C. Chien, Chau‐Fong Chen, S. Hsu, L. Chiang, M. Lai
Apoptosis induced by oxidative stress, especially reactive oxygen species, resulting from ischemia/reperfusion would lead to organ dysfunction. C60(glucosamine)6, a water-soluble fullerene with strong free radical scavenging activity, was applied to evaluate its effect on renal ischemia/reperfusion-induced apoptosis formation and superoxide generation. C60(glucosamine)6 pretreatment, but not posttreatment, significantly reduced renal ischemia/reperfusion-induced apoptosis and superoxide generation and, consequently, ameliorated renal hemodynamic effects. Up-regulation in bcl-2 and bcl-xL of the rat kidney was evident in C60(glucosamine)6 pretreated, posttreated, and nontreated groups. However, exaggerated forced expression of bcl-2 and bcl-xL was found in the C60(glucosamine)6 pretreated group. Our results conclude that forced expression of bcl-2 and bcl-xL by the novel water-soluble fullerene, C60(glucosamine)6, can reduce renal ischemia/ reperfusion-induced oxidative stress.
{"title":"FORCED EXPRESSION OF BCL-2 AND BCL-xL BY NOVEL WATER-SOLUBLE FULLERENE, C60(GLUCOSAMINE)6, REDUCES RENAL ISCHEMIA/REPERFUSION-INDUCED OXIDATIVE STRESS","authors":"C. Chien, Chau‐Fong Chen, S. Hsu, L. Chiang, M. Lai","doi":"10.1081/FST-100000167","DOIUrl":"https://doi.org/10.1081/FST-100000167","url":null,"abstract":"Apoptosis induced by oxidative stress, especially reactive oxygen species, resulting from ischemia/reperfusion would lead to organ dysfunction. C60(glucosamine)6, a water-soluble fullerene with strong free radical scavenging activity, was applied to evaluate its effect on renal ischemia/reperfusion-induced apoptosis formation and superoxide generation. C60(glucosamine)6 pretreatment, but not posttreatment, significantly reduced renal ischemia/reperfusion-induced apoptosis and superoxide generation and, consequently, ameliorated renal hemodynamic effects. Up-regulation in bcl-2 and bcl-xL of the rat kidney was evident in C60(glucosamine)6 pretreated, posttreated, and nontreated groups. However, exaggerated forced expression of bcl-2 and bcl-xL was found in the C60(glucosamine)6 pretreated group. Our results conclude that forced expression of bcl-2 and bcl-xL by the novel water-soluble fullerene, C60(glucosamine)6, can reduce renal ischemia/ reperfusion-induced oxidative stress.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"123 1","pages":"77 - 88"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"86576334","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
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.
{"title":"SIMULTANEOUS DETERMINATION OF C60 AND C70 FULLERENES BY A SPECTROPHOTOMETRIC METHOD","authors":"B. Çiçek, A. Kenar, H. Nazır","doi":"10.1081/FST-100000169","DOIUrl":"https://doi.org/10.1081/FST-100000169","url":null,"abstract":"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.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"48 1","pages":"103 - 111"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"86013422","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Yu. K. Golicov, L. N. Gall’, Z. Z. Latypov, N. Gall’
The quasiclassical approach has been used to calculate a fullerene and an endofullerene molecular interaction with electric fields. A physical model for an endofullerene molecular polarizability in electric fields has been developed and equations describing the interaction have been deduced.
{"title":"ENDOFULLERENE POLARIZATION AND DYNAMICS IN ELECTRIC FIELD: THE QUASICLASSIC APPROACH","authors":"Yu. K. Golicov, L. N. Gall’, Z. Z. Latypov, N. Gall’","doi":"10.1081/FST-100000159","DOIUrl":"https://doi.org/10.1081/FST-100000159","url":null,"abstract":"The quasiclassical approach has been used to calculate a fullerene and an endofullerene molecular interaction with electric fields. A physical model for an endofullerene molecular polarizability in electric fields has been developed and equations describing the interaction have been deduced.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"22 1","pages":"1 - 8"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"87487697","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The free radical scavenging property of fullerenes and their derivatives is demonstrated by a facile color reaction of C60 with the 1,1-diphenyl-2-picryl hydrazyl radical. A rapid test by simply monitoring the reaction using ultraviolet-visible spectroscopy is suggested.
{"title":"RAPID ASSESSMENT OF THE FREE RADICAL SCAVENGING PROPERTY OF FULLERENES","authors":"K. Geckeler, S. Samal","doi":"10.1081/FST-100000161","DOIUrl":"https://doi.org/10.1081/FST-100000161","url":null,"abstract":"The free radical scavenging property of fullerenes and their derivatives is demonstrated by a facile color reaction of C60 with the 1,1-diphenyl-2-picryl hydrazyl radical. A rapid test by simply monitoring the reaction using ultraviolet-visible spectroscopy is suggested.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"1 1","pages":"17 - 23"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"80798516","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Although there exists no general agreement on mechanistic pathways for fullerene formation, there are some reasonable schemes in the literature explaining most of the features. However, as far as the existing production processes and the final yields are concerned, not the formation but rather chemical stabilization of the relatively hot products was more influence on the final production yield. A continuous helium jet was blown into the reactive zone by a quartz microprobe located 20 mm away from the arc to enhance rapid removal of the products from the high temperature zone. Decreased residence times appear to improve production efficiency.
{"title":"EFFECT OF RESIDENCE TIME ON FULLERENE YIELD","authors":"B. Çiçek","doi":"10.1081/FST-100000165","DOIUrl":"https://doi.org/10.1081/FST-100000165","url":null,"abstract":"Although there exists no general agreement on mechanistic pathways for fullerene formation, there are some reasonable schemes in the literature explaining most of the features. However, as far as the existing production processes and the final yields are concerned, not the formation but rather chemical stabilization of the relatively hot products was more influence on the final production yield. A continuous helium jet was blown into the reactive zone by a quartz microprobe located 20 mm away from the arc to enhance rapid removal of the products from the high temperature zone. Decreased residence times appear to improve production efficiency.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"27 1","pages":"63 - 69"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82635741","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The thermal stability of the C60 photopolymer, the C60 ozo-polymer, and photochlorinated C60 was studied by thermogravimetric analysis (TGA) ultraviolet-visible (UV-vis) and TGA-differential thermal analysis techniques up to 950°C in comparison to graphite and pure C60. The ozopolymer was found to be the least stable material followed by C60Cl x . The resulting residual carbonaceous matter formed by the decomposition of the photopolymer and the ozopolymer has been studied by Fourier transform-infrared (FTIR) spectroscopy and has been found to be completely comparable to carbon black. The thermal decomposition of the C60 photopolymer prepared in solution yields negligible amounts of C60. The main product is carbon black.
{"title":"A STUDY ON THE THERMAL STABILITY OF THE PHOTOPOLYMER, THE OZOPOLYMER, AND THE PHOTOCHLORINATED DERIVATIVE OF C60 FULLERENE","authors":"F. Cataldo","doi":"10.1081/FST-100000164","DOIUrl":"https://doi.org/10.1081/FST-100000164","url":null,"abstract":"The thermal stability of the C60 photopolymer, the C60 ozo-polymer, and photochlorinated C60 was studied by thermogravimetric analysis (TGA) ultraviolet-visible (UV-vis) and TGA-differential thermal analysis techniques up to 950°C in comparison to graphite and pure C60. The ozopolymer was found to be the least stable material followed by C60Cl x . The resulting residual carbonaceous matter formed by the decomposition of the photopolymer and the ozopolymer has been studied by Fourier transform-infrared (FTIR) spectroscopy and has been found to be completely comparable to carbon black. The thermal decomposition of the C60 photopolymer prepared in solution yields negligible amounts of C60. The main product is carbon black.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"47 1","pages":"55 - 61"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"83266795","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this paper, we report the study of the production of MoTe2 (molybdenum ditelluride) samples after a high dose of electron irradition. A 2 MeV Van de Graaff accelerator was used to irradiate the sample at the following conditions: 1.3 MeV voltage, 5 μA current, 25 kGy/min dose rate, and 1000 kGy total dosage. These conditions are maintain fixed while the irradiation dosages were changed to 50, 100, 200, and 500 Mrad. The optimization of the dosage used for the production of MoTe2 nanotubes was obtained from the analysis of the samples that were examined in a high-resolution transmission electron microscope. The most efficient production of MoTe2 nanotubes was obtained at the range between 100 and 200 Mrad. A very typical characteristic was obtained for rotated structures with angles of 4, 5, 7, 8, and 12° observed in the diffraction pattern for MoTe2.
本文报道了高剂量电子辐照制备二碲化钼样品的研究。采用2 MeV Van de Graaff加速器，在1.3 MeV电压、5 μA电流、25 kGy/min剂量率、1000 kGy总剂量下辐照样品。当辐照剂量改变为50、100、200和500毫摩尔时，这些条件保持不变。通过高分辨率透射电子显微镜对样品进行分析，获得了用于生产MoTe2纳米管的最佳用量。MoTe2纳米管的最有效生产在100和200 Mrad之间。在MoTe2衍射图中观察到的角度为4、5、7、8和12°的旋转结构具有非常典型的特征。
{"title":"OPTIMIZATION OF THE ELECTRON IRRADIATION IN THE PRODUCTION OF MoTe2 NANOTUBES","authors":"E. Flores, A. Tlahuice, E. Adem, D. Galván","doi":"10.1081/FST-100000160","DOIUrl":"https://doi.org/10.1081/FST-100000160","url":null,"abstract":"In this paper, we report the study of the production of MoTe2 (molybdenum ditelluride) samples after a high dose of electron irradition. A 2 MeV Van de Graaff accelerator was used to irradiate the sample at the following conditions: 1.3 MeV voltage, 5 μA current, 25 kGy/min dose rate, and 1000 kGy total dosage. These conditions are maintain fixed while the irradiation dosages were changed to 50, 100, 200, and 500 Mrad. The optimization of the dosage used for the production of MoTe2 nanotubes was obtained from the analysis of the samples that were examined in a high-resolution transmission electron microscope. The most efficient production of MoTe2 nanotubes was obtained at the range between 100 and 200 Mrad. A very typical characteristic was obtained for rotated structures with angles of 4, 5, 7, 8, and 12° observed in the diffraction pattern for MoTe2.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"21 1","pages":"16 - 9"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"84659961","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Optical absorption studies on aqueous solutions of C60(C4H8SO3Na) n (n = 4–6) revealed deviation from the Beer-Lambert law in the 250–350 nm region, which is assigned to the formation of solute aggregates at concentrations higher than 1 × 10−3 mol dm−3. Dynamic light scattering experiments showed aggregates with an average size of ∼100 nm. The solute has a broad weak fluorescence emission (ϕf = 1.8 × 10−3) in the 450–650 nm region, which remained independent of solute concentration. The broad transient absorption band in the 450–900 nm region (ϵ660 = 2170 dm3 mol−1 cm−1), which formed immediately on laser flash photolysis (λex = 355 nm, 35 ps), is assigned to singlet-singlet transition. It decays to a triplet excited state whose absorption is observed to depend strongly on solute concentration. In dilute solutions, an absorption band with λmax = 590 nm is seen, and at high solute concentration a broad absorption in the 500–900 nm region is observed. The eaq − reacts with the solute with a bimolecular rate constant of 1.7 × 108 dm3 mol−1 s−1 and forms weak broad absorption bands at 440, 540, 620, 870, 940, and 1020 nm. Isopropanol radicals also react with the solute with a bimolecular rate constant of 2.3 × 108 dm3 mol−1 s−1 with the formation of a transient optical absorption spectrum similar to that observed on reaction with eaq − and assigned to a solute radical anion. The •H and −OH radicals react with bimolecular rate constants of 3.2 × 109 and 4.4 × 109 dm3 mol−1 s−1, respectively, and form transient absorption bands at 440, 510, and 660 nm. Based on electron transfer studies with suitable electron donor/acceptor substrates, the ranges of the reduction and oxidation potentials of the solute an estimated.
{"title":"RADIATION CHEMICAL AND PHOTOPHYSICAL PROPERTIES OF C60(C4H8SO3Na) n IN AQUEOUS SOLUTION: A LASER FLASH PHOTOLYSIS AND PULSE RADIOLYSIS STUDY","authors":"H. Mohan, D. Palit, L. Chiang, J. Mittal","doi":"10.1081/FST-100000163","DOIUrl":"https://doi.org/10.1081/FST-100000163","url":null,"abstract":"Optical absorption studies on aqueous solutions of C60(C4H8SO3Na) n (n = 4–6) revealed deviation from the Beer-Lambert law in the 250–350 nm region, which is assigned to the formation of solute aggregates at concentrations higher than 1 × 10−3 mol dm−3. Dynamic light scattering experiments showed aggregates with an average size of ∼100 nm. The solute has a broad weak fluorescence emission (ϕf = 1.8 × 10−3) in the 450–650 nm region, which remained independent of solute concentration. The broad transient absorption band in the 450–900 nm region (ϵ660 = 2170 dm3 mol−1 cm−1), which formed immediately on laser flash photolysis (λex = 355 nm, 35 ps), is assigned to singlet-singlet transition. It decays to a triplet excited state whose absorption is observed to depend strongly on solute concentration. In dilute solutions, an absorption band with λmax = 590 nm is seen, and at high solute concentration a broad absorption in the 500–900 nm region is observed. The eaq − reacts with the solute with a bimolecular rate constant of 1.7 × 108 dm3 mol−1 s−1 and forms weak broad absorption bands at 440, 540, 620, 870, 940, and 1020 nm. Isopropanol radicals also react with the solute with a bimolecular rate constant of 2.3 × 108 dm3 mol−1 s−1 with the formation of a transient optical absorption spectrum similar to that observed on reaction with eaq − and assigned to a solute radical anion. The •H and −OH radicals react with bimolecular rate constants of 3.2 × 109 and 4.4 × 109 dm3 mol−1 s−1, respectively, and form transient absorption bands at 440, 510, and 660 nm. Based on electron transfer studies with suitable electron donor/acceptor substrates, the ranges of the reduction and oxidation potentials of the solute an estimated.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"8 1","pages":"37 - 53"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75000079","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
E. B. Stukalin, N. V. Avramenko, M. Korobov, R. Ruoff
Differential scanning calorimetry, X-ray, and solubility measurements were used to study phase equilibria in the ternary system C60-C70-1,2-dimethylbenzene up to the boiling point of the solvent. Formation of the two ternary phases was confirmed. Partial solubilities of C60 and C70 were measured and calculated.
{"title":"TERNARY SYSTEM OF C60 AND C70 WITH 1,2-DIMETHYLBENZENE","authors":"E. B. Stukalin, N. V. Avramenko, M. Korobov, R. Ruoff","doi":"10.1081/FST-100000170","DOIUrl":"https://doi.org/10.1081/FST-100000170","url":null,"abstract":"Differential scanning calorimetry, X-ray, and solubility measurements were used to study phase equilibria in the ternary system C60-C70-1,2-dimethylbenzene up to the boiling point of the solvent. Formation of the two ternary phases was confirmed. Partial solubilities of C60 and C70 were measured and calculated.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"33 1","pages":"113 - 130"},"PeriodicalIF":0.0,"publicationDate":"2001-02-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"85813473","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2000-11-01DOI: 10.1080/10641220009351440
Z. Slanina
The contributed volume of fourteen chapters is opened by a remark from one of the editors K. Fukui (1918-1998). The Nobel laureate of 1981 calls nanotubes and fullerenes 'splendid gift' and points out that such developments of mesoscopic scale suggest the possibility to realize the 'Schrodinger-cat states'. The following three chapters treat various essential aspects of carbon nanotubes. M. Yumura deals with synthesis and purification of nanotubes. Their electron diffraction and microscopy is described by S. Amelinckx e t al. The third chapter in this block, written by T. Hanada e t al., discusses electron energy loss spectroscopy as a tool for nanotube structural studies. The group of the next five chapters is devoted to more specific aspects of nanotube structure and behavior. Electronic structure of single-walled nanotubes is analyzed in a theoretical chapter by K. Tanaka e t al. The following chapter from R. Saito et al. deals with phonon structure and Raman effect of single-walled nanotubes. Contribution from H. Ajiki and T. Ando describes behavior of single-walled nanotubes in magnetic fields. M.
{"title":"The Science and Technology of Carbon Nanotubes K. Tanaka, T. Yamabe, K. Fukui, Eds.: Elsevier Science, Amsterdam, 1999","authors":"Z. Slanina","doi":"10.1080/10641220009351440","DOIUrl":"https://doi.org/10.1080/10641220009351440","url":null,"abstract":"The contributed volume of fourteen chapters is opened by a remark from one of the editors K. Fukui (1918-1998). The Nobel laureate of 1981 calls nanotubes and fullerenes 'splendid gift' and points out that such developments of mesoscopic scale suggest the possibility to realize the 'Schrodinger-cat states'. The following three chapters treat various essential aspects of carbon nanotubes. M. Yumura deals with synthesis and purification of nanotubes. Their electron diffraction and microscopy is described by S. Amelinckx e t al. The third chapter in this block, written by T. Hanada e t al., discusses electron energy loss spectroscopy as a tool for nanotube structural studies. The group of the next five chapters is devoted to more specific aspects of nanotube structure and behavior. Electronic structure of single-walled nanotubes is analyzed in a theoretical chapter by K. Tanaka e t al. The following chapter from R. Saito et al. deals with phonon structure and Raman effect of single-walled nanotubes. Contribution from H. Ajiki and T. Ando describes behavior of single-walled nanotubes in magnetic fields. M.","PeriodicalId":12470,"journal":{"name":"Fullerene Science and Technology","volume":"48 1","pages":"639 - 640"},"PeriodicalIF":0.0,"publicationDate":"2000-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79761089","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
京公网安备 11010802042870号
京ICP备2023020795号-1
扫码关注我们
求助内容：
应助结果提醒方式：