6 research outputs found
Tetrabenzo[8]circulene: Aromatic Saddles from Negatively Curved Graphene
An
aromatic saddle was designed from the hypothetical three-dimensional
graphene with the negative Gaussian curvature (Schwarzite P192). Two
aromatic saddles, tetrabenzo[8]circulene (<b>TB8C</b>) and its
octamethyl derivative <b>OM-TB8C</b>, were synthesized by the
Scholl reaction of cyclic octaphenylene precursors. The structure
of <b>TB8C</b> greatly deviates from planarity, and the deep
saddle shape was confirmed by single-crystal X-ray crystallography.
There are two conformers with the <i>S</i><sub>4</sub> symmetry,
which are twisted compared to the DFT structure (<i>D</i><sub>2<i>d</i></sub>). The theoretical studies propose
that the interconversion of <b>TB8C</b> via the planar transition
state (125 kcal mol<sup>–1</sup>) is not possible. However,
the pseudorotation leads to a low-energy tub-to-tub inversion via
the nonplanar transition state (7.3 kcal mol<sup>–1</sup>).
The ground-state structure of <b>TB8C</b> in solution is quite
different from the X-ray structure because of the crystal-packing
force and low-energy pseudorotation. <b>OM-TB8C</b> is a good
electron donor and works as the p-type semiconductor
Perfluorinated and Half-Fluorinated Rubrenes: Synthesis and Crystal Packing Arrangements
Perfluororubrene
(PF-RUB) has been synthesized by cycloaddition
of perfluorinated 1,3-diphenylisobenzofuran and 1,4-diphenyl-2,3-didehydronaphthalene
followed by reductive deoxygenation. This method was easily applied
for the synthesis of half-fluorinated rubrene (F<sub>14</sub>-RUB).
The electrochemical measurements and DFT calculations indicate that
perfluorination strongly lowers the HOMO and LUMO energies. Recrystallization
and sublimation of PF-RUB gave two different crystals with planar
and twisted conformations, respectively. In both cases, perfluorination
leads to the formation of short C–F and F–F contacts
and completely disrupts face-to-face π interactions. Single
crystals of F<sub>14</sub>-RUB were grown by sublimation, and twisted
molecules display the two-dimensional π-stacking with a face-to-face
distance of 3.54 Å
Tetrabenzo[8]circulene: Aromatic Saddles from Negatively Curved Graphene
An
aromatic saddle was designed from the hypothetical three-dimensional
graphene with the negative Gaussian curvature (Schwarzite P192). Two
aromatic saddles, tetrabenzo[8]circulene (<b>TB8C</b>) and its
octamethyl derivative <b>OM-TB8C</b>, were synthesized by the
Scholl reaction of cyclic octaphenylene precursors. The structure
of <b>TB8C</b> greatly deviates from planarity, and the deep
saddle shape was confirmed by single-crystal X-ray crystallography.
There are two conformers with the <i>S</i><sub>4</sub> symmetry,
which are twisted compared to the DFT structure (<i>D</i><sub>2<i>d</i></sub>). The theoretical studies propose
that the interconversion of <b>TB8C</b> via the planar transition
state (125 kcal mol<sup>–1</sup>) is not possible. However,
the pseudorotation leads to a low-energy tub-to-tub inversion via
the nonplanar transition state (7.3 kcal mol<sup>–1</sup>).
The ground-state structure of <b>TB8C</b> in solution is quite
different from the X-ray structure because of the crystal-packing
force and low-energy pseudorotation. <b>OM-TB8C</b> is a good
electron donor and works as the p-type semiconductor
Tetrabenzo[8]circulene: Aromatic Saddles from Negatively Curved Graphene
An
aromatic saddle was designed from the hypothetical three-dimensional
graphene with the negative Gaussian curvature (Schwarzite P192). Two
aromatic saddles, tetrabenzo[8]circulene (<b>TB8C</b>) and its
octamethyl derivative <b>OM-TB8C</b>, were synthesized by the
Scholl reaction of cyclic octaphenylene precursors. The structure
of <b>TB8C</b> greatly deviates from planarity, and the deep
saddle shape was confirmed by single-crystal X-ray crystallography.
There are two conformers with the <i>S</i><sub>4</sub> symmetry,
which are twisted compared to the DFT structure (<i>D</i><sub>2<i>d</i></sub>). The theoretical studies propose
that the interconversion of <b>TB8C</b> via the planar transition
state (125 kcal mol<sup>–1</sup>) is not possible. However,
the pseudorotation leads to a low-energy tub-to-tub inversion via
the nonplanar transition state (7.3 kcal mol<sup>–1</sup>).
The ground-state structure of <b>TB8C</b> in solution is quite
different from the X-ray structure because of the crystal-packing
force and low-energy pseudorotation. <b>OM-TB8C</b> is a good
electron donor and works as the p-type semiconductor
Tetracyclo(2,7-carbazole)s: Diatropicity and Paratropicity of Inner Regions of Nanohoops
Three
N-substituted tetracyclo(2,7-carbazole)s were synthesized to investigate
the inner regions of nanohoops. One compound has a 5,5-dimethylnonane
bridge between two neighboring <i>anti</i>-carbazoles, which
can be used as covalently bonded “methane probes”. These
probes near the ring center are strongly shielded by local ring currents
and exhibit a singlet at δ = −2.70 ppm in <sup>1</sup>H NMR. To visualize local and macrocyclic ring currents separately,
we drew nucleus-independent chemical shift contour maps of tetracyclo(9-methyl-2,7-carbazole)
and [<i>n</i>]cycloparaphenylenes (CPPs). Local ring currents
make the interior diatropic, and paratropic regions exist only outside
the ring. Macrocyclic ring currents in [5]CPP to [7]CPP generate deshielding
cones, which are typical of antiaromatic [4<i>n</i>]annulenes
Tetracyclo(2,7-carbazole)s: Diatropicity and Paratropicity of Inner Regions of Nanohoops
Three
N-substituted tetracyclo(2,7-carbazole)s were synthesized to investigate
the inner regions of nanohoops. One compound has a 5,5-dimethylnonane
bridge between two neighboring <i>anti</i>-carbazoles, which
can be used as covalently bonded “methane probes”. These
probes near the ring center are strongly shielded by local ring currents
and exhibit a singlet at δ = −2.70 ppm in <sup>1</sup>H NMR. To visualize local and macrocyclic ring currents separately,
we drew nucleus-independent chemical shift contour maps of tetracyclo(9-methyl-2,7-carbazole)
and [<i>n</i>]cycloparaphenylenes (CPPs). Local ring currents
make the interior diatropic, and paratropic regions exist only outside
the ring. Macrocyclic ring currents in [5]CPP to [7]CPP generate deshielding
cones, which are typical of antiaromatic [4<i>n</i>]annulenes