research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

Synthesis and structure of 4-[(2,3,4,5,6-penta­fluoro­phen­­oxy)carbon­yl]phenyl 4-(dec­yl­oxy)benzoate

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aDepartment of Physics, Yuvaraja's College, University of Mysore, Mysore-570005, Karnataka, India, bDepartment of Physics, Government Science College, Chithradurga-577501, Kanataka, India, cDepartment of PG Studies and Research in Physics, Albert Einstein Block, UCS, Tumkur University, Tumkur, Karnataka-572103, India, dRaman Research Institute, C. V. Raman, Avenue, Sadashivanagar, Bangalore, Karnataka, India, and eDepartment of Physics, Yuvaraja's College, University of Mysore, Mysore-570005, Karnaataka, India
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 22 June 2026; accepted 28 July 2026; online 4 August 2026)

In the title compound, C30H29F5O5, the dihedral angle between the central carbonyl­phenyl and peripheral perfluoro­phen­oxy and benzoate rings are 76.57 (2) and 69.71 (3)°, respectively. The pendant C10 alkyl chain adopts an all-anti conformation. In the crystal, weak C—H⋯O hydrogen bonds connect the mol­ecules, generating [010] C(7) chains. The packing is consolidated by C—H⋯F and C—H⋯π inter­actions and weak aromatic ππ stacking. A Hirshfeld surface analysis revealed that the major contributions to the packing are from H⋯H (42.2%), H⋯F/F⋯H (19.0%), H⋯O/O⋯H (10.3%), C⋯H/H⋯C (8.7%) and F⋯C/C⋯F (8.0%) contacts.

1. Chemical context

The family of aromatic ester derivatives incorporating a para-dec­yloxy substituent attached to a benzoate core constitute an important class of organic compounds due to their wide-ranging applications in liquid-crystalline materials, supra­molecular assemblies, optoelectronic devices and functional organic systems. The incorporation of long flexible alk­oxy chains into rigid aromatic ester frameworks significantly influences mol­ecular anisotropy, inter­molecular inter­actions and mesophase organization, thereby promoting ordered mol­ecular packing and thermal stability (Muchenedi & Madhu Mohan, 2020View full citation). In particular, dec­yloxy-substituted benzoate derivatives have attracted considerable attention because the extended alkyl chain enhances van der Waals inter­actions and contributes to improved mol­ecular ordering, mesophase stability and thermo-responsive behaviour (Ashmawy et al., 2022View full citation). Phenyl 4-(dec­yloxy)benzoate belongs to the family of calamitic liquid-crystalline aromatic esters containing a rigid phenyl benzoate core connected to a flexible dec­yloxy substituent in the para position. Such mol­ecular architectures are well known for exhibiting structural anisotropy together with favourable inter­molecular ππ stacking inter­actions between aromatic rings and hydro­phobic inter­actions involving the long alkyl chain. These features strongly influence crystal packing arrangements, thermal transitions and mesomorphic properties (Das et al., 2012View full citation).

As part of our ongoing studies on these systems (Ahmed et al., 2026aView full citation,bView full citation), we present the synthesis and crystal structure of the title compound, C30H29F5O5 (I), herein.

[Scheme 1]

2. Structural commentary

The mol­ecular structure of (I) is shown in Fig. 1[link]. The dihedral angles between the central carbonyl­phenyl (C8–C13) ring and pendant perfluoro­phen­oxy (C1–C6) and (dec­yloxy)benzoate (C15–C20) rings are 76.57 (2) and 69.71 (2)°, respectively, thus the central ring is close to normal to both peripheral rings. The C7/O1/O2 carboxyl­ate group is twisted from its attached C8–C13 ring by 3.5 (5)° and the corresponding value for the C14/O3/O4 group and the C15–C20 ring is 4.5 (6)°. The pendant C10 alkyl chain adopts an all-anti conformation with the smallest and largest torsion angles being −107.17 (3)° and −178.34 (3)°, respectively, close to the ideal ±180°. Two short intra­molecular C—H⋯O contacts (Table 1[link]) are observed. Otherwise the bond lengths and angles in (I) may be regarded as normal.

Table 1
Hydrogen-bond geometry (Å, °)

Cg3 and Cg2 are the centroids of the C15–C20 and C8–C13 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C13—H13⋯O2 0.95 2.38 2.705 (6) 99
C16—H16⋯O3 0.95 2.42 2.737 (6) 99
C12—H12⋯F4i 0.95 2.48 3.427 (6) 174
C9—H9⋯O4ii 0.95 2.51 3.175 (7) 127
C3—F2⋯Cg3iii 1.340 (6) 3.242 (4) 3.630 (6) 95.8 (3)
C5—F4⋯Cg3iv 1.337 (6) 3.106 (4) 3.403 (6) 91.0 (3)
C6—F5⋯Cg2v 1.336 (6) 3.446 (4) 4.011 (6) 105.3 (3)
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation; (v) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of (I) showing 50% probability ellipsoids and short C—H⋯O intra­molecular contacts as green dotted lines.

3. Supra­molecular features

In the extended structure, the mol­ecules of (I) are connected by weak C9—H9⋯O4 hydrogen bonds to generate a C(7) chain propagating in zigzag fashion along [010] as shown in Fig. 2[link]. The chain is reinforced by C12—H12⋯F4 hydrogen bonds, which lead to a C(10) chain motif (Fig. 3[link]). The packing is consolidated by C—F⋯π inter­actions namely C3—F2⋯Cg3, C5—F4⋯Cg3 and C6—F5⋯Cg2, where Cg3 and Cg2 are the centroids of the C15–C20 and C8–C13 rings, respectively (Fig. 4[link]). A weak aromatic ππ stacking inter­action between pairs of Cg2 rings related by inversion symmetry (1 − x, 1 − y, −z) with a centroid–centroid distance of 3.918 (4) Å and a slippage of 1.830 Å is observed and is shown in Fig. 5[link].

[Figure 2]
Figure 2
Detail of the extended structure of (I) showing C—H⋯O hydrogen bonds (grey dotted lines) connecting the mol­ecules into C(7) chains.
[Figure 3]
Figure 3
Detail of the extended structure of (I) showing C—H⋯F hydrogen bonds (grey dotted lines) connecting the mol­ecules into C(10) chains.
[Figure 4]
Figure 4
Detail of the extended structure of (I) showing C—F⋯π inter­actions.
[Figure 5]
Figure 5
Detail of the extended structure of (I) showing ππ stacking inter­actions.

4. Hirshfeld surface analysis

A Hirshfeld surface (HS) analysis for (I) was performed using CrystalExplorer (Spackman et al., 2021View full citation) and the HS mapped over dnorm and shape-index are illustrated in Fig. 6[link]. The red triangular region viewed normal to the centre of carbophenyl ring indicates the existence of ππ stacking. The two-dimensional fingerprint plots shown in Fig. 7[link] indicate that the major contributions to the HS for (I) arise from H⋯H (42.2%), H⋯F/F⋯H (19.0%), H⋯O/O⋯H (10.3%), C⋯H/H⋯C (8.7%), F⋯C/C⋯F (8.0%) contacts, with C⋯C (3.8%) and F⋯F (2.0%) contacts playing a smaller role.

[Figure 6]
Figure 6
View of the three-dimensional Hirshfeld surface of (I) plotted over (a) dnorm. and (b) shape-index.
[Figure 7]
Figure 7
The two- dimensional fingerprint plots of (I) showing the contributions from the different contact types.

5. Database survey

A search of the Cambridge Structural Database (CSD version 6.01, March 2026; Groom et al., 2016View full citation) for structures containing the 4-(dec­yloxy)benzoate moiety yielded five related entries, namely CSD refcodes LASLIE (Kazem-Rostam et al., 2019View full citation), PUWQOP (Dutronc et al., 2016View full citation), ROJWOE and ROJWUK (Kuz'Mina et al., 2014View full citation) and TUVBUI (Cheng et al., 2010View full citation). The dihedral angles between the substituent planes and the 4-(dec­yloxy) benzoate moiety in these structures are 66.7, 58.0, 58.4, 64.6 and 48.5°, respectively, compared to a value of 69.71 (3) ° for (I).

6. Synthesis and crystallization

A mixture of 2,3,4,5,6-penta­fluoro­phenol (0.184 g, 1 eq.) and 4-((4- (dec­yloxy)benzo­yl)­oxy)benzoic acid (0.398 g, 1 eq.) in di­chloro­methane was stirred at room temperature overnight using di­cyclo­hexyl­carbodi­imide (1.2 eq) to promote the esterification reaction in the presence of N,N-di­methyl­amino­pyrimidine as a catalyst. The insoluble byproduct, di­cyclo­hexyl urea, was removed by filtration. The filtrate was washed with 5% acetic acid solution in water, and then with pure water. The filtrate was passed through silica gel, and then left for a week to grow crystals for X-ray studies. 1H NMR (500 MHz, CDCl 3) : δ 8.12–8.02 (m, 4H, Ar-H), 7.54 (m, 2H, Ar-H), 7.10 (d, J = 8.5 Hz, 2H, Ar-H), 4.01 (t, J = 6.5 Hz, 2H, –OCH2–), 1.74–1.25 (m, 16H, –CH2–alk­yl), 0.91 (t, J = 4.5Hz, 3H, –CH3) ppm. Elemental analysis calculated: C, 63.83; H, 5.18; F, 16.83%; found C, 63.90; H, 5.15; F, 16.79%.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. All H atoms were positioned with idealized geometry and refined using a riding model with C—H = 0.95–0.99 Å and Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).

Table 2
Experimental details

Crystal data
Chemical formula C30H29F5O5
Mr 564.53
Crystal system, space group Monoclinic, P21/c
Temperature (K) 143
a, b, c (Å) 23.579 (9), 8.255 (3), 13.959 (5)
β (°) 97.524 (10)
V3) 2693.9 (17)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.12
Crystal size (mm) 0.33 × 0.28 × 0.18
 
Data collection
Diffractometer Bruker SMART APEXII CCD
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.954, 0.970
No. of measured, independent and observed [I > 2σ(I)] reflections 12617, 4156, 2799
Rint 0.079
θmax (°) 24.0
(sin θ/λ)max−1) 0.572
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.091, 0.187, 1.09
No. of reflections 4156
No. of parameters 362
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.29, −0.27
Computer programs: APEX2 and SAINT (Bruker, 2017View full citation), SHELXT2019/2 (Sheldrick, 2015aView full citation), SHELXL2019/2 (Sheldrick, 2015bView full citation), Mercury (Macrae et al., 2020View full citation) and publCIF (Westrip, 2010View full citation).

Supporting information


Computing details top

4-[(2,3,4,5,6-Pentafluorophenoxy)carbonyl]phenyl 4-(decyloxy)benzoate top
Crystal data top
C30H29F5O5Prism
Mr = 564.53Dx = 1.392 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 23.579 (9) ÅCell parameters from 4231 reflections
b = 8.255 (3) Åθ = 2–26°
c = 13.959 (5) ŵ = 0.12 mm1
β = 97.524 (10)°T = 143 K
V = 2693.9 (17) Å3Prism, colourless
Z = 40.33 × 0.28 × 0.18 mm
F(000) = 1176
Data collection top
Bruker SMART APEXII CCD
diffractometer
4156 independent reflections
Radiation source: fine-focus sealed tube2799 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.079
Detector resolution: 1.09 pixels mm-1θmax = 24.0°, θmin = 2.9°
ω scansh = 2626
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
k = 98
Tmin = 0.954, Tmax = 0.970l = 1515
12617 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.091Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.187H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0315P)2 + 8.3116P]
where P = (Fo2 + 2Fc2)/3
4156 reflections(Δ/σ)max < 0.001
362 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = 0.27 e Å3
0 constraints
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
F10.31015 (14)0.5559 (4)1.0898 (2)0.0496 (9)
F20.22703 (13)0.5716 (4)1.2053 (2)0.0507 (9)
F30.24087 (13)0.7618 (4)1.3653 (2)0.0496 (9)
F40.33676 (13)0.9403 (4)1.4064 (2)0.0423 (8)
F50.41825 (12)0.9326 (4)1.2885 (2)0.0397 (8)
O10.36415 (14)0.8802 (4)1.0164 (2)0.0308 (9)
O20.41087 (14)0.7276 (5)1.1340 (2)0.0372 (10)
O30.60858 (13)0.7810 (4)0.8770 (2)0.0300 (9)
O40.57335 (14)0.6245 (5)0.7522 (2)0.0366 (10)
O50.81567 (13)0.8385 (5)0.6407 (2)0.0356 (9)
C10.3659 (2)0.7414 (7)1.1878 (4)0.0285 (12)
C20.3166 (2)0.6550 (7)1.1675 (4)0.0335 (13)
C30.2746 (2)0.6603 (7)1.2264 (4)0.0335 (13)
C40.2817 (2)0.7555 (7)1.3077 (4)0.0322 (13)
C50.3306 (2)0.8456 (6)1.3280 (4)0.0291 (12)
C60.3716 (2)0.8405 (6)1.2688 (4)0.0279 (12)
C70.4065 (2)0.8078 (6)1.0468 (3)0.0236 (11)
C80.45875 (19)0.7889 (6)1.0016 (3)0.0215 (11)
C90.46190 (19)0.8706 (6)0.9151 (3)0.0222 (11)
H90.4299830.9314970.8861950.027*
C100.51070 (19)0.8639 (6)0.8713 (3)0.0252 (12)
H100.5126930.9186720.8119680.030*
C110.55630 (19)0.7772 (6)0.9145 (3)0.0258 (12)
C120.5545 (2)0.6922 (6)0.9994 (3)0.0291 (12)
H120.5864700.6297451.0266580.035*
C130.5053 (2)0.6994 (6)1.0442 (3)0.0285 (12)
H130.5034810.6438261.1032680.034*
C140.6116 (2)0.7045 (6)0.7913 (4)0.0276 (12)
C150.66591 (19)0.7375 (6)0.7540 (3)0.0242 (11)
C160.70963 (19)0.8289 (6)0.8044 (3)0.0246 (12)
H160.7052860.8708600.8663870.029*
C170.7589 (2)0.8585 (7)0.7652 (4)0.0323 (13)
H170.7886310.9198490.8005800.039*
C180.76585 (19)0.7992 (6)0.6733 (4)0.0258 (12)
C190.7228 (2)0.7059 (7)0.6232 (4)0.0302 (13)
H190.7270380.6631520.5613380.036*
C200.6741 (2)0.6764 (6)0.6640 (4)0.0294 (12)
H200.6448510.6118090.6296310.035*
C210.8205 (2)0.8072 (7)0.5404 (4)0.0335 (13)
H21A0.7912610.8700420.4985260.040*
H21B0.8142030.6906760.5260390.040*
C220.8789 (2)0.8558 (7)0.5216 (4)0.0344 (13)
H22A0.9074790.7881480.5616370.041*
H22B0.8856670.9699540.5415010.041*
C230.8877 (2)0.8384 (8)0.4163 (4)0.0365 (14)
H23A0.8745050.7294950.3934640.044*
H23B0.8634600.9191940.3777340.044*
C240.9486 (2)0.8604 (7)0.3977 (4)0.0363 (14)
H24A0.9725650.7767850.4341920.044*
H24B0.9622740.9675300.4228960.044*
C250.9571 (2)0.8495 (7)0.2918 (4)0.0347 (13)
H25A0.9395780.7476820.2645920.042*
H25B0.9366300.9406870.2564620.042*
C261.0188 (2)0.8536 (8)0.2745 (4)0.0384 (14)
H26A1.0388100.7593790.3072090.046*
H26B1.0368020.9528240.3045760.046*
C271.0274 (2)0.8509 (8)0.1688 (4)0.0375 (14)
H27A1.0075720.7546970.1381240.045*
H27B1.0089320.9480670.1369910.045*
C281.0890 (2)0.8467 (8)0.1499 (4)0.0408 (15)
H28A1.1095130.9400610.1828050.049*
H28B1.1071670.7466250.1784860.049*
C291.0960 (2)0.8521 (8)0.0440 (4)0.0435 (15)
H29A1.0806600.9563720.0169030.052*
H29B1.0726760.7644000.0103340.052*
C301.1572 (2)0.8342 (9)0.0223 (4)0.0516 (17)
H30A1.1584670.8511920.0468470.077*
H30B1.1711920.7251310.0404130.077*
H30C1.1815380.9146520.0594590.077*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.073 (2)0.047 (2)0.0280 (18)0.0045 (18)0.0051 (16)0.0068 (16)
F20.0429 (19)0.057 (3)0.051 (2)0.0179 (17)0.0027 (15)0.0054 (17)
F30.0466 (19)0.062 (3)0.047 (2)0.0015 (17)0.0323 (16)0.0047 (17)
F40.064 (2)0.036 (2)0.0286 (17)0.0027 (16)0.0148 (15)0.0079 (15)
F50.0388 (17)0.042 (2)0.0380 (18)0.0093 (15)0.0056 (14)0.0129 (15)
O10.0321 (19)0.034 (2)0.028 (2)0.0032 (17)0.0069 (15)0.0063 (16)
O20.041 (2)0.045 (3)0.029 (2)0.0143 (18)0.0178 (17)0.0144 (18)
O30.0291 (18)0.039 (2)0.0236 (19)0.0033 (16)0.0087 (15)0.0106 (16)
O40.036 (2)0.045 (3)0.031 (2)0.0128 (19)0.0125 (16)0.0152 (18)
O50.0297 (19)0.050 (3)0.029 (2)0.0049 (17)0.0105 (15)0.0048 (18)
C10.032 (3)0.028 (3)0.027 (3)0.011 (2)0.011 (2)0.010 (2)
C20.046 (3)0.036 (4)0.019 (3)0.003 (3)0.010 (2)0.001 (2)
C30.030 (3)0.040 (4)0.030 (3)0.008 (3)0.004 (2)0.006 (3)
C40.034 (3)0.034 (4)0.033 (3)0.005 (3)0.022 (2)0.010 (3)
C50.039 (3)0.023 (3)0.026 (3)0.001 (2)0.008 (2)0.003 (2)
C60.028 (3)0.024 (3)0.032 (3)0.002 (2)0.004 (2)0.007 (2)
C70.035 (3)0.017 (3)0.020 (3)0.001 (2)0.009 (2)0.001 (2)
C80.027 (3)0.021 (3)0.018 (3)0.003 (2)0.006 (2)0.004 (2)
C90.028 (3)0.020 (3)0.018 (3)0.004 (2)0.002 (2)0.001 (2)
C100.035 (3)0.023 (3)0.019 (3)0.002 (2)0.009 (2)0.003 (2)
C110.030 (3)0.029 (3)0.020 (3)0.000 (2)0.010 (2)0.006 (2)
C120.031 (3)0.031 (4)0.026 (3)0.006 (2)0.005 (2)0.004 (2)
C130.037 (3)0.027 (3)0.022 (3)0.002 (2)0.006 (2)0.006 (2)
C140.033 (3)0.016 (3)0.035 (3)0.002 (2)0.009 (2)0.003 (2)
C150.028 (3)0.025 (3)0.020 (3)0.002 (2)0.007 (2)0.005 (2)
C160.033 (3)0.026 (3)0.016 (3)0.002 (2)0.005 (2)0.002 (2)
C170.029 (3)0.036 (4)0.031 (3)0.002 (2)0.002 (2)0.003 (2)
C180.026 (3)0.019 (3)0.033 (3)0.000 (2)0.006 (2)0.001 (2)
C190.031 (3)0.041 (4)0.020 (3)0.002 (2)0.011 (2)0.004 (2)
C200.035 (3)0.017 (3)0.037 (3)0.003 (2)0.009 (2)0.003 (2)
C210.035 (3)0.042 (4)0.026 (3)0.004 (3)0.011 (2)0.004 (2)
C220.031 (3)0.044 (4)0.029 (3)0.002 (3)0.006 (2)0.002 (3)
C230.037 (3)0.051 (4)0.022 (3)0.009 (3)0.008 (2)0.002 (3)
C240.033 (3)0.043 (4)0.033 (3)0.000 (3)0.006 (2)0.001 (3)
C250.033 (3)0.045 (4)0.027 (3)0.002 (3)0.010 (2)0.002 (3)
C260.039 (3)0.049 (4)0.029 (3)0.003 (3)0.010 (2)0.006 (3)
C270.037 (3)0.046 (4)0.031 (3)0.004 (3)0.008 (2)0.006 (3)
C280.037 (3)0.054 (4)0.032 (3)0.005 (3)0.006 (2)0.005 (3)
C290.049 (3)0.049 (4)0.034 (3)0.005 (3)0.014 (3)0.005 (3)
C300.053 (4)0.067 (5)0.040 (4)0.003 (3)0.022 (3)0.009 (3)
Geometric parameters (Å, º) top
F1—C21.351 (6)C17—C181.403 (7)
F2—C31.340 (6)C17—H170.9500
F3—C41.333 (5)C18—C191.388 (7)
F4—C51.337 (6)C19—C201.369 (7)
F5—C61.336 (6)C19—H190.9500
O1—C71.192 (5)C20—H200.9500
O2—O20.000 (11)C21—C221.491 (7)
O2—C71.378 (6)C21—H21A0.9900
O2—C11.382 (6)C21—H21B0.9900
O3—O30.000 (7)C22—C231.517 (7)
O3—C141.363 (6)C22—H22A0.9900
O3—C111.401 (5)C22—H22B0.9900
O4—C141.191 (6)C23—C241.504 (7)
O5—C181.354 (6)C23—H23A0.9900
O5—C211.442 (6)C23—H23B0.9900
C1—C21.360 (7)C24—C251.520 (7)
C1—C61.389 (7)C24—H24A0.9900
C2—C31.369 (7)C24—H24B0.9900
C3—C41.373 (7)C25—C261.506 (7)
C4—C51.369 (7)C25—H25A0.9900
C5—C61.352 (7)C25—H25B0.9900
C7—C81.465 (6)C26—C271.516 (7)
C8—C131.390 (7)C26—H26A0.9900
C8—C91.393 (6)C26—H26B0.9900
C9—C101.373 (6)C27—C281.511 (7)
C9—H90.9500C27—H27A0.9900
C10—C111.365 (7)C27—H27B0.9900
C10—H100.9500C28—C291.509 (7)
C11—C121.382 (7)C28—H28A0.9900
C12—C131.390 (7)C28—H28B0.9900
C12—H120.9500C29—C301.520 (7)
C13—H130.9500C29—H29A0.9900
C14—C151.470 (7)C29—H29B0.9900
C15—C201.390 (7)C30—H30A0.9800
C15—C161.392 (7)C30—H30B0.9800
C16—C171.369 (7)C30—H30C0.9800
C16—H160.9500
O2—O2—C70 (10)O5—C18—C19125.0 (4)
O2—O2—C10 (10)O5—C18—C17115.8 (4)
C7—O2—C1117.8 (4)C19—C18—C17119.2 (4)
O3—O3—C140 (10)C20—C19—C18119.2 (5)
O3—O3—C110 (10)C20—C19—H19120.4
C14—O3—C11117.9 (4)C18—C19—H19120.4
C18—O5—C21117.7 (4)C19—C20—C15122.3 (5)
C2—C1—O2122.6 (5)C19—C20—H20118.9
C2—C1—O2122.6 (5)C15—C20—H20118.9
O2—C1—O20.0 (4)O5—C21—C22108.4 (4)
C2—C1—C6117.9 (4)O5—C21—H21A110.0
O2—C1—C6119.4 (5)C22—C21—H21A110.0
O2—C1—C6119.4 (5)O5—C21—H21B110.0
F1—C2—C1119.3 (5)C22—C21—H21B110.0
F1—C2—C3119.1 (5)H21A—C21—H21B108.4
C1—C2—C3121.5 (5)C21—C22—C23113.1 (4)
F2—C3—C2120.1 (5)C21—C22—H22A109.0
F2—C3—C4120.1 (5)C23—C22—H22A109.0
C2—C3—C4119.7 (5)C21—C22—H22B109.0
F3—C4—C5120.6 (5)C23—C22—H22B109.0
F3—C4—C3120.1 (5)H22A—C22—H22B107.8
C5—C4—C3119.3 (4)C24—C23—C22114.2 (4)
F4—C5—C6120.5 (5)C24—C23—H23A108.7
F4—C5—C4119.0 (4)C22—C23—H23A108.7
C6—C5—C4120.4 (5)C24—C23—H23B108.7
F5—C6—C5119.5 (5)C22—C23—H23B108.7
F5—C6—C1119.5 (4)H23A—C23—H23B107.6
C5—C6—C1121.0 (5)C23—C24—C25114.3 (4)
O1—C7—O2121.2 (4)C23—C24—H24A108.7
O1—C7—O2121.2 (4)C25—C24—H24A108.7
O2—C7—O20.0 (4)C23—C24—H24B108.7
O1—C7—C8127.8 (4)C25—C24—H24B108.7
O2—C7—C8111.0 (4)H24A—C24—H24B107.6
O2—C7—C8111.0 (4)C26—C25—C24114.0 (4)
C13—C8—C9119.9 (4)C26—C25—H25A108.7
C13—C8—C7122.3 (4)C24—C25—H25A108.7
C9—C8—C7117.7 (4)C26—C25—H25B108.7
C10—C9—C8120.6 (4)C24—C25—H25B108.7
C10—C9—H9119.7H25A—C25—H25B107.6
C8—C9—H9119.7C25—C26—C27114.3 (4)
C11—C10—C9118.8 (4)C25—C26—H26A108.7
C11—C10—H10120.6C27—C26—H26A108.7
C9—C10—H10120.6C25—C26—H26B108.7
C10—C11—C12122.3 (4)C27—C26—H26B108.7
C10—C11—O3120.2 (4)H26A—C26—H26B107.6
C12—C11—O3117.3 (4)C28—C27—C26115.1 (4)
C10—C11—O3120.2 (4)C28—C27—H27A108.5
C12—C11—O3117.3 (4)C26—C27—H27A108.5
O3—C11—O30.0 (4)C28—C27—H27B108.5
C11—C12—C13119.0 (5)C26—C27—H27B108.5
C11—C12—H12120.5H27A—C27—H27B107.5
C13—C12—H12120.5C29—C28—C27113.7 (4)
C12—C13—C8119.3 (5)C29—C28—H28A108.8
C12—C13—H13120.3C27—C28—H28A108.8
C8—C13—H13120.3C29—C28—H28B108.8
O4—C14—O3122.4 (4)C27—C28—H28B108.8
O4—C14—O3122.4 (4)H28A—C28—H28B107.7
O3—C14—O30.0 (3)C28—C29—C30114.9 (5)
O4—C14—C15125.7 (5)C28—C29—H29A108.6
O3—C14—C15111.9 (4)C30—C29—H29A108.6
O3—C14—C15111.9 (4)C28—C29—H29B108.6
C20—C15—C16118.2 (4)C30—C29—H29B108.6
C20—C15—C14118.9 (4)H29A—C29—H29B107.5
C16—C15—C14122.9 (4)C29—C30—H30A109.5
C17—C16—C15120.3 (5)C29—C30—H30B109.5
C17—C16—H16119.8H30A—C30—H30B109.5
C15—C16—H16119.8C29—C30—H30C109.5
C16—C17—C18120.7 (5)H30A—C30—H30C109.5
C16—C17—H17119.6H30B—C30—H30C109.5
C18—C17—H17119.6
O2—O2—C1—C20.0 (7)C9—C10—C11—C121.8 (8)
C7—O2—C1—C278.7 (6)C9—C10—C11—O3173.6 (4)
C7—O2—C1—O20 (100)C9—C10—C11—O3173.6 (4)
O2—O2—C1—C60.0 (8)O3—O3—C11—C100.0 (5)
C7—O2—C1—C6104.7 (5)C14—O3—C11—C1070.8 (6)
O2—C1—C2—F12.5 (8)O3—O3—C11—C120.0 (6)
O2—C1—C2—F12.5 (8)C14—O3—C11—C12113.5 (5)
C6—C1—C2—F1179.1 (5)C14—O3—C11—O30 (100)
O2—C1—C2—C3174.4 (5)C10—C11—C12—C132.2 (8)
O2—C1—C2—C3174.4 (5)O3—C11—C12—C13173.4 (4)
C6—C1—C2—C32.3 (8)O3—C11—C12—C13173.4 (4)
F1—C2—C3—F22.0 (8)C11—C12—C13—C81.4 (8)
C1—C2—C3—F2178.8 (5)C9—C8—C13—C120.3 (7)
F1—C2—C3—C4177.4 (5)C7—C8—C13—C12177.3 (5)
C1—C2—C3—C40.5 (8)O3—O3—C14—O40.0 (11)
F2—C3—C4—F30.9 (8)C11—O3—C14—O46.3 (7)
C2—C3—C4—F3179.7 (5)C11—O3—C14—O30 (100)
F2—C3—C4—C5179.9 (5)O3—O3—C14—C150.0 (13)
C2—C3—C4—C50.8 (8)C11—O3—C14—C15171.9 (4)
F3—C4—C5—F40.1 (8)O4—C14—C15—C202.2 (8)
C3—C4—C5—F4178.9 (5)O3—C14—C15—C20176.0 (4)
F3—C4—C5—C6179.2 (5)O3—C14—C15—C20176.0 (4)
C3—C4—C5—C60.2 (8)O4—C14—C15—C16178.4 (5)
F4—C5—C6—F50.9 (8)O3—C14—C15—C163.5 (7)
C4—C5—C6—F5178.3 (5)O3—C14—C15—C163.5 (7)
F4—C5—C6—C1179.3 (5)C20—C15—C16—C170.8 (8)
C4—C5—C6—C11.6 (8)C14—C15—C16—C17178.7 (5)
C2—C1—C6—F5177.0 (5)C15—C16—C17—C180.8 (8)
O2—C1—C6—F56.2 (7)C21—O5—C18—C1911.8 (7)
O2—C1—C6—F56.2 (7)C21—O5—C18—C17168.6 (4)
C2—C1—C6—C52.8 (8)C16—C17—C18—O5178.7 (5)
O2—C1—C6—C5174.0 (5)C16—C17—C18—C191.7 (8)
O2—C1—C6—C5174.0 (5)O5—C18—C19—C20179.3 (5)
O2—O2—C7—O10.0 (14)C17—C18—C19—C201.1 (8)
C1—O2—C7—O13.6 (7)C18—C19—C20—C150.5 (8)
C1—O2—C7—O20 (100)C16—C15—C20—C191.4 (8)
O2—O2—C7—C80.0 (16)C14—C15—C20—C19178.1 (5)
C1—O2—C7—C8176.7 (4)C18—O5—C21—C22178.6 (4)
O1—C7—C8—C13179.3 (5)O5—C21—C22—C23176.3 (5)
O2—C7—C8—C130.4 (7)C21—C22—C23—C24170.6 (5)
O2—C7—C8—C130.4 (7)C22—C23—C24—C25177.8 (5)
O1—C7—C8—C93.6 (8)C23—C24—C25—C26173.8 (5)
O2—C7—C8—C9176.7 (4)C24—C25—C26—C27177.2 (5)
O2—C7—C8—C9176.7 (4)C25—C26—C27—C28177.2 (5)
C13—C8—C9—C100.1 (7)C26—C27—C28—C29177.3 (5)
C7—C8—C9—C10177.0 (4)C27—C28—C29—C30175.2 (5)
C8—C9—C10—C110.7 (7)
Hydrogen-bond geometry (Å, º) top
Cg3 and Cg2 are the centroids of the C15–C20 and C8–C13 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C13—H13···O20.952.382.705 (6)99
C16—H16···O30.952.422.737 (6)99
C12—H12···F4i0.952.483.427 (6)174
C9—H9···O4ii0.952.513.175 (7)127
C3—F2···Cg3iii1.34 (1)3.24 (1)3.630 (6)96 (1)
C5—F4···Cg3iv1.34 (1)3.11 (1)3.403 (6)91 (1)
C6—F5···Cg2v1.34 (1)3.45 (1)4.011 (6)105 (1)
Symmetry codes: (i) x+1, y1/2, z+5/2; (ii) x+1, y+1/2, z+3/2; (iii) x+1, y+1, z+2; (iv) x+1, y+2, z+2; (v) x, y+3/2, z+1/2.
 

Acknowledgements

The authors acknowledge the IISc-iSTEM facilities for their help in the collection of single-crystal XRD data, Raman Research Institute, Bangalore for the use of a laboratory to synthesis the sample and the Center of Innovative Science, Engineering and Education (CISEE), UCS, Tumkur University for constant support in extending the laboratory facilities. KA is thankful to BSPM's lab for use of their computing facilities at Department of PG Studies and Research in Physics, Albert Einstein Block, UCS, Tumkur University, Tumkur.

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