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Scientific Report 2007-2009<br />
Condensed matter physics and biophysics<br />
C34. Design of electronic properties at hybrid organic-inorganic<br />
systems<br />
The appealing optical, magnetic and transport properties<br />
of organometallic materials, the virtually unlimited<br />
choice of organic molecules and the processing flexibility<br />
of molecular films has led to exceptionally rapid progress<br />
in the development of organic devices over the past<br />
decade. Engineering of these devices requires an atomic<br />
level understanding of the parameters that control the<br />
structure and the function of these flexible molecular architectures.<br />
Today, several open questions enliven the<br />
scientific debate, primarily referred to organic/inorganic<br />
interface control (e.g. charge carrier injection, interaction<br />
at the interfaces, metal-semiconductor transition,<br />
spin coupling, etc.). Recent research has focussed on aromatic<br />
oligomers, whose pi-conjugation guarantees charge<br />
delocalization and electron mobility, an important issue<br />
for possible band-transport, and whose typical energy<br />
gaps lie in the visible energy range, with potential application<br />
in novel opto-electronic devices. A crucial issue<br />
for these organic-inorganic systems is the achievement<br />
of long-range order in exotic configurations (twodimensional<br />
arrays, one-dimensional wires) such as to<br />
allow formation of exemplary hybrid structures with peculiar<br />
electronic properties.<br />
at the Fermi level (Fig. 1), as confirmed by highresolution<br />
angular-resolved photoemission (HR-ARUPS)<br />
and ab-initio calculations [1, 2]. The control of the electron/hole<br />
injection barrier has been determined using an<br />
organic buffer single-layer [3], whose mechanisms have<br />
also been explained by a theoretical model valid for a<br />
wide class of organic hetherojunctions[3].<br />
Among the aromatic oligomers, metalphthalocyanines<br />
(MPcs, M-C 32 H 16 N 8 ) are promising<br />
active elements for many optical, electronic and<br />
magnetic applications, and the central metal atom<br />
in MPcs can play a crucial role to establish the electronic/magnetic<br />
properties of the interface. A careful<br />
control of the nature and character of the induced electronic<br />
states at the interface with the metal substrate<br />
is a crucial issue. We have succeded in building-up<br />
highly-ordered MPc arrays on Au(110), and we determined<br />
the energy band diagram by HR-ARUPS (Fig.<br />
2). In particular, by using alkali-metal intercalation we<br />
could tailor the energy gap, adjusting the hole-injection<br />
barrier and observing electron correlation effects due to<br />
the electron-injection into the localised states [4].<br />
Figure 2: CuPc single-layer on Au(110): (left) interface band<br />
dispersion; (right) spectral density of electronic states as a<br />
function of K doping [4].<br />
Figure 1: Pentacene nano-rails grown on Cu(119): (left)<br />
STM image; (right) electronic spectral density of states [1].<br />
Within this appealing research field, in the LOTUS<br />
aboratory we have studied one-dimensional (1D) and<br />
two-dimensional (2D) highly-ordered structures of π-<br />
conjugated molecules assembled on single crystal metal<br />
surfaces, presenting nanometer-scale patterning. Wellordered<br />
nano-rails of pentacene (C 22 H 14 ) have been<br />
grown on the Cu(119) vicinal surface, whose electronic<br />
structure shows an enhanced density of electronic states<br />
The control of the spin coupling of MPc molecules<br />
with a central magnetic atom with the underlying metal<br />
substrate can give rise to enhanced magnetic moments,<br />
with new 1D and 2D architectures for the fabrication of<br />
molecular spintronic devices. Objective of the on-going<br />
work is the study of MPcs formed by a magnetic<br />
central atom that can be used as chemical ”cage”<br />
for anchoring the magnetic ion to a metal surface,<br />
so that the spin-state of the central atom could couple<br />
with the underlying magnetic or non magnetic metal.<br />
References<br />
1. A. Ferretti, et al., Phys. Rev. Lett. 99, 046802 (2007).<br />
2. M. Chiodi, et al., Phys. Rev. B 77, 115321 (2008).<br />
3. M.G. Betti, et al., Phys. Rev. Lett. 100, 027601 (2008).<br />
4. A. Calabrese, et al., Phys. Rev. B 79, 115446 (2009).<br />
Authors<br />
M.G. Betti, C. Mariani, P. Gargiani<br />
http://server2.phys.uniroma1.it/gr/lotus/index.htm<br />
<strong>Sapienza</strong> Università di Roma 87 Dipartimento di Fisica