G. Pavia
STMicroelectronics
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Featured researches published by G. Pavia.
Applied Physics Letters | 2003
A. Armigliato; Roberto Balboni; Gianpietro Carnevale; G. Pavia; D. Piccolo; Stefano Frabboni; Alessandro Benedetti; A. G. Cullis
A method of obtaining quantitative two-dimensional (2D) maps of strain by the convergent beam electron diffraction technique in a transmission electron microscope is described. It is based on the automatic acquisition of a series of diffraction patterns generated from digital rastering the electron spot in a matrix of points within a selected area of the sample. These patterns are stored in a database and the corresponding strain tensor at each point is calculated, thus yielding a 2D strain map. An example of application of this method to cross-sectioned cells fabricated for the 0.15 μm technology of flash memories is reported.
Applied Physics Letters | 2007
Alessandro Molle; C. Wiemer; Md. Nurul Kabir Bhuiyan; G. Tallarida; M. Fanciulli; G. Pavia
Thin crystalline films of Gd2O3 are grown on an atomically flat Ge(001) surface by molecular beam epitaxy and are characterized in situ by reflection high energy electron diffraction and x-ray photoelectron spectroscopy, and ex situ by x-ray diffraction (XRD), atomic force microscopy (AFM), and transmission electron microscopy. The first stage of the growth corresponds to a cubic (110) structure, with two equiprobable, 90° rotated, in-plane domains. Increasing the thickness of the films, a phase transition from cubic (110) to monoclinic (100) oriented crystallites is observed which keeps the in-plane domain rotation, as evidenced by XRD and AFM.
Micron | 2000
A. Armigliato; Roberto Balboni; S Balboni; Stefano Frabboni; A. Tixier; Gianpietro Carnevale; P. Colpani; G. Pavia; A. Marmiroli
The convergent beam electron diffraction technique (CBED) of the transmission electron microscopy (TEM) has been employed to determine the strain distribution along a cutline parallel to the padoxide/Si interface in a 0.80 micron wide recessed-LOCOS structure. The values of the components of the strain tensor so obtained have been compared with those computed by two simulator codes. It has been found that both the LOCOS morphology and the strain distribution deduced from TEM images and TEM/CBED patterns, respectively, were in agreement with the simulation results, if some oxidation-related parameters were modified.
Journal of Physics: Condensed Matter | 2002
I. Mica; Maria Luisa Polignano; Gianpietro Carnevale; P Ghezzi; M Brambilla; F. Cazzaniga; M Martinelli; G. Pavia; E Bonera
In this paper, the correlation between dislocation density and transistor leakage current is demonstrated. The stress evolution and the generation of defects are studied as a function of the process step, and experimental evidence is given of the role of structure geometry in determining the stress level and hence defect formation. Finally, the role of high-dose implantations and the related silicon amorphization and recrystallization is investigated.
Applied Physics Letters | 2003
C. Wiemer; M. Fanciulli; B. Crivelli; G. Pavia; M. Alessandri
The evolution of the morphology and of the crystallographic ordering of hafnium aluminates deposited by atomic layer deposition has been investigated. Annealing at temperatures as high as 900 °C in N2 or O2 atmosphere is found to promote crystallization of the high-κ layer, together with the growth of an interfacial low-κ oxide. The crystallographic phase has been identified by indexation of transmission electron microscopy selected area diffraction patterns and by Rietveld refinement of grazing incidence x-ray diffractograms. The high κ is found to crystallize in an orthorhombic ternary Hf1−xAlxO2 phase even for an Al content as high as x=0.74. The temperature of crystallization is higher for the Al-richer alloy. The thickness and the electronic density of the interfacial layer are evaluated by combining cross-sectional transmission electron microscopy and x-ray reflectivity analysis.
Applied Physics Letters | 1999
Leo Miglio; M. Iannuzzi; M. Celino; R. Pastorelli; C. E. Bottani; A. Sabbadini; G. Pavia
In this letter, we show that the polymorphic C49 form of TiSi2 has much smaller elastic constants than those of the C54 bulk-stable structure and that its melting temperature is about 300 °C lower. These issues supply intriguing hints in explaining the kinetic advantage of the C49 over the C54 phase and in understanding the role of the elastic energy in the phase transformation from C49 to C54.
Materials Science and Engineering B-advanced Functional Solid-state Materials | 1998
Maria Luisa Polignano; C Bresolin; G. Pavia; V Soncini; F Zanderigo; G. Queirolo; M. Di Dio
Abstract In this work the use of lifetime techniques in the presence of a non-uniform profile of recombination centers is discussed. It is shown that measurements with different probing depths can be used in order to obtain information about the in-depth distribution of recombination centers. Molibdenum was chosen for this study, because it is probably the most common slowly diffusing contaminant. In this study, it is also shown that molibdenum inactivation does take place by segregation at the wafer surface. The evidence from lifetime techniques is confirmed by TEM analyses, revealing tiny molibdenum clusters at the wafer surface.
Journal of Applied Physics | 2006
A. Armigliato; Alessio Spessot; Roberto Balboni; Alessandro Benedetti; Gianpietro Carnevale; Stefano Frabboni; Gianfranco Mastracchio; G. Pavia
The deformation induced onto silicon by the formation of Ti self-aligned silicides (salicides) in shallow trench isolation structures has been investigated by the convergent beam electron diffraction technique (CBED) in the transmission electron microscope (TEM). The splitting of the high order Laue zone (HOLZ) lines in the CBED patterns taken in TEM cross sections close to the salicide/silicon interface has been explained assuming that the salicide grains induce a local bending of the lattice planes of the underlying matrix. This bending, which affects in opposite sense the silicon areas below adjacent grains, decreases with the distance from the interface, eventually vanishing at a depth of 300–400nm. The proposed strain field has been implemented into a fully dynamical simulation of the CBED patterns and has proved to be able to reproduce both the asymmetry of the HOLZ line splitting and the associated subsidiary fringes. This model is confirmed by the shift of a Bragg contour observed in large angle C...
Applied Physics Letters | 2006
Claudia Dallera; F. Fracassi; L. Braicovich; G. Scarel; C. Wiemer; M. Fanciulli; G. Pavia; Bruce C. C. Cowie
The authors present novel results on the interface between silicon and the high-κ oxides Al2O3 and HfO2 grown by atomic layer deposition. The determination of the thickness of the interfacial layer between oxide and Si(100) is crucial to the evaluation of the performances of devices based on high-κ dielectrics. They find through hard x-ray photoemission spectroscopy (HaXPES) that no interfacial layer forms between Al2O3 and Si(100) whereas almost one monolayer forms between HfO2 and Si(100). HaXPES does not involve any destructive procedure nor any sample preparation. High-energy photoemission could therefore be widely employed for the characterization of real devices.
Microelectronic Engineering | 2003
C. Wiemer; G. Tallarida; E Bonera; E Ricci; M. Fanciulli; Gianfranco Mastracchio; G. Pavia; S Marangon
Cobalt silicide films have been prepared by rapid thermal annealing of cobalt layers sputter deposited on silicon substrates. We report on the evolution of silicide phases, surface and interface roughness as a function of the annealing temperature and silicon surface preparation. The characterizations are carried out by atomic force microscopy, X-ray diffraction, X-ray reflectivity, Raman spectroscopy, and transmission electron microscopy. The cleaning procedure of the silicon substrate affects the interface roughness and the silicide thickness, whereas little effects are found on the surface. On the other hand, surface roughness increases with annealing temperature.