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Keywords = nanobands

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39 pages, 6816 KiB  
Review
Symmetry and Combinatorial Concepts for Cyclopolyarenes, Nanotubes and 2D-Sheets: Enumerations, Isomers, Structures Spectra & Properties
by Krishnan Balasubramanian
Symmetry 2022, 14(1), 34; https://doi.org/10.3390/sym14010034 - 28 Dec 2021
Cited by 4 | Viewed by 2846
Abstract
This review article highlights recent developments in symmetry, combinatorics, topology, entropy, chirality, spectroscopy and thermochemistry pertinent to 2D and 1D nanomaterials such as circumscribed-cyclopolyarenes and their heterocyclic analogs, carbon and heteronanotubes and heteronano wires, as well as tessellations of cyclopolyarenes, for example, kekulenes, [...] Read more.
This review article highlights recent developments in symmetry, combinatorics, topology, entropy, chirality, spectroscopy and thermochemistry pertinent to 2D and 1D nanomaterials such as circumscribed-cyclopolyarenes and their heterocyclic analogs, carbon and heteronanotubes and heteronano wires, as well as tessellations of cyclopolyarenes, for example, kekulenes, septulenes and octulenes. We establish that the generalization of Sheehan’s modification of Pólya’s theorem to all irreducible representations of point groups yields robust generating functions for the enumeration of chiral, achiral, position isomers, NMR, multiple quantum NMR and ESR hyperfine patterns. We also show distance, degree and graph entropy based topological measures combined with techniques for distance degree vector sequences, edge and vertex partitions of nanomaterials yield robust and powerful techniques for thermochemistry, bond energies and spectroscopic computations of these species. We have demonstrated the existence of isentropic tessellations of kekulenes which were further studied using combinatorial, topological and spectral techniques. The combinatorial generating functions obtained not only enumerate the chiral and achiral isomers but also aid in the machine construction of various spectroscopic and ESR hyperfine patterns of the nanomaterials that were considered in this review. Combinatorial and topological tools can become an integral part of robust machine learning techniques for rapid computation of the combinatorial library of isomers and their properties of nanomaterials. Future applications to metal organic frameworks and fullerene polymers are pointed out. Full article
(This article belongs to the Section Chemistry: Symmetry/Asymmetry)
Show Figures

Figure 1

Figure 1
<p>Structures of kekulene, septulene and circumkekulene in the series of circum-polyarenes. Reprinted with permission from [<a href="#B124-symmetry-14-00034" class="html-bibr">124</a>] copyright (2018) American Chemical Society.</p>
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<p>Structures of coronoids and circumscribed-coronoids with holes forming <span class="html-italic">D</span><sub>6<span class="html-italic">h</span></sub> symmetries (Reprinted with permission from [<a href="#B75-symmetry-14-00034" class="html-bibr">75</a>] copyright (1993) American Chemical Society).</p>
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<p>A TUC4[4,m]-Tubular nanotube of cross section C<sub>4</sub> of length m. Reprinted with permission from [<a href="#B129-symmetry-14-00034" class="html-bibr">129</a>] copyright (2021) Taylor &amp; Francis.</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of even length m (20): <span class="html-italic">D</span><sub>6<span class="html-italic">h</span></sub>.</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of odd length m (21): <span class="html-italic">D</span><sub>6<span class="html-italic">h</span></sub>. Reprinted with permission from [<a href="#B129-symmetry-14-00034" class="html-bibr">129</a>] copyright (2021) Taylor &amp; Francis.</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of even length: One of achiral isomers enumerated in <a href="#symmetry-14-00034-t004" class="html-table">Table 4</a> for the partition [100 20].</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of even length: One of chiral isomers enumerated in <a href="#symmetry-14-00034-t004" class="html-table">Table 4</a> out of 1,227,592,588,139,680,180,808 chiral pairs for the partition [100 20]. Reprinted with permission from [<a href="#B129-symmetry-14-00034" class="html-bibr">129</a>] copyright (2021) Taylor &amp; Francis.</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of odd length: One of achiral isomers enumerated in <a href="#symmetry-14-00034-t005" class="html-table">Table 5</a> for the partition [105 21].</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of odd length: One of chiral isomers enumerated in <a href="#symmetry-14-00034-t004" class="html-table">Table 4</a> out of 17,889,827,492,074,590,075,716 chiral pairs for the partition [105 21].</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of even length with alternating arrangement of carbon and nitrogen atoms: One of achiral isomers enumerated in <a href="#symmetry-14-00034-t004" class="html-table">Table 4</a> for the partition [60 60].</p>
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<p>Tubular nanotube of cross section C<sub>6</sub> of odd length with alternating arrangement of carbon and nitrogen atoms: One of achiral isomers enumerated in <a href="#symmetry-14-00034-t005" class="html-table">Table 5</a> for the partition [63 63]. Reprinted with permission from [<a href="#B129-symmetry-14-00034" class="html-bibr">129</a>] copyright (2021) Taylor &amp; Francis.</p>
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<p>(<b>Left</b>) A Tessellation of kekulene providing cavities to trap F<sup>−</sup> ions; Octulenes have been proposed to have suitable pore size to transport Cl<sup>−</sup>. Reprinted with permission from [<a href="#B144-symmetry-14-00034" class="html-bibr">144</a>] copyright (2021) American Chemical Society. (<b>Right</b>) Porphyrin-analogs of Kekulene tessellations as complexation traps for metal ions such as Cd2+, Hg+2, and U(VI) ions. Figure shows a complex of Cd2+ with porphyrin-analog of kekulene; the distance between Cd and N is roughly 2.75 Ǻ° providing an optimal cavity trap Cd2+. Reprinted with permission from [<a href="#B160-symmetry-14-00034" class="html-bibr">160</a>] copyright (2021) Springer Nature. (<b>Bottom</b>) A polyphenolic compound derived from septulene as a marcocycle crown for toxic heavy metal ions. Figure shows a proposed complex with Cd(II) and also intramolecular hydrogen bonds exhibited by the complex. Reprinted with permission from [<a href="#B160-symmetry-14-00034" class="html-bibr">160</a>] copyright (2021) Springer Nature.</p>
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<p>Two topological tessellations of kekulenes that exhibit the same graph entropies: (<b>Left</b>; (<b>a</b>)) <span class="html-italic">AHK</span>(2) (<b>Right</b>; (<b>b</b>)) <span class="html-italic">RK</span>(3,3). Reprinted with permission from [<a href="#B144-symmetry-14-00034" class="html-bibr">144</a>] copyright (2021) American Chemical Society.</p>
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<p>Computed ESR hyperfine patterns of (<b>Top</b>; (<b>a</b>)) AHK(2) (<b>Bottom</b>; (<b>b</b>)) RK(3,3). Reprinted with permission from [<a href="#B144-symmetry-14-00034" class="html-bibr">144</a>] copyright (2021) American Chemical Society.</p>
Full article ">Figure 14 Cont.
<p>Computed ESR hyperfine patterns of (<b>Top</b>; (<b>a</b>)) AHK(2) (<b>Bottom</b>; (<b>b</b>)) RK(3,3). Reprinted with permission from [<a href="#B144-symmetry-14-00034" class="html-bibr">144</a>] copyright (2021) American Chemical Society.</p>
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<p>A 3D geometrical structure of a nanoband or a necklace-choker made of 16 hexagons.</p>
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<p>(<b>Top</b>) Zigzag versus (<b>Bottom</b>) Linear Arrangements of (C<sub>60</sub>)<sub>n,</sub> Reproduced under creative commons License from Ref. [<a href="#B161-symmetry-14-00034" class="html-bibr">161</a>].</p>
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13 pages, 3886 KiB  
Article
Structural, Morphological, and Optical Properties of Iron Doped WO3 Thin Film Prepared by Pulsed Laser Deposition
by Mariana Osiac, Nicoleta Cioatera and Maria Jigau
Coatings 2020, 10(4), 412; https://doi.org/10.3390/coatings10040412 - 21 Apr 2020
Cited by 11 | Viewed by 2901
Abstract
The iron doped tungsten-oxide (Fe and WO3) thin film with different morphology and crystalline structures were obtained for different substrate temperatures at the oxygen pressure of 14.66 Pa. The Fe-doped WO3 films were deposited by pulsed laser deposition (PLD). The [...] Read more.
The iron doped tungsten-oxide (Fe and WO3) thin film with different morphology and crystalline structures were obtained for different substrate temperatures at the oxygen pressure of 14.66 Pa. The Fe-doped WO3 films were deposited by pulsed laser deposition (PLD). The influence of the substrate temperature on the surface and on the crystalline phases of the films was studied. The XRD (X-ray diffraction) analysis indicates the changing in the crystalline phases from γ-monoclinic to a mixture of γ-monoclinic and hexagonal phases dependent on the temperature of annealing and as-grown films. Related to the as-grown and annealing films conditions, the SEM (scanning electron microscopy) shows a change in the image surface from nanoneedles, to nanoporous, and further to long nanowires and broad nanobands. Energy-dispersive X-ray spectroscopy (EDX) shows the elemental composition of the Fe-doped WO3 film as-grown and after annealing treatment. Raman spectroscopy presented the main vibration mode of the Fe-doped WO3 thin film. The optical energy bandgap of the films is decreasing as the substrate temperature increases. Full article
(This article belongs to the Section Surface Characterization, Deposition and Modification)
Show Figures

Figure 1

Figure 1
<p>The GIXRD pattern for WO<sub>3</sub> and Fe-doped WO<sub>3</sub> thin films, respectively. (<b>a</b>) S1 sample: the red spectrum corresponds to S1 grown at T = 600 °C; the green, blue, and magenta spectra belong to S1 samples annealed at T = 700, 720, and T = 750 °C, respectively. (<b>b</b>) S2 sample: the dark green spectrum belongs to S2 grown at 720 °C and the pink spectrum corresponds to S2 annealed to 750 °C, respectively. The black spectrum corresponds to WO<sub>3</sub> deposited at T = 600 °C. The dotted lines show the γ-monoclinic plane positions of WO<sub>3</sub>. The circles correspond to hexagonal phase.</p>
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<p>The top view topography of the Fe-doped WO<sub>3</sub>: (<b>a</b>) the surface of the film grown at T = 600 °C, (<b>b</b>) T = 650 °C, (<b>c</b>) T = 700 °C, (<b>d</b>) T = 720 °C, (<b>e</b>) T = 750 °C.</p>
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<p>The top view topography of the Fe-doped WO<sub>3</sub>: (<b>a</b>) S1 sample–the surface of the film grown at T = 600 °C, (<b>b</b>) the film annealed at T = 700 °C, (<b>c</b>) the film annealed at T = 720 °C, (<b>d</b>) the film annealed at T = 750 °C, (<b>e</b>) S2 sample–the film grown at 720 °C, (<b>f</b>) the film annealed at 750 °C.</p>
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<p>The image of the S1 sample annealed at 750 °C; (<b>a</b>) the EDX mapping between the nanowires, (<b>b</b>) 10 EDX points selected on the surface.</p>
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<p>The EDX mapping of the S2 sample at T = 750 °C. (<b>a</b>) EDX mapping on a large nanoband; (<b>b</b>) EDX mapping made on a large nanoband and slice of the film surface.</p>
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<p>Raman spectra of WO<sub>3</sub> and Fe-doped WO<sub>3</sub> films. (<b>a</b>) the black spectrum belongs WO<sub>3</sub> film grown at 600 °C; the blue spectrum belongs to S1 sample grown at 600 °C; the red and green spectra belong to S1 sample annealed at 700 and 720 °C, respectively. (<b>b</b>) the red spectrum belongs to S1 sample annealed at 750 °C, the green spectrum to S2 sample as-grown at 720 °C and the black spectrum to S2 sample annealed at 750 °C.</p>
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<p>The <span class="html-italic">Eg</span> for WO<sub>3</sub> film and Fe-doped WO<sub>3</sub> film samples. (<b>a</b>) WO<sub>3</sub> film grown at 600 °C (undoped); (<b>b</b>) Fe-doped WO<sub>3</sub> as-grown at 720 °C; (<b>c</b>) Fe-doped WO<sub>3</sub> annealed at 720 °C.</p>
Full article ">
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