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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

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