supplementary materials


bi2220 scheme

Acta Cryst. (2007). E63, o3941    [ doi:10.1107/S1600536807038731 ]

(4'S)-4'-Ethyl-3',10'-dioxo-3',4',7',8'-tetrahydrospiro[1,3-dioxolane-2,6'-1'H,6'H-pyrano[3,4-f]indolizin]-4'-yl N-(1-phenylethyl)carbamate

Y. Bao, F.-E. Chen and M.-Q. Chen

Abstract top

The title compound, C24H26N2O7, is an intermediate in the resolution of a tertiary alcohol using a chiral isocyanate reagent. On the basis of the unchanging S configuration of the chiral C atom introduced by the isocyanate reagent, the chiral centre on the tricyclo ring system is shown to adopt an S configuration. In the crystal structure, N-H...O hydrogen bonds link the molecules into chains.

Comment top

The method for resolution of a tertiary alcohol using a chiral isocyanate reagent has been widely applied (Gibbs et al., 1989). The title compound is a key intermediate in the resolution process of alcohol 1 using the (S)-isocyanate 2 (Scheme 2).

On the basis of the unchanging S configuration of C17, the molecular structure (Figure 1) indicates that the chiral C atom C3 adopts an S configuration. The six-membered lactone ring is twisted with an O1/C2/C3/C4 torsion angle of −21.4 (3) °. The pyrrole ring is also twisted, with a N1/C6/C7/C8 torsion angle of 22.3 (2) °. N—H···O hydrogen bonds exist between molecules, linking them into chains along the c axis.

Related literature top

For related literature, see: Duggan & Imagire (1989); Gibbs et al. (1989).

Experimental top

The (S)-isocyanate 2 (2.0 mmol) was added to a mixture of alcohol 1 (1.0 mmol) and reagent grade CuCl (0.2 mmol) in dry CH2Cl2 (12 ml) at room temperature (Scheme 2; Duggan & Imagire, 1989). After stirring for 12 h, the reaction mixture was filtered and the filtrate was diluted with CH2Cl2 (20 ml), washed with H2O (20 ml) and brine (20 ml), dried over MgSO4 and concentrated. The crude product (0.43 g, 94%) was recrystallized from 2-propanol (31 ml) to yield a white powder (m.p. 485 K). Crystals suitable for X-ray analysis were obtained from ethyl acetate.

Refinement top

All H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H distances in the range 0.93–0.98 Å and N—H = 0.88 Å, and with Uiso(H) = 1.5Ueq(C) for methyl H atoms and 1.2Ueq(C) for other H atoms. The methyl groups were allowed to rotate about their local threefold axes. In the absence of significant anomalous scattering effects, Friedel pairs have been merged as equivalent data. The absolute structure was assigned on the basis of the unchanging chiral centre C17, originating from the isocyanate reactant.

Computing details top

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

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound showing displacement ellipsoids at 30% probability for non-H atoms.
[Figure 2] Fig. 2. Unit-cell contents viewed along the b axis.
[Figure 3] Fig. 3. The formation of the title compound.
(4'S)-4'-Ethyl-3',10'-dioxo-3',4',7',8'-tetrahydrospiro[1,3-dioxolane-2,6'- 1'H,6'H-pyrano[3,4-f]indolizin]-4'-yl N-(1-phenylethyl)carbamate top
Crystal data top
C24H26N2O7F000 = 480
Mr = 454.47Dx = 1.352 Mg m3
Monoclinic, P21Mo Kα radiation
λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 2722 reflections
a = 7.3998 (10) Åθ = 2.2–25.4º
b = 16.383 (2) ŵ = 0.10 mm1
c = 9.2162 (13) ÅT = 296 (2) K
β = 92.322 (2)ºPrism, colourless
V = 1116.4 (3) Å30.30 × 0.25 × 0.20 mm
Z = 2
Data collection top
Bruker SMART APEX II CCD
diffractometer
2612 independent reflections
Radiation source: fine-focus sealed tube2352 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.023
T = 296(2) Kθmax = 27.5º
φ and ω scansθmin = 2.2º
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 8→9
Tmin = 0.971, Tmax = 0.980k = 18→21
7148 measured reflectionsl = 9→11
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full  w = 1/[σ2(Fo2) + (0.0485P)2 + 0.0587P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.034(Δ/σ)max < 0.001
wR(F2) = 0.087Δρmax = 0.21 e Å3
S = 1.06Δρmin = 0.13 e Å3
2612 reflectionsExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
302 parametersExtinction coefficient: 0.015 (3)
1 restraintAbsolute structure: Friedel pairs merged as equivalent data
Primary atom site location: structure-invariant direct methodsFlack parameter: ?
Secondary atom site location: difference Fourier mapRogers parameter: ?
Hydrogen site location: inferred from neighbouring sites
Crystal data top
C24H26N2O7V = 1116.4 (3) Å3
Mr = 454.47Z = 2
Monoclinic, P21Mo Kα
a = 7.3998 (10) ŵ = 0.10 mm1
b = 16.383 (2) ÅT = 296 (2) K
c = 9.2162 (13) Å0.30 × 0.25 × 0.20 mm
β = 92.322 (2)º
Data collection top
Bruker SMART APEX II CCD
diffractometer
2612 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2352 reflections with I > 2σ(I)
Tmin = 0.971, Tmax = 0.980Rint = 0.023
7148 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.087Δρmax = 0.21 e Å3
S = 1.06Δρmin = 0.13 e Å3
2612 reflectionsAbsolute structure: Friedel pairs merged as equivalent data
302 parametersFlack parameter: ?
1 restraintRogers parameter: ?
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 > 2sigma(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
O10.9756 (3)0.86809 (10)0.37052 (17)0.0497 (4)
O21.0016 (3)0.90832 (11)0.14679 (19)0.0571 (5)
O30.8961 (2)0.75590 (10)0.03780 (15)0.0361 (3)
O40.6197 (2)0.46524 (11)0.2027 (2)0.0518 (4)
O50.8933 (2)0.44686 (10)0.31575 (17)0.0438 (4)
O60.8228 (2)0.68765 (11)0.66980 (16)0.0445 (4)
O71.1799 (2)0.74245 (12)0.13801 (17)0.0483 (4)
N10.7652 (2)0.59843 (11)0.48365 (19)0.0342 (4)
N21.1043 (3)0.69448 (13)0.0887 (2)0.0429 (5)
H21.01380.69190.15380.043 (7)*
C10.9037 (3)0.81619 (15)0.4800 (2)0.0415 (5)
H1A0.80130.84340.52120.050*
H1B0.99530.80900.55730.050*
C20.9466 (3)0.85775 (14)0.2281 (2)0.0395 (5)
C30.8317 (3)0.78525 (13)0.1735 (2)0.0337 (4)
C40.8214 (3)0.71695 (12)0.2830 (2)0.0314 (4)
C50.7784 (3)0.63660 (14)0.2365 (2)0.0343 (4)
H50.76610.62380.13830.041*
C60.7561 (3)0.57932 (13)0.3391 (2)0.0331 (4)
C70.7254 (3)0.48743 (13)0.3259 (3)0.0382 (5)
C80.6437 (3)0.46579 (16)0.4706 (3)0.0479 (6)
H8A0.51270.46820.46250.057*
H8B0.67980.41130.50120.057*
C90.7175 (3)0.52940 (15)0.5779 (3)0.0442 (6)
H9A0.62650.54530.64540.053*
H9B0.82300.50900.63230.053*
C100.8130 (3)0.67425 (14)0.5379 (2)0.0342 (4)
C110.8446 (3)0.73440 (13)0.4266 (2)0.0326 (4)
C120.9214 (4)0.43939 (19)0.1647 (3)0.0581 (7)
H12A0.99340.39150.14470.070*
H12B0.98150.48730.12810.070*
C130.7343 (5)0.4315 (2)0.0987 (3)0.0685 (9)
H13A0.72300.46130.00780.082*
H13B0.70460.37460.08040.082*
C140.6397 (3)0.81741 (16)0.1294 (2)0.0432 (5)
H14A0.64880.85180.04440.052*
H14B0.56400.77120.10180.052*
C150.5467 (3)0.86541 (17)0.2454 (3)0.0510 (6)
H15A0.61080.91550.26380.076*
H15B0.54560.83380.33300.076*
H15C0.42470.87730.21270.076*
C161.0725 (3)0.73094 (14)0.0376 (2)0.0357 (5)
C171.2862 (3)0.66796 (18)0.1258 (3)0.0493 (6)
H171.36940.71380.10830.059*
C181.3521 (6)0.5967 (3)0.0323 (3)0.0880 (13)
H18A1.26450.55350.03830.132*
H18B1.36800.61430.06680.132*
H18C1.46530.57740.06620.132*
C191.2817 (3)0.64878 (15)0.2861 (2)0.0378 (5)
C201.2066 (3)0.57611 (15)0.3382 (2)0.0424 (5)
H201.16240.53830.27320.051*
C211.1968 (4)0.55937 (18)0.4847 (3)0.0517 (7)
H211.14850.51000.51750.062*
C221.2572 (4)0.6144 (2)0.5813 (3)0.0611 (8)
H221.24880.60300.68030.073*
C231.3300 (4)0.6861 (2)0.5336 (3)0.0696 (9)
H231.37130.72370.60030.084*
C241.3436 (4)0.70394 (18)0.3862 (3)0.0558 (7)
H241.39450.75310.35470.067*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0722 (12)0.0424 (9)0.0346 (8)0.0192 (9)0.0029 (8)0.0057 (7)
O20.0855 (14)0.0408 (9)0.0462 (10)0.0161 (10)0.0177 (9)0.0003 (8)
O30.0421 (8)0.0407 (8)0.0254 (7)0.0030 (7)0.0020 (6)0.0044 (6)
O40.0513 (9)0.0465 (10)0.0567 (11)0.0033 (8)0.0082 (8)0.0087 (8)
O50.0487 (9)0.0429 (9)0.0396 (8)0.0118 (7)0.0007 (7)0.0048 (7)
O60.0530 (9)0.0532 (10)0.0274 (8)0.0067 (8)0.0001 (7)0.0026 (7)
O70.0462 (9)0.0642 (12)0.0339 (8)0.0019 (8)0.0043 (7)0.0097 (8)
N10.0365 (9)0.0356 (10)0.0306 (9)0.0042 (8)0.0044 (7)0.0025 (7)
N20.0400 (10)0.0571 (13)0.0313 (9)0.0084 (9)0.0022 (8)0.0104 (9)
C10.0527 (13)0.0394 (12)0.0324 (11)0.0061 (11)0.0010 (10)0.0039 (10)
C20.0478 (12)0.0348 (12)0.0363 (12)0.0035 (10)0.0083 (10)0.0043 (10)
C30.0405 (11)0.0331 (10)0.0274 (10)0.0012 (9)0.0020 (8)0.0041 (8)
C40.0326 (10)0.0323 (10)0.0295 (10)0.0019 (8)0.0021 (8)0.0033 (8)
C50.0413 (11)0.0341 (11)0.0274 (10)0.0003 (9)0.0010 (8)0.0046 (8)
C60.0326 (10)0.0322 (11)0.0344 (11)0.0026 (8)0.0008 (8)0.0044 (9)
C70.0394 (11)0.0310 (11)0.0441 (13)0.0014 (9)0.0010 (9)0.0002 (9)
C80.0508 (13)0.0394 (13)0.0545 (15)0.0010 (11)0.0133 (11)0.0048 (11)
C90.0528 (14)0.0399 (12)0.0408 (13)0.0058 (11)0.0130 (10)0.0095 (10)
C100.0339 (10)0.0393 (11)0.0295 (10)0.0065 (9)0.0019 (8)0.0020 (9)
C110.0343 (10)0.0357 (11)0.0278 (10)0.0018 (9)0.0016 (8)0.0045 (8)
C120.0686 (18)0.0605 (17)0.0456 (14)0.0120 (14)0.0076 (13)0.0118 (13)
C130.087 (2)0.0624 (19)0.0550 (16)0.0104 (16)0.0080 (15)0.0230 (15)
C140.0458 (12)0.0446 (13)0.0390 (12)0.0085 (10)0.0000 (10)0.0004 (10)
C150.0477 (13)0.0490 (14)0.0567 (15)0.0068 (12)0.0083 (11)0.0009 (12)
C160.0439 (11)0.0357 (11)0.0276 (10)0.0011 (9)0.0021 (9)0.0009 (9)
C170.0441 (13)0.0624 (17)0.0411 (13)0.0119 (11)0.0027 (10)0.0115 (12)
C180.110 (3)0.115 (3)0.0382 (15)0.065 (3)0.0092 (16)0.0031 (17)
C190.0324 (10)0.0446 (13)0.0365 (12)0.0058 (9)0.0046 (8)0.0024 (10)
C200.0445 (12)0.0438 (13)0.0390 (12)0.0037 (10)0.0025 (10)0.0011 (10)
C210.0482 (14)0.0552 (15)0.0512 (15)0.0099 (12)0.0054 (11)0.0172 (12)
C220.0525 (15)0.092 (2)0.0383 (14)0.0138 (15)0.0034 (12)0.0036 (14)
C230.0656 (18)0.093 (3)0.0515 (17)0.0036 (18)0.0146 (14)0.0258 (17)
C240.0545 (15)0.0497 (15)0.0633 (18)0.0088 (12)0.0033 (13)0.0010 (13)
Geometric parameters (Å, °) top
O1—C21.333 (3)C9—H9A0.970
O1—C11.438 (3)C9—H9B0.970
O2—C21.199 (3)C10—C111.448 (3)
O3—C161.369 (3)C12—C131.495 (5)
O3—C31.439 (2)C12—H12A0.970
O4—C71.400 (3)C12—H12B0.970
O4—C131.419 (4)C13—H13A0.970
O5—C71.416 (3)C13—H13B0.970
O5—C121.421 (3)C14—C151.515 (3)
O6—C101.235 (3)C14—H14A0.970
O7—C161.210 (3)C14—H14B0.970
N1—C61.368 (3)C15—H15A0.960
N1—C101.380 (3)C15—H15B0.960
N1—C91.478 (3)C15—H15C0.960
N2—C161.337 (3)C17—C191.510 (3)
N2—C171.468 (3)C17—C181.519 (4)
N2—H20.88C17—H170.980
C1—C111.487 (3)C18—H18A0.960
C1—H1A0.970C18—H18B0.960
C1—H1B0.970C18—H18C0.960
C2—C31.534 (3)C19—C241.382 (4)
C3—C41.511 (3)C19—C201.391 (3)
C3—C141.553 (3)C20—C211.377 (3)
C4—C111.358 (3)C20—H200.930
C4—C51.417 (3)C21—C221.356 (4)
C5—C61.347 (3)C21—H210.930
C5—H50.930C22—C231.359 (5)
C6—C71.527 (3)C22—H220.930
C7—C81.528 (3)C23—C241.390 (4)
C8—C91.523 (4)C23—H230.930
C8—H8A0.970C24—H240.930
C8—H8B0.970
C2—O1—C1124.53 (18)O5—C12—C13103.7 (2)
C16—O3—C3116.79 (16)O5—C12—H12A111.0
C7—O4—C13108.6 (2)C13—C12—H12A111.0
C7—O5—C12105.57 (19)O5—C12—H12B111.0
C6—N1—C10124.12 (18)C13—C12—H12B111.0
C6—N1—C9113.22 (18)H12A—C12—H12B109.0
C10—N1—C9122.67 (18)O4—C13—C12105.1 (2)
C16—N2—C17122.03 (19)O4—C13—H13A110.7
C16—N2—H2117.3C12—C13—H13A110.7
C17—N2—H2120.3O4—C13—H13B110.7
O1—C1—C11114.38 (17)C12—C13—H13B110.7
O1—C1—H1A108.7H13A—C13—H13B108.8
C11—C1—H1A108.7C15—C14—C3115.36 (19)
O1—C1—H1B108.7C15—C14—H14A108.4
C11—C1—H1B108.7C3—C14—H14A108.4
H1A—C1—H1B107.6C15—C14—H14B108.4
O2—C2—O1118.8 (2)C3—C14—H14B108.4
O2—C2—C3121.9 (2)H14A—C14—H14B107.5
O1—C2—C3119.10 (18)C14—C15—H15A109.5
O3—C3—C4111.14 (17)C14—C15—H15B109.5
O3—C3—C2110.17 (16)H15A—C15—H15B109.5
C4—C3—C2113.39 (17)C14—C15—H15C109.5
O3—C3—C14102.54 (16)H15A—C15—H15C109.5
C4—C3—C14110.84 (18)H15B—C15—H15C109.5
C2—C3—C14108.18 (18)O7—C16—N2127.0 (2)
C11—C4—C5120.59 (19)O7—C16—O3123.32 (19)
C11—C4—C3119.16 (18)N2—C16—O3109.65 (18)
C5—C4—C3120.17 (18)N2—C17—C19107.78 (18)
C6—C5—C4117.85 (19)N2—C17—C18111.8 (3)
C6—C5—H5121.1C19—C17—C18112.9 (2)
C4—C5—H5121.1N2—C17—H17108.1
C5—C6—N1121.5 (2)C19—C17—H17108.1
C5—C6—C7130.8 (2)C18—C17—H17108.1
N1—C6—C7107.74 (18)C17—C18—H18A109.5
O4—C7—O5106.74 (19)C17—C18—H18B109.5
O4—C7—C6113.41 (19)H18A—C18—H18B109.5
O5—C7—C6109.87 (18)C17—C18—H18C109.5
O4—C7—C8114.8 (2)H18A—C18—H18C109.5
O5—C7—C8109.14 (19)H18B—C18—H18C109.5
C6—C7—C8102.82 (19)C24—C19—C20117.9 (2)
C9—C8—C7105.3 (2)C24—C19—C17121.5 (2)
C9—C8—H8A110.7C20—C19—C17120.6 (2)
C7—C8—H8A110.7C21—C20—C19120.9 (2)
C9—C8—H8B110.7C21—C20—H20119.6
C7—C8—H8B110.7C19—C20—H20119.6
H8A—C8—H8B108.8C22—C21—C20120.4 (3)
N1—C9—C8103.28 (19)C22—C21—H21119.8
N1—C9—H9A111.1C20—C21—H21119.8
C8—C9—H9A111.1C21—C22—C23119.9 (3)
N1—C9—H9B111.1C21—C22—H22120.0
C8—C9—H9B111.1C23—C22—H22120.0
H9A—C9—H9B109.1C22—C23—C24120.7 (3)
O6—C10—N1121.4 (2)C22—C23—H23119.6
O6—C10—C11124.9 (2)C24—C23—H23119.6
N1—C10—C11113.73 (18)C19—C24—C23120.1 (3)
C4—C11—C10121.9 (2)C19—C24—H24119.9
C4—C11—C1122.42 (19)C23—C24—H24119.9
C10—C11—C1115.64 (17)
C2—O1—C1—C1119.3 (3)C6—N1—C9—C89.5 (2)
C1—O1—C2—O2174.3 (2)C10—N1—C9—C8170.22 (18)
C1—O1—C2—C31.0 (3)C7—C8—C9—N123.0 (2)
C16—O3—C3—C468.2 (2)C6—N1—C10—O6178.39 (19)
C16—O3—C3—C258.3 (2)C9—N1—C10—O61.9 (3)
C16—O3—C3—C14173.30 (18)C6—N1—C10—C113.0 (3)
O2—C2—C3—O338.1 (3)C9—N1—C10—C11176.68 (18)
O1—C2—C3—O3146.7 (2)C5—C4—C11—C105.0 (3)
O2—C2—C3—C4163.4 (2)C3—C4—C11—C10171.69 (18)
O1—C2—C3—C421.4 (3)C5—C4—C11—C1175.1 (2)
O2—C2—C3—C1473.2 (3)C3—C4—C11—C18.2 (3)
O1—C2—C3—C14102.0 (2)O6—C10—C11—C4176.1 (2)
O3—C3—C4—C11150.41 (18)N1—C10—C11—C42.5 (3)
C2—C3—C4—C1125.7 (3)O6—C10—C11—C13.8 (3)
C14—C3—C4—C1196.2 (2)N1—C10—C11—C1177.63 (18)
O3—C3—C4—C532.9 (3)O1—C1—C11—C414.4 (3)
C2—C3—C4—C5157.67 (18)O1—C1—C11—C10165.72 (18)
C14—C3—C4—C580.4 (2)C7—O5—C12—C1331.7 (3)
C11—C4—C5—C62.0 (3)C7—O4—C13—C123.3 (3)
C3—C4—C5—C6174.58 (19)O5—C12—C13—O421.5 (3)
C4—C5—C6—N13.3 (3)O3—C3—C14—C15170.4 (2)
C4—C5—C6—C7174.3 (2)C4—C3—C14—C1570.9 (3)
C10—N1—C6—C56.0 (3)C2—C3—C14—C1554.0 (3)
C9—N1—C6—C5173.7 (2)C17—N2—C16—O74.6 (4)
C10—N1—C6—C7172.05 (18)C17—N2—C16—O3174.3 (2)
C9—N1—C6—C78.3 (2)C3—O3—C16—O710.1 (3)
C13—O4—C7—O516.4 (3)C3—O3—C16—N2170.89 (18)
C13—O4—C7—C6104.7 (2)C16—N2—C17—C19166.5 (2)
C13—O4—C7—C8137.5 (2)C16—N2—C17—C1868.9 (3)
C12—O5—C7—O430.5 (3)N2—C17—C19—C2499.6 (3)
C12—O5—C7—C692.8 (2)C18—C17—C19—C24136.5 (3)
C12—O5—C7—C8155.1 (2)N2—C17—C19—C2077.4 (3)
C5—C6—C7—O435.3 (3)C18—C17—C19—C2046.5 (3)
N1—C6—C7—O4146.85 (19)C24—C19—C20—C210.9 (4)
C5—C6—C7—O584.0 (3)C17—C19—C20—C21177.9 (2)
N1—C6—C7—O593.8 (2)C19—C20—C21—C221.3 (4)
C5—C6—C7—C8159.9 (2)C20—C21—C22—C230.8 (4)
N1—C6—C7—C822.3 (2)C21—C22—C23—C240.0 (5)
O4—C7—C8—C9151.2 (2)C20—C19—C24—C230.0 (4)
O5—C7—C8—C989.0 (2)C17—C19—C24—C23177.1 (3)
C6—C7—C8—C927.6 (2)C22—C23—C24—C190.4 (5)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2···O6i0.882.112.988 (2)173
Symmetry codes: (i) x, y, z−1.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N2—H2···O6i0.882.112.988 (2)173
Symmetry codes: (i) x, y, z−1.
references
References top

Bruker (1997). SMART (Version 5.611), SAINT (Version 6.0) and SHELXTL (Version 5.10). Bruker AXS Inc., Madison, Wisconsin, USA.

Duggan, M. E. & Imagire, J. S. (1989). Synthesis, 2, 131–132.

Gibbs, R. A., Bartels, K., Lee, R. W. K. & Okamura, W. H. (1989). J. Am. Chem. Soc. 111, 3717–3725.

Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.

Sheldrick, G. M. (1997). SHELXL97 and SHELXS97. University of Göttingen, Germany.