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The dihedral angle between the sydnone moiety and methoxy­phenyl ring of the title compound, C20H16N2O4, is 66.32 (10)°. Electron conjugation is observed between the pentadienone group and the attached phenyl ring. In the crystal structure, symmetry-related mol­ecules are linked by weak intermolecular C—H...O interactions to form a sheet-like structure, which lies parallel to the ab plane.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536803011309/cv6197sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536803011309/cv6197Isup2.hkl
Contains datablock I

CCDC reference: 214861

Key indicators

  • Single-crystal X-ray study
  • T = 160 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.044
  • wR factor = 0.119
  • Data-to-parameter ratio = 7.4

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Yellow Alert Alert Level C:
PLAT_601 Alert C Structure Contains Solvent Accessible VOIDS of 40.00 A   3 General Notes
REFLT_03 From the CIF: _diffrn_reflns_theta_max 25.01 From the CIF: _reflns_number_total 1752 Count of symmetry unique reflns 1761 Completeness (_total/calc) 99.49% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 0 Fraction of Friedel pairs measured 0.000 Are heavy atom types Z>Si present no Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.
0 Alert Level A = Potentially serious problem
0 Alert Level B = Potential problem
1 Alert Level C = Please check

Comment top

Sydnones are the product of dehydration of N-nitroso-α-amino acids and are named after the site of their discovery at the University of Sydney (Earl & Mackney, 1935). They have attained importance due, not only to their structural features and chemical properties, but also to their biological properties. Sydnones are less toxic (Pillai et al., 1993), but potent porphyrinogenic (Sutherland et al., 1986; Marks, 1987) and anti-inflammatory (Satyanarayana & Rao, 1995) compounds, and have the effect of scavenging free-radicals (Narla & Rao, 1995). Sydnone halogen derivatives change their colour irreversibly under the influence of UV light (λ < 400 nm) (Hašek et al., 1979). In view of its biological importance, the crystal structure analysis of the title sydnone, (I), was carried out.

The bond lengths in the sydnone ring of (I) agree with the corresponding average values given in Table 1 for other 3,4-disubstituted sydnones (Hašek et al., 1978, 1979; Ueng et al., 1987a,b, 1989; Ajees et al., 2002). The dihedral angles between the planes of the sydnone ring and the attached phenyl ring in the 3,4-disubstituted sydnone derivatives (55–79°) are larger than those in the 3-substituted sydnone derivatives (2–39°; Ueng et al., 1987a). In (I), the dihedral angle between the planes of the sydnone moiety and the methoxyphenyl ring is 66.32 (10)°. The carbonyl group (C14O14) is in an s–cis conformation, as can be seen from the torsion angle C16—C15—C14—O14 of −1.5 (4)°. The pentadienone moiety is effectively planar and its mean plane is oriented at angles of 10.98 (17) and 6.57 (18)° with respect to those of the sydnone and methoxyphenyl rings, respectively. The lengths of the C19—C18 [1.462 (4) Å], C18—C17 [1.333 (5) Å], C17—C16 [1.435 (4) Å], C16—C15 [1.330 (4) Å], C15—C14 [1.471 (3) Å], C14—O14 [1.228 (4) Å] and C14—C4 [1.457 (4) Å] bonds indicate conjugation. Atoms H15 and H16; H17 and H18 are trans to each other. The widening of the bond angles C15—C16—C17 [124.3 (3)°], C16—C17—C18 [123.9 (3)°] and C17—C18—C19 [127.2 (3)°] are significantly larger than the normal value of 120°, and this may be due to steric repulsion between atoms H15 and H17 (2.46 Å), between atoms H16 and H18 (2.41 Å), and between atoms H17 and H20 (2.18 Å). A close intramolecular contact between O5 and H15 (2.43 Å) being a repulsive interaction, may have caused the significant opening of the C5—C4—C14 [129.7 (4)°] and C4—C5—O5 [137.3 (3)°].

In the crystal, atom C8 acts as a hydrogen bond donor and forms a weak intermolecular C—H···O interaction with the carbonyl O14 atom of an adjacent molecule, therely linking the molecules into extended chains which have a graph-set motif of C(8) (Bernstein et al., 1995). Atom C11 atom acts as a donor for an intermolecular C—H···O interaction with atom O5 of the sydnone ring of another adjacent molecule. This weak intermolecular interaction also links the molecules into extended chains which have a graph-set motif of C(7) (Bernstein et al., 1995). The above two weak intermolecular C—H···O interactions are combined to form a sheet-like structure which lies parallel to the ab plane (Fig. 2).

Experimental top

4-Acetyl-3-(4-methoxy)phenylsydnone (2.34 g, 0.01 mol) was suspended in sodium hydroxide solution (0.5 g sodium hydroxide in 5 ml water and 5 ml e thanol) and benzaldehyde (1 g, 0.01 mol) was added. The reaction mixture was stirred for 30 min at room temperature and the precipitate obtained was collected immediately and washed with water. Recrystallization from acetone and ethanol mixture afforded crystals of (I) suitable for X-ray analysis (m.p. 449–451 K).

Refinement top

The methyl H atoms were constrained to an ideal geometry (C—H = 0.98 Å) with Uiso(H) = 1.5Ueq(C), but were allowed to rotate freely about the C—C bonds. All remaining H atoms were placed in geometrically idealized positions (C—H = 0.95 Å) and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C). Although the molecule is achiral, the structure possesses a polar axis. Due to the absence of any significant anomalous scatterers in the compound, the absolute structure was assigned arbitrarily and Friedel pairs were merged before the final refinement. Reflections 001 and 101 were partially obscured by the beam stop and were omitted.

Computing details top

Data collection: COLLECT (Nonius, 2000); cell refinement: DENZO–SMN (Otwinowski & Minor, 1997); data reduction: DENZO–SMN (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. View of the molecule of (I), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented by circles of arbitrary radii.
[Figure 2] Fig. 2. Packing diagram showing C—H···O interactions, viewed down the b axis.
3-(4-Methoxyphenyl)-4-(4-phenyl-1,3-butadienoyl)sydnone top
Crystal data top
C20H16N2O4F(000) = 364
Mr = 348.35Dx = 1.317 Mg m3
Monoclinic, P21Melting point: 449 K
Hall symbol: P 2ybMo Kα radiation, λ = 0.71073 Å
a = 12.0961 (8) ÅCell parameters from 1742 reflections
b = 4.7750 (4) Åθ = 1.0–25.0°
c = 15.3516 (12) ŵ = 0.09 mm1
β = 97.719 (3)°T = 160 K
V = 878.66 (12) Å3Prism, yellow
Z = 20.25 × 0.18 × 0.13 mm
Data collection top
Nonius KappaCCD
diffractometer
1389 reflections with I > 2σ(I)
Radiation source: Nonius FR590 sealed tube generatorRint = 0.078
Horizontally mounted graphite crystal monochromatorθmax = 25.0°, θmin = 2.3°
Detector resolution: 9 pixels mm-1h = 014
ϕ and ω scans with κ offsetsk = 05
1752 measured reflectionsl = 1818
1752 independent reflections
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)] = 0.044H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.120 w = 1/[σ2(Fo2) + (0.0734P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
1752 reflectionsΔρmax = 0.18 e Å3
237 parametersΔρmin = 0.17 e Å3
1 restraintExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.049 (11)
Crystal data top
C20H16N2O4V = 878.66 (12) Å3
Mr = 348.35Z = 2
Monoclinic, P21Mo Kα radiation
a = 12.0961 (8) ŵ = 0.09 mm1
b = 4.7750 (4) ÅT = 160 K
c = 15.3516 (12) Å0.25 × 0.18 × 0.13 mm
β = 97.719 (3)°
Data collection top
Nonius KappaCCD
diffractometer
1389 reflections with I > 2σ(I)
1752 measured reflectionsRint = 0.078
1752 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0441 restraint
wR(F2) = 0.120H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 0.18 e Å3
1752 reflectionsΔρmin = 0.17 e Å3
237 parameters
Special details top

Experimental. Solvent used: Acetone-Ethanol Cooling Device: Oxford Cryosystems Cryostream 700 Crystal mount: glued on a glass fibre Mosaicity (°.): 1.959 (5) Frames collected: 292 Seconds exposure per frame: 52 Degrees rotation per frame: 1.5 Crystal-Detector distance (mm): 30.0

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
O10.56558 (17)0.6640 (5)0.98738 (13)0.0548 (6)
O50.51971 (16)0.5667 (5)0.84256 (13)0.0580 (7)
O121.04462 (17)0.0971 (7)1.25044 (14)0.0682 (8)
O140.78389 (15)0.0615 (5)0.92462 (11)0.0481 (6)
N20.6412 (2)0.5766 (6)1.05647 (16)0.0554 (8)
N30.70059 (19)0.3854 (6)1.02391 (14)0.0456 (7)
C40.6713 (2)0.3339 (7)0.93643 (17)0.0424 (7)
C50.5812 (2)0.5154 (8)0.90953 (19)0.0489 (8)
C60.7893 (2)0.2604 (8)1.08461 (17)0.0474 (8)
C70.8990 (2)0.3071 (10)1.07271 (19)0.0604 (10)
H70.91630.42071.02560.073*
C80.9823 (2)0.1874 (10)1.12980 (19)0.0614 (11)
H81.05820.21951.12290.074*
C90.9559 (2)0.0199 (9)1.1974 (2)0.0562 (9)
C100.8454 (2)0.0252 (8)1.20951 (18)0.0514 (8)
H100.82780.13961.25640.062*
C110.7609 (2)0.0995 (7)1.15192 (17)0.0460 (8)
H110.68480.07331.15920.055*
C131.0209 (3)0.2849 (10)1.3166 (2)0.0723 (11)
H1310.97380.43741.28980.108*
H1321.09070.36221.34670.108*
H1330.98150.18521.35900.108*
C140.7191 (2)0.1128 (7)0.88778 (17)0.0415 (7)
C150.6827 (2)0.1097 (7)0.79242 (17)0.0462 (8)
H150.63380.25290.76750.055*
C160.7156 (2)0.0855 (8)0.73964 (17)0.0454 (7)
H160.76510.22630.76530.054*
C170.6811 (2)0.0975 (9)0.64653 (17)0.0499 (8)
H170.63000.04010.62100.060*
C180.7164 (3)0.2902 (8)0.59382 (18)0.0539 (9)
H180.76650.42720.62110.065*
C190.6867 (3)0.3138 (8)0.49861 (17)0.0530 (9)
C200.6063 (3)0.1447 (10)0.45160 (19)0.0632 (11)
H200.56870.00780.48160.076*
C210.5802 (3)0.1741 (10)0.36056 (19)0.0683 (12)
H210.52550.05590.32920.082*
C220.6327 (3)0.3718 (10)0.3161 (2)0.0711 (12)
H220.61440.39160.25420.085*
C230.7116 (4)0.5400 (12)0.3615 (2)0.0824 (13)
H230.74800.67760.33090.099*
C240.7396 (3)0.5127 (10)0.45278 (19)0.0706 (11)
H240.79490.63090.48340.085*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0601 (13)0.0478 (14)0.0600 (12)0.0008 (12)0.0206 (10)0.0054 (12)
O50.0555 (12)0.0631 (17)0.0565 (12)0.0065 (12)0.0119 (10)0.0097 (12)
O120.0511 (12)0.094 (2)0.0576 (13)0.0002 (15)0.0003 (10)0.0040 (16)
O140.0520 (11)0.0540 (14)0.0386 (10)0.0036 (12)0.0067 (8)0.0035 (10)
N20.0580 (15)0.055 (2)0.0565 (15)0.0069 (15)0.0192 (13)0.0141 (15)
N30.0496 (14)0.0462 (17)0.0435 (13)0.0078 (13)0.0155 (11)0.0118 (13)
C40.0411 (15)0.049 (2)0.0381 (15)0.0043 (15)0.0090 (12)0.0033 (14)
C50.0527 (17)0.0463 (19)0.0508 (18)0.0063 (15)0.0182 (15)0.0019 (16)
C60.0447 (16)0.060 (2)0.0374 (15)0.0069 (15)0.0073 (13)0.0147 (16)
C70.0535 (18)0.089 (3)0.0402 (15)0.0208 (19)0.0108 (14)0.0110 (18)
C80.0461 (17)0.095 (3)0.0439 (16)0.012 (2)0.0102 (14)0.015 (2)
C90.0460 (17)0.073 (2)0.0490 (16)0.0040 (17)0.0039 (14)0.0221 (18)
C100.0532 (17)0.058 (2)0.0439 (16)0.0068 (17)0.0088 (13)0.0114 (16)
C110.0447 (15)0.055 (2)0.0399 (14)0.0074 (16)0.0107 (12)0.0120 (16)
C130.064 (2)0.076 (3)0.073 (2)0.006 (2)0.0020 (17)0.008 (2)
C140.0388 (14)0.0465 (19)0.0403 (15)0.0024 (15)0.0097 (12)0.0027 (16)
C150.0461 (16)0.053 (2)0.0391 (14)0.0006 (16)0.0046 (12)0.0013 (16)
C160.0476 (15)0.053 (2)0.0359 (14)0.0025 (17)0.0064 (12)0.0037 (15)
C170.0493 (16)0.062 (2)0.0369 (15)0.0016 (17)0.0019 (12)0.0021 (16)
C180.0611 (18)0.060 (2)0.0410 (15)0.0050 (17)0.0079 (13)0.0100 (16)
C190.0606 (18)0.060 (2)0.0383 (16)0.0125 (19)0.0077 (14)0.0079 (16)
C200.0592 (19)0.089 (3)0.0405 (16)0.012 (2)0.0043 (14)0.0117 (19)
C210.065 (2)0.098 (3)0.0408 (17)0.023 (2)0.0001 (15)0.008 (2)
C220.089 (3)0.087 (3)0.0384 (17)0.029 (3)0.0141 (17)0.008 (2)
C230.120 (3)0.082 (3)0.049 (2)0.009 (3)0.030 (2)0.019 (2)
C240.101 (3)0.072 (3)0.0413 (17)0.003 (2)0.0198 (17)0.0076 (19)
Geometric parameters (Å, º) top
O1—N21.369 (3)C13—H1320.9800
O1—C51.424 (4)C13—H1330.9800
O5—C51.210 (3)C14—C151.471 (3)
O12—C91.375 (4)C15—C161.330 (4)
O12—C131.413 (5)C15—H150.9500
O14—C141.228 (4)C16—C171.435 (4)
N2—N31.303 (4)C16—H160.9500
N3—C41.364 (3)C17—C181.333 (5)
N3—C61.452 (4)C17—H170.9500
C4—C51.411 (5)C18—C191.462 (4)
C4—C141.457 (4)C18—H180.9500
C6—C111.368 (4)C19—C241.388 (5)
C6—C71.381 (4)C19—C201.389 (5)
C7—C81.369 (5)C20—C211.398 (4)
C7—H70.9500C20—H200.9500
C8—C91.382 (5)C21—C221.370 (6)
C8—H80.9500C21—H210.9500
C9—C101.391 (4)C22—C231.365 (6)
C10—C111.392 (4)C22—H220.9500
C10—H100.9500C23—C241.402 (4)
C11—H110.9500C23—H230.9500
C13—H1310.9800C24—H240.9500
N2—O1—C5110.4 (2)H132—C13—H133109.5
C9—O12—C13117.7 (3)O14—C14—C4121.9 (2)
N3—N2—O1105.2 (2)O14—C14—C15122.6 (3)
N2—N3—C4114.9 (3)C4—C14—C15115.6 (3)
N2—N3—C6116.1 (2)C16—C15—C14122.6 (3)
C4—N3—C6129.0 (3)C16—C15—H15118.7
N3—C4—C5105.4 (3)C14—C15—H15118.7
N3—C4—C14124.5 (3)C15—C16—C17124.3 (3)
C5—C4—C14129.7 (2)C15—C16—H16117.8
O5—C5—C4137.3 (3)C17—C16—H16117.8
O5—C5—O1118.5 (3)C18—C17—C16123.9 (3)
C4—C5—O1104.2 (2)C18—C17—H17118.1
C11—C6—C7122.3 (3)C16—C17—H17118.1
C11—C6—N3118.4 (2)C17—C18—C19127.2 (3)
C7—C6—N3119.3 (3)C17—C18—H18116.4
C8—C7—C6119.1 (3)C19—C18—H18116.4
C8—C7—H7120.5C24—C19—C20118.2 (3)
C6—C7—H7120.5C24—C19—C18119.4 (3)
C7—C8—C9119.9 (3)C20—C19—C18122.4 (3)
C7—C8—H8120.1C19—C20—C21120.6 (4)
C9—C8—H8120.1C19—C20—H20119.7
O12—C9—C8116.1 (3)C21—C20—H20119.7
O12—C9—C10123.1 (3)C22—C21—C20120.7 (4)
C8—C9—C10120.9 (3)C22—C21—H21119.7
C9—C10—C11119.1 (3)C20—C21—H21119.7
C9—C10—H10120.5C23—C22—C21119.3 (3)
C11—C10—H10120.5C23—C22—H22120.3
C6—C11—C10118.8 (2)C21—C22—H22120.3
C6—C11—H11120.6C22—C23—C24121.0 (4)
C10—C11—H11120.6C22—C23—H23119.5
O12—C13—H131109.5C24—C23—H23119.5
O12—C13—H132109.5C19—C24—C23120.3 (4)
H131—C13—H132109.5C19—C24—H24119.9
O12—C13—H133109.5C23—C24—H24119.9
H131—C13—H133109.5
C5—O1—N2—N30.1 (3)O12—C9—C10—C11179.3 (3)
O1—N2—N3—C40.1 (3)C8—C9—C10—C110.4 (5)
O1—N2—N3—C6179.1 (2)C7—C6—C11—C101.1 (5)
N2—N3—C4—C50.2 (3)N3—C6—C11—C10178.9 (3)
C6—N3—C4—C5179.0 (3)C9—C10—C11—C60.7 (5)
N2—N3—C4—C14174.3 (3)N3—C4—C14—O146.4 (4)
C6—N3—C4—C146.9 (5)C5—C4—C14—O14166.2 (3)
N3—C4—C5—O5179.0 (4)N3—C4—C14—C15174.9 (3)
C14—C4—C5—O55.3 (6)C5—C4—C14—C1512.5 (4)
N3—C4—C5—O10.2 (3)O14—C14—C15—C161.5 (4)
C14—C4—C5—O1173.9 (3)C4—C14—C15—C16177.3 (3)
N2—O1—C5—O5179.2 (3)C14—C15—C16—C17179.3 (3)
N2—O1—C5—C40.2 (3)C15—C16—C17—C18178.4 (3)
N2—N3—C6—C1166.6 (4)C16—C17—C18—C19179.0 (3)
C4—N3—C6—C11114.6 (3)C17—C18—C19—C24174.0 (3)
N2—N3—C6—C7113.4 (3)C17—C18—C19—C206.4 (5)
C4—N3—C6—C765.4 (5)C24—C19—C20—C210.4 (5)
C11—C6—C7—C80.4 (5)C18—C19—C20—C21179.9 (3)
N3—C6—C7—C8179.6 (3)C19—C20—C21—C220.6 (6)
C6—C7—C8—C90.8 (6)C20—C21—C22—C230.3 (6)
C13—O12—C9—C8175.8 (3)C21—C22—C23—C240.1 (6)
C13—O12—C9—C104.0 (5)C20—C19—C24—C230.1 (6)
C7—C8—C9—O12178.5 (4)C18—C19—C24—C23179.5 (4)
C7—C8—C9—C101.2 (5)C22—C23—C24—C190.3 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O14i0.952.383.281 (4)159
C11—H11···O5ii0.952.473.410 (3)170
Symmetry codes: (i) x+2, y1/2, z+2; (ii) x+1, y+1/2, z+2.

Experimental details

Crystal data
Chemical formulaC20H16N2O4
Mr348.35
Crystal system, space groupMonoclinic, P21
Temperature (K)160
a, b, c (Å)12.0961 (8), 4.7750 (4), 15.3516 (12)
β (°) 97.719 (3)
V3)878.66 (12)
Z2
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.25 × 0.18 × 0.13
Data collection
DiffractometerNonius KappaCCD
diffractometer
Absorption correction
No. of measured, independent and
observed [I > 2σ(I)] reflections
1752, 1752, 1389
Rint0.078
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.120, 1.05
No. of reflections1752
No. of parameters237
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.18, 0.17

Computer programs: COLLECT (Nonius, 2000), DENZO–SMN (Otwinowski & Minor, 1997) and SCALEPACK, SIR92 (Altomare et al., 1994), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997), SHELXL97 and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8···O14i0.952.383.281 (4)159
C11—H11···O5ii0.952.473.410 (3)170
Symmetry codes: (i) x+2, y1/2, z+2; (ii) x+1, y+1/2, z+2.
Comparison of the bond lengths (Å) in the sydnone ring of (I) with the corresponding average values found in 3,4-disubstituted sydnone derivatives top
(I)Average value
O1—C51.424 (4)1.407 (4)
O1—N21.369 (3)1.379 (3)
N2—N31.303 (4)1.310 (3)
N3—C41.364 (3)1.351 (3)
C4—C51.411 (5)1.413 (3)
C5—O51.210 (3)1.206 (3)
 

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