
O3W0.0427 (19)0.0131 (15)0.0120 (14)0.0147 (14)0.0085 (13)0.0021 (11)
O4W0.0287 (17)0.035 (2)0.0127 (14)0.0167 (15)0.0026 (13)0.0014 (13)
Geometric parameters (Å, º) top
Pr—O12.402 (2)C7—O11.264 (4)
Pr—O132.417 (2)C8—O31.249 (4)
Pr—O2W2.463 (2)C8—O41.267 (4)
Pr—O4i2.466 (2)N11—C161.330 (4)
Pr—O3W2.473 (3)N11—C121.344 (4)
Pr—O3ii2.528 (2)C12—C131.389 (5)
Pr—O1W2.557 (3)C12—C171.520 (5)
Pr—N4i2.789 (3)C13—N141.344 (4)
Pr—N12.811 (3)C13—C181.506 (5)
Zn—N112.082 (3)N14—C151.329 (4)
Zn—N11iii2.082 (3)C15—C161.384 (5)
Zn—O11iii2.088 (2)C15—H150.9500
Zn—O112.088 (2)C16—H160.9500
Zn—O14iv2.204 (2)C17—O121.235 (4)
Zn—O14v2.204 (2)C17—O111.259 (4)
N1—C61.334 (4)C18—O131.248 (4)
N1—C21.343 (4)C18—O141.258 (4)
C2—C31.399 (5)O1W—H1A0.8801
C2—C71.523 (5)O1W—H1B0.8810
C3—N41.348 (4)O2W—H2A0.8714
C3—C81.514 (5)O2W—H2B0.8707
N4—C51.336 (4)O3W—H3A0.8726
C5—C61.387 (5)O3W—H3B0.8719
C5—H50.9500O4W—H4A0.8502
C6—H60.9500O4W—H4B0.8501
C7—O21.228 (4)
O1—Pr—O1376.00 (8)N4—C3—C2119.7 (3)
O1—Pr—O2W130.75 (8)N4—C3—C8113.8 (3)
O13—Pr—O2W81.78 (8)C2—C3—C8126.4 (3)
O1—Pr—O4i75.66 (8)C5—N4—C3117.6 (3)
O13—Pr—O4i80.67 (8)C5—N4—Prvi128.7 (2)
O2W—Pr—O4i142.62 (9)C3—N4—Prvi112.7 (2)
O1—Pr—O3W139.28 (9)N4—C5—C6121.6 (3)
O13—Pr—O3W134.05 (9)N4—C5—H5119.2
O2W—Pr—O3W86.22 (9)C6—C5—H5119.2
O4i—Pr—O3W82.75 (9)N1—C6—C5121.2 (3)
O1—Pr—O3ii99.31 (8)N1—C6—H6119.4
O13—Pr—O3ii146.76 (8)C5—C6—H6119.4
O2W—Pr—O3ii76.80 (8)O2—C7—O1126.8 (3)
O4i—Pr—O3ii130.77 (8)O2—C7—C2117.7 (3)
O3W—Pr—O3ii69.74 (9)O1—C7—C2115.4 (3)
O1—Pr—O1W133.05 (8)C7—O1—Pr132.0 (2)
O13—Pr—O1W68.76 (9)O3—C8—O4125.2 (3)
O2W—Pr—O1W73.92 (9)O3—C8—C3119.1 (3)
O4i—Pr—O1W69.00 (9)O4—C8—C3115.5 (3)
O3W—Pr—O1W65.29 (9)C8—O3—Prvii135.3 (2)
O3ii—Pr—O1W127.09 (8)C8—O4—Prvi123.1 (2)
O1—Pr—N4i65.59 (8)C16—N11—C12118.9 (3)
O13—Pr—N4i131.34 (8)C16—N11—Zn129.7 (2)
O2W—Pr—N4i146.43 (9)C12—N11—Zn111.4 (2)
O4i—Pr—N4i62.22 (8)N11—C12—C13119.3 (3)
O3W—Pr—N4i73.86 (9)N11—C12—C17115.9 (3)
O3ii—Pr—N4i71.10 (8)C13—C12—C17124.8 (3)
O1W—Pr—N4i118.82 (9)N14—C13—C12122.6 (3)
O1—Pr—N160.78 (8)N14—C13—C18114.3 (3)
O13—Pr—N176.96 (8)C12—C13—C18123.0 (3)
O2W—Pr—N171.70 (8)C15—N14—C13116.2 (3)
O4i—Pr—N1134.52 (8)N14—C15—C16122.6 (3)
O3W—Pr—N1139.52 (9)N14—C15—H15118.7
O3ii—Pr—N172.36 (8)C16—C15—H15118.7
O1W—Pr—N1134.08 (9)N11—C16—C15120.4 (3)
N4i—Pr—N1106.64 (8)N11—C16—H16119.8
N11—Zn—N11iii180.00 (12)C15—C16—H16119.8
N11—Zn—O11iii100.09 (10)O12—C17—O11127.3 (4)
N11iii—Zn—O11iii79.91 (10)O12—C17—C12116.5 (3)
N11—Zn—O1179.91 (10)O11—C17—C12116.1 (3)
N11iii—Zn—O11100.09 (10)C17—O11—Zn112.8 (2)
O11iii—Zn—O11180.00 (10)O13—C18—O14124.8 (3)
N11—Zn—O14iv95.21 (10)O13—C18—C13118.1 (3)
N11iii—Zn—O14iv84.79 (10)O14—C18—C13116.8 (3)
O11iii—Zn—O14iv79.34 (9)C18—O13—Pr154.9 (2)
O11—Zn—O14iv100.66 (9)C18—O14—Znviii136.1 (2)
N11—Zn—O14v84.79 (10)Pr—O1W—H1A110.5
N11iii—Zn—O14v95.21 (10)Pr—O1W—H1B111.0
O11iii—Zn—O14v100.66 (9)H1A—O1W—H1B103.1
O11—Zn—O14v79.34 (9)Pr—O2W—H2A110.5
O14iv—Zn—O14v180.00 (12)Pr—O2W—H2B110.2
C6—N1—C2117.1 (3)H2A—O2W—H2B103.5
C6—N1—Pr128.5 (2)Pr—O3W—H3A110.4
C2—N1—Pr114.3 (2)Pr—O3W—H3B110.1
N1—C2—C3121.8 (3)H3A—O3W—H3B103.4
N1—C2—C7115.2 (3)H4A—O4W—H4B104.5
C3—C2—C7122.6 (3)
Symmetry codes: (i) x1/2, y+3/2, z+1/2; (ii) x+1/2, y+3/2, z+1/2; (iii) x+2, y+1, z; (iv) x+1, y+1, z; (v) x+1, y, z; (vi) x+1/2, y+3/2, z1/2; (vii) x1/2, y+3/2, z1/2; (viii) x1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O3v0.952.573.121 (4)118
C6—H6···O13v0.952.503.379 (4)154
C6—H6···O2W0.952.593.169 (4)120
C15—H15···O2vi0.952.493.040 (4)117
C16—H16···O2vi0.952.302.941 (4)124
O1W—H1A···O4W0.881.922.742 (4)156
O1W—H1B···O4Wix0.882.102.962 (4)165
O2W—H2A···O120.872.503.031 (4)120
O2W—H2A···O1Wx0.872.443.242 (4)153
O2W—H2A···O4Wv0.872.553.019 (4)115
O2W—H2B···O4ii0.871.952.751 (4)152
O3W—H3A···O12x0.872.122.731 (4)127
O3W—H3B···O2ii0.871.892.618 (4)140
Symmetry codes: (ii) x+1/2, y+3/2, z+1/2; (v) x+1, y, z; (vi) x+1/2, y+3/2, z1/2; (ix) x, y+1, z+1; (x) x+1, y+1, z+1.
 

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