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De-en Jiang

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Beschreibung

What are the chemical aspects of graphene as a novel 2D material and how do they relate to the molecular structure? This book addresses these important questions from a theoretical and computational standpoint. 

Graphene Chemistry: Theoretical Perspectives presents recent exciting developments to correlate graphene’s properties and functions to its structure through state-of-the-art computational studies. This book focuses on the chemistry aspect of the structure-property relationship for many fascinating derivatives of graphene; various properties such as electronic structure, magnetism, and chemical reactivity, as well as potential applications in energy storage, catalysis, and nanoelectronics are covered. The book also includes two chapters with significant experimental portions, demonstrating how deep insights can be obtained by joint experimental and theoretical efforts. 

Topics covered include:

  • Graphene ribbons: Edges, magnetism, preparation from unzipping, and electronic transport
  • Nanographenes: Properties, reactivity, and synthesis
  • Clar sextet rule in nanographene and graphene nanoribbons
  • Porous graphene, nanomeshes, and graphene-based architecture and assemblies
  • Doped graphene: Theory, synthesis, characterization and applications
  • Mechanisms of graphene growth in chemical vapor deposition
  • Surface adsorption and functionalization of graphene
  • Conversion between graphene and graphene oxide
  • Applications in gas separation, hydrogen storage, and catalysis

Graphene Chemistry: Theoretical Perspectives provides a useful overview for computational and theoretical chemists who are active in this field and those who have not studied graphene before. It is also a valuable resource for experimentalist scientists working on graphene and related materials, who will benefit from many concepts and properties discussed here.

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Veröffentlichungsjahr: 2013

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Contents

Cover

Title Page

Copyright

List of Contributors

Preface

Acknowledgements

Chapter 1: Introduction

References

Chapter 2: Intrinsic Magnetism in Edge-Reconstructed Zigzag Graphene Nanoribbons

2.1 Methodology

2.2 Polyacene

2.3 Polyazulene

2.4 Edge-Reconstructed Graphene

2.5 Conclusion

Acknowledgments

References

Chapter 3: Understanding Aromaticity of Graphene and Graphene Nanoribbons by the Clar Sextet Rule

3.1 Introduction

3.2 Armchair Graphene Nanoribbons

3.3 Zigzag Graphene Nanoribbons

3.4 Aromaticity of Graphene

3.5 Perspectives

Acknowledgements

References

Chapter 4: Physical Properties of Graphene Nanoribbons: Insights from First-Principles Studies

4.1 Introduction

4.2 Electronic Properties of Graphene Nanoribbons

4.3 Mechanical and Electromechanical Properties of GNRs

4.4 Summary

Acknowledgements

References

Chapter 5: Cutting Graphitic Materials: A Promising Way to Prepare Graphene Nanoribbons

5.1 Introduction

5.2 Oxidative Cutting of Graphene Sheets

5.3 Unzipping Carbon Nanotubes

5.4 Beyond Oxidative Cutting

5.5 Summary

References

Chapter 6: Properties of Nanographenes

6.1 Introduction

6.2 Synthesis

6.3 Computation

6.4 Geometry of Zigzag-Edged Hexangulenes

6.5 Geometry of Armchair-Edged Hexangulenes

6.6 Geometry of Zigzag-Edged Triangulenes

6.7 Magnetism of Zigzag-Edged Hexangulenes

6.8 Magnetism of Zigzag-Edged Triangulenes

6.9 Chimeric Magnetism

6.10 Magnetism of Oligocenes, Bisanthene-Homologs, Squares and Rectangles

6.11 Concluding Remarks

Acknowledgment

References

Chapter 7: Porous Graphene and Nanomeshes

7.1 Introduction

7.2 Transition State Theory

7.3 Gas and Isotope Separation

7.4 Conclusion and Perspectives

Acknowledgement

References

Chapter 8: Graphene-Based Architecture and Assemblies

8.1 Introduction

8.2 Fullerene Polymers

8.3 Carbon Nanotube Superarchitecture

8.4 Graphene Superarchitectures

8.5 C60/Carbon Nanotube/Graphene Hybrid Superarchitectures

8.6 Boron-Nitride Nanotubes and Monolayer Superarchitectures

8.7 Conclusion

Acknowledgments

References

Chapter 9: Doped Graphene: Theory, Synthesis, Characterization, and Applications

9.1 Introduction

9.2 Substitutional Doping of Graphene Sheets

9.3 Substitutional Doping of Graphene Nanoribbons

9.4 Synthesis and Characterization Techniques of Doped Graphene

9.5 Applications of Doped Graphene Sheets and Nanoribbons

9.6 Future Work

Acknowledgments

References

Chapter 10: Adsorption of Molecules on Graphene

10.1 Introduction

10.2 Physisorption versus Chemisorption

10.3 General Aspects of Adsorption of Molecules on Graphene

10.4 Various Ways of Doping Graphene with Molecules

10.5 Enhancing the Graphene-Molecule Interaction

10.6 Conclusion

References

Chapter 11: Surface Functionalization of Graphene

11.1 Introduction

11.2 Functionalized Graphene: Properties and Challenges

11.3 Theoretical Approach

11.4 Interaction of Graphene with Specific Atoms and Functional Groups

11.5 Surface Functionalization of Graphene Nanoribbons

11.6 Conclusions

References

Chapter 12: Mechanisms of Graphene Chemical Vapor Deposition (CVD) Growth

12.1 Background

12.2 The Initial Nucleation Stage of Graphene CVD Growth

12.3 Continuous Growth of Graphene

12.4 Graphene Orientation Determination in CVD Growth

12.5 Summary and Perspectives

References

Chapter 13: From Graphene to Graphene Oxide and Back

13.1 Introduction

13.2 From Graphene to Graphene Oxide

13.3 Modeling Using PBC Models

13.4 From Graphene Oxide back to Graphene

13.5 Concluding Remarks

Acknowledgement

References

Chapter 14: Electronic Transport in Graphitic Carbon Nanoribbons

14.1 Introduction

14.2 Theoretical Background

14.3 From Graphene to Ribbons

14.4 Graphene Nanoribbon Synthesis and Processing

14.5 Tailoring GNR’s Electronic Properties

14.6 Thermoelectric Properties of Graphene-Based Materials

14.7 Conclusions

Acknowledgements

References

Chapter 15: Graphene-Based Materials as Nanocatalysts

15.1 Introduction

15.2 Electrocatalysts

15.3 Photocatalysts

15.4 CO Oxidation

15.5 Others

15.6 Conclusion

Acknowledgements

References

Chapter 16: Hydrogen Storage in Graphene

16.1 Introduction

16.2 Hydrogen Storage in Molecule Form

16.3 Hydrogen Storage in Atomic Form

16.4 Conclusion

Acknowledgements

References

Chapter 17: Linking Theory to Reactivity and Properties of Nanographenes

17.1 Introduction

17.2 Nanographenes with Only Armchair Edges

17.3 Nanographenes with Both Armchair and Zigzag Edges

17.4 Nanographene with Only Zigzag Edges

17.5 Quinoidal Nanographenes

17.6 Conclusion

References

Chapter 18: Graphene Moiré Supported Metal Clusters for Model Catalytic Studies

18.1 Introduction

18.2 Graphene Moiré on Ru(0001)

18.3 Metal Cluster Formation on g/Ru(0001)

18.4 Two-dimensional Au Islands on g/Ru(0001) and its Catalytic Activity

18.5 Summary

Acknowledgments

References

Index

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Library of Congress Cataloging-in-Publication Data

Graphene chemistry : theoretical perspectives / edited by De-en Jiang, Zhongfang Chen. pages cm Includes bibliographical references and index. ISBN 978-1-119-94212-2 (hardback) 1. Graphene. I. Jiang, De-en, 1975– II. Chen, Zhongfang, 1971– QD341.H9G693 2014 546′.68142–dc23 2013015047

A catalogue record for this book is available from the British Library.

ISBN: 978-1-119-94212-2 (Hardback)

List of Contributors

Zhongfang Chen Department of Chemistry, Institute for Functional Nanomaterials, University of Puerto Rico, USA
Chunyan Chi Department of Chemistry, National University of Singapore, Singapore
Eduardo Costa Girão Departamento de Física, Universidade Federal do Piauí, Brazil
Eduardo Cruz-Silva Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, USA and Department of Polymer Science and Engineering, University of Massachusetts, USA
Feng Ding Institute of Textiles and Clothing, Hong Kong Polytechnic University, Hong Kong
Aijun Du Centre for Computational Molecular Science, Australian Institute for Bioengineering and Nanotechnology, The University of Queensland, Australia
Xingfa Gao Key Laboratory for Biomedical Effects of Nanomaterials and Nanosafety, Institute of High Energy Physics, Chinese Academy of Sciences, China
Hongyan Guo Department of Materials Science and Engineering, CAS Key Laboratory of Materials for Energy Conversion, and Hefei National Laboratory for Physical Science at the Microscale, University of Science and Technology of China, China
Bradley F. Habenicht Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, USA
Marlies Hankel Centre for Computational Molecular Science, Australian Institute for Bioengineering and Nanotechnology, The University of Queensland, Australia
Oded Hod Department of Chemical Physics, School of Chemistry, The Raymond and Beverly Sackler Faculty of Exact Sciences, Tel-Aviv University, Israel
De-en Jiang Chemical Sciences Division, Oak Ridge National Laboratory, USA
Yan Jiao Centre for Computational Molecular Science, Australian Institute for Bioengineering and Nanotechnology, The University of Queensland, Australia and School of Chemical Engineering, The University of Queensland, Australia
Dana Krepel Department of Chemical Physics, School of Chemistry, The Raymond and Beverly Sackler Faculty of Exact Sciences, Tel-Aviv University, Israel
O. Leenaerts Department of Physics, University of Antwerp, Belgium
Fengyu Li Department of Physics and Department of Chemistry, Institute for Functional Nanomaterials, University of Puerto Rico, USA
Yafei Li Department of Chemistry, Institute for Functional Nanomaterials, University of Puerto Rico, USA
Zhenyu Li Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, China
Liangbo Liang Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, USA
Chungen Liu Institute of Theoretical and Computational Chemistry, Key Laboratory of Mesoscopic Chemistry of the Ministry of Education (MOE), Nanjing University, China
Li Liu Department of Chemistry, Texas A&M University, USA
Rui Liu Department of Chemistry, University of Nebraska-Lincoln, USA
Florentino López-Urías Department of Physics, The Pennsylvania State University, USA and Advanced Materials Department, IPICYT, México
Ruitao Lv Department of Physics, The Pennsylvania State University, USA
Vincent Meunier Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, USA
Jonathan Owens Department of Physics, Applied Physics, and Astronomy, Rensselaer Polytechnic Institute, USA
B. Partoens Department of Physics, University of Antwerp, Belgium
F. M. Peeters Department of Physics, University of Antwerp, Belgium
Maria Peressi Department of Physics, University of Trieste, Trieste, Italy and CNR-IOM DEMOCRITOS National Simulation Center, Italy
Michael R. Philpott Visiting Scholar, Kenneth S. Pitzer Center for Theoretical Chemistry, University of California Berkeley, USA and Center for Computational Materials Science, Institute of Materials Research, Tohoku University, Japan
Zexing Qu Institute of Theoretical and Computational Chemistry, Key Laboratory of Mesoscopic Chemistry of the Ministry of Education (MOE), Nanjing University, China
Haibo Shu Institute of Textiles and Clothing, Hong Kong Polytechnic University, Hong Kong
Sean C. Smith Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, USA
Bobby G. Sumpter Center of Nanophase Materials Sciences, Oak Ridge National Laboratory, USA
Zhe Sun Department of Chemistry, National University of Singapore, Singapore
Humberto Terrones Department of Physics, The Pennsylvania State University, USA and Departamento de Física, Universidade Federal do Ceará, Brazil
Mauricio Terrones Department of Physics, The Pennsylvania State University, USA and Department of Materials Science and Engineering and Materials Research Institute, The Pennsylvania State University,USA and Research Center for Exotic Nanocarbons (JST), Shinshu University, Japan
Dihua Wu Tianjin Key Laboratory of Metal and Molecule Based Material Chemistry, Key Laboratory of Advanced Energy Materials Chemistry (Ministry of Education), Computational Centre for Molecular Science, Institute of New Energy Material Chemistry, Nankai University, China
Jishan Wu Department of Chemistry, National University of Singapore, Singapore
Xiaojun Wu Department of Materials Science and Engineering, CAS Key Laboratory of Materials for Energy Conversion, and Hefei National Laboratory for Physical Science at the Microscale, University of Science and Technology of China, China
Ye Xu Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, USA
Qun Ye Department of Chemistry, National University of Singapore, Singapore
Qinghong Yuan Institute of Textiles and Clothing, Hong Kong Polytechnic University, Hong Kong
Xiao Cheng Zeng Department of Chemistry, University of Nebraska-Lincoln, USA
Wenhua Zhang Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, China
Xiuyun Zhang Institute of Textiles and Clothing, Hong Kong Polytechnic University, Hong Kong
Yuliang Zhao Key Laboratory for Biomedical Effects of Nanomaterials and Nanosafety, Institute of High Energy Physics, Chinese Academy of Sciences, China
Zhen Zhou Tianjin Key Laboratory of Metal and Molecule Based Material Chemistry, Key Laboratory of Advanced Energy Materials Chemistry (Ministry of Education), Computational Centre for Molecular Science, Institute of New Energy Material Chemistry, Nankai University, China

Preface

The book before you is about the chemistry of graphene from theoretical perspectives. The sp2 carbon and its various manifestations are dear to all chemists’ hearts. Graphene is no exception. No doubt, graphene is a new wonder material. Since its isolation in 2004, graphene has rapidly risen to be one of the hottest stars for various disciplines of basic and applied sciences due to its many exciting unusual characteristics. Over 8000 papers related to graphene were published in 2012, and graphene keeps occupying the headlines of scientific news media.

As stated by John Dewey, “Every great advance in science has issued from a new audacity of the imagination.” The discovery of graphene was a strong proof. In 1947, Canadian theorist Philip Russell Wallace predicted the relativistic behavior of electrons of graphene using the tight-binding approximation, though no one believed then that such a monolayer could exist. The groundbreaking experiments on realizing graphene by mechanical cleavage in 2004 totally changed our minds, and led to the Nobel Prize for Physics in 2010 being given to Andre Geim and Konstantin Novoselov. This path immediately reminds us of the history of fullerenes, especially C60, which was theoretically predicted by Eiji Osawa 1970, experimentally realized in 1985, and won Richard Smalley, Robert Curl and Harold Kroto the Nobel Prize for Chemistry in 1996.

Chemistry will play an increasingly important role in realizing graphene’s potentials, as synthesizing targeted graphene nanosystems, scaling up the synthesis, controlling defects, introducing functional groups, making composites, and so on, all involve chemistry. This book intends to provide a comprehensive state-of-the-art understanding of graphene chemistry at the atomic level from theoretical perspectives, especially on the structure-property-function relationship. The diverse group of contributors are leading experts and their dedication has made this book possible. Computational and theoretical chemists who have not studied graphene before will find this book useful in giving them an overview of the field. Graduate students in computational nanosciences will find this book particularly helpful in learning how one addresses important problems in an interesting and hot topic. Experimentalists in graphene will benefit from the many concepts and interesting properties predicted here for many novel graphene systems; what’s more, this book has two chapters with a significant experimental portion, which demonstrates how deeper insights can be obtained by joint experimental and theoretical efforts. Even experts in the theoretical studies of graphene will find this book interesting thanks to the diverse topics covered in this book.

Future discoveries, innovation, and development in graphene chemistry will continue to be accelerated by modern theoretical and computational studies. We hope that the readers in both theoretical and experimental communities will enjoy this book, and discover more of the magic power of the sp2 carbon.

Acknowledgements

We thank generous financial support from the funding agencies: the Division of Chemical Sciences, Geosciences, and Biosciences, Office of Basic Energy Sciences, U.S. Department of Energy (D.J.); US Department of Defense and National Science Foundation (Z.C.). We are grateful to Sarah Hall of John Wiley & Sons, Ltd for initiating the idea of this book and working through the book proposal with us; and to Sarah Tilley of John Wiley & Sons, Ltd for helping us deliver this book. We thank all the authors who contributed to this book and the reviewers for their time; and Ms. Adi Shinar for creating the cover image.

1

Introduction

De-en Jianga and Zhongfang Chenb

aChemical Sciences Division, Oak Ridge National Laboratory, USA

bDepartment of Chemistry, Institute for Functional Nanomaterials, University of Puerto Rico, USA

From the breakthrough discovery in 2004 [1], to the award of the Nobel Prize for Physics to Geim and Novosolov in 2010, it took only six years for graphene to reach the pinnacle of scientific research. However, this is not the first time that sp2 carbon has won a Nobel Prize. Remember that Smalley, Kroto, and Curl won the Nobel Prize for Chemistry in 1996 for their discovery of fullerenes in 1985 [2]; only that took 11 years. What's more interesting is what the late Smalley said in his Nobel lecture: “Carbon has this genius of making a chemically stable two-dimensional, one-atom-thick membrane in a three-dimensional world. And that, I believe, is going to be very important in the future of chemistry and technology in general.” We have to admire his foresight of the explosion of interest in graphene 10 years later.

The fact that graphene won the Nobel Prize for Physics also reflects the community's focus on the physics aspect of graphene research. However, any large-scale application of graphene would undoubtedly rely on the chemistry of graphene. The expanding interest in graphene oxide through the Hummers method [3] or chemical-vapor deposition [4] approach to graphene synthesis are just two typical examples. The versatility of chemistry presents endless opportunities in graphene research.

Why do we focus on the theoretical perspectives of graphene chemistry? On one hand, there are books already discussing the experimental aspects of graphene chemistry; on the other hand, graphene provides an ideal proving ground for testing theoretical methods and computational imagination. In addition, sp2 or graphitic carbons are the basis of many important materials, such as carbon fibers for building cars and planes; activated carbons for supercapacitors; and graphite and hard carbons for lithium-ion batteries. Understanding graphene chemistry would also lay a foundation of understanding of complex carbonaceous materials. Therefore, the aim of this book is to deliver a comprehensive view of graphene chemistry from various theoretical and computational perspectives.

As a truly two-dimensional system, the honeycomb lattice of graphene has given rise to many interesting physical properties. However, no size is infinite in the real world and we eventually come to the edge of the graphene sheet just like the vast ocean greeting the shore line. Thus, we can expect that edge geometry will have a profound effect on the π-electronic structure.

A chemist relates to graphene by thinking about benzene: graphene is nothing but fused benzene rings. The geometric character is the same: each carbon atom has sp2 hybridization and contributes one 2pz electron for π bonding. However, when contrasting the electronic structure of benzene with that of graphene, we can immediately see the difference: the benzene molecule has a large HOMO-LUMO gap (Figure 1.1), while graphene is a zero-gap semiconductor where the conduction band and the valence band touch at one point at the Fermi level (Figure 1.2). How does the electronic structure evolve from a large-gap six-membered ring to a zero-gap lattice of infinite number of fused rings? This is a rather intriguing question. It turns out that the chemical details matter. Let's take acenes, or linearly fused benzene rings, as an example. Quite a few theoretical papers have been devoted to examining the evolution of the electronic structure with the number of benzene rings in these interesting systems, starting with the earlier studies by Whangbo et al. [5] and Kivelson et al. [6]. In the experimental community, researchers have been trying to synthesize ever longer acenes. The record so far seems to be a nonacene derivative which has nine fused rings as its core [7]. Chapter 2 examines acenes or polyacenes by applying the effective valence bond model and the density-matrix-renormalization-group method, compared to density functional theory (DFT). More often than not, the linearly fused six-membered rings may not be as happy as alternating five-membered and seven-membered rings. This leads to a class of molecules called fused-azulenes or polyazulenes which also forms on the graphene edge due to reconstruction. Chapter 2 addresses this system too.

Figure 1.1 The π-orbitals of the benzene molecule

Figure 1.2 The graphene lattice (left) and its electronic density of states (right) computed using density functional theory

Extending acenes infinitely results in a ribbon with two zigzag edges. The width of the ribbon can also be further increased while preserving the two zigzag edges. What is unique about the zigzag edge is the edge state, as predicted by Fujita et al. [8–9] from the tight-binding method. This pioneering study has inspired many follow-up theoretical investigations and experiments. DFT calculations in particular, revealed that the edge state also possesses a radical-like chemical reactivity [10]. Chapter 4 examines the electronic, mechanical, and electromechanical properties of both zigzag-edged and armchair-edged graphene ribbons.

The uniqueness of the zigzag edge not only manifests itself in ribbons but also in nanographenes. This is fundamentally related to the inherent instability of the zigzag edge. Furthermore, this may be due to the difficulty that π-electrons have in forming localized double bonds since the consecutive zigzag edges do not support bond-length variation well [11]. In contrast, this is not a problem for armchair edges. The geometry-related π-electron distribution is captured by the Clar's sextet rule which seems to be particularly useful in predicting stable nanographenes [12] and ribbons. Chapter 3 seeks to understand aromaticity of graphene and graphene nanoribbons from the perspective of Clar's sextet rule, while Chapter 4 also briefly discusses the electronic structure of nanographenes or finite graphene flakes as the authors call them. Chapter 6 focuses on nanographene exclusively where the authors interrogates C–C bond length variation, orbital energies, and magnetization with the nanographene's size.

A most natural way to relate carbon nanotubes and graphene ribbons is probably to think of unzipping a carbon nanotube to a graphene ribbon. Amazingly, this idea, put forward for fun in 2007 [10] (Figure 1.3), was realized by two experiments two years later through plasma etching [13] and chemical oxidation [14]. Chapter 5 examines the mechanisms of various ways to cut open not only carbon nanotubes, but also graphene itself.

Figure 1.3 Cutting open a carbon nanotube leads to a graphene nanoribbon. Reprinted with permission from [10] © 2007 American Institute of Physics

A straightforward way to utilize the one-atom thickness of graphene is to use it as a membrane, since a membrane's permeance is inversely proportional to its thickness. But a perfect graphene is impermeable to molecules as small as helium [15]. Hence, it is necessary to create holes to empower the graphene sheet for membrane separations; for example, the pore as shown in Figure 1.4 was computationally shown to be highly selective towards H2 [16] and CO2 [17]. More interestingly, this idea of using porous graphene to sieve gas molecules was recently experimentally confirmed through a clever setup [18]. Chapter 7 gives a detailed discussion of how to apply transition state theory to understand porous graphene and graphene nanomeshes for gas and isotope separations.

Figure 1.4 H2 molecule inside a subnanometer pore in the graphene sheet. Electron density contours of both H2 and the porous graphene are shown. Reprinted with permission from [16] © 2009 American Chemical Society

Using Lego bricks, a kid will let the imagination fly and build all sorts of things. Similarly, when given sp2-carbon building blocks, namely, fullerene, carbon nanotubes, and graphene, scientists can assemble them into sp2-hybridized carbon-based superarchitectures, such as fullerene polymers, nanotube clathrates, nanopeapods, nanobuds, nanofunnels, and nanofoams. Chapter 8 reviews the recent efforts in designing the prototypes of such materials and discusses their potential applications in electronics and energy storage.

Doping is an important topic in terms of graphene chemistry, as it is the major approach to opening and tuning the electronic band gap of graphene for device applications, and for modifying the graphene surface to improve reactivity and its interface with other materials for desired applications. Chapter 9 reviews different ways to dope graphene and their resulting changes in graphene's properties, as well as the characterization of doped graphenes and their applications.

Interaction between graphene and a foreign atom, functional group, or molecule is also interesting. From a chemical perspective, this is directly related to functionalization of graphene, a hot topic in itself [19]. From a physical perspective, one immediately thinks about sensing. The preference of π-electron delocalization in graphene dictates that converting a sp2 carbon to sp3 won't be easy. However, this could happen in a pair-wise fashion [20]. Chapter 10 examines in detail the physical adsorption of molecules on graphene, while Chapter 11 focuses on the chemical interaction of functional groups such as –OH with the graphene sheet.

Chemical vapor deposition is the method of choice for large-scale production of high-quality graphene. Various substrates especially copper have been used for CVD growth of graphene. Chapter 12 discusses the mechanistic insights into graphene CVD growth obtained by DFT computations for the nucleation stage and the kinetic Wulff plots for the growth stage.

Graphene oxide is the preferred medium by chemists and materials scientists for manipulating graphene due to its easy preparation and processability [21]. Due to the difficulties in experimentally characterizing the oxygen-containing groups, computational methods are of great help. Chapter 13 discusses the mechanistic insights into oxidation of graphene and reduction of graphene oxide from DFT computation.

Applications of graphene in electronic devices rely on our understanding how the electrons in graphene nanostructures respond to applied potentials. In other words, how do the factors governing the nanographene electronic structure (such as zigzag edges versus armchair edges, doping, boundary shape, etc.) manifest in electronic transport? Chapter 14 reviews recent progress in elucidating the electronic transport of graphene nanoribbons and their assemblies.

Graphene has many applications in energy-related fields, such as batteries [22–23], pseudo-capacitors [24–25] and electrochemical double-layer capacitors [26]. More excitingly, nitrogen doped graphene and carbon nanotubes have been found to be excellent fuel cell catalysts [27]. Chapter 15 covers a variety of topics related to catalysis by graphene, including oxygen reduction reaction, photocatalysis, and CO oxidation. Chapter 16 focuses on hydrogen storage by graphene-based materials.

Chapter 17 and Chapter 18 are unique in this book in that they have a significant experimental portion. This is to show the ever-increasing need to integrate computational insights into experimental discoveries. Chapter 17 is written by experts in synthesis of nanographenes who examine the challenge, strategy, and reward in making novel nanographene molecules of unique electronic and magnetic properties, often predicted by theory. Chapter 18 examines the growth of metal clusters on the moiré structure of graphene on the Ru(0001) surface: both surface science experiments and large-scale DFT calculations are used to understand catalysis in such a model system.

The chapters in this book aim to provide the reader a comprehensive snapshot of our present understanding of graphene chemistry from theoretical perspectives. We hope that both experimental and computational researchers will find reading through the chapters a rewarding experience.

References

1. Novoselov, K. S.; Geim, A. K.; Morozov, S. V.; Jiang, D.; Zhang, Y.; Dubonos, S. V.; et al., “Electric field effect in atomically thin carbon films,” Science, 2004, 306, 666–669.

2. Kroto, H. W.; Heath, J. R.; Obrien, S. C.; Curl, R. F.; and Smalley, R. E., “C-60 – Buckminsterfullerene,” Nature, 1985, 318, 162–163.

3. Hummers, W. S. and Offeman, R. E., “Preparation of graphitic oxide,” J. Am. Chem. Soc., 1958, 80, 1339–1339.

4. Li, X. S.; Cai, W. W.; An, J. H.; Kim, S.; Nah, J.; Yang, et al., “Large-area synthesis of high-quality and uniform graphene films on copper foils,” Science, 2009, 324, 1312–1314.

5. Whangbo, M. H.; Hoffmann, R. and Woodward, R. B., “Conjugated one and two-dimensional polymers,” Proc. R. Soc. London A, 1979, 366, 23–46.

6. Kivelson, S. and Chapman, O. L., “Polyacene and a new class of quasi-one-dimensional conductors,” Phys. Rev. B, 1983, 28, 7236–7243.

7. Purushothaman, B.; Bruzek, M.; Parkin, S. R.; Miller, A. F. and Anthony, J. E., “Synthesis and structural characterization of crystalline nonacenes,” Angew. Chem.-Int. Edit., 2011, 50, 7013–7017.

8. Fujita, M.; Wakabayashi, K.; Nakada, K. and Kusakabe, K., “Peculiar localized state at zigzag graphite edge,” J. Phys. Soc. Jpn., 1996, 65, 1920–1923.

9. Nakada, K.; Fujita, M.; Dresselhaus, G. and Dresselhaus, M. S., “Edge state in graphene ribbons: Nanometer size effect and edge shape dependence,” Phys. Rev. B, 1996, 54, 17954–17961.

10. Jiang, D. E.; Sumpter, B. G. and Dai, S., “Unique chemical reactivity of a graphene nanoribbon's zigzag edge,” J. Chem. Phys., 2007, 126, 134701.

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2

Intrinsic Magnetism in Edge-Reconstructed Zigzag Graphene Nanoribbons

Zexing Qu and Chungen Liu

Institute of Theoretical and Computational Chemistry, School of Chemistry and Chemical Engineering, Nanjing University, China

Graphene, a two-dimensional carbon-based monolayer honeycomb lattice, is considered to be a prospective material for future electronics [1–3]. One-dimensional nano-structure strips of graphene a few nanometers in width, known as graphene nanoribbons (GNR) have been chemically synthesized and studied in laboratory, [4,5] which quickly attracted attention from theorists [4,5].

Zigzag-terminated graphene nanoribbons (ZGNRs) are of particular interest, due to observed room-temperature ferromagnetism as well as indirect evidence of a magnetic edge state, suggesting potential applications for spintronics [2,10–14]. However, numerous theoretical studies on pure and hydrogen-passivated ZGNRs using density functional theory (DFT) methods have predicted an anti-ferromagnetic (AFM) ground state with a minor band gap of approximately several meV between the lowest ferromagnetic (FM) and AFM states [15–18]. It seems that, instead of being an inherent feature of GNRs, room-temperature magnetism could come from easily generated edge or in-body structure defects.

Edge defects, which could shift the edge states from their Fermi energy level (EF), play a critical role in tuning the electronic properties of graphene nanoribbons [17,19–21]. Among them, a novel mechanism is the planar edge reconstructions on zigzag edges, resulted in the appearance of alternating pentagon-heptagon carbon rings on those edges. It is believed that the energy barrier involved in edge reconstruction is less than 1 eV [21]. Such reconstructed structures are usually denoted Rc-ZGNRs. As revealed by density functional theory (DFT) computations, a Rc-ZGNR edge is energetically more favorable by 0.35 eVÅ than a normal zigzag edge [19,22]. The existence of different lengths of alternating pentagon-heptagon structure on ZGNR edges has already been confirmed by aberration-corrected transmission electron microscopy (TEM) observations [23,24].

Furthermore, spin-polarized DFT calculations on one-edge reconstructed ZGNRs indicated an FM ground state, with a finite magnetic moment arising from the opposite (unreconstructed) zigzag edge [19], which supplies a yet to be confirmed theoretical foundation of the ferromagnetism of GNRs, since that the calculated energy gap between the lowest FM and AFM states is too small to maintain a stable magnetic ground state at room temperature [17]. At this stage, the origin of room-temperature magnetism of ZGNRs remains an open problem.

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