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The crystal structures of six industrially produced benzimidazolone pigments [Pigment Orange 36 (β phase), Pigment Orange 62, Pigment Yellow 151, Pigment Yellow 154 (α phase), Pigment Yellow 181 (β phase) and Pigment Yellow 194] were determined from laboratory X-ray powder diffraction data by means of real-space methods using the programs DASH and MRIA, respectively. Subsequent Rietveld refinements were carried out with TOPAS. The crystal phases correspond to those produced industrially. Additionally, the crystal structures of the non-commercial compound `BIRZIL' (a chloro derivative of Pigment Yellow 194) and of a dimethylsulfoxide solvate of Pigment Yellow 154 were determined by single-crystal structure analyses. All eight crystal structures are different; the six industrial pigments even exhibit five different hydrogen-bond topologies. Apparently, the good application properties of the benzimidazolone pigments are not the result of one specific hydrogen-bonding pattern, but are the result of a combination of efficient molecular packing and strong intermolecular hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108768108041529/og5035sup1.cif
Contains datablocks BIRZIL, PY154-DMSO, global, PO36, PO62, PY151, PY154, PY181, PY194

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035BIRZILsup2.hkl
Contains datablock BIRZIL

fcf

Structure factor file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PY154-DMSOsup3.fcf
Contains datablock PY154-DMSO

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PO36sup4.rtv
Contains datablock PO36

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PO62sup5.rtv
Contains datablock PO62

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PY151sup6.rtv
Contains datablock PY151

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PY154sup7.rtv
Contains datablock PY154

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PY181sup8.rtv
Contains datablock PY181

rtv

Rietveld powder data file (CIF format) https://doi.org/10.1107/S0108768108041529/og5035PY194sup9.rtv
Contains datablock PY194

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S0108768108041529/og5035sup10.pdf
Extra tables and figures

CCDC references: 737339; 737340; 737341; 737342; 737343; 737344; 737346

Computing details top

Data collection: STOE WINXPOW (STOE & CIE GmbH, 2004) for PO36, PO62, PY151, PY154, PY181, PY194; Nicolet software for BIRZIL; X-AREA (Stoe & Cie, 2001) for PY154-DMSO. Cell refinement: TOPAS (Coelho, 2006) for PO36, PO62, PY151, PY154, PY181, PY194; Nicolet software for BIRZIL; X-AREA (Stoe & Cie, 2001) for PY154-DMSO. Data reduction: DASH (David et al., 2006) for PO36, PO62, PY151, PY154, PY181, PY194; Nicolet software for BIRZIL; X-AREA (Stoe & Cie, 2001) for PY154-DMSO. Program(s) used to solve structure: DASH (David et al., 2006) for PO36, PO62, PY151, PY154, PY181, PY194; SHELXS97 (Sheldrick, 1990) for BIRZIL, PY154-DMSO. Program(s) used to refine structure: TOPAS (Coelho, 2006) for PO36, PO62, PY151, PY154, PY181, PY194; SHELXL97 (Sheldrick, 1997) for BIRZIL, PY154-DMSO. Molecular graphics: Mercury (Macrae et al., 2006) for PO36, PO62, PY151, PY154, PY181, PY194; SHELX97 (Sheldrick, 1997) for BIRZIL; XP in SHELXTL-Plus (Sheldrick, 1991) for PY154-DMSO. Software used to prepare material for publication: DASH, TOPAS, Mercury for PO36, PO62, PY151, PY154, PY181, PY194; SHELX97 (Sheldrick, 1997) for BIRZIL; SHELXL97 for PY154-DMSO.

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
[Figure 4]
[Figure 5]
[Figure 6]
[Figure 7]
[Figure 8]
[Figure 9]
[Figure 10]
[Figure 11]
[Figure 12]
[Figure 13]
(PO36) top
Crystal data top
C17H13ClN6O5Z = 2
Mr = 416.78F(000) = 428
Triclinic, P1Dx = 1.616 Mg m3
Hall symbol: -P 1Cu Kα1 radiation, λ = 1.54056 Å
a = 8.6533 (7) ŵ = 2.41 mm1
b = 9.1170 (6) ÅT = 293 K
c = 11.3831 (6) ÅParticle morphology: no specific habit
α = 74.717 (2)°orange
β = 81.597 (4)°cylinder, 10 × 0.7 mm
γ = 88.982 (3)°Specimen preparation: Prepared at 293 K and 0.00 kPa
V = 856.78 (10) Å3
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 2.00°, 2θmax = 75.00°, 2θstep = 0.01°
Specimen mounting: 'glass capillary'
Refinement top
Refinement on Inet191 parameters
Least-squares matrix: full with fixed elements per cycle116 restraints
Rp = 0.0290 constraints
Rwp = 0.039H-atom parameters constrained
Rexp = 0.094Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.103(Δ/σ)max = 0.001
9800 data pointsBackground function: Chebyshev polynomial with 20 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C17H13ClN6O5γ = 88.982 (3)°
Mr = 416.78V = 856.78 (10) Å3
Triclinic, P1Z = 2
a = 8.6533 (7) ÅCu Kα1 radiation, λ = 1.54056 Å
b = 9.1170 (6) ŵ = 2.41 mm1
c = 11.3831 (6) ÅT = 293 K
α = 74.717 (2)°cylinder, 10 × 0.7 mm
β = 81.597 (4)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: 'glass capillary'2θmin = 2.00°, 2θmax = 75.00°, 2θstep = 0.01°
Data collection mode: transmission
Refinement top
Rp = 0.0299800 data points
Rwp = 0.039191 parameters
Rexp = 0.094116 restraints
χ2 = 1.103H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.2785 (6)0.2449 (8)0.5094 (8)0.03645
C20.1249 (6)0.1646 (8)0.5732 (9)0.03645
N30.2846 (7)0.3689 (9)0.4220 (8)0.03645
C40.4333 (6)0.1940 (8)0.5449 (8)0.03645
N50.1331 (6)0.0240 (6)0.6486 (6)0.03645
O60.0048 (8)0.2186 (9)0.5406 (10)0.03645
N70.1623 (6)0.4383 (6)0.3810 (5)0.03645
O80.4456 (9)0.0761 (9)0.6222 (9)0.03645
C90.5765 (6)0.2895 (6)0.4751 (5)0.03645
C100.0091 (6)0.0756 (6)0.7174 (5)0.03645
H110.237940.007670.660940.04374
H120.058290.397720.414950.04374
C130.1850 (6)0.5706 (5)0.2850 (4)0.03645
H140.586240.297300.377050.04374
H150.569010.403100.488970.04374
H160.681200.236660.508640.04374
C170.1470 (6)0.0522 (5)0.6988 (5)0.03645
C180.0528 (6)0.2013 (6)0.8064 (5)0.03645
C190.3352 (6)0.6324 (5)0.2434 (3)0.03645
C200.0607 (6)0.6434 (4)0.2284 (4)0.03645
C210.2512 (6)0.1602 (4)0.7745 (3)0.03645
H220.183690.036690.634920.04374
C230.0542 (6)0.3085 (5)0.8821 (5)0.03645
H240.167700.214050.816140.04374
C250.3592 (6)0.7641 (5)0.1468 (3)0.03645
H260.429300.583240.281670.04374
C270.0869 (6)0.7766 (4)0.1312 (3)0.03645
N280.0982 (6)0.5794 (6)0.2718 (5)0.03645
C290.2077 (6)0.2909 (4)0.8683 (3)0.03645
N300.4138 (6)0.1742 (5)0.7834 (5)0.03645
H310.019120.397540.946290.04374
C320.2356 (6)0.8373 (4)0.0902 (4)0.03645
H330.469900.807480.117250.04374
H340.003590.829300.090180.04374
O350.2056 (8)0.6568 (9)0.2139 (8)0.03645
O360.1318 (9)0.4806 (9)0.3634 (7)0.03645
N370.3432 (6)0.3715 (6)0.9251 (4)0.03645
H380.475360.101820.731970.04374
C390.4722 (6)0.3021 (7)0.8737 (5)0.03645
Cl400.2696 (5)1.0008 (5)0.0306 (4)0.04567
H410.350160.464780.990300.04374
O420.6075 (8)0.3435 (9)0.9003 (7)0.03645
Geometric parameters (Å, º) top
C1—C21.518 (7)C18—C231.382 (6)
C1—N31.29 (1)C19—C251.395 (5)
C1—C41.486 (8)C20—C271.408 (4)
C2—N51.347 (8)C20—N281.467 (7)
C2—O61.207 (9)C21—C291.461 (5)
N3—N71.303 (8)C21—N301.402 (7)
C4—C91.520 (7)C23—C291.361 (7)
N5—C101.416 (6)C25—C321.400 (7)
N5—H110.99 (2)C27—C321.375 (7)
N7—C131.392 (6)N28—O351.305 (9)
C9—H141.08 (2)N28—O361.186 (8)
C9—H151.07 (2)C29—N371.374 (6)
C9—H161.08 (2)N30—H380.98 (2)
C10—C171.401 (7)N30—C391.383 (6)
C10—C181.402 (7)C32—Cl401.736 (5)
C13—C191.391 (7)N37—C391.399 (7)
C13—C201.403 (7)N37—H410.98 (2)
C17—C211.372 (6)C39—O421.209 (8)
C2—C1—N3122.0 (5)C25—C19—H26121 (1)
C2—C1—C4123.9 (6)C13—C20—C27120.8 (4)
N3—C1—C4114.0 (5)C13—C20—N28119.2 (3)
C1—C2—N5116.8 (5)C27—C20—N28120.0 (4)
C1—C2—O6118.9 (7)C17—C21—C29124.2 (5)
N5—C2—O6123.3 (6)C17—C21—N30131.0 (4)
C1—N3—N7124.3 (5)C29—C21—N30104.8 (3)
C1—C4—O8120.8 (6)C18—C23—C29118.3 (4)
C1—C4—C9117.7 (5)C18—C23—H31120 (1)
O8—C4—C9121.2 (6)C29—C23—H31122 (1)
C2—N5—C10128.3 (5)C19—C25—C32121.7 (4)
C2—N5—H11116 (1)C19—C25—H33118 (1)
C10—N5—H11116 (1)C32—C25—H33120 (1)
N3—N7—H12120 (1)C20—C27—C32120.3 (4)
N3—N7—C13118.5 (5)C20—C27—H34119 (1)
H12—N7—C13120 (1)C32—C27—H34120 (1)
C4—C9—H14112 (1)C20—N28—O35114.3 (5)
C4—C9—H16108 (1)C20—N28—O36123.3 (6)
H14—C9—H16111 (1)O35—N28—O36121.3 (6)
H15—C9—H16109 (2)C21—C29—C23118.4 (4)
N5—C10—C17123.1 (4)C21—C29—N37106.9 (4)
N5—C10—C18115.3 (5)C23—C29—N37134.6 (4)
C17—C10—C18121.6 (4)C21—N30—C39111.4 (4)
N7—C13—C19119.3 (4)C25—C32—C27118.7 (3)
N7—C13—C20121.8 (4)C25—C32—Cl40120.6 (4)
C19—C13—C20118.8 (3)C27—C32—Cl40120.6 (4)
C10—C17—C21114.8 (4)C29—N37—C39110.9 (4)
C10—C17—H22123 (1)C29—N37—H41127 (1)
C21—C17—H22122 (1)C39—N37—H41122 (1)
C10—C18—C23122.6 (5)N30—C39—N37105.9 (4)
C10—C18—H24118 (1)N30—C39—O42126.0 (6)
C23—C18—H24119 (1)N37—C39—O42128.1 (5)
C13—C19—C25119.7 (4)
(PO62) top
Crystal data top
C17H14N6O5Z = 2
Mr = 382.34F(000) = 396
Triclinic, P1Dx = 1.505 Mg m3
Hall symbol: -P 1Cu Kα1 radiation, λ = 1.54056 Å
a = 7.2689 (8) ŵ = 0.97 mm1
b = 10.3176 (14) ÅT = 293 K
c = 12.1761 (15) ÅParticle morphology: no specific habit
α = 96.462 (6)°orange
β = 95.869 (4)°flat_sheet, 10 × 1.2 mm
γ = 109.849 (8)°Specimen preparation: Prepared at 293 K and 0.00 kPa
V = 843.78 (19) Å3
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 3.00°, 2θmax = 34.00°, 2θstep = 0.02°
Specimen mounting: flat sample holder
Refinement top
Refinement on Inet190 parameters
Least-squares matrix: full with fixed elements per cycle118 restraints
Rp = 0.0300 constraints
Rwp = 0.040H-atom parameters constrained
Rexp = 0.055Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.277(Δ/σ)max = 0.001
1550 data pointsBackground function: Chebyshev polynomial with 15 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C17H14N6O5γ = 109.849 (8)°
Mr = 382.34V = 843.78 (19) Å3
Triclinic, P1Z = 2
a = 7.2689 (8) ÅCu Kα1 radiation, λ = 1.54056 Å
b = 10.3176 (14) ŵ = 0.97 mm1
c = 12.1761 (15) ÅT = 293 K
α = 96.462 (6)°flat_sheet, 10 × 1.2 mm
β = 95.869 (4)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: flat sample holder2θmin = 3.00°, 2θmax = 34.00°, 2θstep = 0.02°
Data collection mode: transmission
Refinement top
Rp = 0.0301550 data points
Rwp = 0.040190 parameters
Rexp = 0.055118 restraints
χ2 = 1.277H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.418 (2)0.0163 (8)0.1595 (7)0.03800
N20.511 (3)0.1432 (9)0.2055 (8)0.03800
C30.286 (2)0.0251 (8)0.0471 (7)0.03800
C40.4288 (18)0.0815 (8)0.2383 (7)0.03800
N50.5307 (11)0.2457 (7)0.1517 (6)0.03800
N60.1525 (13)0.1566 (8)0.0248 (6)0.03800
O70.288 (3)0.0629 (12)0.0132 (12)0.03800
O80.344 (3)0.2077 (11)0.2090 (11)0.03800
C90.5908 (11)0.0225 (8)0.3397 (6)0.03800
C100.6518 (9)0.3800 (6)0.2040 (6)0.03800
H110.493 (7)0.223 (3)0.068 (2)0.04559
C120.0268 (12)0.2242 (7)0.0768 (6)0.03800
H130.134 (4)0.208 (3)0.0896 (19)0.04559
H140.626 (5)0.090 (3)0.3618 (19)0.04559
H150.725 (4)0.035 (3)0.321 (2)0.04559
H160.543 (4)0.076 (3)0.409 (2)0.04559
C170.7483 (7)0.4024 (7)0.3130 (5)0.03800
C180.6725 (8)0.4920 (6)0.1424 (5)0.03800
C190.0054 (9)0.1503 (7)0.1625 (6)0.03800
C200.0748 (11)0.3683 (7)0.0890 (6)0.03800
C210.8702 (7)0.5385 (7)0.3637 (6)0.03800
H220.726 (4)0.314 (3)0.356 (2)0.04559
C230.7923 (7)0.6253 (6)0.1933 (5)0.03800
H240.597 (4)0.475 (3)0.057 (2)0.04559
C250.1228 (7)0.2275 (6)0.2606 (5)0.03800
H260.086 (4)0.041 (2)0.1513 (19)0.04559
C270.2026 (9)0.4477 (7)0.1860 (6)0.03800
H280.055 (4)0.421 (2)0.022 (3)0.04559
C290.8926 (7)0.6493 (7)0.3053 (5)0.03800
H300.946 (4)0.557 (2)0.447 (2)0.04559
H310.807 (4)0.710 (3)0.1474 (19)0.04559
C320.2258 (8)0.3763 (4)0.2709 (4)0.03800
N330.1857 (10)0.1946 (7)0.3637 (6)0.03800
H340.285 (5)0.561 (3)0.1951 (19)0.04559
N351.0167 (11)0.7926 (7)0.3543 (7)0.03800
N360.3376 (10)0.4238 (7)0.3739 (6)0.03800
H370.144 (5)0.100 (3)0.3876 (19)0.04559
C380.3205 (11)0.3136 (8)0.4365 (6)0.03800
O391.118 (2)0.8169 (15)0.4472 (10)0.03800
O400.966 (3)0.8797 (10)0.3125 (11)0.03800
H410.420 (4)0.523 (2)0.4014 (17)0.04559
O420.4031 (15)0.3162 (12)0.5334 (8)0.03800
Geometric parameters (Å, º) top
C1—N21.28 (1)C18—H241.09 (3)
C1—C31.52 (1)C19—C251.408 (8)
C1—C41.48 (1)C19—H261.07 (2)
N2—N51.28 (1)C20—C271.404 (9)
C3—N61.35 (1)C20—H281.05 (3)
C3—O71.23 (2)C21—C291.38 (1)
C4—O81.23 (1)C21—H301.07 (2)
C4—C91.53 (1)C23—C291.431 (8)
N5—C101.399 (8)C23—H311.07 (3)
N5—H111.00 (3)C25—C321.446 (7)
N6—C121.412 (9)C25—N331.41 (1)
N6—H131.00 (3)C27—C321.363 (9)
C9—H141.09 (3)C27—H341.10 (2)
C9—H151.07 (3)C29—N351.464 (8)
C9—H161.08 (3)C32—N361.363 (8)
C10—C171.392 (9)N33—H371.01 (3)
C10—C181.422 (9)N33—C381.420 (8)
C12—C191.38 (1)N35—O391.23 (1)
C12—C201.400 (9)N35—O401.22 (2)
C17—C211.409 (8)N36—C381.42 (1)
C17—H221.07 (3)N36—H410.99 (2)
C18—C231.385 (7)C38—O421.26 (1)
N2—C1—C3123 (1)C25—C19—H26124 (1)
N2—C1—C4111.0 (9)C12—C20—C27123.7 (7)
C3—C1—C4124.6 (6)C12—C20—H28118 (1)
C1—N2—N5122.2 (9)C27—C20—H28118 (1)
C1—C3—N6116.6 (8)C17—C21—C29120.0 (6)
C1—C3—O7120.1 (9)C17—C21—H30120 (1)
N6—C3—O7123 (1)C29—C21—H30120 (1)
C1—C4—O8120 (1)C18—C23—C29120.7 (6)
C1—C4—C9116.1 (7)C18—C23—H31118 (1)
O8—C4—C9122 (1)C29—C23—H31121 (1)
N2—N5—C10118.9 (7)C19—C25—C32121.4 (6)
N2—N5—H11117 (2)C19—C25—N33134.7 (6)
C10—N5—H11121 (2)C32—C25—N33103.9 (4)
C3—N6—C12127.5 (8)C20—C27—C32116.1 (5)
C3—N6—H13115 (1)C20—C27—H34124 (1)
C12—N6—H13117 (1)C32—C27—H34120 (1)
C4—C9—H14110 (2)C21—C29—C23120.0 (5)
C4—C9—H15110 (1)C21—C29—N35122.1 (6)
C4—C9—H16110 (1)C23—C29—N35117.9 (6)
H14—C9—H15106 (2)C25—C32—C27121.4 (5)
H14—C9—H16111 (2)C25—C32—N36108.9 (5)
H15—C9—H16109 (2)C27—C32—N36129.7 (5)
N5—C10—C18117.9 (6)C25—N33—H37127 (1)
C17—C10—C18121.4 (5)C25—N33—C38112.3 (6)
N6—C12—C19121.0 (6)H37—N33—C38121 (1)
N6—C12—C20118.2 (7)C29—N35—O39120.2 (9)
C19—C12—C20120.8 (6)C29—N35—O40113.0 (8)
C10—C17—C21119.7 (6)O39—N35—O40123 (1)
C10—C17—H22118 (1)C32—N36—C38111.4 (5)
C21—C17—H22122 (1)C32—N36—H41124 (1)
C10—C18—C23118.3 (5)C38—N36—H41124 (1)
C10—C18—H24121 (1)N33—C38—N36103.5 (6)
C23—C18—H24120 (1)N33—C38—O42126.6 (8)
C12—C19—C25116.6 (6)N36—C38—O42129.8 (7)
C12—C19—H26119 (1)
(PY151) top
Crystal data top
C18H15N5O5Z = 2
Mr = 381.35F(000) = 396
Triclinic, P1Dx = 1.553 Mg m3
Hall symbol: -P 1Cu Kα1 radiation, λ = 1.54056 Å
a = 5.12970 (14) ŵ = 0.98 mm1
b = 9.2292 (3) ÅT = 293 K
c = 17.4094 (6) ÅParticle morphology: no specific habit
α = 95.857 (2)°orange
β = 95.5056 (17)°cylinder, 10 × 0.7 mm
γ = 91.7980 (13)°Specimen preparation: Prepared at 293 K and 0.00 kPa
V = 815.42 (4) Å3
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 4.00°, 2θmax = 74.00°, 2θstep = 0.01°
Specimen mounting: 'glass capillary'
Refinement top
Refinement on Inet194 parameters
Least-squares matrix: full with fixed elements per cycle118 restraints
Rp = 0.0150 constraints
Rwp = 0.021H-atom parameters constrained
Rexp = 0.054Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.369(Δ/σ)max = 0.001
7000 data pointsBackground function: Chebyshev polynomial with 20 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C18H15N5O5γ = 91.7980 (13)°
Mr = 381.35V = 815.42 (4) Å3
Triclinic, P1Z = 2
a = 5.12970 (14) ÅCu Kα1 radiation, λ = 1.54056 Å
b = 9.2292 (3) ŵ = 0.98 mm1
c = 17.4094 (6) ÅT = 293 K
α = 95.857 (2)°cylinder, 10 × 0.7 mm
β = 95.5056 (17)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: 'glass capillary'2θmin = 4.00°, 2θmax = 74.00°, 2θstep = 0.01°
Data collection mode: transmission
Refinement top
Rp = 0.0157000 data points
Rwp = 0.021194 parameters
Rexp = 0.054118 restraints
χ2 = 1.369H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.7418 (7)0.1407 (4)0.76861 (17)0.03680
C20.5843 (7)0.1220 (4)0.83607 (18)0.03680
N30.7080 (8)0.0571 (4)0.70371 (19)0.03680
C40.9503 (7)0.2575 (4)0.76977 (17)0.03680
N50.6345 (5)0.2211 (3)0.89847 (16)0.03680
O60.3994 (8)0.0326 (5)0.8246 (3)0.03680
N70.5357 (6)0.0512 (3)0.68773 (15)0.03680
O81.0236 (7)0.3383 (5)0.8277 (2)0.03680
C91.0975 (5)0.2516 (3)0.69777 (16)0.03680
C100.5215 (5)0.2398 (3)0.96951 (16)0.03680
H110.778780.288110.893570.04416
H120.418750.073970.725440.04416
C130.5197 (4)0.1361 (3)0.61585 (15)0.03680
H141.173030.143840.685180.04416
H150.966160.277350.648460.04416
H161.260910.331310.706940.04416
C170.6210 (5)0.3427 (3)1.02889 (15)0.03680
C180.3042 (6)0.1521 (3)0.97876 (16)0.03680
C190.6890 (5)0.1046 (2)0.56204 (15)0.03680
C200.3340 (5)0.2541 (3)0.59660 (15)0.03680
C210.5029 (4)0.3546 (2)1.09601 (13)0.03680
H220.780030.408581.023010.04416
C230.1821 (5)0.1628 (3)1.04593 (16)0.03680
H240.227510.076980.935290.04416
C250.6716 (5)0.1908 (3)0.49044 (15)0.03680
H260.826090.020570.573120.04416
C270.3208 (5)0.3382 (3)0.52449 (15)0.03680
C280.1484 (6)0.2910 (3)0.65291 (17)0.03680
C290.2807 (4)0.26350 (19)1.10470 (14)0.03680
N300.5556 (5)0.4440 (3)1.16446 (15)0.03680
H310.022710.098621.051930.04416
C320.4907 (5)0.3059 (3)0.47148 (14)0.03680
H330.797420.166920.451310.04416
H340.187530.423260.510230.04416
O350.0248 (7)0.4027 (4)0.6268 (2)0.03680
O360.1339 (7)0.2206 (5)0.7143 (2)0.03680
N370.2182 (5)0.3076 (3)1.17946 (15)0.03680
H380.697620.517091.173370.04416
C390.3824 (6)0.4172 (3)1.21659 (16)0.03680
H400.483270.366200.418830.04416
H410.157510.430510.659550.04416
H420.075960.266381.203980.04416
O430.3770 (7)0.4781 (4)1.2817 (2)0.03680
Geometric parameters (Å, º) top
C1—C21.509 (5)C17—H221.05 (1)
C1—N31.296 (4)C18—C231.374 (4)
C1—C41.492 (5)C19—C251.402 (3)
C2—N51.347 (4)C20—C271.402 (3)
C2—O61.225 (5)C20—C281.486 (4)
N3—N71.303 (4)C21—C291.423 (3)
C4—O81.213 (5)C21—N301.378 (3)
C4—C91.521 (4)C23—C291.356 (3)
N5—C101.412 (4)C25—C321.379 (3)
N5—H110.98 (1)C27—C321.376 (4)
N7—C131.401 (3)C28—O351.352 (4)
C9—H141.10 (1)C28—O361.203 (5)
C9—H151.10 (1)C29—N371.393 (3)
C9—H161.08 (1)N30—H380.99 (1)
C10—C171.377 (4)N30—C391.365 (4)
C10—C181.390 (4)O35—H410.94 (1)
C13—C191.383 (4)N37—C391.364 (4)
C13—C201.417 (3)N37—H420.97 (1)
C17—C211.363 (4)C39—O431.215 (5)
C2—C1—N3123.2 (3)C13—C19—C25118.8 (2)
C2—C1—C4123.4 (3)C13—C19—H26119.4 (6)
N3—C1—C4113.3 (3)C25—C19—H26121.7 (6)
C1—C2—N5116.3 (3)C13—C20—C27121.0 (2)
C1—C2—O6116.7 (3)C13—C20—C28120.4 (2)
N5—C2—O6125.8 (3)C27—C20—C28118.6 (2)
C1—N3—N7125.3 (4)C17—C21—C29121.0 (2)
C1—C4—O8122.4 (3)C17—C21—N30132.2 (2)
C1—C4—C9115.1 (2)C29—C21—N30106.8 (2)
O8—C4—C9121.4 (3)C18—C23—C29117.9 (2)
C2—N5—C10131.5 (3)C18—C23—H31119.2 (7)
C2—N5—H11112.1 (7)C29—C23—H31122.9 (7)
N3—N7—H12118.7 (7)C19—C25—C32122.5 (2)
N3—N7—C13120.4 (3)C19—C25—H33119.4 (6)
H12—N7—C13119.8 (7)C32—C25—H33118.1 (6)
C4—C9—H14109.4 (7)C20—C27—C32119.5 (2)
C4—C9—H15110.5 (7)C20—C27—H34119.4 (7)
C4—C9—H16107.6 (6)C32—C27—H34121.1 (7)
H14—C9—H15108.1 (8)C20—C28—O35114.7 (3)
H14—C9—H16109.5 (7)C20—C28—O36123.7 (3)
H15—C9—H16111.6 (9)O35—C28—O36121.2 (3)
N5—C10—C17121.4 (2)C21—C29—C23120.4 (2)
N5—C10—C18118.7 (2)C21—C29—N37104.0 (2)
C17—C10—C18119.9 (3)C23—C29—N37135.5 (2)
N7—C13—C19119.6 (2)C25—C32—C27119.3 (2)
N7—C13—C20121.6 (2)C25—C32—H40119.4 (6)
C19—C13—C20118.8 (2)C27—C32—H40121.3 (6)
C10—C17—C21118.5 (2)C29—N37—C39112.8 (2)
C10—C17—H22120.8 (7)C29—N37—H42127.3 (6)
C21—C17—H22120.8 (7)C39—N37—H42119.9 (7)
C10—C18—C23122.4 (2)N30—C39—N37104.7 (2)
C10—C18—H24120.3 (7)N30—C39—O43127.4 (3)
C23—C18—H24117.3 (7)N37—C39—O43127.9 (3)
(PY154) top
Crystal data top
C18H14F3N5O3F(000) = 832
Mr = 405.34Dx = 1.577 Mg m3
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
Hall symbol: -P 2ybcµ = 1.15 mm1
a = 14.5848 (5) ÅT = 293 K
b = 8.5448 (2) ÅParticle morphology: no specific habit
c = 13.7794 (4) Åorange
β = 96.0670 (19)°cylinder, 10 × 0.7 mm
V = 1707.62 (9) Å3Specimen preparation: Prepared at 293 K and 0.00 kPa
Z = 4
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 3.00°, 2θmax = 70.00°, 2θstep = 0.01°
Specimen mounting: 'glass capillary'
Refinement top
Refinement on Inet180 parameters
Least-squares matrix: full with fixed elements per cycle120 restraints
Rp = 0.0360 constraints
Rwp = 0.047H-atom parameters constrained
Rexp = 0.090Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.369(Δ/σ)max = 0.001
6700 data pointsBackground function: Chebyshev polynomial with 20 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C18H14F3N5O3V = 1707.62 (9) Å3
Mr = 405.34Z = 4
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
a = 14.5848 (5) ŵ = 1.15 mm1
b = 8.5448 (2) ÅT = 293 K
c = 13.7794 (4) Åcylinder, 10 × 0.7 mm
β = 96.0670 (19)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: 'glass capillary'2θmin = 3.00°, 2θmax = 70.00°, 2θstep = 0.01°
Data collection mode: transmission
Refinement top
Rp = 0.0366700 data points
Rwp = 0.047180 parameters
Rexp = 0.090120 restraints
χ2 = 1.369H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.0241 (3)0.1756 (5)0.6301 (8)0.03162
C20.0354 (3)0.0265 (5)0.6201 (8)0.03162
N30.1138 (4)0.1724 (6)0.6498 (7)0.03162
C40.0158 (3)0.3461 (6)0.6192 (7)0.03162
N50.1277 (3)0.0532 (5)0.6081 (4)0.03162
O60.0011 (5)0.1055 (6)0.6245 (7)0.03162
N70.1620 (3)0.0435 (5)0.6504 (4)0.03162
O80.0989 (4)0.3709 (7)0.6042 (6)0.03162
C90.0563 (3)0.4770 (5)0.6328 (4)0.03162
C100.2002 (3)0.0542 (5)0.5942 (4)0.03162
H110.143990.162650.607490.03794
H120.132730.057080.638840.03794
C130.2569 (3)0.0572 (5)0.6668 (2)0.03162
H140.101410.470590.574750.03794
H150.097580.465120.702890.03794
H160.022150.590430.629690.03794
C170.1864 (3)0.2210 (5)0.5915 (3)0.03162
C180.2886 (3)0.0122 (5)0.5801 (4)0.03162
C190.2963 (3)0.2060 (5)0.6766 (2)0.03162
C200.3122 (3)0.0799 (5)0.6737 (3)0.03162
C210.2651 (3)0.3072 (5)0.5741 (2)0.03162
H220.123470.273390.601360.03794
C230.3684 (3)0.0803 (5)0.5618 (3)0.03162
H240.295520.130710.582450.03794
C250.3927 (3)0.2119 (5)0.6935 (2)0.03162
H260.258510.306800.672030.03794
C270.4092 (3)0.0686 (5)0.6899 (2)0.03162
C280.2660 (3)0.2439 (6)0.6651 (3)0.03162
C290.3539 (3)0.2423 (5)0.5596 (2)0.03162
N300.2743 (3)0.4711 (5)0.5682 (3)0.03162
H310.432700.032560.550920.03794
C320.4494 (3)0.0793 (5)0.7003 (3)0.03162
H330.422870.319430.700160.03794
H340.449650.165730.693870.03794
F350.3269 (4)0.3606 (6)0.6775 (5)0.03162
F360.2146 (4)0.2693 (7)0.5837 (4)0.03162
F370.2071 (4)0.2582 (7)0.7353 (4)0.03162
N380.4136 (3)0.3693 (5)0.5448 (3)0.03162
H390.222600.542530.575420.03794
C400.3660 (3)0.5119 (5)0.5494 (4)0.03162
H410.519230.090560.711890.03794
H420.479690.360830.530000.03794
O430.3975 (5)0.6418 (6)0.5339 (4)0.03162
Geometric parameters (Å, º) top
C1—C21.540 (6)C19—C251.402 (6)
C1—N31.308 (7)C20—C271.412 (6)
C1—C41.570 (7)C20—C281.554 (7)
C2—N51.357 (6)C21—C291.403 (6)
C2—O61.246 (7)C21—N301.409 (6)
C4—O81.226 (7)C23—C291.401 (6)
C4—C91.534 (6)C25—C321.400 (6)
N5—C101.398 (6)C27—C321.394 (6)
C9—H141.07 (2)C28—F351.334 (7)
C9—H151.07 (2)C28—F361.300 (7)
C9—H161.09 (2)C28—F371.365 (8)
C10—C171.441 (6)C29—N381.393 (6)
C10—C181.402 (6)N30—H391.00 (2)
C13—C191.396 (6)N30—C401.380 (6)
C13—C201.419 (6)N38—C401.400 (6)
C17—C211.364 (6)C40—O431.211 (7)
C18—C231.408 (6)
C2—C1—N3122.9 (4)C13—C20—C27120.4 (4)
C2—C1—C4124.0 (4)C13—C20—C28120.0 (4)
N3—C1—C4113.1 (4)C27—C20—C28119.5 (4)
C1—C2—N5114.5 (4)C17—C21—C29124.0 (4)
C1—C2—O6120.7 (5)C17—C21—N30128.3 (4)
N5—C2—O6124.8 (5)C29—C21—N30107.7 (4)
C1—N3—N7123.0 (5)C18—C23—C29115.7 (4)
C1—C4—O8121.8 (5)C18—C23—H31123 (1)
C1—C4—C9115.0 (4)C29—C23—H31121 (1)
O8—C4—C9123.2 (5)C19—C25—C32123.8 (4)
C2—N5—C10129.2 (4)C19—C25—H33118 (1)
C2—N5—H11116 (1)C32—C25—H33118 (1)
C10—N5—H11114 (1)C20—C27—C32118.8 (4)
N3—N7—C13117.3 (4)C20—C27—H34120 (1)
C4—C9—H14109 (1)C32—C27—H34121 (1)
C4—C9—H15111 (1)C20—C28—F35112.7 (4)
C4—C9—H16111 (1)C20—C28—F36115.0 (4)
H14—C9—H16108 (1)C20—C28—F37109.1 (4)
H15—C9—H16112 (1)F35—C28—F36107.5 (5)
N5—C10—C17123.1 (4)F35—C28—F37107.6 (5)
N5—C10—C18115.1 (4)F36—C28—F37104.3 (5)
C17—C10—C18121.7 (4)C21—C29—C23121.8 (4)
N7—C13—C19119.1 (4)C21—C29—N38105.4 (4)
N7—C13—C20119.5 (4)C23—C29—N38132.8 (4)
C19—C13—C20121.4 (4)C21—N30—C40110.2 (4)
C10—C17—C21114.9 (4)C25—C32—C27119.2 (4)
C10—C17—H22123.3 (9)C25—C32—H41120.7 (1)
C21—C17—H22121.8 (9)C27—C32—H41120 (1)
C10—C18—C23121.9 (4)C29—N38—C40111.8 (4)
C10—C18—H24117 (1)C29—N38—H42126.9 (9)
C23—C18—H24121 (1)C40—N38—H42121.2 (9)
C13—C19—C25116.3 (4)N30—C40—N38104.8 (4)
C13—C19—H26120 (1)N30—C40—O43127.3 (5)
C25—C19—H26123 (1)N38—C40—O43127.8 (5)
(PY181) top
Crystal data top
C25H21N7O5F(000) = 1040
Mr = 499.49Dx = 1.477 Mg m3
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
Hall symbol: -P 2ybcµ = 0.89 mm1
a = 22.5510 (8) ÅT = 293 K
b = 4.96366 (13) ÅParticle morphology: no specific habit
c = 21.2815 (6) Åorange
β = 109.4539 (13)°cylinder, 10 × 0.7 mm
V = 2246.16 (12) Å3Specimen preparation: Prepared at 293 K and 0.00 kPa
Z = 4
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 3.00°, 2θmax = 60.00°, 2θstep = 0.01°
Specimen mounting: 'glass capillary'
Refinement top
Refinement on Inet224 parameters
Least-squares matrix: full with fixed elements per cycle162 restraints
Rp = 0.0120 constraints
Rwp = 0.015H-atom parameters constrained
Rexp = 0.036Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.188(Δ/σ)max = 0.001
5700 data pointsBackground function: Chebyshev polynomial with 20 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C25H21N7O5V = 2246.16 (12) Å3
Mr = 499.49Z = 4
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
a = 22.5510 (8) ŵ = 0.89 mm1
b = 4.96366 (13) ÅT = 293 K
c = 21.2815 (6) Åcylinder, 10 × 0.7 mm
β = 109.4539 (13)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: 'glass capillary'2θmin = 3.00°, 2θmax = 60.00°, 2θstep = 0.01°
Data collection mode: transmission
Refinement top
Rp = 0.0125700 data points
Rwp = 0.015224 parameters
Rexp = 0.036162 restraints
χ2 = 1.188H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzBiso*/Beq
C10.66678 (15)0.5335 (7)0.04782 (17)2.50 (13)
N20.71619 (17)0.5825 (9)0.02379 (17)2.50 (13)
C30.65657 (16)0.6821 (7)0.09860 (17)2.50 (13)
C40.62626 (16)0.3226 (6)0.01783 (18)2.50 (13)
N50.7589 (2)0.7575 (12)0.0517 (3)2.50 (13)
H60.719670.474750.012703.00 (15)
C70.60538 (16)0.6173 (6)0.11909 (14)2.50 (13)
H80.685670.837240.120853.00 (15)
C90.57640 (15)0.2614 (7)0.03846 (16)2.50 (13)
H100.633650.212870.019473.00 (15)
C110.80788 (19)0.7920 (10)0.0341 (2)2.50 (13)
C120.56517 (17)0.4074 (7)0.08941 (15)2.50 (13)
H130.597990.726430.156423.00 (15)
H140.547570.106240.015903.00 (15)
C150.82224 (19)0.6163 (10)0.0162 (2)2.50 (13)
C160.85275 (19)1.0001 (11)0.0734 (2)2.50 (13)
C170.50966 (18)0.3246 (7)0.1085 (2)2.50 (13)
N180.87669 (17)0.6653 (8)0.0279 (2)2.50 (13)
O190.7849 (3)0.4389 (12)0.0436 (3)2.50 (13)
O200.9018 (2)1.0451 (13)0.0626 (3)2.50 (13)
C210.83546 (16)1.1592 (8)0.12501 (18)2.50 (13)
O220.4936 (3)0.0918 (10)0.1053 (3)2.50 (13)
N230.48302 (17)0.5249 (7)0.1344 (2)2.50 (13)
C240.90009 (17)0.5254 (8)0.07246 (19)2.50 (13)
H250.901950.810560.002443.00 (15)
H260.790361.257630.102473.00 (15)
H270.832141.026930.164513.00 (15)
H280.871151.311600.146323.00 (15)
H290.501550.702120.137253.00 (15)
C300.43253 (17)0.5046 (7)0.15993 (17)2.50 (13)
C310.86734 (17)0.3138 (8)0.11406 (19)2.50 (13)
C320.95801 (18)0.6101 (8)0.0747 (2)2.50 (13)
C330.38787 (16)0.2995 (7)0.13488 (14)2.50 (13)
C340.42550 (16)0.6774 (7)0.20801 (16)2.50 (13)
C350.89497 (16)0.1938 (5)0.15652 (13)2.50 (13)
H360.824740.245620.114373.00 (15)
C370.98555 (18)0.4895 (7)0.11712 (18)2.50 (13)
H380.981130.764400.044653.00 (15)
C390.33768 (16)0.2704 (6)0.15820 (16)2.50 (13)
H400.390830.170570.098823.00 (15)
C410.37527 (16)0.6467 (7)0.23096 (17)2.50 (13)
H420.457390.827690.226583.00 (15)
C430.95397 (13)0.2823 (5)0.15799 (15)2.50 (13)
N440.87591 (16)0.0158 (7)0.20326 (18)2.50 (13)
H451.028210.552140.118303.00 (15)
C460.33065 (17)0.4431 (7)0.20630 (17)2.50 (13)
H470.305700.120340.139143.00 (15)
H480.371300.776450.266453.00 (15)
N490.96860 (16)0.1249 (8)0.20455 (19)2.50 (13)
H500.836390.110260.212933.00 (15)
C510.92107 (18)0.0618 (8)0.23346 (19)2.50 (13)
C520.27697 (18)0.4158 (8)0.2321 (2)2.50 (13)
H531.006730.147140.215223.00 (15)
O540.9186 (2)0.2246 (10)0.2762 (2)2.50 (13)
O550.2484 (3)0.2070 (10)0.2258 (3)2.50 (13)
N560.26068 (18)0.6416 (8)0.2592 (3)2.50 (13)
H570.282170.810880.259943.00 (15)
H580.226130.633810.276663.00 (15)
Geometric parameters (Å, º) top
C1—N21.394 (6)C24—C321.385 (6)
C1—C31.386 (6)C30—C331.403 (5)
N2—N51.285 (5)C30—C341.383 (6)
N2—H60.99 (2)C31—C351.391 (6)
C3—C71.404 (6)C32—C371.391 (7)
C4—C91.371 (6)C33—C391.385 (6)
N5—C111.299 (5)C34—C411.384 (6)
C7—C121.389 (5)C35—C431.412 (5)
C9—C121.397 (6)C35—N441.404 (5)
C12—C171.496 (7)C37—C431.378 (5)
C15—N181.346 (6)C39—C461.382 (5)
C15—O191.220 (4)C41—C461.402 (5)
C16—O201.228 (7)C43—N491.385 (6)
C16—C211.502 (6)N44—H501.00 (1)
C17—O221.202 (7)N44—C511.394 (7)
C17—N231.367 (6)C46—C521.494 (7)
N18—C241.414 (7)N49—C511.396 (6)
N18—H251.00 (1)N49—H530.99 (2)
C21—H261.09 (1)C51—O541.205 (7)
C21—H271.08 (2)C52—O551.204 (7)
C21—H281.08 (1)C52—N561.367 (7)
N23—H290.99 (1)N56—H570.99 (2)
N23—C301.420 (7)N56—H580.98 (2)
C24—C311.413 (6)
N2—C1—C3123.7 (3)C31—C24—C32120.2 (4)
N2—C1—C4116.2 (4)N23—C30—C33118.1 (4)
C3—C1—C4120.1 (4)N23—C30—C34122.8 (3)
C1—N2—N5121.0 (4)C33—C30—C34119.1 (4)
C1—N2—H6120.3 (9)C24—C31—C35118.3 (4)
N5—N2—H6117 (1)C24—C31—H36120.2 (9)
C1—C3—C7119.2 (3)C35—C31—H36121.5 (9)
C1—C3—H8120 (1)C24—C32—C37121.5 (4)
C7—C3—H8120 (1)C24—C32—H38119 (1)
C1—C4—C9120.1 (3)C37—C32—H38120 (1)
C1—C4—H10119.8 (9)C30—C33—C39120.5 (3)
C9—C4—H10120.1 (8)C30—C33—H40119.7 (9)
N2—N5—C11123.7 (3)C39—C33—H40119.7 (9)
C3—C7—C12120.7 (3)C30—C34—C41120.0 (3)
C3—C7—H13119.2 (9)C30—C34—H42119 (1)
C12—C7—H13120.1 (9)C41—C34—H42120 (1)
C4—C9—C12120.9 (3)C31—C35—C43120.6 (3)
C4—C9—H14120 (1)C31—C35—N44132.9 (3)
C12—C9—H14119 (1)C43—C35—N44106.5 (3)
C15—C11—C16123.3 (3)C32—C37—C43118.7 (4)
C7—C12—C9119.0 (4)C32—C37—H45120 (1)
C7—C12—C17124.0 (4)C43—C37—H45121 (1)
C9—C12—C17117.0 (3)C33—C39—C46120.6 (3)
C11—C15—O19119.3 (4)C33—C39—H47120 (1)
N18—C15—O19125.1 (4)C46—C39—H47120 (1)
C11—C16—O20120.6 (4)C34—C41—C46121.1 (4)
C11—C16—C21118.8 (3)C34—C41—H48119.5 (9)
O20—C16—C21120.4 (4)C46—C41—H48119.3 (9)
C12—C17—O22120.5 (5)C35—C43—C37120.7 (3)
C12—C17—N23115.6 (3)C35—C43—N49106.8 (3)
O22—C17—N23123.7 (5)C37—C43—N49132.5 (4)
C15—N18—C24126.5 (4)C35—N44—C51110.5 (3)
C15—N18—H25114 (1)C39—C46—C41118.6 (4)
C24—N18—H25114 (1)C39—C46—C52121.7 (3)
C16—C21—H26109.0 (8)C41—C46—C52119.7 (4)
C16—C21—H27112 (1)C43—N49—C51111.2 (4)
C16—C21—H28108.3 (9)C43—N49—H53126 (1)
H26—C21—H27107 (1)N44—C51—N49104.9 (4)
H26—C21—H28110 (1)N44—C51—O54127.3 (5)
H27—C21—H28110 (1)N49—C51—O54127.8 (5)
C17—N23—H29116 (1)C46—C52—O55119.9 (5)
C17—N23—C30128.2 (4)C46—C52—N56116.7 (4)
H29—N23—C30115 (1)O55—C52—N56123.2 (5)
N18—C24—C31123.4 (4)C52—N56—H57119.9 (1)
N18—C24—C32116.4 (4)H57—N56—H58116 (1)
(PY194) top
Crystal data top
C18H17N5O4F(000) = 768
Mr = 367.37Dx = 1.468 Mg m3
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
Hall symbol: -P 2ybcµ = 0.89 mm1
a = 14.7172 (16) ÅT = 293 K
b = 5.9852 (5) ÅParticle morphology: no specific habit
c = 20.7919 (13) Åorange
β = 114.818 (4)°flat_sheet, 10 × 1.2 mm
V = 1662.3 (2) Å3Specimen preparation: Prepared at 293 K and 0.00 kPa
Z = 4
Data collection top
STOE-Stadi-P
diffractometer
Data collection mode: transmission
Radiation source: sealed X-ray tube, laboratory diffractometerScan method: step
Primary focussing, Ge 111 monochromator2θmin = 3.00°, 2θmax = 34.00°, 2θstep = 0.02°
Specimen mounting: flat sample holder
Refinement top
Refinement on Inet176 parameters
Least-squares matrix: full with fixed elements per cycle122 restraints
Rp = 0.0290 constraints
Rwp = 0.039H-atom parameters constrained
Rexp = 0.048Weighting scheme based on measured s.u.'s w = 1/σ[Yobs]2
χ2 = 1.322(Δ/σ)max = 0.001
1550 data pointsBackground function: Chebyshev polynomial with 15 terms
Excluded region(s): nonePreferred orientation correction: none
Profile function: modified Thompson-Cox-Hastings pseudo-Voigt (Young, 1993)
Crystal data top
C18H17N5O4V = 1662.3 (2) Å3
Mr = 367.37Z = 4
Monoclinic, P21/cCu Kα1 radiation, λ = 1.54056 Å
a = 14.7172 (16) ŵ = 0.89 mm1
b = 5.9852 (5) ÅT = 293 K
c = 20.7919 (13) Åflat_sheet, 10 × 1.2 mm
β = 114.818 (4)°
Data collection top
STOE-Stadi-P
diffractometer
Scan method: step
Specimen mounting: flat sample holder2θmin = 3.00°, 2θmax = 34.00°, 2θstep = 0.02°
Data collection mode: transmission
Refinement top
Rp = 0.0291550 data points
Rwp = 0.039176 parameters
Rexp = 0.048122 restraints
χ2 = 1.322H-atom parameters constrained
Special details top

Experimental. specimen was rotated in its plane

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzBiso*/Beq
C10.1777 (5)0.8522 (9)0.95496 (17)2.53665
C20.0630 (3)0.8367 (10)0.91732 (18)2.53665
N30.2320 (6)0.6866 (13)0.9461 (3)2.53665
C40.2315 (6)1.0409 (15)1.0014 (3)2.53665
N50.0098 (5)0.9996 (12)0.9255 (3)2.53665
O60.0244 (7)0.6727 (15)0.8806 (3)2.53665
N70.1973 (5)0.5046 (12)0.9046 (3)2.53665
O80.1843 (9)1.1852 (19)1.0117 (6)2.53665
C90.3452 (6)1.0289 (15)1.0434 (5)2.53665
C100.0911 (7)1.0541 (15)0.8849 (4)2.53665
H110.0495 (18)1.119 (4)0.9565 (11)3.04398
H120.1238 (17)0.471 (5)0.8794 (14)3.04398
C130.2644 (6)0.3865 (12)0.8878 (3)2.53665
H140.3792 (15)0.912 (4)1.0201 (11)3.04398
H150.3633 (17)0.971 (4)1.0959 (11)3.04398
H160.3761 (16)1.195 (4)1.0463 (11)3.04398
C170.1164 (6)1.2549 (14)0.9044 (4)2.53665
C180.1617 (6)0.9195 (15)0.8336 (5)2.53665
C190.3638 (6)0.4434 (11)0.9122 (3)2.53665
C200.2292 (6)0.1948 (13)0.8479 (3)2.53665
C210.2153 (4)1.3147 (12)0.8707 (3)2.53665
H220.061 (2)1.358 (4)0.9442 (12)3.04398
C230.2604 (6)0.9783 (13)0.7985 (4)2.53665
H240.1387 (15)0.767 (4)0.8196 (10)3.04398
C250.4263 (6)0.3070 (12)0.8965 (3)2.53665
H260.3905 (16)0.591 (4)0.9424 (11)3.04398
C270.2932 (6)0.0539 (11)0.8318 (3)2.53665
O280.1256 (7)0.1513 (18)0.8238 (4)2.53665
C290.2888 (5)1.1746 (10)0.8164 (2)2.53665
N300.2699 (6)1.5011 (14)0.8752 (4)2.53665
H310.3120 (17)0.872 (5)0.7588 (11)3.04398
C320.3914 (6)0.1107 (11)0.8562 (3)2.53665
H330.5031 (19)0.356 (4)0.9162 (10)3.04398
H340.2662 (17)0.096 (4)0.8012 (11)3.04398
C350.0875 (6)0.0068 (14)0.7680 (4)2.53665
N360.3802 (5)1.2856 (14)0.7931 (4)2.53665
H370.2429 (17)1.633 (4)0.9073 (11)3.04398
C380.3721 (6)1.4825 (15)0.8272 (5)2.53665
H390.4399 (17)0.005 (4)0.8440 (10)3.04398
H400.1422 (16)0.135 (4)0.7772 (12)3.04398
H410.0738 (17)0.076 (5)0.7196 (10)3.04398
H420.020 (2)0.081 (11)0.7650 (13)3.04398
H430.445 (2)1.236 (7)0.7565 (11)3.04398
O440.4398 (8)1.6082 (19)0.8181 (5)2.53665
Geometric parameters (Å, º) top
C1—N31.36 (1)C20—C271.426 (9)
C4—C91.497 (8)C21—C291.447 (6)
N5—H110.97 (3)C23—C291.377 (8)
N7—H120.98 (2)C23—H311.00 (2)
N7—C131.364 (9)C25—C321.423 (7)
C9—H141.08 (2)C25—H331.02 (2)
C9—H151.08 (2)C27—H341.04 (2)
C9—H161.09 (2)O28—C351.453 (9)
C10—C171.39 (1)N30—H370.97 (2)
C10—C181.385 (8)C32—H391.03 (2)
C13—C191.404 (8)C35—H401.10 (2)
C17—H221.01 (2)C35—H411.10 (2)
C18—C231.397 (8)C35—H421.12 (3)
C18—H240.99 (2)N36—C381.374 (9)
C19—H261.02 (2)N36—H430.97 (2)
C2—C1—C4125.0 (7)C13—C20—O28116.8 (6)
C1—C2—O6120.7 (9)C27—C20—O28121.8 (5)
C1—N3—N7127.4 (7)C17—C21—C29120.2 (5)
C1—C4—O8119.6 (7)C17—C21—N30133.7 (5)
C2—N5—H11114 (1)C29—C21—N30106.1 (4)
C10—N5—H11114 (1)C18—C23—C29118.3 (5)
N3—N7—H12117 (2)C18—C23—H31122 (1)
H12—N7—C13119 (2)C29—C23—H31120 (1)
C4—C9—H14110 (1)C19—C25—C32121.7 (5)
C4—C9—H15111 (1)C19—C25—H33119 (1)
C4—C9—H16111 (1)C32—C25—H33119 (1)
H14—C9—H15108 (2)C20—C27—C32118.1 (4)
H14—C9—H16108 (1)C20—C27—H34122 (1)
H15—C9—H16108 (2)C32—C27—H34120 (1)
N5—C10—C17113.3 (5)C21—C29—C23120.0 (4)
N5—C10—C18126.0 (7)C21—C29—N36108.5 (4)
C17—C10—C18120.7 (6)C23—C29—N36131.5 (4)
N7—C13—C19122.8 (5)C21—N30—H37126 (1)
N7—C13—C20117.6 (5)H37—N30—C38126 (1)
C19—C13—C20119.5 (5)C25—C32—C27120.2 (5)
C10—C17—C21118.2 (5)C25—C32—H39119 (1)
C10—C17—H22120 (1)C27—C32—H39120 (1)
C21—C17—H22122 (1)O28—C35—H40110 (1)
C10—C18—C23122.5 (6)O28—C35—H41111 (1)
C10—C18—H24119 (1)O28—C35—H42110 (2)
C23—C18—H24118 (1)H40—C35—H41109 (1)
C13—C19—C25119.1 (5)H40—C35—H42108 (1)
C13—C19—H26121 (1)H41—C35—H42109 (2)
C25—C19—H26120 (1)C29—N36—H43125 (2)
C13—C20—C27121.4 (5)N36—C38—O44126.4 (6)
(BIRZIL) top
Crystal data top
C18H16ClN5O4Z = 8
Mr = 401.81F(000) = 1664
Monoclinic, C2/cDx = 1.470 Mg m3
a = 17.126 (2) ÅCu Kα radiation, λ = 1.54180 Å
b = 5.036 (2) ŵ = 2.19 mm1
c = 42.45 (1) ÅT = 293 K
β = 97.36 (2)°Needle, yellow
V = 3631 (2) Å30.5 × 0.25 × 0.05 mm
Data collection top
Nicolet R3 computer-controlled four circle
diffractometer
Rint = 0.047
Radiation source: fine-focus sealed tubeθmax = 55.2°, θmin = 4.2°
Graphite monochromatorh = 180
2θ/θ scank = 50
2394 measured reflectionsl = 4445
2303 independent reflections1 standard reflections every 40 reflections
971 reflections with I > 2σ(I) intensity decay: no decay
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.078H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.198 w = 1/[σ2(Fo2) + (0.0883P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.92(Δ/σ)max < 0.001
2303 reflectionsΔρmax = 0.25 e Å3
254 parametersΔρmin = 0.25 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.00042 (8)
Crystal data top
C18H16ClN5O4V = 3631 (2) Å3
Mr = 401.81Z = 8
Monoclinic, C2/cCu Kα radiation
a = 17.126 (2) ŵ = 2.19 mm1
b = 5.036 (2) ÅT = 293 K
c = 42.45 (1) Å0.5 × 0.25 × 0.05 mm
β = 97.36 (2)°
Data collection top
Nicolet R3 computer-controlled four circle
diffractometer
Rint = 0.047
2394 measured reflectionsθmax = 55.2°
2303 independent reflections1 standard reflections every 40 reflections
971 reflections with I > 2σ(I) intensity decay: no decay
Refinement top
R[F2 > 2σ(F2)] = 0.0780 restraints
wR(F2) = 0.198H atoms treated by a mixture of independent and constrained refinement
S = 0.92Δρmax = 0.25 e Å3
2303 reflectionsΔρmin = 0.25 e Å3
254 parameters
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
Cl10.08431 (12)0.7367 (6)1.22574 (6)0.0982 (10)
O10.4148 (3)0.5895 (12)1.17342 (13)0.0805 (19)
O20.2234 (3)0.3797 (12)1.09074 (14)0.0737 (18)
O30.4167 (3)0.0453 (12)1.11704 (13)0.0729 (18)
O40.7848 (3)0.4688 (11)1.02475 (13)0.0753 (18)
N10.3079 (3)0.2890 (13)1.15254 (14)0.0561 (18)
H10.35710.27441.14550.061*
N20.2565 (3)0.1362 (14)1.14113 (15)0.0553 (19)
N30.3781 (3)0.2708 (14)1.08444 (14)0.0619 (19)
H30.33630.34301.07900.071*
N40.6684 (3)0.3011 (13)1.05183 (14)0.063 (2)
H40.68730.17501.06220.064*
N50.6601 (3)0.6391 (13)1.02007 (15)0.0623 (19)
H50.67300.76451.00670.070*
C010.1839 (5)0.7001 (19)1.2104 (2)0.064 (2)
C020.2043 (4)0.5024 (18)1.18818 (18)0.060 (2)
H020.16640.39111.18150.063*
C030.2836 (4)0.4755 (17)1.17614 (18)0.053 (2)
C040.3394 (4)0.6498 (18)1.1868 (2)0.059 (2)
C050.3167 (5)0.8381 (17)1.20906 (18)0.062 (2)
H050.35420.94721.21650.067*
C060.2374 (5)0.8677 (17)1.2207 (2)0.068 (3)
H060.22131.00061.23530.072*
C070.2796 (4)0.0410 (17)1.11936 (19)0.052 (2)
C080.3651 (4)0.0866 (17)1.1067 (2)0.054 (2)
C090.4746 (5)0.7648 (19)1.1819 (2)0.091 (3)
H0910.52510.70871.17160.091*
H0920.47490.76081.20450.091*
H0930.46410.94231.17540.091*
C100.2131 (5)0.2024 (17)1.11081 (19)0.060 (2)
C110.1304 (4)0.1397 (18)1.12526 (19)0.077 (3)
H1110.13130.00221.14030.081*
H1120.10720.29441.13590.081*
H1130.09990.08711.10880.081*
C120.4502 (4)0.3694 (17)1.06797 (17)0.053 (2)
C130.5228 (4)0.2498 (16)1.07110 (16)0.053 (2)
H130.52680.10261.08400.048*
C140.5878 (4)0.3638 (16)1.05384 (18)0.051 (2)
C150.5833 (5)0.5793 (18)1.03372 (19)0.061 (2)
C160.5115 (5)0.6936 (17)1.02995 (19)0.068 (3)
H160.50760.83671.01640.067*
C170.4458 (5)0.5829 (17)1.04749 (19)0.065 (2)
H170.39670.65451.04550.075*
C180.7116 (5)0.4641 (19)1.0316 (2)0.063 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cl10.0571 (13)0.121 (2)0.1124 (19)0.0172 (16)0.0052 (12)0.020 (2)
O10.049 (3)0.085 (5)0.108 (5)0.008 (3)0.010 (3)0.025 (4)
O20.051 (3)0.078 (5)0.094 (5)0.010 (3)0.015 (3)0.010 (4)
O30.045 (3)0.080 (4)0.093 (5)0.005 (3)0.007 (3)0.024 (4)
O40.047 (3)0.081 (4)0.098 (4)0.006 (3)0.008 (3)0.020 (4)
N10.040 (3)0.059 (5)0.069 (5)0.002 (4)0.002 (3)0.013 (4)
N20.047 (4)0.068 (5)0.052 (4)0.002 (4)0.012 (3)0.007 (4)
N30.046 (4)0.074 (5)0.065 (5)0.003 (4)0.005 (3)0.013 (4)
N40.048 (4)0.063 (5)0.076 (5)0.001 (4)0.001 (3)0.018 (4)
N50.055 (4)0.058 (5)0.072 (5)0.006 (4)0.003 (4)0.015 (4)
C010.053 (5)0.073 (7)0.066 (6)0.017 (5)0.005 (4)0.006 (6)
C020.049 (5)0.067 (6)0.063 (6)0.010 (5)0.007 (4)0.010 (5)
C030.053 (5)0.049 (6)0.056 (5)0.012 (5)0.004 (4)0.001 (5)
C040.046 (5)0.059 (6)0.072 (6)0.006 (5)0.008 (4)0.001 (5)
C050.060 (6)0.052 (6)0.073 (6)0.004 (5)0.007 (5)0.002 (5)
C060.073 (6)0.052 (6)0.077 (6)0.018 (5)0.003 (5)0.011 (5)
C070.044 (5)0.053 (6)0.060 (6)0.002 (4)0.008 (4)0.005 (5)
C080.047 (5)0.052 (6)0.063 (6)0.010 (5)0.005 (4)0.006 (5)
C090.067 (6)0.092 (8)0.113 (8)0.008 (6)0.005 (5)0.027 (7)
C100.073 (6)0.055 (6)0.053 (6)0.006 (5)0.009 (5)0.004 (5)
C110.044 (5)0.095 (8)0.094 (7)0.010 (5)0.013 (5)0.003 (6)
C120.054 (5)0.058 (6)0.047 (5)0.003 (5)0.009 (4)0.003 (5)
C130.048 (4)0.055 (5)0.059 (5)0.012 (5)0.013 (4)0.020 (5)
C140.047 (5)0.047 (5)0.061 (5)0.001 (4)0.013 (4)0.005 (5)
C150.052 (5)0.064 (7)0.066 (6)0.002 (5)0.005 (4)0.010 (5)
C160.070 (6)0.069 (7)0.065 (6)0.005 (5)0.011 (5)0.021 (5)
C170.060 (5)0.058 (6)0.077 (6)0.007 (5)0.013 (5)0.011 (5)
C180.057 (5)0.069 (7)0.064 (6)0.003 (6)0.012 (5)0.015 (5)
Geometric parameters (Å, º) top
Cl1—C011.756 (8)C03—C041.415 (10)
O1—C041.377 (8)C04—C051.359 (10)
O1—C091.433 (9)C05—C061.393 (10)
O2—C101.231 (9)C05—H050.9300
O3—C081.230 (9)C06—H060.9300
O4—C181.250 (8)C07—C101.483 (11)
N1—N21.309 (8)C07—C081.511 (9)
N1—C031.397 (9)C09—H0910.9600
N1—H10.8600C09—H0920.9600
N2—C071.309 (9)C09—H0930.9600
N3—C081.324 (9)C10—C111.502 (10)
N3—C121.428 (9)C11—H1110.9600
N3—H30.8600C11—H1120.9600
N4—C181.340 (9)C11—H1130.9600
N4—C141.408 (8)C12—C171.391 (10)
N4—H40.8600C12—C131.403 (9)
N5—C181.381 (9)C13—C141.377 (9)
N5—C151.400 (9)C13—H130.9300
N5—H50.8600C14—C151.389 (10)
C01—C061.358 (11)C15—C161.386 (10)
C01—C021.386 (10)C16—C171.383 (10)
C02—C031.394 (9)C16—H160.9300
C02—H020.9300C17—H170.9300
C04—O1—C09115.0 (7)N3—C08—C07115.3 (8)
N2—N1—C03120.5 (6)O1—C09—H091109.5
N2—N1—H1119.8O1—C09—H092109.5
C03—N1—H1119.8H091—C09—H092109.5
C07—N2—N1120.3 (6)O1—C09—H093109.5
C08—N3—C12130.5 (7)H091—C09—H093109.5
C08—N3—H3114.7H092—C09—H093109.5
C12—N3—H3114.7O2—C10—C07121.3 (8)
C18—N4—C14111.0 (7)O2—C10—C11118.7 (8)
C18—N4—H4124.5C07—C10—C11119.9 (8)
C14—N4—H4124.5C10—C11—H111109.5
C18—N5—C15109.0 (7)C10—C11—H112109.5
C18—N5—H5125.5H111—C11—H112109.5
C15—N5—H5125.5C10—C11—H113109.5
C06—C01—C02122.9 (8)H111—C11—H113109.5
C06—C01—Cl1118.6 (7)H112—C11—H113109.5
C02—C01—Cl1118.4 (7)C17—C12—C13120.7 (7)
C01—C02—C03117.9 (8)C17—C12—N3117.6 (7)
C01—C02—H02121.0C13—C12—N3121.7 (7)
C03—C02—H02121.0C14—C13—C12115.9 (7)
C02—C03—N1121.0 (8)C14—C13—H13122.1
C02—C03—C04119.2 (8)C12—C13—H13122.1
N1—C03—C04119.7 (7)C13—C14—C15123.3 (7)
C05—C04—O1127.6 (8)C13—C14—N4131.2 (7)
C05—C04—C03120.7 (8)C15—C14—N4105.6 (7)
O1—C04—C03111.5 (8)C16—C15—C14121.0 (8)
C04—C05—C06120.0 (8)C16—C15—N5131.6 (8)
C04—C05—H05120.0C14—C15—N5107.4 (7)
C06—C05—H05120.0C17—C16—C15116.3 (8)
C01—C06—C05119.2 (8)C17—C16—H16121.9
C01—C06—H06120.4C15—C16—H16121.9
C05—C06—H06120.4C16—C17—C12122.9 (8)
N2—C07—C10111.9 (7)C16—C17—H17118.6
N2—C07—C08123.1 (8)C12—C17—H17118.6
C10—C07—C08124.8 (8)O4—C18—N4128.1 (8)
O3—C08—N3124.7 (7)O4—C18—N5124.9 (8)
O3—C08—C07120.0 (8)N4—C18—N5107.0 (7)
C03—N1—N2—C07179.0 (7)C08—C07—C10—O24.5 (12)
C06—C01—C02—C030.4 (13)N2—C07—C10—C113.9 (10)
Cl1—C01—C02—C03179.9 (6)C08—C07—C10—C11179.3 (7)
C01—C02—C03—N1176.9 (7)C08—N3—C12—C17174.3 (8)
C01—C02—C03—C040.3 (11)C08—N3—C12—C138.3 (12)
N2—N1—C03—C020.4 (11)C17—C12—C13—C142.5 (11)
N2—N1—C03—C04176.2 (7)N3—C12—C13—C14179.8 (7)
C09—O1—C04—C056.5 (12)C12—C13—C14—C151.7 (11)
C09—O1—C04—C03177.3 (7)C12—C13—C14—N4178.4 (7)
C02—C03—C04—C051.3 (12)C18—N4—C14—C13179.3 (8)
N1—C03—C04—C05178.0 (7)C18—N4—C14—C150.6 (9)
C02—C03—C04—O1177.8 (7)C13—C14—C15—C160.1 (12)
N1—C03—C04—O15.5 (10)N4—C14—C15—C16180.0 (8)
O1—C04—C05—C06178.3 (8)C13—C14—C15—N5179.4 (7)
C03—C04—C05—C062.4 (12)N4—C14—C15—N50.5 (8)
C02—C01—C06—C051.5 (13)C18—N5—C15—C16179.7 (9)
Cl1—C01—C06—C05179.0 (6)C18—N5—C15—C140.3 (9)
C04—C05—C06—C012.5 (12)C14—C15—C16—C170.7 (12)
N1—N2—C07—C10177.1 (7)N5—C15—C16—C17179.9 (8)
N1—N2—C07—C081.6 (11)C15—C16—C17—C120.1 (12)
C12—N3—C08—O32.4 (14)C13—C12—C17—C161.8 (12)
C12—N3—C08—C07178.3 (7)N3—C12—C17—C16179.2 (7)
N2—C07—C08—O30.3 (12)C14—N4—C18—O4178.2 (8)
C10—C07—C08—O3174.5 (8)C14—N4—C18—N50.4 (9)
N2—C07—C08—N3179.1 (7)C15—N5—C18—O4178.0 (8)
C10—C07—C08—N36.1 (11)C15—N5—C18—N40.1 (9)
N2—C07—C10—O2179.9 (7)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.862.282.616 (9)103
C13—H13···O30.932.322.899 (9)120
N1—H1···O30.861.872.555 (8)135
N3—H3···O20.861.942.685 (8)144
N4—H4···O2i0.862.062.919 (9)174
N5—H5···O4ii0.861.962.819 (8)173
Symmetry codes: (i) x1/2, y1/2, z; (ii) x3/2, y+3/2, z+2.
(PY154-DMSO) top
Crystal data top
C20H20F3N5O4SZ = 2
Mr = 483.47F(000) = 500
Triclinic, P1Dx = 1.460 Mg m3
a = 7.5478 (14) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.941 (2) ÅCell parameters from 5696 reflections
c = 13.530 (2) Åθ = 3.6–25.7°
α = 103.996 (14)°µ = 0.21 mm1
β = 101.670 (15)°T = 173 K
γ = 104.491 (14)°Plate, dark yellow
V = 1099.9 (3) Å30.17 × 0.11 × 0.02 mm
Data collection top
STOE IPDS II two-circle-
diffractometer
4108 independent reflections
Radiation source: fine-focus sealed tube2452 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.091
ω scansθmax = 25.6°, θmin = 3.5°
Absorption correction: multi-scan
MULABS (Spek, 2003; Blessing, 1995)
h = 97
Tmin = 0.965, Tmax = 0.996k = 1414
11729 measured reflectionsl = 1616
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.065H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.166 w = 1/[σ2(Fo2) + (0.0714P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.95(Δ/σ)max < 0.001
4108 reflectionsΔρmax = 0.32 e Å3
316 parametersΔρmin = 0.36 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.023 (4)
Crystal data top
C20H20F3N5O4Sγ = 104.491 (14)°
Mr = 483.47V = 1099.9 (3) Å3
Triclinic, P1Z = 2
a = 7.5478 (14) ÅMo Kα radiation
b = 11.941 (2) ŵ = 0.21 mm1
c = 13.530 (2) ÅT = 173 K
α = 103.996 (14)°0.17 × 0.11 × 0.02 mm
β = 101.670 (15)°
Data collection top
STOE IPDS II two-circle-
diffractometer
4108 independent reflections
Absorption correction: multi-scan
MULABS (Spek, 2003; Blessing, 1995)
2452 reflections with I > 2σ(I)
Tmin = 0.965, Tmax = 0.996Rint = 0.091
11729 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0650 restraints
wR(F2) = 0.166H atoms treated by a mixture of independent and constrained refinement
S = 0.95Δρmax = 0.32 e Å3
4108 reflectionsΔρmin = 0.36 e Å3
316 parameters
Special details top

Experimental.

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
S10.50971 (16)0.62448 (9)0.13129 (9)0.0458 (3)
O1S0.4647 (5)0.4967 (2)0.1358 (3)0.0557 (8)
C1S0.5563 (10)0.7168 (5)0.2632 (5)0.0856 (19)
H1S10.43760.70440.28410.128*
H1S20.60830.80250.26800.128*
H1S30.64870.69490.31070.128*
C2S0.7445 (7)0.6686 (4)0.1193 (4)0.0541 (11)
H2S10.74640.62400.04870.081*
H2S20.83000.65000.17350.081*
H2S30.78710.75610.12930.081*
N10.7916 (4)0.7730 (3)0.6740 (3)0.0316 (7)
H10.754 (6)0.738 (4)0.611 (3)0.040 (12)*
N20.8494 (4)0.7069 (3)0.7317 (2)0.0321 (7)
C30.8468 (5)0.5961 (3)0.6855 (3)0.0326 (8)
C310.9199 (6)0.5368 (4)0.7632 (3)0.0391 (9)
O310.9171 (5)0.4300 (3)0.7345 (2)0.0516 (8)
C320.9941 (7)0.6095 (4)0.8792 (3)0.0476 (11)
H32A0.88750.62200.90660.071*
H32B1.08440.68850.88790.071*
H32C1.05870.56530.91860.071*
C40.7819 (5)0.5376 (3)0.5669 (3)0.0331 (8)
O410.7212 (4)0.5922 (2)0.5066 (2)0.0403 (7)
N50.7990 (5)0.4258 (3)0.5324 (2)0.0339 (7)
H50.845 (6)0.394 (4)0.589 (3)0.054 (13)*
C110.7977 (5)0.8916 (3)0.7249 (3)0.0348 (9)
C120.7627 (5)0.9682 (3)0.6638 (3)0.0361 (9)
C130.7635 (6)1.0856 (4)0.7151 (4)0.0493 (11)
H130.74111.13780.67430.059*
C140.7965 (7)1.1267 (4)0.8239 (4)0.0562 (12)
H140.79291.20540.85770.067*
C150.8348 (6)1.0510 (4)0.8830 (4)0.0518 (11)
H150.86091.07930.95800.062*
C160.8355 (6)0.9351 (4)0.8346 (3)0.0426 (10)
H160.86210.88480.87650.051*
C170.7271 (6)0.9258 (4)0.5462 (3)0.0397 (9)
F10.5689 (3)0.8273 (2)0.49774 (17)0.0454 (6)
F20.7004 (4)1.0103 (2)0.4994 (2)0.0551 (7)
F30.8703 (3)0.8917 (2)0.51621 (19)0.0479 (6)
C510.7531 (5)0.3478 (3)0.4275 (3)0.0327 (8)
C520.6655 (5)0.3738 (3)0.3373 (3)0.0313 (8)
H520.63680.44770.34210.038*
C530.6236 (5)0.2848 (3)0.2408 (3)0.0317 (8)
C540.6653 (5)0.1758 (3)0.2319 (3)0.0331 (8)
C550.7525 (5)0.1505 (3)0.3207 (3)0.0336 (8)
H550.78030.07630.31500.040*
C560.7974 (5)0.2381 (3)0.4182 (3)0.0333 (8)
H560.85960.22410.48030.040*
N570.5347 (5)0.2801 (3)0.1374 (2)0.0372 (8)
H570.508 (6)0.344 (4)0.125 (3)0.043 (11)*
C580.5177 (6)0.1715 (3)0.0662 (3)0.0393 (9)
O580.4399 (5)0.1368 (2)0.0309 (2)0.0484 (8)
N590.6035 (5)0.1099 (3)0.1242 (3)0.0369 (8)
H590.602 (6)0.044 (4)0.103 (3)0.033 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0469 (6)0.0313 (5)0.0601 (7)0.0178 (5)0.0050 (5)0.0182 (5)
O1S0.072 (2)0.0297 (15)0.071 (2)0.0220 (15)0.0165 (16)0.0208 (14)
C1S0.097 (5)0.058 (3)0.086 (4)0.019 (3)0.034 (3)0.007 (3)
C2S0.051 (3)0.058 (3)0.059 (3)0.023 (2)0.015 (2)0.022 (2)
N10.0345 (18)0.0260 (16)0.0355 (18)0.0111 (13)0.0083 (14)0.0114 (14)
N20.0294 (16)0.0316 (17)0.0409 (17)0.0116 (13)0.0123 (13)0.0171 (13)
C30.032 (2)0.0280 (19)0.041 (2)0.0115 (16)0.0097 (16)0.0152 (15)
C310.041 (2)0.037 (2)0.049 (2)0.0177 (18)0.0122 (18)0.0246 (18)
O310.071 (2)0.0423 (17)0.0500 (17)0.0280 (15)0.0088 (14)0.0250 (13)
C320.052 (3)0.051 (3)0.043 (2)0.018 (2)0.008 (2)0.023 (2)
C40.028 (2)0.0256 (18)0.044 (2)0.0070 (15)0.0057 (16)0.0134 (16)
O410.0509 (17)0.0294 (14)0.0387 (14)0.0154 (12)0.0026 (12)0.0128 (11)
N50.0397 (18)0.0257 (16)0.0382 (17)0.0130 (14)0.0077 (14)0.0131 (13)
C110.029 (2)0.0265 (19)0.048 (2)0.0082 (15)0.0075 (16)0.0122 (16)
C120.0273 (19)0.0269 (19)0.054 (2)0.0079 (15)0.0101 (17)0.0144 (17)
C130.049 (3)0.031 (2)0.072 (3)0.020 (2)0.016 (2)0.017 (2)
C140.054 (3)0.029 (2)0.073 (3)0.011 (2)0.013 (2)0.001 (2)
C150.047 (3)0.046 (3)0.048 (2)0.011 (2)0.005 (2)0.0015 (19)
C160.037 (2)0.034 (2)0.048 (2)0.0094 (17)0.0050 (18)0.0046 (17)
C170.037 (2)0.035 (2)0.057 (2)0.0166 (18)0.0185 (19)0.0228 (18)
F10.0424 (14)0.0451 (14)0.0466 (13)0.0099 (11)0.0079 (10)0.0182 (10)
F20.0686 (18)0.0478 (14)0.0733 (16)0.0322 (13)0.0274 (13)0.0412 (13)
F30.0461 (14)0.0534 (15)0.0633 (15)0.0276 (12)0.0254 (11)0.0311 (12)
C510.032 (2)0.0268 (18)0.042 (2)0.0101 (15)0.0087 (16)0.0157 (15)
C520.030 (2)0.0203 (17)0.045 (2)0.0087 (14)0.0093 (16)0.0126 (15)
C530.0303 (19)0.0278 (18)0.042 (2)0.0115 (15)0.0096 (16)0.0165 (16)
C540.0300 (19)0.0245 (18)0.047 (2)0.0083 (15)0.0112 (16)0.0143 (16)
C550.034 (2)0.0241 (18)0.052 (2)0.0133 (15)0.0166 (17)0.0202 (17)
C560.0296 (19)0.0302 (19)0.046 (2)0.0118 (15)0.0104 (16)0.0196 (17)
N570.045 (2)0.0203 (16)0.0464 (19)0.0152 (14)0.0055 (15)0.0106 (14)
C580.044 (2)0.0244 (19)0.048 (2)0.0124 (17)0.0084 (18)0.0110 (17)
O580.066 (2)0.0306 (15)0.0435 (16)0.0199 (14)0.0002 (14)0.0092 (12)
N590.046 (2)0.0213 (16)0.0440 (19)0.0158 (15)0.0077 (15)0.0102 (14)
Geometric parameters (Å, º) top
S1—O1S1.497 (3)C12—C171.494 (6)
S1—C1S1.768 (6)C13—C141.383 (7)
S1—C2S1.770 (5)C13—H130.9500
C1S—H1S10.9800C14—C151.387 (7)
C1S—H1S20.9800C14—H140.9500
C1S—H1S30.9800C15—C161.382 (6)
C2S—H2S10.9800C15—H150.9500
C2S—H2S20.9800C16—H160.9500
C2S—H2S30.9800C17—F31.348 (5)
N1—N21.325 (4)C17—F21.349 (4)
N1—C111.402 (5)C17—F11.359 (5)
N1—H10.81 (4)C51—C521.408 (5)
N2—C31.313 (5)C51—C561.415 (5)
C3—C311.495 (5)C52—C531.387 (5)
C3—C41.507 (5)C52—H520.9500
C31—O311.233 (5)C53—C541.397 (5)
C31—C321.507 (6)C53—N571.406 (5)
C32—H32A0.9800C54—C551.386 (5)
C32—H32B0.9800C54—N591.396 (5)
C32—H32C0.9800C55—C561.387 (5)
C4—O411.248 (4)C55—H550.9500
C4—N51.351 (5)C56—H560.9500
N5—C511.414 (5)N57—C581.375 (5)
N5—H50.97 (4)N57—H570.88 (5)
C11—C161.391 (6)C58—O581.244 (5)
C11—C121.409 (5)C58—N591.373 (5)
C12—C131.404 (5)N59—H590.77 (4)
O1S—S1—C1S105.4 (3)C14—C13—H13119.5
O1S—S1—C2S107.5 (2)C12—C13—H13119.5
C1S—S1—C2S97.9 (3)C13—C14—C15118.9 (4)
S1—C1S—H1S1109.5C13—C14—H14120.5
S1—C1S—H1S2109.5C15—C14—H14120.5
H1S1—C1S—H1S2109.5C16—C15—C14121.1 (4)
S1—C1S—H1S3109.5C16—C15—H15119.4
H1S1—C1S—H1S3109.5C14—C15—H15119.4
H1S2—C1S—H1S3109.5C15—C16—C11120.5 (4)
S1—C2S—H2S1109.5C15—C16—H16119.7
S1—C2S—H2S2109.5C11—C16—H16119.7
H2S1—C2S—H2S2109.5F3—C17—F2106.2 (3)
S1—C2S—H2S3109.5F3—C17—F1105.3 (3)
H2S1—C2S—H2S3109.5F2—C17—F1105.5 (3)
H2S2—C2S—H2S3109.5F3—C17—C12113.1 (3)
N2—N1—C11119.4 (3)F2—C17—C12113.6 (3)
N2—N1—H1114 (3)F1—C17—C12112.5 (3)
C11—N1—H1127 (3)C52—C51—N5123.6 (3)
C3—N2—N1120.3 (3)C52—C51—C56121.0 (3)
N2—C3—C31112.5 (3)N5—C51—C56115.4 (3)
N2—C3—C4123.3 (3)C53—C52—C51115.9 (3)
C31—C3—C4124.2 (3)C53—C52—H52122.1
O31—C31—C3121.4 (4)C51—C52—H52122.1
O31—C31—C32120.0 (3)C52—C53—C54123.0 (3)
C3—C31—C32118.6 (3)C52—C53—N57130.7 (3)
C31—C32—H32A109.5C54—C53—N57106.3 (3)
C31—C32—H32B109.5C55—C54—N59132.0 (3)
H32A—C32—H32B109.5C55—C54—C53121.1 (3)
C31—C32—H32C109.5N59—C54—C53106.8 (3)
H32A—C32—H32C109.5C54—C55—C56117.2 (3)
H32B—C32—H32C109.5C54—C55—H55121.4
O41—C4—N5123.6 (3)C56—C55—H55121.4
O41—C4—C3120.8 (3)C55—C56—C51121.7 (3)
N5—C4—C3115.6 (3)C55—C56—H56119.2
C4—N5—C51129.6 (3)C51—C56—H56119.2
C4—N5—H5114 (3)C58—N57—C53110.2 (3)
C51—N5—H5116 (3)C58—N57—H57129 (3)
C16—C11—N1121.4 (3)C53—N57—H57121 (3)
C16—C11—C12119.1 (4)O58—C58—N59127.4 (3)
N1—C11—C12119.5 (3)O58—C58—N57126.5 (3)
C13—C12—C11119.2 (4)N59—C58—N57106.2 (3)
C13—C12—C17120.2 (4)C58—N59—C54110.4 (3)
C11—C12—C17120.6 (3)C58—N59—H59125 (3)
C14—C13—C12121.1 (4)C54—N59—H59123 (3)
C11—N1—N2—C3179.3 (3)C13—C12—C17—F20.9 (5)
N1—N2—C3—C31179.1 (3)C11—C12—C17—F2178.5 (3)
N1—N2—C3—C40.6 (5)C13—C12—C17—F1118.9 (4)
N2—C3—C31—O31175.6 (4)C11—C12—C17—F161.7 (5)
C4—C3—C31—O316.0 (6)C4—N5—C51—C524.3 (6)
N2—C3—C31—C323.1 (5)C4—N5—C51—C56177.0 (4)
C4—C3—C31—C32175.4 (4)N5—C51—C52—C53177.5 (3)
N2—C3—C4—O412.1 (6)C56—C51—C52—C531.1 (5)
C31—C3—C4—O41179.5 (4)C51—C52—C53—C540.3 (6)
N2—C3—C4—N5176.2 (4)C51—C52—C53—N57178.7 (4)
C31—C3—C4—N52.1 (5)C52—C53—C54—C550.1 (6)
O41—C4—N5—C511.2 (6)N57—C53—C54—C55179.2 (3)
C3—C4—N5—C51179.5 (4)C52—C53—C54—N59180.0 (4)
N2—N1—C11—C169.7 (5)N57—C53—C54—N590.9 (4)
N2—N1—C11—C12171.0 (3)N59—C54—C55—C56179.5 (4)
C16—C11—C12—C131.2 (6)C53—C54—C55—C560.4 (6)
N1—C11—C12—C13178.2 (4)C54—C55—C56—C511.2 (6)
C16—C11—C12—C17178.2 (4)C52—C51—C56—C551.7 (6)
N1—C11—C12—C172.4 (6)N5—C51—C56—C55177.0 (3)
C11—C12—C13—C140.5 (6)C52—C53—N57—C58178.0 (4)
C17—C12—C13—C14179.9 (4)C54—C53—N57—C581.1 (4)
C12—C13—C14—C151.9 (7)C53—N57—C58—O58177.4 (4)
C13—C14—C15—C161.7 (7)C53—N57—C58—N592.6 (4)
C14—C15—C16—C110.0 (7)O58—C58—N59—C54176.8 (4)
N1—C11—C16—C15177.9 (4)N57—C58—N59—C543.2 (4)
C12—C11—C16—C151.4 (6)C55—C54—N59—C58177.6 (4)
C13—C12—C17—F3122.0 (4)C53—C54—N59—C582.5 (4)
C11—C12—C17—F357.5 (5)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O410.81 (4)1.88 (4)2.578 (4)144 (4)
N5—H5···O310.97 (4)1.85 (4)2.684 (4)143 (4)
N57—H57···O1S0.88 (5)1.91 (5)2.770 (4)165 (4)
N59—H59···O58i0.77 (4)2.05 (4)2.815 (4)172 (4)
Symmetry code: (i) x+1, y, z.

Experimental details

(PO36)(PO62)(PY151)(PY154)
Crystal data
Chemical formulaC17H13ClN6O5C17H14N6O5C18H15N5O5C18H14F3N5O3
Mr416.78382.34381.35405.34
Crystal system, space groupTriclinic, P1Triclinic, P1Triclinic, P1Monoclinic, P21/c
Temperature (K)293293293293
a, b, c (Å)8.6533 (7), 9.1170 (6), 11.3831 (6)7.2689 (8), 10.3176 (14), 12.1761 (15)5.12970 (14), 9.2292 (3), 17.4094 (6)14.5848 (5), 8.5448 (2), 13.7794 (4)
α, β, γ (°)74.717 (2), 81.597 (4), 88.982 (3)96.462 (6), 95.869 (4), 109.849 (8)95.857 (2), 95.5056 (17), 91.7980 (13)90, 96.0670 (19), 90
V3)856.78 (10)843.78 (19)815.42 (4)1707.62 (9)
Z2224
Radiation typeCu Kα1, λ = 1.54056 ÅCu Kα1, λ = 1.54056 ÅCu Kα1, λ = 1.54056 ÅCu Kα1, λ = 1.54056 Å
µ (mm1)2.410.970.981.15
Specimen shape, size (mm)Cylinder, 10 × 0.7Flat_sheet, 10 × 1.2Cylinder, 10 × 0.7Cylinder, 10 × 0.7
Data collection
DiffractometerSTOE-Stadi-P
diffractometer
STOE-Stadi-P
diffractometer
STOE-Stadi-P
diffractometer
STOE-Stadi-P
diffractometer
Specimen mounting'glass capillary'Flat sample holder'glass capillary''glass capillary'
Data collection modeTransmissionTransmissionTransmissionTransmission
Data collection methodStepStepStepStep
Absorption correction
Tmin, Tmax
No. of measured, independent and
observed reflections
Rint
θ values (°)2θmin = 2.00 2θmax = 75.00 2θstep = 0.012θmin = 3.00 2θmax = 34.00 2θstep = 0.022θmin = 4.00 2θmax = 74.00 2θstep = 0.012θmin = 3.00 2θmax = 70.00 2θstep = 0.01
Distance from source to specimen (mm)
Refinement
R factors and goodness of fitRp = 0.029, Rwp = 0.039, Rexp = 0.094, χ2 = 1.103Rp = 0.030, Rwp = 0.040, Rexp = 0.055, χ2 = 1.277Rp = 0.015, Rwp = 0.021, Rexp = 0.054, χ2 = 1.369Rp = 0.036, Rwp = 0.047, Rexp = 0.090, χ2 = 1.369
No. of reflections/data points9800155070006700
No. of parameters191190194180
No. of restraints116118118120
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)


(PY181)(PY194)(BIRZIL)(PY154-DMSO)
Crystal data
Chemical formulaC25H21N7O5C18H17N5O4C18H16ClN5O4C20H20F3N5O4S
Mr499.49367.37401.81483.47
Crystal system, space groupMonoclinic, P21/cMonoclinic, P21/cMonoclinic, C2/cTriclinic, P1
Temperature (K)293293293173
a, b, c (Å)22.5510 (8), 4.96366 (13), 21.2815 (6)14.7172 (16), 5.9852 (5), 20.7919 (13)17.126 (2), 5.036 (2), 42.45 (1)7.5478 (14), 11.941 (2), 13.530 (2)
α, β, γ (°)90, 109.4539 (13), 9090, 114.818 (4), 9090, 97.36 (2), 90103.996 (14), 101.670 (15), 104.491 (14)
V3)2246.16 (12)1662.3 (2)3631 (2)1099.9 (3)
Z4482
Radiation typeCu Kα1, λ = 1.54056 ÅCu Kα1, λ = 1.54056 ÅCu KαMo Kα
µ (mm1)0.890.892.190.21
Specimen shape, size (mm)Cylinder, 10 × 0.7Flat_sheet, 10 × 1.20.5 × 0.25 × 0.050.17 × 0.11 × 0.02
Data collection
DiffractometerSTOE-Stadi-P
diffractometer
STOE-Stadi-P
diffractometer
Nicolet R3 computer-controlled four circle
diffractometer
STOE IPDS II two-circle-
diffractometer
Specimen mounting'glass capillary'Flat sample holder
Data collection modeTransmissionTransmission
Data collection methodStepStep2θ/θ scanω scans
Absorption correctionMulti-scan
MULABS (Spek, 2003; Blessing, 1995)
Tmin, Tmax0.965, 0.996
No. of measured, independent and
observed reflections
2394, 2303, 971 11729, 4108, 2452
Rint0.0470.091
θ values (°)2θmin = 3.00 2θmax = 60.00 2θstep = 0.012θmin = 3.00 2θmax = 34.00 2θstep = 0.02θmax = 55.2, θmin = 4.2θmax = 25.6, θmin = 3.5
Distance from source to specimen (mm)0.5320.608
Refinement
R factors and goodness of fitRp = 0.012, Rwp = 0.015, Rexp = 0.036, χ2 = 1.188Rp = 0.029, Rwp = 0.039, Rexp = 0.048, χ2 = 1.322R[F2 > 2σ(F2)] = 0.078, wR(F2) = 0.198, S = 0.92R[F2 > 2σ(F2)] = 0.065, wR(F2) = 0.166, S = 0.95
No. of reflections/data points5700155023034108
No. of parameters224176254316
No. of restraints16212200
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH atoms treated by a mixture of independent and constrained refinementH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.25, 0.250.32, 0.36

Computer programs: STOE WINXPOW (STOE & CIE GmbH, 2004), Nicolet software, X-AREA (Stoe & Cie, 2001), TOPAS (Coelho, 2006), DASH (David et al., 2006), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), Mercury (Macrae et al., 2006), SHELX97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991), DASH, TOPAS, Mercury, SHELXL97.

Hydrogen-bond geometry (Å, º) for (BIRZIL) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.862.282.616 (9)103.3
C13—H13···O30.932.322.899 (9)119.8
N1—H1···O30.861.872.555 (8)134.9
N3—H3···O20.861.942.685 (8)143.7
N4—H4···O2i0.862.062.919 (9)174.1
N5—H5···O4ii0.861.962.819 (8)173.1
Symmetry codes: (i) x1/2, y1/2, z; (ii) x3/2, y+3/2, z+2.
Hydrogen-bond geometry (Å, º) for (PY154-DMSO) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O410.81 (4)1.88 (4)2.578 (4)144 (4)
N5—H5···O310.97 (4)1.85 (4)2.684 (4)143 (4)
N57—H57···O1S0.88 (5)1.91 (5)2.770 (4)165 (4)
N59—H59···O58i0.77 (4)2.05 (4)2.815 (4)172 (4)
Symmetry code: (i) x+1, y, z.
 

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