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Theoretical Study of Structures and Chemical Functionalization of Endohedral Metallofullerenes
https://ir.soken.ac.jp/records/247
https://ir.soken.ac.jp/records/2476801c167-a231-4c6d-81a2-7d3972cea900
名前 / ファイル | ライセンス | アクション |
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要旨・審査要旨 (309.3 kB)
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Item type | 学位論文 / Thesis or Dissertation(1) | |||||
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公開日 | 2010-02-22 | |||||
タイトル | ||||||
タイトル | Theoretical Study of Structures and Chemical Functionalization of Endohedral Metallofullerenes | |||||
タイトル | ||||||
タイトル | Theoretical Study of Structures and Chemical Functionalization of Endohedral Metallofullerenes | |||||
言語 | en | |||||
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言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_46ec | |||||
資源タイプ | thesis | |||||
著者名 |
溝呂木, 直美
× 溝呂木, 直美 |
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フリガナ |
ミゾロギ, ナオミ
× ミゾロギ, ナオミ |
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著者 |
MIZOROGI, Naomi
× MIZOROGI, Naomi |
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学位授与機関 | ||||||
学位授与機関名 | 総合研究大学院大学 | |||||
学位名 | ||||||
学位名 | 博士(理学) | |||||
学位記番号 | ||||||
内容記述タイプ | Other | |||||
内容記述 | 総研大甲第1025号 | |||||
研究科 | ||||||
値 | 物理科学研究科 | |||||
専攻 | ||||||
値 | 07 構造分子科学専攻 | |||||
学位授与年月日 | ||||||
学位授与年月日 | 2007-03-23 | |||||
学位授与年度 | ||||||
値 | 2006 | |||||
要旨 | ||||||
内容記述タイプ | Other | |||||
内容記述 | Endohedral metallofullerenes (fullerenes encapsulating metal atoms inside the hollow spherical cages)have long attracted wide interest because of the promising material, catalytic, and biomedical applications. The electronic properties and reactivities of endohedral metallofullerenes have been extensively investigated both theoretically and experimentally. It is currently the focus of interest to determine the cage structures and metalpositions, since these are fundamental in the investigation and application of endohedral metallofullerenes.<br /> In this thesis, she has disclosed (1) the cage structures of the representative trimetallofullerene Sc<small>3</small> C<small>82</small> and dimetallofullerene Sc<small>2</small>C<small>84</small>, (2) the metal positions for Ce@C<small>82</small>, Eu@C<small>82</small>, Eu@C<small>82</small> and Gd@C<small>82</small>, (3) how the encapsulation of La<small>2</small> and Sc<small>3</small>N indside C<small>80</small> tunes the reactivities of the C<small>80</small> cage, and (4) how the rotationalmotion of La<small>2</small> and Sc<small>3</small>N inside C<small>80</small> in controllable by exohedral chemical functionalization, by using densityfunctional calculations in collaboration with experiment.<br /> (1) It is widely accepted that the maximum entropy method (MEM)/Rietveld analysis of synchrotron X-ray powder diffraction data is powerful for structural determination of endohedral metallofullerenes. Since the first application to Y@C<small>82</small>, the structured of many representative metallofullerenes have been determined and reported by the MEM/Rietveld method. For example, the MEM/Rietveld analysis of Sc<small>3</small>C<small>82</small> shows that three Sc atoms are encapsulated inside a <i>C</i><small>3v</small> isomer of C<small>82</small> as a trimer. However, this Sc<small>3</small>@C<small>82</small> structure does not correspond to an energy minimum. From density functional calculrations and <sup>13</sup>C NMR data, it has been disclosed that the cage structure of Sc<small>3</small>C<small>82</small> originates from the <i>I</i><small>h</small> isomer of C<small>80</small> (not from the <i>C</i><small>3</small>v isomer of C<small>82</small>)and two C atoms as well as three Sc atoms are encaged inside the C<small>80</small> fullerene, the Sc<small>3</small>C<small>2</small>@C<Small>80</small> structure being much more stable than the Sc<small>3</small>@C<small>82</small> structure determined by the MEM/Rietveld analysis. This noticeable finding has been corroborated by the single-crystal X-ray diffraction analysis of a carbine derivative of Sc<small>3</small>C<small>2</small>@C<small>80</small>. The carbide metallofullerene, Sc<small>3</small>C<small>2</small>@C<small>80</small>, is noteworthy since the number of encapsulated atomsis the largest known up to now. As another interesting example, it has been disclosed that Sc<small>2</small>C<small>84</small> takes the from of Sc<small>2</small>C<small>2</small>@C<small>82</small>, though Sc<small>2</small>C<small>84</small> has been believed to have the form of Sc<small>2</small>@C<small>84</small> from the MEM/Rietveld analysis. These results suggest that the structures of endohedral metallofullerenes determined by the MEM/Rietveld analysis are not always reliable enough, though the determined structures have been widely employed to explain the electronic properties and reactivities as well as spectroscopic data.<br /> (2)Since the first successful extraction of La@C<small>82</small>(M=Sc, Y, and La ) has been known as atypical monometallofullerene. The M atom is mostly encapsulated inside the <i>C</i><small>2v</small> cage of C <small>82</small> and located at an off-centered position near a hexagonal ring along the <i>C</i><small>2</small> axis. From the MEM/Rietveld analysis, however, it has been very recently claimed that Eu@C<small>82</small> and Gd@C<small>82</small> have exceptionally an anomalous endohedral structure since the metal atom having <i>f</i> electrons is located near the C-C double bond on the opposite side of the C<small>2v</small>-C<small>82</small> cage along the C<small>2</small> axis. To provide theoretical insight to this exception, density functional calculations were performed for Eu@C<small>82</small> and Gd@C<small>82</small> as well as Ce@C<small>82</small>. For all these metallofullerenes, it was found that the metal positions near the C-C double bond on the opposite side are highly unstable and do not correspond to energy minima, as also supported from the analysis of electrostatic potentials. The Eu, Gd, and Ce atoms move without any barrier to the positions near the hexagonal ring. The metal positions near the hexagonal ring are 30,52, and 50 kcal/mol more stable for Eu@C<small>82</small>, Gd@C<small>82</small>, and Ce@C<small>82</small>, respectively, than those near the C-Cdouble bond. These results suggest that Eu@C<small>82</small>, Gd@C<small>82</small>, and Ce@C<small>82</small> have a normal endohedral structure, as found for M@C<small>82</small>(M=Sc, Y, and La). In collaboration with experiment, the normal structure of Ce@C<small>82</small>has been verified from the paramagnetic NMR spectral analysis of the anion.<br /> (3)Both La<small>2</small>@C<small>80</small> and Sc<small>3</small>N@C<small>80</small> have the same carbon cage that originates from the <i>I</i><small>h</small> isomer of C<small>80</small> andthe electronic structures are formally described as (La<small>2</small>)<sup>6+</sup>C<small>80</small><sup>6-</sup> and (Sc<small>3</small>N)<sup>6+</sup>C<small>80</small><sup>6-</sup> as a result of six-electron transfer to the C<small>80</small> cage. However, Sc<small>3</small>.However, Sc<small>3</small>N@C<small>80</small> has a much higher LUMO level than La<small>2</small>@C<small>80</small>. The LUMO of Sc<small>3</small>N@C<small>80</small> is delocalized not only on the Sc<small>3</small>N cation but also on the C<small>80</small> anion, while the LUMO of La<small>2</small>@C<small>80</small> islocalized on the La cation and more suitable as an electron accommodation. These suggest that La<small>2</small>@C<small>80</small> is more reactive toward nucleophiles than Sc<small>3</small>N@C<small>80</small>. In fact, the different reactivities of La<small>2</small>@C<small>80</small> and Sc<small>3</small>N@C<small>80</small> have been verified for the reactions with disilirane. As this example shows, it is interesting that the reactivities of metallofullerenes are tunable by encapsulated species.<br /> (4) For La<small>2</small>@C<small>80</small> and Sc<small>3</small>N@C<small>80</small>, it is known that the two La atoms and the Sc<small>3</small>N cluster rotate freely inside the round <i>I</i><small>h</small>-C<small>80</small> cage at room temperature. By density functional calculations, however, it was found that the two La atoms stand still at a specific position upon the exohedral chemical functionalization of La<small>2</small>@C<small>80</small> by azomethine ylides, while the three-dimensional random motion of the Sc<small>3</small>N cluster in Sc<small>3</small>N@C<small>80</small> is fixied in the plane perpendicular to the equator by attaching electron-donating molecules such as disilirane. These theoretical findings have been recently confirmed by experiment. Control of motion of encapsulated species within a hollow cage is expected to be helpful in designing molecular devices with electronic or magnetic properties. | |||||
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