Abstract
The redetermined crystal structure of the title compound, C11H13N2O2 +·Br−, is reported. Data collection at 100 K about three crystallographic axes resulted in a crystal structure with significantly higher precision in comparison to the two-dimensional data collected at 176 K [Takigawa et al. [(1966) Bull. Chem. Soc. Jpn, 39, 2369–2378]. The carboxyl group and indole ring system are planar, with maximum deviations of 0.002 (2) and 0.007 (2) Å, respectively, and make an angle of 70.17 (1)° with each other. The molecules are arranged in double layers of carboxyl and amino groups parallel to the ab plane, stabilized by an extensive network of N—H⋯Br and O—H⋯Br hydrogen bonds. The polar layer is held together by a network of three N—H⋯Br hydrogen bonds and one O—H⋯Br hydrogen bond. In the non-polar layer, the indole rings are linked mainly by electrostatic N—H⋯C interactions between the polarized bond N—H (H is δ+) of the pyrrole unit and two of the ring C atoms (δ−) of the benzene rings of adjacent molecules. The distances of these electrostatic interactions are 2.57 and 2.68 Å, respectively. C—H⋯O and C—H⋯π interactions are also present.
Related literature
For a previous determination of the crystal structure of the title compound, see: Takigawa et al. (1966 ▶). Study of crystal structures of amino acids and their complexes has provided information about aggregation and the effect of other molecules on their interactions and molecular properties, see: Vijayan (1988 ▶); Prasad & Vijayan (1993 ▶). For the structure of histidine hydrochloride monohydrate, see: Takigawa et al. (1966 ▶). Donohue & Caron (1964 ▶). The structures of many amino acids with non-polar side chains feature a double-layered arrangement, see: Harding & Long (1968 ▶); Torii & Iitaka (1970 ▶, 1971 ▶, 1973 ▶).
Experimental
Crystal data
C11H13N2O2 +·Br−
M r = 285.13
Monoclinic,
a = 7.6272 (3) Å
b = 5.3840 (2) Å
c = 14.4358 (5) Å
β = 100.688 (3)°
V = 582.52 (4) Å3
Z = 2
Mo Kα radiation
μ = 3.52 mm−1
T = 100 K
0.40 × 0.15 × 0.15 mm
Data collection
Oxford Xcalibur2 CCD diffractometer
Absorption correction: multi-scan (SCALE3 ABSPACK in CrysAlis RED; Oxford Diffraction, 2008 ▶) T min = 0.334, T max = 0.621
5749 measured reflections
2731 independent reflections
2507 reflections with I > 2σ(I)
R int = 0.024
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.063
S = 1.01
2731 reflections
147 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.33 e Å−3
Δρmin = −1.14 e Å−3
Absolute structure: Flack (1983 ▶), 523 Freidel pairs
Flack parameter: 0.009 (9)
Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809017322/at2781sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809017322/at2781Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C7—H4⋯Cg1i | 0.95 | 2.66 | 3.494 (3) | 146 |
| N1—H5⋯Cg2i | 0.88 | 2.72 | 3.406 (2) | 136 |
| N2—H11⋯Br1ii | 0.91 | 2.56 | 3.3208 (17) | 142 |
| N2—H12⋯Br1iii | 0.91 | 2.42 | 3.322 (3) | 173 |
| N2—H13⋯Br1iv | 0.91 | 2.52 | 3.320 (3) | 147 |
| C4—H1⋯Br1iii | 0.95 | 2.85 | 3.750 (2) | 159 |
| C10—H9⋯O1v | 1.00 | 2.49 | 3.404 (3) | 153 |
| C10—H9⋯O1ii | 1.00 | 2.56 | 3.199 (3) | 121 |
| O2—H10⋯Br1 | 0.84 | 2.34 | 3.173 (2) | 169 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
. Cg1 is the centroid of the N1/C1–C3/C8 ring and Cg2 is the centroid of the C3–C8 ring.
Acknowledgments
The author gratefully acknowledges financial support from the University of Kwazulu-Natal. Thanks are also due to Ms C. Janse Van Rensburg for the mass spectrum analysis.
supplementary crystallographic information
Comment
The crystal structures of amino acids and their complexes have provided interesting information about aggregation, and the effect of other molecules on their interaction and molecular properties (Vijayan, 1988; Prasad & Vijayan 1993).
The crystal structure of L-tryptophan hydrobromide was determined some 40 years ago (Takigawa et al., 1966). The final refinement was carried out to only R = 0.101 with no data available for H atoms. The reported structure possesses almost identical crystal parameters to the structure reported here in terms of space group and unit-cell dimensions and angles. However, the collection of data at 100 K about three crystallographic axes in comparison to the data reported by Takigawa et al. resulted in more accurate data thus allowing some previously unidentified notable conclusions to be drawn about the crystal structure.
The C—N distance 1.488 (3) Å coincides well with those in e.g. histidine hydrochloride monohydrate (1.495 Å) (Donohue & Caron, 1964). The two C—O bond lengths are 1.316 (3) Å and 1.204 (3) Å for C11—O2 and C11—O1, respectively and the three angles around the C11 atom are O2—C11—O1 = 125.8 (2)°, O2—C11—C10 = 110.0 (2) ° and O1—C11—C10 = 124.1 (2) °.
The planarity of the carboxyl group with the α-carbon has been established in many investigations and the deviations of the amino nitrogen range from 0.00 to 0.82 Å for the amino acids so far investigated. For the present molecule, the amino nitrogen is 0.094 Å out of the plane, so the amide group is essentially planar in this case.
The mean plane through the atoms of the indole ring with the methylene carbon attached to it forms a dihedral angle of 70.17 (1) ° with the mean plane of the carboxyl group.
The structures of many amino acids with non-polar side chains have the arrangement of a double layered system (Torii & Iitaka 1970; Torii & Iitaka, 1971; Torii & Iitaka, 1973; Harding & Long, 1968) which is characteristic for a structure containing polar and non-polar groups together. The polar layer is held together by a network of hydrogen bonds between the halide ions and the amino nitrogen and the halide ions and the carboxyl group.
The amino nitrogen forms three N—H···Br hydrogen bonds, in the lengths of 2.56 (1) Å, 2.41 (1) Å and 2.52 (1) Å. The three acceptor halogen ions are approximately at the three vertices of a regular tetrahedron centred around the nitrogen atom, with the fourth vortex positioned in the direction of the α-carbon.
The fourth hydrogen bond completing the network is a O—H···Br- which is 2.34 (1) Å in length.
In the non-polar layer, the indole rings are packed in a manner similar to that found for typical aromatic molecules. A weak electrostatic interaction with a separation of 2.677 (1) Å exists between N1—H5 from the pyrrole moiety and the slightly positively charged C6 from the benzene moiety of a neighbouring symmetry related molecule [-x, -1/2 + y, 1 - z]. A similar interaction with a separation of 2.573 (1) Å exists between the same N1—H5 and C7 from the benzene moiety of molecule [-x, -1/2 + y, 1 - z]. The metrics of such interactions are reflected in the T-shaped edge-to-face geometry in the non-polar layer.
Experimental
L-tryptophan hydrobromide was obtained in the form of plate-like crystals by dissolving L-tryptophan in concentrated hydrobromic acid followed by slow evaporation at room temperature.
HRMS (ES-): Found [M—H] 283.0082 C11H12N2O2Br Expected 283.0080 (-0.7 ppm).
Refinement
All H atoms were positioned in geometrically idealized positions and constrained to ride on their parent atoms with N—H = 0.91 Å, O—H = 0.84 Å and C—H distances in the range 0.95–1.00 Å. and Uiso(H)= 1.2–1.5 Ueq(parent atom).
Figures
Fig. 1.
Molecular structure of (L)-2-amino-3-(1H-indol-3-yl)-propionic acid hydrobromide, showing 50% probability displacement ellipsoids and atomic numbering.
Fig. 2.
Packing diagram showing a view along the a axis.
Crystal data
| C11H13N2O2+·Br− | F(000) = 288 |
| Mr = 285.13 | Dx = 1.626 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 4434 reflections |
| a = 7.6272 (3) Å | θ = 3.8–31.9° |
| b = 5.3840 (2) Å | µ = 3.52 mm−1 |
| c = 14.4358 (5) Å | T = 100 K |
| β = 100.688 (3)° | Needle, colourless |
| V = 582.52 (4) Å3 | 0.40 × 0.15 × 0.15 mm |
| Z = 2 |
Data collection
| Oxford Xcalibur2 CCD diffractometer | 2731 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 2507 reflections with I > 2σ(I) |
| graphite | Rint = 0.024 |
| Detector resolution: 8.4190 pixels mm-1 | θmax = 32.0°, θmin = 4.1° |
| ω/2θ scans | h = −11→10 |
| Absorption correction: multi-scan (SCALE3 ABSPACK in CrysAlis RED; Oxford Diffraction, 2008) | k = −6→7 |
| Tmin = 0.334, Tmax = 0.621 | l = −21→21 |
| 5749 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.027 | H-atom parameters constrained |
| wR(F2) = 0.063 | w = 1/[σ2(Fo2) + (0.0388P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.01 | (Δ/σ)max < 0.001 |
| 2731 reflections | Δρmax = 0.33 e Å−3 |
| 147 parameters | Δρmin = −1.14 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 523 Freidel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.009 (9) |
Special details
| 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)
| x | y | z | Uiso*/Ueq | ||
| C1 | 0.2755 (3) | 0.4954 (5) | 0.66336 (17) | 0.0112 (4) | |
| H6 | 0.4001 | 0.5280 | 0.6774 | 0.013* | |
| C2 | 0.1920 (3) | 0.3004 (4) | 0.69909 (15) | 0.0095 (5) | |
| C3 | 0.0055 (3) | 0.3213 (4) | 0.65929 (15) | 0.0086 (4) | |
| C4 | −0.1449 (3) | 0.1811 (5) | 0.66802 (15) | 0.0111 (4) | |
| H1 | −0.1339 | 0.0367 | 0.7065 | 0.013* | |
| C5 | −0.3108 (3) | 0.2569 (9) | 0.61935 (14) | 0.0141 (4) | |
| H2 | −0.4140 | 0.1638 | 0.6253 | 0.017* | |
| C6 | −0.3286 (3) | 0.4686 (5) | 0.56162 (17) | 0.0141 (5) | |
| H3 | −0.4436 | 0.5159 | 0.5291 | 0.017* | |
| C7 | −0.1815 (3) | 0.6103 (5) | 0.55101 (17) | 0.0125 (4) | |
| H4 | −0.1932 | 0.7530 | 0.5116 | 0.015* | |
| C8 | −0.0151 (3) | 0.5338 (5) | 0.60080 (16) | 0.0103 (4) | |
| C9 | 0.2770 (3) | 0.0989 (5) | 0.76424 (16) | 0.0100 (4) | |
| H7 | 0.3862 | 0.0421 | 0.7428 | 0.012* | |
| H8 | 0.1939 | −0.0438 | 0.7591 | 0.012* | |
| C10 | 0.3269 (3) | 0.1746 (5) | 0.86847 (15) | 0.0109 (4) | |
| H9 | 0.3832 | 0.0280 | 0.9049 | 0.013* | |
| C11 | 0.4583 (3) | 0.3889 (5) | 0.88531 (16) | 0.0124 (5) | |
| N1 | 0.1513 (3) | 0.6363 (4) | 0.60405 (14) | 0.0120 (4) | |
| H5 | 0.1746 | 0.7698 | 0.5733 | 0.014* | |
| N2 | 0.1651 (2) | 0.2443 (6) | 0.90642 (12) | 0.0142 (3) | |
| H13 | 0.1107 | 0.3761 | 0.8735 | 0.021* | |
| H11 | 0.1972 | 0.2860 | 0.9683 | 0.021* | |
| H12 | 0.0885 | 0.1133 | 0.9006 | 0.021* | |
| O1 | 0.4357 (3) | 0.5748 (4) | 0.92793 (13) | 0.0166 (4) | |
| O2 | 0.5974 (2) | 0.3408 (4) | 0.84628 (15) | 0.0229 (4) | |
| H10 | 0.6731 | 0.4547 | 0.8596 | 0.034* | |
| Br1 | 0.90610 (3) | 0.74408 (5) | 0.873511 (13) | 0.01394 (7) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0119 (10) | 0.0122 (12) | 0.0092 (10) | −0.0014 (9) | 0.0012 (8) | −0.0008 (8) |
| C2 | 0.0108 (9) | 0.0105 (14) | 0.0072 (9) | 0.0005 (7) | 0.0017 (7) | −0.0011 (7) |
| C3 | 0.0107 (10) | 0.0096 (10) | 0.0051 (9) | 0.0013 (7) | 0.0001 (7) | −0.0008 (7) |
| C4 | 0.0132 (10) | 0.0116 (11) | 0.0080 (9) | 0.0002 (8) | 0.0005 (7) | 0.0008 (7) |
| C5 | 0.0117 (9) | 0.0175 (11) | 0.0133 (9) | −0.0010 (17) | 0.0028 (7) | −0.0037 (17) |
| C6 | 0.0122 (11) | 0.0190 (13) | 0.0104 (11) | 0.0051 (9) | 0.0002 (8) | 0.0005 (9) |
| C7 | 0.0176 (11) | 0.0114 (11) | 0.0084 (10) | 0.0043 (9) | 0.0024 (8) | 0.0010 (8) |
| C8 | 0.0150 (11) | 0.0099 (10) | 0.0063 (10) | −0.0006 (9) | 0.0027 (8) | −0.0012 (8) |
| C9 | 0.0107 (10) | 0.0092 (10) | 0.0089 (10) | −0.0004 (8) | −0.0010 (8) | −0.0020 (8) |
| C10 | 0.0142 (11) | 0.0095 (10) | 0.0081 (10) | −0.0010 (8) | −0.0002 (7) | −0.0002 (8) |
| C11 | 0.0128 (10) | 0.0127 (12) | 0.0091 (10) | −0.0035 (9) | −0.0048 (8) | 0.0010 (9) |
| N1 | 0.0172 (10) | 0.0092 (10) | 0.0095 (9) | −0.0020 (8) | 0.0023 (7) | 0.0019 (7) |
| N2 | 0.0194 (8) | 0.0124 (8) | 0.0120 (7) | −0.0064 (15) | 0.0062 (6) | −0.0017 (14) |
| O1 | 0.0216 (9) | 0.0114 (9) | 0.0158 (9) | −0.0046 (7) | 0.0009 (7) | −0.0030 (7) |
| O2 | 0.0124 (9) | 0.0217 (10) | 0.0354 (11) | −0.0078 (8) | 0.0061 (8) | −0.0112 (9) |
| Br1 | 0.01610 (10) | 0.01382 (11) | 0.01214 (9) | −0.00518 (15) | 0.00322 (6) | 0.00128 (14) |
Geometric parameters (Å, °)
| C1—C2 | 1.377 (3) | C8—N1 | 1.377 (3) |
| C1—N1 | 1.381 (3) | C9—C10 | 1.537 (3) |
| C1—H6 | 0.9500 | C9—H7 | 0.9900 |
| C2—C3 | 1.436 (3) | C9—H8 | 0.9900 |
| C2—C9 | 1.502 (3) | C10—N2 | 1.488 (3) |
| C3—C4 | 1.398 (3) | C10—C11 | 1.518 (3) |
| C3—C8 | 1.413 (3) | C10—H9 | 1.0000 |
| C4—C5 | 1.390 (3) | C11—O1 | 1.204 (3) |
| C4—H1 | 0.9500 | C11—O2 | 1.316 (3) |
| C5—C6 | 1.404 (5) | N1—H5 | 0.8800 |
| C5—H2 | 0.9500 | N2—H13 | 0.9100 |
| C6—C7 | 1.389 (4) | N2—H11 | 0.9100 |
| C6—H3 | 0.9500 | N2—H12 | 0.9100 |
| C7—C8 | 1.399 (3) | O2—H10 | 0.8400 |
| C7—H4 | 0.9500 | ||
| C2—C1—N1 | 109.8 (2) | C2—C9—H7 | 108.5 |
| C2—C1—H6 | 125.1 | C10—C9—H7 | 108.5 |
| N1—C1—H6 | 125.1 | C2—C9—H8 | 108.5 |
| C1—C2—C3 | 106.5 (2) | C10—C9—H8 | 108.5 |
| C1—C2—C9 | 127.5 (2) | H7—C9—H8 | 107.5 |
| C3—C2—C9 | 126.0 (2) | N2—C10—C11 | 108.5 (2) |
| C4—C3—C8 | 119.2 (2) | N2—C10—C9 | 110.80 (18) |
| C4—C3—C2 | 133.6 (2) | C11—C10—C9 | 113.26 (19) |
| C8—C3—C2 | 107.1 (2) | N2—C10—H9 | 108.0 |
| C5—C4—C3 | 118.8 (3) | C11—C10—H9 | 108.0 |
| C5—C4—H1 | 120.6 | C9—C10—H9 | 108.0 |
| C3—C4—H1 | 120.6 | O1—C11—O2 | 125.8 (2) |
| C4—C5—C6 | 121.1 (3) | O1—C11—C10 | 124.1 (2) |
| C4—C5—H2 | 119.4 | O2—C11—C10 | 110.0 (2) |
| C6—C5—H2 | 119.4 | C8—N1—C1 | 108.9 (2) |
| C7—C6—C5 | 121.4 (2) | C8—N1—H5 | 125.6 |
| C7—C6—H3 | 119.3 | C1—N1—H5 | 125.6 |
| C5—C6—H3 | 119.3 | C10—N2—H13 | 109.5 |
| C6—C7—C8 | 117.1 (2) | C10—N2—H11 | 109.5 |
| C6—C7—H4 | 121.4 | H13—N2—H11 | 109.5 |
| C8—C7—H4 | 121.4 | C10—N2—H12 | 109.5 |
| N1—C8—C7 | 129.9 (2) | H13—N2—H12 | 109.5 |
| N1—C8—C3 | 107.7 (2) | H11—N2—H12 | 109.5 |
| C7—C8—C3 | 122.4 (2) | C11—O2—H10 | 109.5 |
| C2—C9—C10 | 114.9 (2) | ||
| N1—C1—C2—C3 | 0.3 (3) | C2—C3—C8—N1 | 0.6 (2) |
| N1—C1—C2—C9 | 178.4 (2) | C4—C3—C8—C7 | 0.1 (3) |
| C1—C2—C3—C4 | 179.8 (2) | C2—C3—C8—C7 | −179.7 (2) |
| C9—C2—C3—C4 | 1.6 (4) | C1—C2—C9—C10 | 78.8 (3) |
| C1—C2—C3—C8 | −0.5 (2) | C3—C2—C9—C10 | −103.4 (3) |
| C9—C2—C3—C8 | −178.7 (2) | C2—C9—C10—N2 | 62.4 (3) |
| C8—C3—C4—C5 | −0.6 (3) | C2—C9—C10—C11 | −59.8 (3) |
| C2—C3—C4—C5 | 179.1 (3) | N2—C10—C11—O1 | 4.3 (3) |
| C3—C4—C5—C6 | 0.6 (4) | C9—C10—C11—O1 | 127.8 (3) |
| C4—C5—C6—C7 | −0.1 (4) | N2—C10—C11—O2 | −175.31 (19) |
| C5—C6—C7—C8 | −0.4 (4) | C9—C10—C11—O2 | −51.8 (3) |
| C6—C7—C8—N1 | −179.9 (2) | C7—C8—N1—C1 | 179.9 (2) |
| C6—C7—C8—C3 | 0.4 (3) | C3—C8—N1—C1 | −0.4 (3) |
| C4—C3—C8—N1 | −179.7 (2) | C2—C1—N1—C8 | 0.1 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C7—H4···Cg1i | 0.95 | 2.66 | 3.494 (3) | 146 |
| N1—H5···Cg2i | 0.88 | 2.72 | 3.406 (2) | 136 |
| N2—H11···Br1ii | 0.91 | 2.56 | 3.3208 (17) | 142 |
| N2—H12···Br1iii | 0.91 | 2.42 | 3.322 (3) | 173 |
| N2—H13···Br1iv | 0.91 | 2.52 | 3.320 (3) | 147 |
| C4—H1···Br1iii | 0.95 | 2.85 | 3.750 (2) | 159 |
| C10—H9···O1v | 1.00 | 2.49 | 3.404 (3) | 153 |
| C10—H9···O1ii | 1.00 | 2.56 | 3.199 (3) | 121 |
| O2—H10···Br1 | 0.84 | 2.34 | 3.173 (2) | 169 |
Symmetry codes: (i) −x, y−1/2, −z+1; (ii) −x+1, y−1/2, −z+2; (iii) x−1, y−1, z; (iv) x−1, y, z; (v) x, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: AT2781).
References
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- Oxford Diffraction (2008). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Abingdon, England.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809017322/at2781sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809017322/at2781Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


