Photonic crystals in biology
Photonic crystals in biology
Photonic crystals in biology
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Poster Session, Tuesday, June 15<br />
Theme A1 - B702<br />
Morphological and electronic properties of Moiré patterns on graphene<br />
and graphitic layers on HOPG<br />
1 , Tansu Ersoy 1 and 1 *<br />
1 stanbul Technical University, Department of Physics, Maslak, 34469, stanbul, Turkey<br />
Abstract - Super periodicities can be observed upon shift<strong>in</strong>g of similar periodic structures on each other. Such structures are named as Moiré<br />
patterns. When a graphene layer compos<strong>in</strong>g the highly oriented pyrolytic graphite (HOPG) crystal is slightly moved from its orig<strong>in</strong>al position<br />
hexagonal or l<strong>in</strong>ear super periodicities form. We <strong>in</strong>vestigate the ways to produce these patterns on HOPG <strong>crystals</strong> and study their physical<br />
properties us<strong>in</strong>g scann<strong>in</strong>g tunnel<strong>in</strong>g microscopy and spectroscopy.<br />
Graphite is a widely used and taken for guaranteed<br />
material <strong>in</strong> daily life as solid lubricant or as pencil. Its<br />
derivatives (such as highly oriented pyrolytic graphite<br />
(HOPG)) are also used extensively <strong>in</strong> advanced scientific<br />
studies such as calibration samples for scann<strong>in</strong>g<br />
tunnel<strong>in</strong>g microscopy (STM) systems or also as <strong>in</strong>ert<br />
substrates for <strong>in</strong>vestigation of nano scale structures. It is<br />
so much popular <strong>in</strong> surface science because it has quite a<br />
smooth surface. HOPG is composed of stacked two<br />
dimensional hexagonal lattices with carbon atoms,<br />
popularly named as graphene layers (figure.1). However,<br />
this property may disturb that almost perfect smoothness.<br />
(a)<br />
(b)<br />
(a)<br />
(b)<br />
Figure 2. (a) Moire pattern due to two slightly rotated, 2D<br />
hexagonal lattices. (b) STM image of a graphene flake on HOPG<br />
surface show<strong>in</strong>g Moire pattern (I=0.8nA, V=1.3V, size 91 nm x<br />
91 nm).<br />
Figure 1. (a) HOPG crystal model show<strong>in</strong>g graphene layers. (b)<br />
STM image of HOPG (I=0.7nA, V=60mV, size 3.2 nmx 3.2 nm).<br />
Atoms <strong>in</strong> the graphene layers are strongly bonded but the<br />
layers are not bonded so strongly with each other. That is why<br />
it is easy to exfoliate one atom thick graphene layer from the<br />
HOPG surface even with sticky tape. Additionally, the layers<br />
can shift on each other creat<strong>in</strong>g local Moiré patterns.<br />
When a graphene layer is placed on a regular HOPG surface<br />
with a slight shift/rotation from its expected position or some<br />
broken graphene layer is replaced on the HOPG surface,<br />
Moiré patterns due to the hexagonal lattice may form<br />
(figure.2a) [1,2]. These patterns on HOPG surfaces can be<br />
observed us<strong>in</strong>g scann<strong>in</strong>g tunnel<strong>in</strong>g microscopy (STM).<br />
We use scann<strong>in</strong>g tunnel<strong>in</strong>g microscopy and spectroscopy<br />
(STM and STS) to observe morphological and electronic<br />
properties of graphene Moiré patterns on HOPG. There are<br />
several methods mentioned <strong>in</strong> the literature for produc<strong>in</strong>g<br />
these patterns on HOPG surfaces but the methodology is not<br />
well established. Moreover, <strong>in</strong> our study we <strong>in</strong>vestigate the<br />
types of the patterns (with respect to their periodicities and<br />
shapes (hexagonal or l<strong>in</strong>ear)) and look for certa<strong>in</strong> selection<br />
rules as there are <strong>in</strong>f<strong>in</strong>itely many possibilit ies for the<br />
periodicities. Also the correlation between the patterns and the<br />
procedures applied to atta<strong>in</strong> those patterns are looked upon.<br />
Furthermore, we <strong>in</strong>vestigate the effect of these patterns on the<br />
local electronic structure due to the change <strong>in</strong> the surface<br />
periodicities.<br />
*Correspond<strong>in</strong>g author: 2Tgurlu@itu.edu.tr<br />
[1] . BW<strong>in</strong>g-Tat Pong and Colm Durkan (2005), J. Phys. D: Appl.<br />
Phys. 38 R329–R355.<br />
[2] Yongfeng Wang, Y<strong>in</strong>gchun Ye and Kai Wu (2006) , Surface<br />
Science 600 pp.729–734.<br />
6th Nanoscience and Nanotechnology Conference, zmir, 2010 391