A single layer of bismuth deposited on the Cu(100) surface forms long range ordered structural phases at various Bi density. A highly ordered c (2×2) reconstruction is accomplished at 0.5 ML, further Bi deposition induces a c (92×2) R45° structure and a subsequent p (10×10) phase related to the formation of regular dislocations arrays. The transition from a c (2×2) superstructure to the c (92×2) R45° phase is accompanied by a sudden decrease in the work function. Photoemission measurements reveal that the Bi induced states close to the Fermi level, associated to the c (2×2) phase, are strongly quenched when the arrays of dislocations are formed, while at higher binding energies, they undergo an energy shift probably due to a confinement effect. The low-energy single particle excitations and the electron dispersion of the Bi induced states of the c (2×2) phase are compared to the electronic states deduced by theoretical band structure obtained by ab initio calculation performed within the embedding method applied to a realistic semi-infinite system. © 2010 American Institute of Physics.
Gargiani, P., Izzo, M., Bussolotti, F., Betti, M., Achilli, S., Trioni, M. (2010). Bi ordered phases on Cu(100): periodic arrays of dislocations influence the electronic properties. THE JOURNAL OF CHEMICAL PHYSICS, 132(17), 174706-174711 [10.1063/1.3424741].
Bi ordered phases on Cu(100): periodic arrays of dislocations influence the electronic properties
ACHILLI, SIMONA;
2010
Abstract
A single layer of bismuth deposited on the Cu(100) surface forms long range ordered structural phases at various Bi density. A highly ordered c (2×2) reconstruction is accomplished at 0.5 ML, further Bi deposition induces a c (92×2) R45° structure and a subsequent p (10×10) phase related to the formation of regular dislocations arrays. The transition from a c (2×2) superstructure to the c (92×2) R45° phase is accompanied by a sudden decrease in the work function. Photoemission measurements reveal that the Bi induced states close to the Fermi level, associated to the c (2×2) phase, are strongly quenched when the arrays of dislocations are formed, while at higher binding energies, they undergo an energy shift probably due to a confinement effect. The low-energy single particle excitations and the electron dispersion of the Bi induced states of the c (2×2) phase are compared to the electronic states deduced by theoretical band structure obtained by ab initio calculation performed within the embedding method applied to a realistic semi-infinite system. © 2010 American Institute of Physics.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.