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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Jun 27;68(Pt 7):o2237. doi: 10.1107/S1600536812028097

1-{4-[Bis(4-fluoro­phen­yl)meth­yl]piperazin-1-yl}ethanone

A S Dayananda a, H S Yathirajan a, Amanda C Keeley b, Jerry P Jasinski b,*
PMCID: PMC3394028  PMID: 22798893

Abstract

In the title compound, C19H20F2N2O, the six-membered piperazine group adopts a slightly distorted chair conformation. The dihedral angle between the mean planes of the two benzene rings is 73.4 (6)°. The mean plane of the ethanone group is twisted from the mean planes of the two benzene rings by 66.7 (8) and 86.2 (6)°. In the crystal, C—H⋯O and C—H⋯F inter­actions link the molecules, forming a three-dimensional structure.

Related literature  

For the biological activity of piperazines, see: Bogatcheva et al. (2006); Brockunier et al. (2004). For a review of pharmacological and toxicological information for piperazine derivatives, see: Elliott (2011). For related structures, see: Betz et al. (2011a ,b ); Dai et al. (2012); Dayananda et al. (2012a ,b ); Zhong et al. (2011). For puckering parameters, see: Cremer & Pople (1975). For reference bond-length data, see Allen et al. (1987).graphic file with name e-68-o2237-scheme1.jpg

Experimental  

Crystal data  

  • C19H20F2N2O

  • M r = 330.37

  • Monoclinic, Inline graphic

  • a = 10.1701 (5) Å

  • b = 16.5521 (5) Å

  • c = 11.1690 (5) Å

  • β = 114.690 (5)°

  • V = 1708.27 (14) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 0.79 mm−1

  • T = 173 K

  • 0.48 × 0.32 × 0.22 mm

Data collection  

  • Oxford Xcalibur Eos Gemini diffractometer

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2010) T min = 0.802, T max = 1.000

  • 10536 measured reflections

  • 3297 independent reflections

  • 2809 reflections with I > 2σ(I)

  • R int = 0.026

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.054

  • wR(F 2) = 0.155

  • S = 1.04

  • 3297 reflections

  • 218 parameters

  • H-atom parameters constrained

  • Δρmax = 0.41 e Å−3

  • Δρmin = −0.34 e Å−3

Data collection: CrysAlis PRO (Oxford Diffraction, 2010); cell refinement: CrysAlis PRO; data reduction: CrysAlis RED (Oxford Diffraction, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812028097/zj2086sup1.cif

e-68-o2237-sup1.cif (19.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812028097/zj2086Isup2.hkl

e-68-o2237-Isup2.hkl (161.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812028097/zj2086Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C13—H13⋯O1i 0.93 2.46 3.371 (2) 167
C15—H15⋯O1i 0.93 2.55 3.351 (3) 145
C18—H18⋯F2ii 0.93 2.54 3.319 (3) 142

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

ASD thanks the University of Mysore for research facilities. JPJ acknowledges the NSF–MRI program (grant No. CHE1039027) for funds to purchase the X-ray diffractometer.

supplementary crystallographic information

Comment

4,4'-Difluorobenzhydryl piperazine is an intermediate for the preparation of flunarizine which is a calcium channel blocker. Piperazines are among the most important building blocks in today's drug discovery and are found in biologically active compounds across a number of different therapeutic areas (Brockunier et al., 2004; Bogatcheva et al., 2006). A review on the current pharmacological and toxicological information for piperazine derivatives is described (Elliott, 2011).

The crystal structures of 4-[bis(4-fluorophenyl)methyl]piperazin-1-ium 2-(2-phenylethyl) benzoate (Betz et al., 2011a), 4-[bis(4-fluorophenyl)methyl]piperazin-1-ium picrate (Betz et al., 2011b), (E)-1-{4-[bis(4-fluorophenyl)methyl]piperazin-1-yl}-3-(4-ethoxyphenyl) prop-2-en-1-one (Zhong et al., 2011), 4-[bis(4-fluorophenyl) methyl]piperazin-1-ium bis(trichloroacetate) 0.4-hydrate (Dayananda et al., 2012a), 4-[bis(4-fluorophenyl)methyl] piperazin-1-ium 2-hydroxybenzoate 2-hydroxybenzoic acid monosolvate (Dayananda et al., 2012b) and 1-[bis(4-fluorophenyl) methyl]-4-[2-(2-methylphenoxy)ethyl]piperazine (Dai et al., 2012) have been reported. In the course of our studies on the salts of piperazines and in view of the importance of piperazines, this paper reports the crystal and molecular structure of the title compound, C19H20F2N2O, (I), which was accidentally obtained by the reaction of 4,4'-difluorobenzhydryl piperazine and acetyl salicylic acid.

In the asymmetric unit of the title compound, (I), the 6-membered piperazine group (N1/C3/C4/N2/C5/C6) adopts a slightly distorted chair conformation with puckering parameters Q, θ and φ of 0.568 (9) Å, 172.2 (7)°, and 350.979 (8)° (Cremer & Pople, 1975), respectively (Fig. 1). For an ideal chair θ has a value of 0 or 180°. Bond lengths are in normal ranges (Allen et al., 1987). The dihedral angle between the mean planes of the two benzene rings is 73.4 (6)°. The mean plane of the ethanone group (C1/C2/O1/N1) is twisted from the mean planes of the two benzene rings by 66.7 (8)° and 86.2 (6)°. Weak C—H···O and C—H···F intermolecular interactions (Table 1) are observed providing increased stability with crystal packing (Fig. 2).

Experimental

4,4'-Difluorobenzhydryl piperazine was obtained from R. L. Fine Chem., Bengaluru, India. 4,4'-Difluorobenzhydryl piperazine (2.88 g, 0.01 mol) was dissolved in 10 ml of absolute ethanol and acetylsalicylic acid (1.81 g, 0.01 mol) was also dissolved in 10 ml of absolute ethanol. Both the solutions were mixed and stirred in a beaker at 333 K for 30 min. The mixture was kept aside for a day at room temperature. The compound formed was filtered and dried in a vacuum desiccator over phosphorous pentoxide. The compound was recrystallized from a mixture of toluene and dimethyl formamide by slow evaporation (m.p. 418–423 K).

Refinement

All of the H atoms were placed in their calculated positions and then refined using the riding model with C—H lengths of 0.93, 0.98 (CH) or 0.96 Å (CH3). The isotropic displacement parameters for these atoms were set to 1.19 to 1.20 (CH), 1.19 to 1.20 (CH2) or 1.50 (CH3) times Ueq of the parent atom.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound showing the atom labeling scheme and 50% probability displacement ellipsoids.

Fig. 2.

Fig. 2.

Packing diagram of the title compound viewed along the c axis. Dashed lines indicate weak C—H···O and C—H···F intermolecular interactions. The remaining H atoms have been removed for clarity.

Crystal data

C19H20F2N2O F(000) = 696
Mr = 330.37 Dx = 1.285 Mg m3
Monoclinic, P21/n Cu Kα radiation, λ = 1.54178 Å
Hall symbol: -P 2yn Cell parameters from 4103 reflections
a = 10.1701 (5) Å θ = 4.4–71.2°
b = 16.5521 (5) Å µ = 0.79 mm1
c = 11.1690 (5) Å T = 173 K
β = 114.690 (5)° Chunk, colourless
V = 1708.27 (14) Å3 0.48 × 0.32 × 0.22 mm
Z = 4

Data collection

Oxford Xcalibur Eos Gemini diffractometer 3297 independent reflections
Radiation source: Enhance (Cu) X-ray Source 2809 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.026
Detector resolution: 16.1500 pixels mm-1 θmax = 71.4°, θmin = 5.0°
ω scans h = −12→12
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2010) k = −12→20
Tmin = 0.802, Tmax = 1.000 l = −13→13
10536 measured reflections

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.155 H-atom parameters constrained
S = 1.04 w = 1/[σ2(Fo2) + (0.0781P)2 + 0.7598P] where P = (Fo2 + 2Fc2)/3
3297 reflections (Δ/σ)max < 0.001
218 parameters Δρmax = 0.41 e Å3
0 restraints Δρmin = −0.34 e Å3

Special details

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)

x y z Uiso*/Ueq
F1 0.5160 (2) 0.80482 (10) −0.24955 (14) 0.0811 (5)
F2 0.86017 (18) 1.06144 (9) 0.55722 (15) 0.0788 (5)
O1 0.29530 (17) 0.50309 (9) 0.41107 (15) 0.0534 (4)
N1 0.40533 (18) 0.62266 (10) 0.42534 (15) 0.0410 (4)
N2 0.48228 (15) 0.75448 (8) 0.30161 (13) 0.0304 (3)
C1 0.3741 (3) 0.57161 (13) 0.6169 (2) 0.0520 (5)
H1A 0.3212 0.5298 0.6371 0.078*
H1B 0.3382 0.6234 0.6280 0.078*
H1C 0.4749 0.5674 0.6752 0.078*
C2 0.3555 (2) 0.56254 (11) 0.47665 (19) 0.0395 (4)
C3 0.3933 (2) 0.61611 (12) 0.29096 (19) 0.0465 (5)
H3A 0.3142 0.5801 0.2406 0.056*
H3B 0.4819 0.5935 0.2922 0.056*
C4 0.3666 (2) 0.69801 (12) 0.22666 (17) 0.0406 (4)
H4A 0.3605 0.6930 0.1380 0.049*
H4B 0.2749 0.7189 0.2206 0.049*
C5 0.4817 (2) 0.76336 (11) 0.43201 (17) 0.0363 (4)
H5A 0.3886 0.7842 0.4222 0.044*
H5B 0.5555 0.8019 0.4835 0.044*
C6 0.5101 (2) 0.68390 (12) 0.50348 (18) 0.0426 (5)
H6A 0.6072 0.6658 0.5213 0.051*
H6B 0.5038 0.6909 0.5872 0.051*
C7 0.46380 (18) 0.83174 (11) 0.23205 (16) 0.0333 (4)
H7 0.3663 0.8519 0.2120 0.040*
C8 0.47860 (19) 0.82157 (11) 0.10209 (17) 0.0356 (4)
C9 0.5661 (2) 0.76331 (12) 0.0844 (2) 0.0430 (4)
H9 0.6165 0.7276 0.1526 0.052*
C10 0.5799 (2) 0.75726 (12) −0.0344 (2) 0.0508 (5)
H10 0.6388 0.7181 −0.0465 0.061*
C11 0.5044 (3) 0.81058 (13) −0.1324 (2) 0.0522 (5)
C12 0.4182 (3) 0.86953 (15) −0.1176 (2) 0.0576 (6)
H12 0.3689 0.9055 −0.1856 0.069*
C13 0.4060 (2) 0.87437 (13) 0.00127 (19) 0.0472 (5)
H13 0.3477 0.9141 0.0129 0.057*
C14 0.5726 (2) 0.89431 (11) 0.31739 (16) 0.0349 (4)
C15 0.5244 (2) 0.96762 (12) 0.34201 (19) 0.0426 (4)
H15 0.4259 0.9791 0.3044 0.051*
C16 0.6209 (3) 1.02416 (12) 0.4218 (2) 0.0522 (5)
H16 0.5883 1.0736 0.4384 0.063*
C17 0.7645 (3) 1.00628 (13) 0.4757 (2) 0.0507 (5)
C18 0.8181 (2) 0.93527 (13) 0.4525 (2) 0.0496 (5)
H18 0.9171 0.9251 0.4897 0.060*
C19 0.7207 (2) 0.87896 (12) 0.37212 (19) 0.0419 (4)
H19 0.7546 0.8303 0.3544 0.050*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
F1 0.1304 (14) 0.0839 (11) 0.0563 (9) 0.0159 (10) 0.0658 (9) 0.0004 (7)
F2 0.0951 (11) 0.0602 (9) 0.0724 (10) −0.0414 (8) 0.0264 (8) −0.0204 (7)
O1 0.0659 (9) 0.0428 (8) 0.0519 (8) −0.0214 (7) 0.0250 (7) −0.0029 (6)
N1 0.0530 (9) 0.0380 (8) 0.0314 (8) −0.0133 (7) 0.0170 (7) −0.0030 (6)
N2 0.0345 (7) 0.0299 (7) 0.0268 (7) −0.0034 (6) 0.0128 (6) −0.0012 (5)
C1 0.0722 (14) 0.0438 (11) 0.0454 (11) −0.0056 (10) 0.0300 (10) 0.0073 (9)
C2 0.0417 (9) 0.0368 (10) 0.0405 (10) −0.0024 (8) 0.0177 (8) 0.0035 (8)
C3 0.0651 (12) 0.0400 (10) 0.0374 (10) −0.0168 (9) 0.0245 (9) −0.0084 (8)
C4 0.0477 (10) 0.0448 (10) 0.0278 (8) −0.0129 (8) 0.0143 (8) −0.0043 (7)
C5 0.0448 (10) 0.0348 (9) 0.0278 (9) −0.0085 (7) 0.0137 (7) −0.0037 (7)
C6 0.0516 (11) 0.0410 (10) 0.0305 (9) −0.0107 (8) 0.0126 (8) −0.0011 (7)
C7 0.0355 (8) 0.0342 (9) 0.0315 (9) 0.0023 (7) 0.0152 (7) 0.0004 (7)
C8 0.0410 (9) 0.0347 (9) 0.0334 (9) −0.0048 (7) 0.0181 (7) −0.0038 (7)
C9 0.0492 (11) 0.0379 (10) 0.0447 (11) 0.0022 (8) 0.0224 (9) 0.0050 (8)
C10 0.0624 (13) 0.0402 (11) 0.0652 (14) 0.0035 (9) 0.0420 (11) −0.0045 (9)
C11 0.0776 (14) 0.0523 (12) 0.0429 (11) 0.0011 (11) 0.0411 (11) −0.0009 (9)
C12 0.0765 (15) 0.0617 (14) 0.0387 (11) 0.0184 (12) 0.0281 (11) 0.0106 (10)
C13 0.0594 (12) 0.0488 (11) 0.0398 (10) 0.0111 (9) 0.0271 (9) 0.0023 (8)
C14 0.0449 (9) 0.0345 (9) 0.0265 (8) −0.0055 (7) 0.0161 (7) 0.0033 (7)
C15 0.0501 (11) 0.0404 (10) 0.0392 (10) 0.0029 (8) 0.0206 (8) 0.0048 (8)
C16 0.0821 (16) 0.0304 (10) 0.0503 (12) −0.0004 (10) 0.0338 (11) −0.0008 (8)
C17 0.0689 (14) 0.0413 (11) 0.0399 (10) −0.0249 (10) 0.0207 (10) −0.0024 (8)
C18 0.0448 (10) 0.0541 (12) 0.0472 (11) −0.0080 (9) 0.0165 (9) 0.0082 (9)
C19 0.0500 (11) 0.0349 (10) 0.0442 (10) 0.0001 (8) 0.0232 (9) 0.0015 (8)

Geometric parameters (Å, º)

F1—C11 1.364 (2) C7—C14 1.524 (2)
F2—C17 1.367 (2) C7—C8 1.530 (2)
O1—C2 1.227 (2) C7—H7 0.9800
N1—C2 1.349 (2) C8—C13 1.372 (3)
N1—C3 1.458 (2) C8—C9 1.381 (3)
N1—C6 1.465 (2) C9—C10 1.396 (3)
N2—C4 1.462 (2) C9—H9 0.9300
N2—C5 1.466 (2) C10—C11 1.365 (3)
N2—C7 1.467 (2) C10—H10 0.9300
C1—C2 1.505 (3) C11—C12 1.368 (3)
C1—H1A 0.9600 C12—C13 1.386 (3)
C1—H1B 0.9600 C12—H12 0.9300
C1—H1C 0.9600 C13—H13 0.9300
C3—C4 1.505 (3) C14—C15 1.378 (3)
C3—H3A 0.9700 C14—C19 1.393 (3)
C3—H3B 0.9700 C15—C16 1.379 (3)
C4—H4A 0.9700 C15—H15 0.9300
C4—H4B 0.9700 C16—C17 1.359 (3)
C5—C6 1.503 (3) C16—H16 0.9300
C5—H5A 0.9700 C17—C18 1.365 (3)
C5—H5B 0.9700 C18—C19 1.383 (3)
C6—H6A 0.9700 C18—H18 0.9300
C6—H6B 0.9700 C19—H19 0.9300
C2—N1—C3 119.85 (15) C14—C7—C8 109.55 (14)
C2—N1—C6 124.48 (15) N2—C7—H7 108.2
C3—N1—C6 113.10 (15) C14—C7—H7 108.2
C4—N2—C5 107.26 (13) C8—C7—H7 108.2
C4—N2—C7 111.08 (13) C13—C8—C9 119.04 (17)
C5—N2—C7 112.70 (13) C13—C8—C7 118.44 (16)
C2—C1—H1A 109.5 C9—C8—C7 122.48 (16)
C2—C1—H1B 109.5 C8—C9—C10 120.84 (18)
H1A—C1—H1B 109.5 C8—C9—H9 119.6
C2—C1—H1C 109.5 C10—C9—H9 119.6
H1A—C1—H1C 109.5 C11—C10—C9 118.04 (18)
H1B—C1—H1C 109.5 C11—C10—H10 121.0
O1—C2—N1 121.36 (17) C9—C10—H10 121.0
O1—C2—C1 121.08 (17) F1—C11—C10 118.60 (19)
N1—C2—C1 117.55 (16) F1—C11—C12 118.8 (2)
N1—C3—C4 110.18 (16) C10—C11—C12 122.56 (19)
N1—C3—H3A 109.6 C11—C12—C13 118.4 (2)
C4—C3—H3A 109.6 C11—C12—H12 120.8
N1—C3—H3B 109.6 C13—C12—H12 120.8
C4—C3—H3B 109.6 C8—C13—C12 121.12 (19)
H3A—C3—H3B 108.1 C8—C13—H13 119.4
N2—C4—C3 111.16 (15) C12—C13—H13 119.4
N2—C4—H4A 109.4 C15—C14—C19 118.84 (17)
C3—C4—H4A 109.4 C15—C14—C7 119.82 (17)
N2—C4—H4B 109.4 C19—C14—C7 121.33 (16)
C3—C4—H4B 109.4 C14—C15—C16 120.7 (2)
H4A—C4—H4B 108.0 C14—C15—H15 119.7
N2—C5—C6 111.14 (15) C16—C15—H15 119.7
N2—C5—H5A 109.4 C17—C16—C15 118.8 (2)
C6—C5—H5A 109.4 C17—C16—H16 120.6
N2—C5—H5B 109.4 C15—C16—H16 120.6
C6—C5—H5B 109.4 C16—C17—C18 122.94 (19)
H5A—C5—H5B 108.0 C16—C17—F2 118.9 (2)
N1—C6—C5 111.02 (15) C18—C17—F2 118.1 (2)
N1—C6—H6A 109.4 C17—C18—C19 118.0 (2)
C5—C6—H6A 109.4 C17—C18—H18 121.0
N1—C6—H6B 109.4 C19—C18—H18 121.0
C5—C6—H6B 109.4 C18—C19—C14 120.79 (19)
H6A—C6—H6B 108.0 C18—C19—H19 119.6
N2—C7—C14 111.23 (13) C14—C19—H19 119.6
N2—C7—C8 111.40 (14)
C3—N1—C2—O1 −2.5 (3) C7—C8—C9—C10 −178.25 (18)
C6—N1—C2—O1 −163.00 (19) C8—C9—C10—C11 0.0 (3)
C3—N1—C2—C1 178.49 (18) C9—C10—C11—F1 −179.4 (2)
C6—N1—C2—C1 17.9 (3) C9—C10—C11—C12 0.8 (4)
C2—N1—C3—C4 145.48 (18) F1—C11—C12—C13 179.4 (2)
C6—N1—C3—C4 −51.9 (2) C10—C11—C12—C13 −0.8 (4)
C5—N2—C4—C3 −62.16 (19) C9—C8—C13—C12 0.6 (3)
C7—N2—C4—C3 174.28 (15) C7—C8—C13—C12 178.3 (2)
N1—C3—C4—N2 58.1 (2) C11—C12—C13—C8 0.1 (4)
C4—N2—C5—C6 60.94 (19) N2—C7—C14—C15 −124.60 (17)
C7—N2—C5—C6 −176.50 (14) C8—C7—C14—C15 111.80 (18)
C2—N1—C6—C5 −147.07 (18) N2—C7—C14—C19 55.1 (2)
C3—N1—C6—C5 51.2 (2) C8—C7—C14—C19 −68.5 (2)
N2—C5—C6—N1 −56.0 (2) C19—C14—C15—C16 −1.4 (3)
C4—N2—C7—C14 172.68 (14) C7—C14—C15—C16 178.28 (17)
C5—N2—C7—C14 52.28 (18) C14—C15—C16—C17 0.0 (3)
C4—N2—C7—C8 −64.78 (18) C15—C16—C17—C18 1.3 (3)
C5—N2—C7—C8 174.82 (14) C15—C16—C17—F2 −178.55 (18)
N2—C7—C8—C13 151.90 (17) C16—C17—C18—C19 −1.1 (3)
C14—C7—C8—C13 −84.6 (2) F2—C17—C18—C19 178.75 (18)
N2—C7—C8—C9 −30.5 (2) C17—C18—C19—C14 −0.4 (3)
C14—C7—C8—C9 93.0 (2) C15—C14—C19—C18 1.6 (3)
C13—C8—C9—C10 −0.7 (3) C7—C14—C19—C18 −178.09 (16)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C13—H13···O1i 0.93 2.46 3.371 (2) 167
C15—H15···O1i 0.93 2.55 3.351 (3) 145
C18—H18···F2ii 0.93 2.54 3.319 (3) 142

Symmetry codes: (i) −x+1/2, y+1/2, −z+1/2; (ii) −x+2, −y+2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZJ2086).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812028097/zj2086sup1.cif

e-68-o2237-sup1.cif (19.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812028097/zj2086Isup2.hkl

e-68-o2237-Isup2.hkl (161.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812028097/zj2086Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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