organic compounds
of the 2-(1,2,3,4-tetrahydronaphthalen-1-ylidene)hydrazinecarbothioamide–pyrazine-2,3,5,6-tetracarbonitrile (2/1)
aInstitut für Anorganische Chemie, Universität Bonn, Gerhard-Domagk-Strasse 1, D-53121 Bonn, Germany, and bDepartamento de Química, Universidade Federal de Sergipe, Av. Marechal Rondon s/n, Campus, 49100-000 São Cristóvão-SE, Brazil
*Correspondence e-mail: unc40018@uni-bonn.de
The reaction of 2-(1,2,3,4-tetrahydronapthalen-1-ylidene)hydrazinecarbothioamide (TTSC) with pyrazine-2,3,5,6-tetracarbonitrile (tetracyanopyrazine, TCNP) yields the title 2:1 charge-transfer adduct, 2C11H12N3S·C6N8. The complete TCNP molecule is generated by a crystallographic inversion centre and the non-aromatic ring in the TTSC molecule adopts an with a methylene C atom as the flap. In the crystal, the thiosemicarbazone molecules are connected through inversion-related pairs of N—H⋯S interactions, building a polymeric chain along the b-axis direction. The TCNP molecules are embedded in the structure, forming TTSC–TCNP–TTSC stacks with the aromatic rings of TTSC and the molecular plane of TCNP in a parallel arrangement [centroid–centroid distance = 3.5558 (14) Å]. Charge-transfer (CT) via π-stacking is indicated by a CT band around 550 cm−1 in the single-crystal absorption spectrum.
Keywords: charge-transfer composite compound; tetracyanopyrazine; thiosemicarbazone; crystal structure.
CCDC reference: 1022549
1. Related literature
For one of the first reports of the synthesis of thiosemicarbazone derivatives, see: Freund & Schander (1902). For the of tetralone–thiosemicarbazone, see: de Oliveira et al. (20127). For charge-transfer compounds involving TCNP, see: Rosokha et al. (2004). Tetracyanopyrazine was obtained by condensation of diiminosuccinonitrile with diaminomaleonitrile according to a literature procedure (Begland et al., 1974) For bond lengths in neat TCNP, see: Rosokha et al. (2009) and for the electronic situation in the TCNP molecule, see: Novoa et al. (2009).
2. Experimental
2.1. Crystal data
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2.3. Refinement
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Data collection: COLLECT (Nonius, 1998); cell SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
CCDC reference: 1022549
10.1107/S1600536814019795/hb7278sup1.cif
contains datablocks I, publication_text. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536814019795/hb7278Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814019795/hb7278Isup3.cml
The title compound represents a charge-transfer adduct composite of tetrahydronaphtalene-thiosemicarbazone (TTSC) and the strong
pyrazinetetracarbonitrile (tetracyanopyrazine, TCNP) in stoichiometry 2:1 (Fig. 1). TTSC has the maximum deviation from the mean plane of the non-H atoms of 0.448 (2) Å for C3, which corresponds to an for the non-aromatic ring. The structure of the thiosemicarbazone derivative is quite similar to the structure reported in the literature (Oliveira et al., 2012). The molecule shows an E conformation for the atoms about the N1–N2 bond. The torsion angle at the atoms N1, N2, C11 and S1 amounts to 176.4 (2)°, building a slightly distorted planar environment. The molecules are connected through inversion centres via pairs of N1–H···S interactions (Fig. 2 and Table 1) forming a one-dimensional hydrogen-bonded polymer running along the b-axis (Fig. 2).The TCNP molecule is essentially planar with the maximum deviation of 0.006 Å from the least squares plane through all atoms. Bond lengths differ less than 0.01 Å to neat TCNP (Rosokha et al. 2009). These non-significant differences show that the amount of charge-transfer is comparably small and the electronic situation of the TCNP molecule is mainly unaltered (Novoa et al., 2009).
The molecular planes of TTSC and TCNP molecules are parallel and arranged perpendicular to the [101] direction (Fig. 3). The TCNP molecules from stacks with each two neighboring TTSC molecules. The aromatic rings of two TTSC molecules and the TCNP planes are in an almost parallel arrangement. The shortest distances between the six-membered rings of 3.233 Å are observed between C7 of TTSC and C13 of TCNP (Fig. 4). As typical for weak to medium strong charge-transfer complexes between π systems, the normals through the midpoints of the aromatic rings are not coincident, instead the stack is slipped by about 15°.
The presence of a substantial charge-transfer in the title compound is indicated by the red colour, since the starting materials are light-yellow (TTSC) and colourless (TCNP) (Fig. 5). Moreover, the crystals are dichroitic and show a colour change in polarized light from red to light-brown.
In the single crystal
the charge-transfer band is present in the range 500 -650 nm (Fig. 6). Depending on the incident angle of the plane of polarization a distinct change of the charge-transfer band both in intensity and energy is present, explaining the different colours.The synthesis of 2-(1,2,3,4-tetrahydronaphthalen-1-ylidene)hydrazinecarbothioamide was adapted from a procedure reported over 100 years' ago (Freund & Schander, 1902). Tetracyanopyrazine was obtained by condensation of diiminosuccinonitrile with diaminomaleonitrile according to literature (Begland et al., 1974). The title compound (TTSC)2(TCNP) is formed only if an excess of TCNP is present. Solutions of two molar equivalents of TNCP and of one molar equivalent of TTSC in acetonitrile are prepared. On mixing the solutions, no significant colour change is observed. Slow evaporation of the solvent affords crystals of (TTSC)2(TCNP) as thin light-red plates, embedded in a matrix of excess TCNP. Crystals of the title compound had to be separated mechanically.
Data collection: COLLECT (Nonius, 1998); cell
SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO and SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).2C11H13N3S·C8N6 | Z = 1 |
Mr = 618.74 | F(000) = 322 |
Triclinic, P1 | Dx = 1.404 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.1363 (4) Å | Cell parameters from 15334 reflections |
b = 8.2574 (3) Å | θ = 2.9–27.5° |
c = 15.3303 (9) Å | µ = 0.23 mm−1 |
α = 86.659 (3)° | T = 293 K |
β = 78.751 (2)° | Plate, red |
γ = 73.893 (3)° | 0.06 × 0.04 × 0.02 mm |
V = 731.95 (7) Å3 |
Nonius KappaCCD diffractometer | 2601 independent reflections |
Radiation source: fine-focus sealed tube, Nonius KappaCCD | 1775 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.073 |
Detector resolution: 9 pixels mm-1 | θmax = 25.1°, θmin = 3.5° |
CCD rotation images, thick slices scans | h = −7→7 |
Absorption correction: analytical (Alcock, 1970) | k = −9→9 |
Tmin = 0.987, Tmax = 0.995 | l = −18→18 |
10255 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.096 | All H-atom parameters refined |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0321P)2 + 0.1427P] where P = (Fo2 + 2Fc2)/3 |
2601 reflections | (Δ/σ)max < 0.001 |
251 parameters | Δρmax = 0.26 e Å−3 |
0 restraints | Δρmin = −0.31 e Å−3 |
2C11H13N3S·C8N6 | γ = 73.893 (3)° |
Mr = 618.74 | V = 731.95 (7) Å3 |
Triclinic, P1 | Z = 1 |
a = 6.1363 (4) Å | Mo Kα radiation |
b = 8.2574 (3) Å | µ = 0.23 mm−1 |
c = 15.3303 (9) Å | T = 293 K |
α = 86.659 (3)° | 0.06 × 0.04 × 0.02 mm |
β = 78.751 (2)° |
Nonius KappaCCD diffractometer | 2601 independent reflections |
Absorption correction: analytical (Alcock, 1970) | 1775 reflections with I > 2σ(I) |
Tmin = 0.987, Tmax = 0.995 | Rint = 0.073 |
10255 measured reflections |
R[F2 > 2σ(F2)] = 0.045 | 0 restraints |
wR(F2) = 0.096 | All H-atom parameters refined |
S = 1.08 | Δρmax = 0.26 e Å−3 |
2601 reflections | Δρmin = −0.31 e Å−3 |
251 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.57106 (12) | 0.24556 (8) | 0.49235 (5) | 0.0255 (2) | |
N1 | −0.0374 (4) | 0.4493 (2) | 0.63392 (13) | 0.0209 (5) | |
N2 | 0.1759 (4) | 0.4342 (3) | 0.58009 (13) | 0.0202 (5) | |
N3 | 0.2050 (4) | 0.1530 (3) | 0.57790 (17) | 0.0311 (6) | |
C1 | −0.1576 (4) | 0.5967 (3) | 0.66381 (15) | 0.0187 (6) | |
C2 | −0.0813 (5) | 0.7547 (3) | 0.64597 (19) | 0.0218 (6) | |
C3 | −0.2709 (5) | 0.9130 (3) | 0.67964 (19) | 0.0267 (6) | |
C4 | −0.3900 (5) | 0.8872 (3) | 0.77390 (18) | 0.0271 (6) | |
C5 | −0.4936 (4) | 0.7411 (3) | 0.77777 (16) | 0.0213 (6) | |
C10 | −0.3814 (4) | 0.6016 (3) | 0.72246 (15) | 0.0191 (6) | |
C9 | −0.4809 (4) | 0.4679 (3) | 0.72410 (17) | 0.0226 (6) | |
C8 | −0.6878 (5) | 0.4710 (3) | 0.78065 (17) | 0.0260 (6) | |
C7 | −0.7975 (5) | 0.6088 (3) | 0.83626 (19) | 0.0274 (6) | |
C6 | −0.7026 (5) | 0.7431 (3) | 0.83434 (17) | 0.0265 (6) | |
C11 | 0.3029 (4) | 0.2765 (3) | 0.55299 (16) | 0.0203 (6) | |
H2A | −0.030 (4) | 0.763 (3) | 0.5850 (16) | 0.012 (6)* | |
H2B | 0.059 (5) | 0.742 (3) | 0.6765 (17) | 0.030 (7)* | |
H3A | −0.383 (5) | 0.937 (3) | 0.6388 (19) | 0.039 (8)* | |
H3B | −0.205 (4) | 1.011 (3) | 0.6756 (16) | 0.028 (7)* | |
H4A | −0.509 (5) | 0.991 (3) | 0.7973 (17) | 0.034 (7)* | |
H4B | −0.275 (5) | 0.862 (3) | 0.8164 (17) | 0.032 (7)* | |
H6 | −0.404 (4) | 0.373 (3) | 0.6829 (17) | 0.032 (7)* | |
H7 | −0.754 (5) | 0.383 (3) | 0.7821 (17) | 0.030 (7)* | |
H8 | −0.933 (5) | 0.612 (3) | 0.8765 (19) | 0.038 (8)* | |
H9 | −0.779 (5) | 0.839 (3) | 0.8738 (18) | 0.035 (8)* | |
HN2 | 0.242 (5) | 0.518 (3) | 0.5664 (18) | 0.037 (8)* | |
HN3A | 0.283 (5) | 0.047 (4) | 0.5558 (19) | 0.044 (9)* | |
HN3B | 0.065 (6) | 0.176 (4) | 0.607 (2) | 0.053 (10)* | |
N4 | 0.2849 (4) | 0.4881 (3) | 0.04821 (14) | 0.0251 (5) | |
N5 | 0.1068 (4) | 0.8479 (3) | 0.17016 (16) | 0.0355 (6) | |
N6 | 0.2570 (4) | 0.1174 (3) | −0.02636 (15) | 0.0375 (6) | |
C12 | 0.3663 (4) | 0.6193 (3) | 0.05758 (16) | 0.0228 (6) | |
C13 | 0.4196 (4) | 0.3699 (3) | −0.00991 (16) | 0.0231 (6) | |
C14 | 0.2226 (5) | 0.7472 (3) | 0.12048 (18) | 0.0263 (6) | |
C15 | 0.3294 (5) | 0.2286 (3) | −0.01969 (18) | 0.0282 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0220 (4) | 0.0187 (3) | 0.0324 (4) | −0.0062 (3) | 0.0051 (3) | −0.0043 (3) |
N1 | 0.0186 (12) | 0.0223 (11) | 0.0218 (12) | −0.0064 (9) | −0.0019 (10) | −0.0011 (9) |
N2 | 0.0174 (12) | 0.0189 (12) | 0.0232 (12) | −0.0073 (10) | 0.0027 (10) | −0.0028 (9) |
N3 | 0.0210 (15) | 0.0194 (13) | 0.0476 (16) | −0.0074 (11) | 0.0105 (12) | −0.0064 (11) |
C1 | 0.0198 (14) | 0.0176 (13) | 0.0185 (14) | −0.0044 (10) | −0.0040 (11) | −0.0006 (10) |
C2 | 0.0202 (16) | 0.0215 (14) | 0.0207 (16) | −0.0030 (11) | 0.0001 (13) | −0.0009 (11) |
C3 | 0.0286 (17) | 0.0185 (14) | 0.0320 (17) | −0.0075 (12) | −0.0009 (14) | −0.0023 (11) |
C4 | 0.0271 (17) | 0.0229 (15) | 0.0279 (16) | −0.0044 (12) | 0.0007 (14) | −0.0047 (12) |
C5 | 0.0207 (15) | 0.0216 (13) | 0.0198 (14) | −0.0029 (11) | −0.0044 (12) | 0.0011 (10) |
C10 | 0.0169 (14) | 0.0227 (13) | 0.0172 (14) | −0.0046 (11) | −0.0032 (11) | 0.0004 (10) |
C9 | 0.0221 (16) | 0.0224 (14) | 0.0244 (15) | −0.0076 (12) | −0.0049 (12) | 0.0012 (11) |
C8 | 0.0219 (16) | 0.0306 (16) | 0.0276 (16) | −0.0110 (13) | −0.0062 (13) | 0.0067 (12) |
C7 | 0.0171 (16) | 0.0365 (16) | 0.0242 (16) | −0.0033 (12) | 0.0001 (13) | 0.0035 (12) |
C6 | 0.0223 (16) | 0.0290 (15) | 0.0233 (16) | −0.0011 (12) | −0.0007 (13) | −0.0016 (12) |
C11 | 0.0186 (15) | 0.0193 (13) | 0.0224 (14) | −0.0064 (11) | 0.0002 (11) | −0.0026 (10) |
N4 | 0.0221 (13) | 0.0290 (12) | 0.0256 (13) | −0.0091 (10) | −0.0043 (10) | −0.0011 (10) |
N5 | 0.0277 (15) | 0.0353 (14) | 0.0398 (16) | −0.0039 (11) | −0.0027 (12) | −0.0060 (12) |
N6 | 0.0369 (16) | 0.0411 (15) | 0.0373 (15) | −0.0173 (13) | −0.0027 (12) | −0.0048 (11) |
C12 | 0.0198 (15) | 0.0278 (14) | 0.0206 (14) | −0.0047 (11) | −0.0051 (12) | −0.0011 (11) |
C13 | 0.0214 (15) | 0.0282 (14) | 0.0205 (14) | −0.0086 (12) | −0.0030 (12) | 0.0000 (11) |
C14 | 0.0217 (16) | 0.0319 (15) | 0.0267 (16) | −0.0098 (13) | −0.0042 (13) | 0.0004 (12) |
C15 | 0.0238 (16) | 0.0319 (16) | 0.0289 (16) | −0.0097 (13) | −0.0009 (13) | −0.0039 (12) |
S1—C11 | 1.684 (2) | C5—C6 | 1.398 (4) |
N1—C1 | 1.292 (3) | C5—C10 | 1.402 (3) |
N1—N2 | 1.382 (3) | C10—C9 | 1.399 (3) |
N2—C11 | 1.360 (3) | C9—C8 | 1.385 (4) |
N2—HN2 | 0.89 (3) | C9—H6 | 0.98 (3) |
N3—C11 | 1.324 (3) | C8—C7 | 1.392 (4) |
N3—HN3A | 0.92 (3) | C8—H7 | 0.92 (3) |
N3—HN3B | 0.86 (3) | C7—C6 | 1.385 (4) |
C1—C10 | 1.479 (3) | C7—H8 | 0.93 (3) |
C1—C2 | 1.498 (3) | C6—H9 | 0.98 (3) |
C2—C3 | 1.526 (3) | N4—C12 | 1.338 (3) |
C2—H2A | 0.93 (2) | N4—C13 | 1.340 (3) |
C2—H2B | 1.04 (3) | N5—C14 | 1.146 (3) |
C3—C4 | 1.519 (4) | N6—C15 | 1.143 (3) |
C3—H3A | 0.99 (3) | C12—C13i | 1.397 (4) |
C3—H3B | 0.99 (3) | C12—C14 | 1.447 (4) |
C4—C5 | 1.505 (3) | C13—C12i | 1.396 (4) |
C4—H4A | 0.99 (3) | C13—C15 | 1.450 (4) |
C4—H4B | 1.02 (3) | ||
C1—N1—N2 | 118.6 (2) | C6—C5—C4 | 121.2 (2) |
C11—N2—N1 | 117.3 (2) | C10—C5—C4 | 119.6 (2) |
C11—N2—HN2 | 117.5 (18) | C9—C10—C5 | 119.7 (2) |
N1—N2—HN2 | 124.9 (18) | C9—C10—C1 | 120.8 (2) |
C11—N3—HN3A | 117.4 (19) | C5—C10—C1 | 119.6 (2) |
C11—N3—HN3B | 120 (2) | C8—C9—C10 | 120.6 (2) |
HN3A—N3—HN3B | 122 (3) | C8—C9—H6 | 120.5 (16) |
N1—C1—C10 | 115.3 (2) | C10—C9—H6 | 118.9 (16) |
N1—C1—C2 | 124.8 (2) | C9—C8—C7 | 119.6 (3) |
C10—C1—C2 | 119.9 (2) | C9—C8—H7 | 120.9 (17) |
C1—C2—C3 | 113.1 (2) | C7—C8—H7 | 119.5 (17) |
C1—C2—H2A | 108.4 (13) | C6—C7—C8 | 120.4 (3) |
C3—C2—H2A | 110.3 (14) | C6—C7—H8 | 118.5 (16) |
C1—C2—H2B | 107.8 (13) | C8—C7—H8 | 121.1 (17) |
C3—C2—H2B | 109.8 (13) | C7—C6—C5 | 120.6 (2) |
H2A—C2—H2B | 107 (2) | C7—C6—H9 | 120.3 (16) |
C4—C3—C2 | 110.8 (2) | C5—C6—H9 | 119.0 (16) |
C4—C3—H3A | 110.5 (16) | N3—C11—N2 | 116.4 (2) |
C2—C3—H3A | 107.6 (15) | N3—C11—S1 | 123.34 (19) |
C4—C3—H3B | 111.5 (14) | N2—C11—S1 | 120.27 (18) |
C2—C3—H3B | 109.8 (15) | C12—N4—C13 | 116.1 (2) |
H3A—C3—H3B | 106 (2) | N4—C12—C13i | 121.5 (2) |
C5—C4—C3 | 110.5 (2) | N4—C12—C14 | 116.4 (2) |
C5—C4—H4A | 110.8 (15) | C13i—C12—C14 | 122.1 (2) |
C3—C4—H4A | 111.5 (15) | N4—C13—C12i | 122.5 (2) |
C5—C4—H4B | 107.9 (14) | N4—C13—C15 | 115.6 (2) |
C3—C4—H4B | 110.8 (15) | C12i—C13—C15 | 121.9 (2) |
H4A—C4—H4B | 105 (2) | N5—C14—C12 | 179.3 (3) |
C6—C5—C10 | 119.1 (2) | N6—C15—C13 | 179.2 (3) |
C1—N1—N2—C11 | 177.1 (2) | N1—C1—C10—C5 | 162.0 (2) |
N2—N1—C1—C10 | −178.73 (19) | C2—C1—C10—C5 | −15.5 (3) |
N2—N1—C1—C2 | −1.3 (3) | C5—C10—C9—C8 | −0.8 (4) |
N1—C1—C2—C3 | 172.5 (2) | C1—C10—C9—C8 | 178.4 (2) |
C10—C1—C2—C3 | −10.1 (3) | C10—C9—C8—C7 | 0.1 (4) |
C1—C2—C3—C4 | 46.8 (3) | C9—C8—C7—C6 | 0.9 (4) |
C2—C3—C4—C5 | −58.8 (3) | C8—C7—C6—C5 | −1.1 (4) |
C3—C4—C5—C6 | −144.3 (2) | C10—C5—C6—C7 | 0.3 (4) |
C3—C4—C5—C10 | 34.5 (3) | C4—C5—C6—C7 | 179.1 (2) |
C6—C5—C10—C9 | 0.6 (4) | N1—N2—C11—N3 | 2.8 (3) |
C4—C5—C10—C9 | −178.1 (2) | N1—N2—C11—S1 | −176.37 (16) |
C6—C5—C10—C1 | −178.7 (2) | C13—N4—C12—C13i | −0.6 (4) |
C4—C5—C10—C1 | 2.6 (3) | C13—N4—C12—C14 | −179.7 (2) |
N1—C1—C10—C9 | −17.2 (3) | C12—N4—C13—C12i | 0.6 (4) |
C2—C1—C10—C9 | 165.2 (2) | C12—N4—C13—C15 | −179.9 (2) |
Symmetry code: (i) −x+1, −y+1, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—HN2···S1ii | 0.89 (3) | 2.57 (3) | 3.450 (2) | 173 (2) |
N3—HN3A···S1iii | 0.92 (3) | 2.44 (3) | 3.348 (2) | 170 (3) |
Symmetry codes: (ii) −x+1, −y+1, −z+1; (iii) −x+1, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—HN2···S1i | 0.89 (3) | 2.57 (3) | 3.450 (2) | 173 (2) |
N3—HN3A···S1ii | 0.92 (3) | 2.44 (3) | 3.348 (2) | 170 (3) |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1, −y, −z+1. |
Acknowledgements
We gratefully acknowledge financial support by the German Research Foundation (DFG) through the Collaborative Research Center SFB 813, Chemistry at Spin Centers, and by FAPITEC/SE/FUNTEC/CNPq through the PPP Program 04/ 2011.
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