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A redetermination of the structure of poly[[μ4-(R)-2-ammonio-3-sulfonato­propano­ato]aqua­sodium], originally reported as poly[[μ7-L-cysteato(2−)]disodium]

aBrockhouse Institute for Materials Research, McMaster University Hamilton, Ontario, Canada L8S 4M1
*Correspondence e-mail: idbrown@mcmaster.ca

(Received 27 February 2012; accepted 5 March 2012; online 10 March 2012)

The structure originally reported as poly[[μ7-L-cysteato(2−)]disodium], [Na2(C3H5NO5S)]n [Liu (2002). Acta Cryst. E67, m1346–m1347], has been redetermined with one of the sodium atoms replaced with a water mol­ecule and an additional proton attached to the amine group, resulting in the revised formula [Na{CO2CH(CH2SO3)NH3}(H2O)]n. The agreement index, wR, has been reduced from 0.159 to 0.087 and the global instability index from 0.56 vu (valence units) to the acceptable value of 0.11 vu.

Related literature

The original structure determination of this compound was reported by Liu (2011[Liu, F.-H. (2011). Acta Cryst. E67, m1346-m1347.]). The bond-valence methods are described in Brown (2002[Brown, I. D. (2002). The Chemical Bond in Inorganic Chemistry, The Bond Valence Model, IUCr Monographs on Crystallography 12, p. 166. Oxford University Press.]).

[Scheme 1]

Experimental

Crystal data
  • [Na(C3H6NO5S)(H2O)]

  • Mr = 209.15

  • Monoclinic, P 21 /c

  • a = 5.7574 (12) Å

  • b = 11.875 (2) Å

  • c = 11.691 (3) Å

  • β = 109.15 (3)°

  • V = 755.1 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.48 mm−1

  • T = 298 K

  • 0.24 × 0.22 × 0.20 mm

Data collection
  • Rigaku SCX-Mini CCD diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995[Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.]) Tmin = 0.894, Tmax = 0.911

  • 7845 measured reflections

  • 1740 independent reflections

  • 1463 reflections with I > 2Σ(I)

  • Rint = 0.044

Refinement
  • R[F2 > 2σ(F2)] = 0.038

  • wR(F2) = 0.087

  • S = 1.10

  • 1740 reflections

  • 118 parameters

  • 2 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.39 e Å−3

  • Δρmin = −0.35 e Å−3

Table 1
Selected bond lengths (Å)

Na1—O4i 2.3512 (19)
Na1—O5ii 2.3619 (19)
Na1—O3 2.4183 (18)
Na1—O2iii 2.4272 (19)
Na1—O1W 2.450 (2)
Na1—O1 2.4778 (18)
Symmetry codes: (i) x-1, y, z; (ii) [x, -y+{\script{3\over 2}}, z+{\script{1\over 2}}]; (iii) [-x, y-{\script{1\over 2}}, -z+{\script{1\over 2}}].

Table 2
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O1Wiv 0.89 2.16 2.981 (3) 153
N1—H1B⋯O1v 0.89 1.97 2.842 (2) 166
N1—H1C⋯O2iv 0.89 1.88 2.766 (2) 173
O1W—H1WA⋯O3ii 0.85 (1) 2.10 (1) 2.912 (3) 160 (4)
O1W—H1WB⋯O5vi 0.85 (1) 2.08 (1) 2.930 (2) 178 (3)
Symmetry codes: (ii) [x, -y+{\script{3\over 2}}, z+{\script{1\over 2}}]; (iv) x+1, y, z; (v) -x+1, -y+2, -z+1; (vi) [x-1, -y+{\script{3\over 2}}, z+{\script{1\over 2}}].

Data collection: PROCESS-AUTO (Rigaku, 1998[Rigaku (1998). PROCESS-AUTO. Rigaku Corporation, Tokyo, Japan.]); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2002[Rigaku/MSC (2002). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.]); method used to solve structure: coordinates taken from the previous refinement (Liu, 2011[Liu, F.-H. (2011). Acta Cryst. E67, m1346-m1347.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: Mercury (Macrae et al., 2006[Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453-457.]); software used to prepare material for publication: publCIF (Westrip, 2010[Westrip, S. P. (2010). J. Appl. Cryst. 43, 920-925.]).

Supporting information


Comment top

In a recent issue of this journal, Liu (2011) reported the structure of the title compound, but a close examination of this structure shows a serious problem with the environment of one of the sodium atoms, Na2. In the Comment the author describes this atom as 'tetracoordinated within an NO3 coordination sphere. The Na+ ion binds to the amino N atom, to one of the O atom of the carboxylic residue and to two O atoms of the sulfonate group in a distorted tetrahedral arrangement'. The Comment does not point out that the atomic displacement parameter of Na2 is almost three times larger than the next largest atomic displacement parameter, nor does it point out that the lengths of the four bonds around Na2 all lie in the range 2.90 to 3.03 Å, distances whose bond valence sum of 0.21 vu (valence unit) indicates that they are much longer than would be expected for a four-coordinate sodium cation. The global instability index [root mean square deviation of the bond valence sums of all atoms from their atomic valence, (Brown, 2002)] is 0.56 vu, much higher than the generally accepted limit of 0.20 vu for a stable structure. The environment of Na2 is, however, one that would be expected for a water molecule that forms moderate to weak hydrogen bonds. An additional hydrogen ion is required for charge neutrality, but protonating the water molecule is unlikely as this would require much shorter hydrogen bonds than are observed for this site, but protonating the amine group would not only increase the bond valence sum around the nitrogen from 2.51 vu to a value closer to the expected 3.00 vu, it would also result in an N—H bond positioned to form a hydrogen bond with the water molecule.

This proposed model has been refined and is reported in this paper. The bond valence sum of 0.21 vu around the original Na2 has been replaced by a sum of 1.94 vu around the oxygen of water, and the sum around the N1 atom has been increased to 3.17 vu. Moreover, Na1 now has a meaningful octahedral environment (Fig. 1) with a Na1—O1W contact of 2.450 (2) Å instead of a Na1—Na2 contact as in the original model.

Based on the rerefinement of the structure, this crystal must be reformulated as sodium (R)-2-ammonium-3-sulfopropanoate monohydrate, Na(CO2CH(CH2SO3)NH3)(H2O).

Related literature top

The original structure determination of this compound was reported by Liu (2011). The bond-valence methods are described in Brown (2002).

Experimental top

The preparation of the compound is detailed in the original report (Liu, 2011).

Refinement top

The structure was refined using the original diffraction measurements of Liu (2011). For re-refinement of the original model, all H atoms were removed in the first refinement cycle and the doubtful atom Na2 replaced by an O atom (O1W). All H atoms were discernible from difference maps. H atoms attached to C atoms were finally included in calculated positions using a riding model with bond lengths C—H = 0.97 or 0.98 Å and Uiso(H) = 1.2 times Ueq(C); H atoms attached to the ammonium group were constrained to bond lengths N—H = 0.89 Å with Uiso(H) = 1.5 times Ueq(N). The water H atoms were restrained to bond lengths of 0.85 (1) Å.

Structure description top

In a recent issue of this journal, Liu (2011) reported the structure of the title compound, but a close examination of this structure shows a serious problem with the environment of one of the sodium atoms, Na2. In the Comment the author describes this atom as 'tetracoordinated within an NO3 coordination sphere. The Na+ ion binds to the amino N atom, to one of the O atom of the carboxylic residue and to two O atoms of the sulfonate group in a distorted tetrahedral arrangement'. The Comment does not point out that the atomic displacement parameter of Na2 is almost three times larger than the next largest atomic displacement parameter, nor does it point out that the lengths of the four bonds around Na2 all lie in the range 2.90 to 3.03 Å, distances whose bond valence sum of 0.21 vu (valence unit) indicates that they are much longer than would be expected for a four-coordinate sodium cation. The global instability index [root mean square deviation of the bond valence sums of all atoms from their atomic valence, (Brown, 2002)] is 0.56 vu, much higher than the generally accepted limit of 0.20 vu for a stable structure. The environment of Na2 is, however, one that would be expected for a water molecule that forms moderate to weak hydrogen bonds. An additional hydrogen ion is required for charge neutrality, but protonating the water molecule is unlikely as this would require much shorter hydrogen bonds than are observed for this site, but protonating the amine group would not only increase the bond valence sum around the nitrogen from 2.51 vu to a value closer to the expected 3.00 vu, it would also result in an N—H bond positioned to form a hydrogen bond with the water molecule.

This proposed model has been refined and is reported in this paper. The bond valence sum of 0.21 vu around the original Na2 has been replaced by a sum of 1.94 vu around the oxygen of water, and the sum around the N1 atom has been increased to 3.17 vu. Moreover, Na1 now has a meaningful octahedral environment (Fig. 1) with a Na1—O1W contact of 2.450 (2) Å instead of a Na1—Na2 contact as in the original model.

Based on the rerefinement of the structure, this crystal must be reformulated as sodium (R)-2-ammonium-3-sulfopropanoate monohydrate, Na(CO2CH(CH2SO3)NH3)(H2O).

The original structure determination of this compound was reported by Liu (2011). The bond-valence methods are described in Brown (2002).

Computing details top

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO (Rigaku, 1998); data reduction: CrystalStructure (Rigaku/MSC, 2002); program(s) used to solve structure: coordinates taken from the previous refinement (Liu, 2011); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Figures top
[Figure 1] Fig. 1. The environment of the Na+ cation with atomic displacement parameters drawn at the 50% probability level. [Symmetry codes: (i) x - 1, y, z; (ii) x, -y + 3/2, z + 1/2; (iii) -x, y - 1/2, -z + 1/2.]
poly[[µ4-(R)-2-ammonio-3-sulfonatopropanoato]aquasodium] top
Crystal data top
[Na(C3H6NO5S)(H2O)]F(000) = 432
Mr = 209.15Dx = 1.840 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 7309 reflections
a = 5.7574 (12) Åθ = 3.4–27.5°
b = 11.875 (2) ŵ = 0.48 mm1
c = 11.691 (3) ÅT = 298 K
β = 109.15 (3)°Prism, colourless
V = 755.1 (3) Å30.24 × 0.22 × 0.20 mm
Z = 4
Data collection top
Rigaku SCX-Mini CCD
diffractometer
1740 independent reflections
Radiation source: fine-focus sealed tube1463 reflections with I > 2Σ(I)
Graphite monochromatorRint = 0.044
ω scansθmax = 27.5°, θmin = 3.4°
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
h = 77
Tmin = 0.894, Tmax = 0.911k = 1515
7845 measured reflectionsl = 1515
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: inferred from neighbouring sites
wR(F2) = 0.087H atoms treated by a mixture of independent and constrained refinement
S = 1.10 w = 1/[σ2(Fo2) + (0.0337P)2 + 0.5281P]
where P = (Fo2 + 2Fc2)/3
1740 reflections(Δ/σ)max = 0.001
118 parametersΔρmax = 0.39 e Å3
2 restraintsΔρmin = 0.35 e Å3
Crystal data top
[Na(C3H6NO5S)(H2O)]V = 755.1 (3) Å3
Mr = 209.15Z = 4
Monoclinic, P21/cMo Kα radiation
a = 5.7574 (12) ŵ = 0.48 mm1
b = 11.875 (2) ÅT = 298 K
c = 11.691 (3) Å0.24 × 0.22 × 0.20 mm
β = 109.15 (3)°
Data collection top
Rigaku SCX-Mini CCD
diffractometer
1740 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
1463 reflections with I > 2Σ(I)
Tmin = 0.894, Tmax = 0.911Rint = 0.044
7845 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0382 restraints
wR(F2) = 0.087H atoms treated by a mixture of independent and constrained refinement
S = 1.10Δρmax = 0.39 e Å3
1740 reflectionsΔρmin = 0.35 e Å3
118 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Na10.04743 (15)0.74874 (7)0.32550 (8)0.0227 (2)
C10.2113 (4)1.00587 (18)0.31408 (19)0.0187 (4)
C20.4306 (4)1.03306 (18)0.27159 (19)0.0183 (4)
H20.43921.11530.26770.022*
C30.3962 (4)0.98919 (18)0.14342 (19)0.0202 (5)
H3A0.52011.02410.11550.024*
H3B0.23711.01460.09050.024*
N10.6664 (3)0.99540 (16)0.36077 (16)0.0229 (4)
H1A0.66380.92100.36940.034*
H1B0.68691.02840.43180.034*
H1C0.79001.01430.33470.034*
O10.2380 (3)0.93424 (13)0.39576 (13)0.0244 (4)
O20.0199 (3)1.06104 (14)0.26136 (16)0.0294 (4)
O30.2321 (3)0.78831 (14)0.17151 (15)0.0310 (4)
O40.6636 (3)0.80928 (14)0.19436 (15)0.0300 (4)
O50.3578 (3)0.82358 (14)0.00367 (13)0.0251 (4)
S10.41302 (9)0.84075 (4)0.12587 (5)0.01761 (15)
O1W0.1946 (4)0.76543 (17)0.46236 (17)0.0356 (4)
H1WA0.090 (5)0.759 (4)0.5329 (15)0.090 (15)*
H1WB0.326 (3)0.740 (3)0.471 (3)0.058 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Na10.0214 (5)0.0242 (5)0.0216 (5)0.0005 (4)0.0058 (4)0.0015 (4)
C10.0195 (11)0.0171 (10)0.0209 (11)0.0036 (9)0.0087 (9)0.0060 (9)
C20.0178 (10)0.0169 (10)0.0221 (11)0.0000 (8)0.0091 (9)0.0003 (8)
C30.0228 (11)0.0187 (11)0.0209 (11)0.0011 (9)0.0094 (9)0.0013 (9)
N10.0174 (9)0.0297 (10)0.0223 (10)0.0022 (8)0.0073 (8)0.0045 (8)
O10.0275 (9)0.0259 (8)0.0216 (8)0.0031 (7)0.0105 (7)0.0012 (7)
O20.0195 (8)0.0306 (9)0.0411 (10)0.0060 (7)0.0139 (7)0.0091 (8)
O30.0366 (10)0.0311 (9)0.0319 (9)0.0106 (8)0.0203 (8)0.0026 (7)
O40.0256 (9)0.0286 (9)0.0291 (9)0.0075 (7)0.0000 (7)0.0007 (7)
O50.0264 (8)0.0309 (9)0.0184 (8)0.0045 (7)0.0079 (7)0.0053 (6)
S10.0193 (3)0.0179 (3)0.0160 (3)0.0013 (2)0.0063 (2)0.0006 (2)
O1W0.0274 (10)0.0517 (12)0.0302 (10)0.0023 (9)0.0127 (9)0.0119 (9)
Geometric parameters (Å, º) top
Na1—O4i2.3512 (19)C3—S11.781 (2)
Na1—O5ii2.3619 (19)C3—H3A0.9700
Na1—O32.4183 (18)C3—H3B0.9700
Na1—O2iii2.4272 (19)N1—H1A0.8900
Na1—O1W2.450 (2)N1—H1B0.8900
Na1—O12.4778 (18)N1—H1C0.8900
C1—O11.250 (3)O3—S11.4567 (16)
C1—O21.256 (3)O4—S11.4505 (17)
C1—C21.535 (3)O5—S11.4561 (16)
C2—N11.484 (3)O1W—H1WA0.8499 (11)
C2—C31.537 (3)O1W—H1WB0.8500 (11)
C2—H20.9800
O4i—Na1—O5ii162.02 (7)C2—C3—H3A108.1
O4i—Na1—O390.22 (7)S1—C3—H3A108.1
O5ii—Na1—O3107.74 (7)C2—C3—H3B108.1
O4i—Na1—O2iii91.21 (7)S1—C3—H3B108.1
O5ii—Na1—O2iii89.57 (7)H3A—C3—H3B107.3
O3—Na1—O2iii85.17 (6)C2—N1—H1A109.5
O4i—Na1—O1W77.69 (7)C2—N1—H1B109.5
O5ii—Na1—O1W84.94 (7)H1A—N1—H1B109.5
O3—Na1—O1W162.46 (7)C2—N1—H1C109.5
O2iii—Na1—O1W107.49 (7)H1A—N1—H1C109.5
O4i—Na1—O199.41 (7)H1B—N1—H1C109.5
O5ii—Na1—O185.01 (6)C1—O1—Na1114.94 (13)
O3—Na1—O179.58 (6)C1—O2—Na1iv132.70 (14)
O2iii—Na1—O1161.39 (6)S1—O3—Na1153.84 (11)
O1W—Na1—O189.79 (7)S1—O4—Na1v172.12 (12)
O1—C1—O2126.7 (2)S1—O5—Na1vi140.97 (10)
O1—C1—C2118.85 (19)O4—S1—O5112.10 (10)
O2—C1—C2114.45 (18)O4—S1—O3112.88 (11)
N1—C2—C1111.67 (17)O5—S1—O3112.51 (10)
N1—C2—C3112.25 (17)O4—S1—C3105.86 (10)
C1—C2—C3112.80 (17)O5—S1—C3104.88 (10)
N1—C2—H2106.5O3—S1—C3107.96 (10)
C1—C2—H2106.5Na1—O1W—H1WA105 (3)
C3—C2—H2106.5Na1—O1W—H1WB140 (2)
C2—C3—S1116.96 (15)H1WA—O1W—H1WB103 (3)
Symmetry codes: (i) x1, y, z; (ii) x, y+3/2, z+1/2; (iii) x, y1/2, z+1/2; (iv) x, y+1/2, z+1/2; (v) x+1, y, z; (vi) x, y+3/2, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1Wv0.892.162.981 (3)153
N1—H1B···O1vii0.891.972.842 (2)166
N1—H1C···O2v0.891.882.766 (2)173
O1W—H1WA···O3ii0.85 (1)2.10 (1)2.912 (3)160 (4)
O1W—H1WB···O5viii0.85 (1)2.08 (1)2.930 (2)178 (3)
Symmetry codes: (ii) x, y+3/2, z+1/2; (v) x+1, y, z; (vii) x+1, y+2, z+1; (viii) x1, y+3/2, z+1/2.

Experimental details

Crystal data
Chemical formula[Na(C3H6NO5S)(H2O)]
Mr209.15
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)5.7574 (12), 11.875 (2), 11.691 (3)
β (°) 109.15 (3)
V3)755.1 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.48
Crystal size (mm)0.24 × 0.22 × 0.20
Data collection
DiffractometerRigaku SCX-Mini CCD
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.894, 0.911
No. of measured, independent and
observed [I > 2Σ(I)] reflections
7845, 1740, 1463
Rint0.044
(sin θ/λ)max1)0.649
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.038, 0.087, 1.10
No. of reflections1740
No. of parameters118
No. of restraints2
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.39, 0.35

Computer programs: PROCESS-AUTO (Rigaku, 1998), CrystalStructure (Rigaku/MSC, 2002), coordinates taken from the previous refinement (Liu, 2011), SHELXL97 (Sheldrick, 2008), Mercury (Macrae et al., 2006), publCIF (Westrip, 2010).

Selected bond lengths (Å) top
Na1—O4i2.3512 (19)Na1—O2iii2.4272 (19)
Na1—O5ii2.3619 (19)Na1—O1W2.450 (2)
Na1—O32.4183 (18)Na1—O12.4778 (18)
Symmetry codes: (i) x1, y, z; (ii) x, y+3/2, z+1/2; (iii) x, y1/2, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1Wiv0.892.162.981 (3)152.5
N1—H1B···O1v0.891.972.842 (2)166.3
N1—H1C···O2iv0.891.882.766 (2)172.6
O1W—H1WA···O3ii0.8499 (11)2.100 (14)2.912 (3)160 (4)
O1W—H1WB···O5vi0.8500 (11)2.081 (3)2.930 (2)178 (3)
Symmetry codes: (ii) x, y+3/2, z+1/2; (iv) x+1, y, z; (v) x+1, y+2, z+1; (vi) x1, y+3/2, z+1/2.
 

Acknowledgements

I wish to thank Dr Liu for supplying the original diffraction measurements through the editorial office of the journal.

References

First citationBrown, I. D. (2002). The Chemical Bond in Inorganic Chemistry, The Bond Valence Model, IUCr Monographs on Crystallography 12, p. 166. Oxford University Press.  Google Scholar
First citationHigashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationLiu, F.-H. (2011). Acta Cryst. E67, m1346–m1347.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationMacrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.  Web of Science CSD CrossRef CAS IUCr Journals Google Scholar
First citationRigaku (1998). PROCESS-AUTO. Rigaku Corporation, Tokyo, Japan.  Google Scholar
First citationRigaku/MSC (2002). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationWestrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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