A B S T R A C T S FRIDAY, JULY 2 N A N O S E A 2 0 1 0 electron-electron repulsion is approximated by the simple Yukawa potential. The key-quantity in our study is the differential cross- <strong>of</strong> H0, with the corestate empty, to a final state with the core-state occupied and an ejected electron <strong>of</strong> kinetic energy E, within H0 and V is treated as a small perturbation. The tight-binding (TB) calculational scheme allows to select only CVV processes in which either the neutralizing or the ejected electrons, in the initial state, lie within nearest neighbor atomic sites to the core-hole site. Many-body corrections, outside the Fermi's golden rule, are included in a broadening function B(E) containing: (a) a Lorentian component to cope with lifetime effects, (b) a Gaussian function to account for the electron-phonon interaction and (c) an asymmetric broadening function, describing the electron shake-up. The kinetic energy distribution <strong>of</strong> ejected electrons, are taken from literature. Measurements <strong>of</strong> CVV electron emissions from bundles <strong>of</strong> Single Wall CNTs are correctly reproduced by averaging N(E) over a statistical mixture <strong>of</strong> tubes, whose diameters are in the range <strong>of</strong> commercial Bucky papers (Fig. 1). 3 – Conclusion. We used a tight-binding procedure to calculate CVV spectra <strong>of</strong> electron emitted from ideal CNTs; manybody electron correlations have been included in a broadening function whose asymmetric component is to be ascribed to the non negligible role <strong>of</strong> shake-up electrons. This result has confirmed the validity <strong>of</strong> the analysis proposed in Ref.[3], where shake-up effects have been isolated in ion-induced Auger electron emission from Aluminum and in X-ray photoemission spectra from CNTs . References [1] J.J. Lander, Phys. Rev. 91 (1953) 1382; H.D. Hagstrum, Inelastic Ion-Surface Collisions, (Ac.Press, NY, 1977), 1. [2] C.-O. Almbladh, A. L. Morales, and G. Grossmann, Phys. Rev. B 39 (1989), 3489; C.-O. Almbladh and A. L. Morales, ibid. 39 (1989), 3503; C.-M. Liegener, Phys. Rev. B 43, 7561 (1991); M. Cini, Solid State Commun. 24 (1977), 681; Phys. Rev. B 17 (1978), 2788. [3] A. Sindona, R.A. Baragiola, G. Falcone, A. Oliva, P. Riccardi, Phys. Rev. A 71, 052903 (2005); A. Sindona, S.A. Rudi, S. Maletta, R.A. Baragiola, G. Falcone, P. Riccardi, Surf. Sci. 601, 1205 (2007); A. Sindona, F. Plastina, A. Cupolillo, C. Giallombardo, G. Falcone and L. Papagno, Surf. Sci., 601, 2805 (2007). [4] G.D. Mahan, Phys. Rev. 163, 612 (1967); P. Nozieres and C.T. De Dominicis, Phys. Rev. 178, 1097 (1969); K. Othaka and Y. Tanabe, Rev. Mod. Phys. 62, 929 (1990). [5] E. Perfetto et al., Phys Rev B 76, 233408 (2007). 9H50-10H10 High photoconductivity in carbon nanotube sheets. V. Grossi, S. Santucci and M. Passacantando (Dipartimento di Fisica, Università degli Studi dell'Aquila, Via Vetoio 10, I-67100 Coppito (L'Aquila), Italy). valentina.grossi@aquila.infn.it, sandro.santucci@aquila.infn.it, maurizio.passacantando@aquila.infn.it 1 – Introduction Photocurrent measurements derived by light excitation have been reported in different configurations exploiting carbon nanotubes (CNTs) [1]. Photoresponse in macro-bundles <strong>of</strong> multi-walled carbon nanotubes (MWCNTs) has been recently observed [2], and a technologically promising high photon-to-current conversion has been demonstrated for MWCNTs by means <strong>of</strong> an electrochemical method [3]. Studies on large area sheets <strong>of</strong> MWCNTs grown on sapphire substrate [4] using also pulsed laser beams [5] may provide us opportunities for constructing smart structures with multiple functionalities. 2 – Abstract 133
A B S T R A C T S FRIDAY, JULY 2 N A N O S E A 2 0 1 0 CNTs have been synthesised at 750 °C by thermal chemical vapour deposition (CVD) <strong>of</strong> acetylene (C2H2) gas, in ammonia (NH3) atmosphere, onto SiO2/Si(100) substrates with nickel (Ni) catalyst nanoparticles. A Ni thin film (3 nm) has been deposited by thermal evaporation onto a masked substrates (100 nm <strong>of</strong> SiO2 grown onto a silicon (100) wafer) in order to obtain four single rectangular Ni strips <strong>of</strong> different length. CNTs are grown only onto the Ni strips. Gold rectangular electrodes have been evaporated on the ends <strong>of</strong> each strip overlapping the nanotubes for about 1 mm. This device has been used in order to investigate the photoconductivity properties <strong>of</strong> MWCNTs under white light and different radiation in the visible region. It has been observed that the dark current versus bias voltage characteristics <strong>of</strong> each strip have an Ohmic behaviour, and the presence <strong>of</strong> continuous white light illumination, as well as monochromatic radiation, induces a photocurrent in each strip. The photocurrent has been generated by illuminating either the whole device surface with white light or a small part <strong>of</strong> the CNT strips with a laser spot. We have obtained a current <strong>of</strong> few mA in a narrow range <strong>of</strong> bias voltages -1
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