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CHEM01200604009 Sreejith Kaniyankandy - Homi Bhabha ...

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155<br />

CHAPTER 6<br />

Charge Separation in CdTe Decorated Graphene<br />

6.1. Introduction<br />

Graphene is a 2-D array consisting of sp 2 hybridized carbon atoms in a honeycomb lattice.<br />

This distinctive structure imparts graphene with a unique linear electronic dispersion near the<br />

K-point of the Brillouin zone [6.1] which leads to relativistic velocity of ~ 10 6 m/s and<br />

mobility of ~15000 cm 2 /Vs for the electrons [6.2]. These unique properties are ideally suited<br />

for application in fast electronic devices like transistors, diodes and oscillators [6.3]. Apart<br />

from these applications, graphene has been exploited for verifying table top quantum<br />

electrodynamics experiments due to its unique electronic structure. Previously, several<br />

groups have verified a number of exotic behaviors like the observation of room temperature<br />

Quantum Hall Effect [6.4], Klein paradox [6.5] etc. These applications and interesting novel<br />

properties of graphene have given impetus to their synthesis by different routes. The first<br />

report on synthesis of graphene was by Geim et al [6.4] who produced graphene by<br />

micromechanical cleavage from highly oriented pyrolitic graphite (HOPG) using a scotch<br />

tape [6.2]. Graphene prepared by micromechanical cleavage was used to verify several novel<br />

attributes of graphene like observation of Klein paradox, Quantum Hall Effect, high mobility<br />

etc. at room temperature. However, from the application point of view, the scotch tape<br />

method is not very conducive due to non scalability.

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