organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

Journal logoIUCrDATA
ISSN: 2414-3146

2-(10-Phenyl­anthracen-9-yl)-2,3-di­hydro-1H-naphtho­[1,8-de][1,3,2]di­aza­borinine

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aShandong Experimental High School, Jinan, 250001, People's Republic of China, and bShandong Shanke Institute for Industrial Development Research, Jinan 250022, People's Republic of China
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 16 June 2025; accepted 25 June 2025; online 1 July 2025)

In the title compound, C30H21BN2, the dihedral angle between the naphtho­[1,8-de][1,3,2]di­aza­borinine moiety and the anthracene ring system is 79.30 (3)°. In the crystal, weak C—H⋯π inter­actions link the mol­ecules into a three-dimensional network.

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

Structure description

Aryl-B(dan) derivatives, where B(dan) is the naphtho­[1,8-de][1,3,2]di­aza­borinine fragment have emerged as not only stable boron-containing regents for coupling reactions (Yoshida et al., 2020[Yoshida, H., Seki, M., Kamio, S., Tanaka, H., Izumi, Y., Li, J., Osaka, I., Abe, M., Andoh, H., Yajima, T., Tani, T. & Tsuchimoto, T. (2020). ACS Catal. 10, 346-351.]), chemosensors for explosives (Wan et al., 2018[Wan, W.-M., Tian, D., Jing, Y.-N., Zhang, X.-Y., Wu, W., Ren, H. & Bao, H.-L. (2018). Angew. Chem. Int. Ed. 57, 15510-15516.]) and per­oxy­nitrite species (Yoon et al., 2024[Yoon, S., Kim, H. Y., Park, S., Cha, M., Kim, Y., Lee, S., Kim, J., Bhang, S. & Kim, Y. (2024). Angew. Chem. Int. Ed. 63, e202411942.]), but also precursors for large NBN-embedded polycyclic aromatic hydro­carbons (Ju et al., 2021[Ju, C.-W., Li, B., Li, L., Yan, G., Cui, C., Ma, X. & Zhao, D. (2021). J. Am. Chem. Soc. 143, 5903-5916.]). Anthracene is a classical polycyclic aromatic hydro­carbon and a promising platform for optoelectronic materials; 9,10-di­phenyl­anthracene is well known as a reference of determining fluorescence quantum yield. Herein, we describe the synthesis and structure of the title compound, C30H21BN2, which is new derivative of a B(dan)-substituted anthracene.

The title compound crystallizes in the monoclinic space group P21/c. The C1–C10/N1/N2/B1 B(dan) moiety is close to planar, with the largest deviation from the least squares plane being −0.041 (1) Å for atom N2. Both the B(dan) unit at the 9-position and the C25–C30 phenyl ring at the 10-position are close to perpendicular to the central C11–C24 anthracene ring system with dihedral angles of 79.30 (3)° and 71.71 (6)°, respectively (Fig. 1[link]). The lengths of the B—N bonds [1.4186 (19) and 1.412 (2) Å] are close to that of a localized B=N double bond (1.40 Å) and much shorter than that of a typical B—N single bond (1.68 Å), which indicates a significant π-electron delocalization in the NBN moiety. As shown in the packing diagram (Fig. 2[link]), weak C—H⋯π inter­actions (Table 1[link]) link the mol­ecules into a three-dimensional network.

Table 1
Hydrogen-bond geometry (Å, °)

Cg1, Cg3, Cg4 and Cg6 are the centroids of the C1/C8/C9/N1/N2/B1, C5–C10, C11–C16 and C18–C23 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C2—H2⋯Cg6i 0.95 2.86 3.7466 (17) 156
C3—H3⋯Cg3ii 0.95 2.85 3.4906 (17) 125
C4—H4⋯Cg1ii 0.95 2.67 3.5538 (18) 156
C6—H6⋯Cg4iii 0.95 2.83 3.6552 (17) 146
C27—H27⋯Cg6iv 0.95 2.73 3.5364 (18) 143
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of the title compound showing 50% displacement ellipsoids.
[Figure 2]
Figure 2
The unit-cell packing of the title compound viewed approximately down [001].

Synthesis and crystallization

The synthesis of 9-B(dan)-10-phenyl-anthracene followed the previously reported procedure (Wan et al., 2018[Wan, W.-M., Tian, D., Jing, Y.-N., Zhang, X.-Y., Wu, W., Ren, H. & Bao, H.-L. (2018). Angew. Chem. Int. Ed. 57, 15510-15516.]). 9-B(OH)2–10-phenyl-anthracene, 1,8-di­amine-naphthalene and anhydrous magnesium sulfate was added into adequate toluene. After heating 12 h at 120°C, the mixture was cooled to room temperature and concentrated under vacuum then purified by column chromatography of silica gel.

Single crystals of the title compound were obtained as pale-yellow plates by slow diffusion of hexane into its chloro­form solution at room temperature. A suitable crystal for collection was chosen under an optical microscope and quickly coated with high vacuum grease (Dow Corning Corporation) to prevent decomposition.

Refinement

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

Table 2
Experimental details

Crystal data
Chemical formula C30H21BN2
Mr 420.30
Crystal system, space group Monoclinic, P21/c
Temperature (K) 150
a, b, c (Å) 17.5431 (7), 8.6734 (3), 14.3967 (5)
β (°) 95.268 (2)
V3) 2181.32 (14)
Z 4
Radiation type Cu Kα
μ (mm−1) 0.57
Crystal size (mm) 0.60 × 0.30 × 0.03
 
Data collection
Diffractometer Bruker APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015[Krause, L., Herbst-Irmer, R., Sheldrick, G. M. & Stalke, D. (2015). J. Appl. Cryst. 48, 3-10.])
Tmin, Tmax 0.727, 0.983
No. of measured, independent and observed [I > 2σ(I)] reflections 21224, 4302, 3582
Rint 0.075
(sin θ/λ)max−1) 0.618
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.066, 0.191, 1.06
No. of reflections 4302
No. of parameters 299
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.31, −0.46
Computer programs: APEX2 and SAINT (Bruker, 2014[Bruker (2014). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]), SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]), SHELXL2014/7 (Sheldrick, 2015[Sheldrick, G. M. (2015). Acta Cryst. C71, 3-8.]) and SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]).

Structural data


Computing details top

2-(10-Phenylanthracen-9-yl)-2,3-dihydro-1H-naphtho[1,8-de][1,3,2]diazaborinine top
Crystal data top
C30H21BN2F(000) = 880
Mr = 420.30Dx = 1.280 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54178 Å
a = 17.5431 (7) ÅCell parameters from 8257 reflections
b = 8.6734 (3) Åθ = 2.5–72.4°
c = 14.3967 (5) ŵ = 0.57 mm1
β = 95.268 (2)°T = 150 K
V = 2181.32 (14) Å3Plate, yellow
Z = 40.60 × 0.30 × 0.03 mm
Data collection top
Bruker APEXII CCD
diffractometer
3582 reflections with I > 2σ(I)
Detector resolution: 8.3 pixels mm-1Rint = 0.075
φ and ω scansθmax = 72.4°, θmin = 2.5°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 2121
Tmin = 0.727, Tmax = 0.983k = 108
21224 measured reflectionsl = 1717
4302 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.066 w = 1/[σ2(Fo2) + (0.1385P)2 + 0.0802P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.191(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.31 e Å3
4302 reflectionsΔρmin = 0.46 e Å3
299 parametersExtinction correction: SHELXL2014/7 (Sheldrick, 2015), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0049 (10)
Primary atom site location: structure-invariant direct methods
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.40392 (7)0.71226 (15)0.48003 (8)0.0253 (3)
H1n0.41020.67080.53600.030*
N20.32303 (7)0.77065 (15)0.34048 (8)0.0258 (3)
H2n0.27870.76300.30690.031*
C10.38142 (8)0.85573 (17)0.30400 (10)0.0229 (3)
C20.37099 (9)0.92903 (18)0.21940 (10)0.0283 (4)
H20.32250.92530.18430.034*
C30.43185 (10)1.00993 (18)0.18426 (11)0.0318 (4)
H30.42371.06230.12620.038*
C40.50265 (10)1.01356 (19)0.23321 (11)0.0309 (4)
H40.54351.06590.20780.037*
C50.58784 (9)0.9433 (2)0.37404 (12)0.0315 (4)
H50.62990.99360.35000.038*
C60.59746 (9)0.8743 (2)0.45948 (11)0.0319 (4)
H60.64610.87830.49430.038*
C70.53651 (9)0.79721 (19)0.49716 (10)0.0275 (4)
H70.54420.75030.55690.033*
C80.46576 (8)0.79027 (17)0.44684 (10)0.0233 (3)
C90.45398 (8)0.86217 (16)0.35783 (10)0.0226 (3)
C100.51564 (9)0.94070 (18)0.32070 (10)0.0264 (4)
C110.29367 (8)0.38239 (19)0.36154 (10)0.0285 (4)
H110.33090.44440.33540.034*
C120.28219 (9)0.2357 (2)0.33022 (11)0.0318 (4)
H120.31110.19640.28280.038*
C130.22677 (9)0.14105 (19)0.36864 (11)0.0313 (4)
H130.21920.03820.34700.038*
C140.18461 (9)0.19629 (19)0.43598 (10)0.0282 (4)
H140.14790.13110.46070.034*
C150.19434 (8)0.35107 (18)0.47053 (10)0.0245 (4)
C160.25144 (8)0.44634 (18)0.43274 (10)0.0241 (3)
C170.26557 (8)0.59722 (18)0.46628 (10)0.0242 (4)
C180.22333 (8)0.65395 (18)0.53736 (10)0.0246 (4)
C190.23519 (9)0.80720 (19)0.57303 (11)0.0287 (4)
H190.27110.87210.54660.034*
C200.19669 (9)0.8622 (2)0.64341 (11)0.0319 (4)
H200.20660.96350.66650.038*
C210.14117 (9)0.7681 (2)0.68292 (11)0.0327 (4)
H210.11420.80690.73220.039*
C220.12693 (9)0.6227 (2)0.64991 (11)0.0292 (4)
H220.08960.56170.67660.035*
C230.16661 (8)0.55915 (18)0.57620 (10)0.0243 (4)
C240.15212 (8)0.40916 (18)0.54149 (10)0.0242 (4)
C250.09206 (8)0.31027 (18)0.57894 (10)0.0253 (4)
C260.02449 (9)0.2781 (2)0.52390 (11)0.0342 (4)
H260.01570.32310.46370.041*
C270.03026 (9)0.1806 (2)0.55622 (13)0.0394 (4)
H270.07600.15930.51790.047*
C280.01857 (10)0.1149 (2)0.64349 (13)0.0382 (4)
H280.05580.04720.66500.046*
C290.04799 (11)0.1482 (2)0.69986 (12)0.0382 (4)
H290.05610.10470.76050.046*
C300.10270 (9)0.2451 (2)0.66742 (10)0.0316 (4)
H300.14810.26720.70630.038*
B10.33158 (10)0.6966 (2)0.42817 (12)0.0240 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0295 (6)0.0258 (7)0.0196 (6)0.0046 (5)0.0034 (5)0.0037 (5)
N20.0264 (6)0.0237 (7)0.0257 (6)0.0020 (5)0.0062 (5)0.0004 (5)
C10.0307 (7)0.0151 (7)0.0221 (7)0.0003 (5)0.0025 (5)0.0026 (5)
C20.0397 (8)0.0203 (8)0.0234 (7)0.0032 (6)0.0042 (6)0.0002 (6)
C30.0521 (9)0.0205 (8)0.0227 (7)0.0015 (7)0.0030 (6)0.0035 (6)
C40.0426 (8)0.0202 (8)0.0306 (8)0.0042 (6)0.0066 (6)0.0003 (6)
C50.0317 (7)0.0285 (9)0.0343 (8)0.0101 (6)0.0031 (6)0.0058 (6)
C60.0282 (7)0.0332 (10)0.0329 (8)0.0060 (6)0.0039 (6)0.0057 (7)
C70.0315 (7)0.0273 (9)0.0225 (7)0.0036 (6)0.0052 (6)0.0017 (6)
C80.0287 (7)0.0191 (8)0.0214 (7)0.0024 (5)0.0016 (5)0.0040 (5)
C90.0302 (7)0.0152 (8)0.0219 (7)0.0012 (5)0.0009 (5)0.0043 (5)
C100.0349 (8)0.0179 (8)0.0263 (7)0.0028 (6)0.0031 (6)0.0050 (6)
C110.0310 (7)0.0274 (9)0.0262 (8)0.0006 (6)0.0022 (6)0.0001 (6)
C120.0371 (8)0.0306 (9)0.0267 (8)0.0043 (7)0.0029 (6)0.0040 (6)
C130.0397 (8)0.0206 (9)0.0314 (8)0.0004 (6)0.0079 (6)0.0044 (6)
C140.0313 (7)0.0245 (9)0.0269 (8)0.0040 (6)0.0071 (6)0.0006 (6)
C150.0267 (7)0.0232 (8)0.0218 (7)0.0027 (6)0.0076 (5)0.0019 (6)
C160.0265 (6)0.0234 (8)0.0211 (7)0.0020 (6)0.0058 (5)0.0005 (6)
C170.0251 (6)0.0241 (8)0.0217 (7)0.0019 (6)0.0062 (5)0.0004 (6)
C180.0256 (7)0.0246 (8)0.0219 (7)0.0027 (6)0.0063 (5)0.0004 (6)
C190.0289 (7)0.0255 (9)0.0302 (8)0.0052 (6)0.0050 (6)0.0016 (6)
C200.0365 (8)0.0242 (9)0.0334 (8)0.0014 (7)0.0054 (6)0.0070 (6)
C210.0356 (8)0.0338 (10)0.0281 (8)0.0010 (7)0.0002 (6)0.0062 (7)
C220.0306 (7)0.0308 (9)0.0254 (7)0.0019 (6)0.0017 (6)0.0006 (6)
C230.0249 (6)0.0256 (8)0.0209 (7)0.0013 (6)0.0063 (5)0.0014 (6)
C240.0243 (6)0.0253 (8)0.0212 (7)0.0027 (6)0.0073 (5)0.0022 (6)
C250.0282 (7)0.0220 (8)0.0248 (7)0.0027 (6)0.0032 (6)0.0009 (6)
C260.0333 (8)0.0380 (10)0.0294 (8)0.0073 (7)0.0072 (6)0.0072 (7)
C270.0311 (8)0.0440 (11)0.0418 (9)0.0119 (7)0.0042 (7)0.0017 (8)
C280.0399 (9)0.0350 (10)0.0408 (9)0.0110 (7)0.0101 (7)0.0023 (7)
C290.0504 (10)0.0370 (10)0.0273 (8)0.0049 (8)0.0035 (7)0.0049 (7)
C300.0363 (8)0.0331 (9)0.0239 (8)0.0041 (7)0.0048 (6)0.0010 (6)
B10.0284 (7)0.0184 (9)0.0244 (8)0.0013 (6)0.0017 (6)0.0043 (6)
Geometric parameters (Å, º) top
N1—H1n0.8800C15—C141.436 (2)
N1—C81.3993 (19)C15—C241.409 (2)
N1—B11.4186 (19)C16—C111.431 (2)
N2—H2n0.8800C16—C151.443 (2)
N2—C11.4030 (19)C17—C161.409 (2)
N2—B11.412 (2)C17—C181.406 (2)
C1—C91.429 (2)C18—C191.433 (2)
C2—C11.371 (2)C18—C231.443 (2)
C2—H20.9500C19—H190.9500
C3—C21.410 (2)C19—C201.355 (2)
C3—H30.9500C20—H200.9500
C4—C31.371 (2)C20—C211.428 (2)
C4—H40.9500C21—H210.9500
C4—C101.409 (2)C21—C221.363 (2)
C5—H50.9500C22—H220.9500
C5—C61.364 (2)C22—C231.432 (2)
C5—C101.420 (2)C24—C231.408 (2)
C6—H60.9500C24—C251.497 (2)
C6—C71.411 (2)C25—C261.392 (2)
C7—H70.9500C25—C301.391 (2)
C7—C81.3799 (19)C26—H260.9500
C8—C91.423 (2)C26—C271.391 (2)
C10—C91.423 (2)C27—H270.9500
C11—H110.9500C27—C281.378 (3)
C11—C121.359 (2)C28—H280.9500
C12—H120.9500C28—C291.390 (3)
C12—C131.423 (2)C29—H290.9500
C13—H130.9500C30—C291.388 (2)
C13—C141.360 (2)C30—H300.9500
C14—H140.9500B1—C171.582 (2)
C8—N1—H1n118.3C24—C15—C16119.87 (14)
C8—N1—B1123.41 (12)C11—C16—C15118.11 (14)
B1—N1—H1n118.3C17—C16—C11121.29 (14)
C1—N2—H2n118.2C17—C16—C15120.60 (14)
C1—N2—B1123.54 (12)C16—C17—B1119.92 (13)
B1—N2—H2n118.2C18—C17—C16119.11 (14)
N2—C1—C9117.52 (12)C18—C17—B1120.87 (13)
C2—C1—N2122.27 (13)C17—C18—C19121.09 (14)
C2—C1—C9120.20 (14)C17—C18—C23120.72 (14)
C1—C2—H2119.8C19—C18—C23118.19 (14)
C1—C2—C3120.39 (14)C18—C19—H19119.1
C3—C2—H2119.8C20—C19—C18121.89 (15)
C2—C3—H3119.8C20—C19—H19119.1
C4—C3—C2120.48 (14)C19—C20—H20119.9
C4—C3—H3119.8C19—C20—C21120.13 (15)
C3—C4—H4119.5C21—C20—H20119.9
C3—C4—C10120.91 (15)C20—C21—H21120.0
C10—C4—H4119.5C22—C21—C20119.98 (15)
C6—C5—H5119.6C22—C21—H21120.0
C6—C5—C10120.74 (14)C21—C22—H22119.0
C10—C5—H5119.6C21—C22—C23121.92 (15)
C5—C6—H6119.4C23—C22—H22119.0
C5—C6—C7121.27 (14)C22—C23—C18117.86 (14)
C7—C6—H6119.4C24—C23—C18119.83 (14)
C6—C7—H7120.1C24—C23—C22122.30 (14)
C8—C7—C6119.71 (14)C15—C24—C25119.38 (14)
C8—C7—H7120.1C23—C24—C15119.86 (13)
N1—C8—C9117.80 (12)C23—C24—C25120.77 (13)
C7—C8—N1122.01 (13)C26—C25—C24120.04 (13)
C7—C8—C9120.19 (14)C30—C25—C24121.55 (13)
C8—C9—C1121.30 (14)C30—C25—C26118.39 (14)
C8—C9—C10119.70 (13)C25—C26—H26119.7
C10—C9—C1119.00 (13)C27—C26—C25120.62 (15)
C4—C10—C5122.65 (14)C27—C26—H26119.7
C4—C10—C9118.97 (14)C26—C27—H27119.8
C5—C10—C9118.39 (14)C28—C27—C26120.46 (15)
C12—C11—H11119.0C28—C27—H27119.8
C12—C11—C16122.02 (15)C27—C28—H28120.2
C16—C11—H11119.0C27—C28—C29119.54 (16)
C11—C12—H12120.1C29—C28—H28120.2
C11—C12—C13119.81 (15)C28—C29—H29120.0
C13—C12—H12120.1C30—C29—C28119.94 (15)
C12—C13—H13119.7C30—C29—H29120.0
C14—C13—C12120.66 (15)C25—C30—H30119.5
C14—C13—H13119.7C29—C30—C25121.03 (14)
C13—C14—H14119.3C29—C30—H30119.5
C13—C14—C15121.42 (15)N1—B1—C17121.18 (13)
C15—C14—H14119.3N2—B1—N1116.33 (14)
C14—C15—C16117.98 (14)N2—B1—C17122.47 (13)
C24—C15—C14122.12 (14)
N1—C8—C9—C10.2 (2)C16—C11—C12—C130.1 (2)
N1—C8—C9—C10179.01 (13)C16—C15—C14—C131.1 (2)
N1—B1—C17—C16100.23 (17)C16—C15—C24—C230.9 (2)
N1—B1—C17—C1876.1 (2)C16—C15—C24—C25178.91 (12)
N2—C1—C9—C82.5 (2)C16—C17—C18—C19179.38 (12)
N2—C1—C9—C10176.75 (12)C16—C17—C18—C230.4 (2)
N2—B1—C17—C1677.95 (19)C17—C16—C11—C12178.19 (13)
N2—B1—C17—C18105.73 (17)C17—C16—C15—C14177.68 (12)
C1—N2—B1—N10.1 (2)C17—C16—C15—C240.1 (2)
C1—N2—B1—C17178.11 (13)C17—C18—C19—C20177.97 (14)
C2—C1—C9—C8178.45 (13)C17—C18—C23—C22178.55 (13)
C2—C1—C9—C102.3 (2)C17—C18—C23—C241.3 (2)
C3—C2—C1—N2178.32 (14)C18—C17—C16—C11179.02 (13)
C3—C2—C1—C90.7 (2)C18—C17—C16—C150.1 (2)
C3—C4—C10—C5179.27 (15)C18—C19—C20—C211.4 (2)
C3—C4—C10—C90.2 (2)C19—C18—C23—C221.62 (19)
C4—C3—C2—C11.4 (2)C19—C18—C23—C24178.57 (12)
C4—C10—C9—C11.8 (2)C19—C20—C21—C220.1 (2)
C4—C10—C9—C8178.90 (14)C20—C21—C22—C230.4 (2)
C5—C6—C7—C80.3 (2)C21—C22—C23—C180.4 (2)
C5—C10—C9—C1178.64 (13)C21—C22—C23—C24179.83 (14)
C5—C10—C9—C80.6 (2)C23—C18—C19—C202.2 (2)
C6—C5—C10—C4178.42 (15)C23—C24—C25—C26109.45 (17)
C6—C5—C10—C91.1 (2)C23—C24—C25—C3072.4 (2)
C6—C7—C8—N1178.50 (14)C24—C15—C14—C13178.80 (13)
C6—C7—C8—C90.8 (2)C24—C25—C26—C27177.03 (16)
C7—C8—C9—C1179.54 (13)C24—C25—C30—C29177.20 (16)
C7—C8—C9—C100.3 (2)C25—C24—C23—C18178.35 (12)
C8—N1—B1—N22.6 (2)C25—C24—C23—C221.8 (2)
C8—N1—B1—C17175.65 (13)C25—C26—C27—C280.3 (3)
C10—C4—C3—C21.9 (2)C25—C30—C29—C280.1 (3)
C10—C5—C6—C70.6 (3)C26—C25—C30—C291.0 (3)
C11—C12—C13—C140.5 (2)C26—C27—C28—C290.9 (3)
C11—C16—C15—C141.50 (19)C27—C28—C29—C301.1 (3)
C11—C16—C15—C24179.29 (12)C30—C25—C26—C271.2 (3)
C12—C13—C14—C150.0 (2)B1—N1—C8—C7176.85 (15)
C14—C15—C24—C23176.77 (12)B1—N1—C8—C92.4 (2)
C14—C15—C24—C253.4 (2)B1—N2—C1—C2178.65 (14)
C15—C16—C11—C121.0 (2)B1—N2—C1—C92.3 (2)
C15—C24—C23—C181.5 (2)B1—C17—C16—C112.6 (2)
C15—C24—C23—C22178.31 (13)B1—C17—C16—C15176.51 (12)
C15—C24—C25—C2670.4 (2)B1—C17—C18—C194.3 (2)
C15—C24—C25—C30107.78 (17)B1—C17—C18—C23175.91 (12)
Hydrogen-bond geometry (Å, º) top
Cg1, Cg3, Cg4 and Cg6 are the centroids of the C1/C8/C9/N1/N2/B1, C5–C10, C11–C16 and C18–C23 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C2—H2···Cg6i0.952.863.7466 (17)156
C3—H3···Cg3ii0.952.853.4906 (17)125
C4—H4···Cg1ii0.952.673.5538 (18)156
C6—H6···Cg4iii0.952.833.6552 (17)146
C27—H27···Cg6iv0.952.733.5364 (18)143
Symmetry codes: (i) x, y+3/2, z1/2; (ii) x+1, y+1/2, z+1/2; (iii) x+1, y+1, z+1; (iv) x, y+1, z+1.
 

Funding information

This work was supported by Natural Science Foundation of Shandong Province (ZR2024QB376).

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