2006
DOI: 10.1103/physrevb.74.045426
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Electronic properties of acenes: Oligomer to polymer structure

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Cited by 76 publications
(59 citation statements)
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“…8,9 Naphthacene ͑also referred to as tetracene͒, pentacene, and derivative compounds have been used recently to prepare highly ordered conducting organic materials or thin films with particularly large charge carrier mobilities. 10 In contrast with the prevailing view 11 that large acenes have a closed-shell singlet or open-shell triplet electronic ground states, a few groups [12][13][14][15][16] recently conjectured that large acenes such as hexacene, heptacene, or octacene should rather be regarded as open-shell singlet biradical systems, as a result of the instability of unrestricted ͑UBLYP, UB3LYP, UPW91, UBPW91, etc.͒ wave functions, in conjunction with rather modest basis sets ͑STO-3G, 6-31G ‫ء‬ , or cc-pVDZ͒. This in-stability was diagnosed 12 from the fact that in these unrestricted calculations the two outermost singly occupied ␣ and ␤ spin orbitals do not smoothly follow the D 2h symmetry point group imposed by the nuclear frame, but rather reflect an overwhelmingly strong symmetry breaking of the electronic wave function, 12 in the form of a localization of the two frontier electrons on opposite polyacetylenic strands.…”
Section: Introductionmentioning
confidence: 94%
“…8,9 Naphthacene ͑also referred to as tetracene͒, pentacene, and derivative compounds have been used recently to prepare highly ordered conducting organic materials or thin films with particularly large charge carrier mobilities. 10 In contrast with the prevailing view 11 that large acenes have a closed-shell singlet or open-shell triplet electronic ground states, a few groups [12][13][14][15][16] recently conjectured that large acenes such as hexacene, heptacene, or octacene should rather be regarded as open-shell singlet biradical systems, as a result of the instability of unrestricted ͑UBLYP, UB3LYP, UPW91, UBPW91, etc.͒ wave functions, in conjunction with rather modest basis sets ͑STO-3G, 6-31G ‫ء‬ , or cc-pVDZ͒. This in-stability was diagnosed 12 from the fact that in these unrestricted calculations the two outermost singly occupied ␣ and ␤ spin orbitals do not smoothly follow the D 2h symmetry point group imposed by the nuclear frame, but rather reflect an overwhelmingly strong symmetry breaking of the electronic wave function, 12 in the form of a localization of the two frontier electrons on opposite polyacetylenic strands.…”
Section: Introductionmentioning
confidence: 94%
“…First, although in this work the optimized geometries for acenes up to 12 all collapse to the D 2h point group, it does not necessarily mean that it will always keep such a high symmetry without any Jahn-Teller distortion or Peierls distortion as the number of benzene rings becomes even larger. In fact, some existing literature has already pointed out the possibility (95). Second, even if we assume the absence of the distortion and trust a geometry with D 2h symmetry, from Fig.…”
Section: St Energy Gapmentioning
confidence: 99%
“…magnetism without ions presenting partially filled d or f shells [7][8][9][10][11][12]. If the larger magnetic acenes can be stabilized, their magnetism coupled with the long spin-diffusion length will make this material class extremely appealing for the next generation of organic spintronics devices [29][30][31][32][33].…”
Section: Introductionmentioning
confidence: 99%
“…The smaller acenes have a non-magnetic (diamagnetic) ground state. For the higher acenes calculations predict the edges of the molecule to be spin polarized [7][8][9]11,12,18]. In this case there are two degenerate highest occupied molecular orbitals (HOMOs), each of them populated by a single electron.…”
Section: Introductionmentioning
confidence: 99%