Nothing Special   »   [go: up one dir, main page]

You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (849)

Search Parameters:
Keywords = fullerene

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
12 pages, 2756 KiB  
Article
C60 Fullerene Reduces the Development of Post-Traumatic Dysfunction in Rat Soleus Muscle
by Yuriy Prylutskyy, Dmytro Nozdrenko, Olexandr Motuziuk, Svitlana Prylutska, Kateryna Bogutska, Olga Abramchuk, Alevtyna Morenko, Daria Franskevych, Peter Scharff and Uwe Ritter
Int. J. Mol. Sci. 2024, 25(22), 12206; https://doi.org/10.3390/ijms252212206 - 14 Nov 2024
Viewed by 291
Abstract
Traumatic skeletal muscle injury is a complex pathology caused by high-energy trauma to muscle tissue. Previously, a positive effect was established when C60 fullerene was administered against the background of muscle ischemia, mechanical muscle injury, and other muscle dysfunctions, which probably protected [...] Read more.
Traumatic skeletal muscle injury is a complex pathology caused by high-energy trauma to muscle tissue. Previously, a positive effect was established when C60 fullerene was administered against the background of muscle ischemia, mechanical muscle injury, and other muscle dysfunctions, which probably protected the muscle tissue from damage caused by oxidative stress. Using tensiometry and biochemical analysis, the biomechanical parameters of skeletal muscle contraction and biochemical indices of the blood of rats 15 days after traumatic injury of the soleus muscle caused by myocyte destruction by compression were studied. The intraperitoneal administration of C60 fullerene aqueous solution (C60FAS) in a daily dose of 1 mg/kg improved its contractile function by 28–40 ± 2% and the values of the investigated biochemical indices of the animals’ blood by 15–34 ± 2% relative to the trauma group. The obtained results indicate the potential ability of C60 fullerenes, as powerful antioxidants, to reduce the development of post-traumatic dysfunction of the soleus muscle. Full article
(This article belongs to the Special Issue Recent Research of Nanomaterials in Molecular Science)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Force generation curves of soleus muscle contraction 15 days after its injury: mechanograms of muscle contraction (<b>a</b>); integrated muscle power (S; relative to the control, which was taken as 100%) (<b>b</b>); injury and injury + C<sub>60</sub>FAS—injury group (<span class="html-italic">n</span> = 30) and injury group against the background of C<sub>60</sub>FAS injection (<span class="html-italic">n</span> = 30), respectively; 1, 2, and 3—the severity of muscle injury; t<sub>start</sub>—the time between the beginning of stimulation and the beginning of muscle contraction; t<sub>0</sub>—the time between the end of stimulation and the power curve reaching the initial level; * <span class="html-italic">p</span> &lt; 0.05 relative to the control group (<span class="html-italic">n</span> = 30); # <span class="html-italic">p</span> &lt; 0.05 relative to the injury group (<span class="html-italic">n</span> = 30).</p>
Full article ">Figure 2
<p>The biomechanical parameters of soleus muscle contraction 15 days after its injury: F<sub>min</sub>—minimal force of muscle contraction (<b>a</b>); t<sub>0</sub>—time between the end of stimulation and the force curve reaching the initial level (<b>b</b>); t<sub>start</sub>—time between the beginning of stimulation and the beginning of muscle contraction (<b>c</b>); injury and injury + C<sub>60</sub>FAS—injury group (<span class="html-italic">n</span> = 30) and injury group against the background of C<sub>60</sub>FAS injections (<span class="html-italic">n</span> = 30), respectively; 1, 2, and 3—severity of muscle injury; * <span class="html-italic">p</span> &lt; 0.05 relative to the control group (<span class="html-italic">n</span> = 30); # <span class="html-italic">p</span> &lt; 0.05 relative to the injury group (<span class="html-italic">n</span> = 30).</p>
Full article ">Figure 3
<p>The mechanograms of soleus muscle contraction induced by the stimulation frequency of 1 Hz with a duration of 500 s, on the 15th day after traumatic injury initiation: injury and injury + C<sub>60</sub>FAS—injury group (<span class="html-italic">n</span> = 30) and injury group against the background of C<sub>60</sub>FAS injection (<span class="html-italic">n</span> = 30), respectively; 1, 2, and 3—severity of muscle injury; t<sub>50</sub>—time of contraction force reduction by 50% from the initial level; S—integrated muscle power.</p>
Full article ">Figure 4
<p>The biomechanical parameters of soleus muscle contraction 15 days after its injury: curves of changes in maximum contraction forces (F<sub>max</sub>) during 500 s of stimulation pool (<b>a</b>); changes in integrated muscle power (S) during 500 s of stimulation (<b>b</b>); time of reduction of contraction force by 50% from the initial level (t<sub>50</sub>) (<b>c</b>); injury and injury + C<sub>60</sub>FAS—injury group (<span class="html-italic">n</span> = 30) and injury group against the background of C<sub>60</sub>FAS injections (<span class="html-italic">n</span> = 30), respectively; 1, 2, and 3—severity of muscle injury; * <span class="html-italic">p</span> &lt; 0.05 relative to the control group (<span class="html-italic">n</span> = 30); # <span class="html-italic">p</span> &lt; 0.05 relative to the injury group (<span class="html-italic">n</span> = 30).</p>
Full article ">Figure 5
<p>The biochemical indices of fatigue processes’ development (the levels of creatinine and lactate and the activities of CPK and LDH in blood plasma) 15 days after soleus muscle injury: injury and injury + C<sub>60</sub>FAS—the injury group (<span class="html-italic">n</span> = 30) and the injury group against the background of C<sub>60</sub>FAS injections (<span class="html-italic">n</span> = 30), respectively; 1, 2, and 3—degrees of severity of muscle injury; * <span class="html-italic">p</span> &lt; 0.05 relative to the control group (<span class="html-italic">n</span> = 30); ** <span class="html-italic">p</span> &lt; 0.04 relative to the control group (<span class="html-italic">n</span> = 30); # <span class="html-italic">p</span> &lt; 0.05 relative to the injury group (<span class="html-italic">n</span> = 30).</p>
Full article ">
15 pages, 4194 KiB  
Article
Encapsulating Proton Inside C60 Fullerene: A Density Functional Theory Study on the Electronic Properties of Cationic X+@C60 (X+ = H+, H3O+ and NH4+)
by Lei Zhao and Bo Wang
Int. J. Mol. Sci. 2024, 25(22), 12014; https://doi.org/10.3390/ijms252212014 - 8 Nov 2024
Viewed by 300
Abstract
Confining protons into an enclosed carbon cage is expected to give rise to unique electronic properties for both the inner proton and the outer cage. In this work, we systematically investigated the geometric and electronic structures of cationic X+@C60 (X [...] Read more.
Confining protons into an enclosed carbon cage is expected to give rise to unique electronic properties for both the inner proton and the outer cage. In this work, we systematically investigated the geometric and electronic structures of cationic X+@C60 (X+ = H+, H3O+, and NH4+), and their corresponding neutral species (X = H2O, NH3), by quantum chemical density functional theory calculations. We show that C60 can trap H2O, NH3, H3O+ and NH4+ at the cage center and only slightly influence their geometries. The single proton clings to the inner wall of C60, forming a C-H chemical bond. The encapsulated neutral species almost do not change the electronic structure of the C60, while the internal cations have obvious effects. The charge transfer effect from the inner species to the C60 cage was found for all X@C60 (X = H2O, NH3) (about 0.0 e), X+@C60 (X+ = H3O+, NH4+) (about 0.5 e) and H+@C60 (about 1.0 e) systems. Encapsulating different forms of protons also regulates the fundamental physico-chemical properties of the hollow C60, such as the HOMO-LUMO gaps, infrared spectra, and electrostatic potential, etc., which are discussed in detail. These findings provide a theoretical insight into protons’ applications, especially in energy. Full article
Show Figures

Figure 1

Figure 1
<p>Structures of C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, and NH<sub>4</sub><sup>+</sup>) and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>) at the B3LYP-D3(BJ)/6-31G(d, p) level of theory. C, H, O, and N atoms are indicated by orange, white, red, and blue spheres, respectively.</p>
Full article ">Figure 2
<p>Energy profile for H diffusion from the atom to the 5-6 bond and 6-6 bond. The atomic geometries of the initial (IS), transition (TS), and final (FS) states are also given. The blue boxes and red circles indicate the 5-6 bond and 6-6 bond of the intrinsic reaction coordinate (IRC), respectively. The diffusion barrier is denoted by an arrow.</p>
Full article ">Figure 3
<p>Electron density difference maps of X/X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>, X = H<sub>2</sub>O, NH<sub>3</sub>) and C<sub>60</sub> cage at the B3LYP-D3(BJ)/6-31G(d, p) level of theory. The green and blue indicate the accumulation and the depletion of the electron density, respectively.</p>
Full article ">Figure 4
<p>Total density of states (TDOS) and the partial density of states (PDOS) for C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>), and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>) at the B3LYP-D3(BJ)/6-31G(d, p) level of theory. Black represents the TDOS of X/X<sup>+</sup>@C<sub>60</sub>. Red and blue lines represent the contribution of two fragments of the C<sub>60</sub> cage and X/X<sup>+</sup> to the DOS, respectively. H and L represent the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO), respectively. The energy gap is marked in the figure (unit is kcal/mol).</p>
Full article ">Figure 5
<p>Frontier molecular orbitals (HOMO and LUMO) for C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>), and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>) at the B3LYP-D3(BJ)/6-31G(d, p) level of theory. The molecular orbitals involved for the first time in confined species are also depicted. Molecular orbitals are denoted by blue and red.</p>
Full article ">Figure 6
<p>IR spectra for X = H<sub>2</sub>O, NH<sub>3</sub>, X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>, and X/X<sup>+</sup>@C<sub>60</sub> at the B3LYP-D3(BJ)/6-31G(d, p) level of theory.</p>
Full article ">Figure 7
<p>The electrostatic potential of C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>), and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>) at the B3LYP-D3(BJ)/6-31G(d, p) level of theory. Blue and red colors represent negative potential and positive potential, respectively (unit is a.u.).</p>
Full article ">Figure 8
<p>Optimized water adsorption structures on C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>), and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>). In these structures, red, white, cyan, and blue denote O, H, C, and N atoms, respectively.</p>
Full article ">Figure 9
<p>The solvation afree energy of C<sub>60</sub>, X<sup>+</sup>@C<sub>60</sub> (X<sup>+</sup> = H<sup>+</sup>, H<sub>3</sub>O<sup>+</sup>, NH<sub>4</sub><sup>+</sup>), and X@C<sub>60</sub> (X = H<sub>2</sub>O, NH<sub>3</sub>) (unit is kcal/mol).</p>
Full article ">
18 pages, 7084 KiB  
Review
Innovative Materials for High-Performance Tin-Based Perovskite Solar Cells: A Review
by Xiansheng Wang, Jianjun Yang, Jian Zhong, Junsheng Yu and Xinjian Pan
Polymers 2024, 16(21), 3053; https://doi.org/10.3390/polym16213053 - 30 Oct 2024
Viewed by 656
Abstract
With the rapid development of lead-based perovskite solar cells, tin-based perovskite solar cells are emerging as a non-toxic alternative. Material engineering has been an effective approach for the fabrication of efficient perovskite solar cells. This paper summarizes the novel materials used in tin-based [...] Read more.
With the rapid development of lead-based perovskite solar cells, tin-based perovskite solar cells are emerging as a non-toxic alternative. Material engineering has been an effective approach for the fabrication of efficient perovskite solar cells. This paper summarizes the novel materials used in tin-based perovskite solar cells over the past few years and analyzes the roles of various materials in tin-based devices. It is found that self-assembling materials and fullerene derivatives have shown remarkable performance in tin-based perovskite solar cells. Finally, this article discusses design strategies for new materials, providing constructive suggestions for the development of innovative materials in the future. Full article
Show Figures

Figure 1

Figure 1
<p>NREL announces latest perovskite solar cell efficiencies.</p>
Full article ">Figure 2
<p>(<b>a</b>) Schematic illustration of defect profile in pristine Sn perovskite film with a variety of Sn- or I-related defects, and corresponding passivation strategy caused by hydrogen bonding and van der Waals interactions between perovskite and α-T [<a href="#B35-polymers-16-03053" class="html-bibr">35</a>]. (<b>b</b>) Efficient devices prepared with optimal Br content [<a href="#B33-polymers-16-03053" class="html-bibr">33</a>]. (<b>c</b>) Schematics of interactions and grain growth mechanism of FASnI3 perovskite with thioacetamide [<a href="#B36-polymers-16-03053" class="html-bibr">36</a>]. (<b>d</b>) Adding 10% AC and 3% Rb optimizes the device (E<sub>1</sub>AC<sub>10</sub>Rb<sub>3</sub>) to achieve 14.5% power conversion efficiency [<a href="#B37-polymers-16-03053" class="html-bibr">37</a>].</p>
Full article ">Figure 3
<p>Schematic diagrams of (<b>a</b>) the n-i-p-type TPSC and (<b>b</b>) the p-i-n-type TPSC [<a href="#B38-polymers-16-03053" class="html-bibr">38</a>]. (<b>c</b>) Energy level diagram of a typical p-i-n-type TPSC [<a href="#B38-polymers-16-03053" class="html-bibr">38</a>].</p>
Full article ">Figure 4
<p>Schematics of representative (<b>a</b>) polyelectrolytes and (<b>b</b>) soluble processable polymers with EDOT derivates via copolymer engineering and side-chain tailoring [<a href="#B39-polymers-16-03053" class="html-bibr">39</a>].</p>
Full article ">Figure 5
<p>(<b>a</b>) Device configuration of the HTL-free tin PSCs with a structure of ITO/FASnI<sub>3</sub>-based perovskite/PCBM/BCP/Ag and SEM cross-sectional image of the HTL-free tin PSCs [<a href="#B48-polymers-16-03053" class="html-bibr">48</a>]. (<b>b</b>) A layer of PEDOT:PSS was inserted in-between the ITO electrode and SA-modified PEDOT:PSS to form a pseudo bilayered PS/SA@PS HTL [<a href="#B40-polymers-16-03053" class="html-bibr">40</a>]. (<b>c</b>) Post-treatment of PEDOT:PSS surfaces using diammonium salts of aromatic acetic acid dissolved in highly volatile but interacting solvents to modify the surface [<a href="#B45-polymers-16-03053" class="html-bibr">45</a>]. (<b>d</b>) Trimethoxy(3,3,3-trifluoropropyl)silane (F3-TMOS) with molecular dipole moments pointing to the hole transport layer was used as a buried interface modification material [<a href="#B34-polymers-16-03053" class="html-bibr">34</a>].</p>
Full article ">Figure 6
<p>SAM molecules that have been reported. Right: Chemical structure of reported self-assembled monolayers (SAMs) for the PSCs. Chemical structures of SAMs: PQx (1), TQx, (2), PQxD (3) and TQxD (4) for Sn-based PSCs studied in the reference [<a href="#B56-polymers-16-03053" class="html-bibr">56</a>].</p>
Full article ">Figure 7
<p>(<b>a</b>) Schematic diagram of SAM-2PADBC-embedded NiOx film and differential charge density simulation of the perovskite–NiOx and perovskite–2PADBC [<a href="#B57-polymers-16-03053" class="html-bibr">57</a>]. (<b>b</b>) The compact surface morphology of the Sn perovskite fabricated on bilayers consisting of 2PACz monolayer on PEDOT-PSS and the suppression of direct contact between PEDOT-PSS and perovskite film [<a href="#B59-polymers-16-03053" class="html-bibr">59</a>]. (<b>c</b>) In the two-step deposition, the SnI<sub>2</sub> in DMSO and FAI in a cosolvent system were sequentially deposited using spin-coating to form FASnI<sub>3</sub> [<a href="#B60-polymers-16-03053" class="html-bibr">60</a>]. (<b>d</b>) Mechanical behavior of the ETL/MHP interface [<a href="#B61-polymers-16-03053" class="html-bibr">61</a>]. (<b>e</b>) Schematic of the Sn-PSC based on CEPA buried interface modification [<a href="#B58-polymers-16-03053" class="html-bibr">58</a>].</p>
Full article ">Figure 8
<p>Schematic of the defects and functional molecules [<a href="#B63-polymers-16-03053" class="html-bibr">63</a>].</p>
Full article ">Figure 9
<p>(<b>a</b>) A tin-based perovskite solar cell with significantly improved stability against oxidation was prepared by introducing hydroxybenzene sulfonic acid or a salt thereof as an antioxidant additive into the perovskite precursor solution [<a href="#B70-polymers-16-03053" class="html-bibr">70</a>]. (<b>b</b>) Schematic illustration of possible SRTSP mechanism for PHCl [<a href="#B73-polymers-16-03053" class="html-bibr">73</a>]. (<b>c</b>) Simultaneous band energy alignment and trap site passivation has been achieved by regulating the A-site cation of tin halide perovskites [<a href="#B71-polymers-16-03053" class="html-bibr">71</a>]. (<b>d</b>) Ethylenediammonium halide salts (i.e., EDAI2 and EDABr2) as additives in Sn perovskite [<a href="#B68-polymers-16-03053" class="html-bibr">68</a>].</p>
Full article ">Figure 10
<p>(<b>a</b>) Trimethylthiourea (3T) was introduced during spin-coating of FASnI<sub>3</sub> films [<a href="#B75-polymers-16-03053" class="html-bibr">75</a>]. (<b>b</b>) Schematic device structure of the inverted perovskite devices. Current density–voltage (J-V) curves of the champion devices containing pure 3D FASnI<sub>3</sub> and 2D/3D perovskite with different FPEABr [<a href="#B69-polymers-16-03053" class="html-bibr">69</a>]. (<b>c</b>) The structure of the Sn-based PSC device. The energy level diagram of the Sn-based PSC device [<a href="#B76-polymers-16-03053" class="html-bibr">76</a>]. (<b>d</b>) Sn 3d<sub>5/2</sub> X-ray photoelectron spectroscopy spectra of the SnI<sub>2</sub>, CPPF-SnI<sub>2</sub> and TPPF-SnI<sub>2</sub> films. a.u., arbitrary units. Simulations of the interaction between the CPPF and perovskite components showing N (highlighted by red dashed circles) coordinating with one <math display="inline"><semantics> <mrow> <mi>S</mi> <mi mathvariant="normal">n</mi> <msubsup> <mi>I</mi> <mn>6</mn> <mo>−</mo> </msubsup> </mrow> </semantics></math> cluster and simulations of the interaction between TPPF and perovskite components showing N coordinating with two <math display="inline"><semantics> <mrow> <mi>S</mi> <mi mathvariant="normal">n</mi> <msubsup> <mi>I</mi> <mn>6</mn> <mo>−</mo> </msubsup> </mrow> </semantics></math> clusters [<a href="#B18-polymers-16-03053" class="html-bibr">18</a>].</p>
Full article ">Figure 11
<p>(<b>a</b>) C60. (<b>b</b>) PC61BM. (<b>c</b>) IC<sub>60</sub>BA. (<b>d</b>) Band structures of C<sub>60</sub>,PC<sub>61</sub>BM, and IC<sub>60</sub>BA. (<b>e</b>) The field effect transistor (FET) transfer characteristics of C<sub>60</sub>, PC<sub>61</sub>BM, and IC<sub>60</sub>BA. (<b>f</b>) Electroluminescence spectra of the Sn-based perovskites films with different ETLs (PC<sub>61</sub>BM and IC<sub>60</sub>BA) under a bias voltage of 2 V [<a href="#B38-polymers-16-03053" class="html-bibr">38</a>].</p>
Full article ">Figure 12
<p>(<b>a</b>) Precise synthesis route of multidentate fullerenes, and single-crystal structures of FM3, FM4, FM5, and FM6, accompanied by corresponding fullerene structural models in the lower right corner; the solid vertex indicates that the position is occupied by a functional group, while a hollow vertex indicates that it is not occupied [<a href="#B83-polymers-16-03053" class="html-bibr">83</a>]. (<b>b</b>) Design and synthesis of a cross-linkable fullerene, lipoic acid-functionalized C60 fuller pyrrolidinium iodide (FTAI) for the preparation of high-efficiency devices [<a href="#B84-polymers-16-03053" class="html-bibr">84</a>]. (<b>c</b>) Schematic illustrations of the effect of FTAI on perovskite film. Molecular structure of FTAI and diagram of cross-linked FTAI interact with perovskite. Schematic diagrams of formation and bending performance of the control and TA- and FTAI-based perovskite films [<a href="#B84-polymers-16-03053" class="html-bibr">84</a>]. (<b>d</b>) Optimized slab model (1 0 0) of perovskite of W/T and PMPS [<a href="#B85-polymers-16-03053" class="html-bibr">85</a>].</p>
Full article ">Figure 13
<p>(<b>a</b>) Schematic of interaction between [SnI<sub>6</sub>]<sup>4−</sup> and PEA (left) or XDA (right) [<a href="#B86-polymers-16-03053" class="html-bibr">86</a>]. (<b>b</b>) Left: Deposition process of 2D/3D perovskite using different organic spacers; cyclohexylammonium (CHA), piperidinium (PD), and morpholinium (MP). Right: Schematic illustration of the crystal structure of MP-based 2D/3D perovskite [<a href="#B87-polymers-16-03053" class="html-bibr">87</a>]. (<b>c</b>) Structural model of MP-based 2D perovskite. Structural model of 2D MP-based perovskite with vacancies. V<sub>I</sub>(e): neutral I vacancies in the equatorial position; V<sub>I</sub>(a): neutral I vacancies in the apical position; V<sub>Sn</sub>: neutral Sn vacancies [<a href="#B87-polymers-16-03053" class="html-bibr">87</a>].</p>
Full article ">
14 pages, 361 KiB  
Article
On a Study of Photoionization of Atoms and Ions from Endohedral Anions
by Valeriy K. Dolmatov, Larissa V. Chernysheva and Victor G. Yarzhemsky
Atoms 2024, 12(11), 56; https://doi.org/10.3390/atoms12110056 - 30 Oct 2024
Viewed by 330
Abstract
We study the relationship between the results of two qualitatively different semi-empirical models for photoionization cross sections, σn, of neutral atoms (A) and their cations (A+) centrally encapsulated inside a fullerene anion, CNq [...] Read more.
We study the relationship between the results of two qualitatively different semi-empirical models for photoionization cross sections, σn, of neutral atoms (A) and their cations (A+) centrally encapsulated inside a fullerene anion, CNq, where q represents the negative excess charge on the shell. One of the semi-empirical models, broadly employed in previous studies, assumes a uniform excess negative charge distribution over the entire fullerene cage, by analogy with a charged metallic sphere. The other model, presented here, considers the quantum states of the excess electrons on the shell, determined by specific n and values of their quantum numbers. Remarkably, both models yield similar photoionization cross sections for the encapsulated species. Consequently, we find that the photoionization of the encapsulated atoms or cations inside the CNq anion is influenced only slightly by the quantum states of the excess electrons on the fullerene cage. Furthermore, we demonstrate that the influence decreases even further as the size of the fullerene cage increases. All this holds true at least under the assumption that the encapsulated atom or cation is compact, i.e., its electron density remains primarily within itself rather than being drawn into the fullerene shell. This remarkable finding results from Hartree–Fock calculations combined with a popular modeling of the fullerene shell which is simulated by an attractive spherical annular potential. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Calculated <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> radial function of hydrogen in the structureless <math display="inline"><semantics> <msubsup> <mrow> <mi mathvariant="normal">H</mi> <mo>@</mo> <mi mathvariant="normal">C</mi> </mrow> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> </semantics></math> system, along with the <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> function for hydrogen, and the <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>3</mn> <mi>d</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> radial functions of the attached electrons in the structured <math display="inline"><semantics> <mrow> <mi mathvariant="normal">H</mi> <mo>@</mo> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mi>n</mi> <mi mathvariant="sans-serif-italic">ℓ</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> systems (<math display="inline"><semantics> <mrow> <mi>n</mi> <mi mathvariant="sans-serif-italic">ℓ</mi> <mo>=</mo> <mn>2</mn> <mi>p</mi> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mi>n</mi> <mi mathvariant="sans-serif-italic">ℓ</mi> <mo>=</mo> <mn>3</mn> <mi>d</mi> </mrow> </semantics></math>), as indicated in the figure. (<b>b</b>) The same as in (<b>a</b>) but for the giant <math display="inline"><semantics> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </semantics></math>. Note that the <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> function for the encapsulated hydrogen atom is practically the same in both the structureless and structured models of the endohedral fullerene anion.</p>
Full article ">Figure 2
<p>Calculated <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> photoionization cross sections for the H<math display="inline"><semantics> <mrow> <mo>(</mo> <mn>1</mn> <mi>s</mi> <mo>)</mo> </mrow> </semantics></math> atom confined inside (<b>a</b>) the structureless H@<math display="inline"><semantics> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> </semantics></math> and structured H@<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and H@<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> systems, as well as (<b>b</b>) the structureless H@<math display="inline"><semantics> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>240</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> </semantics></math> and structured H@<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>240</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and H@<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>240</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> giant fullerene anions, as designated in the figure.</p>
Full article ">Figure 3
<p>(<b>a</b>) Calculated <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> of neutral He in He<math display="inline"><semantics> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> </semantics></math>, along with the <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>3</mn> <mi>d</mi> </mrow> </msub> </semantics></math> functions of the attached electron in the He<math display="inline"><semantics> <mrow> <mo>@</mo> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and He<math display="inline"><semantics> <mrow> <mo>@</mo> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> fullerene anions, as indicated in the figure. (<b>b</b>) Calculated <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> of the <math display="inline"><semantics> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> </semantics></math> ion in the doubly-charged <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msubsup> </mrow> </semantics></math>, along with the <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>2</mn> <mi>s</mi> </mrow> </msub> </semantics></math>, <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>2</mn> <mi>p</mi> </mrow> </msub> </semantics></math>, and <math display="inline"><semantics> <msub> <mi>P</mi> <mrow> <mn>3</mn> <mi>d</mi> </mrow> </msub> </semantics></math> functions of the attached electrons in the doubly-charged <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <mi mathvariant="normal">C</mi> <msup> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <mi mathvariant="normal">C</mi> <msup> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>, as shown in the figure. Note: Similar to the case of the H atom, the <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> function of He in He<math display="inline"><semantics> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> </semantics></math> is nearly identical to the corresponding <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> functions of He in He<math display="inline"><semantics> <mrow> <mo>@</mo> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and He<math display="inline"><semantics> <mrow> <mo>@</mo> <msubsup> <mi mathvariant="normal">C</mi> <mrow> <mn>60</mn> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msubsup> <mrow> <mo>(</mo> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>. The same applies to the <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> function of <math display="inline"><semantics> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> </semantics></math> in the corresponding doubly-charged fullerene anions. Therefore, <math display="inline"><semantics> <mrow> <msub> <mi>P</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> <mrow> <mo>(</mo> <mi>r</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> is only plotted once in both parts of the figure for clarity.</p>
Full article ">Figure 4
<p>(<b>a</b>) Calculated <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> photoionization cross sections of He<math display="inline"><semantics> <mrow> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> as well as He<math display="inline"><semantics> <mrow> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and He<math display="inline"><semantics> <mrow> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> along with <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> for the helium atom in neutral He<math display="inline"><semantics> <msub> <mi>C</mi> <mn>60</mn> </msub> </semantics></math>, as marked in the figure. (<b>b</b>) Calculated <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> photoionization cross sections of <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>, as well as <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> of <math display="inline"><semantics> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> </semantics></math> inside neutral <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>60</mn> </msub> </mrow> </semantics></math>, as marked in the figure.</p>
Full article ">Figure 5
<p>(<b>a</b>) Calculated <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> photoionization cross sections of He<math display="inline"><semantics> <mrow> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>1</mn> </mrow> </msup> </mrow> </semantics></math> as well as He<math display="inline"><semantics> <mrow> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and He<math display="inline"><semantics> <mrow> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> <mrow> <mo>(</mo> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> along with <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> of neutral He<math display="inline"><semantics> <mrow> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> </semantics></math>, as designated in the figure. (<b>b</b>) Calculated <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> photoionization cross sections of <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>2</mn> <mi>p</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msup> <mrow> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> <mrow> <mo>(</mo> <mn>2</mn> <mi>s</mi> <mn>3</mn> <mi>d</mi> <mo>)</mo> </mrow> </mrow> </semantics></math>, as well as <math display="inline"><semantics> <msub> <mi>σ</mi> <mrow> <mn>1</mn> <mi>s</mi> </mrow> </msub> </semantics></math> of <math display="inline"><semantics> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> </semantics></math> in neutral <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">He</mi> <mo>+</mo> </msup> <mo>@</mo> <msub> <mi mathvariant="normal">C</mi> <mn>240</mn> </msub> </mrow> </semantics></math>, as marked in the figure.</p>
Full article ">
17 pages, 4413 KiB  
Article
MAPLE-Deposited Perylene Diimide Derivative Based Layers for Optoelectronic Applications
by Carmen Breazu, Mihaela Girtan, Anca Stanculescu, Nicoleta Preda, Oana Rasoga, Andreea Costas, Ana Maria Catargiu, Gabriel Socol, Andrei Stochioiu, Gianina Popescu-Pelin, Sorina Iftimie, Gabriela Petre and Marcela Socol
Nanomaterials 2024, 14(21), 1733; https://doi.org/10.3390/nano14211733 - 29 Oct 2024
Viewed by 478
Abstract
Nowadays, the development of devices based on organic materials is an interesting research challenge. The performance of such devices is strongly influenced by material selection, material properties, design, and the manufacturing process. Usually, buckminsterfullerene (C60) is employed as electron transport material in organic [...] Read more.
Nowadays, the development of devices based on organic materials is an interesting research challenge. The performance of such devices is strongly influenced by material selection, material properties, design, and the manufacturing process. Usually, buckminsterfullerene (C60) is employed as electron transport material in organic photovoltaic (OPV) devices due to its high mobility. However, considering its low solubility, there have been many attempts to replace it with more soluble non-fullerene compounds. In this study, bulk heterojunction thin films with various compositions of zinc phthalocyanine (ZnPc), a perylene diimide derivative, or C60 were prepared by matrix-assisted pulsed laser evaporation (MAPLE) technique to assess the influence of C60 replacement on fabricated heterostructure properties. The investigations revealed that the optical features and the electrical parameters of the organic heterostructures based on this perylene diimide derivative used as an organic acceptor were improved. An increase in the JSC value (4.3 × 10−4 A/cm2) was obtained for the structures where the perylene diimide derivative acceptor entirely replaced C60 compared to the JSC value (7.5 × 10−8 A/cm2) for the heterostructure fabricated only with fullerene. These results are encouraging, demonstrating the potential of non-fullerene compounds as electron transport material in OPV devices. Full article
(This article belongs to the Section Nanocomposite Materials)
Show Figures

Figure 1

Figure 1
<p>Chemical structure of the organic materials used in the MAPLE deposition and schematic representation of the structure developed with the MAPLE-deposited thin films.</p>
Full article ">Figure 2
<p>FESEM images of the MAPLE-deposited organic thin films.</p>
Full article ">Figure 3
<p>2D AFM images of the MAPLE-deposited organic layers.</p>
Full article ">Figure 4
<p>FTIR spectra of the MAPLE-deposited organic layers: (<b>a</b>) ZnPc and AMC14 thin films and (<b>b</b>) mixed thin films.</p>
Full article ">Figure 5
<p>UV-Vis spectra of the MAPLE-deposited organic layers: (<b>a</b>) single thin films on glass substrates and (<b>b</b>) mixed thin films on ITO–glass substrates.</p>
Full article ">Figure 6
<p>PL spectra of the MAPLE-deposited organic layers: (<b>a</b>) AMC14 thin film on Si substrate and (<b>b</b>) mixed thin films on ITO/glass substrates.</p>
Full article ">Figure 7
<p>J-V characteristics, plotted in the dark (<b>a</b>,<b>b</b>) and under illumination (<b>c</b>,<b>d</b>), of the structures prepared with the MAPLE-deposited organic films.</p>
Full article ">Scheme 1
<p>The synthesis route of the AMC14 compound.</p>
Full article ">
17 pages, 2816 KiB  
Article
Z-Scheme BiVO4/g-C3N4 Photocatalyst—With or Without an Electron Mediator?
by Tomasz Łęcki, Kamila Zarębska, Ewelina Wierzyńska, Krzysztof P. Korona, Paulina Chyży, Piotr Piotrowski and Magdalena Skompska
Molecules 2024, 29(21), 5092; https://doi.org/10.3390/molecules29215092 - 28 Oct 2024
Viewed by 464
Abstract
The hybrid system BiVO4/g-C3N4 is a prospective photocatalyst because of the favorable mutual alignment of the energy bands of both semiconductors. However, the path of the photocatalytic process is still unclear because of contradictory information in the literature [...] Read more.
The hybrid system BiVO4/g-C3N4 is a prospective photocatalyst because of the favorable mutual alignment of the energy bands of both semiconductors. However, the path of the photocatalytic process is still unclear because of contradictory information in the literature on whether the mechanism of charge carrier separation at the BiVO4/g-C3N4 interface is band-to-band or Z-scheme. In this work, we clarified this issue by comparative photocatalytic studies with the use of systems without a mediator and with different kinds of mediators including Au nanoparticles, fullerene derivatives, and the Fe3+/Fe2+ redox couple. Additionally, the charge transfer dynamics at the BiVO4/g-C3N4 and BiVO4/mediator/g-C3N4 interfaces were investigated by time-resolved photoluminescence (TRPL) measurements, while the influence of the mediator on the surface recombination of the charge carriers was verified by intensity-modulated photocurrent spectroscopy (IMPS). We proved that the charge carrier separation at the BiVO4/g-C3N4 interface occurs according to the mechanism typical for a heterojunction of type II, while the incorporation of the mediator between BiVO4 and g-C3N4 leads to the Z-scheme mechanism. Moreover, a very strong synergetic effect on caffeine (CAF) degradation rate was found for the system BiVO4/Au/g-C3N4 in the presence of Fe3+ ions in the CAF solution. Full article
(This article belongs to the Special Issue Advances in Composite Photocatalysts)
Show Figures

Figure 1

Figure 1
<p>SEM images of (<b>a</b>) BiVO<sub>4</sub>, (<b>b</b>) BiVO<sub>4</sub>/Au NPs obtained by Au sputtering and (<b>c</b>) by drop casting of HAuCl<sub>4</sub>, followed by annealing, (<b>d</b>) BiVO<sub>4</sub>/C<sub>60</sub>-MPB, (<b>e</b>) BiVO<sub>4</sub>/Au(NPs)/g-C<sub>3</sub>N<sub>4</sub>. (<b>f</b>) Distribution of N and Au in BiVO<sub>4</sub>/Au(NPs)/g-C<sub>3</sub>N<sub>4</sub> for selected part of the sample.</p>
Full article ">Figure 2
<p>(<b>a</b>) FTIR spectra and (<b>b</b>) optical absorption spectra of BiVO<sub>4</sub> (lines 1), g-C<sub>3</sub>N<sub>4</sub> (lines 2), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> (lines 3), BiVO<sub>4</sub>/Au(NPs)/g-C<sub>3</sub>N<sub>4</sub> (line 4), and Au(NPs) suspended in aqueous solution (line 5). UV-Vis absorption spectra of fullerene derivatives: (<b>c</b>) C<sub>60</sub>-MEB, C<sub>60</sub>-MPB, and C<sub>60</sub>-MPhB, and (<b>d</b>) C<sub>70</sub>-MEB, C<sub>70</sub>-MPB, and C<sub>70</sub>-MPhB dissolved in dichloromethane (chemical structures of fullerene derivatives are depicted in the inset).</p>
Full article ">Figure 3
<p>(<b>a</b>) Band diagram of BiVO<sub>4</sub> with indicated potentials corresponding to the Fermi level of Au, LUMO level of the fullerenes, and oxidation/reduction potentials of the solution species involved in the photocatalytic process. (<b>b</b>) Changes i the concentration ratio (c/c<sub>o</sub>) of CAF in a function of irradiation time with a diode 400 nm, in the presence of bare BiVO<sub>4</sub> (B, line 1), BiVO<sub>4</sub>/Au(NPs) (B/Au, line 2), BiVO<sub>4</sub>/fullerene (B/Ful, line 3), and BiVO<sub>4</sub> in the presence of Fe<sup>3+</sup> ions in the CAF solution (B/Fe<sup>3+</sup>, line 4); inset: the corresponding rate constants of CAF degradation.</p>
Full article ">Figure 4
<p>(<b>a</b>) Comparison of the plots c/c<sub>o</sub> in a function of irradiation time (at diode 400 nm) of CAF solution in the presence of bare BiVO<sub>4</sub> (B, line 1), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> (B/CN, line 2), BiVO<sub>4</sub>/Fe<sup>3+</sup> (B/Fe<sup>3+</sup>, line 3), BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> (B/Au/CN, line 4), BiVO<sub>4</sub>/C<sub>60</sub>-MPB/g-C<sub>3</sub>N<sub>4</sub> (B/Ful/CN, line 5), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> in the presence of Fe<sup>3+</sup> ions (B/CN/Fe<sup>3+</sup>, line 6), and BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> in the presence of Fe<sup>3+</sup> ions (B/Au/CN/Fe<sup>3+</sup>, line 7). (<b>b</b>) Comparison of apparent rate constants of the photocatalytic decomposition of CAF with the use of t different photocatalytic systems, obtained from the plots presented in (<b>a</b>). (<b>c</b>) Band diagram and proposed scheme of photocatalytic CAF degradation with the use of BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> without a mediator. (<b>d</b>) Band diagram and proposed scheme of photocatalytic CAF degradation with the use of BiVO<sub>4</sub>/M/g-C<sub>3</sub>N<sub>4</sub>, where M is the charge separation mediator: Au, fullerene, or Fe<sup>3+</sup> ions.</p>
Full article ">Figure 5
<p>(<b>a</b>) PL spectra of the solution containing 5⋅10<sup>−4</sup> M TA and 2⋅10<sup>−3</sup> M NaOH after 10 min of illumination in the presence of BiVO<sub>4</sub> (line 1), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> (line 2), and BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> (line 3). The dashed line (0) corresponds to the background solution (without illumination); the excitation wavelength was 315 nm. Evolution of UV-vis spectra of CAF solution during irradiation in the presence of (<b>b</b>) BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> and (<b>c</b>) BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub>.</p>
Full article ">Figure 6
<p>(<b>a</b>) Photoluminescence spectra and (<b>b</b>) PL transients recorded at 530 nm in air for g-C<sub>3</sub>N<sub>4</sub> (curves1), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> (curves 2), BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> (curves 3), BiVO<sub>4</sub>/C<sub>60</sub>-MPhB/g-C<sub>3</sub>N<sub>4</sub> (curves 4) and pure BiVO<sub>4</sub> (curves 5) at optical excitation wavelength 300 nm; inset: comparison of PL data in semi-logarithmic scale for better comparison of the results. (<b>c</b>) Cyclic voltammograms of FTO/BiVO<sub>4</sub> and FTO/BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> electrodes in the solution of 0.1 M Na<sub>2</sub>SO<sub>4</sub> in dark and under illumination with a diode 365 nm at illumination intensity 100 mW cm<sup>−2</sup>. (<b>d</b>) Comparison of IMPS spectra for BiVO<sub>4</sub>, BiVO<sub>4</sub>/Au (B/Au), BiVO<sub>4</sub>/g-C<sub>3</sub>N<sub>4</sub> (B/CN), BiVO<sub>4</sub>/fullerene/g-C<sub>3</sub>N<sub>4</sub> (B/Ful/CN), and BiVO<sub>4</sub>/Au/g-C<sub>3</sub>N<sub>4</sub> (B/Au/CN), obtained in aqueous solution of 0.1 M Na<sub>2</sub>SO<sub>4</sub> at the polarization potential 0.3 V vs. Ag/AgCl at the wavelength 370 nm (frequency range from 0.1 Hz to 1 kHz).</p>
Full article ">
12 pages, 2897 KiB  
Article
Highly Water-Dispersed Natural Fullerenes Coated with Pluronic Polymers as Novel Nanoantioxidants for Enhanced Antioxidant Activity
by Hyeryeon Oh, Jin Sil Lee, Panmo Son, Jooyoung Sim, Min Hee Park, Young Eun Bang, Daekyung Sung, Jong-Min Lim and Won Il Choi
Antioxidants 2024, 13(10), 1240; https://doi.org/10.3390/antiox13101240 - 15 Oct 2024
Viewed by 680
Abstract
Fullerene is a cosmic material with a buckyball-like structure comprising 60 carbon atoms. It has attracted significant interest because of its outstanding antioxidant, antiviral, and antibacterial properties. Natural fullerene (NC60) in shungite meets the demand of biomedical fields to scavenge reactive oxygen species [...] Read more.
Fullerene is a cosmic material with a buckyball-like structure comprising 60 carbon atoms. It has attracted significant interest because of its outstanding antioxidant, antiviral, and antibacterial properties. Natural fullerene (NC60) in shungite meets the demand of biomedical fields to scavenge reactive oxygen species in many diseases. However, its hydrophobicity and poor solubility in water hinder its use as an antioxidant. In this study, highly water-dispersed and stable Pluronic-coated natural fullerene nanoaggregates (NC60/Plu) were prepared from various Pluronic polymers. The water dispersity and stability of NC60 were compared and optimized based on the characteristics of Pluronic polymers including F68, F127, L35, P123, and L81. In particular, NC60 coated with Pluronic F127 at a weight ratio of 1 to 5 showed excellent antioxidant effects both in situ and in vitro. This suggests that the high solubilization of NC60 in Pluronic polymers increases its chance of interacting with reactive oxygen radicals and improves radical scavenging activity. Thus, the optimized NC60/PF127 may be a novel biocompatible antioxidant for treating various diseases associated with oxidative stress. Full article
(This article belongs to the Special Issue Nanoantioxidants―3rd Edition)
Show Figures

Figure 1

Figure 1
<p>Schematic of the preparation and antioxidant activity demonstration of water-dispersible natural fullerene nanoaggregates using Pluronic polymers (NC60/Plu).</p>
Full article ">Figure 2
<p>Characterization of natural fullerene (NC60) and Pluronic-coated NC60 nanoaggregates (NC60/Plu) with different hydrophile–lipophile balance values. (<b>A</b>) Photographs, (<b>B</b>) ultraviolet–visible (UV–Vis) absorption spectra, (<b>C</b>) hydrodynamic diameters, (<b>D</b>) polydispersity indexes (PDI), (<b>E</b>) zeta potentials of NC60 and NC60/Plu.</p>
Full article ">Figure 3
<p>Characterization of natural fullerene (NC60) and Pluronic F127-coated NC60 nanoaggregates (NC60/PF127) at different polymer weight ratios (NC60:PF127 = 1:0, 1:1, 1:5, 1:10, and 1:20). (<b>A</b>) Photographs, (<b>B</b>) UV–Vis absorption spectra, (<b>C</b>) hydrodynamic diameters, (<b>D</b>) polydispersity indexes (PDI), (<b>E</b>) zeta potentials of NC60 and NC60/PF127 at different polymer weight ratios.</p>
Full article ">Figure 4
<p>Stability analysis of natural fullerene (NC60) and Pluronic F127-coated NC60 nanoaggregates (NC60/PF127) at the polymer weight ratio of 1:5 in water at 25 °C. (<b>A</b>) Hydrodynamic diameters, (<b>B</b>) polydispersity indexes (PDIs), (<b>C</b>) photographs after 4 weeks of storage at 25 °C. ▲ denotes partial aggregation of the nanoaggregates. Characterization of NC60/PF127 after lyophilization (FD). (<b>D</b>) Photographs of powder (left) and aqueous dispersion of NC60/PF127 (right). (<b>E</b>) Hydrodynamic diameters and (<b>F</b>) PDIs of NC60/PF127 before and after FD.</p>
Full article ">Figure 5
<p>(<b>A</b>) In situ antioxidant activity of ascorbic acid (AA), fullerene (C60), natural fullerene (NC60), and Pluronic F127-coated NC60 nanoaggregates (NC60/PF127) via beta-carotene assay. In vitro cytotoxicity and antioxidant activity of Pluronic F127-coated NC60 (NC60/PF127) in CCK-8 and H<sub>2</sub>DCFDA assay. (<b>B</b>) Cell viability and (<b>C</b>) intracellular ROS level after treatment with NC60/PF127 (1:5). Negative control (Neg) and positive control (Pos) groups indicate the lowest and highest ROS levels, respectively (* <span class="html-italic">p</span> &lt; 0.05).</p>
Full article ">
13 pages, 4869 KiB  
Article
Dispersion of Hydrophilic Nanoparticles in Natural Rubber with Phospholipids
by Jiramate Kitjanon, Nililla Nisoh, Saree Phongphanphanee, Nattaporn Chattham, Mikko Karttunen and Jirasak Wong-ekkabut
Polymers 2024, 16(20), 2901; https://doi.org/10.3390/polym16202901 - 15 Oct 2024
Viewed by 634
Abstract
Coarse-grained molecular dynamics (CGMD) simulations were employed to investigate the effects of phospholipids on the aggregation of hydrophilic, modified carbon-nanoparticle fillers in cis-polyisoprene (cis-PI) composites. The MARTINI force field was applied to model dipalmitoylphosphatidylcholine (DPPC) lipids and hydrophilic modified fullerenes [...] Read more.
Coarse-grained molecular dynamics (CGMD) simulations were employed to investigate the effects of phospholipids on the aggregation of hydrophilic, modified carbon-nanoparticle fillers in cis-polyisoprene (cis-PI) composites. The MARTINI force field was applied to model dipalmitoylphosphatidylcholine (DPPC) lipids and hydrophilic modified fullerenes (HMFs). The simulations of DPPC in cis-PI composites show that the DPPC lipids self-assemble to form a reverse micelle in a rubber matrix. Moreover, HMF molecules readily aggregate into a cluster, in agreement with the previous studies. Interestingly, the mixture of the DPPC and HMF in the rubber matrix shows a cluster of HMF is encapsulated inside the DPPC reverse micelle. The HMF encapsulated micelles disperse well in the rubber matrix, and their sizes are dependent on the lipid concentration. Mechanical and thermal properties of the composites were analyzed by calculating the diffusion coefficients (D), bulk modulus (κ), and glass transition temperatures (Tg). The results suggest that DPPC acts as a plasticizer and enhances the flexibility of the HMF-DPPC rubber composites. These findings provide valuable insights into the design and process of high-performance rubber composites, offering improved mechanical and thermal properties for various applications. Full article
(This article belongs to the Collection Feature Papers in Polymer Processing and Engineering)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Mapping the atomistic model onto the CG model for <span class="html-italic">cis</span>-PI, DPPC, and HMF molecules: (<b>a</b>) DPPC model with CG bead type names Q0 (charged), Qa (charged), Na (nonpolar), and C1 (apolar) connected beads; (<b>b</b>) pristine fullerene and HMF with CG bead type names SQda (charged) interconnected beads; (<b>c</b>) rubber chain with atom type name C3 (apolar) connected to form a chain. Note that: the bead types Q0, Qa, Na, and C1 are adopted from the standard MARTINI force field [<a href="#B42-polymers-16-02901" class="html-bibr">42</a>].</p>
Full article ">Figure 2
<p>Snapshots of (<b>a</b>) DPPC-<span class="html-italic">cis</span>-PI composites and (<b>b</b>) HMF-<span class="html-italic">cis</span>-PI composites. Cyan chain: <span class="html-italic">cis</span>-PI chain, cyan cylinders: lipid tail, dark yellow: phosphate group, pink: glycerol backbone, blue: choline group, and orange: HMF.</p>
Full article ">Figure 3
<p>Snapshots of HMF-DPPC-<span class="html-italic">cis</span>-PI composites at DPPC concentrations of 5, 10, 20, and 30 phr. Cyan chain: <span class="html-italic">cis</span>-PI chain, cyan cylinders: lipid tail, dark yellow: phosphate group, pink: glycerol backbone, blue: choline group, and orange: HMF.</p>
Full article ">Figure 4
<p>The average cluster size of HMF within DPPC-<span class="html-italic">cis</span>-PI composites as a function of lipid concentration.</p>
Full article ">Figure 5
<p>(<b>a</b>) HMF-HMF radial distribution function (RDF) within the HMF-DPPC-<span class="html-italic">cis</span>-PI composites. (<b>b</b>) Snapshots of representative filler configurations corresponding to the specific numbers in figure (<b>a</b>). (<b>c</b>) Side view of Mackay’s icosahedron structure.</p>
Full article ">Figure 6
<p>(<b>a</b>) Diffusion coefficients of <span class="html-italic">cis</span>-PI (black line) and HMF (red line). (<b>b</b>) Bulk modulus of HMF-DPPC-<span class="html-italic">cis</span>-PI composites as a function of DPPC concentration.</p>
Full article ">Figure 7
<p>Glass transition temperature (<span class="html-italic">T<sub>g</sub></span>) of HMF-DPPC-<span class="html-italic">cis</span>-PI composites as a function of DPPC concentrations.</p>
Full article ">
10 pages, 1900 KiB  
Article
Photocatalytic Ammonia Decomposition Using Dye-Encapsulated Single-Walled Carbon Nanotubes
by Tomoyuki Tajima, Kotone Yano, Kazushi Mukai and Yutaka Takaguchi
Catalysts 2024, 14(10), 715; https://doi.org/10.3390/catal14100715 - 12 Oct 2024
Viewed by 576
Abstract
The photocatalytic decomposition of ammonia to produce N2 and H2 was achieved using single-walled carbon nanotube (SWCNT) nanohybrids. The physical modification of ferrocene-dye-encapsulated CNTs by amphiphilic C60-dendron yielded nanohybrids with a dye/CNT/C60 coaxial heterojunction. Upon irradiation with visible [...] Read more.
The photocatalytic decomposition of ammonia to produce N2 and H2 was achieved using single-walled carbon nanotube (SWCNT) nanohybrids. The physical modification of ferrocene-dye-encapsulated CNTs by amphiphilic C60-dendron yielded nanohybrids with a dye/CNT/C60 coaxial heterojunction. Upon irradiation with visible light, an aqueous solution of NH3 and dye@CNT/C60-dendron nanohybrids produced both N2 and H2 in a stoichiometric ratio of 1/3. The action spectra of this reaction clearly demonstrated that the encapsulated dye acted as the photosensitizer, exhibiting an apparent quantum yield (AQY) of 0.22% at 510 nm (the λmax of the dye). This study reports the first example of dye-sensitized ammonia decomposition and provides a new avenue for developing efficient and sustainable photocatalytic hydrogen production systems. Full article
(This article belongs to the Section Nanostructured Catalysts)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Fabrication process of <b>1</b>@CNT/C<sub>60</sub>-dendron photocatalyst. (<b>a</b>) Encapsulation of dye <b>1</b> into CNTs via solution process, producing <b>1</b>@CNT. (<b>b</b>) Physical modification of <b>1</b>@CNT with C<sub>60</sub>-dendron.</p>
Full article ">Figure 2
<p>(<b>a</b>) Photograph of a water dispersion of CNT/C<sub>60</sub>-dendron (<b>left</b>) and <b>1</b>@CNT/C<sub>60</sub>-dendron (<b>right</b>), (<b>b</b>) absorption spectra of dye <b>1</b>, CNT/C<sub>60</sub>-dendron, and <b>1</b>@CNT/C<sub>60</sub>-dendron in water.</p>
Full article ">Figure 3
<p>Time course of the H<sub>2</sub> (blue) and N<sub>2</sub> (red) evolution using <b>1</b>@CNT/C<sub>60</sub>-dendron photocatalyst under irradiation with visible light (300W-Xe; λ &gt; 422 nm, 3000 Wm<sup>2</sup>).</p>
Full article ">Figure 4
<p>UV–vis spectrum of <b>1</b> (solid line) and <b>1</b>@CNT (dotted line) in chloroform, as well as action spectra for the evolution of H<sub>2</sub> from H<sub>2</sub>O using <b>1</b>@CNT/C<sub>60</sub>-dendron.</p>
Full article ">Figure 5
<p>An energy-level diagram of the photocatalytic decomposition of NH<sub>3</sub> using <b>1</b>@SWCNT/C<sub>60</sub>-dendron to evolute H<sub>2</sub> and N<sub>2</sub>.</p>
Full article ">Figure 6
<p>Time course of the H<sub>2</sub> (blue) and N<sub>2</sub> (red) evolution using <b>1</b>@CNT/C<sub>60</sub>-dendron photocatalyst under irradiation with simulated sunlight (AM-1.5G; 1000 Wm<sup>2</sup>).</p>
Full article ">
13 pages, 2699 KiB  
Article
Insight into the Reversible Hydrogen Storage of Titanium-Decorated Boron-Doped C20 Fullerene: A Theoretical Prediction
by Zhiliang Chai, Lili Liu, Congcong Liang, Yan Liu and Qiang Wang
Molecules 2024, 29(19), 4728; https://doi.org/10.3390/molecules29194728 - 6 Oct 2024
Viewed by 794
Abstract
Hydrogen storage has been a bottleneck factor for the application of hydrogen energy. Hydrogen storage capacity for titanium-decorated boron-doped C20 fullerenes has been investigated using the density functional theory. Different boron-doped C20 fullerene absorbents are examined to avoid titanium atom clustering. [...] Read more.
Hydrogen storage has been a bottleneck factor for the application of hydrogen energy. Hydrogen storage capacity for titanium-decorated boron-doped C20 fullerenes has been investigated using the density functional theory. Different boron-doped C20 fullerene absorbents are examined to avoid titanium atom clustering. According to our research, with three carbon atoms in the pentagonal ring replaced by boron atoms, the binding interaction between the Ti atom and C20 fullerene is stronger than the cohesive energy of titanium. The calculated results revealed that one Ti atom can reversibly adsorb four H2 molecules with an average adsorption energy of −1.52 eV and an average desorption temperature of 522.5 K. The stability of the best absorbent structure with a gravimetric density of 4.68 wt% has been confirmed by ab initio molecular dynamics simulations. These findings suggest that titanium-decorated boron-doped C20 fullerenes could be considered as a potential candidate for hydrogen storage devices. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Top and side views of C<sub>20</sub>. (<b>b</b>) Top and side views of the adsorbent B123 model. (<b>c</b>) Binding energy of different amounts of boron doping, where brown, green and blue represent carbon, boron and titanium atoms respectively. (<b>d</b>) Changes in energy and bond length in the ab initio molecular dynamics simulation (300 K, 5 ps) of the B123 model.</p>
Full article ">Figure 2
<p>Hydrogen adsorption on the B123 model, where brown, green, blue and white represent carbon, boron, titanium and hydrogen atoms respectively.</p>
Full article ">Figure 3
<p>Desorption temperature as a function of pressure in the B123 model.</p>
Full article ">Figure 4
<p>(<b>a</b>) Relative energy as a function of temperature under a given pressure in the B123 model. (<b>b</b>) Relative energy as a function of pressure under a given temperature in the B123 model.</p>
Full article ">Figure 5
<p>Total density of states of C<sub>20</sub> fullerene and B123 model.</p>
Full article ">Figure 6
<p>Partial density of states for (<b>a</b>) C 2p orbital of C<sub>20</sub>; (<b>b</b>) C 2p orbital of B123; (<b>c</b>) B 2p orbital of isolated B; (<b>d</b>) Ti 3d orbital of isolated Ti; (<b>e</b>) B 2p orbital of B123; and (<b>f</b>) Ti 3d orbital of B123.</p>
Full article ">Figure 7
<p>Partial density of states for the (<b>a</b>) H 1s orbital of isolated H<sub>2</sub>; (<b>b</b>) H 1s orbital of C<sub>20</sub> fullerene + H<sub>2</sub>; (<b>c</b>) H 1s orbital of B123 + H<sub>2</sub>; (<b>d</b>) Ti 3d orbital of B123; and (<b>e</b>) Ti 3d orbital of B123 + H<sub>2</sub>. Fermi level is set to zero energy.</p>
Full article ">Figure 8
<p>Charge density difference for the (<b>a</b>) B123 system; (<b>b</b>) B123 + H<sub>2</sub> system. Yellow and blue colors represent charge-gained and charge-lost regions, respectively.</p>
Full article ">
14 pages, 3318 KiB  
Article
A Quantum Mechanical MP2 Study of the Electronic Effect of Nonplanarity on the Carbon Pyramidalization of Fullerene C60
by Yuemin Liu, Yunxiang Gao, Tariq Altalhi, Di-Jia Liu and Boris I. Yakobson
Nanomaterials 2024, 14(19), 1576; https://doi.org/10.3390/nano14191576 - 29 Sep 2024
Cited by 1 | Viewed by 684
Abstract
Among C60’s diverse functionalities, its potential application in CO2 sequestration has gained increasing interest. However, the processes involved are sensitive to the molecule’s electronic structure, aspects of which remain debated and require greater precision. To address this, we performed structural [...] Read more.
Among C60’s diverse functionalities, its potential application in CO2 sequestration has gained increasing interest. However, the processes involved are sensitive to the molecule’s electronic structure, aspects of which remain debated and require greater precision. To address this, we performed structural optimization of fullerene C60 using the QM MP2/6–31G* method. The nonplanarity of the optimized icosahedron is characterized by two types of dihedral angles: 138° and 143°. The 120 dihedrals of 138° occur between two hexagons intersecting at C–C bonds of 1.42 Å, while the 60 dihedrals of 143° are observed between hexagons and pentagons at C–C bonds of 1.47 Å. NBO analysis reveals less pyramidal sp1.78 hybridization for carbons at the 1.42 Å bonds and more pyramidal sp2.13 hybridization for the 1.47 Å bonds. Electrostatic potential charges range from −0.04 a.u. to 0.04 a.u. on the carbon atoms. Second-order perturbation analysis indicates that delocalization interactions in the C–C bonds of 1.42 Å (143.70 kcal/mol) and 1.47 Å (34.98 kcal/mol) are 22% and 38% higher, respectively, than those in benzene. MP2/Def2SVP calculations yield a correlation energy of 13.49 kcal/mol per electron for C60, slightly higher than the 11.68 kcal/mol for benzene. However, the results from HOMO-LUMO calculations should be interpreted with caution. This study may assist in the rational design of fullerene C60 derivatives for CO2 reduction systems. Full article
Show Figures

Figure 1

Figure 1
<p>Profiles of bond lengths and bond angles of C<sub>60</sub>. (<b>a</b>) Bond lengths of C<sub>60</sub>; (<b>b</b>) Bond angles of C<sub>60</sub>.</p>
Full article ">Figure 2
<p>Dihedral angle and ESP partial charge of C<sub>60</sub>. (<b>a</b>) Dihedral angles of C<sub>60</sub>; (<b>b</b>) ESP charges of fullerene C<sub>60</sub>.</p>
Full article ">Figure 3
<p>Structure of fullerene C<sub>60</sub>. (<b>a</b>) The hexagon and pentagon in CPK representation of fullerene C<sub>60</sub>; (<b>b</b>) The C1–C6 natural hybrid orbital (NHO) directionality described by a vector in a coordinating system. All figures are prepared using the visual molecular dynamics package [<a href="#B69-nanomaterials-14-01576" class="html-bibr">69</a>].</p>
Full article ">Figure 4
<p>(<b>a</b>) Natural bond orbital coefficients and hybrids of fullerene C<sub>60</sub>; (<b>b</b>) natural bond orbital coefficients and hybrids of benzene.</p>
Full article ">Figure 5
<p>(<b>a</b>) Natural bond orbital delocalization of fullerene C<sub>60</sub>; (<b>b</b>) natural bond orbital delocalization of benzene. The star indicates antibond, the arrow indicates bond–antibond interaction.</p>
Full article ">Figure 6
<p>Comparison of correlation energy per electron between fullerene C<sub>60</sub> and benzene.</p>
Full article ">Figure 7
<p>Energy level diagram of the L = 5 for fullerene C<sub>60</sub> based on the results computed using MP2 method.</p>
Full article ">
18 pages, 1287 KiB  
Article
Performance Assessment of Flat Plate Solar Collector Using Simple and Hybrid Carbon Nanofluids at Low Thermal Capacity
by José Michael Cruz, Sandra Angélica Crepaldi, Geydy Luz Gutiérrez-Urueta, José de Jesús Rubio, Alejandro Zacarías, Cuauhtémoc Jiménez, Guerlin Romage, José Alfredo Jiménez, Abel López and Ricardo Balcazar
Appl. Sci. 2024, 14(19), 8732; https://doi.org/10.3390/app14198732 - 27 Sep 2024
Viewed by 678
Abstract
Installation of flat solar collectors (FSCs) has been increasing due to the zero cost of renewable energy. However, the performance of this equipment is limited by the area, the material and the thermophysical properties of the working fluid. To improve the properties of [...] Read more.
Installation of flat solar collectors (FSCs) has been increasing due to the zero cost of renewable energy. However, the performance of this equipment is limited by the area, the material and the thermophysical properties of the working fluid. To improve the properties of the fluid, metal and metal oxide nanoparticles have mainly been used. This paper presents the performance assessment of the FSCs using simple and hybrid carbon nanofluids of low thermal capacity. Energy and mass balance modeling was performed for this study. A parametric analysis was conducted to examine the impact of key variables on the performance of the solar collectors using simple graphite and fullerene nanofluids, as well as hybrid metal–oxide–carbon nanofluids. From the results of heat transfer in FSCs, using graphite and fullerene nanofluids, it can be concluded that adding these nanoparticles improves the convection coefficient by 40% and 30%, respectively, with 10% nanoparticles. The graphite and fullerene nanoparticles can enhance the efficiency of FSCs by 2% and 1.5% more than base fluid. As the decrease in efficiency using fullerene with magnesium oxide is less than 0.2%, fullerene hybrid nanofluids could still be used in FSCs. Full article
(This article belongs to the Section Energy Science and Technology)
Show Figures

Figure 1

Figure 1
<p>Physical model of the system: (<b>a</b>) FSC system; (<b>b</b>) sectional view of FSC.</p>
Full article ">Figure 2
<p>Physical model of the system: (<b>a</b>) FSC cross-section view; (<b>b</b>) 3D thermodynamic system of FSC.</p>
Full article ">Figure 3
<p>Flowchart followed in the simulation.</p>
Full article ">Figure 4
<p>Useful heat and efficiency of the FSC with respect to the mass flow of the base fluid.</p>
Full article ">Figure 5
<p>Density, viscosity and specific heat capacity as a function of volume fraction for the graphite and fullerene nanofluids.</p>
Full article ">Figure 6
<p>(<b>a</b>) TC and (<b>b</b>) thermal diffusivity as a function of volume fraction for the graphite and fullerene nanofluids.</p>
Full article ">Figure 7
<p>The nanofluid’s (<b>a</b>) Reynolds and (<b>b</b>) Prandtl number with respect to volume fraction for graphite and fullerene nanofluids.</p>
Full article ">Figure 8
<p>Nusselt number and internal convection heat transfer coefficient with respect to volume fraction for graphite and fullerene nanofluids.</p>
Full article ">Figure 9
<p>Useful heat with respect to the volume fraction for metal oxide and carbon nanofluids.</p>
Full article ">Figure 10
<p>Efficiency with respect to the volume fraction for metal oxide and carbon nanofluids.</p>
Full article ">Figure 11
<p>Useful heat of hybrid carbon nanofluids with respect to volume fraction.</p>
Full article ">Figure 12
<p>Efficiency of hybrid carbon nanofluids with respect to volume fraction.</p>
Full article ">
12 pages, 843 KiB  
Article
Advances of the Holographic Technique to Test the Basic Properties of the Thin-Film Organics: Refractivity Change and Novel Mechanism of the Nonlinear Attenuation Prediction
by Natalia Kamanina
Polymers 2024, 16(18), 2645; https://doi.org/10.3390/polym16182645 - 19 Sep 2024
Viewed by 568
Abstract
A large number of the thin-film organic structures (polyimides, 2-cyclooctylarnino-5-nitropyridine, N-(4-nitrophenyl)-(L)-prolinol, 2-(n-Prolinol)-5-nitropyridine) sensitized with the different types of the nano-objects (fullerenes, carbon nanotubes, quantum dots, shungites, reduced graphene oxides) are presented, which are studied using the holographic technique under the Raman–Nath diffraction conditions. [...] Read more.
A large number of the thin-film organic structures (polyimides, 2-cyclooctylarnino-5-nitropyridine, N-(4-nitrophenyl)-(L)-prolinol, 2-(n-Prolinol)-5-nitropyridine) sensitized with the different types of the nano-objects (fullerenes, carbon nanotubes, quantum dots, shungites, reduced graphene oxides) are presented, which are studied using the holographic technique under the Raman–Nath diffraction conditions. Pulsed laser irradiation testing of these materials predicts a dramatic increase of the laser-induced refractive index, which is in several orders of the magnitude greater compared to pure materials. The estimated nonlinear refraction coefficients and the cubic nonlinearities for the materials studied are close to or larger than those known for volumetric inorganic crystals. The role of the intermolecular charge transfer complex formation is considered as the essential in the refractivity increase in nano-objects-doped organics. As a new idea, the shift of charge from the intramolecular donor fragment to the intermolecular acceptors can be proposed as the development of Janus particles. The energy losses via diffraction are considered as an additional mechanism to explain the nonlinear attenuation of the laser beam. Full article
(This article belongs to the Special Issue Advanced Polymer Nanocomposites III)
Show Figures

Figure 1

Figure 1
<p>The proposed extended scheme of intermolecular charge transfer using organic conjugated materials, where the introduced intermolecular doping nano-object has an electron affinity significantly greater than the intramolecular acceptor of the matrix system.</p>
Full article ">
16 pages, 3519 KiB  
Article
From 2D to 3D In Vitro World: Sonodynamically-Induced Prooxidant Proapoptotic Effects of C60-Berberine Nanocomplex on Cancer Cells
by Aleksandar Radivoievych, Sophia Schnepel, Svitlana Prylutska, Uwe Ritter, Oliver Zolk, Marcus Frohme and Anna Grebinyk
Cancers 2024, 16(18), 3184; https://doi.org/10.3390/cancers16183184 - 18 Sep 2024
Viewed by 688
Abstract
Objectives: The primary objective of this research targeted the biochemical effects of SDT on human cervix carcinoma (HeLa) and mouse Lewis lung carcinoma (LLC) cells grown in 2D monolayer and 3D spheroid cell culture. Methods: HeLa and LLC monolayers and spheroids were treated [...] Read more.
Objectives: The primary objective of this research targeted the biochemical effects of SDT on human cervix carcinoma (HeLa) and mouse Lewis lung carcinoma (LLC) cells grown in 2D monolayer and 3D spheroid cell culture. Methods: HeLa and LLC monolayers and spheroids were treated with a 20 µM C60-Ber for 24 h, followed by irradiation with 1 MHz, 1 W/cm2 US. To evaluate the efficacy of the proposed treatment on cancer cells, assessments of cell viability, caspase 3/7 activity, ATP levels, and ROS levels were conducted. Results: Our results revealed that US irradiation alone had negligible effects on LLC and HeLa cancer cells. However, both monolayers and spheroids irradiated with US in the presence of the C60-Ber exhibited a significant decrease in viability (32% and 37%) and ATP levels (42% and 64%), along with a notable increase in ROS levels (398% and 396%) and caspase 3/7 activity (437% and 246%), for HeLa monolayers and spheroids, respectively. Similar tendencies were observed with LLC cells. In addition, the anticancer effects of C60-Ber surpassed those of C60, Ber, or their mixture (C60 + Ber) in both cell lines. Conclusions: The detected intensified ROS generation and ATP level drop point to mitochondria dysfunction, while increased caspase 3/7 activity points on the apoptotic pathway induction. The combination of 1 W/cm2 US with C60-Ber showcased a promising platform for synergistic sonodynamic chemotherapy for cancer treatment. Full article
(This article belongs to the Special Issue Old Drugs in a New Package: Future of Cancer Nanomedicine)
Show Figures

Figure 1

Figure 1
<p>Combination of sonodynamic therapy and chemotherapy with a C<sub>60</sub>-Ber nanocomplex: cell exposure to high-frequency US (1); acoustic cavitation (2); C<sub>60</sub> excitation with sonoluminescence (3); ROS generation by excited C<sub>60</sub> (4); apoptotic death caused by generated ROS and co-delivered Ber (5).</p>
Full article ">Figure 2
<p>Diagram of the ultrasound exposure set-up for cells cultured in 2D (<b>a</b>) and 3D (<b>b</b>) conditions.</p>
Full article ">Figure 3
<p>Viability of LLC (<b>a</b>) and HeLa (<b>b</b>) cell monolayers (2D) and spheroids (3D) incubated in the presence of 20 µM C<sub>60</sub>-Ber nanocomplex (C<sub>60</sub>-Ber) or mixture of 20 µM C<sub>60</sub> and 20 µM Ber (C<sub>60</sub> + Ber) and treated with 1 MHz ultrasound (US); * <span class="html-italic">p</span> ≤ 0.01 in comparison with the viability of cells treated with the respective duration of US.</p>
Full article ">Figure 4
<p>Phase contrast microscopy images of monolayers (2D) and spheroids (3D) of LLC and HeLa cells incubated in the presence of 20 µM C<sub>60</sub>-Ber nanocomplex and irradiated with 60 s 1 MHz 1 W/cm<sup>2</sup> ultrasound (US) in the “transducer in well” set-up; scale bar is 100 µm.</p>
Full article ">Figure 5
<p>ROS level of LLC (<b>a</b>) and HeLa (<b>b</b>) cell monolayers (2D) and spheroids (3D) incubated in the presence of 20 µM C<sub>60</sub>-Ber nanocomplex (C<sub>60</sub>-Ber) or mixture of 20 µM C<sub>60</sub> and 20 µM Ber (C<sub>60</sub> + Ber) and treated with 1 MHz ultrasound (US); * <span class="html-italic">p</span> ≤ 0.01 in comparison with the ROS level of cells treated with the respective duration of US.</p>
Full article ">Figure 6
<p>ATP level of LLC (<b>a</b>) and HeLa (<b>b</b>) cell monolayers (2D) and spheroids (3D) incubated in the presence of 20 µM C<sub>60</sub>-Ber nanocomplex (C<sub>60</sub>-Ber) or mixture of 20 µM C<sub>60</sub> and 20 µM Ber (C<sub>60</sub> + Ber) and treated with 1 MHz ultrasound (US); * <span class="html-italic">p</span> ≤ 0.01 in comparison with the ATP level of cells treated with the respective duration of US.</p>
Full article ">Figure 7
<p>Caspase 3/7 activity of LLC (<b>a</b>) and HeLa (<b>b</b>) cell monolayers (2D) and spheroids (3D) incubated in the presence of 20 µM C<sub>60</sub>-Ber nanocomplex (C<sub>60</sub>-Ber) or mixture of 20 µM C<sub>60</sub> and 20 µM Ber (C<sub>60</sub> + Ber) and treated with 1 MHz ultrasound (US); * <span class="html-italic">p</span> ≤ 0.01 in comparison with the caspase 3/7 activity of cells treated with the respective duration of US.</p>
Full article ">Figure A1
<p>Cell viability (<b>a</b>,<b>b</b>), ATP level (<b>c</b>,<b>d</b>), ROS level (<b>e</b>,<b>f</b>) and caspase 3/7 (<b>g</b>,<b>h</b>) activity of LLC and HeLa spheroids, incubated in the presence of 20 µM C<sub>60</sub> and 20 µM Ber separately and treated with 1 MHz 1 W/cm<sup>2</sup> US. * <span class="html-italic">p</span> ≤ 0.01 in comparison with controls, treated with the respective duration of US.</p>
Full article ">
47 pages, 6874 KiB  
Review
Nanoalchemy: Unveiling the Power of Carbon Nanostructures and Carbon–Metal Nanocomposites in Synthesis and Photocatalytic Activity
by Yalini Devi Neelan, Senthil Bakthavatchalam, Shanmugam Mahalingam, Krishnasamy Sreenivason Yoganand, Shunmuga Vadivu Ramalingam, Umamaheswari Rajendran, Rajasekaran Ramu, Tae-Youl Yang, Junghwan Kim and Raji Atchudan
Catalysts 2024, 14(9), 618; https://doi.org/10.3390/catal14090618 - 13 Sep 2024
Viewed by 1053
Abstract
Due to a rise in industrial pollutants in modern life, the climate and energy crisis have grown more widespread. One of the best ways to deal with dye degradation, hydrogen production, and carbon dioxide reduction issues is the photocatalytic technique. Among various methods, [...] Read more.
Due to a rise in industrial pollutants in modern life, the climate and energy crisis have grown more widespread. One of the best ways to deal with dye degradation, hydrogen production, and carbon dioxide reduction issues is the photocatalytic technique. Among various methods, catalytic technology has demonstrated tremendous promise in recent years as a cheap, sustainable, and environmentally benign technology. The expeditious establishment of carbon-based metal nanoparticles as catalysts in the disciplines of materials and chemical engineering for catalytic applications triggered by visible light is largely attributed to their advancement. There have been many wonderful catalysts created, but there are still many obstacles to overcome, which include the cost of catalysts being reduced and their effectiveness being increased. Carbon-based materials exhibit a unique combination of characteristics that make them ideal catalysts for various reaction types. These characteristics include an exceptional electrical conductivity, well-defined structures at the nanoscale, inherent water repellency, and the ability to tailor surface properties for specific applications. This versatility allows them to be effective in diverse catalytic processes, encompassing organic transformations and photocatalysis. The emergence of carbon-based nanostructured materials, including fullerenes, carbon dots, carbon nanotubes, graphitic carbon nitride, and graphene, presents a promising alternative to conventional catalysts. This review focuses on the diverse functionalities of these materials within the realm of catalysis materials for degradation, hydrogen production, and carbon dioxide reduction. Additionally, it explores the potential for their commercialization, delving into the underlying mechanisms and key factors that influence their performance. It is anticipated that this review will spur more research to develop high-performance carbon-based materials for environmental applications. Full article
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Illustrating the various features of photocatalysts.</p>
Full article ">Figure 2
<p>Illustrates the various roles of the carbon material in photocatalysts.</p>
Full article ">Figure 3
<p>Schematic representation of various forms of carbon.</p>
Full article ">Figure 4
<p>The image illustrates the different properties of carbon.</p>
Full article ">Figure 5
<p>The soccer-ball-like form of the carbon-60 Bucky ball [<a href="#B29-catalysts-14-00618" class="html-bibr">29</a>].</p>
Full article ">Figure 6
<p>Various shapes of carbon nanotubes, such as (<b>a</b>) structures of SCNT and CNT and (<b>b</b>) geometrical structures of SCNT and CNT [<a href="#B40-catalysts-14-00618" class="html-bibr">40</a>].</p>
Full article ">Figure 7
<p>Illustrates the classification of carbon dots [<a href="#B46-catalysts-14-00618" class="html-bibr">46</a>].</p>
Full article ">Figure 8
<p>Various synthesis techniques used in top-down approaches.</p>
Full article ">Figure 9
<p>Different synthesis methods for bottom-up approaches.</p>
Full article ">Figure 10
<p>Different approaches for improving photocatalyst performance.</p>
Full article ">Figure 11
<p>Schematic design of the photodegradation mechanism [<a href="#B116-catalysts-14-00618" class="html-bibr">116</a>].</p>
Full article ">Figure 12
<p>Schematic illustration for the mechanism of hydrogen production.</p>
Full article ">Figure 13
<p>Schematic illustration for the mechanism of carbon dioxide reduction.</p>
Full article ">
Back to TopTop