Substance containing two π-congested aromatic systems are attractive targets in synthetic studies as well as efforts designed to explore the unique properties that originate from π-congestion. Since the time of the computational studies by Schleyer and Warner, the concept of stacked aromaticity created by the encounter of two antiaromatic rings has received much attention. In contrast, questions about what happens when two aromatic rings are closely stacked have remained unanswered. To the best of our knowledge, only one computational study has been performed by Herges, the results of which suggest that [2.2]paracyclophane, possessing short distance (<3.00 Å) between two aromatic ring planes, has a paratropic ring current between two the benzene rings. This observation is consistent with the conclusion that stacked antiaromaticity exists within the π-congested space between aromatic rings. Herein, we investigated the antiaromaticity of highly π-congested anthracene dimers using anthracenophane, which possesses a short inter-plane carbon-carbon distance of ca. 2.80 Å. The absorption spectrum of this substance contains a weak broad band from 450 to 550 nm that is attributed from HOMO-LUMO transition. These properties exist in planar cyclooctatetraene derivatives that having 8π-electron antiaromaticity. The results of nucleus-independent chemical shift and anisotropy of the induced current density calculations indicate that relatively weak antiaromatic character exists between the central six-membered rings of the two anthracene moieties in anthracenophane. In addition, an attempt to enhance the stacked antiaromaticity of anthracenophane using pressure to enhance π-congestion using was unsuccessful.
Substance containing two π-congested aromatic systems are attractive targets in synthetic studies as well as efforts designed to explore the unique properties that originate from π-congestion. Since the time of the computational studies by Schleyer and Warner, the concept of stacked aromaticity created by the encounter of two antiaromatic rings has received much attention. In contrast, questions about what happens when two aromatic rings are closely stacked have remained unanswered. To the best of our knowledge, only one computational study has been performed by Herges, the results of which suggest that [2.2]paracyclophane, possessing short distance (<3.00 Å) between two aromatic ring planes, has a paratropic ring current between two the benzene rings. This observation is consistent with the conclusion that stacked antiaromaticity exists within the π-congested space between aromatic rings. Herein, we investigated the antiaromaticity of highly π-congested anthracene dimers using anthracenophane, which possesses a short inter-plane carbon-carbon distance of ca. 2.80 Å. The absorption spectrum of this substance contains a weak broad band from 450 to 550 nm that is attributed from HOMO-LUMO transition. These properties exist in planar cyclooctatetraene derivatives that having 8π-electron antiaromaticity. The results of nucleus-independent chemical shift and anisotropy of the induced current density calculations indicate that relatively weak antiaromatic character exists between the central six-membered rings of the two anthracene moieties in anthracenophane. In addition, an attempt to enhance the stacked 3D antiaromaticity of anthracenophane using pressure to enhance π-congestion using was unsuccessful.
Substance containing two π-congested aromatic systems are attractive targets in synthetic studies as well as efforts designed to explore the unique properties that originate from π-congestion. Since the time of the computational studies by Schleyer and Warner, the concept of stacked 3D aromaticity created by the encounter of two antiaromatic rings has received much attention. In contrast, questions about what happens when two aromatic rings are closely stacked have remained unanswered. To the best of our knowledge, only one computational study has been performed by Herges, the results of which suggest that [2.2]paracyclophane, possessing short distance (<3.00 Å) between two aromatic ring planes, has a paratropic ring current between two the benzene rings. This observation is consistent with the conclusion that stacked 3D antiaromaticity exists within the π-congested space between aromatic rings. Herein, we investigated the 3D antiaromaticity of highly -congested anthracene dimers using anthracenophane, which possesses a short inter-plane carbon-carbon distance of ca. 2.80 Å. The absorption spectrum of this substance contains a weak broad band from 450 to 550 nm that is attributed from HOMO-LUMO transition. These properties exist in planar cyclooctatetraene derivatives that having 8π-electron antiaromaticity. The results of nucleus-independent chemical shift and anisotropy of the induced current density calculations indicate that relatively weak antiaromatic character exists between the central six-membered rings of the two anthracene moieties in anthracenophane. In addition, an attempt to enhance the stacked 3D antiaromaticity of anthracenophane using pressure to enhance π-congestion using was unsuccessful.
We demonstrated the computational study of the π-congestion effects in benzene, naphthalane, anthracene, teteracene, and pentacene dimers close with two positions at Ca···Ca’ and Cb···Cb’ to elucidate the singlet biradical characters as well as the stacked antiaromaticity. By extending the π-system from benzene to pentacene, the singlet biradical character increase whereas the stacked antiaromaticity decrease at near the transition state of [4+4]pericyclic reaction in ground state. Especially, the pentacene dimer exhibits large biradical character y0 = 61% with a weak antiaromaticity of NICSxx = +11 ppm at the distance of 2.80 Å between π-planes. These calculated results provided a unique idea to extract the similar electronic and magnetic natures as seen in transition state where the bond-order of the sp2 and sp3 carbon changes, like the graphite-to-diamond transformation.
Substance containing two π-congested aromatic systems are attractive targets in synthetic studies as well as efforts designed to explore the unique properties that originate from π-congestion. Since the time of the computational studies by Schleyer and Warner, the concept of stacked 3D aromaticity created by the encounter of two antiaromatic rings has received much attention. In contrast, questions about what happens when two aromatic rings are closely stacked have remained unanswered. To the best of our knowledge, only one computational study has been performed by Herges, the results of which suggest that [2.2]paracyclophane, possessing short distance (<3.00 Å) between two aromatic ring planes, has a paratropic ring current between two the benzene rings. This observation is consistent with the conclusion that stacked 3D antiaromaticity exists within the π-congested space between aromatic rings. Herein, we investigated the 3D antiaromaticity of highly π-congested anthracene dimers using anthracenophane, which possesses a short inter-plane carbon-carbon distance of ca. 2.80 Å. The absorption spectrum of this substance contains a weak broad band from 450 to 550 nm that is attributed from HOMO-LUMO transition. These properties exist in planar cyclooctatetraene derivatives that having 8π-electron antiaromaticity. The results of nucleus-independent chemical shift and anisotropy of the induced current density calculations indicate that relatively weak antiaromatic character exists between the central six-membered rings of the two anthracene moieties in anthracenophane. In addition, an attempt to enhance the stacked 3D antiaromaticity of anthracenophane using pressure to enhance π-congestion using was unsuccessful.
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