Crystal structures of the three closely related compounds: bis-[(1H-tetra-zol-5-yl)meth-yl]nitramide, tri-amino-guanidinium 5-({[(1H-tetra-zol-5-yl)meth-yl](nitro)-amino}-meth-yl)tetra-zol-1-ide, and di-ammonium bis-[(tetra-zol-1-id-5-yl)meth-yl]nitramide monohydrate.

In the mol-ecule of neutral bis-[(1H-tetra-zol-5-yl)meth-yl]nitramide, (I), C4H6N10O2, there are two intra-molecular N-H⋯O hydrogen bonds. In the crystal, N-H⋯N hydrogen bonds link mol-ecules, forming a two-dimensional network parallel to (-201) and weak C-H⋯O, C-H⋯N hydrogen bonds, and inter-molecular π-π stacking completes the three-dimensional network. The anion in the molecular salt, tri-amino-guanidinium 5-({[(1H-tetra-zol-5-yl)meth-yl](nitro)-amino}-meth-yl)tetra-zol-1-ide, (II), CH9N6+·C4H5N10O2-, displays intra-molecular π-π stacking and in the crystal, N-H⋯N and N-H⋯O hydrogen bonds link the components of the structure, forming a three-dimensional network. In the crystal of di-ammonium bis-[(tetra-zol-1-id-5-yl)meth-yl]nitramide monohydrate, (III), 2NH4+·C4H4N10O22-·H2O, O-H⋯N, N-H⋯N, and N-H⋯O hydrogen bonds link the components of the structure into a three-dimensional network. In addition, there is inter-molecular π-π stacking. In all three structures, the central N atom of the nitramide is mainly sp2-hybridized. Bond lengths indicate delocalization of charges on the tetra-zole rings for all three compounds. Compound (II) was found to be a non-merohedral twin and was solved and refined in the major component.

Chemical context

Materials which release large amount of energy during chemical transformations are characterized as energetic materials. Inter­est is high in improving energetics to reduce environmental impact and to improve safety and performance (Talawar et al., 2009 ▸). These materials can pose a hazard if they have high sensitivities to friction, heat, electrostatic discharge or impact. Compounds containing both <span class="Species">tetran>­zole and <span class="Chemical">nitro groups have frequently been used in the development of energetic materials (Klapötke et al., 2009 ▸; Wei et al., 2015 ▸). <span class="Species">Tetra­zoles have been of special inter­est because of their high nitro­gen content, which lead to high heats of formation and to more environmentally benign decomposition products like N2 (Jaidann et al., 2010 ▸). Nitro groups have been commonly utilized to achieve an optimum oxygen balance (Wu et al., 2014 ▸). Herein is a discussion of the X-ray crystal structures of three nitro-containing tetra­zole complexes. Structure (I), bis­[(1H-tetra­zol-5-yl)meth­yl]nitramide, is the neutral form, structure (II), tri­amino­guanidinium 5-({[(1H-tetra­zol-5-yl)meth­yl](nitro)­amino}­meth­yl)tetra­zol-1-ide, has one deprotonated tetra­zole ring with a tri­amino­guandidinium counter-ion, and structure (III), di­ammonium bis­[(tetra­zol-1-id-5-yl)meth­yl]nitramide monohydrate, has both tetra­zole rings deprotonated with ammonium counter-ions.

Structural commentary

In the mol­ecule of complex (I), two intra­molecular <span class="Chemical">hydrogenn> bonds, N4—H4⋯O15 and N10—H10⋯O16, both between <span class="Species">tetra­zole <span class="Species">donors and nitro acceptors are present (Fig. 1 ▸). This mol­ecule adopts a chair-like conformation where the tetra­zole rings are trans to one another. Mol­ecule (III) adopts a similar conformation, despite not having any similar intra­molecular hydrogen bonds (Fig. 2 ▸). Surprisingly, while structures (I) and (III) are both in a chair conformation, with respect to the tetra­zole rings, structure (II) is bent into a boat where the tetra­zole rings are cis to one another (Fig. 3 ▸).

Figure 1

The mol­ecular structure of structure (I), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. (a) Front view, dashed lines indicate intra­molecular hydrogen bonds. (b) Side view, H atoms omitted for clarity.

Figure 2

The mol­ecular structure of structure (III), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. (a) Front view. (b) Side view, H atoms, cations, and solvent omitted for clarity.

Figure 3

The mol­ecular structure of structure (II), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. (a) Front view. (b) Side view, H atoms and cation omitted for clarity.

This unusual conformation is likely due to the intra­molecular π–π stacking inter­actions observed between the <span class="Species">tetran>­zole rings [centroid–centroid distance = 3.4978 (10) Å]. Both <span class="Species">tetra­zole rings are nearly planar with an r.m.s. deviation of 0.0007 for the protonated ring and 0.00004 Å for the deprotonated ring.

For all three compounds, the C—N (ranging from 1.321 to 1.338 Å) and N—N (ranging from 1.301 to 1.362 Å) bond lengths for the <span class="Species">tetran>­zole rings were found to match more closely with bonds of multiple character than of discrete single and double bonds, signifying a delocalized aromatic system (Allen et al., 1987 ▸).

In structure (II), the N18—C17, N20—C17, and N22—C17 bond lengths for the tri­amino­guandidinium cation were all found to be relatively equal (maximum difference 0.006 Å), indicating delocalization of the charge over all three branches.

The pyramidality of the <span class="Chemical">aminen> functionality for the central tertiary <span class="Chemical">amine was ex<span class="Chemical">amined for all three structures by examining χ, the angle between the Namine—Nnitro vector and the Cmethyl­ene1/Namine/Cmethyl­ene2 plane, described by Allen et al. (1995 ▸). Structure (I) has a χ of 13.1 (5)° for vector N2–N1 and plane C11/C5/N1, structure (II) has a χ of 26.11 (18)° for vector N14–N7 and plane C6/N7/C8, and structure (III) has a χ of 6.21 (11)° for vector N7A–N7 and plane C6/N7/C8. This indicated the hybridization of the central nitro­gen atom is mainly sp hybridized for all three structures (sp χ ≃ 0°, sp χ ≃ 60°).

Supra­molecular features

The packing and inter­molecular <span class="Chemical">hydrogenn> bonding vary greatly between the three structures. Structure (I) has four inter­molecular <span class="Chemical">hydrogen bonds (Table 1 ▸). The <span class="Species">tetra­zole rings of adjacent mol­ecules are linked via N—H⋯N bonds, forming a two-dimensional network parallel to (01). These inter­actions cause the tetra­zole rings to lie in the same plane, resulting in the alignment of the tetra­zole rings seen when viewed along the b axis (Fig. 4 ▸). Additionally, there is one weak C—H⋯N and one weak C—H⋯O hydrogen bond linking the mol­ecules into a three-dimensional network.

Table 1

Hydrogen-bond geometry (Å, °) for (I)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N4—H4⋯N2i	0.80 (6)	2.19 (6)	2.957 (5)	160 (4)
N4—H4⋯O15	0.80 (6)	2.45 (5)	2.924 (5)	119 (4)
C6—H6B⋯O15ii	0.99	2.37	3.264 (5)	150
C8—H8B⋯N11iii	0.99	2.44	3.316 (5)	147
N10—H10⋯N13iv	0.87 (1)	1.99 (3)	2.770 (5)	149 (4)
N10—H10⋯O16	0.87 (1)	2.28 (4)	2.796 (4)	118 (4)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) .

Figure 4

Packing diagram for structure (I) viewed along the b axis. Dashed lines indicate inter­molecular hydrogen bonds.

Structure (II) does not have any non-classical inter­molecular <span class="Chemical">hydrogenn> bonds (Table 2 ▸). There are twelve N—H⋯N bonds and three N—H⋯O bonds, with the majority of the inter­actions between the main residue and the tri­amino-guandidinium counter-ion. The additional <span class="Chemical">hydrogen bonds link the mol­ecules into a three-dimensional network. The compound packs into columns of alternating anions and cations along the c axis (Fig. 5 ▸).

Table 2

Hydrogen-bond geometry (Å, °) for (II)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N1—H1⋯N10i	0.929 (19)	1.804 (19)	2.713 (2)	165.6 (17)
N1—H1⋯N11i	0.929 (19)	2.673 (19)	3.422 (2)	138.2 (14)
N1—H1⋯O16i	0.929 (19)	2.596 (18)	2.9952 (18)	106.5 (13)
N18—H18⋯O15	0.84 (2)	2.569 (19)	3.1451 (18)	126.4 (16)
N18—H18⋯N21	0.84 (2)	2.292 (19)	2.650 (2)	105.9 (15)
N19—H19A⋯N4	0.92 (2)	2.29 (2)	3.026 (2)	137.3 (17)
N19—H19B⋯N13ii	0.91 (2)	2.54 (2)	3.275 (2)	138.5 (16)
N20—H20⋯N13iii	0.86 (2)	2.09 (2)	2.867 (2)	149.0 (17)
N20—H20⋯N23	0.86 (2)	2.358 (18)	2.660 (2)	100.9 (14)
N21—H21A⋯N11ii	0.89 (2)	2.46 (2)	3.143 (2)	134.4 (16)
N21—H21B⋯O15iv	0.89 (2)	2.31 (2)	3.090 (2)	146.3 (18)
N22—H22⋯N2v	0.86 (2)	2.40 (2)	3.118 (2)	142.3 (17)
N22—H22⋯N19	0.86 (2)	2.325 (19)	2.650 (2)	102.9 (15)
N23—H23A⋯N11vi	0.89 (2)	2.22 (2)	3.087 (2)	166.5 (18)
N23—H23B⋯N3vi	0.92 (2)	2.38 (2)	3.091 (2)	133.9 (17)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) .

Figure 5

Packing diagram for structure (II) viewed along the a axis. Dashed lined indicate inter­molecular hydrogen bonds.

Structure (III) contains several inter­molecular <span class="Chemical">hydrogenn> bonds, which also form a three-dimensional network (Table 3 ▸). There are seven N—H⋯N bonds between <span class="Chemical">ammonium <span class="Species">donors and tetra­zole acceptors, two O—H⋯N bonds between water donors and tetra­zole acceptors, two N—H⋯O bonds between ammonium donors and water acceptors, and one N—H⋯O bond between an ammonium donor and a nitro acceptor. The ions and mol­ecules pack into columns along the b axis (Fig. 6 ▸).

Table 3

Hydrogen-bond geometry (Å, °) for (III)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
O1S—H1SA⋯N13i	0.88 (2)	2.06 (2)	2.9253 (12)	168.0 (18)
O1S—H1SB⋯N3ii	0.83 (2)	2.31 (2)	2.9498 (13)	134.8 (17)
N1A—H1A⋯N12iii	0.859 (16)	2.211 (16)	3.0533 (13)	166.7 (14)
N1A—H1B⋯O16	0.847 (16)	2.388 (16)	3.0079 (13)	130.5 (13)
N1A—H1B⋯N13iv	0.847 (16)	2.540 (15)	3.2862 (14)	147.6 (13)
N1A—H1B⋯N12iv	0.847 (16)	2.585 (15)	3.2472 (14)	136.0 (13)
N2A—H2A⋯O1S	0.880 (16)	2.030 (16)	2.9062 (14)	173.2 (14)
N2A—H2B⋯N1v	0.854 (16)	2.179 (16)	3.0243 (13)	170.3 (14)
N1A—H1C⋯N2v	0.882 (16)	2.107 (16)	2.9654 (12)	164.2 (14)
N2A—H2C⋯O1S vi	0.849 (17)	2.147 (17)	2.9766 (13)	165.2 (14)
N2A—H2D⋯N1	0.896 (16)	2.117 (16)	3.0096 (13)	174.0 (13)
N1A—H1D⋯N10vii	0.906 (16)	2.045 (16)	2.9273 (13)	164.2 (13)

Symmetry codes: (i) ; (ii) ; (iii) ; (iv) ; (v) ; (vi) ; (vii) .

Figure 6

Packing diagram for structure (III) viewed along the b axis. Dashed lined indicate inter­molecular hydrogen bonds.

Although compounds (I) and (III) do not exhibit any intra­molecular π–π stacking, inter­molecular π–π stacking is present between <span class="Species">tetran>­zole rings of adjacent mol­ecules. Compound (I) displays head-to-tail stacking inter­actions with a centroid–centroid distance of 3.627 (2) Å. Compound (II) displays head-to-head and tail-to-tail stacking with a centroid–centroid distance of 3.8472 (10) Å for plane N1/N2/N3/N4/C5 to N1/N2/N3/N4/C5 and 4.0025 (8) Å for plane C9/N10/N11/N12/N13 to C9/N10/N11/N12/N13. There is no inter­molecular π–π stacking for compound (II), which contains the larger counter-ion, tri­amino­guandidinium.

The neutral complex, compound (I), has a density of 1.825 g cm−3 (173 K). This is similar to the density, determined by X-ray crystallography, of the well known energetics RDX (α-hexa­hydro-1,3,5-tri­<span class="Chemical">nitron>-1,3,5-triazine) and HMX (1,3,5,7-<span class="Species">tetra- <span class="Chemical">nitro-1,3,5,7-tetra­aza­cyclo­octa­ne) at 1.794 g cm−3 (298 K) and 1.948 g cm−3 (120 K) respectively (Zhurov et al., 2011 ▸). The ionic compounds have much lower densities. The density of compound (II) is 1.611 g cm−3 (293 K), and the density of compound (III) is 1.579 g cm−3 (296 K).

Database survey

A search of the Cambridge Structural Database (version 5.36, last updated May 2015; Groom et al., 2016 ▸) found 392 complexes that contained both <span class="Species">tetran>­zole and <span class="Chemical">nitro groups. The most similar compounds were 5-<span class="Chemical">nitro-2H-tetra­zole (Klapötke et al., 2009 ▸), ammonium 5-nitro­tetra­zolate (Klapötke et al., 2008 ▸), and tri­amino­guanidinium 5-nitro­tetra­zolate (Klapötke et al., 2008 ▸). A search for tri­amino­guandidinium containing compounds found 47 hits. The compounds from the CSD had similar bond lengths and angles to the tri­amino­guandidinium cation in complex (II). The average difference in C—N bond lengths for the tri­amino­guandidinium complexes in the CSD was found to be 0.015 Å, indicating a high level of charge delocalization, similar to that seen in complex (II).

Synthesis and crystallization

Compound (I)

A 100 ml round-bottom flask was charged with N,N-bis(cyano­meth­yl)<span class="Chemical">nitramiden> (2.5 g, 18 mmol), <span class="Chemical">zinc bromide (3.9 g, 17 mmol), 30 ml <span class="Chemical">water, and a magnetic stirbar. The reaction was heated to 323 K with stirring. Sodium azide (2.5 g, 38 mmol) was dissolved in 30 ml water and added to the heated reaction. A reflux condenser was fitted to the flask and the reaction was heated to 363 K for 1 h causing a gradual color change to light brown and the formation of a precipitate. The reaction was allowed to cool to room temperature, then 37% HCl (5 ml) was added and the mixture was allowed to stir for 30 min. The product was collected by vacuum filtration using a Buchner funnel and recrystallized from hot water. Yield 95%, 4 g. Melting point 475–477 K (dec.). CHN: Expected: C, 21.24; H, 2.67; N, 61.93. Found: C, 21.82(0.08); H, 2.96(0.08); N, 62.20(0.30). 1H NMR (DMSO-d 6): 4.15 (2, s), 5.49 (4, s) ppm. 13C NMR (DMSO-d 6): 40.33, 152.74 ppm. IR: 637, 685, 765, 875, 933, 1042, 1088, 1111, 1246, 1284, 1408, 1481, 1524, 1557, 2864, 3022 cm−1.

Compound (II)

A 50 ml round-bottom flask was charged with a stir bar, barium hydroxide octa­hydrate (3.2 g, 10 mmol) and 20 mmol <span class="Chemical">watern>. The base was stirred until fully dissolved. Compound (I) (4.5 g, 20 mmol) was added to the basic solution, dissolved, and the mixture was stirred 30 min as the color darkened to brown. The brown mixture was filtered to remove insoluble material, the filtrate was returned to the 50 ml round-bottom flask and stirred. Tri­amino­guanidinium sulfate (3.06 g, 10 mmol) was added to the stirring solution, causing immediate precipitation of <span class="Chemical">barium sulfate. The mixture was stirred for 30 min and then allowed to stand for 10 min. <span class="Chemical">Barium sulfate was removed by Buchner filtration and the filtrate was rotovapped until a precipitate formed. After isolating the product by filtration, it was recrystallized from water/ethanol solution. Yield 34%, 1.35 g. Melting point 428–430 K (dec.). 1H NMR (DMSO-d 6): 4.65 (8, s), 5.20 (4, s), 8.6 (1, s) ppm. 13C NMR (DMSO-d 6): 46.95, 157.60, 159.64 ppm. IR: 637, 685, 765, 875, 933, 1042, 1088, 1111, 1246, 1284, 1408, 1481, 1524, 1557, 2864, 3022 cm−1.

Compound (III)

A 50 ml round-bottom flask was charged with (I) (2.5 g, 11 mmol), 10 ml <span class="Chemical">watern>, and a magnetic stir bar and then stirred. An <span class="Chemical">ammonium hydroxide solution (30%, 3 ml) was added to the reaction. After stirring for 1 h at 298 K, 10 ml <span class="Chemical">ethanol was added and the resulting precipitate was collected by Buchner filtration. The product was recrystallized from water/methanol solution. Yield 80%, 2.3 g. Melting point 389–393 K (dec.). 1H NMR (DMSO-d 6): 5.13 (4, s), 3.70 (broad) ppm. 13C NMR (DMSO-d 6): 40.05; 155.80 ppm. IR: 2908; 2149; 1869; 1844; 1717; 1700; 1684; 1676; 1653; 1636; 1617; 1540; 1521; 1456; 1419; 1364; 1270; 1209; 1159; 1140; 1113; 1076; 920; 877; 809; 706; 612 cm−1.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 4 ▸. The methyl­ene <span class="Disease">H atomsn> were positioned geometrically and refined using a riding model, with C—H = 0.99 Å and U iso(H) = 1.2U eq(C). All other <span class="Disease">H atoms were located in a difference Fourier map using. Compound (II) was found to be a non-merohedral twin and was solved and refined in the major component. The N10—H10 bond length in structure (I) was restrained.

Table 4

Experimental details

	(I)	(II)	(III)
Crystal data
Chemical formula	C4H6N10O2	CH9N6 +·C4H5N10O2 −	2NH4 +·C4H4N10O2 2−·H2O
M r	226.19	330.32	278.27
Crystal system, space group	Monoclinic, P21	Monoclinic, P21/c	Triclinic, P
Temperature (K)	173	100	296
a, b, c (Å)	6.3640 (17), 9.627 (3), 6.8627 (18)	6.5312 (11), 12.682 (2), 16.183 (3)	7.5893 (11), 7.6077 (11), 11.2319 (15)
α, β, γ (°)	90, 101.805 (4), 90	90, 97.118 (3), 90	85.564 (4), 85.555 (4), 65.007 (4)
V (Å3)	411.57 (19)	1330.0 (4)	585.29 (14)
Z	2	4	2
Radiation type	Mo Kα	Mo Kα	Mo Kα
μ (mm−1)	0.15	0.13	0.13
Crystal size (mm)	0.36 × 0.32 × 0.01	0.52 × 0.06 × 0.02	0.75 × 0.63 × 0.24
Data collection
Diffractometer	Bruker SMART APEXII CCD	Bruker SMART APEXII CCD	Bruker SMART APEXII CCD
Absorption correction	Multi-scan (TWINABS; Bruker, 2008 ▸)	Multi-scan (SADABS; Bruker, 2008 ▸)	Multi-scan (SADABS; Bruker, 2008 ▸)
T min, T max	0.615, 0.745	0.674, 0.745	0.687, 0.746
No. of measured, independent and observed [I > 2σ(I)] reflections	889, 889, 835	11821, 2733, 2141	38379, 3178, 3000
R int	0.038	0.037	0.057
(sin θ/λ)max (Å−1)	0.625	0.628	0.688
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S	0.036, 0.102, 1.14	0.037, 0.093, 1.00	0.036, 0.106, 1.12
No. of reflections	889	2733	3178
No. of parameters	151	238	202
No. of restraints	2	0	0
H-atom treatment	H atoms treated by a mixture of independent and constrained refinement	H atoms treated by a mixture of independent and constrained refinement	H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3)	0.25, −0.32	0.23, −0.25	0.29, −0.27

Computer programs: APEX2, SAINT and XPREP (Bruker, 2008 ▸), SHELXTL (Sheldrick, 2008 ▸), SHELXL2014 (Sheldrick, 2015 ▸) within WinGX (Farrugia, 2012 ▸) and publCIF (Westrip, 2010 ▸).

Crystal structure: contains datablock(s) I, II, III. DOI: 10.1107/S2056989017008817/lh5843sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017008817/lh5843Isup2.hkl

Structure factors: contains datablock(s) II. DOI: 10.1107/S2056989017008817/lh5843IIsup3.hkl

Structure factors: contains datablock(s) III. DOI: 10.1107/S2056989017008817/lh5843IIIsup4.hkl

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989017008817/lh5843Isup5.cml

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989017008817/lh5843IIsup6.cml

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989017008817/lh5843IIIsup7.cml

CCDC references: 1555912, 1555911, 1555910

Additional supporting information: crystallographic information; 3D view; checkCIF report

C4H6N10O2	F(000) = 232
Mr = 226.19	Dx = 1.825 Mg m−3
Monoclinic, P21	Mo Kα radiation, λ = 0.71073 Å
a = 6.3640 (17) Å	Cell parameters from 2717 reflections
b = 9.627 (3) Å	θ = 3.0–26.2°
c = 6.8627 (18) Å	µ = 0.15 mm−1
β = 101.805 (4)°	T = 173 K
V = 411.57 (19) Å3	Thin plate, colorless
Z = 2	0.36 × 0.32 × 0.01 mm

Bruker SMART APEXII CCD diffractometer	889 independent reflections
Radiation source: fine focus sealed tube	835 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.038
ω scans	θmax = 26.4°, θmin = 3.0°
Absorption correction: multi-scan (TWINABS; Bruker, 2008)	h = −7→7
Tmin = 0.615, Tmax = 0.745	k = 0→12
889 measured reflections	l = 0→8

Refinement on F2	2 restraints
Least-squares matrix: full	Hydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.036	H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.102	w = 1/[σ2(Fo2) + (0.0513P)2 + 0.4169P] where P = (Fo2 + 2Fc2)/3
S = 1.14	(Δ/σ)max < 0.001
889 reflections	Δρmax = 0.25 e Å−3
151 parameters	Δρmin = −0.32 e Å−3

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.

	x	y	z	Uiso*/Ueq
N1	0.0174 (5)	0.3550 (3)	0.2473 (5)	0.0132 (7)
N2	−0.0013 (5)	0.3439 (4)	0.0467 (5)	0.0133 (7)
N3	0.0000 (5)	0.4659 (4)	−0.0356 (5)	0.0124 (7)
N4	0.0208 (5)	0.5581 (4)	0.1139 (5)	0.0117 (7)
H4	0.028 (7)	0.640 (7)	0.099 (6)	0.014*
C5	0.0317 (6)	0.4901 (4)	0.2851 (5)	0.0108 (7)
C6	0.0466 (6)	0.5533 (4)	0.4880 (5)	0.0125 (7)
H6A	−0.0542	0.6326	0.4769	0.015*
H6B	0.0009	0.4834	0.5768	0.015*
N7	0.2620 (5)	0.6017 (3)	0.5783 (5)	0.0122 (7)
C8	0.4251 (6)	0.5139 (4)	0.6986 (5)	0.0129 (8)
H8A	0.5573	0.5178	0.6438	0.015*
H8B	0.3738	0.4165	0.6889	0.015*
C9	0.4788 (5)	0.5559 (5)	0.9148 (5)	0.0113 (7)
N10	0.5184 (5)	0.6848 (3)	0.9857 (5)	0.0118 (7)
H10	0.510 (7)	0.764 (3)	0.924 (6)	0.014*
N11	0.5665 (5)	0.6792 (3)	1.1860 (5)	0.0128 (7)
N12	0.5574 (5)	0.5489 (4)	1.2341 (4)	0.0127 (7)
N13	0.5023 (5)	0.4701 (4)	1.0666 (4)	0.0110 (7)
N14	0.3273 (5)	0.7226 (3)	0.5122 (4)	0.0112 (7)
O15	0.2034 (4)	0.7844 (3)	0.3794 (4)	0.0142 (6)
O16	0.5086 (4)	0.7636 (3)	0.5919 (4)	0.0154 (6)

	U11	U22	U33	U12	U13	U23
N1	0.0148 (14)	0.0102 (17)	0.0139 (15)	−0.0015 (13)	0.0011 (12)	−0.0015 (13)
N2	0.0141 (15)	0.0093 (18)	0.0164 (17)	0.0004 (13)	0.0029 (12)	0.0010 (13)
N3	0.0141 (14)	0.0082 (17)	0.0144 (16)	−0.0017 (13)	0.0017 (12)	−0.0040 (13)
N4	0.0139 (15)	0.0074 (16)	0.0135 (15)	−0.0021 (13)	0.0021 (11)	−0.0019 (14)
C5	0.0104 (16)	0.0071 (18)	0.0139 (17)	−0.0023 (14)	0.0003 (13)	0.0004 (15)
C6	0.0139 (18)	0.0113 (18)	0.0122 (16)	−0.0044 (16)	0.0020 (13)	0.0004 (16)
N7	0.0152 (16)	0.0061 (15)	0.0142 (15)	−0.0045 (13)	0.0003 (12)	−0.0008 (13)
C8	0.022 (2)	0.0062 (18)	0.0093 (16)	0.0041 (14)	0.0013 (14)	0.0004 (13)
C9	0.0091 (16)	0.0115 (18)	0.0130 (17)	0.0008 (15)	0.0015 (13)	−0.0036 (16)
N10	0.0171 (16)	0.0060 (17)	0.0131 (15)	0.0011 (13)	0.0049 (12)	0.0014 (13)
N11	0.0155 (16)	0.0101 (17)	0.0122 (14)	0.0020 (13)	0.0013 (11)	0.0001 (13)
N12	0.0136 (15)	0.0112 (15)	0.0131 (15)	−0.0003 (14)	0.0019 (11)	0.0003 (15)
N13	0.0131 (15)	0.0079 (18)	0.0112 (15)	−0.0010 (13)	0.0007 (11)	−0.0005 (13)
N14	0.0147 (15)	0.0078 (15)	0.0115 (14)	−0.0016 (12)	0.0037 (12)	−0.0003 (12)
O15	0.0182 (13)	0.0099 (13)	0.0136 (12)	0.0031 (12)	0.0012 (10)	0.0029 (11)
O16	0.0165 (13)	0.0148 (14)	0.0144 (12)	−0.0052 (10)	0.0021 (10)	−0.0007 (11)

N1—C5	1.326 (5)	C8—C9	1.508 (5)
N1—N2	1.361 (4)	C8—H8A	0.9900
N2—N3	1.304 (5)	C8—H8B	0.9900
N3—N4	1.343 (5)	C9—N13	1.314 (5)
N4—C5	1.334 (5)	C9—N10	1.338 (5)
N4—H4	0.80 (6)	N10—N11	1.347 (4)
C5—C6	1.505 (5)	N10—H10	0.867 (11)
C6—N7	1.460 (5)	N11—N12	1.301 (5)
C6—H6A	0.9900	N12—N13	1.362 (5)
C6—H6B	0.9900	N14—O15	1.230 (4)
N7—N14	1.346 (4)	N14—O16	1.236 (4)
N7—C8	1.457 (5)
C5—N1—N2	105.2 (3)	N7—C8—C9	113.2 (3)
N3—N2—N1	111.1 (3)	N7—C8—H8A	108.9
N2—N3—N4	105.8 (3)	C9—C8—H8A	108.9
C5—N4—N3	109.1 (4)	N7—C8—H8B	108.9
C5—N4—H4	127 (3)	C9—C8—H8B	108.9
N3—N4—H4	124 (3)	H8A—C8—H8B	107.8
N1—C5—N4	108.7 (4)	N13—C9—N10	108.2 (3)
N1—C5—C6	124.5 (3)	N13—C9—C8	125.3 (4)
N4—C5—C6	126.7 (3)	N10—C9—C8	126.5 (4)
N7—C6—C5	113.4 (3)	C9—N10—N11	108.7 (3)
N7—C6—H6A	108.9	C9—N10—H10	130 (3)
C5—C6—H6A	108.9	N11—N10—H10	121 (3)
N7—C6—H6B	108.9	N12—N11—N10	106.6 (3)
C5—C6—H6B	108.9	N11—N12—N13	109.9 (3)
H6A—C6—H6B	107.7	C9—N13—N12	106.7 (3)
N14—N7—C8	117.4 (3)	O15—N14—O16	124.9 (3)
N14—N7—C6	117.4 (3)	O15—N14—N7	118.2 (3)
C8—N7—C6	123.6 (3)	O16—N14—N7	116.9 (3)
C5—N1—N2—N3	−0.4 (4)	N7—C8—C9—N13	135.9 (4)
N1—N2—N3—N4	0.3 (4)	N7—C8—C9—N10	−46.8 (5)
N2—N3—N4—C5	0.0 (4)	N13—C9—N10—N11	−0.4 (4)
N2—N1—C5—N4	0.3 (4)	C8—C9—N10—N11	−178.1 (3)
N2—N1—C5—C6	177.6 (3)	C9—N10—N11—N12	0.5 (4)
N3—N4—C5—N1	−0.2 (4)	N10—N11—N12—N13	−0.4 (4)
N3—N4—C5—C6	−177.4 (3)	N10—C9—N13—N12	0.1 (4)
N1—C5—C6—N7	104.7 (4)	C8—C9—N13—N12	177.8 (3)
N4—C5—C6—N7	−78.6 (5)	N11—N12—N13—C9	0.2 (4)
C5—C6—N7—N14	77.3 (4)	C8—N7—N14—O15	165.5 (3)
C5—C6—N7—C8	−87.9 (4)	C6—N7—N14—O15	−0.6 (5)
N14—N7—C8—C9	82.6 (4)	C8—N7—N14—O16	−15.0 (4)
C6—N7—C8—C9	−112.2 (4)	C6—N7—N14—O16	178.9 (3)

D—H···A	D—H	H···A	D···A	D—H···A
N4—H4···N2i	0.80 (6)	2.19 (6)	2.957 (5)	160 (4)
N4—H4···O15	0.80 (6)	2.45 (5)	2.924 (5)	119 (4)
C6—H6B···O15ii	0.99	2.37	3.264 (5)	150
C8—H8B···N11iii	0.99	2.44	3.316 (5)	147
N10—H10···N13iv	0.87 (1)	1.99 (3)	2.770 (5)	149 (4)
N10—H10···O16	0.87 (1)	2.28 (4)	2.796 (4)	118 (4)

CH9N6+·C4H5N10O2−	F(000) = 688
Mr = 330.32	Dx = 1.650 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
a = 6.5312 (11) Å	Cell parameters from 2664 reflections
b = 12.682 (2) Å	θ = 3.0–25.8°
c = 16.183 (3) Å	µ = 0.13 mm−1
β = 97.118 (3)°	T = 100 K
V = 1330.0 (4) Å3	Thin plate, colorless
Z = 4	0.52 × 0.06 × 0.02 mm

Bruker SMART APEXII CCD diffractometer	2733 independent reflections
Radiation source: fine focus sealed tube	2141 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.037
ω scans	θmax = 26.5°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2008)	h = −8→8
Tmin = 0.674, Tmax = 0.745	k = −15→15
11821 measured reflections	l = −20→17

Refinement on F2	0 restraints
Least-squares matrix: full	Hydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.037	H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.093	w = 1/[σ2(Fo2) + (0.044P)2 + 0.6423P] where P = (Fo2 + 2Fc2)/3
S = 1.00	(Δ/σ)max < 0.001
2733 reflections	Δρmax = 0.23 e Å−3
238 parameters	Δρmin = −0.25 e Å−3

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.

	x	y	z	Uiso*/Ueq
N1	0.8295 (2)	0.71404 (10)	0.35827 (9)	0.0141 (3)
H1	0.937 (3)	0.7311 (14)	0.3283 (12)	0.017*
N2	0.8025 (2)	0.61115 (11)	0.37468 (9)	0.0181 (3)
N3	0.6329 (2)	0.60429 (11)	0.40878 (9)	0.0178 (3)
N4	0.5480 (2)	0.70155 (10)	0.41515 (9)	0.0162 (3)
C5	0.6732 (2)	0.76797 (12)	0.38346 (10)	0.0128 (3)
C6	0.6426 (2)	0.88578 (12)	0.37832 (11)	0.0142 (3)
H6A	0.697088	0.918049	0.432299	0.017*
H6B	0.721587	0.914793	0.335095	0.017*
N7	0.42480 (19)	0.91361 (10)	0.35817 (9)	0.0132 (3)
C8	0.3282 (2)	0.90418 (12)	0.27155 (10)	0.0151 (3)
H8A	0.416201	0.939648	0.234379	0.018*
H8B	0.192815	0.940317	0.265472	0.018*
C9	0.2981 (2)	0.79121 (12)	0.24561 (10)	0.0128 (3)
N10	0.1481 (2)	0.72878 (10)	0.26607 (9)	0.0152 (3)
N11	0.1891 (2)	0.63274 (11)	0.23517 (9)	0.0164 (3)
N12	0.3573 (2)	0.63861 (11)	0.19785 (9)	0.0176 (3)
N13	0.4297 (2)	0.73864 (11)	0.20361 (9)	0.0165 (3)
N14	0.3000 (2)	0.89963 (10)	0.41915 (9)	0.0140 (3)
O15	0.38074 (18)	0.89379 (9)	0.49195 (7)	0.0185 (3)
O16	0.11190 (17)	0.89812 (9)	0.39797 (8)	0.0189 (3)
C17	−0.0806 (2)	0.68873 (12)	0.58804 (10)	0.0133 (3)
N18	0.0711 (2)	0.72677 (11)	0.54903 (9)	0.0170 (3)
H18	0.086 (3)	0.7929 (16)	0.5481 (12)	0.020*
N19	0.2228 (2)	0.65585 (12)	0.52819 (11)	0.0209 (3)
H19A	0.255 (3)	0.6740 (16)	0.4767 (14)	0.027*
H19B	0.337 (3)	0.6698 (16)	0.5647 (14)	0.027*
N20	−0.2213 (2)	0.75296 (10)	0.61240 (9)	0.0145 (3)
H20	−0.311 (3)	0.7310 (14)	0.6435 (12)	0.017*
N21	−0.1977 (2)	0.86203 (11)	0.59874 (10)	0.0181 (3)
H21A	−0.139 (3)	0.8920 (16)	0.6454 (14)	0.024*
H21B	−0.324 (3)	0.8875 (15)	0.5871 (13)	0.024*
N22	−0.0899 (2)	0.58573 (11)	0.60267 (9)	0.0160 (3)
H22	−0.002 (3)	0.5432 (15)	0.5856 (12)	0.019*
N23	−0.2648 (2)	0.54700 (12)	0.63607 (11)	0.0212 (3)
H23A	−0.221 (3)	0.4982 (17)	0.6733 (14)	0.028*
H23B	−0.346 (3)	0.5116 (16)	0.5941 (14)	0.028*

	U11	U22	U33	U12	U13	U23
N1	0.0119 (6)	0.0132 (7)	0.0177 (8)	−0.0008 (5)	0.0036 (6)	−0.0010 (6)
N2	0.0145 (7)	0.0147 (7)	0.0253 (9)	−0.0003 (5)	0.0024 (6)	−0.0011 (6)
N3	0.0144 (7)	0.0140 (7)	0.0249 (8)	0.0012 (5)	0.0026 (6)	0.0029 (6)
N4	0.0144 (7)	0.0144 (7)	0.0202 (8)	0.0007 (5)	0.0036 (6)	−0.0001 (6)
C5	0.0110 (7)	0.0148 (8)	0.0122 (8)	−0.0010 (6)	0.0002 (6)	−0.0010 (6)
C6	0.0097 (7)	0.0134 (8)	0.0195 (9)	−0.0002 (6)	0.0017 (6)	−0.0005 (7)
N7	0.0112 (6)	0.0136 (7)	0.0151 (7)	0.0000 (5)	0.0031 (5)	0.0009 (5)
C8	0.0158 (8)	0.0152 (8)	0.0140 (9)	−0.0002 (6)	0.0012 (6)	0.0019 (6)
C9	0.0130 (7)	0.0153 (8)	0.0095 (8)	0.0007 (6)	−0.0015 (6)	0.0007 (6)
N10	0.0145 (7)	0.0145 (7)	0.0163 (8)	−0.0004 (5)	0.0010 (6)	−0.0007 (6)
N11	0.0171 (7)	0.0158 (7)	0.0161 (8)	−0.0004 (5)	0.0015 (6)	−0.0013 (6)
N12	0.0167 (7)	0.0168 (7)	0.0196 (8)	−0.0012 (5)	0.0038 (6)	−0.0020 (6)
N13	0.0168 (7)	0.0169 (7)	0.0159 (8)	−0.0007 (6)	0.0029 (6)	−0.0002 (6)
N14	0.0144 (7)	0.0103 (6)	0.0180 (8)	−0.0004 (5)	0.0042 (6)	−0.0007 (5)
O15	0.0210 (6)	0.0207 (6)	0.0135 (6)	0.0011 (5)	0.0013 (5)	−0.0004 (5)
O16	0.0098 (6)	0.0205 (6)	0.0267 (7)	−0.0007 (4)	0.0032 (5)	−0.0027 (5)
C17	0.0137 (8)	0.0148 (8)	0.0104 (8)	−0.0011 (6)	−0.0021 (6)	0.0000 (6)
N18	0.0167 (7)	0.0125 (7)	0.0233 (8)	0.0000 (5)	0.0082 (6)	0.0006 (6)
N19	0.0184 (8)	0.0223 (8)	0.0240 (9)	0.0020 (6)	0.0104 (7)	−0.0017 (7)
N20	0.0141 (7)	0.0115 (7)	0.0186 (8)	0.0001 (5)	0.0049 (6)	0.0020 (6)
N21	0.0183 (7)	0.0113 (7)	0.0237 (9)	0.0015 (6)	−0.0016 (6)	0.0005 (6)
N22	0.0142 (7)	0.0127 (7)	0.0226 (8)	0.0013 (5)	0.0081 (6)	0.0014 (6)
N23	0.0197 (8)	0.0147 (7)	0.0312 (10)	−0.0033 (6)	0.0112 (7)	0.0024 (7)

N1—C5	1.334 (2)	N12—N13	1.3530 (19)
N1—N2	1.3475 (19)	N14—O15	1.2319 (18)
N1—H1	0.929 (19)	N14—O16	1.2337 (17)
N2—N3	1.300 (2)	C17—N20	1.324 (2)
N3—N4	1.3614 (19)	C17—N18	1.330 (2)
N4—C5	1.321 (2)	C17—N22	1.330 (2)
C5—C6	1.508 (2)	N18—N19	1.410 (2)
C6—N7	1.463 (2)	N18—H18	0.84 (2)
C6—H6A	0.9900	N19—H19A	0.92 (2)
C6—H6B	0.9900	N19—H19B	0.91 (2)
N7—N14	1.3673 (19)	N20—N21	1.4123 (19)
N7—C8	1.469 (2)	N20—H20	0.86 (2)
C8—C9	1.499 (2)	N21—H21A	0.89 (2)
C8—H8A	0.9900	N21—H21B	0.89 (2)
C8—H8B	0.9900	N22—N23	1.4112 (19)
C9—N10	1.333 (2)	N22—H22	0.86 (2)
C9—N13	1.338 (2)	N23—H23A	0.89 (2)
N10—N11	1.3558 (19)	N23—H23B	0.92 (2)
N11—N12	1.3196 (19)
C5—N1—N2	108.22 (13)	N12—N11—N10	109.37 (13)
C5—N1—H1	134.4 (11)	N11—N12—N13	108.97 (13)
N2—N1—H1	117.0 (11)	C9—N13—N12	105.14 (13)
N3—N2—N1	106.71 (13)	O15—N14—O16	123.94 (14)
N2—N3—N4	110.36 (13)	O15—N14—N7	118.36 (13)
C5—N4—N3	105.71 (13)	O16—N14—N7	117.62 (14)
N4—C5—N1	109.01 (14)	N20—C17—N18	120.25 (15)
N4—C5—C6	124.68 (14)	N20—C17—N22	120.16 (15)
N1—C5—C6	126.31 (14)	N18—C17—N22	119.59 (15)
N7—C6—C5	111.70 (12)	C17—N18—N19	117.99 (14)
N7—C6—H6A	109.3	C17—N18—H18	117.6 (13)
C5—C6—H6A	109.3	N19—N18—H18	122.9 (13)
N7—C6—H6B	109.3	N18—N19—H19A	107.8 (13)
C5—C6—H6B	109.3	N18—N19—H19B	105.4 (13)
H6A—C6—H6B	107.9	H19A—N19—H19B	106.1 (18)
N14—N7—C6	117.27 (13)	C17—N20—N21	117.55 (14)
N14—N7—C8	117.01 (13)	C17—N20—H20	121.3 (12)
C6—N7—C8	118.94 (13)	N21—N20—H20	120.1 (12)
N7—C8—C9	111.78 (13)	N20—N21—H21A	109.3 (13)
N7—C8—H8A	109.3	N20—N21—H21B	105.9 (13)
C9—C8—H8A	109.3	H21A—N21—H21B	108.4 (19)
N7—C8—H8B	109.3	C17—N22—N23	117.82 (14)
C9—C8—H8B	109.3	C17—N22—H22	120.9 (13)
H8A—C8—H8B	107.9	N23—N22—H22	120.6 (13)
N10—C9—N13	111.61 (14)	N22—N23—H23A	107.1 (13)
N10—C9—C8	124.97 (14)	N22—N23—H23B	107.8 (13)
N13—C9—C8	123.25 (14)	H23A—N23—H23B	105.5 (19)
C9—N10—N11	104.91 (13)
C5—N1—N2—N3	0.17 (18)	C8—C9—N10—N11	−175.43 (14)
N1—N2—N3—N4	−0.10 (18)	C9—N10—N11—N12	−0.01 (17)
N2—N3—N4—C5	−0.01 (18)	N10—N11—N12—N13	0.01 (18)
N3—N4—C5—N1	0.11 (18)	N10—C9—N13—N12	0.00 (18)
N3—N4—C5—C6	−179.14 (15)	C8—C9—N13—N12	175.53 (14)
N2—N1—C5—N4	−0.18 (19)	N11—N12—N13—C9	0.00 (17)
N2—N1—C5—C6	179.06 (15)	C6—N7—N14—O15	20.04 (19)
N4—C5—C6—N7	−38.1 (2)	C8—N7—N14—O15	170.96 (13)
N1—C5—C6—N7	142.82 (16)	C6—N7—N14—O16	−162.96 (13)
C5—C6—N7—N14	72.31 (18)	C8—N7—N14—O16	−12.05 (19)
C5—C6—N7—C8	−78.03 (17)	N20—C17—N18—N19	176.83 (15)
N14—N7—C8—C9	−78.88 (16)	N22—C17—N18—N19	−3.0 (2)
C6—N7—C8—C9	71.53 (17)	N18—C17—N20—N21	−2.8 (2)
N7—C8—C9—N10	77.91 (19)	N22—C17—N20—N21	177.00 (15)
N7—C8—C9—N13	−97.02 (18)	N20—C17—N22—N23	6.8 (2)
N13—C9—N10—N11	0.01 (18)	N18—C17—N22—N23	−173.34 (15)

D—H···A	D—H	H···A	D···A	D—H···A
N1—H1···N10i	0.929 (19)	1.804 (19)	2.713 (2)	165.6 (17)
N1—H1···N11i	0.929 (19)	2.673 (19)	3.422 (2)	138.2 (14)
N1—H1···O16i	0.929 (19)	2.596 (18)	2.9952 (18)	106.5 (13)
N18—H18···O15	0.84 (2)	2.569 (19)	3.1451 (18)	126.4 (16)
N18—H18···N21	0.84 (2)	2.292 (19)	2.650 (2)	105.9 (15)
N19—H19A···N4	0.92 (2)	2.29 (2)	3.026 (2)	137.3 (17)
N19—H19B···N13ii	0.91 (2)	2.54 (2)	3.275 (2)	138.5 (16)
N20—H20···N13iii	0.86 (2)	2.09 (2)	2.867 (2)	149.0 (17)
N20—H20···N23	0.86 (2)	2.358 (18)	2.660 (2)	100.9 (14)
N21—H21A···N11ii	0.89 (2)	2.46 (2)	3.143 (2)	134.4 (16)
N21—H21B···O15iv	0.89 (2)	2.31 (2)	3.090 (2)	146.3 (18)
N22—H22···N2v	0.86 (2)	2.40 (2)	3.118 (2)	142.3 (17)
N22—H22···N19	0.86 (2)	2.325 (19)	2.650 (2)	102.9 (15)
N23—H23A···N11vi	0.89 (2)	2.22 (2)	3.087 (2)	166.5 (18)
N23—H23B···N3vi	0.92 (2)	2.38 (2)	3.091 (2)	133.9 (17)

2NH4+·C4H4N10O22−·H2O	Z = 2
Mr = 278.27	F(000) = 292
Triclinic, P1	Dx = 1.579 Mg m−3
a = 7.5893 (11) Å	Mo Kα radiation, λ = 0.71073 Å
b = 7.6077 (11) Å	Cell parameters from 9690 reflections
c = 11.2319 (15) Å	θ = 3.0–29.3°
α = 85.564 (4)°	µ = 0.13 mm−1
β = 85.555 (4)°	T = 296 K
γ = 65.007 (4)°	Irregular, colorless
V = 585.29 (14) Å3	0.75 × 0.63 × 0.24 mm

Bruker SMART APEXII CCD diffractometer	3178 independent reflections
Radiation source: fine-focus sealed tube	3000 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.057
ω and φ scans	θmax = 29.3°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 2008)	h = −10→10
Tmin = 0.687, Tmax = 0.746	k = −10→10
38379 measured reflections	l = −15→15

Refinement on F2	0 restraints
Least-squares matrix: full	Hydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.036	H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.106	w = 1/[σ2(Fo2) + (0.0606P)2 + 0.0988P] where P = (Fo2 + 2Fc2)/3
S = 1.12	(Δ/σ)max < 0.001
3178 reflections	Δρmax = 0.29 e Å−3
202 parameters	Δρmin = −0.27 e Å−3

Experimental. Output from intergration and final cell refinement: A B C Alpha Beta Gamma Vol 7.59208 7.60543 11.22509 85.5941 85.5165 64.9686 584.79 0.00008 0.00008 0.00012 0.0004 0.0004 0.0004 0.01 Corrected for goodness of fit: 0.00040 0.00041 0.00058 0.0020 0.0022 0.0019 0.07

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.

	x	y	z	Uiso*/Ueq
N1	0.63637 (12)	0.17356 (11)	−0.03243 (7)	0.02642 (17)
N2	0.74077 (12)	0.11482 (12)	−0.13592 (7)	0.02770 (18)
N3	0.86114 (14)	−0.06786 (13)	−0.12320 (8)	0.0330 (2)
N4	0.84018 (14)	−0.13474 (12)	−0.01067 (8)	0.03243 (19)
C5	0.70207 (12)	0.01714 (12)	0.04216 (7)	0.02088 (17)
C6	0.62734 (14)	0.01115 (14)	0.16882 (8)	0.02520 (18)
H6A	0.4887	0.0929	0.1739	0.030*
H6B	0.6459	−0.1207	0.1923	0.030*
N7	0.72326 (12)	0.07574 (11)	0.25251 (7)	0.02516 (17)
C8	0.88186 (13)	−0.06259 (14)	0.32289 (8)	0.02571 (18)
H8A	0.9528	0.0041	0.3523	0.031*
H8B	0.9712	−0.1626	0.2717	0.031*
C9	0.81243 (12)	−0.15606 (13)	0.42648 (8)	0.02285 (17)
N10	0.76291 (15)	−0.08633 (13)	0.53514 (7)	0.0334 (2)
N11	0.70900 (16)	−0.21454 (14)	0.59893 (8)	0.0382 (2)
N12	0.72763 (14)	−0.35383 (13)	0.53058 (8)	0.0343 (2)
N13	0.79270 (14)	−0.32036 (13)	0.41982 (8)	0.03096 (19)
N14	0.65021 (12)	0.26410 (12)	0.27363 (7)	0.02663 (17)
O15	0.52737 (13)	0.37956 (11)	0.20606 (7)	0.03769 (19)
O16	0.71072 (13)	0.31354 (12)	0.35853 (7)	0.03772 (19)
O1S	0.02418 (14)	0.53216 (13)	−0.20467 (7)	0.0398 (2)
H1SA	0.086 (3)	0.482 (3)	−0.2719 (18)	0.060*
H1SB	−0.028 (3)	0.650 (3)	−0.2242 (18)	0.060*
N1A	0.36192 (14)	0.69706 (13)	0.37735 (8)	0.02941 (18)
H1A	0.317 (2)	0.615 (2)	0.4054 (13)	0.035*
H1B	0.484 (2)	0.643 (2)	0.3830 (13)	0.035*
H1C	0.336 (2)	0.730 (2)	0.3016 (14)	0.035*
H1D	0.318 (2)	0.807 (2)	0.4177 (13)	0.035*
N2A	0.24096 (13)	0.50259 (13)	0.00386 (9)	0.03122 (19)
H2A	0.184 (2)	0.504 (2)	−0.0618 (14)	0.037*
H2B	0.267 (2)	0.601 (2)	0.0049 (14)	0.037*
H2C	0.181 (2)	0.493 (2)	0.0693 (15)	0.037*
H2D	0.356 (2)	0.399 (2)	−0.0029 (13)	0.037*

	U11	U22	U33	U12	U13	U23
N1	0.0331 (4)	0.0229 (4)	0.0194 (3)	−0.0083 (3)	−0.0005 (3)	0.0001 (3)
N2	0.0362 (4)	0.0283 (4)	0.0188 (3)	−0.0141 (3)	0.0003 (3)	−0.0004 (3)
N3	0.0396 (4)	0.0297 (4)	0.0238 (4)	−0.0096 (3)	0.0059 (3)	−0.0034 (3)
N4	0.0401 (4)	0.0235 (4)	0.0250 (4)	−0.0057 (3)	0.0027 (3)	−0.0005 (3)
C5	0.0251 (4)	0.0211 (4)	0.0183 (4)	−0.0112 (3)	−0.0024 (3)	−0.0011 (3)
C6	0.0331 (4)	0.0290 (4)	0.0186 (4)	−0.0181 (4)	0.0001 (3)	−0.0009 (3)
N7	0.0336 (4)	0.0236 (4)	0.0188 (3)	−0.0122 (3)	−0.0026 (3)	−0.0015 (3)
C8	0.0245 (4)	0.0294 (4)	0.0217 (4)	−0.0103 (3)	0.0015 (3)	−0.0005 (3)
C9	0.0242 (4)	0.0232 (4)	0.0196 (4)	−0.0082 (3)	−0.0023 (3)	−0.0009 (3)
N10	0.0513 (5)	0.0298 (4)	0.0210 (4)	−0.0194 (4)	0.0034 (3)	−0.0031 (3)
N11	0.0540 (6)	0.0349 (5)	0.0256 (4)	−0.0203 (4)	0.0061 (4)	0.0008 (3)
N12	0.0430 (5)	0.0329 (4)	0.0302 (4)	−0.0197 (4)	−0.0012 (3)	0.0038 (3)
N13	0.0420 (5)	0.0293 (4)	0.0251 (4)	−0.0181 (3)	−0.0024 (3)	−0.0016 (3)
N14	0.0365 (4)	0.0257 (4)	0.0188 (3)	−0.0147 (3)	0.0027 (3)	−0.0019 (3)
O15	0.0502 (5)	0.0281 (4)	0.0272 (4)	−0.0092 (3)	−0.0055 (3)	0.0028 (3)
O16	0.0533 (5)	0.0357 (4)	0.0295 (4)	−0.0222 (4)	−0.0043 (3)	−0.0086 (3)
O1S	0.0512 (5)	0.0321 (4)	0.0275 (4)	−0.0099 (3)	0.0021 (3)	0.0005 (3)
N1A	0.0372 (4)	0.0266 (4)	0.0222 (4)	−0.0108 (3)	−0.0040 (3)	−0.0008 (3)
N2A	0.0307 (4)	0.0263 (4)	0.0381 (5)	−0.0132 (3)	−0.0010 (4)	−0.0022 (3)

N1—C5	1.3325 (11)	N10—N11	1.3475 (13)
N1—N2	1.3480 (11)	N11—N12	1.3095 (14)
N2—N3	1.3051 (12)	N12—N13	1.3485 (12)
N3—N4	1.3488 (12)	N14—O16	1.2373 (11)
N4—C5	1.3312 (12)	N14—O15	1.2375 (11)
C5—C6	1.4948 (12)	O1S—H1SA	0.88 (2)
C6—N7	1.4611 (12)	O1S—H1SB	0.83 (2)
C6—H6A	0.9700	N1A—H1A	0.859 (16)
C6—H6B	0.9700	N1A—H1B	0.847 (16)
N7—N14	1.3334 (11)	N1A—H1C	0.882 (16)
N7—C8	1.4593 (12)	N1A—H1D	0.906 (16)
C8—C9	1.4935 (12)	N2A—H2A	0.880 (16)
C8—H8A	0.9700	N2A—H2B	0.854 (16)
C8—H8B	0.9700	N2A—H2C	0.849 (17)
C9—N13	1.3284 (12)	N2A—H2D	0.896 (16)
C9—N10	1.3315 (12)
C5—N1—N2	104.67 (7)	N13—C9—C8	123.16 (8)
N3—N2—N1	109.51 (7)	N10—C9—C8	124.72 (8)
N2—N3—N4	109.43 (8)	C9—N10—N11	104.58 (8)
C5—N4—N3	104.71 (8)	N12—N11—N10	109.26 (8)
N4—C5—N1	111.67 (8)	N11—N12—N13	109.62 (8)
N4—C5—C6	124.00 (8)	C9—N13—N12	104.41 (8)
N1—C5—C6	124.32 (8)	O16—N14—O15	123.83 (8)
N7—C6—C5	113.19 (7)	O16—N14—N7	118.24 (8)
N7—C6—H6A	108.9	O15—N14—N7	117.93 (8)
C5—C6—H6A	108.9	H1SA—O1S—H1SB	102.1 (18)
N7—C6—H6B	108.9	H1A—N1A—H1B	107.3 (14)
C5—C6—H6B	108.9	H1A—N1A—H1C	111.5 (14)
H6A—C6—H6B	107.8	H1B—N1A—H1C	108.9 (14)
N14—N7—C8	119.43 (8)	H1A—N1A—H1D	114.4 (14)
N14—N7—C6	118.69 (8)	H1B—N1A—H1D	106.7 (14)
C8—N7—C6	121.50 (8)	H1C—N1A—H1D	107.9 (13)
N7—C8—C9	112.80 (7)	H2A—N2A—H2B	111.5 (14)
N7—C8—H8A	109.0	H2A—N2A—H2C	116.2 (14)
C9—C8—H8A	109.0	H2B—N2A—H2C	108.9 (15)
N7—C8—H8B	109.0	H2A—N2A—H2D	103.5 (13)
C9—C8—H8B	109.0	H2B—N2A—H2D	106.1 (14)
H8A—C8—H8B	107.8	H2C—N2A—H2D	110.1 (14)
N13—C9—N10	112.13 (8)
C5—N1—N2—N3	0.47 (10)	N7—C8—C9—N13	90.37 (11)
N1—N2—N3—N4	−0.27 (12)	N7—C8—C9—N10	−89.46 (11)
N2—N3—N4—C5	−0.06 (12)	N13—C9—N10—N11	−0.21 (12)
N3—N4—C5—N1	0.37 (11)	C8—C9—N10—N11	179.64 (9)
N3—N4—C5—C6	179.15 (8)	C9—N10—N11—N12	0.43 (12)
N2—N1—C5—N4	−0.52 (11)	N10—N11—N12—N13	−0.50 (13)
N2—N1—C5—C6	−179.30 (8)	N10—C9—N13—N12	−0.08 (11)
N4—C5—C6—N7	95.25 (11)	C8—C9—N13—N12	−179.93 (8)
N1—C5—C6—N7	−86.12 (11)	N11—N12—N13—C9	0.35 (11)
C5—C6—N7—N14	88.66 (10)	C8—N7—N14—O16	−5.08 (12)
C5—C6—N7—C8	−98.39 (9)	C6—N7—N14—O16	168.02 (8)
N14—N7—C8—C9	96.03 (10)	C8—N7—N14—O15	174.04 (8)
C6—N7—C8—C9	−76.87 (10)	C6—N7—N14—O15	−12.86 (12)

D—H···A	D—H	H···A	D···A	D—H···A
O1S—H1SA···N13i	0.88 (2)	2.06 (2)	2.9253 (12)	168.0 (18)
O1S—H1SB···N3ii	0.83 (2)	2.31 (2)	2.9498 (13)	134.8 (17)
N1A—H1A···N12iii	0.859 (16)	2.211 (16)	3.0533 (13)	166.7 (14)
N1A—H1B···O16	0.847 (16)	2.388 (16)	3.0079 (13)	130.5 (13)
N1A—H1B···N13iv	0.847 (16)	2.540 (15)	3.2862 (14)	147.6 (13)
N1A—H1B···N12iv	0.847 (16)	2.585 (15)	3.2472 (14)	136.0 (13)
N2A—H2A···O1S	0.880 (16)	2.030 (16)	2.9062 (14)	173.2 (14)
N2A—H2B···N1v	0.854 (16)	2.179 (16)	3.0243 (13)	170.3 (14)
N1A—H1C···N2v	0.882 (16)	2.107 (16)	2.9654 (12)	164.2 (14)
N2A—H2C···O1Svi	0.849 (17)	2.147 (17)	2.9766 (13)	165.2 (14)
N2A—H2D···N1	0.896 (16)	2.117 (16)	3.0096 (13)	174.0 (13)
N1A—H1D···N10vii	0.906 (16)	2.045 (16)	2.9273 (13)	164.2 (13)