Growth and electron quantization of metastable silver films on Si(001) - art. no. 125325

Citation
I. Matsuda et al., Growth and electron quantization of metastable silver films on Si(001) - art. no. 125325, PHYS REV B, 6312(12), 2001, pp. 5325
Citations number
46
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
01631829 → ACNP
Volume
6312
Issue
12
Year of publication
2001
Database
ISI
SICI code
0163-1829(20010315)6312:12<5325:GAEQOM>2.0.ZU;2-W
Abstract
The growth morphology and the electronic structures of thin metastable Ag f ilms grown on the Si(001)2 x 1 surface at low temperatures are investigated by scanning tunneling microscopy and angle-resolved photoemission spectros copy using synchrotron radiation. The morphology of Ag films exhibits a str ong thickness and temperature dependence indicating an intriguing growth me chanism. The as-deposited film at similar to 100 K is composed of nanoclust ers with flat tops in a uniform quasi-layer-by-layer film at 2-3 ML and of homogeneous clusters having more three-dimensional (3D) character above sim ilar to5 ML. By subsequent annealing at 300-450 K, flat epitaxial Ag(111) f ilms are formed at a nominal coverage larger than 5 ML, while a percolating network of 2D islands is formed at a lower coverage. For the optimally ann ealed epitaxial films, discrete Ag 5s states are observed at binding energi es of 0.3-3 eV together with the Ag(111) surface state. The discrete electr onic states are consistently interpreted by a standard description of the q uantum-well states (QWS's) based on phase-shift quantization. No such well- defined QWS is observed for the films with a coverage less than similar to5 ML. The phase shift, the energy dispersion, and the thickness-versus-energ y relation of the QWS's of the epitaxial Ag(111) films are consistently der ived. The QWS's in photoemission spectra show two distinctive types of the photon-energy dependence in their binding energies; the oscillatory shifts for h v= 5-15 eV and no such shift at hv =20-25 eV. This can be explained i n terms of the different final states in the photoemission process.