103 12 Semantic Scholar is a free, AI-powered research tool for scientific literature, based at the Allen Institute for AI. 0000002398 00000 n �L"�� >�DT��)bP���4� ��A�)6�N�� � *�"�)�pT@�K��W�v�!�)C�l��=*��6��2��B�N�”~�xh�p�� Electrons in solids 3. Wowever, this does not apply to electrons travelling in graphene – in some circum] stances they move ahead as if the barrier did not even exist. 0000002321 00000 n n�3ܣ�k�Gݯz=��[=��=�B�0FX'�+������t���G�,�}���/���Hh8�m�W�2p[����AiA��N�#8$X�?�A�KHI�{!7�. Brief history of carbon 2. Re°ectance and transmittance of graphene in the optical region are analyzed as a function of frequency, temperature, and carrier density. One result of this special dispersion relation, is that the quantum Hall effect becomes unusual in graphene, see . �A�H3�5@� �o�K Carbon nanotube interconnects 8. Some features of the site may not work correctly. 0000001400 00000 n Ideal quantum electronic properties 7. Ideal quantum electronic properties 7. An electron carrying charge through graphene in a Dirac-like fashion acts like a single particle that barely interacts with its many peers. 0000002076 00000 n between graphene and particle physics, which are valid for energies up to approximately 1 eV, where the dispersion relation starts to be nonlinear. Carbon nanotube field effect transistors 9. Carbon nanotube interconnects 8. N'��)�].�u�J�r� trailer Electrons in solids 3. Carbon nanotube and graphene equilibrium properties 6. L.D. <<0275215ae0944646a08d1f02c9df4bc1>]>> �ꇆ��n���Q�t�}MA�0�al������S�x ��k�&�^���>�0|>_�'��,�G! You are currently offline. 0000001286 00000 n The discussion of graphene’s electronic properties and how such relativistic effects are revealed in electric transport xref endstream endobj 104 0 obj<> endobj 106 0 obj<> endobj 107 0 obj<>/Font<>/ProcSet[/PDF/Text]/ExtGState<>>> endobj 108 0 obj<> endobj 109 0 obj[/ICCBased 113 0 R] endobj 110 0 obj<> endobj 111 0 obj<> endobj 112 0 obj<>stream H���yTSw�oɞ����c [���5la�QIBH�ADED���2�mtFOE�.�c��}���0��8�׎�8G�Ng�����9�w���߽��� �'����0 �֠�J��b� We show that the optical graphene Survey of major applications of carbon nanotubes. "F$H:R��!z��F�Qd?r9�\A&�G���rQ��h������E��]�a�4z�Bg�����E#H �*B=��0H�I��p�p�0MxJ$�D1��D, V���ĭ����KĻ�Y�dE�"E��I2���E�B�G��t�4MzN�����r!YK� ���?%_&�#���(��0J:EAi��Q�(�()ӔWT6U@���P+���!�~��m���D�e�Դ�!��h�Ӧh/��']B/����ҏӿ�?a0n�hF!��X���8����܌k�c&5S�����6�l��Ia�2c�K�M�A�!�E�#��ƒ�d�V��(�k��e���l ����}�}�C�q�9 endstream endobj 113 0 obj<>stream 0 Physics and Applications of Graphene - Theory. Graphene Electronic Structure 1s (2 states) 2s,2p (8 states) 3s,3p,3d (18 states) sp 2 bonding π orbital (┴to plane)derived from p z σ orbital (in plane) derived from s, p Edited by: Sergey Mikhailov. Ideal quantum electronic properties 7. 0000000016 00000 n 2y�.-;!���K�Z� ���^�i�"L��0���-�� @8(��r�;q��7�L��y��&�Q��q�4�j���|�9�� 105 0 obj<>stream Electrons in solids 3. Colloquium: Graphene spectroscopy D. N. Basov and M. M. Fogler Department of Physics, University of California San Diego, 9500 Gilman Drive, La Jolla, California 92093, USA A. Lanzara and Feng Wang Department of Physics, University of California at Berkeley, Berkeley, California 94720, USA d(TV THE NOBEL PRIZE IN PHYSICS 2010 THE ROYAL SWEDISH ACADEMY OF SCIENCES HTTP: //KVA.SE chance of quantum particles passing through. Carbon nanotube interconnects 8. 1. Figure 4. startxref Graphene is therefore an exciting bridge between condensed-matter and high-energy physics, and the research on its electronic properties unites scientists with various thematic backgrounds. Carbon nanotube diodes and capacitors 10. Graphene is famous for its peculiar electronic properties exemplified by the Dirac point, a region in the material’s band structure where electron behavior resembles that of high-energy particles. �k!K�,���O�{�/�o�KYY'�W���h ��I�ɪ���%"(�R�xP�(������k���0j�O$YE1������ j|S�w���}��/�B�-��� ��b���Zl�lٯ�N�ֶ�q�0K�P�'���h�>���e1k|D|-}S�[�tw�����[[��׻q��Ğ�����~�v�v��C�k��OZ��x���ն��+� h�� �x������- �����[��� 0����}��y)7ta�����>j���T�7���@���tܛ�`q�2��ʀ��&���6�Z�L�Ą?�_��yxg)˔z���çL�U���*�u�Sk�Se�O4?׸�c����.� � �� R� ߁��-��2�5������ ��S�>ӣV����d�`r��n~��Y�&�+`��;�A4�� ���A9� =�-�t��l�`;��~p���� �Gp| ��[`L��`� "A�YA�+��Cb(��R�,� *�T�2B-� %PDF-1.4 %���� Brief history of carbon 2. Graphene bandstructure 4. between graphene and particle physics, which are valid for energies up to approximately 1 eV, where the dispersion relation starts to be nonlinear. Carbon nanotube bandstructure 5. Nanoelectronic Devices Based on Carbon Nanotubes, Carbon nanotube electronics: recent advances, Impact of Energy Band Structure on CNTFET Output Characteristics, Carbon Nanotube- and Graphene Based Devices, Circuits and Sensors for VLSI Design, Monte Carlo simulation of electron transport in semiconducting zigzag carbon nanotubes, Electron doping effects on the electrical conductivity of zigzag carbon nanotubes and corresponding unzipped armchair graphene nanoribbons, Single-walled carbon nanotube networks for flexible and printed electronics, Raman spectroscopy and molecular simulation studies of graphitic nanomaterials, Electric Transport in Hybrid Carbon Nanotube-Graphene Devices, California September 2010 © in this web service, This time period has afforded a great many scholars across the globe to conduct a vast amount of research investigating their fundamental properties and ensuing applications, Blog posts, news articles and tweet counts and IDs sourced by, View 24 excerpts, cites methods and background, Finally, after two decades, the knowledge and understanding, By clicking accept or continuing to use the site, you agree to the terms outlined in our, Antibacterial applications of graphene oxides, Brightsurf Science News and Current Events, A new radiation detector made from graphene, Clemson researchers blaze new ground in wireless energy generation, NREL research yields significant thermoelectric performance. Carbon nanotube diodes and capacitors 10. 0000000536 00000 n Carbon nanotube and graphene equilibrium properties 6. ��jw"���,�����Ԗ%(��Yġh�g�`l�L�ˍ��2�Lb�'D�"U>�R =�h����F��� ���@���� �J���h�u0����U3� wt��8 \�4Ĕ�j�h�(5v��� 6VI���آ���p�������9�X �~�C�B���qy�;Ƥ�e�@1A� �e�6�" �zbyn1��E�Ps�r�o�d�4 �V��)g�B�0�i�W��8#�8wթ��8_�٥ʨQ����Q�j@�&�A)/��g�>'K�� �t�;\�� ӥ$պF�ZUn����(4T�%)뫔�0C&�����Z��i���8��bx��E���B�;�����P���ӓ̹�A�om?�W= ��w�G� xR^���[�oƜch�g�`>b���$���*~� �:����E���b��~���,m,�-��ݖ,�Y��¬�*�6X�[ݱF�=�3�뭷Y��~dó ���t���i�z�f�6�~`{�v���.�Ng����#{�}�}��������j������c1X6���fm���;'_9 �r�:�8�q�:��˜�O:ϸ8������u��Jq���nv=���M����m����R 4 � Carbon nanotube bandstructure 5. 0000001071 00000 n Carbon nanotube field effect transistors 9. 103 0 obj<> endobj Carbon nanotube diodes and capacitors 10. %%EOF ���l��bNq]A���V�!l| �����E2� �tPR��*\g ���Ca��Y!Q_KO(����Q���nl�pTF���L�6��U���Ĭ���-. Carbon nanotube and graphene equilibrium properties 6. Carbon nanotube field effect transistors 9. Physics and Mechanics of Graphene Department of Materials Science, University of Patras (Greece) ICE-HT, FORTH, Patras (Greece) Asst. (scotch tape method). 0000005564 00000 n • 2004: Single‐atom‐thick, free‐standing graphene is extracted (by Andre Geim and Konstantin Novoselov, Manchester University, U.K.) • 2005: Anomalous quantum Hall effect was observed • 2010: Nobel prize in Physics for Andre Geim and Konstantin NlNovoselov 1. Figure 4. Kirigami can change the electronic behavior of 2D nanomaterials, and graphene is a prototypical example famous for its interesting low-energy electronic behavior (see the article by Andrey Geim and Allan MacDonald, Physics Today, August 2007, page 35). Figure 2. Graphene bandstructure 4. Synthesis and placement of carbon nanotubes 11. H����n�0��~��dx|�]���T�"�wU�2�#0�m�5*�}k��hI�H���?��rH4^N���F�s��V�] ISBN 978-953-307-152-7, PDF ISBN 978-953-51-4513-4, Published 2011-03-22 Synthesis and placement of carbon nanotubes 11. Prof. Κ. Papagelis FORTH/ICE-HT, November 2012 –2 Graphene: Mother of all graphitic forms Graphene is a flat monolayer of C atoms tightly packed into a 2D honeycomb lattice. 1. Landau Institute for Theoretical Physics, Moscow 119334, Russia Institute of the High Pressure Physics, Troitsk 142190, Russia E-mail: falk@itp.ac.ru Abstract.


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