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In the title compound, C16H10N2S2, (I), which was synthesized via the reaction of 2,2'-thenil and 1,2-phenyl­enedi­amine, the thienyl rings display ideal geometries, with no evidence of ring-flip disorders often found with unsubstituted terminal 2-thienyl rings [Zheng, Wang, Liu, Carducci, Peyghambarian & Jabbourb (2002). Acta Cryst. C58, m50-m52].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803002976/lh6035sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803002976/lh6035Isup2.hkl
Contains datablock I

CCDC reference: 206775

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.061
  • wR factor = 0.122
  • Data-to-parameter ratio = 14.5

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
ABSTM_02 Alert C The ratio of expected to reported Tmax/Tmin(RR') is < 0.90 Tmin and Tmax reported: 0.753 1.000 Tmin' and Tmax expected: 0.867 0.954 RR' = 0.829 Please check that your absorption correction is appropriate.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SHELXTL (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXL97; software used to prepare material for publication: SHELXL97.

2,3-Dithien-2-ylquinoxaline top
Crystal data top
C16H10N2S2F(000) = 608
Mr = 294.38Dx = 1.475 Mg m3
Monoclinic, P21/cMelting point: 145 K
Hall symbol: -P 2ybcMo Kα radiation, λ = 0.71073 Å
a = 11.521 (3) ÅCell parameters from 11758 reflections
b = 5.2071 (14) Åθ = 2.1–28.3°
c = 22.745 (7) ŵ = 0.39 mm1
β = 103.681 (4)°T = 293 K
V = 1325.8 (6) Å3Needle, yellow
Z = 40.36 × 0.23 × 0.12 mm
Data collection top
Bruker SMART P3/512CCD
diffractometer
2617 independent reflections
Radiation source: fine-focus sealed tube2103 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
ω scansθmax = 26.0°, θmin = 1.8°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1414
Tmin = 0.753, Tmax = 1.000k = 66
10027 measured reflectionsl = 2728
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.061Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.122H-atom parameters constrained
S = 1.19 w = 1/[σ2(Fo2) + (0.0403P)2 + 1.0471P]
where P = (Fo2 + 2Fc2)/3
2617 reflections(Δ/σ)max < 0.001
181 parametersΔρmax = 0.24 e Å3
0 restraintsΔρmin = 0.29 e Å3
Special details top

Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.

Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.3645 (2)0.3248 (5)0.06163 (11)0.0342 (6)
C10.2844 (2)0.1437 (6)0.06298 (12)0.0298 (6)
N20.2168 (2)0.1568 (5)0.17120 (10)0.0339 (6)
C20.2089 (2)0.0560 (6)0.11919 (12)0.0295 (6)
C30.2986 (3)0.3467 (6)0.16997 (13)0.0346 (7)
C40.3094 (3)0.4609 (7)0.22448 (15)0.0476 (9)
H4A0.26140.40510.26100.057*
C50.3896 (3)0.6520 (7)0.22394 (16)0.0512 (9)
H5A0.39550.72820.26010.061*
C60.4640 (3)0.7355 (7)0.16904 (16)0.0481 (9)
H6A0.51910.86600.16920.058*
C70.4562 (3)0.6274 (6)0.11584 (15)0.0422 (8)
H7A0.50560.68390.07970.051*
C80.3733 (2)0.4296 (6)0.11548 (13)0.0330 (7)
C90.2743 (2)0.0475 (6)0.00336 (13)0.0323 (7)
C100.3374 (3)0.1392 (6)0.03159 (13)0.0391 (8)
H10A0.39820.23260.02100.047*
C110.3004 (3)0.1768 (7)0.08615 (14)0.0446 (8)
H11A0.33400.29860.11510.053*
C120.2121 (3)0.0183 (6)0.09152 (14)0.0424 (8)
H12A0.17730.01710.12450.051*
S10.17130 (8)0.18052 (17)0.03086 (4)0.0460 (3)
C130.1193 (2)0.1475 (5)0.12294 (12)0.0294 (6)
C140.0945 (3)0.3165 (6)0.08138 (13)0.0345 (7)
H14A0.13540.31830.04090.041*
C150.0012 (3)0.4866 (6)0.10608 (14)0.0357 (7)
H15A0.02570.61350.08370.043*
C160.0453 (3)0.4470 (6)0.16547 (14)0.0395 (7)
H16A0.10790.54200.18870.047*
S20.02454 (7)0.20146 (17)0.19284 (3)0.0425 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0300 (13)0.0354 (15)0.0362 (14)0.0013 (11)0.0057 (11)0.0025 (12)
C10.0264 (14)0.0308 (16)0.0320 (15)0.0040 (12)0.0062 (12)0.0007 (12)
N20.0338 (13)0.0367 (15)0.0303 (13)0.0032 (12)0.0056 (11)0.0012 (11)
C20.0248 (14)0.0316 (16)0.0318 (16)0.0011 (12)0.0060 (12)0.0030 (13)
C30.0288 (15)0.0372 (18)0.0385 (17)0.0001 (14)0.0091 (13)0.0015 (14)
C40.048 (2)0.055 (2)0.0389 (18)0.0089 (18)0.0085 (15)0.0046 (17)
C50.055 (2)0.056 (2)0.047 (2)0.0071 (19)0.0200 (17)0.0099 (17)
C60.0402 (18)0.044 (2)0.063 (2)0.0105 (16)0.0172 (17)0.0022 (17)
C70.0375 (17)0.040 (2)0.0473 (19)0.0061 (14)0.0072 (15)0.0042 (15)
C80.0269 (14)0.0323 (16)0.0396 (17)0.0013 (13)0.0078 (13)0.0010 (14)
C90.0300 (15)0.0366 (17)0.0291 (15)0.0015 (13)0.0044 (12)0.0061 (13)
C100.0360 (17)0.046 (2)0.0330 (16)0.0044 (15)0.0031 (13)0.0006 (14)
C110.0505 (19)0.047 (2)0.0308 (16)0.0025 (18)0.0009 (14)0.0038 (15)
C120.055 (2)0.042 (2)0.0324 (17)0.0073 (17)0.0142 (15)0.0029 (15)
S10.0570 (5)0.0428 (5)0.0438 (5)0.0106 (4)0.0232 (4)0.0033 (4)
C130.0260 (14)0.0321 (16)0.0291 (15)0.0027 (12)0.0047 (12)0.0037 (12)
C140.0336 (15)0.0342 (17)0.0335 (16)0.0013 (14)0.0033 (12)0.0004 (14)
C150.0370 (17)0.0301 (17)0.0419 (18)0.0018 (14)0.0127 (14)0.0007 (14)
C160.0372 (17)0.0347 (18)0.0457 (19)0.0061 (14)0.0079 (14)0.0068 (15)
S20.0461 (5)0.0469 (5)0.0305 (4)0.0124 (4)0.0015 (3)0.0007 (4)
Geometric parameters (Å, º) top
N1—C11.314 (4)C9—C101.353 (4)
N1—C81.366 (4)C9—S11.712 (3)
C1—C21.440 (4)C10—C111.417 (4)
C1—C91.476 (4)C10—H10A0.9300
N2—C21.317 (4)C11—C121.338 (5)
N2—C31.361 (4)C11—H11A0.9300
C2—C131.468 (4)C12—S11.700 (3)
C3—C81.400 (4)C12—H12A0.9300
C3—C41.407 (4)C13—C141.370 (4)
C4—C51.356 (5)C13—S21.726 (3)
C4—H4A0.9300C14—C151.404 (4)
C5—C61.406 (5)C14—H14A0.9300
C5—H5A0.9300C15—C161.346 (4)
C6—C71.356 (4)C15—H15A0.9300
C6—H6A0.9300C16—S21.705 (3)
C7—C81.406 (4)C16—H16A0.9300
C7—H7A0.9300
C1—N1—C8117.8 (2)C10—C9—C1129.5 (3)
N1—C1—C2121.4 (3)C10—C9—S1110.9 (2)
N1—C1—C9115.4 (2)C1—C9—S1119.6 (2)
C2—C1—C9123.1 (3)C9—C10—C11112.5 (3)
C2—N2—C3117.8 (2)C9—C10—H10A123.7
N2—C2—C1121.0 (3)C11—C10—H10A123.7
N2—C2—C13115.7 (2)C12—C11—C10112.8 (3)
C1—C2—C13123.3 (3)C12—C11—H11A123.6
N2—C3—C8121.3 (3)C10—C11—H11A123.6
N2—C3—C4119.6 (3)C11—C12—S1111.8 (2)
C8—C3—C4119.1 (3)C11—C12—H12A124.1
C5—C4—C3120.3 (3)S1—C12—H12A124.1
C5—C4—H4A119.8C12—S1—C991.96 (16)
C3—C4—H4A119.8C14—C13—C2133.0 (3)
C4—C5—C6120.4 (3)C14—C13—S2110.0 (2)
C4—C5—H5A119.8C2—C13—S2117.0 (2)
C6—C5—H5A119.8C13—C14—C15113.2 (3)
C7—C6—C5120.6 (3)C13—C14—H14A123.4
C7—C6—H6A119.7C15—C14—H14A123.4
C5—C6—H6A119.7C16—C15—C14113.0 (3)
C6—C7—C8119.8 (3)C16—C15—H15A123.5
C6—C7—H7A120.1C14—C15—H15A123.5
C8—C7—H7A120.1C15—C16—S2111.8 (2)
N1—C8—C3120.7 (3)C15—C16—H16A124.1
N1—C8—C7119.5 (3)S2—C16—H16A124.1
C3—C8—C7119.8 (3)C16—S2—C1392.06 (15)
 

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