共查询到20条相似文献,搜索用时 0 毫秒
1.
E. A. Katz D. Faiman S. Goren S. Shtutina B. Mishori Yoram Shapira 《Fullerenes, Nanotubes and Carbon Nanostructures》1998,6(1):103-111
A heterojunction was prepared by depositing a thin film of C60 on a p-Si substrate. Photovoltaic properties were observed using a UV-filtered solar simulator and natural sun light. Surface Photovoltage Spectroscopy was employed to distinguish between the nature of photoconversion in the C60 and Si layers. 相似文献
2.
基于p+-Si与n-ZnO纳米线的p-n异质结的制备及其性质研究 总被引:1,自引:0,他引:1
利用CVD蒸汽俘获法,在p^+硅片上制备了垂直生长的n型ZnO纳米线阵列,用XRD和SEM分析了样品的结构与形貌。测试发现样品的I-V曲线符合典型的p-n异质结特性,正向开启电压为0.5V,反向饱和电流为0.02mA。计算了异质结的理想因子η,发现当异质结两端偏压在0V-0.3V的低压区域,理想因子为1.85,而在0.3v-0.8v的高偏压区域,理想因子为8.36。解释了理想因子偏高的原因是由于金属一半导体接触以及ZnO纳米线与p^+-si界而存在缺陷。 相似文献
3.
It is investigated theoretically why alkali-metal-doped C60, AxC60, is a nonmagnetic semiconductor for x=2 and 4. We find that this is the consequence of the intramolecular negative- U effect due to the strong electron-phonon interaction and the weak Hund coupling between conduction electrons. 相似文献
4.
5.
6.
Au电极作用下C60、2C60与4C60富勒烯分子的电子传输特性 总被引:2,自引:0,他引:2
采用扩展的Hückel方法与格林函数方法,研究了Au电极作用下,C60富勒烯、2C60和4C60聚合体分子的电子结构与导电性,并对它们的电子结构与电子输运特性进行了对比.研究结果表明,C60、2C60或4C60富勒烯分子与Au电极 "接触"后,其HOMO、LUMO间的能隙减小;C60、2C60或4C60分子与Au电极之间的结合既有共价键的成分,又有离子键的成分,其中,C60、4C60分子与Au电极结合的离子键特征更为明显;三种富勒烯分子的电子输运性能依次具有C60>2C60>4C60分子的顺序. 相似文献
7.
8.
9.
It is well established that for an alkali-doped C60 sample to be superconducting, the oxidation state C
3–
60 must be satisfied. It has been found previously that T
c is proportional to crystal parameter a in a face-centered cubic (fcc) structure. It is thus desirable to intercalate the largest possible size of molecule that can contribute one electron into every interstitial space. The successful process of such doping depends on our understanding the interaction among the dopants and C60. We introduce a fabrication scheme of three steps successive doping using alkali (A) and halogen (H) elements along this line. While A
3C60 is superconducting, A
3–x
(AH)
x
C60 was found to be non-superconducting in the second step and the sample became superconducting again after doping with A, leading to stoichiometric ratio of A
3–x
(AH)
x
A
x
C60. We present an explanation based on interaction among dopants and C60 and analyze the process of ionization of dopants, which is consistent with our experimental finding reported here. 相似文献
10.
Dieter Heymann 《Fullerenes, Nanotubes and Carbon Nanostructures》2004,12(4):715-729
This paper presents a literature review of studies of ozonides and oxides of C60 and C70. 相似文献
11.
Tomoyasu Nakamine Shugo Suzuki Kenji Nakao Makoto Okazaki 《Fullerenes, Nanotubes and Carbon Nanostructures》1995,3(4):389-398
respectively. 相似文献
12.
13.
K. K. Singh T. Pradeep D. E. Morris L. Chen J. V. Acrivos 《Fullerenes, Nanotubes and Carbon Nanostructures》2013,21(3):583-598
Abstract The electron spin resonance (esr) of C60.Ox and C60.HMTTEF (hexamethylentetratellurafulvalene) has been investigated at 9.36 GHz as a function of temperature. T (298 T 4 K). C60.Ox shows an esr absorption of equal ‘g’ value to that of C60 exposed to O2 and light but is more intense. The C60 in its pure form is in a singlet state. The impurity sites introduced by O2 produce the esr absorption. The Curie - Weiss plots of inverse esr absorption intensity versus temperature indicate an antiferromagnetic TH = 50 for air exposed C60 and 90K for C60Ox. From the esr intensity at room temperature, the calculated number of free spins (S = 1/2) is =1/3 per mole of C60-Ox. In case of C60.HMTTEF, there is a very weak esr absorption at room temperature suggesting that the room temperature form is diamagnetic with very small charge transfer between C60 and HMTTEF. This conclusion is consistent with the structure and magnetic susceptibility of this cocrystal. As the temperature is lowered, the equilibrium: AD <=> A?? + D?+ is displaced towards the formation of free radical species, A?? and D?+. 相似文献
14.
《Fullerenes, Nanotubes and Carbon Nanostructures》2013,21(3):245-255
Abstract Several dimers: C120, C140, C130 and their oxygen‐containing derivatives as well as some oligomers or polymers of the well known spherical fullerenes have been synthesized so far. Some of the formulas attributed to such compounds represent the first steps in a more complex fate leading to trivalent capped tubulenes. Such a way could even be followed by functionalized fullerenes. A detailed network transformation is given for C60 and its mono‐ and di‐epoxy derivatives. Semiempirical calculations support the presented findings. 相似文献
15.
All the published data on the solubility of C60 in 140 organic and inorganic solvents are summarized and the critical features of the experimental techniques are treated. Data on die temperature dependence of solubility are also listed and analyzed. Experimental evidences on the molecular state of dissolved C60 as well as the interactions between the solute and solvents are discussed. 相似文献
16.
Mircea V. Diudea Csaba L. Nagy Oleg Ursu Teodor Silviu Balaban 《Fullerenes, Nanotubes and Carbon Nanostructures》2003,11(3):245-255
Several dimers: C120, C140, C130 and their oxygen-containing derivatives as well as some oligomers or polymers of the well known spherical fullerenes have been synthesized so far. Some of the formulas attributed to such compounds represent the first steps in a more complex fate leading to trivalent capped tubulenes. Such a way could even be followed by functionalized fullerenes. A detailed network transformation is given for C60 and its mono- and di-epoxy derivatives. Semiempirical calculations support the presented findings. 相似文献
17.
采用Tersoff-Brenner势与L—J势的分子动力学方法,研究了双石墨层作用下C32、C60、C180以及C60@C180富勒烯分子的压缩力学特性。根据计算结果,讨论了几种富勒烯压缩过程中的变形、能量、压缩栽荷等的变化及其差异。研究表明,由于分子几何构形上的差异,压缩时,C180出现了明显的“塌陷”现象,“塌陷”过程中,能量及外载荷一度下降;几种富勒烯压缩时的能量吸收能力排序为:C32〉C60〉C60@C180〉C180,承载能力的排序为:C60@C180〉C180〉C60〉C32。 相似文献
18.
Burhanettin i ek Adnan Kenar Hasan Nazir 《Fullerenes, Nanotubes and Carbon Nanostructures》2001,9(1):103-111
In all fullerene-producing systems, reaction products were black soot extracts reported to contain a 5-25% fullerene mixture. Toluene extraction of the soot results in a solution of C60, C70, and higherc fullerenes. Without separation, absolute determination of the contents is not possible, leaving the researcher to comment only on the C60/C70 ratio of the solution. High-performance liquid chromatography, nuclear magnetic resonance, and scanning tunneling microscopy imaging techniques were reported in the literature for determining the C60/C70 ratio of the mixtures. These methods require tedious experiments and produce slightly differing results as well. In this communication, a new and relatively quick method is proposed for the simultaneous determination of the yields of C60 and C70 (not the ratio) in fullerene-containing solutions by ultraviolet-visible spectrophotometric analysis. 相似文献
19.
C. Sekar C. R. V. Rao C. Subramanian P. Ramasamy 《Fullerenes, Nanotubes and Carbon Nanostructures》1995,3(3):343-358
Good quality C60 crystals have been grown from high purity C60 powder and fullerene mixture (C60/C70) by vacuum sublimation method. The grown crystals were characterized with Optical microscopy, SEM, powder XRD, High Performance Liquid Chromatography and Raman spectroscopic analyses. 相似文献
20.
Abstract The effects of mechanical grinding on polycrystalline C60 and Ca5C60 superconductor are examined. It has been found that mechanical grinding may severely degrade phases of C60 (fcc) and Ca5C60 (sc). The grinding destroys the long-range ordering of crystals and produces a partial amorphous state. The damage of crystal leads to the disappearance of superconductivity for Ca5C60. The samples with an amorphous phase can be recrystallized by annealing at 600°C for pure C60 and Ca5C60. Magnetic susceptibility measurements indicated that the superconductivity of the degraded sample did not recover easily to the initial state. 相似文献