Elizabeth M. Horstman, a Jeffery A. Bertke, b Toby J. Woods b * and Paul J. A. Kenis a

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1 research communications ISSN Crystal structure of a 2:1 piroxicam gentisic acid co-crystal featuring neutral and zwitterionic piroxicam molecules Elizabeth M. Horstman, a Jeffery A. Bertke, b Toby J. Woods b * and Paul J. A. Kenis a Received 21 October 2016 Accepted 27 October 2016 a University of Illinois, Department of Chemical and Biomolecular Engineering, 600 S. Mathews Ave, Urbana, IL 61801, USA, and b University of Illinois, School of Chemical Sciences, Box 59-1, 505 South Mathews Avenue, Urbana, Illinois 61801, USA. *Correspondence tobyw@illinois.edu Edited by W. T. A. Harrison, University of Aberdeen, Scotland Keywords: crystal structure; hydrogen bonding; piroxicam. CCDC reference: Supporting information: this article has supporting information at journals.iucr.org/e A new 2:1 co-crystal of piroxicam and gentisic acid [systematic name: 4-hydroxy- 1,1-dioxo-N-(pyridin-2-yl)-2H-1 6,2-benzothiazine-3-carboxamide 2-(4-oxido- 1,1-dioxo-2H-1 6,2-benzothiazine-3-amido)pyridin-1-ium 2,5-dihydroxybenzoic acid, 2C 15 H 13 N 3 O 4 SC 7 H 6 O 4 ] has been synthesized using a microfluidic platform and initially identified using Raman spectroscopy. In the co-crystal, one piroxicam molecule is in its neutral form and an intramolecular O HO hydrogen bond is observed. The other piroxicam molecule is zwitterionic (proton transfer from the OH group to the pyridine N atom) and two intramolecular N HO hydrogen bonds occur. The gentisic acid molecule shows whole-molecule disorder over two sets of sites in a (2):0.191 (2) ratio. In the crystal, extensive hydrogen bonding between the components forms layers propagating in the ab plane. 1. Chemical context Piroxicam is a non-steroidal anti-inflammatory drug classified as a BCS Class II drug due to its low aqueous solubility (Amidon et al., 1995; Thayer, 2010). Co-crystallization of an active pharmaceutical ingredient (API) and an FDAapproved counter-ion is a common technique employed to increase the solubility of the API (Trask et al., 2005). In this work, we explored the co-crystallization of piroxicam and gentisic acid. In a previous study, piroxicam was co-crystallized with 23 carboxylic acids yielding 50 co-crystals. From this work, three co-crystals of piroxicam and gentisic acid were identified with Raman spectroscopy, but no crystal structures were reported (Childs & Hardcastle, 2007). In our prior work, we reported the crystal structure of two co-crystals of piroxicam and gentisic acid, one was a 1:1 co-crystal and the second was a solvated co-crystal that incorporated acetone into the crystal in a 1:1:1 molar ratio (Horstman et al., 2015). In this work we describe the crystal structure of a 2:1 piroxicam:gentisic acid co-crystal. 2. Structural commentary The asymmetric unit of this co-crystal consists of two piroxicam molecules and one gentisic acid molecule, with all atoms residing on general positions (Fig. 1). One of the piroxicam molecules is neutral and the other is a zwitterion: the two molecules exhibit two different conformations in the crystal structure. In the neutral S2-containing molecule, intramolecular hydrogen bonding exists between the hydroxyl Acta Cryst. (2016). E72,

2 research communications proton H8 [HA = 1.79 (3) Å] and the amide oxygen atom O7. In the S2 molecule, free rotation about the C C bond (C1 and C10) allows a second zwitterionic conformation in which intramolecular hydrogen bonds exist between the amine proton H2 and the enolate oxygen atom O4 [HA = 1.85 (2) Å] and the pyridinium proton H3 and the amide oxygen atom O3 [HA = 2.19 (2) Å]. Further details of the hydrogen bonding are provided in Table 1. Table 1 Hydrogen-bond geometry (Å, ). D HA D H HA DA D HA N2 H2O (2) 1.85 (2) (18) (19) N3 H3O (2) 1.99 (2) (19) 135 (2) N3 H3O3 i 0.78 (2) 2.19 (2) (19) 136 (2) O8 H8O (3) 1.79 (3) (19) 148 (2) N5 H5O (2) 2.25 (2) (2) 167 (2) O10 H10N (3) 1.74 (3) (3) 167 (3) O11 H11O (3) 1.89 (3) (2) 148 (3) O12 H12O4 ii 0.81 (3) 1.94 (3) (3) 164 (4) O10B H10BO4 ii (12) 172 O11B H11BO2 i (6) 118 O11B H11BO9B (9) 143 O12B H12BN (12) 149 Symmetry codes: (i) x þ 1; y þ 1; z þ 1; (ii) x 1; y; z. intramolecular hydrogen bonding between the O11B hydroxide substituent and the O9B oxygen atom of the carboxylic acid (HA = 1.89 Å) but does not participate in intermolecular hydrogen bonding. The gentisic acid molecule shows whole molecule disorder over two orientations rotated by approximately 180 in the plane of the aromatic ring with site occupancies of (2):0.191 (2). The major orientation participates in intramolecular hydrogen bonding between the O11 hydroxide substituent of the benzene ring and the O9 oxygen atom of the carboxylic acid [HA = 1.89 (3) Å]. The major orientation also participates in intermolecular hydrogen bonding. The minor orientation of the gentisic acid molecule also displays 3. Supramolecular features In the crystal, hydrogen bonds (Table 1) between the piroxicam and gentisic acid molecules form hexameric units that propagate along the a-axis direction (Fig. 2). These units pack into layers in the ab plane; the layers stack along the c-axis direction, Fig. 3. The repeating motif of the hexameric unit is formed by one gentisic acid molecule hydrogen bonded to two piroxicam molecules, one of each conformation (i.e. neutral and zwitterion). The non-zwitterionic form of piroxicam accepts hydrogen bonds from the gentisic acid via O HN bonds between the carboxylic acid and the pyridine ring of piroxicam [HA = 1.74 (3) Å] as well as N HO bonds between the carbonyl oxygen atom of gentisic acid and the amine nitrogen atom of piroxicam [HA = 2.25 (2) Å]. The zwitterionic form of piroxicam accepts hydrogen bonds from the gentisic acid via O HO bonds between the 5-hydroxy substituent of gentisic acid and the enolate oxygen atom of piroxicam [HA = 1.94 (3) Å]. The repeat units are linked together by N HO bonds between the pyridinium nitrogen atoms and Figure 1 The molecular structure of the title co-crystal, showing 35% probability ellipsoids for non-h atoms and spheres of arbitrary size for H atoms. Only the major component of the disordered gentisic acid is shown. Figure 2 Ball-and-stick model highlighting the hydrogen-bonding network in the title co-crystal. Only the major component of the disordered gentisic acid is shown. Color key: C gray, N blue, H green, O red, and S yellow. H atoms not involved in hydrogen bonding have been omitted for clarity. Acta Cryst. (2016). E72, Horstman et al. 2C 15 H 13 N 3 O 4 SC 7 H 6 O

3 research communications Figure 3 Ball-and-stick packing diagram of the co-crystal, as viewed approximately down the b axis, highlighting the layers formed by the packing of the hexameric units. Color key: C gray, N blue, O red, and S yellow. H atoms have been omitted for clarity. the amide oxygen atoms of the zwitterionic form of piroxicam [HA = 2.19 (2) Å]. Piroxicam (>=98.0%) and gentisic acid (>=98.0%) were used as purchased from Sigma Aldrich (St. Louis, MO, USA). Acetonitrile (>=99.9%) was used as purchased from Fisher Scientific (Fair Lawn, NJ, USA). A 1:2 molar ratio of piroxicam:gentisic acid was dissolved in acetonitrile. The concentration of piroxicam in acetonitrile was near saturation (0.034 M). The resulting solution was introduced into a microfluidic platform. The microfluidic platform was a 6 6 array of single microwells (100 nl) (Horstman et al., 2015). After being filled, the microfluidic platform was placed inside a petri dish and then the petri dish was sealed with parafilm to slow the rate of solvent evaporation. The crystallization solution evaporated over the course of one day, after which crystals were observed via optical microscopy. Specifics of the microfluidic platform fabrication and operation have been previously reported (Horstman et al., 2015). Once crystals were observed, Raman spectroscopy was used to distinguish between crystals. Within one microfluidic chip, three different co-crystals of piroxicam and gentisic acid were observed, two of which had been previously reported (Horstman et al., 2015) and one new solid form, reported here. Once the new cocrystals had been identified, we removed the crystals from the microfluidic platform. 4. Synthesis and crystallization 5. Refinement Crystal data, data collection and structure refinement details are summarized in Table 2. The gentisic acid molecule shows whole molecule disorder over two sets of sites: the like C O and C C distances were restrained to be similar (s.u Å). Similar displacement amplitudes (s.u. 0.01) were imposed on disordered sites overlapping by less than the sum of van der Waals radii. All O H and N H hydrogen atoms were located in the difference map except for those on the minor-disordered component of the gentisic acid. The H atoms located in the difference map were allowed to refine the O H/N H bond distances. These H atoms refined to good hydrogen-bonding positions (Hamilton & Ibers, 1968). The hydroxyl H atoms on the minor-disordered component of gentisic acid were optimized by rotation about R O bonds with idealized O H and R H distances. These H atoms are also in good hydrogenbonding locations. Methyl H-atom positions, R CH 3, were optimized by rotation about R C bonds with idealized C H, RH and HH distances. The remaining H atoms were included as riding idealized contributors. Methyl, hydroxyl and amine H atom U iso values were assigned as 1.5U eq of the 1716 Horstman et al. 2C 15 H 13 N 3 O 4 SC 7 H 6 O 4 Acta Cryst. (2016). E72,

4 research communications Table 2 Experimental details. Crystal data Chemical formula 2C 15 H 13 N 3 O 4 SC 7 H 6 O 4 M r Crystal system, space group Triclinic, P1 Temperature (K) 105 a, b, c (Å) (3), (5), (6),, ( ) (15), (15), (15) V (Å 3 ) (11) Z 2 Radiation type Cu K (mm 1 ) 2.05 Crystal size (mm) Data collection Diffractometer Bruker D8 Venture/Photon 100 Absorption correction Integration (SADABS; Bruker, 2014) T min, T max 0.867, No. of measured, independent and 49307, 6416, 5801 observed [I > 2(I)] reflections R int (sin /) max (Å 1 ) Refinement R[F 2 >2(F 2 )], wr(f 2 ), S 0.033, 0.086, 1.11 No. of reflections 6416 No. of parameters 637 No. of restraints 374 H-atom treatment H atoms treated by a mixture of independent and constrained refinement max, min (e Å 3 ) 0.24, 0.40 Computer programs: APEX2, SAINT, XPREP, and XCIF (Bruker, 2014), SHELXS and SHELXTL (Sheldrick, 2008), SHELXL (Sheldrick, 2015) and CrystalMaker (CrystalMaker, 1994). carrier atom; remaining H-atom U iso were assigned as 1.2 carrier U eq. The (112) reflection was omitted from the final refinement because it was partially obscured by the shadow of the beamstop in some orientations. Acknowledgements The Materials Chemistry Laboratory at the University of Illinois was supported in part by grants NSF CHE and NSF CHE from the National Science Foundation. References Amidon, G. L., Lennernäs, H., Shah, V. P. & Crison, J. R. (1995). Pharm. Res. 12, Bruker (2014). APEX2, SAINT, XPREP, XCIF and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA. Childs, S. L. & Hardcastle, K. I. (2007). Cryst. Growth Des. 7, CrystalMaker (1994). CrystalMaker. CrystalMaker Software Ltd, Oxfordshire, England. Hamilton, W. C. & Ibers, J. A. (1968). In Hydrogen Bonding in Solids. New York: W. A. Benjamin Inc. Horstman, E. M., Bertke, J. A., Kim, E. H., Gonzalez, L. C., Zhang, G. G. Z., Gong, Y. & Kenis, P. J. A. (2015). CrystEngComm, 17, Sheldrick, G. M. (2008). Acta Cryst. A64, Sheldrick, G. M. (2015). Acta Cryst. C71, 3 8. Thayer, A. M. (2010). Chem. Eng. News, 88, Trask, A. V., Motherwell, W. D. S. & Jones, W. (2005). Cryst. Growth Des. 5, Acta Cryst. (2016). E72, Horstman et al. 2C 15 H 13 N 3 O 4 SC 7 H 6 O

5 supporting information [ Crystal structure of a 2:1 piroxicam gentisic acid co-crystal featuring neutral and zwitterionic piroxicam molecules Elizabeth M. Horstman, Jeffery A. Bertke, Toby J. Woods and Paul J. A. Kenis Computing details Data collection: APEX2 (Bruker, 2014); cell refinement: SAINT (Bruker, 2014); data reduction: SAINT (Bruker, 2014) and XPREP (Bruker, 2014); program(s) used to solve structure: SHELXS (Sheldrick, 2008); program(s) used to refine structure: SHELXL (Sheldrick, 2015); molecular graphics: SHELXTL (Sheldrick, 2008), CrystalMaker (CrystalMaker, 1994); software used to prepare material for publication: XCIF (Bruker, 2014). 4-Hydroxy-1,1-dioxo-N-(pyridin-2-yl)-2H-1λ 6,2-benzothiazine-3-carboxamide 2-(4-oxido-1,1-dioxo-2H-1λ 6,2- benzothiazine-3-amido)pyridin-1-ium 2,5-dihydroxybenzoic acid Crystal data 2C 15 H 13 N 3 O 4 S C 7 H 6 O 4 M r = Triclinic, P1 a = (3) Å b = (5) Å c = (6) Å α = (15) β = (15) γ = (15) V = (11) Å 3 Data collection Bruker D8 Venture/Photon 100 diffractometer Radiation source: microfocus sealed tube Multilayer mirrors monochromator profile data from φ and ω scans Absorption correction: integration (SADABS; Bruker, 2014) T min = 0.867, T max = Refinement Refinement on F 2 Least-squares matrix: full R[F 2 > 2σ(F 2 )] = wr(f 2 ) = S = reflections Z = 2 F(000) = 848 D x = Mg m 3 Cu Kα radiation, λ = Å Cell parameters from 9375 reflections θ = µ = 2.05 mm 1 T = 105 K Plate, colourless mm measured reflections 6416 independent reflections 5801 reflections with I > 2σ(I) R int = θ max = 68.3, θ min = 2.9 h = k = l = parameters 374 restraints Hydrogen site location: mixed H atoms treated by a mixture of independent and constrained refinement sup-1

6 w = 1/[σ 2 (F o2 ) + (0.0348P) P] where P = (F o 2 + 2F c2 )/3 (Δ/σ) max = Δρ max = 0.24 e Å 3 Δρ min = 0.40 e Å 3 Special details Experimental. One distinct cell was identified using APEX2 (Bruker, 2014). Thirty frame series were integrated and filtered for statistical outliers using SAINT (Bruker, 2013) then corrected for absorption by integration using SAINT/SADABS v2014/2 (Bruker, 2014) to sort, merge, and scale the combined data. No decay correction was applied. 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. Structure was phased by direct methods (Sheldrick, 2014). Systematic conditions suggested the ambiguous space group. The space group choice was confirmed by successful convergence of the full-matrix least-squares refinement on F 2. The final map had no significant features. A final analysis of variance between observed and calculated structure factors showed little dependence on amplitude and resolution. Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å 2 ) x y z U iso */U eq Occ. (<1) S (4) (3) (3) (10) O (14) (9) (8) (3) O (13) (9) (8) (3) O (13) (9) (8) (3) O (13) (9) (8) (3) N (16) (11) (9) (3) N (16) (11) (10) (3) H (3) (16) (14) 0.023* N (16) (12) (10) (3) H (3) (18) (14) 0.023* C (19) (13) (11) (3) C (19) (13) (11) (3) C (19) (13) (11) (3) C (19) (14) (11) (4) H4A * C (2) (14) (12) (4) H5A * C (2) (14) (12) (4) H6A * C (2) (14) (12) (4) H7A * C (19) (13) (11) (3) C (2) (14) (12) (4) H9A * H9B * H9C * C (19) (13) (11) (3) C (19) (13) (11) (3) C (2) (13) (11) (4) sup-2

7 H12A * C (2) (13) (11) (4) H13A * C (2) (13) (11) (3) H14A * C (19) (13) (11) (3) H15A * S (5) (3) (3) (11) O (14) (10) (9) (3) O (14) (10) (8) (3) O (14) (10) (8) (3) O (15) (11) (8) (3) H (3) (2) (15) 0.034* N (17) (11) (9) (3) N (18) (12) (10) (3) H (3) (18) (15) 0.030* N (17) (12) (11) (4) C (2) (14) (11) (4) C (2) (14) (11) (4) C (2) (14) (11) (4) C (2) (15) (12) (4) H19A * C (2) (15) (13) (4) H20A * C (2) (15) (12) (4) H21A * C (2) (14) (12) (4) H22A * C (2) (14) (11) (4) C (2) (15) (12) (4) H24A * H24B * H24C * C (2) (14) (11) (4) C (2) (14) (12) (4) C (2) (16) (16) (5) H27A * C (2) (16) (16) (5) H28A * C (2) (16) (14) (5) H29A * C (2) (16) (13) (4) H30A * O (18) (12) (11) (4) (2) O (3) (2) (3) (7) (2) H (4) (2) (19) 0.035* (2) O (19) (14) (11) (4) (2) H (4) (2) (2) 0.031* (2) sup-3

8 O (3) (2) (2) (6) (2) H (4) (3) (2) 0.035* (2) C (2) (16) (14) (5) (2) C (3) (19) (19) (6) (2) C (3) (19) (15) (5) (2) H33A * (2) C (3) (2) (17) (5) (2) H34A * (2) C (3) (17) (14) (5) (2) C (5) (2) (4) (7) (2) H36A * (2) C (3) (2) (14) (5) (2) O9B (7) (5) (4) (16) (2) O10B (14) (6) (10) (2) (2) H10B * (2) O11B (7) (5) (4) (15) (2) H11B * (2) O12B (13) (8) (12) (3) (2) H12B * (2) C31B (8) (5) (5) (14) (2) C32B (10) (6) (8) (2) (2) C33B (9) (8) (7) (18) (2) H33B * (2) C34B (10) (6) (6) (17) (2) H34B * (2) C35B (9) (6) (6) (17) (2) C36B (19) (9) (17) (3) (2) H36B * (2) C37B (10) (6) (7) (2) (2) Atomic displacement parameters (Å 2 ) U 11 U 22 U 33 U 12 U 13 U 23 S (19) (2) (2) (15) (15) (15) O (6) (6) (6) (5) (5) (5) O (6) (6) (6) (5) (5) (5) O (6) (6) (7) (5) (5) (5) O (6) (6) (6) (5) (5) (5) N (7) (7) (7) (5) (6) (6) N (7) (7) (7) (6) (6) (6) N (7) (7) (7) (6) (6) (6) C (8) (8) (8) (7) (6) (6) C (8) (9) (8) (7) (6) (6) C (8) (9) (8) (7) (6) (6) C (8) (9) (9) (7) (7) (7) C (9) (10) (9) (7) (7) (7) C (9) (9) (10) (7) (7) (7) C (9) (9) (9) (7) (7) (7) sup-4

9 C (8) (9) (8) (7) (6) (7) C (9) (9) (9) (7) (7) (7) C (8) (9) (8) (7) (6) (6) C (8) (8) (8) (6) (6) (6) C (8) (9) (9) (7) (7) (7) C (9) (9) (9) (7) (7) (7) C (8) (9) (8) (7) (7) (7) C (8) (9) (8) (7) (6) (7) S (2) (2) (2) (16) (16) (16) O (7) (7) (8) (5) (6) (6) O (7) (7) (7) (5) (5) (5) O (6) (7) (7) (5) (5) (6) O (6) (7) (7) (5) (5) (6) N (8) (8) (7) (6) (6) (6) N (7) (8) (8) (6) (6) (6) N (8) (8) (9) (6) (7) (7) C (9) (9) (8) (7) (7) (7) C (9) (10) (8) (7) (7) (7) C (9) (9) (8) (7) (7) (7) C (10) (10) (9) (8) (7) (7) C (11) (10) (10) (8) (8) (8) C (10) (10) (9) (8) (8) (7) C (9) (10) (9) (7) (7) (7) C (9) (9) (8) (7) (7) (7) C (10) (10) (9) (8) (7) (7) C (9) (10) (8) (7) (7) (7) C (8) (9) (9) (7) (7) (7) C (10) (10) (14) (8) (9) (9) C (10) (11) (14) (8) (9) (9) C (9) (12) (11) (8) (8) (9) C (9) (11) (10) (8) (8) (8) O (9) (8) (9) (6) (7) (6) O (11) (14) (16) (10) (10) (12) O (9) (9) (9) (7) (7) (7) O (14) (14) (11) (10) (11) (12) C (10) (11) (10) (8) (8) (8) C (14) (11) (12) (11) (12) (9) C (12) (13) (12) (10) (9) (9) C (12) (14) (11) (11) (9) (12) C (11) (11) (10) (9) (8) (9) C (14) (13) (2) (10) (10) (10) C (12) (13) (11) (11) (9) (9) O9B (3) (3) (4) (3) (3) (3) O10B (6) (5) (4) (4) (4) (4) O11B (3) (4) (4) (3) (3) (3) O12B (5) (6) (6) (4) (4) (5) C31B (3) (3) (3) (2) (2) (2) C32B (4) (3) (3) (3) (4) (3) sup-5

10 C33B (4) (4) (4) (4) (3) (4) C34B (4) (4) (3) (3) (3) (3) C35B (3) (4) (3) (3) (3) (3) C36B (4) (4) (4) (4) (3) (4) C37B (4) (4) (4) (4) (3) (4) Geometric parameters (Å, º) S1 O (12) C18 C (3) S1 O (12) C18 C (3) S1 N (14) C19 C (3) S1 C (17) C19 H19A O3 C (2) C20 C (3) O4 C (2) C20 H20A N1 C (2) C21 C (3) N1 C (2) C21 H21A N2 C (2) C22 C (3) N2 C (2) C22 H22A N2 H (2) C24 H24A N3 C (2) C24 H24B N3 C (2) C24 H24C N3 H (2) C26 C (3) C1 C (2) C27 C (3) C1 C (2) C27 H27A C2 C (2) C28 C (3) C3 C (2) C28 H28A C3 C (2) C29 C (3) C4 C (2) C29 H29A C4 H4A C30 H30A C5 C (3) O9 C (3) C5 H5A O10 C (4) C6 C (3) O10 H (3) C6 H6A O11 C (3) C7 C (2) O11 H (3) C7 H7A O12 C (4) C9 H9A O12 H (3) C9 H9B C31 C (4) C9 H9C C31 C (3) C11 C (2) C31 C (3) C12 C (3) C32 C (4) C12 H12A C33 C (4) C13 C (2) C33 H33A C13 H13A C34 C (3) C14 C (2) C34 H34A C14 H14A C35 C (5) C15 H15A C36 H36A S2 O (13) O9B C37B (8) S2 O (13) O10B C37B (9) sup-6

11 S2 N (15) O10B H10B S2 C (18) O11B C32B (8) O7 C (2) O11B H11B O8 C (2) O12B C35B (9) O8 H (3) O12B H12B N4 C (2) C31B C36B (9) N4 C (2) C31B C32B (8) N5 C (2) C31B C37B (8) N5 C (2) C32B C33B (9) N5 H (2) C33B C34B (9) N6 C (2) C33B H33B N6 C (3) C34B C35B (8) C16 C (3) C34B H34B C16 C (3) C35B C36B (10) C17 C (3) C36B H36B O2 S1 O (7) C20 C19 H19A O2 S1 N (7) C18 C19 H19A O1 S1 N (7) C19 C20 C (18) O2 S1 C (7) C19 C20 H20A O1 S1 C (8) C21 C20 H20A N1 S1 C (8) C22 C21 C (18) C1 N1 C (13) C22 C21 H21A C1 N1 S (11) C20 C21 H21A C9 N1 S (11) C23 C22 C (17) C11 N2 C (15) C23 C22 H22A C11 N2 H (14) C21 C22 H22A C10 N2 H (14) C22 C23 C (17) C11 N3 C (16) C22 C23 S (14) C11 N3 H (16) C18 C23 S (14) C12 N3 H (16) N4 C24 H24A C2 C1 C (15) N4 C24 H24B C2 C1 N (15) H24A C24 H24B C10 C1 N (14) N4 C24 H24C O4 C2 C (15) H24A C24 H24C O4 C2 C (14) H24B C24 H24C C1 C2 C (15) O7 C25 N (17) C4 C3 C (15) O7 C25 C (17) C4 C3 C (15) N5 C25 C (16) C8 C3 C (15) N6 C26 C (17) C5 C4 C (16) N6 C26 N (16) C5 C4 H4A C30 C26 N (17) C3 C4 H4A N6 C27 C (2) C6 C5 C (16) N6 C27 H27A C6 C5 H5A C28 C27 H27A C4 C5 H5A C27 C28 C (19) C5 C6 C (16) C27 C28 H28A C5 C6 H6A C29 C28 H28A sup-7

12 C7 C6 H6A C30 C29 C (19) C8 C7 C (16) C30 C29 H29A C8 C7 H7A C28 C29 H29A C6 C7 H7A C29 C30 C (19) C7 C8 C (15) C29 C30 H30A C7 C8 S (13) C26 C30 H30A C3 C8 S (13) C37 O10 H (19) N1 C9 H9A C32 O11 H (2) N1 C9 H9B C35 O12 H (3) H9A C9 H9B C36 C31 C (2) N1 C9 H9C C36 C31 C (2) H9A C9 H9C C32 C31 C (2) H9B C9 H9C O11 C32 C (2) O3 C10 N (15) O11 C32 C (2) O3 C10 C (15) C33 C32 C (2) N2 C10 C (14) C34 C33 C (2) N3 C11 N (15) C34 C33 H33A N3 C11 C (15) C32 C33 H33A N2 C11 C (15) C33 C34 C (2) N3 C12 C (16) C33 C34 H34A N3 C12 H12A C35 C34 H34A C13 C12 H12A O12 C35 C (2) C12 C13 C (16) O12 C35 C (2) C12 C13 H13A C36 C35 C (2) C14 C13 H13A C35 C36 C (2) C15 C14 C (16) C35 C36 H36A C15 C14 H14A C31 C36 H36A C13 C14 H14A O9 C37 O (2) C14 C15 C (15) O9 C37 C (2) C14 C15 H15A O10 C37 C (2) C11 C15 H15A C37B O10B H10B O6 S2 O (8) C32B O11B H11B O6 S2 N (8) C35B O12B H12B O5 S2 N (8) C36B C31B C32B (7) O6 S2 C (8) C36B C31B C37B (7) O5 S2 C (8) C32B C31B C37B (6) N4 S2 C (8) O11B C32B C33B (7) C17 O8 H (16) O11B C32B C31B (7) C16 N4 C (14) C33B C32B C31B (7) C16 N4 S (11) C34B C33B C32B (8) C24 N4 S (12) C34B C33B H33B C25 N5 C (16) C32B C33B H33B C25 N5 H (16) C33B C34B C35B (8) C26 N5 H (16) C33B C34B H34B C26 N6 C (17) C35B C34B H34B C17 C16 N (16) O12B C35B C36B (9) C17 C16 C (16) O12B C35B C34B (9) N4 C16 C (15) C36B C35B C34B (7) sup-8

13 O8 C17 C (17) C35B C36B C31B (9) O8 C17 C (16) C35B C36B H36B C16 C17 C (16) C31B C36B H36B C19 C18 C (17) O9B C37B O10B (8) C19 C18 C (16) O9B C37B C31B (7) C23 C18 C (16) O10B C37B C31B (8) C20 C19 C (18) O2 S1 N1 C (13) C16 C17 C18 C (3) O1 S1 N1 C (11) C23 C18 C19 C (3) C8 S1 N1 C (13) C17 C18 C19 C (16) O2 S1 N1 C (12) C18 C19 C20 C (3) O1 S1 N1 C (14) C19 C20 C21 C (3) C8 S1 N1 C (13) C20 C21 C22 C (3) C9 N1 C1 C (19) C21 C22 C23 C (3) S1 N1 C1 C (19) C21 C22 C23 S (13) C9 N1 C1 C (18) C19 C18 C23 C (3) S1 N1 C1 C (13) C17 C18 C23 C (16) C10 C1 C2 O4 1.0 (3) C19 C18 C23 S (13) N1 C1 C2 O (15) C17 C18 C23 S2 0.6 (2) C10 C1 C2 C (15) O6 S2 C23 C (15) N1 C1 C2 C3 5.3 (2) O5 S2 C23 C (17) O4 C2 C3 C (2) N4 S2 C23 C (14) C1 C2 C3 C (16) O6 S2 C23 C (15) O4 C2 C3 C (15) O5 S2 C23 C (13) C1 C2 C3 C (2) N4 S2 C23 C (15) C8 C3 C4 C5 0.6 (2) C26 N5 C25 O7 3.8 (3) C2 C3 C4 C (16) C26 N5 C25 C (16) C3 C4 C5 C6 0.4 (3) C17 C16 C25 O7 7.8 (3) C4 C5 C6 C7 0.1 (3) N4 C16 C25 O (15) C5 C6 C7 C8 0.0 (3) C17 C16 C25 N (16) C6 C7 C8 C3 0.2 (3) N4 C16 C25 N5 6.2 (2) C6 C7 C8 S (14) C27 N6 C26 C (3) C4 C3 C8 C7 0.5 (2) C27 N6 C26 N (17) C2 C3 C8 C (15) C25 N5 C26 N (16) C4 C3 C8 S (13) C25 N5 C26 C (3) C2 C3 C8 S1 1.1 (2) C26 N6 C27 C (3) O2 S1 C8 C (15) N6 C27 C28 C (3) O1 S1 C8 C (16) C27 C28 C29 C (3) N1 S1 C8 C (14) C28 C29 C30 C (3) O2 S1 C8 C (14) N6 C26 C30 C (3) O1 S1 C8 C (13) N5 C26 C30 C (17) N1 S1 C8 C (15) C36 C31 C32 O (3) C11 N2 C10 O3 4.3 (3) C37 C31 C32 O (4) C11 N2 C10 C (15) C36 C31 C32 C (4) C2 C1 C10 O (16) C37 C31 C32 C (2) N1 C1 C10 O3 6.1 (2) O11 C32 C33 C (2) C2 C1 C10 N2 4.4 (2) C31 C32 C33 C (4) sup-9

14 N1 C1 C10 N (14) C32 C33 C34 C (4) C12 N3 C11 N (16) C33 C34 C35 O (3) C12 N3 C11 C (2) C33 C34 C35 C (4) C10 N2 C11 N3 2.9 (3) O12 C35 C36 C (4) C10 N2 C11 C (15) C34 C35 C36 C (6) C11 N3 C12 C (3) C32 C31 C36 C (6) N3 C12 C13 C (3) C37 C31 C36 C (3) C12 C13 C14 C (3) C36 C31 C37 O (3) C13 C14 C15 C (3) C32 C31 C37 O9 7.3 (3) N3 C11 C15 C (2) C36 C31 C37 O (4) N2 C11 C15 C (15) C32 C31 C37 O (3) O6 S2 N4 C (13) C36B C31B C32B O11B (16) O5 S2 N4 C (12) C37B C31B C32B O11B 3.3 (16) C23 S2 N4 C (13) C36B C31B C32B C33B 2 (2) O6 S2 N4 C (12) C37B C31B C32B C33B (10) O5 S2 N4 C (15) O11B C32B C33B C34B (9) C23 S2 N4 C (14) C31B C32B C33B C34B 1.3 (17) C24 N4 C16 C (2) C32B C33B C34B C35B 0.1 (16) S2 N4 C16 C (2) C33B C34B C35B O12B (12) C24 N4 C16 C (18) C33B C34B C35B C36B 0 (2) S2 N4 C16 C (14) O12B C35B C36B C31B (17) N4 C16 C17 O (15) C34B C35B C36B C31B 1 (3) C25 C16 C17 O8 7.1 (3) C32B C31B C36B C35B 2 (3) N4 C16 C17 C (3) C37B C31B C36B C35B (16) C25 C16 C17 C (16) C36B C31B C37B O9B (16) O8 C17 C18 C (2) C32B C31B C37B O9B 1.5 (15) C16 C17 C18 C (17) C36B C31B C37B O10B 1 (2) O8 C17 C18 C (16) C32B C31B C37B O10B (11) Hydrogen-bond geometry (Å, º) D H A D H H A D A D H A N2 H2 O (2) 1.85 (2) (18) (19) N3 H3 O (2) 1.99 (2) (19) 135 (2) N3 H3 O3 i 0.78 (2) 2.19 (2) (19) 136 (2) O8 H8 O (3) 1.79 (3) (19) 148 (2) N5 H5 O (2) 2.25 (2) (2) 167 (2) O10 H10 N (3) 1.74 (3) (3) 167 (3) O11 H11 O (3) 1.89 (3) (2) 148 (3) O12 H12 O4 ii 0.81 (3) 1.94 (3) (3) 164 (4) O10B H10B O4 ii (12) 172 O11B H11B O2 i (6) 118 O11B H11B O9B (9) 143 O12B H12B N (12) 149 Symmetry codes: (i) x+1, y+1, z+1; (ii) x 1, y, z. sup-10

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