The Recent State of Endohedral Fullerene Research
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Photoionization of the Cerium Isonuclear Sequence and Cerium Endohedral Fullerene
University of Nevada, Reno Photoionization of the Cerium Isonuclear Sequence and Cerium Endohedral Fullerene A dissertation submitted in partial ful¯llment of the requirements for the degree of Doctor of Philosophy in Physics by Mustapha Habibi Prof. Ronald A. Phaneuf/Dissertation Advisor May, 2009 THE GRADUATE SCHOOL We recommend that the dissertation prepared under our supervision by MUSTAPHA HABIBI entitled Photoionization Of The Cerium Isonuclear Sequence And Cerium Endohedral Fullerene be accepted in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Ronald A. Phaneuf, Ph. D., Advisor Jeffrey S. Thompson, Ph. D., Committee Member Peter Winkler, Ph. D., Committee Member Paul Neill, Ph. D., Committee Member Mohammed S. Fadali, Ph. D., Graduate School Representative Marsha H. Read, Ph. D., Associate Dean, Graduate School May, 2009 To the souls of my mother and my father, to my beloved wife and daughters, to all my family, friends and colleagues for their love and unconditional support. i Abstract This dissertation presents an experimental photoionization study of the cerium isonuclear sequence ions in the energy range of the 4d inner-shell giant resonance. In addition, single and double photoionization and photofragmentation cross sections of the cerium endohe- + dral ion Ce@C82 were also measured and studied in the 4d excitation-ionization energy range of cerium. Relative and absolute cross-section measurements were performed at un- dulator beamline 10.0.1 of the Advanced Light Source (ALS) for nine parent cerium ions: Ce+ { Ce9+. Double-to-single ionization cross-section ratios were measured for photoion- + + ization of the endohedral Ce@C82 and empty fullerene C82 molecular ions. -
Synthesis and Characterization of Non-IPR Monometallic Actinide
Article Cite This: J. Am. Chem. Soc. XXXX, XXX, XXX−XXX pubs.acs.org/JACS Synthesis and Characterization of Non-Isolated-Pentagon-Rule C ‑ Actinide Endohedral Metallofullerenes U@ 1(17418) C76, C ‑ C ‑ U@ 1(28324) C80, and Th@ 1(28324) C80: Low-Symmetry Cage Selection Directed by a Tetravalent Ion † § ⊥ ‡ ⊥ † ⊥ † ∥ † Wenting Cai, , , Laura Abella, , Jiaxin Zhuang, , Xingxing Zhang, Lai Feng, Yaofeng Wang, ‡ § # § Roser Morales-Martínez, Ronda Esper, Mauro Boero, Alejandro Metta-Magaña, ‡ ‡ § † Antonio Rodríguez-Fortea, Josep M. Poblet,*, Luis Echegoyen,*, and Ning Chen*, † Laboratory of Advanced Optoelectronic Materials, College of Chemistry, Chemical Engineering and Materials Science, Soochow University, Suzhou, Jiangsu 215123, PR China ‡ Departament de Química Física i Inorganica,̀ Universitat Rovira i Virgili, c/Marcel·lí Domingo 1, 43007 Tarragona, Spain § Department of Chemistry, University of Texas at El Paso, 500 W University Avenue, El Paso, Texas 79968, United States # University of Strasbourg, CNRS, Institut de Physique et Chimie des Materiaux́ de Strasbourg UMR 7504, 23 rue du Loess, F-67034 Strasbourg, France ∥ Soochow Institute for Energy and Materials InnovationS (SIEMIS), College of Physics, Optoelectronics and Energy & Collaborative, Soochow University, Suzhou, Jiangsu 215006, PR China *S Supporting Information ABSTRACT: For the first time, actinide endohedral metal- lofullerenes (EMFs) with non-isolated-pentagon-rule (non-IPR) carbon cages, U@C80,Th@C80,andU@C76, have been successfully synthesized and fully characterized by mass spectrometry, single crystal X-ray diffractometry, UV−vis−NIR and Raman spectroscopy, and cyclic voltammetry. Crystallo- graphic analysis revealed that the U@C80 and Th@C80 share the same non-IPR cage of C1(28324)-C80, and U@C76 was assigned to non-IPR U@C1(17418)-C76. -
1. INTRODUCTION Geometric Structure
1. INTRODUCTION Clusters, in general, are aggregates of atoms that are too large compared to atoms and molecules and too small compared to small pieces of crystals (bulk materials). Generally, clusters does not have the same structure or atomic arrangements as a bulk solid and can change its structure with the addition of just one or few atoms. As the number of atoms in the cluster increase, the bulk structure is established and the addition of atoms has no more effect on the structure. Of course there will be some rearrangement of the atoms on the surface of this bulk structure, but since the surface to volume ratio is very low in bulk material it can be neglected with a good approximation. However, in case of clusters, most of the atoms lie on the surface (extremely high surface to volume ratio) and such rearrangement produce a drastic effect. Owning to their high surface to volume ratio, the surface science from both chemical and physical point of view has become crucial in order to collect data and information about such systems. The ways to study such small cluster is nearly the same as the way they have been fabricated. With Bottom-up approach (chemical point of view) these clusters are formed from atoms and/or molecules by assembling it together to form the cluster, and there were many calculation based on this view point. Also these clusters can be fabricated, starting from the bulk material by reducing its dimension somehow, which is the Top-down approach. Geometric structure Usually the crystal structure of a large nanocluster is the same as the bulk structure of the material, with somewhat different lattice parameters (in general clusters are slightly contracted as compared to bulk). -
Structure of Endohedral Fullerene Eu@C74 W
View Online / Journal Homepage / Table of Contents for this issue PAPER www.rsc.org/pccp | Physical Chemistry Chemical Physics Structure of endohedral fullerene Eu@C74w Dmitrij Rappoport* and Filipp Furche Received 2nd February 2009, Accepted 12th May 2009 First published as an Advance Article on the web 10th June 2009 DOI: 10.1039/b902098e Structure determination of endohedral fullerenes in the absence of X-ray data is difficult and often controversial. Here we show that the structure of endohedral fullerene Eu@C74 may be determined by density functional theory aided interpretation of its electronic, infrared and Raman spectra. The use of recently developed analytical polarizability gradient methods to simulate resonance-enhanced Raman spectra is crucial for this approach and allows for a nearly complete assignment of the experimental spectra. Eu@C74 is assigned a pear-shaped C2v symmetric structure and shows strong ionic interaction between the encapsulated metal and the fullerene p system. 1. Introduction spectrum of Eu@C74 to predictions from time-dependent density functional theory (TDDFT) to identify the frontier Endohedral metallofullerenes constitute a large class of molecular orbitals, specifically the electronic configuration of fullerene inner complexes with metal atoms or small metal europium. The structure of the carbon cage is inferred from an clusters.1,2 Group 2 and 3 metals and lanthanides form a assignment of infrared and Raman spectra of Eu@C74. number of endohedral fullerene complexes notable for their An important tool in the structure elucidation of endohedral electronic absorption in the near infrared and for their large fullerenes is 13C nuclear magnetic resonance (NMR) spectro- 1–3 third-order nonlinear susceptibilities. -
Crystalline C60 Fulleride with Metal Inside
Crystalline C60 fulleride with metal inside Ayano Nakagawa1, Makiko Nishino1, Hiroyuki Niwa1, Katsuma Ishino1, Zhiyong Wang1, Haruka Omachi1, Ko Furukawa2, Takahisa Yamaguchi3, Tatsuhisa Kato3, Shunji Bandow4, Jeremy Rio5, Chris Ewels5, Shinobu Aoyagi6 & Hisanori Shinohara1* 1Department of Chemistry and Institute for Advanced Research, Nagoya University, Nagoya 464-8602, Japan. 2Center for Coordination of Research Facilities, Institute for Research Promotion, Niigata University, Niigata 950-2181, Japan. 3Graduate School of Human and Environmental Sciences, Kyoto University, Sakyo-ku, Kyoto 606- 8501, Japan. 4Faculty of Science and Technology, Department of Applied Chemistry, Meijo University, Nagoya 468-8502, Japan. 5Institut des Materiaux Jean Rouxel (IMN), Université de Nantes, CNRS UMR6502, BP3229, 44322 Nantes, France 6Department of Information and Basic Science, Nagoya City University, Nagoya 467-8501, Japan. Endohedral metallofullerenes have been extensively studied, since the first experimental observation of La@C60 in a laser-vaporized supersonic beam in 1985. However, all of these studies have been carried out on metallofullerenes larger than C60 such as (metal)@C82, and there + - are no reported purified C60-based metallofullerenes except for [Li@C60] (SbCl6) salt. Pure (metal)@C60 has not been obtained because of their extremely high chemical reactivity. We report here the first isolation, structural determination and electromagnetic properties of crystalline C60- based metallofullerenes, Gd@C60(CF3)5 and La@C60(CF3)5. Synchrotron X-ray single-crystal diffraction reveals that La and Gd atoms are indeed encapsulated in the Ih-C60 fullerene. The HOMO-LUMO gaps of Gd@C60 and La@C60 are significantly widened by an order of magnitude with addition of CF3- groups. Magnetic measurements show the presense of a weak antiferromagnetic coupling in Gd@C60(CF3)3 crystals at low temperatures. -
Endohedral Fullerenes: the Importance of Electronic, Size and Shape Complementarity Between the Carbon Cages and the Corresponding Encapsulated Clusters† Maira R
Research Article Received: 6 September 2013, Revised: 24 September 2013, Accepted: 6 October 2013, Published online in Wiley Online Library: 9 January 2014 (wileyonlinelibrary.com) DOI: 10.1002/poc.3245 Endohedral fullerenes: the importance of electronic, size and shape complementarity between the carbon cages and the corresponding encapsulated clusters† Maira R. Ceróna, Fang-Fang Lia and Luis A. Echegoyena* Cage-cluster complementarity is of crucial importance in determining the sizes and structures, as well as the properties of endohedral fullerenes. The encapsulated atoms or clusters, which are typically in a positively charged state, are irreversibly, mechanically, and electrostatically trapped inside the typically negatively charged cages. These rather exotic compounds exhibit exquisitely complementary properties between their components. Here, we present a short overview to show that size and shape are crucial in determining the specific structures that are formed, and the presence of electrostatic interactions result in structural motifs that are never observed for pristine fullerene cages. Copyright © 2014 John Wiley & Sons, Ltd. Keywords: electronic properties; endohedral fullerenes; fullerene and cluster cage sizes; fullerene and cluster shapes INTRODUCTION understand the most important factors involved in determining the specific structures that are observed and their relative importance. The discovery and increased interest and to some degree, fascina- tion of trapping and studying atoms and clusters inside the carbon cages -
Actinide-Based Endohedral Metallofullerenes
Actinide-Based Endohedral Metallofullerenes Bailey Bouley Literature Seminar November 14th, 2019 In 1985, Smalley, Curl, and Kroto synthesized a new allotrope of carbon, C60, by laser vaporization methods under a helium atmosphere.1 The discovery of the structure that formed, deemed buckminsterfullerene by the authors, along with the discovery of fullerenes of other sizes with Cn configurations, won them the Nobel Prize in Chemistry in 1996. Two weeks after their discovery, the same authors published the first example of a metal ion encapsulated within the cavity of a fullerene, La-Cn (n = 44 – 76), where the lower carbon count Cn configurations appeared to exhibit an increase in stability with the metal ion inclusion.2 This discovery sparked interest in chemical research focused on using these so-named endohedral metallofullerenes (EMFs) as a new approach to the construction of superconductors (for alkali metal EMFs),3 and as isolated environments to study fundamental principles of poorly understood f-block elements. The first actinide-containing EMF was discovered in 1992, when the authors hypothesized an appropriately sized tetravalent ion would be able to stabilize C28, a fullerene that had been previously detected by TOF-MS, but not isolated due to poor stability.4 The low stability of this cluster was attributed to the presence of highly reactive sites centralized on fused pentagon rings, systems that violated the isolated pentagon rule (IPR), which states that fullerenes containing fused 5 pentagon rings are destabilized due to high geometric strain. It was believed, and subsequently supported by DFT calculations, that non-IPR cages can be stabilized through an ionic model in which electrons are transferred from the metal atom to the cage itself, localizing negative charge on the reactive carbon center, resulting in stabilization of these sites.6,7 Figure 1. -
Nanotechnology - Fundamentals and Applications 1
D. Cremer, CHEM 6342, Nanotechnology - Fundamentals and Applications 1 CHEM 6342 Nanotechnology – Fundamentals and Applications Class location: TBD Lectures, time and location: TBD Lab times and location: TBD Instructor: Dieter Cremer, 325 FOSC, ext 8-1300, [email protected] http://smu.edu/catco/ Office Hours: By appointment Units: 3 Grading: ABC Letter Grade Class number TBD 1. Rationale: Nanotechnology (NT) is a rather young discipline, which came up in the nineties. Nevertheless, NT has gained so much importance within the last years that universities at all rankings have introduced or are going to introduce NT teaching programs. Predictions say that NT will change our lives and society more than computer technology and electricity have done together. The course will provide an overview over NT. It will show that the nano regime is so different from other regimes because both classical and quantum effects can be active thus leading to unique properties of nano devices. NT is a highly interdisciplinary science, which will be reflected in the course by making reference to chemistry, physics, biology, pharmacy, and engineering. Applications of NT, as they are already in use today or as they are planned for the future, will be discussed. 2. Course Recommendations: The course is designed to reach all graduate students who had have an education in chemistry, physics, engineering or biology. It does not require special knowledge in mathematics or theoretical physics. The course contents will be presented in self-sustained modules, which make it possible to follow the course without special knowledge. The course will prepare for the interdisciplinary work in NT. -
Transformation of Doped Graphite Into Cluster- Encapsulated Fullerene Cages
ARTICLE DOI: 10.1038/s41467-017-01295-9 OPEN Transformation of doped graphite into cluster- encapsulated fullerene cages Marc Mulet-Gas1, Laura Abella2, Maira R. Cerón 3, Edison Castro 3, Alan G. Marshall1,4, Antonio Rodríguez-Fortea 2, Luis Echegoyen3, Josep M. Poblet 2 & Paul W. Dunk 1 An ultimate goal in carbon nanoscience is to decipher formation mechanisms of highly ordered systems. Here, we disclose chemical processes that result in formation of high- 1234567890 symmetry clusterfullerenes, which attract interest for use in applications that span biome- dicine to molecular electronics. The conversion of doped graphite into a C80 cage is shown to occur through bottom-up self-assembly reactions. Unlike conventional forms of fullerene, the iconic Buckminsterfullerene cage, Ih-C60, is entirely avoided in the bottom-up formation mechanism to afford synthesis of group 3-based metallic nitride clusterfullerenes. The effects of structural motifs and cluster–cage interactions on formation of compounds in the solvent- extractable C70–C100 region are determined by in situ studies of defined clusterfullerenes under typical synthetic conditions. This work establishes the molecular origin and mechanism that underlie formation of unique carbon cage materials, which may be used as a benchmark to guide future nanocarbon explorations. 1 National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL 32310, USA. 2 Departament de Química Física i Inorgànica, Universitat Rovira i Virgili, Tarragona 43007, Spain. 3 Department of Chemistry, University of Texas at El Paso, El Paso, TX 79968, USA. 4 Department of Chemistry and Biochemistry, Florida State University, Tallahassee, FL 32306, USA. Marc Mulet-Gas and Laura Abella contributed equally to this work. -
Clusters: Structure, Energetics, and Dynamics of Intermediate States of Matter A
Subscriber access provided by Johns Hopkins Libraries Article Clusters: Structure, Energetics, and Dynamics of Intermediate States of Matter A. W. Castleman, and K. H. Bowen J. Phys. Chem., 1996, 100 (31), 12911-12944• DOI: 10.1021/jp961030k • Publication Date (Web): 01 August 1996 Downloaded from http://pubs.acs.org on May 8, 2009 More About This Article Additional resources and features associated with this article are available within the HTML version: • Supporting Information • Links to the 42 articles that cite this article, as of the time of this article download • Access to high resolution figures • Links to articles and content related to this article • Copyright permission to reproduce figures and/or text from this article The Journal of Physical Chemistry is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 J. Phys. Chem. 1996, 100, 12911-12944 12911 Clusters: Structure, Energetics, and Dynamics of Intermediate States of Matter A. W. Castleman, Jr.* Department of Chemistry, PennsylVania State UniVersity, 152 DaVey Laboratory, UniVersity Park, PennsylVania 16802 K. H. Bowen, Jr. Department of Chemistry, The Johns Hopkins UniVersity, 3400 N. Charles Street, Baltimore, Maryland 21218 ReceiVed: April 4, 1996; In Final Form: June 20, 1996X The field of cluster research can trace its origins back to the mid-nineteenth century when early studies of colloids, aerosols, and nucleation phenomena were reported. The field underwent a resurgence of interest several decades ago when well-defined clusters were observed in supersonic expansions that could be investigated using mass spectrometers. The advent of the laser provided a new dimension, enabling detailed spectroscopic observations through the probing of systems of varying size and degree of solvation. -
Transformation of Doped Graphite Into Cluster- Encapsulated Fullerene Cages
ARTICLE DOI: 10.1038/s41467-017-01295-9 OPEN Transformation of doped graphite into cluster- encapsulated fullerene cages Marc Mulet-Gas1, Laura Abella2, Maira R. Cerón 3, Edison Castro 3, Alan G. Marshall1,4, Antonio Rodríguez-Fortea 2, Luis Echegoyen3, Josep M. Poblet 2 & Paul W. Dunk 1 An ultimate goal in carbon nanoscience is to decipher formation mechanisms of highly ordered systems. Here, we disclose chemical processes that result in formation of high- 1234567890 symmetry clusterfullerenes, which attract interest for use in applications that span biome- dicine to molecular electronics. The conversion of doped graphite into a C80 cage is shown to occur through bottom-up self-assembly reactions. Unlike conventional forms of fullerene, the iconic Buckminsterfullerene cage, Ih-C60, is entirely avoided in the bottom-up formation mechanism to afford synthesis of group 3-based metallic nitride clusterfullerenes. The effects of structural motifs and cluster–cage interactions on formation of compounds in the solvent- extractable C70–C100 region are determined by in situ studies of defined clusterfullerenes under typical synthetic conditions. This work establishes the molecular origin and mechanism that underlie formation of unique carbon cage materials, which may be used as a benchmark to guide future nanocarbon explorations. 1 National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL 32310, USA. 2 Departament de Química Física i Inorgànica, Universitat Rovira i Virgili, Tarragona 43007, Spain. 3 Department of Chemistry, University of Texas at El Paso, El Paso, TX 79968, USA. 4 Department of Chemistry and Biochemistry, Florida State University, Tallahassee, FL 32306, USA. Marc Mulet-Gas and Laura Abella contributed equally to this work. -
A Unified View of Ligand-Protected Gold Clusters As Superatom Complexes
A unified view of ligand-protected gold clusters as superatom complexes Michael Walter†, Jaakko Akola†‡, Olga Lopez-Acevedo†, Pablo D. Jadzinsky§¶, Guillermo Calero§, Christopher J. Ackerson§ʈ, Robert L. Whetten††, Henrik Gro¨ nbeck‡‡, and Hannu Ha¨ kkinen†§§¶¶ Departments of †Physics and §§Chemistry, Nanoscience Center, University of Jyva¨skyla¨, FI-40014 Jyva¨skyla¨, Finland; ‡Institut fu¨r Festko¨rperforschung, Forschungszentrum Ju¨lich, D-52425 Ju¨lich, Germany; §Department of Structural Biology, Stanford University School of Medicine, Stanford, CA 94305; ¶Department of Applied Physics, Stanford University, Stanford, CA 94305; ††School of Chemistry and Biochemistry, Georgia Institute of Technology, Atlanta, GA 30332; and ‡‡Competence Centre for Catalysis and Department of Applied Physics, Chalmers University of Technology, SE-41296, Go¨teborg, Sweden Edited by Royce W. Murray, University of North Carolina, Chapel Hill, NC, and approved April 10, 2008 (received for review January 31, 2008) Synthesis, characterization, and functionalization of self-assembled, 6s orbitals (10, 11), representing a finite-system analogy to the ligand-stabilized gold nanoparticles are long-standing issues in the bulk conduction electron states, which have 6s-character close to chemistry of nanomaterials. Factors driving the thermodynamic the Fermi surface. Exceptional stability is associated with a total stability of well documented discrete sizes are largely unknown. count of Herein, we provide a unified view of principles that underlie the stability of