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In the alkali-metal doped C60, the charge transfer induces the distortion of the bond structure and forms the self-trapping electronic bound states. Our theory manifests: 1, the charge transfer reduces the symmetry of C60 from Ih to D5d. 2, Both the bond distortion and the self-trapping states possess layer structures and are localized in the equatorial area. 3, The carbon atoms in charged C60 are divided into eight layers with an inversion center, then there exist four nonequivalent groups of carbon atoms. It makes the NMR line split into a fine structure with strength ratio 1:1:2:2. 4, The charged C60 has two self-trapping bound states, one is 0.06eV above HOMO with odd parity and the other is 0.05 eV below LUMO with even parity. 相似文献
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用气相法生长出了毫米尺寸的具有规则晶面和金属光泽的高质量的纯C60单晶.X射线衍射分析表明,C60单晶在室温下具有面心立方(fcc)结构,晶格常数为α=1.4199(4)nm。用扫描电子显微镜和光学显微镜观察了C60单晶的形貌,除观察到fcc结构的晶体所特有的{111}和{200}两种稳定晶面以及非常容易形成的孪晶之外,还发现了在{111}面上的树枝状、垄状和生长丘以及在{200}面上的树枝状、游泳池状和生长丘的生长缺陷。对C60
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本文在独立电子近似的基础上,根据多重散射自洽场理论方法,计算了C2和C2+,C2-分子(离子)的电子结构,阐明了势形共振能量和上述分子(离子)电子数的关系,结果表明,随着电子数的减少,C原子2s-2p轨道杂化减弱,势形共振的能量将降低(如降低到阈值下,则势形共振消失)。
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在200 keV重离子加速器上,用120—360 keV的H,N,Ar和Mo离子注入C60薄膜.对注入后薄膜的拉曼谱进行了分析.结果表明,不同离子注入C60薄膜后,C60的1469 cm-1特征峰随注入剂量的增加均呈指数式下降,同时在1300—1700 cm-1范围出现非晶碳峰,并逐渐增强,最终完全非晶化.而且1469 cm-1拉曼峰的强度及C60薄膜完全非晶化所对应的剂量与注入离子的种类和能量有关.进一步的分析表明,C60分子的损伤主要是由注入离子的核能量转移所造成,与电子能量转移无关.H离子注入C60薄膜后,1469 cm-1处特征拉曼峰向短波方向非对称展宽,这可能是注入的H离子通过电子能量转移使C60分子发生聚合的结果.
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A possible superconducting mechanism of the hole-doped C60 solid is discussed. Under the assumption that the superconductivity results from the strong coupling between electrons at Fermi surface and intramolecular vibrations, a simple expression for the electron-phonon coupling parameter λ is derived. The related transition temperature is estimated and can be much greater than that of the alkali-metal-doped C60 solid. 相似文献
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The electronic structure and vibrational spectrum of the C60 film condensed on a 2H- MoS2(0001) surface have been investigated by X-ray photoelectron spectroscopy (XPS), ul-traviolet photoelectron spectroscopy (UPS), Auger electron spectroscopy (AES) and infrared high-resolution electron-energy-loss spectroscopy (HREELS). AES analysis showed that at low energy side of the main transition, C60 contains a total of three peaks just like that of graphite. However, the energy position of the KLL main Auger transition of C60 looks like that of diamond, indicating that the hybridization of the carbon atoms in C60 is not strictly in sp2- bonded state but that the curvature of the molecular surface introduces some sp2pz- bonded character into the molecular orbitals. XPS showed that the C 1s binding energy in C60 was 285.0eV, and its main line was very symmetric and offered no indication of more than a single carbon species. In UPS measurement the valence band spectrum of C60 within 10eV below the Fermi level (EF) shows a very distinct five-band structure that character-izes the electronic structure of the C60 molecule. HREEL results showed that the spectrum obtained from the C60 film has very rich vibrational structure. At least, four distinct main loss peaks can be identified below 200 meV. The most intense loss was recorded at 66 meV, and relatively less intense losses were recorded at 95, 164 and 197meV at a primary energy of electron beam EP = 2.0eV. The other energy-loss peaks at 46, 136, 157 and 186meV in HREEL spectrum are rather weak. These results have been compared to infrared spectrum data of the crystalline solid C60 taken from recent literatures. 相似文献
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本文是文献[1—3]工作的继续,在前面工作中发展的方法被推广到讨论半无限n-s多层膜结构的电子态,构造这种系统的步骤如下:首先把一完整无限的晶体沿两个分开的原子平面切割开得一晶体薄膜,它可以是正常金属也可以是超导体;然后把薄膜A和B通过金属型接触形成一混合单元O;最后沿垂直于界面方向依次排上单元O构成一半无限多层膜结构,我们导出了上述每一步所对应的单位子格林函数,对两种不同正常金属组成的多层膜结构,给出了单粒子状态密度和能带的数值计算结果,当两种正常金属相同时,所得的公式结果与文献[7]等价,进而,对薄膜
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