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4H,5H,6H,7H,8H,9H-Cyclo­octa­[d][1,2,3]selena­diazol-7-one

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aUniversity of Mainz, Department of Chemistry, Duesbergweg 10-14, 55099 Mainz, Germany
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 28 October 2026; accepted 2 November 2026; online 6 November 2026)

In the title compound, C8H10N2OSe, an almost planar 1,2,3-selena­diazole ring is annulated to a cyclo­octenone ring with a twist-boat conformation. The heterocycle and C—C(=O)—C carbonyl moieties subtend a dihedral angle of 54.25 (11)°. In the extended structure, weak C—H⋯O and C—H⋯N inter­actions link the mol­ecules into double layers lying parallel to the bc plane.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

The title compound, C8H10N2OSe (I) (Fig. 1[link]), was prepared in a project on medium sized rings with geometrical strain (Bissinger et al. 1988View full citation; Detert & Meier, 1997aView full citation,bView full citation). 1,2,3-Selena­diazo­les are important precursors for the synthesis of strained cyclo­alkynes (Yalpani et al. 1971View full citation; Meier & Voigt,1972View full citation). The title compound had been prepared for the first synthesis of cyclo­octynone (Meier & Petersen, 1978View full citation). The crystal structures of related cyclo­octeno-1,2,3-selana­diazo­les have been reported recently (Schollmeyer & Detert, 2020View full citation, 2025View full citation). The C4/C8/N7/N6/Se5 selena­diazole ring in (I) is planar to within 0.0044 (2) Å and the C2—C1(=O12)—C11 carbonyl moiety to within 0.004 (2) Å at C1; these planes subtend a dihedral angle of 54.25 (11)°. Further characteristics are a dihedral angle of 3.51 (19)° for the selena­diazole C4/C8 fragment and its adjacent methyl­ene C atoms (C3—C4—C8—C9) and a twist-boat conformation of the cyclo­octene ring.

[Figure 1]
Figure 1
The mol­ecular structure of (I) with displacement ellipsoids drawn at the 50% probability level.

In the extended structure of (I), the mol­ecules are connected via weak C—H⋯O and C—H⋯N hydrogen bonds with H⋯X (X = O, N) lengths of 2.58 to 2.68 Å (Table 1[link], Fig. 2[link]). These bridges connect the mol­ecules into a double-layer system with the layers lying parallel to the bc plane. Within one layer, the mol­ecules are related by translation symmetry along the b axis and a c glide plane; a centre of inversion connects mol­ecules of both layers, as centrosymmetric dimers are formed. While the C—H⋯O and C—H⋯N hydrogen bonds are within a layer and connect the double layer, the selena­diazole rings are on both surfaces of this subsystem.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A D⋯A D—H⋯A
C2—H2B⋯O12i 0.99 2.58 3.339 (3) 133
C3—H3A⋯N7ii 0.99 2.68 3.473 (3) 138
C9—H9A⋯O12iii 0.99 2.65 3.608 (3) 162
C9—H9B⋯N7ii 0.99 2.64 3.547 (3) 152
C10—H10B⋯O12iv 0.99 2.63 3.461 (3) 142
C11—H11A⋯O12i 0.99 2.63 3.467 (3) 143
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 2]
Figure 2
Partial packing diagram of (I) viewed along the b-axis direction. Hydrogen bonds are shown as dashed lines.

Synthesis and crystallization

The synthesis of the title compound was performed according to the literature (Meier & Petersen, 1978View full citation) from cyclo­octa­diene-1,5 via hydro­boration/oxidation, partial oxidation of the diol, transformation of the ketone to a 1,2,3-selena­diazole and oxidation of the remaining alcohol group. After recrystallization from the mixed solvents of chloro­form and propanol-2-ol, colourless blocks with m.p. 371 K were formed. Analytical data are given by Meier and Petersen (1978View full citation), 1H-NMR (400 MHz, CDCl2): δ = 3.45 (m, 2 H), 3.26 (m, 2 H), 2.73 (m, 2 H), 2.47 (m, 2 H), 1.98 (qui, 2 H). 77Se-NMR (73 MHz, CDCl3, SeO2/D2O as reference): δ = 223.7.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C8H10N2OSe
Mr 229.14
Crystal system, space group Monoclinic, P21/c
Temperature (K) 120
a, b, c (Å) 12.7015 (6), 7.2450 (2), 9.7070 (5)
β (°) 90.288 (4)
V (Å3) 893.25 (7)
Z 4
Radiation type Mo Kα
μ (mm−1) 4.16
Crystal size (mm) 0.95 × 0.53 × 0.21
 
Data collection
Diffractometer Stoe IPDS 2T
Absorption correction Integration
Tmin, Tmax 0.071, 0.405
No. of measured, independent and observed [I > 2σ(I)] reflections 4432, 2134, 2070
Rint 0.027
(sin θ/λ)max (Å−1) 0.661
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.031, 0.084, 1.14
No. of reflections 2134
No. of parameters 109
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.47, −0.89
Computer programs: X-AREA WinXpose, X-AREA Recipe and X-AREA Integrate (Stoe, 2020View full citation), SHELXT2014 (Sheldrick, 2015aView full citation), SHELXL2019/2 (Sheldrick, 2015bView full citation) and PLATON (Spek, 2009View full citation).

Structural data


Computing details top

4H,5H,6H,7H,8H,9H-Cycloocta[d][1,2,3]selenadiazol-7-one top
Crystal data top
C8H10N2OSeDx = 1.704 Mg m−3
Mr = 229.14Melting point: 371 K
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 12.7015 (6) ÅCell parameters from 8908 reflections
b = 7.2450 (2) Åθ = 2.6–28.6°
c = 9.7070 (5) ŵ = 4.16 mm−1
β = 90.288 (4)°T = 120 K
V = 893.25 (7) Å3Block, colorless
Z = 40.95 × 0.53 × 0.21 mm
F(000) = 456
Data collection top
Stoe IPDS 2T
diffractometer
2070 reflections with I > 2σ(I)
Detector resolution: 6.67 pixels mm-1Rint = 0.027
rotation method, ω scansθmax = 28.0°, θmin = 3.2°
Absorption correction: integrationh = −16→16
Tmin = 0.071, Tmax = 0.405k = −9→9
4432 measured reflectionsl = −11→12
2134 independent reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.031H-atom parameters constrained
wR(F2) = 0.084 w = 1/[σ2(Fo2) + (0.0513P)2 + 0.6455P]
where P = (Fo2 + 2Fc2)/3
S = 1.14(Δ/σ)max = 0.001
2134 reflectionsΔρmax = 0.47 e Å−3
109 parametersΔρmin = −0.89 e Å−3
0 restraints
Special details top

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. Hydrogen atoms attached to carbons were placed at calculated positions and were refined in the riding-model approximation with C—H = 0.99 Å, and with Uiso(H) = 1.2 Ueq(C).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.17825 (15)0.2685 (3)0.3378 (2)0.0186 (4)
C20.27398 (16)0.2237 (3)0.4249 (2)0.0185 (4)
H2A0.3171870.1298930.3772090.022*
H2B0.2510560.1708100.5139220.022*
C30.34108 (16)0.3969 (3)0.4520 (2)0.0179 (4)
H3A0.3033700.4801590.5157850.022*
H3B0.4084260.3606620.4961120.022*
C40.36298 (15)0.4966 (3)0.3194 (2)0.0162 (4)
Se50.47241 (2)0.43962 (3)0.20325 (2)0.01750 (10)
N60.41692 (15)0.6158 (3)0.08121 (18)0.0211 (4)
N70.33379 (14)0.6881 (2)0.13071 (18)0.0204 (3)
C80.30090 (16)0.6286 (3)0.2587 (2)0.0177 (4)
C90.20190 (17)0.7117 (3)0.3166 (2)0.0208 (4)
H9A0.1891330.8319630.2710530.025*
H9B0.2129060.7357490.4160320.025*
C100.10337 (17)0.5907 (3)0.2989 (2)0.0222 (4)
H10A0.0975470.5533330.2010220.027*
H10B0.0405000.6655790.3210890.027*
C110.10277 (17)0.4157 (3)0.3892 (2)0.0204 (4)
H11A0.1223050.4496940.4847770.024*
H11B0.0305930.3642050.3909150.024*
O120.16234 (13)0.1908 (2)0.22902 (17)0.0251 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0176 (9)0.0184 (9)0.0198 (9)−0.0023 (7)0.0034 (7)0.0011 (7)
C20.0202 (9)0.0165 (9)0.0188 (9)0.0017 (7)0.0022 (7)0.0028 (7)
C30.0184 (9)0.0207 (9)0.0147 (8)0.0011 (7)−0.0005 (7)0.0003 (7)
C40.0163 (9)0.0163 (9)0.0159 (8)−0.0007 (7)−0.0016 (7)−0.0001 (7)
Se50.01565 (14)0.01792 (15)0.01893 (14)−0.00037 (6)0.00089 (9)0.00129 (6)
N60.0239 (9)0.0198 (8)0.0195 (8)−0.0040 (7)−0.0010 (7)0.0037 (7)
N70.0231 (8)0.0181 (8)0.0200 (8)−0.0025 (6)−0.0021 (7)0.0037 (6)
C80.0203 (9)0.0152 (9)0.0176 (9)−0.0014 (7)−0.0028 (7)0.0010 (7)
C90.0215 (10)0.0173 (9)0.0237 (9)0.0059 (7)−0.0026 (8)−0.0003 (8)
C100.0170 (10)0.0250 (9)0.0245 (10)0.0058 (8)−0.0007 (8)0.0002 (8)
C110.0152 (9)0.0247 (10)0.0212 (10)0.0030 (7)0.0019 (7)−0.0004 (7)
O120.0256 (8)0.0265 (8)0.0232 (7)−0.0025 (6)0.0001 (6)−0.0048 (6)
Geometric parameters (Å, º) top
C1—O121.213 (3)N6—N71.275 (3)
C1—C21.513 (3)N7—C81.381 (3)
C1—C111.520 (3)C8—C91.506 (3)
C2—C31.539 (3)C9—C101.537 (3)
C2—H2A0.9900C9—H9A0.9900
C2—H2B0.9900C9—H9B0.9900
C3—C41.503 (3)C10—C111.542 (3)
C3—H3A0.9900C10—H10A0.9900
C3—H3B0.9900C10—H10B0.9900
C4—C81.371 (3)C11—H11A0.9900
C4—Se51.8410 (19)C11—H11B0.9900
Se5—N61.8766 (19)
O12—C1—C2121.13 (19)C4—C8—N7115.38 (18)
O12—C1—C11120.60 (19)C4—C8—C9126.73 (18)
C2—C1—C11118.27 (17)N7—C8—C9117.89 (18)
C1—C2—C3111.31 (16)C8—C9—C10114.28 (17)
C1—C2—H2A109.4C8—C9—H9A108.7
C3—C2—H2A109.4C10—C9—H9A108.7
C1—C2—H2B109.4C8—C9—H9B108.7
C3—C2—H2B109.4C10—C9—H9B108.7
H2A—C2—H2B108.0H9A—C9—H9B107.6
C4—C3—C2110.52 (17)C9—C10—C11114.31 (18)
C4—C3—H3A109.5C9—C10—H10A108.7
C2—C3—H3A109.5C11—C10—H10A108.7
C4—C3—H3B109.5C9—C10—H10B108.7
C2—C3—H3B109.5C11—C10—H10B108.7
H3A—C3—H3B108.1H10A—C10—H10B107.6
C8—C4—C3126.52 (18)C1—C11—C10112.67 (17)
C8—C4—Se5109.12 (14)C1—C11—H11A109.1
C3—C4—Se5124.05 (14)C10—C11—H11A109.1
C4—Se5—N687.23 (8)C1—C11—H11B109.1
N7—N6—Se5110.53 (14)C10—C11—H11B109.1
N6—N7—C8117.74 (18)H11A—C11—H11B107.8
O12—C1—C2—C3122.5 (2)C3—C4—C8—C94.8 (3)
C11—C1—C2—C3−56.7 (2)Se5—C4—C8—C9178.63 (17)
C1—C2—C3—C4−50.3 (2)N6—N7—C8—C40.3 (3)
C2—C3—C4—C887.7 (2)N6—N7—C8—C9−179.16 (19)
C2—C3—C4—Se5−85.2 (2)C4—C8—C9—C10−79.8 (3)
C8—C4—Se5—N60.78 (15)N7—C8—C9—C1099.6 (2)
C3—C4—Se5—N6174.77 (17)C8—C9—C10—C1170.4 (2)
C4—Se5—N6—N7−0.63 (15)O12—C1—C11—C10−67.1 (3)
Se5—N6—N7—C80.3 (2)C2—C1—C11—C10112.1 (2)
C3—C4—C8—N7−174.62 (19)C9—C10—C11—C1−73.7 (2)
Se5—C4—C8—N7−0.8 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2A···Se5i0.993.114.025 (2)154
C2—H2B···O12ii0.992.583.339 (3)133
C3—H3A···N7iii0.992.683.473 (3)138
C3—H3B···Se5ii0.993.073.825 (2)134
C9—H9A···O12iv0.992.653.608 (3)162
C9—H9B···N7iii0.992.643.547 (3)152
C10—H10B···O12v0.992.633.461 (3)142
C11—H11A···O12ii0.992.633.467 (3)143
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) x, −y+1/2, z+1/2; (iii) x, −y+3/2, z+1/2; (iv) x, y+1, z; (v) −x, y+1/2, −z+1/2.
 

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