Magnetism of Carbon Nanostructures and in Situ TEM Dynamic Transformations of Carbon-Based Nanomaterials

Total Page:16

File Type:pdf, Size:1020Kb

Magnetism of Carbon Nanostructures and in Situ TEM Dynamic Transformations of Carbon-Based Nanomaterials INSTITUTO POTOSINO DE INVESTIGACION´ CIENT´IFICA Y TECNOLOGICA,´ A.C. POSGRADO EN CIENCIAS APLICADAS Magnetism of carbon nanostructures and in situ TEM dynamic transformations of carbon-based nanomaterials Tesis que presenta Julio Alejandro Rodr´ıguezManzo Para obtener el grado de Doctor en Ciencias Aplicadas En la opci´onde Nanociencias y Nanotecnolog´ıa Codirectores de la Tesis: Dr. Humberto Terrones Maldonado Dr. Mauricio Terrones Maldonado Dr. Florentino L´opez Ur´ıas San Luis Potos´ı,S.L.P., febrero de 2007. Constancia de aprobaci´onde la tesis La tesis Magnetism of carbon nanostructures and in situ TEM dynamic transformations of carbon-based nanomaterials presentada para obtener el Grado de Doctor en Ciencias Aplicadas en la opci´onNanociencias y Nanotec- nolog´ıafue elaborada por Julio Alejandro Rodr´ıguezManzo y aprobada el 1 de febrero de 2007 por los suscritos, designados por el Colegio de Profesores de la Divisi´onde Materiales Avanzados del Instituto Potosino de Investigaci´onCient´ıfica y Tecnol´ogica,A.C. ——————————————————— ——————————————————— Dr. Humberto Terrones Maldonado Dr. Mauricio Terrones Maldonado Codirector de la tesis Codirector de la tesis ——————————————————— ——————————————————— Dr. Florentino L´opez-Ur´ıas Dr. Emilio Mu˜nozSandoval Codirector de la tesis Comit´etutorial iii Cr´editosinstitucionales Esta tesis fue elaborada en la Divisi´onde Materiales Avanzados del Instituto Potosino de Investigaci´onCient´ıficay Tecnol´ogica,A.C., bajo la codirecci´onde los doctores Humberto Terrones Maldonado, Mauricio Terrones Maldonado y Florentino L´opez-Ur´ıas. Durante la realizaci´ondel trabajo el autor recibi´ouna beca acad´emicadel Con- sejo Nacional de Ciencia y Tecnolog´ıa (No. de registro 172777) y del Instituto Potosino de Investigaci´onCient´ıficay Tecnol´ogica,A. C. v Acknowledgments Anybody who knows about the subject will say that searching for a good advisor is a difficult task. Finding two, in quantum mechanics terms, is highly improbable. If both are brothers, good luck must be involved. During these years, Humberto and Mauricio Terrones have been excellent advisors. Always available in their office, they transmitted their joy for science and research and made me feel part of the scientific community dedicated to the study of carbon nanostructures that goes back to Alan Mackay and Harry Kroto, among others, and continues with them. My gratitude to both. The advice given by Florentino L´opez was fundamental for obtaining results on the magnetic properties of carbon nanostructures. I thank him for his willingness to share his programming knowledge, as well as his availability to work as a team. In addition, I thank him and Emilio Mu˜nozfor their generosity: they shared their office with me during the 99% of my stay at IPICYT. The time at IPICYT would have been less fortunate without the support, the share frustration and the enthusiasm of my fellow travelers: Ana Laura El´ıasand Adalberto Zamudio, to whom I am grateful. Also, I wish to acknowledge Jos´eRomo, for being there to hear and talk about ideas related to carbon nanostructures, among other subjects; Eduardo Cruz, for his help with anything related to my computer’s software; David Meneses, who helped me in the analysis of X ray data, and saved me from a row in Guanajuato; and Xavier Lepr´o,who at the end of this stage helped me with everything about Latex. One of the most pleasing aspects of carrying out scientific research is the pos- sibility to meet people in different places who are more than happy to share their expertise and knowledge. I thank David Smith, Martha McCartney and Lin Gu from Arizona State University, for being there to teach me the different techniques that can be used in the transmission electron microscope (TEM). It was during the ix winter school in electron microscopy at ASU that I was first introduced to the ex- citing aspects of this technique. I also thank Manfred R¨uhlefor his invitation to carry out both the synthesis and characterization of single-walled carbon nanotubes at the Max-Planck-Institut f¨urMetallforschung in Stuttgart, where Fabio Lupo was an outstanding host, and I thank him for that. Also, I am grateful to Gerd Kurt Reiband, Juan Jos´eVilatela and Felipe Cervantes for their help to realize quenching experiments at the Santa Rita laboratory. I thank Paola Ayala for her invitation to participate in a series of experiments to deposit nanoparticles on nitrogen-doped carbon nanotubes. The experiments of nanotube electron irradiation in the TEM were motivated by the innovative previous work of Florian Banhart. I thank him for his kind invitation to the University of Mainz, where he shared, enthusiastically, his experience. I thank also Litao Sun who helped me with the irradiation experiments. For the essential technical assistance needed in a laboratory –and even more in a laboratory under construction– I am grateful to Lisette Noyola, Grisel Ram´ırezand Daniel Ram´ırez.I thank Adolfo Mart´ınezfor his support with everything related to Linux. I thank Gabi P´erezAssaf for helping me to elucidate terms and procedures of the complex administration world. For financial support I thank the following institutions: CONACYT, IPICYT, Max-Planck-Institut f¨urMetallforschung, Max-Planck-Institut f¨urPoly- merforschung/Universit¨atMainz and Arizona State University. Anybody who finds this thesis readable should acknowledge, as I do, the effort carried out by Faith Coldren to edit this work: thanks. Finally, I would like to thank mi sister Olga, my brothers Joaqu´ıny Claudio, and my parents Olga y Joaqu´ın.Not only they have indulged my interest in science, but each, in his or her own way, as nurtured it. x Contents Acknowledgments .............................. ix List of Tables ................................. xv List of Figures . xvii Resumen ....................................xxi Abstract . xxiii Preface .....................................xxv 1 General introduction 1 1.1 Carbon nanostructures and related materials . 1 1.1.1 spn hybridizations in carbon . 2 1.1.2 Carbon allotropes . 3 1.2 The concept of curvature . 6 1.3 Magnetism of curved carbon nanostructures . 8 1.4 Electron irradiation of carbon nanostructures . 9 1.5 Organization of the thesis . 9 References . 11 2 Magnetic response of π-electrons 15 2.1 Introduction . 15 2.2 Magnetism of carbon allotropes . 16 2.3 Coalescence of C60 and carbon nanotori . 20 2.3.1 Coalescence of C60 ........................ 20 2.3.2 Carbon nanotori . 21 2.3.3 Corrugated carbon nanotori . 24 2.4 The London theory . 26 xi 2.5 Benzene, C60 and C70: case studies . 28 2.6 Polymerized C60 and C70 molecules . 32 2.7 Nanotori from SWNT (only hexagonal rings) . 38 2.8 Corrugated nanotori (heptagonal and octagonal rings) . 41 2.8.1 Tori C60-C2(8) . 43 2.8.2 Tori C60-C3(7) . 44 2.8.3 Tori C60-C5(8) . 45 2.9 Doped carbon nanotori . 46 2.10 Topologically complex carbon nanostructures . 52 2.11 Conclusions . 53 References . 55 3 Synthesis of different types of CNTs 59 3.1 Introduction . 59 3.2 Carbon nanotube growth methods . 60 3.3 Pyrolysis of aerosolized solutions . 61 3.3.1 Injection aerosol generator . 62 3.3.2 Ultrasonic aerosol generator . 63 3.4 Characterization techniques . 63 3.5 Single-walled carbon nanotubes (SWNTs) . 64 3.5.1 Experimental conditions . 64 3.5.2 SEM and TEM analysis . 65 3.5.3 Raman spectroscopy of SWNTs . 67 3.5.4 SWNT growth model . 70 3.6 Multi-walled carbon nanotubes . 71 3.6.1 Experimental conditions . 72 3.6.2 Characterization of MWNTs . 72 3.6.3 MWNT growth model . 74 3.7 Growth of nitrogen-doped MWNTs . 74 3.7.1 Experimental conditions . 75 3.7.2 Characterization of CNx ..................... 75 3.8 Metal inclusions inside MWNTs . 78 xii 3.8.1 Fe@MWNTs . 78 3.8.2 Co@MWNTs . 79 3.8.3 Ni@MWNTs . 83 3.8.4 FeCo@MWNTs . 86 3.9 Conclusions . 88 References . 90 4 TEM modifications of MWNT-based nanostructures 95 4.1 Introduction . 95 4.2 Electron irradiation effects in solids . 96 4.2.1 Electron irradiation effects in carbon nanostructures . 99 4.2.2 Thermal annealing of defects induced by electron irradiation . 104 4.3 Experimental conditions . 107 4.4 MWNTs as high pressure cells and nanoextruders . 107 4.4.1 Experimental observations . 108 4.4.2 Mechanism of pressure buildup . 113 4.5 Carbon nanotube growth . 115 4.5.1 SWNT growth . 116 4.5.2 MWNT growth . 118 4.5.3 Possible nanotube growth mechanism . 121 4.6 MWNT-metal-MWNT junctions . 123 4.6.1 Formation of MWNT-metal-MWNT junctions . 123 4.6.2 Rupture of MWNT-metal-MWNT junctions . 127 4.7 Coda: curvature in carbon nanostructures . 129 4.8 Conclusions . 131 References . 133 5 Conclusions and future work 139 5.1 Conclusions . 139 5.2 Future work . 141 Published articles ..............................143 xiii List of Tables 2.1 Ring current χ and maximum iij for C60 and C70 . 31 2.2 Ring current χ and maximum iij for C60 dimers . 33 2.3 Ring current χ and maximum iij for nC60-C5(8) and nC70-C5(8) lin- ear chains . 36 max 2.4 Maximum inter-atomic currents iij for corrugated carbon nanotori . 42 4.1 Threshold energies for graphite . 99 4.2 Formation and migration energies for interstitials and vacancies in graphite . 102 4.3 Diffusion rates of carbon interstitials . 105 xv List of Figures 1.1 Different spn hybridizations in carbon . 2 1.2 Allotropes of carbon . 3 1.3 Notation (n, m) to classify SWNTs . 5 1.4 Surfaces, carbon lattices and carbon nanostructures with different Gaussian curvature . 7 2.1 Ring current pattern in anthracene . 17 2.2 Electron microscopy images of carbon nanotubes . 18 2.3 Rhombohedral C60 ...........................
Recommended publications
  • Predicting Experimentally Stable Allotropes: Instability of Penta-Graphene
    Predicting experimentally stable allotropes: Instability of penta-graphene Christopher P. Ewelsa,1, Xavier Rocquefelteb, Harold W. Krotoc,1, Mark J. Raysond,e, Patrick R. Briddone, and Malcolm I. Heggied aInstitut des Matériaux Jean Rouxel, CNRS UMR 6502, Université de Nantes, 44322 Nantes, France; bInstitut des Sciences Chimiques de Rennes, UMR 6226 CNRS, Université de Rennes 1, 35042 Rennes, France; cDepartment of Chemistry and Biochemistry, Florida State University, Tallahassee, FL 32306; dDepartment of Chemistry, University of Surrey, Guildford, Surrey GU2 7XH, United Kingdom; and eSchool of Electrical and Electronic Engineering, University of Newcastle, Newcastle upon Tyne NE1 7RU, United Kingdom Contributed by Harold W. Kroto, October 14, 2015 (sent for review September 25, 2015; reviewed by Peter John Frederick Harris and Humberto Terrones) In recent years, a plethora of theoretical carbon allotropes have been Results and Discussion proposed, none of which has been experimentally isolated. We Thermodynamic Stability: Relative Energy. The first test of any new discuss here criteria that should be met for a new phase to be poten- proposed structure is of its thermodynamic stability. Considering tially experimentally viable. We take as examples Haeckelites, 2D penta-graphene, although real phonon energies (positive eigen- 2 networks of sp -carbon–containing pentagons and heptagons, and values from the Hessian matrix) indicate that it is at least a local “penta-graphene,” consisting of a layer of pentagons constructed structural minimum (4), its formation enthalpy shows that it is a 2 3 from a mixture of sp -andsp -coordinated carbon atoms. In 2D pro- very high-energy structure. We have performed a number of calcu- jection appearing as the “Cairo pattern,” penta-graphene is elegant lations on penta-graphene and structural derivatives, using density and aesthetically pleasing.
    [Show full text]
  • 3 ,)! (Ŗ #(. , .#)(Ŗ1#."Ŗ , )(Ŗ ( ()-.,/ ./, -Ŗ
    %FQBSUNFOUPG"QQMJFE1IZTJDT " BM #') ŗ U P % % ŗ 3,)!(ŗ " 0#& <#( #(.,.#)(ŗ1#."ŗ (ŗ ,)(ŗ 3,) ! (ŗ#(. (()-.,/./,-ŗ , . #) (ŗ1 5JNP7FIWJM»JOFO #. " ŗ ,) (ŗ(() -. ,/ . /, -ŗ 9HSTFMG*aeegjj+ 9HSTFMG*aeegjj+ *4#/ #64*/&44 *4#/ QEG &$0/0.: *44/- *44/ "35 *44/ QEG %&4*(/ "3$)*5&$563& " B "BMUP6OJWFSTJUZ M U 4DIPPMPG4DJFODF 4$*&/$& P %FQBSUNFOUPG"QQMJFE1IZTJDT 5&$)/0-0(: 6 XXXBBMUPGJ OJ W $304407&3 F S T %0$503"- J %0$503"- U %*44&35"5*0/4 Z %*44&35"5*0/4 Aalto University publication series DOCTORAL DISSERTATIONS 5/2012 Hydrogen interaction with carbon nanostructures Timo Vehviläinen Doctoral dissertation for the degree of Doctor of Science in Technology to be presented with due permission of the School of Science for public examination and debate in Auditorium K at the Aalto University School of Science (Espoo, Finland) on the 19th of January 2012 at 13 o’clock. Aalto University School of Science Department of Applied Physics Electronic Properties of Materials Supervisor Prof. Risto Nieminen Instructor Dr. Maria Ganchenkova Preliminary examiners Prof. Tapani Pakkanen, University of Eastern Finland Prof. Gotthard Seifert, Technische Universität Dresden Opponent Prof. Kim Bolton, University of Borås Aalto University publication series DOCTORAL DISSERTATIONS 5/2012 © Timo Vehviläinen ISBN 978-952-60-4469-9 (printed) ISBN 978-952-60-4470-5 (pdf) ISSN-L 1799-4934 ISSN 1799-4934 (printed) ISSN 1799-4942 (pdf) Unigrafia Oy Helsinki 2012 Finland The dissertation can be read at http://lib.tkk.fi/Diss/ Publication orders (printed
    [Show full text]
  • Instability of Penta-Graphene
    Predicting experimentally stable allotropes: Instability of penta-graphene Christopher P. Ewelsa,1, Xavier Rocquefelteb, Harold W. Krotoc,1, Mark J. Raysond,e, Patrick R. Briddone, and Malcolm I. Heggied aInstitut des Matériaux Jean Rouxel, CNRS UMR 6502, Université de Nantes, 44322 Nantes, France; bInstitut des Sciences Chimiques de Rennes, UMR 6226 CNRS, Université de Rennes 1, 35042 Rennes, France; cDepartment of Chemistry and Biochemistry, Florida State University, Tallahassee, FL 32306; dDepartment of Chemistry, University of Surrey, Guildford, Surrey GU2 7XH, United Kingdom; and eSchool of Electrical and Electronic Engineering, University of Newcastle, Newcastle upon Tyne NE1 7RU, United Kingdom Contributed by Harold W. Kroto, October 14, 2015 (sent for review September 25, 2015; reviewed by Peter John Frederick Harris and Humberto Terrones) In recent years, a plethora of theoretical carbon allotropes have been Results and Discussion proposed, none of which has been experimentally isolated. We Thermodynamic Stability: Relative Energy. The first test of any new discuss here criteria that should be met for a new phase to be poten- proposed structure is of its thermodynamic stability. Considering tially experimentally viable. We take as examples Haeckelites, 2D penta-graphene, although real phonon energies (positive eigen- 2 networks of sp -carbon–containing pentagons and heptagons, and values from the Hessian matrix) indicate that it is at least a local “penta-graphene,” consisting of a layer of pentagons constructed structural minimum (4), its formation enthalpy shows that it is a 2 3 from a mixture of sp -andsp -coordinated carbon atoms. In 2D pro- very high-energy structure. We have performed a number of calcu- jection appearing as the “Cairo pattern,” penta-graphene is elegant lations on penta-graphene and structural derivatives, using density and aesthetically pleasing.
    [Show full text]
  • Nanomaterials Introduction Nanomaterials•Top-Down Science •Bottom-Up Science
    nanomaterials introduction Nanomaterials•Top-down Science •Bottom-up Science What are nanomaterials? Nanomaterials are materials are materials possessing grain sizes on the order of a billionth of a meter.(10 -9 M) A material in which at least one side is between 1 and 1000 nm. Nanomaterial research literally exploded in mid -1980’s Some slides by Maya Bhatt history • Big bang • Fires • 1950- fused silica • Why such a buzz word today? Examples • Several biological materials are nanomaterials- bone, hair, wing scales on a butterfly etc. • Viruses are nanomaterials • Clays • Pigments • Volcanic ash Engineered nanomaterials (ENM or EN) Materials manufactured for their properties • Sunscreens • Paints • Cosmetics • Fillers • Catalysts INCIDENTAL: ultrafine airborne particles NATURAL • Conventional materials have grain size anywhere from 100 µm to 1mm and more • Particles with size between 1-100(0) nm are normally regarded as Nanomaterials • The average size of an atom is in the order of 1-2 Angstroms in radius. • 1 nanometer =10 Angstroms • 1 nm there may be 3-5 atoms Two principal factors cause the properties of nanomaterials to differ significantly from Bulk materials: • Increased relative surface area: a greater amount of the material comes into contact with surrounding materials and increases reactivity • Quantum effects. These factors can change or enhance properties such as reactivity, strength and electrical characteristics. Surface Effects • As a particle decreases in size, a greater proportion of atoms are found at the surface compared to those inside. For example, a particle of • Size-30 nm-> 5% of its atoms on its surface • Size-10 nm->20% of its atoms on its surface • Size-3 nm-> 50% of its atoms on its surface • Nanoparticals are more reactive than large particles (Catalyst) Quantum Effects Quantum confinement The quantum confinement effect can be observed once the diameter of the particle is of the same magnitude as the wavelength of the electron Wave function.
    [Show full text]
  • NOTICE: This Is the Author's Version of a Work That Was Accepted For
    NOTICE: this is the author’s version of a work that was accepted for publication in Carbon. Changes resulting from the publishing process, such as peer review, editing, corrections, structural formatting, and other quality control mechanisms may not be reflected in this document. Changes may have been made to this work since it was submitted for publication. A definitive version was subsequently published in Carbon [VOL 50, ISSUE 3, March 2012] DOI 10.1016/j.carbon.2011.11.002 GUEST EDITORIAL Nomenclature of sp2 carbon nanoforms Carbon’s versatile bonding has resulted in the discovery of a bewildering variety of nanoforms which urgently need a systematic and standard nomenclature [1]. Besides fullerenes, nanotubes and graphene, research teams around the globe now produce a plethora of carbon-based nanoforms such as ‘bamboo’ tubes, ‘herringbone’ and ‘bell’ structures. Each discovery duly gains a new, sometimes whimsical, name, often with its discoverer unaware that the same nanoform has already been reported several times but with different names (for example the nanoform in Figure 1i is in different publications referred to as ‘bamboo’ [2], ‘herringbone-bamboo’ [3], ‘stacked-cups’ [4] and ‘stacked-cones’ [5]). In addition, a single name is often used to refer to completely different carbon nanoforms (for example, the ‘bamboo’ structure in [2] is notably different from ‘bamboo’ in Ref [6]). The result is a confusing overabundance of names which makes literature searches and an objective comparison of results extremely difficult, if not impossible. There have been several attempts to bring order to the chaos of carbon nomenclature. An IUPAC subcommittee on carbon terminology and characterization that ran until 1991 produced a glossary of 114 terms for carbon materials.
    [Show full text]
  • Advanced Current Collectors with Carbon Nanofoams for Electrochemically Stable Lithium—Sulfur Cells
    nanomaterials Article Advanced Current Collectors with Carbon Nanofoams for Electrochemically Stable Lithium—Sulfur Cells Shu-Yu Chen 1 and Sheng-Heng Chung 1,2,* 1 Department of Materials Science and Engineering, National Cheng Kung University, No. 1, University Road, Tainan City 701, Taiwan; [email protected] 2 Hierarchical Green-Energy Materials Research Center, National Cheng Kung University, No. 1, University Road, Tainan City 701, Taiwan * Correspondence: [email protected] Abstract: An inexpensive sulfur cathode with the highest possible charge storage capacity is attractive for the design of lithium-ion batteries with a high energy density and low cost. To promote existing lithium–sulfur battery technologies in the current energy storage market, it is critical to increase the electrochemical stability of the conversion-type sulfur cathode. Here, we present the adoption of a carbon nanofoam as an advanced current collector for the lithium–sulfur battery cathode. The carbon nanofoam has a conductive and tortuous network, which improves the conductivity of the sulfur cathode and reduces the loss of active material. The carbon nanofoam cathode thus enables the development of a high-loading sulfur cathode (4.8 mg cm−2) with a high discharge capacity that approaches 500 mA·h g−1 at the C/10 rate and an excellent cycle stability that achieves 90% capacity retention over 100 cycles. After adopting such an optimal cathode configuration, we superficially coat the carbon nanofoam with graphene and molybdenum disulfide (MoS2) to amplify the fast charge transfer and strong polysulfide-trapping capabilities, respectively. The highest charge storage −1 Citation: Chen, S.-Y.; Chung, S.-H.
    [Show full text]
  • Symposium GG: 2004 MRS Fall Meeting (PDF)
    SYMPOSIUM GG Mesoscale Architectures from Nano-Units-Assembly, Fabrication, and Properties November 29 - December 2, 2004 Chairs G. Ramanath Paul V. Braun Dept. of Materials Science & Engineering Dept. of Materials Science & Engineering Rensselaer Polytechnic Institute Univ. of Illinois, Urbana-Champaign 110 Eighth St. 1304 W. Green St. Troy, NY 12180-3590 Urbana, IL 61801 518-276-6844 217-244-7293 Mauricio Terrones Advanced Materials Dept IPICyT Camino ala Presa San Jose 2055 Lomas 4a seccion San Luis Potosi, SLP, 78216 Mexico 52-444-834-2039 Symposium Support Army Research Office Mexican Society of Nanoscience and Nanotechnology * Invited paper 783 SESSION GGl: Nanotemplating for Meso-scale mesoporous hollow spheres while permitting the passage of smaller Assembly I molecules will be described. Chairs: Yunfeng Lu and G. Ramanath Monday Morning, November 29, 2004 9:30 AM GG1.4 Room 311 (Hynes) Fabrication of Asymmetrically Coated Colloid Particles by Microcontact Printing Techniques. Olivier J. Cayre, Dpt of 8:30 AM *GG1.1 chemistry, University of Hull, HULL, United Kingdom. Adding a New Dimension in Nanoscale Materials: Metal Nanoparticles with Phase Separated Ligand Shells. We developed a novel method for preparation of asymmetrically Francesco Stellacci, Department of Materials Science and Engineering, coated colloid parti-cles by using a microcontact printing technique. MIT, Cambridge, Massachusetts. Films of water-insoluble ionic surfactants deposited on PDMS stamps were printed onto latex particle monolayers of opposite surface charge Ligand coated metal nanoparticles are promising nanosize materials in order to produce spherical latex particles of dipolar surface charge for novel electronic and optical devices. Their main strength is in the distribution.
    [Show full text]
  • Nanomaterials •Top-Down Science •Bottom-Up Science
    Nanomaterials •Top-down Science •Bottom-up Science What are nanomaterials? Nanomaterials-9 are materials are materials possessing grain sizes on the order of a billionth of a meter.(10Nanomaterial research M) literally exploded in mid -1980’s Typical size of small particles Particle size µm Tobacco mosaic Virus Hepatitis B Virus Bacteria Pollen Nanoparticles Human Hair Soot Carbon black 0.001 0.01 0.1 1 10 100 1000 • Conventional material have grain size anywhere from 100 µm to 1mm and more • Particles with size between 1-100 nm are normally regarded as Nanomaterials • The average size of an atom is in the order of 1-2 Angstroms in radius. • 1 nanometer =10 Angstroms • 1 nm there may be 3-5 atoms • Two principal factors cause the properties of nanomaterials to differ significantly from Bulk materials: • Increased relative surface area • Quantum effects. These factors can change or enhance properties such as reactivity, strength and electrical characteristics. Surface Effects • As a particle decreases in size, a greater proportion of atoms are found at the surface compared to those inside. For example, a particle of • Size-30 nm-> 5% of its atoms on its surface • Size-10 nm->20% of its atoms on its surface • Size-3 nm-> 50% of its atoms on its surface • Nanoparticals are more reactive than large particles (Catalyst) Quantum Effects Quantum confinement The quantum confinement effect can be observed once the diameter of the particle is of the same magnitude as the wavelength of the electron Wave function. Quantum confinement is responsible for the increase of energy difference between energy states and band gap.
    [Show full text]
  • Large-Scale Synthesis of Carbon Nanomaterials by Catalytic Chemical Vapor Deposition: a Review of the Effects of Synthesis Parameters and Magnetic Properties
    Materials 2010, 3, 4142-4174; doi:10.3390/ma3084142 OPEN ACCESS materials ISSN 1996–1944 www.mdpi.com/journal/materials Review Large-Scale Synthesis of Carbon Nanomaterials by Catalytic Chemical Vapor Deposition: A Review of the Effects of Synthesis Parameters and Magnetic Properties Xiaosi Qi 1, Chuan Qin 1, Wei Zhong 1,*, Chaktong Au 2,*, Xiaojuan Ye 1and Youwei Du 1 1 Nanjing National Laboratory of Microstructures and Jiangsu Provincial Laboratory for NanoTechnology, Nanjing University, Nanjing 210093, China; E-Mails: [email protected] (X.S.Q.); [email protected] (C.Q.); [email protected] (X.J.Y.); [email protected] (Y.W.D.) 2 Chemistry Department, Hong Kong Baptist University, Hong Kong, China * Authors to whom correspondence should be addressed; E-Mails: [email protected] (W.Z.); [email protected] (C.T.A.); Tel.: +86-25-83621200; Fax: +86-25-83595535. Received: 26 June 2010 / Accepted: 26 July 2010 / Published: 30 July 2010 Abstract: The large-scale production of carbon nanomaterials by catalytic chemical vapor deposition is reviewed in context with their microwave absorbing ability. Factors that influence the growth as well as the magnetic properties of the carbon nanomaterials are discussed. Keywords: carbon nanomaterials; catalytic chemical vapor deposition; magnetic properties; microwave absorbing ability 1. Introduction Since the landmark paper of Ijima [1], carbon nanotubes (CNTs) have been studied widely [2-4]. The unique physical and chemical properties of CNTs suggests that the materials can potentially be utilized in areas such as field emission display [5], microelectronic devices [6-12], hydrogen storage [13] and composite material additives [14].
    [Show full text]
  • Nanowire Arrays and 3D Porous Conducting Networks for Li-Ion Battery Electrodes Written by Miao Tian Has Been Approved for the Department of Mechanical Engineering
    Nanowire Arrays and 3D Porous Conducting Networks for Li-Ion Battery Electrodes by Miao Tian B.S., Xi’an Jiaotong University, China, 2007 M.S., University of Colorado at Boulder, 2010 A thesis Submitted to the Faculty of the Graduate School of the University of Colorado in partial fulfillment of the requirements for the degree of Doctor of Philosophy Department of Mechanical Engineering April 2014 This thesis entitled: Nanowire Arrays and 3D Porous Conducting Networks for Li-Ion Battery Electrodes written by Miao Tian has been approved for the Department of Mechanical Engineering (Professor Ronggui Yang, Chair) (Professor Se-Hee Lee) Date The final copy of this thesis has been examined by the signatories, and we Find that both the content and the form meet acceptable presentation standards Of scholarly work in the above mentioned discipline. Abstract Tian, Miao (Ph.D., Department of Mechanical Engineering) Nanowire Electrodes and 3D Porous Conducting Networks for Li-Ion Batteries Thesis directed by Associate Professor Ronggui Yang There have been growing interests in developing high-capacity, high-power, and long-cycle- life lithium-ion (Li-ion) batteries due to the increasing power requirements of portable electronics and electrical vehicles. Various efforts have been made to utilize nano-structured electrodes since they can improve the performance of Li-ion batteries compared to bulk materials in many ways: fast electrode reaction due to the large surface area, efficient volume-change accommodation due to the small size, and fast Li-ion transport along the nanoscale gaps. Among various nanostructures, nanowire arrays present an excellent candidate for high performance lithium-ion battery electrodes, which have attracted intensive research over the past few years.
    [Show full text]
  • Carbon Structures and Defect Planes in Diamond at High Pressure
    PHYSICAL REVIEW B 88, 014102 (2013) Carbon structures and defect planes in diamond at high pressure Silvana Botti,1 Maximilian Amsler,2 Jose´ A. Flores-Livas,1 Paul Ceria,1 Stefan Goedecker,2 and Miguel A. L. Marques1 1Institut Lumiere` Matiere,` UMR5306, Universite´ Lyon 1-CNRS, Universite´ de Lyon, F-69622 Villeurbanne Cedex,France 2Department of Physics, Universitat¨ Basel,Klingelbergstrasse 82, 4056 Basel, Switzerland (Received 26 October 2012; published 8 July 2013) We performed a systematic structural search of high-pressure carbon allotropes for unit cells containing from 6 to 24 atoms using the minima hopping method. We discovered a series of new structures that are consistently lower in enthalpy than the ones previously reported. Most of these include (5 + 7)- or (4 + 8)-membered rings and can therefore be placed in the families proposed by H. Niu et al. [Phys. Rev. Lett. 108, 135501 (2012)]. However, we also found three more families with competitive enthalpies that contain (5 + 5 + 8)-membered rings, sp2 motives, or buckled hexagons. These structures are likely to play an important role in dislocation planes and structural defects of diamond and hexagonal diamond. DOI: 10.1103/PhysRevB.88.014102 PACS number(s): 61.66.Bi, 61.50.Ks, 62.50.−p I. INTRODUCTION (see Fig. 5), most of the proposed theoretical structures fit the experimental data equally well. Many other measurements Carbon has long since enticed the imagination of re- exist, mainly coming from Raman scattering experiments on searchers. Not only is it the key component of life, but it also samples under pressure.27 In this case the interpretation of finds numerous applications in diverse fields of technology.
    [Show full text]
  • Elias Lectures Chemistry of Carbon Fullerenes Final 30Th
    The inorganic chemistry of Carbon Carbon Nano tubes Graphite intercalated compounds Graphene Fullerenes In 1985, Harold Kroto (Sussex), Robert Curl and Richard Smalley, (Rice University,) discovered C 60 , and shortly thereafter came to discover the fullerenes. Kroto, Curl, and Smalley were awarded the 1996 Nobel Prize in Chemistry for their roles in the discovery of this class of H. Kroto R. Smalley molecules. C 60 and other fullerenes were later noticed occurring outside the laboratory (for example, in normal candle-soot).. Fullerenes An idea from outer space Kroto's special interest in red giant stars rich in carbon led to the discovery of the fullerenes. For years, he had had the idea that long- chained molecules of carbon could form near such giant stars. To mimic this special environment in a laboratory, Curl suggested contact with Smalley who had built an apparatus which could evaporate and analyze almost any material with a laser beam. During the crucial week in Houston in 1985 the Nobel laureates, together with their younger co- workers J. R. Heath and J. C. O'Brien, starting from graphite, managed to produce clusters of carbon consisting mainly of 60 or 70 carbon atoms. These clusters proved to be stable and more interesting than long-chained molecules of carbon. Two questions immediately arose. How are these clusters built? Does a new form of carbon exist besides the two well-known The read-out from the mass spectrometer shows forms graphite and diamond? how the peaks corresponding to C 60 and C70 become more distinct when the experimental conditions are optimized.
    [Show full text]