50 research outputs found
Crystallization of phosphorus-doped amorphous silicon films prepared by glow discharge decomposition of silane
Crystallization kinetic of phosphorus-doped amorphous silicon films prepared by glow discharge of silane is observed by using conductivity measurements. The activation energy Ev of the growth rate V g is deduced as a function of doping level Cp (ranging from 0.05 to 5 %). Ev has a constant value equal to 3 eV for Cp ≤ 0.5 % and increases for higher values of Cp. We compare these results with Csepregi et al.'s ones, obtained by channeling. They obtain Ev equal to 2.4 eV in the whole doping level range.La cristallisation dans le silicium amorphe dopé au phosphore, et obtenu par décomposition de silane, a été observée en utilisant les mesures de conductivité électrique. Ceci nous a permis d'obtenir l'énergie d'activation E v de la vitesse de croissance Vg en fonction de la concentration du dopage Cp (variant de 0,05 à 5 %). On trouve une énergie Ev égale à 3 eV pour Cp ≤ 0,5 %. Cette énergie augmente pour des concentrations de dopage supérieures. Ces résultats sont comparés avec ceux obtenus par Csepregi et al. en utilisant la méthode de canalisation. Ils obtiennent une énergie Ev indépendante du dopage et égale à 2,4 eV
Effect of the hydrogen dilution on the local microstructure in hydrogenated amorphous silicon films deposited by radiofrequency magnetron sputtering
The nature of the hydrogen bonding and content and their influence on the film
microstructure have been investigated in detail, as a function of the H2 dilution and the
residual pressure, in hydrogenated amorphous silicon (a-Si:H) films prepared by
radiofrequency (rf) magnetron sputtering at a common substrate temperature (~ 250 °C) and
pressure (5 × 10−4 torr) and high rates (11−15 Å/s). H2 percentages in the gas phase
mixture (Ar + % H2) of 5, 10, 15 and 20% have been introduced during growth. For the 20% of H2,
two different pressures of 5 × 10−4 and 50 × 10−4 torr were used. A combination of
infrared absorption, optical transmission and elastic recoil detection analysis experiments have been
carried out to fully characterize the samples in their as-deposited state. The results clearly
indicate that for H2 percentage equal to or lower than 15% , the total bonded H content in the
films increases as the H2 percentage increases, and then reaches a saturation value or even
decreases for higher H2 percentage. Moreover, the microstructure is also found to be deeply
affected by the H2 dilution and pressure. In particular, for high H2 percentage (20%) and high
pressure (50 × 10−4 torr), unbounded H as well as polyhydride (Si-H2)n chains, possibly
located in structural inhomogeneities such as voids, are also present in the films in addition to the
isolated monohydride Si-H and polyhydride Si-H2 complexes. As a result, a reduction of the
compactness of the film structure associated with a decrease of the refractive index n is
observed. The optical gap is found to be rather controlled by the total bonded hydrogen
content. The lowest proportion of isolated polyhydride Si-H2 complexes and the highest
density are observed for films deposited with 10% of H2 in the gas phase and a pressure of
5 × 10−4 torr
A THEORETICAL STUDY OF HYDROGEN EXODIFFUSION IN a-Si : H, COMPARISON WITH CONDUCTIVITY MEASUREMENTS
Hydrogen evolution in a-Si : H prepared by glow discharge decomposition of silane has been studied previously as a function of annealing temperature, using nuclear reaction, conductivity (σ) and Electron Paramagnetic Resonance (EPR) measurements. Conductivity measurements show the existence of a surface dehydrogenated layer (SDL) for T ⩾ 500 °C. We presented a theoretical kinetic model which takes into account the existence of two kinds of site for hydrogen in the amorphous network : one site is a center from which hydrogen can diffuse, the other is a tightly bound center (corresponding to isolated Si-H bonds). This theoretical model is used here to interpret our conductivity measurements (which are sensitive to the departure of H in the Si-H configuration) for annealing temperatures above 500 °C. This allows us to describe quantitatively the SDL in the same temperature range. We then deduce the thermodynamic parameters which characterize the breaking of the isolated Si-H bond, and the possibility of trapping of a hydrogen by a Si-dangling bond. We obtain the corresponding activation energies respectively equal to 3.3 eV and 4 eV. We thus confirm the value of the Si-H bond energy and give the capture energy of a hydrogen in an isolated Si-dangling bond, which has not been previously determined
Influence of the deposition conditions on the optoelectronic properties of R.F. magnetron sputtered a-Si:H films
We have studied the effect of the deposition conditions on the hydrogen incorporation modes
and content and their effects on the optoelectronic properties of three different series of a-Si:H films
prepared by R.F. magnetron sputtering at high substrate temperature (250 °C)
and high deposition
rates (~ 10Â Ã…/s). We have correlated infrared
absorption measurements with optical transmission
and Photothermal Deflection Spectroscopy (PDS) experiments.
The samples were characterized
successively in their as-deposited state and after annealing at
a temperature around 180 °C. The
results indicate that the modes of H incorporation as well as the hydrogen content in the three series
are completely different from those observed for the samples prepared by Plasma Enhanced Chemical
Vapour Decomposition of pure silane (P.E.C.V.D.) at the same substrate temperature. The
microstructure of the films is also different. The density of deep defects measured in the as-deposited
is slightly higher in the former case. This density decreases
significantly after annealing at 180 °C and
becomes comparable to that obtained for a-Si:H samples prepared
by P.E.C.V.D. at 250 °C at low
deposition rates (~ 1Â Ã…/s), with however a higher disorder in the R.F. sputtered films
STRUCTURAL AND ELECTRONIC PROPERTIES OF CVD SILICON FILMS NEAR THE CRYSTALLIZATION TEMPERATURE
Nous avons examiné les propriétés structurales de
films déposés par C.V.D. dans la gamme de température 600-750°C
avec une attention particulière sur la répartition en volume
des cristaux pour les films déposés autour de la température
de cristallisation. Nous démontrons que le mécanisme général
de cristallisation déterminant la structure est celui de
dépôt de matériau amorphe suivi de cristallisation dans la
phase solide pendant la durée du dépôt. Ce processus dans
la phase solide apparaît par une nucléation prédominante
à l'interface film-substrat. Les implications de ceci sur
la morphologie et les propriétés physiques des films seront
discutées.We have examined the structural properties of
films grown by CVD in the range of temperatures 600-750°C.
with particular emphasis on the volume repartition of
crystals for films deposited around the crystallization
temperature. We find that the general crystallization
mechanism which determines the structure is one of deposition
of an amorphous material followed by subsequent solid phase
crystallization during the deposition time. This solid
phase process occurs through a dominant nucleation at the
film-substrate interface. The implications of this on the
physical properties and morphology of these films will
be discussed
Détermination de la taille et de la concentration de cristallites dans une couche amorphe par mesure de conductivité
On rappelle comment la fraction cristallisée peut être obtenue à partir d'une mesure de conductivité. On montre brièvement comment la vitesse de croissance, la taille et la concentration des cristallites peuvent être déterminés en étudiant la cinétique de cristallisation, suivant que celle-ci est induite en surface ou en volume, dans le cas où il n'y a pas nucléation homogène. On présente des résultats expérimentaux pour des couches de germanium amorphe
Effect of the hydrogen dilution on the short-range and intermediate-range-order in radiofrequency magnetron sputtered hydrogenated amorphous silicon films
Raman spectroscopy experiments correlated with infrared absorption, optical
transmission and photothermal deflection spectroscopy ones are used to
investigate in detail the short-range-order (SRO) and
intermediate-range-order (IRO) in hydrogenated amorphous silicon (a-Si:H)
films elaborated at high rates (~15Â Ã…/s) by radiofrequency
magnetron sputtering with various hydrogen dilution percentage (5 to
20%), leading to different hydrogen-related microstructure and content.
The analysis of the transverse optic (TO)- and transverse acoustic (TA)-like
modes of the Raman spectra indicates that both, the SRO and IRO are more
strongly dependent on the nature of hydrogen bonding configurations, namely
the relative proportion of polyhydride Si-H2 and (Si-H2)n
complexes and/or clustered monohydride (Si-H)n groups incorporated in
the films, rather than on the total bonded hydrogen content. The increase
observed in the line width of the TO- and TA-like modes are well correlated
with that of the disorder parameter E0, also called Urbach edge
parameter, which is related to the exponential absorption from the valence
band tails states distribution. Moreover, the analysis of the optical
transmission data clearly evidences that the dispersion energy Ed and
the static refractive index n0 are also maximum for films having the
lowest value of E0, suggesting that they exhibit the highest mean
coordination number and compactness respectively, consistent with better SRO
and IRO