• 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 Figure 4. You are currently offline. Ideal quantum electronic properties 7. Survey of major applications of carbon nanotubes. Synthesis and placement of carbon nanotubes 11. ��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. Electrons in solids 3. 0000001071 00000 n 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. Re°ectance and transmittance of graphene in the optical region are analyzed as a function of frequency, temperature, and carrier density. �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-� Graphene bandstructure 4. Carbon nanotube bandstructure 5. Physics and Mechanics of Graphene Department of Materials Science, University of Patras (Greece) ICE-HT, FORTH, Patras (Greece) Asst. 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. Brief history of carbon 2. startxref 0000005564 00000 n Synthesis and placement of carbon nanotubes 11. Landau Institute for Theoretical Physics, Moscow 119334, Russia Institute of the High Pressure Physics, Troitsk 142190, Russia E-mail: falk@itp.ac.ru Abstract. Ideal quantum electronic properties 7. 1. trailer 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). The energy, E ��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 L.D. %PDF-1.4 %���� One result of this special dispersion relation, is that the quantum Hall effect becomes unusual in graphene, see . 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 �A�H3�5@� �o�K 0000000016 00000 n H���yTSw�oɞ����c [���5la�QIBH�ADED���2�mtFOE�.�c��}���0��8�׎�8G�Ng�����9�w���߽��� �'����0 �֠�J��b� Electrons in solids 3. "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 Carbon nanotube and graphene equilibrium properties 6. 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 Carbon nanotube diodes and capacitors 10. <<0275215ae0944646a08d1f02c9df4bc1>]>> �����E2� �tPR��*\g ���Ca��Y!Q_KO(����Q���nl�pTF���L�6��U���Ĭ���-.

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