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The aim of this study was to test the applicability of a Bruker AXS CMOS-type PHOTON 100 detector for the purpose of a fine charge density quality data collection. A complex crystal containing oxalic acid, ammonium oxalate and two water molecules was chosen as a test case. The data was collected up to a resolution of 1.31 Å-1 with high completeness (89.1%; Rmrg = 0.0274). The multipolar refinement and subsequent quantum theory of atoms in molecules (QTAIM) analysis resulted in a comprehensive description of the charge density distribution in the crystal studied. The residual density maps are flat and almost featureless. It was possible to derive reliable information on intermolecular interactions to model the anharmonic motion of a water molecule, and also to observe the fine details of the charge density distribution, such as polarization on O and H atoms involved in the strongest hydrogen bonds. When compared with our previous statistical study on oxalic acid data collected with the aid of CCD cameras, the complementary metal-oxide semiconductor (CMOS) detector can certainly be classified as a promising alternative in advanced X-ray diffraction studies.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520614017570/pi5019sup1.cif
Contains datablocks global, CCDC994769

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520614017570/pi5019Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520614017570/pi5019sup3.pdf
Additional figures concerning charge density distribution properties for selected molecular fragments present in the studied crystal structure

CCDC reference: 1017251

Computing details top

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
(CCDC994769) top
Crystal data top
C2H2O4·C2HO4·2(H2O)·H4NZ = 2
Mr = 233.14F(000) = 244
Triclinic, P1Dx = 1.693 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.2372 (4) ÅCell parameters from 50285 reflections
b = 7.1935 (5) Åθ = 2.9–62.7°
c = 10.4745 (7) ŵ = 0.17 mm1
α = 94.5207 (18)°T = 100 K
β = 99.8882 (18)°Block, colourless
γ = 96.7177 (19)°0.24 × 0.21 × 0.09 mm
V = 457.45 (5) Å3
Data collection top
Bruker AXS CMOS-type PHOTON 100 detector
diffractometer
14225 independent reflections
Radiation source: Mo sealed tube9995 reflections with I > 3σ(I)
Bruker AXS TRIUMPH monochromatorRint = 0.027
ω–scansθmax = 62.7°, θmin = 2.9°
Absorption correction: multi-scan
Blessing, R. H. (1995). Acta Cryst. A51, 33.
h = 1515
Tmin = 0.966, Tmax = 0.985k = 1717
50285 measured reflectionsl = 2626
Refinement top
Refinement on F0 constraints
R[F2 > 2σ(F2)] = 0.018H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.019Weighting scheme based on measured s.u.'s
S = 0.89(Δ/σ)max = 0.001
9995 reflectionsΔρmax = 0.21 e Å3
349 parametersΔρmin = 0.22 e Å3
11 restraints
Crystal data top
C2H2O4·C2HO4·2(H2O)·H4Nγ = 96.7177 (19)°
Mr = 233.14V = 457.45 (5) Å3
Triclinic, P1Z = 2
a = 6.2372 (4) ÅMo Kα radiation
b = 7.1935 (5) ŵ = 0.17 mm1
c = 10.4745 (7) ÅT = 100 K
α = 94.5207 (18)°0.24 × 0.21 × 0.09 mm
β = 99.8882 (18)°
Data collection top
Bruker AXS CMOS-type PHOTON 100 detector
diffractometer
14225 independent reflections
Absorption correction: multi-scan
Blessing, R. H. (1995). Acta Cryst. A51, 33.
9995 reflections with I > 3σ(I)
Tmin = 0.966, Tmax = 0.985Rint = 0.027
50285 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.01811 restraints
wR(F2) = 0.019H atoms treated by a mixture of independent and constrained refinement
S = 0.89Δρmax = 0.21 e Å3
9995 reflectionsΔρmin = 0.22 e Å3
349 parameters
Special details top

Refinement. Charge density refinement with MOPRO.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.91907 (3)0.99061 (2)0.434750 (16)0.008183 (18)
O10.99847 (3)1.07806 (2)0.347080 (18)0.01122 (2)
O20.73730 (3)0.89896 (2)0.422253 (18)0.011035 (19)
H10.8864 (7)1.0737 (8)0.2635 (3)0.02215
C20.00527 (3)0.54831 (2)0.436891 (15)0.007976 (18)
O30.16034 (3)0.49158 (2)0.345256 (18)0.011645 (19)
O40.16083 (3)0.66736 (2)0.432415 (18)0.010331 (18)
H20.1597 (10)0.5606 (6)0.2641 (3)0.02258
C30.25600 (3)0.32260 (2)0.079880 (15)0.008246 (19)
C40.22704 (3)0.43423 (2)0.041301 (15)0.008285 (19)
O50.31702 (3)0.42913 (3)0.188972 (19)0.01331 (3)
O60.22397 (3)0.15078 (3)0.068753 (19)0.01157 (2)
O70.26332 (3)0.60867 (3)0.021946 (19)0.01260 (3)
O80.17055 (3)0.33476 (3)0.149168 (18)0.01172 (3)
H30.3583 (11)0.3526 (6)0.2651 (3)0.02424
N10.34265 (3)0.84352 (2)0.224738 (15)0.009907 (18)
H40.2387 (7)0.7924 (8)0.2849 (4)0.02287
H50.5015 (4)0.8681 (8)0.2773 (5)0.02287
H60.3005 (9)0.9689 (4)0.1921 (5)0.02287
H70.3302 (10)0.7418 (5)0.1472 (3)0.02287
O90.73177 (3)0.07349 (2)0.144464 (17)0.01065 (2)
H80.7342 (10)0.1931 (4)0.1100 (5)0.02348
H90.7637 (9)0.0136 (6)0.0785 (4)0.02348
O100.44580 (7)0.25116 (5)0.37589 (9)0.01327 (2)
H100.3578 (7)0.2033 (7)0.4355 (4)0.02610
H110.5895 (4)0.2977 (8)0.4241 (5)0.02610
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.00815 (5)0.00918 (4)0.00676 (4)0.00034 (3)0.00027 (3)0.00162 (3)
O10.01042 (5)0.01478 (5)0.00787 (5)0.00084 (4)0.00041 (4)0.00404 (4)
O20.00902 (5)0.01385 (5)0.00884 (5)0.00195 (4)0.00071 (4)0.00287 (3)
H10.019340.029640.015600.000940.001200.00667
C20.00944 (5)0.00760 (4)0.00638 (4)0.00049 (3)0.00057 (3)0.00190 (3)
O30.01319 (5)0.01180 (5)0.00779 (4)0.00314 (4)0.00204 (4)0.00365 (4)
O40.01067 (5)0.01120 (4)0.00833 (4)0.00227 (4)0.00092 (4)0.00347 (3)
H20.025480.023980.015830.003690.001140.00827
C30.01159 (5)0.00685 (4)0.00616 (4)0.00119 (3)0.00081 (3)0.00165 (3)
C40.01160 (5)0.00688 (4)0.00615 (4)0.00113 (3)0.00062 (3)0.00167 (3)
O50.02403 (9)0.00861 (5)0.00626 (5)0.00190 (4)0.00007 (4)0.00100 (4)
O60.01907 (7)0.00680 (5)0.00811 (5)0.00065 (3)0.00062 (4)0.00204 (3)
O70.02245 (8)0.00664 (5)0.00827 (5)0.00165 (3)0.00123 (4)0.00195 (4)
O80.01921 (7)0.00864 (5)0.00592 (4)0.00011 (3)0.00050 (3)0.00144 (3)
H30.039610.017940.014060.004530.000120.00419
N10.01177 (5)0.00884 (4)0.00870 (4)0.00004 (3)0.00129 (3)0.00165 (3)
H40.022440.026990.019910.000780.006740.00651
H50.018090.027810.020640.000290.000660.00392
H60.030670.016710.021610.005430.002740.00536
H70.031160.018910.017380.003130.002950.00174
O90.01333 (6)0.01079 (5)0.00774 (4)0.00203 (3)0.00071 (4)0.00241 (3)
H80.030650.018460.022280.004330.004270.00751
H90.030230.022270.018540.005820.005690.00057
O100.01135 (5)0.01727 (6)0.01020 (5)0.00168 (4)0.00048 (4)0.00603 (4)
H100.023970.033060.021730.002080.006000.01020
H110.018600.033120.023190.003280.002550.00602
Geometric parameters (Å, º) top
C1—O11.2879 (3)C4—O81.2608 (3)
C1—O21.2238 (3)O5—H31.0180 (9)
O1—H11.0180 (9)N1—H71.0358 (9)
C2—O31.2860 (3)N1—H51.0358 (9)
C2—O41.2266 (3)N1—H61.0359 (9)
O3—H21.0180 (9)N1—H41.0359 (9)
C3—O51.2970 (3)O9—H90.9580 (9)
C3—O61.2217 (3)O9—H80.9581 (9)
C3—C41.5506 (2)O10—H100.9580 (9)
C4—O71.2428 (3)O10—H110.9580 (9)
C1—O1—H1112.3 (3)O7—C4—O8127.63 (3)
O1—C1—O2126.76 (3)H4—N1—H7107.4 (4)
C2—O3—H2113.9 (3)H4—N1—H5108.7 (4)
O3—C2—O4126.67 (2)H4—N1—H6110.9 (5)
C3—O5—H3111.7 (3)H5—N1—H7110.7 (5)
C3—C4—O7117.271 (16)H5—N1—H6108.5 (4)
C3—C4—O8115.096 (19)H6—N1—H7110.7 (4)
C4—C3—O5113.458 (16)H8—O9—H9106.6 (5)
C4—C3—O6121.13 (2)H10—O10—H11108.1 (5)
O5—C3—O6125.41 (2)
O2—C1—O1—H1O5—C3—C4—O8
O4—C2—O3—H2O6—C3—O5—H3
C4—C3—O5—H3O6—C3—C4—O7
O5—C3—C4—O7O6—C3—C4—O8

Experimental details

Crystal data
Chemical formulaC2H2O4·C2HO4·2(H2O)·H4N
Mr233.14
Crystal system, space groupTriclinic, P1
Temperature (K)100
a, b, c (Å)6.2372 (4), 7.1935 (5), 10.4745 (7)
α, β, γ (°)94.5207 (18), 99.8882 (18), 96.7177 (19)
V3)457.45 (5)
Z2
Radiation typeMo Kα
µ (mm1)0.17
Crystal size (mm)0.24 × 0.21 × 0.09
Data collection
DiffractometerBruker AXS CMOS-type PHOTON 100 detector
diffractometer
Absorption correctionMulti-scan
Blessing, R. H. (1995). Acta Cryst. A51, 33.
Tmin, Tmax0.966, 0.985
No. of measured, independent and
observed [I > 3σ(I)] reflections
50285, 14225, 9995
Rint0.027
(sin θ/λ)max1)1.250
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.018, 0.019, 0.89
No. of reflections9995
No. of parameters349
No. of restraints11
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.21, 0.22

 

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