Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807023239/hb2410sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536807023239/hb2410Isup2.hkl |
CCDC reference: 651771
The title compound was synthesized according to the literature method (Furnis et al., 1989) with a yield of 80% and purified by recrystallization from ethanol. Crystals of (I) were grown from DMF solution by slow evaporation (m.p. 423–425 K). Analysis for C9H11N3OS: Found (Calculated): C 51.55 (51.65); H 5.28 (5.30); N 20.15% (20.08%).
The H atoms were found in a difference map, but those bonded to C were refined using a riding model with C—H = 0.95 Å and Uiso(H) = 1.2Ueq(C) or C—H = 0.98 Å and Uiso(H) = 1.5Ueq(Cmethyl). The H atoms bonded to N were refined with an N—H distance restraint of 0.88 (1) Å. The methyl group is disordered over two sites with occupation factors of 0.505 (6) and 0.495 (6).
NLO materials play an important role in the field of fibre optic communications and optical signal processing. In the last two decades, extensive research has shown that organic crystals can exhibit nonlinear optical efficiencies which are two orders of magnitude higher than those of inorganic materials. Thiosemicarbazones (TSCs) of aromatic aldehydes and ketones are widely known as carcinostatic and antimicrobial agents. Semicarbazones of substituted benzaldehydes and acetophenones were reported to be some of the potential organic NLO materials. In the present paper, we report the crystal structure of title compound, (I), C9H11N3OS.
For related structures, see: acetone semicarbazone and benzaldehyde semicarbazone (Naik & Palenik, 1974); 3,4-methylenedioxybenzaldehyde semicarbazone (Wang et al., 2004); 4-(methylsulfanyl)benzaldehyde thiosemicarbazone (Yathirajan et al., 2006).
For related literature, see: Fichou et al. (1988); Furnis et al. (1989); Goto et al. (1991); Tam et al. (1989); Indira et al. (2002); Vijayan et al. (2001); Ramesh Babu et al. (2002); Manivennan & Dhanushkodi (2003).
Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97.
Fig. 1. Perspective view of (I); displacement ellipsoids are at the 50% probability level (arbitrary spheres for the H atoms). One site of the disordered methyl group is shown with dashed bonds. |
C9H11N3OS | F(000) = 440 |
Mr = 209.27 | Dx = 1.391 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 5218 reflections |
a = 15.1006 (19) Å | θ = 3.3–27.2° |
b = 5.3082 (7) Å | µ = 0.29 mm−1 |
c = 13.0746 (17) Å | T = 173 K |
β = 107.494 (9)° | Block, colourless |
V = 999.5 (2) Å3 | 0.48 × 0.45 × 0.43 mm |
Z = 4 |
Stoe IPDS II two-circle diffractometer | 2162 independent reflections |
Radiation source: fine-focus sealed tube | 1678 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.053 |
ω scans | θmax = 27.0°, θmin = 2.8° |
Absorption correction: multi-scan [MULABS (Spek, 2003; Blessing, 1995)] | h = −19→19 |
Tmin = 0.872, Tmax = 0.884 | k = −6→6 |
7445 measured reflections | l = −14→16 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.054 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.168 | w = 1/[σ2(Fo2) + (0.0852P)2 + 0.4974P] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max < 0.001 |
2162 reflections | Δρmax = 0.46 e Å−3 |
152 parameters | Δρmin = −0.66 e Å−3 |
3 restraints | Extinction correction: SHELXL (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.087 (13) |
C9H11N3OS | V = 999.5 (2) Å3 |
Mr = 209.27 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 15.1006 (19) Å | µ = 0.29 mm−1 |
b = 5.3082 (7) Å | T = 173 K |
c = 13.0746 (17) Å | 0.48 × 0.45 × 0.43 mm |
β = 107.494 (9)° |
Stoe IPDS II two-circle diffractometer | 2162 independent reflections |
Absorption correction: multi-scan [MULABS (Spek, 2003; Blessing, 1995)] | 1678 reflections with I > 2σ(I) |
Tmin = 0.872, Tmax = 0.884 | Rint = 0.053 |
7445 measured reflections |
R[F2 > 2σ(F2)] = 0.054 | 3 restraints |
wR(F2) = 0.168 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | Δρmax = 0.46 e Å−3 |
2162 reflections | Δρmin = −0.66 e Å−3 |
152 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 | Occ. (<1) | |
N2 | 0.08441 (13) | −0.2424 (3) | 0.53704 (18) | 0.0462 (5) | |
H2 | 0.0655 (18) | −0.359 (4) | 0.4872 (17) | 0.051 (7)* | |
S1 | 0.42858 (5) | 0.66516 (12) | 0.32545 (8) | 0.0703 (4) | |
O1 | 0.00019 (11) | −0.4136 (3) | 0.63569 (15) | 0.0487 (5) | |
N1 | 0.13881 (12) | −0.0461 (3) | 0.52048 (17) | 0.0439 (5) | |
N3 | 0.07342 (13) | −0.0387 (4) | 0.68943 (18) | 0.0478 (5) | |
H3A | 0.049 (2) | −0.017 (7) | 0.7422 (19) | 0.075 (10)* | |
H3B | 0.1089 (17) | 0.078 (4) | 0.675 (2) | 0.057 (8)* | |
C1 | 0.15927 (14) | −0.0536 (4) | 0.4320 (2) | 0.0440 (6) | |
H1 | 0.1340 | −0.1846 | 0.3823 | 0.053* | |
C2 | 0.04991 (14) | −0.2357 (4) | 0.62250 (19) | 0.0426 (6) | |
C11 | 0.22026 (14) | 0.1332 (4) | 0.4052 (2) | 0.0424 (5) | |
C12 | 0.24456 (15) | 0.1058 (4) | 0.3108 (2) | 0.0477 (6) | |
H12 | 0.2182 | −0.0281 | 0.2631 | 0.057* | |
C13 | 0.30620 (15) | 0.2693 (5) | 0.2850 (2) | 0.0478 (6) | |
H13 | 0.3216 | 0.2469 | 0.2203 | 0.057* | |
C14 | 0.34570 (14) | 0.4670 (4) | 0.3542 (2) | 0.0451 (6) | |
C15 | 0.32039 (15) | 0.4988 (4) | 0.4481 (2) | 0.0482 (6) | |
H15 | 0.3461 | 0.6340 | 0.4953 | 0.058* | |
C16 | 0.25829 (16) | 0.3356 (4) | 0.4730 (2) | 0.0466 (6) | |
H16 | 0.2413 | 0.3611 | 0.5366 | 0.056* | |
C17 | 0.4761 (3) | 0.8650 (9) | 0.4225 (4) | 0.0513 (14) | 0.495 (6) |
H17A | 0.5225 | 0.9672 | 0.4026 | 0.077* | 0.495 (6) |
H17B | 0.5063 | 0.7718 | 0.4885 | 0.077* | 0.495 (6) |
H17C | 0.4280 | 0.9752 | 0.4342 | 0.077* | 0.495 (6) |
C17' | 0.4006 (4) | 0.6638 (12) | 0.1996 (5) | 0.0642 (17) | 0.505 (6) |
H17D | 0.3337 | 0.6944 | 0.1701 | 0.096* | 0.505 (6) |
H17E | 0.4158 | 0.4998 | 0.1749 | 0.096* | 0.505 (6) |
H17F | 0.4347 | 0.7965 | 0.1754 | 0.096* | 0.505 (6) |
U11 | U22 | U33 | U12 | U13 | U23 | |
N2 | 0.0425 (9) | 0.0279 (9) | 0.0604 (12) | −0.0064 (7) | 0.0039 (9) | −0.0055 (8) |
S1 | 0.0441 (4) | 0.0384 (4) | 0.1218 (8) | −0.0049 (2) | 0.0148 (4) | 0.0032 (3) |
O1 | 0.0434 (8) | 0.0270 (7) | 0.0686 (12) | −0.0057 (6) | 0.0062 (7) | −0.0010 (7) |
N1 | 0.0352 (9) | 0.0267 (9) | 0.0601 (13) | −0.0011 (7) | −0.0002 (8) | −0.0003 (8) |
N3 | 0.0440 (10) | 0.0299 (9) | 0.0614 (13) | −0.0066 (8) | 0.0036 (9) | −0.0039 (9) |
C1 | 0.0347 (10) | 0.0293 (10) | 0.0572 (14) | 0.0016 (8) | −0.0027 (9) | −0.0030 (9) |
C2 | 0.0327 (10) | 0.0267 (9) | 0.0575 (14) | 0.0025 (8) | −0.0029 (9) | 0.0019 (9) |
C11 | 0.0318 (9) | 0.0286 (10) | 0.0562 (14) | 0.0048 (7) | −0.0027 (9) | 0.0006 (9) |
C12 | 0.0373 (10) | 0.0354 (11) | 0.0584 (15) | 0.0020 (8) | −0.0036 (10) | −0.0072 (10) |
C13 | 0.0415 (11) | 0.0406 (12) | 0.0540 (14) | 0.0052 (9) | 0.0031 (10) | −0.0035 (10) |
C14 | 0.0363 (10) | 0.0293 (10) | 0.0611 (15) | 0.0067 (8) | 0.0018 (9) | 0.0008 (9) |
C15 | 0.0452 (11) | 0.0290 (10) | 0.0605 (15) | −0.0003 (9) | 0.0009 (10) | −0.0058 (9) |
C16 | 0.0423 (11) | 0.0322 (11) | 0.0562 (14) | 0.0010 (8) | 0.0012 (10) | −0.0008 (9) |
C17 | 0.036 (2) | 0.043 (3) | 0.068 (3) | −0.0043 (18) | 0.005 (2) | 0.007 (2) |
C17' | 0.054 (3) | 0.070 (4) | 0.064 (4) | −0.014 (3) | 0.011 (2) | 0.012 (3) |
N2—C2 | 1.368 (3) | C12—C13 | 1.386 (4) |
N2—N1 | 1.384 (3) | C12—H12 | 0.9500 |
N2—H2 | 0.881 (10) | C13—C14 | 1.397 (3) |
S1—C17' | 1.571 (6) | C13—H13 | 0.9500 |
S1—C17 | 1.644 (5) | C14—C15 | 1.401 (4) |
S1—C14 | 1.760 (2) | C15—C16 | 1.385 (3) |
O1—C2 | 1.250 (3) | C15—H15 | 0.9500 |
N1—C1 | 1.285 (3) | C16—H16 | 0.9500 |
N3—C2 | 1.341 (3) | C17—H17A | 0.9800 |
N3—H3A | 0.886 (10) | C17—H17B | 0.9800 |
N3—H3B | 0.875 (10) | C17—H17C | 0.9800 |
C1—C11 | 1.466 (3) | C17'—H17D | 0.9800 |
C1—H1 | 0.9500 | C17'—H17E | 0.9800 |
C11—C12 | 1.397 (4) | C17'—H17F | 0.9800 |
C11—C16 | 1.402 (3) | ||
C2—N2—N1 | 119.86 (19) | C12—C13—C14 | 120.0 (2) |
C2—N2—H2 | 120.2 (19) | C12—C13—H13 | 120.0 |
N1—N2—H2 | 119.3 (19) | C14—C13—H13 | 120.0 |
C17'—S1—C17 | 136.8 (3) | C13—C14—C15 | 118.8 (2) |
C17'—S1—C14 | 103.7 (2) | C13—C14—S1 | 120.2 (2) |
C17—S1—C14 | 113.2 (2) | C15—C14—S1 | 120.93 (17) |
C1—N1—N2 | 115.62 (19) | C16—C15—C14 | 120.8 (2) |
C2—N3—H3A | 121 (2) | C16—C15—H15 | 119.6 |
C2—N3—H3B | 118 (2) | C14—C15—H15 | 119.6 |
H3A—N3—H3B | 121 (3) | C15—C16—C11 | 120.5 (3) |
N1—C1—C11 | 122.2 (2) | C15—C16—H16 | 119.7 |
N1—C1—H1 | 118.9 | C11—C16—H16 | 119.7 |
C11—C1—H1 | 118.9 | S1—C17—H17A | 109.5 |
O1—C2—N3 | 123.5 (2) | S1—C17—H17B | 109.5 |
O1—C2—N2 | 119.0 (2) | S1—C17—H17C | 109.5 |
N3—C2—N2 | 117.5 (2) | S1—C17'—H17D | 109.5 |
C12—C11—C16 | 118.2 (2) | S1—C17'—H17E | 109.5 |
C12—C11—C1 | 119.5 (2) | H17D—C17'—H17E | 109.5 |
C16—C11—C1 | 122.3 (2) | S1—C17'—H17F | 109.5 |
C13—C12—C11 | 121.6 (2) | H17D—C17'—H17F | 109.5 |
C13—C12—H12 | 119.2 | H17E—C17'—H17F | 109.5 |
C11—C12—H12 | 119.2 | ||
C2—N2—N1—C1 | −172.28 (18) | C12—C13—C14—S1 | 176.68 (16) |
N2—N1—C1—C11 | −176.76 (17) | C17'—S1—C14—C13 | 29.8 (3) |
N1—N2—C2—O1 | 179.36 (18) | C17—S1—C14—C13 | −173.2 (2) |
N1—N2—C2—N3 | −2.1 (3) | C17'—S1—C14—C15 | −152.3 (3) |
N1—C1—C11—C12 | 175.99 (19) | C17—S1—C14—C15 | 4.7 (3) |
N1—C1—C11—C16 | −1.7 (3) | C13—C14—C15—C16 | 0.9 (3) |
C16—C11—C12—C13 | 1.5 (3) | S1—C14—C15—C16 | −177.06 (16) |
C1—C11—C12—C13 | −176.25 (19) | C14—C15—C16—C11 | 0.7 (3) |
C11—C12—C13—C14 | 0.1 (3) | C12—C11—C16—C15 | −1.9 (3) |
C12—C13—C14—C15 | −1.3 (3) | C1—C11—C16—C15 | 175.80 (19) |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2···O1i | 0.88 (1) | 2.02 (1) | 2.886 (3) | 169 (2) |
N3—H3A···O1ii | 0.89 (1) | 2.03 (1) | 2.904 (3) | 171 (4) |
Symmetry codes: (i) −x, −y−1, −z+1; (ii) −x, y+1/2, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | C9H11N3OS |
Mr | 209.27 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 173 |
a, b, c (Å) | 15.1006 (19), 5.3082 (7), 13.0746 (17) |
β (°) | 107.494 (9) |
V (Å3) | 999.5 (2) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.29 |
Crystal size (mm) | 0.48 × 0.45 × 0.43 |
Data collection | |
Diffractometer | Stoe IPDS II two-circle |
Absorption correction | Multi-scan [MULABS (Spek, 2003; Blessing, 1995)] |
Tmin, Tmax | 0.872, 0.884 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7445, 2162, 1678 |
Rint | 0.053 |
(sin θ/λ)max (Å−1) | 0.638 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.054, 0.168, 1.09 |
No. of reflections | 2162 |
No. of parameters | 152 |
No. of restraints | 3 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.46, −0.66 |
Computer programs: X-AREA (Stoe & Cie, 2001), X-AREA, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2003), SHELXL97.
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2···O1i | 0.881 (10) | 2.016 (11) | 2.886 (3) | 169 (2) |
N3—H3A···O1ii | 0.886 (10) | 2.025 (12) | 2.904 (3) | 171 (4) |
Symmetry codes: (i) −x, −y−1, −z+1; (ii) −x, y+1/2, −z+3/2. |
NLO materials play an important role in the field of fibre optic communications and optical signal processing. In the last two decades, extensive research has shown that organic crystals can exhibit nonlinear optical efficiencies which are two orders of magnitude higher than those of inorganic materials. Thiosemicarbazones (TSCs) of aromatic aldehydes and ketones are widely known as carcinostatic and antimicrobial agents. Semicarbazones of substituted benzaldehydes and acetophenones were reported to be some of the potential organic NLO materials. In the present paper, we report the crystal structure of title compound, (I), C9H11N3OS.