Low-pressure discharges have been used for more than three decades for the synthesis of several types of silicon-based thin-films, especially for applications in the fields of microelectronics, large area electronics, and photovoltaics. Radio frequency, capacitively-coupled plasma enhanced chemical vapor deposition (RF-PECVD) and sputtering, with several variations, have been the most commonly used techniques, due to their high flexibility, but several other types of plasma-assisted techniques have been developed, including the use of inductively coupled plasmas (ICP), hollow cathode/anode plasmas, microwave plasmas, as well as electron cyclotron resonance (ECR) discharges. In this section, the most recent developments of low pressure discharges for silicon-based materials are reviewed, dividing them respect to the type of excitation used to produce the plasma discharge: capacitively-coupled direct current (DC) and radio-frequency (RF), inductively-coupled (ICP) or microwave (MW) discharges, while a separated paragraph is dedicated specifically to the synthesis of polymer-like coatings.
2.1. CCP-DC Discharges
Low-pressure plasma discharges activated by means of a DC bias are usually less expensive compared to the ones activated by a RF bias, since the latter typically require a more expansive generator, as well as the use of a matching network to prevent or limit the reflected power [
10]. However, despite of the lower cost, the use of DC-activated discharges is less common, due to their lower versatility compared to RF ones, and the limitations concerning the use of insulating electrodes, due to the problem of surface charging. Moreover, they typically provide a strong ion bombardment on the substrate and the growing film, which may be detrimental for the film properties in some cases, e.g. by increasing the formation of defects in semiconductor materials.
Despite of their intrinsic limitations, DC discharges are quite often used for the deposition of carbon-based materials, such as diamond-like carbon (DLC) or carbon nanotubes (CNT). In fact, they can provide a high electron energy, which is necessary for the dissociation of gases such as CH
4, with strong molecular bonds, that are often used for the synthesis of these materials. In this context, an interesting study was carried out by Delfani et al. [
11] to investigate the effectiveness of silicon-based thin films such as a-Si:H, a-SiC:H and a-SiN:H, deposited by means of pulsed DC-PECVD, to enhance the adhesion of DLC thin films on steel substrates. The Si-based layers and the DLC coatings were grown in succession in the same deposition chamber by means of a pulsed DC discharge, analyzing especially the effect of substrate temperature on the adhesion strength of the DLC films. The authors found that a-SiN:H films grown a temperatures higher than 150 °C provided the best results in terms of adhesion of the DLC films.
Silicon-based interlayers for carbon based materials were also studied by Lakhonchai and coworkers [
12], who investigated the corrosion resistance of hydrogenated amorphous carbon (a-C:H) thin films grown on chromium-plated substrates, which were coated with a-Si, a-Si:N, a-Si:H and a-SixCy:H layers. In this case the silicon-based layers, as well as the a-C:H films, were grown by means of an hybrid PECVD/DC-
sputtering deposition system, in which Ar, H
2 and C
2H
2 were introduced in different amounts, depending on the material to be grown. In this study, the authors found a better effectiveness of a-Si:H interlayers for improving the adhesion of the carbon-based films, compared to the other silicon-based materials investigated, while the worst behavior was observed for the a-SixCy:H material.
Silicon-carbon hybrid materials show interesting properties for the production of anodes for lithium-ion batteries with enhanced stability, as was recently investigated by Sun and coworkers [
13]. In their study, an
active screen plasma was used for the deposition of SiO
x/C nanostructured materials by dispersing ordered mesoporous carbon (CMK3) on a silicon substrate and then activating a discharge at low pressure in a H
2 atmosphere. According to the active screen process, the DC bias was applied between the chamber walls and an
active screen mesh (ASM), composed by a metal grid that surrounded the substrate. The plasma discharge produced radicals that were able to reach the substrate by diffusing through the ASM, while the ion bombardment impinged on the mesh, that protected the substrate from it. Such a configuration allows to use a DC discharge, while strongly reducing substrate and film damage by the ion bombardment. The process resulted in the formation of nanostructures of different shapes, composed by a mixture of SiO
x and amorphous carbon, that revealed interesting properties for the production of battery anodes.
Silicon-carbon based materials are also suitable for biomedical application, as in the case of the recent studies of Grenadyorov and coworkers [14, 15], who investigated the use of a pulsed DC-PECVD discharge for the synthesis of hybrid a-C:H:SiOx materials onto Ti–6Al–4V alloy substrates. The hybrid deposition system exploited both a pulsed DC generator and a hot filament to achieve the dissociation of the polyphenylmethylsiloxane (PPMS) vapor used as precursor. The grown a-C:H:SiOx layers showed good biocompatibility and adhesion, as well as high wear resistance, making them good candidates for application to biomedical devices.
Plasma spray is a kind of
physical vapor deposition (PVD) technique, often used in applications where thick and porous coatings are required such as in thermal insulation and some kind of biomedical surfaces. In this process, a powder precursor is injected in a flow of plasma, being melted or evaporated and then transported to the substrate, where it typically adhere in the form of
microlamellae. The technique can be carried out at atmospheric or reduced pressure, depending on the application, and the flow of plasma can be excited by a DC or a RF bias. An original type of hybrid DC/RF plasma spray at low pressure was used by Ohta and koworkers [
16] for the production of
silicon nanoparticles (Si NP) intended for use in the fabrication of cathodes for lithium-ion batteries. A considerable production rate of 17 g min
−1 was obtained with optimized conditions, with an average nanoparticle diameter of 50 nm. Plasma spray was also used by Harder [
17] for depositing Si-HfO
2 coatings onto SiC substrates, with the aim to obtain a protection of this materials against oxidation in a steam environment, although the author found that the coatings effectiveness resulted limited.
2.2. CCP-RF Discharges
Low-pressure,
capacitively-coupled radiofrequency (CCP-RF)
discharges are the most common type of applications of cold plasmas, and their use is widespread, due to their versatility. More specifically, the use of RF-PECVD and RF
magnetron sputtering [
10] is very common thanks to the ability of these techniques to grow a large number of materials, including silicon-based ones, on substrates of different types, including plastic materials, and to achieve a good control of the material stoichiometry during the synthesis of alloys. These techniques require the use of RF generators, which are often more expensive than DC ones, and matching networks, which are used to tune the impedance of the load coupled with the generator, in order to minimize the amount of power reflected to it. The use of an RF bias provides a greater versatility, allowing for the deposition on insulating substrates and reducing the amount of ion bombardment on the surface of the substrate and the growing film, which is detrimental in some applications.
The RF-PECVD technique is also called
plasma assisted chemical vapor deposition (PACVD) and usually, if not specified otherwise, involves the use of a capacitively-coupled plasma (CCP) generated by the application of a radiofrequency bias between two planar electrodes. Nonplanar configurations and inductive coupling are also possible, but less common. The most common choice for the excitation frequency is 13.56 MHz, since it is an industrial standard for RF generators and lies between typical electron and ion plasma frequencies, allowing a separation between their behavior [
10]. However, higher frequencies, such as 40 MHz of 75 MHz are also used in order to achieve specific material properties, and in this case the technique is often called
very high frequency PECVD (VHF-PECVD
).
One of the most typical applications of RF-PECVD is the growth of amorphous silicon-based materials [
18], such as a-Si, a-SiO
x, a-SiN
x, a-SiC
x, a-SiO
xC
y, a-SiO
xN
y, and even a-SiC
xO
yN
z [
19], the composition of which can be tuned efficiently by the control of precursor gases concentrations. In recent years, a great interest was dedicated to the application of PECVD techniques for depositing silicon-based amorphous thin films for the passivation of heterojunction photovoltaic cells, which are considered very promising for improving the efficiency of solar energy production devices [20-27]. Hydrogenated amorphous silicon (a-Si:H) is the material which was more intensively studied for this application [20-25], but doped amorphous silicon oxide (a-SiO
x) was also considered [26, 27]. Wang and coworkers [
23] compared the effectiveness of a-Si:H passivating layers grown by PECVD using RF (13.56 MHz) and VHF (40 MHz) plasma excitation frequencies, founding a better performance of the former compared to the latter. VHF excitation (40.68 MHz) was also used by Ruan and coworkers [
20], but in their work it was applied for growing the doped layers of the cell, while the intrinsic a-Si:H passivating layer was grow using standard 13.56 MHz excitation frequency. The groups of Chen and Truong [26, 27] used an hybrid dual-mode PECVD for the deposition of a-SiO
x passivating layers, exploiting the synergistic action of microwaves (2.46 GHz) and radiofrequency (13.56 MHz) excitation in the plasma discharge. Of particular interest is the study of Ouaras and coworkers [
25], who developed a novel type of PECVD reactor with interdigitated electrodes, by which they were able to perform a patterned deposition of a-Si:H on a solar cell of area 156 mm x 156 mm, without the need of a lithographic step.
Silicon-based nanoparticles, as well as nanocrystalline materials, in which nanocrystals are usually embedded in an amorphous matrix, are interesting for several applications, including solar energy production, and PECVD is a very common way to synthesize them. In fact, in recent years, several research groups carried out research studies on the use of RF-PECVD techniques for the synthesis of nanocrystalline silicon-based materials [28-30] and nanoparticle-based materials [31-33]. In most cases, a standard RF-PECVD system with parallel-plates electrodes was used to synthesize the material, but a careful study on the process parameters, especially precursors dilution and power density, was usually required to achieve a good control on the material properties. In the work of Ghosh and coworkers [
31], an a-SiN layer was grown on the rear of PV devices, and SiN nanoparticles were subsequently produced by an hydrogen plasma etching, after which an a-Si:H layer was deposited to embed the SiN nanoparticles.
Microcrystalline and polycrystalline silicon layers were grown by PECVD. Li and coworkers [
34] used a VHF (75 MHz) excitation frequency PECVD system for growing intrinsic mc-Si layers on glass substrates, investigating the effect of deposition rate on the film microstructure. Liu and coworkers [
35] achieved the synthesis of polycristalline silicon thin films on polymeric substrates at a temperature of 100 °C by means of a RF-PECVD system. In order to promote film crystallization, they exploited a variable DC negative bias on the substrate to achieve a tunable ion bombardment. They found that a transition between amorphous and polycrystalline structure was obtained for biases higher than 50 V, and the optimal bias value was obtained at 100 V, over which a degradation of the film structure was observed.
The synthesis of silicon-based ternary compounds is another interesting application of RF-PECVD techniques, which allow for a fine-tuning or the elements incorporation in the material, thanks to the possibility of tuning the amount of precursors radicals in the plasma discharge, by regulating the gas flow rates and the RF power [
18]. Song and coworkers [
36] investigated the growth of silicon-carbon-oxygen amorphous ternary alloys (a-SiC
xO
y), doped with nitrogen, by means of VHF-PECVD, with a specific focus on their photoluminescence properties. Hang and coworkers [
37] studied the growth of silicon-nitrogen-oxygen amorphous ternary alloys by means of standard RF-PECVD, while Ke and coworkers [
38] investigated the deposition of silicon-boron-nitrogen amorphous alloys (a-SiB
zN
y) on steel.
Silicon-based nanowires (NWs) are another material which was effectively grown by means of PECVD techniques. Recently, silica and silicon NWs were grown by Wang and coworkers [
39] using a standard RF-PECVD reactor, after having prepared the substrate with mixed catalyst of Sn and Cu. Silicon-tin NWs were also grown by Azrak and coworkers [
40] using a procedure which included the formation of a silane plasma by means of a RF-PECVD reactor.
Atomic layer deposition (ALD) is a technique which relies on the alternate injection of different precursors in the reaction chamber, exploiting specific and highly selective chemical reactions to form extremely conformal alloy coatings with thickness control at the atomic level. Its variant called plasma enhanced ALD (PEALD) exploits the use of a plasma discharge to produce radicals that are then injected in the reaction chamber to be used in the chemical reactions, increasing the technique versatility. This technique has risen in importance with the continuous increase of complexity of nanodevices, the fabrication of which often requires to cover conformally surfaces with very small features such as pores or spikes, and the deposition of layers with nanometric thickness. Recently, Baranov and coworkers [41, 42] studied the growth of GaP/Si superlattices for photovoltaic applications, using a hybrid deposition process that exploited both standard RF-PECVD and PEALD, in which the plasma was obtained by a radiofrequency, capacitively-coupled discharge. The obtained superlattices resulted of purely crystal structure, without an amorphous phase.
Radio-frequency activated sputtering was used for the deposition of silicon-based materials in recent years. As an example, an interesting study of Zhang and coworkers [
43] studied the incorporation of deuterium in silicon carbide thin films grown by means of a conventional RF sputtering system using an atmosphere of deuterium gas.
A simple O
2 RF plasma activation of 1.4404 stainless steel parts, industry relevant as components of microreactors for the production of PVP in aqueous solution, through a radical polymerization of N-vinylpyrrolidone, was applied [
44] for the deposition of an ultra-thin 1H, 1H, 2H, 2H perfluorooctyltriethoxysilane (FOTS) antifouling coating. If compared to the standard sol-gel method (precursors: FOTS and Zirconium(IV)-acetylacetonate (Zr(acac)
4), the plasma assisted process showed outstanding anti-adhesive properties with almost no PVP-deposit formation on the steel components, though their surface roughness remains higher.
Another comparative study involved (3-aminopropyl)trimethoxysilane (APTMS) [
45] as grafting molecule for a type of cross-linked polyethylene which is produced through the silane method, generally known as organosilane-grafted moisture-crosslinked polyethylene or silane-crosslinked polyethylene (Si-XLPE), compounds that are widely used in the electrical and biomaterials industry and can take advantage from the integration of trifunctional organosilanes, such as APTMS. Indeed, this molecule is capable of polymerizing in the presence of water, which gives rise to a different possible configuration structure based on 2-dimensional and 3-dimensional surface-induced polycondensation, through covalent attachment.
Chemical vapor deposition (CVD) and plasma-facilitated in situ grafting methods (grafting-from and grafting onto) were employed to immobilize APTMS. The reactor for the plasma-assisted processes was a low-pressure plasma system operating at a maximum power of 100W and low frequencies (40-100 kHz). The characteristics of obtained samples with the same main preparation principles were compared with each other, in terms of surface chemistry (XPS, EDX, and ATR-FTIR), morphology (by AFM and FESEM), and wettability (by contact angle measurement), thus showing that plasma grafting-from deposition method favoured the highest attachment of APTMS to the surface, by forming multilayer structures instead of monolayers and leading to the creation of hydrophobic surfaces.
2.3. ICP-RF Discharges
Inductively coupled plasma (ICP) discharges exploit the generation of a time-varying magnetic field, by means of an alternating current flowing in one or more coils, which in turns provides the generation of a variable electric field, able to accelerate electrons and ions to generate a plasma discharge [
10]. Compared to CCP discharges, ICP ones typically provide a higher plasma density and have the advantage to avoid the ion bombardment, due to the absence of sheaths. However, when an ion bombardment is required to achieve specific effects during the process, it can be obtained by adding a DC or RF bias to the sample surface, the intensity of which can be tuned as required. ICP discharges were used in recent years to perform the growth of silicon-based materials by means of PECVD [46, 47], PEALD [48, 49], as well as
sputtering [
50] processes. Rumyantsev et al. [
46] exploited an ICP-PECVD reactor to achieve the synthesis of amorphous hydrogenanated silicon-carbon (a-SiC
x:H) and silicon-carbon-nitrogen (a-SiC
xN
y:H) alloys from examethyldisilazane (and nitrogen for N containing films). Also Yang and coworkers [
47] investigated the use of an ICP-PECVD technique for the synthesis at very low temperature (20 °C) of silicon dioxide and silicon thin-films, using silane (SiH
4) and oxygen as precursor gases, for the fabrication of metal-oxide-semiconductor (MOS) and thin-film-transistor (TFT) devices.
A variant of the PEALD techniques involves the use of ICP for the formation of the required radicals and was recently exploited for the synthesis of silicon nitride and oxinitride as well as silicon dioxide. In fact, Song and coworkes [
48] used a multi-ICP system with seven coils connected in parallel to generate N radicals to be incorporated in SiN and SiCN alloys, while Jung and coworkers [
49] exploited a remote ICP plasma for the growth of SiO
2 layers from bis(tertiary-butylamino) silane (BTBAS) and oxygen.
Takenaka and coworkers [
50] exploited an ICP sputtering system, in which low-inductance antenna (LIA) modules were arranged near rectangular silicon sputtering targets, to produce an intense and homogeneous ion bombardment on them, resulting in the deposition of Si thin films with crystallinity in range 73-78% without intentional substrate heating.
2.4. MW Discharges
The use of microwaves (MW) for the excitation of plasma discharges is usually exploited to achieve a more intense plasma and more energetic electrons, but microwave-assisted techniques are usually more expensive, compared to RF-activated ones. Kim and coworkers [
51] studied the growth of low-resistivity polycrystalline silicon thin-films by means of a PECVD technique activated by MW at 2.45 GHz at a pressure of about 67 Pa in a showerhead reactor, with two different gas injection points: one before the showerehead, where a mixture of Ar and H
2 was injected, and second one downstream of the showerhead, where SiH
4 and PH
3 where inserted near the substrate. A remote-plasma reactor activated by microwaves (2.45 GHz) was used by Wrobek and coworkers [
52] to achieve the deposition of hard a-SiCN coatings at a pressure of 75 Pa using a mixture of aminosilane and silazane precursors. Microwave discharges were also investigated for the synthesis of nanostructures: Wollny and coworkes [
53] exploited a microwave-assisted PECVD reactor for the growth of silicon nanoparticles using a mixture of Ar, H
2 and SiH
4 at a reduced pressure of abut 10 kPa. They also developed a theoretical model to explain the synthesis process. A microwave-assisted technique was also used by Daoudi and coworkers [54, 55] for the deposition from silane of silicon nanoparticles with diameter in range 7-37 nm, which were then decorated by silver nanoprisms.
A particular type of microwave-assisted plasma discharge is the
electron cyclotron resonance (ECR), in which the synergist action of microwaves and a static magnetic field is used to achieve high electron energies. In this kind of discharge, the magnetic field intensity is tuned in such a way that the electron cyclotron frequency equals the microwave frequency, thus allowing resonant absorption of the microwave energy by the plasma electrons [
56] (pp. 492–512.). In recent years, Miller and coworkers [
57] reported an interesting study, regarding the synthesis of terbium-doped silicon oxide (a-SiO
x:Tb) by means of a novel hybrid deposition system, in which the silicon oxide was grown exploiting an ECR plasma of silane and oxygen, while Tb atoms were generated by a magnetron sputtering source located in the same vacuum chamber.
2.6. Plasma Polymerization
Since many decades, the plasma polymerized organic thin films are of great interest and, in particular, the thin organosilicon films can be produced from different precursors/methodologies and aimed to a wide range of applications as multifunctional materials. Low pressure plasma processes based on hexamethyldisiloxane (HDMSO) as a precursor were intensively studied and reviewed few years ago only [
61], thus hereinafter the most recent and peculiar advances will be reported. Kleines and coauthors obtained by MW (2.45 GHz) excitation in a PECVD reactor plasma polymerized ultra-smooth SiOCH coatings deposited on polydimethylsiloxane (PDMS) substrates in order to get membranes [
62] for the control of gas separation. According to process parameters (oxygen carrier to HDMSO monomer ratios and of microwave power input), weaker cross-linking of the siloxane bonds as well as a more organic structure with an increased proportion of bound methyl groups was found advantageous for a high permeability and separation performance of the coatings. Especially for the separation of He and N
2, but also partly for other gas pairings (He/CO
2 and CO
2/N
2), the selectivity for all test points decreased with increasing oxygen content in the process gas. Furtherly, the same authors explored the effect of energy density [
63] on the coated membrane permeation properties by varying over the MW power level as well as the MW pulse duration. They found out the highest permeation and separation performance of the produced layers for the low energy density range of the process, as the low power prevented strong fragmentation of the monomer, which resulted in less dense and cross-linked growth of the layers. Due to the low pulse durations, rearranging processes were suppressed and the layer structure did not become denser due to further energy input. The conclusions were proven through several characterizations: ellipsometry, atomic force microscopy (AFM), X-ray photoelectron spectroscopy (XPS) Fourier Transform InfraRed spectroscopy (FTIR) and Field Emission Scanning Electron Microscopy (FESEM).
The HDMSO precursor was studied also for an opposite scope [
64],
i.e. to produce a SiO
x based barrier coating to atomic oxygen (AO) erosion when deposited on Kapton
® (polyimide) by means of a RF activated plasma discharge by varying the ratio of O
2/Ar in the reactor atmosphere, ranging from a 50 to 1000 W power. Kapton
® is employed in the thermal blankets covering the external surface of spacecraft due to its and thermo-optical properties and durability in harsh environments. By testing it in a coaxial ground-based AO simulation facility, it was found that for an AO fluence up to 1.09×10
22 atoms/cm
2, the uncoated sample was eroded and completely broken. On the contrary, when the coated polyimide film was under AO attack, the HDMSO belonging methyl group were decomposed into volatile products (such as CO
2, CO, H
2O), and the silicon formed a dense glassy SiO
x layer resistant to further AO erosion.
HDMSO and hexamethyldisilazane (HDMSN) [
65], were compared as precursors for SiO
x based O
2 permeation barrier coatings and/or interlayers deposited on polyethylene terephthalate (PET) an polypropylene (PP) substrates by MW (2.45 GHz) activated low pressure plasma polymerization. By means of mass spectrometry, the probability for dissociation of HMDSN at a given energy of incident electrons was higher than for HMDSO. Due to the higher number of smaller fragments, HDMSN coatings showed lower oxygen transmission rates (OTRs) for thicknesses larger than 2.5 nm (measured by ellipsometry), compared to HDMSO coatings. By increasing the content of oxygen in the process mixture, HDMSN seemed to produce highly cross-linked SiO
x barrier coating directly well adhering on PP without the presence of a nanometric organic interlayer, instead needed for PET.
The mechanism of organosilicon based thin-film deposition is still under investigation. Typically, the chemical interpretation considers mainly the recombination of free radicals, which is dominated by neutral radicals over ionic radicals. Thus, free radicals formed by the dissociation of precursor molecules diffuse to the surface of the film, where they are first physisorbed and migrate along the surface until they are desorbed or chemisorbed at a binding site on the film surface.
Recently, an interesting study of these fundamentals [
66] was published, focused on tetravinylsilane (TVS) and its plasma polymerization in a low pressure PE-CVD reactor with the capacitively coupled discharge operated at 13.56 MHz in pulsed mode. The power dependence of the plasma species was studied by mass spectrometry. Moreover, it was found that the deposition rate correlates with the flux of these species chemisorbed on the film surface, if distinct sticking coefficients are taken into account. Then, the carbon to silicon ratio in the deposited film strongly correlates with the C/Si flux ratio for the various power-controlled plasmas.
Considering other kinds of organosilicon precursors, tetraethoxysilane (TEOS) [
67] was found to be a good candidate to obtain by low pressure RF plasma polymerization an efficient thin film for the increase of biocompatibility of metal implants. The coating was deposited on sanded and nanotextured Ti6Al4V alloys, and surface, electrochemical properties and biological behaviour was evaluated through the use of mesenchymal stem cells. This well-known precursor for the SiO
2 production by a sol-gel method can be exploited with higher versatility of resulting thin film properties by plasma polymerization techniques, starting from the possibility of getting nanometric thicknesses. In particular, the samples sanded and polymerized by plasma showed a number of viable stem cells higher than the nanotextured and polymerized surface by plasma.
For specific chemical functionalities, plasma polymerization, for instance, was applied to get nanometric organosilicon based NH
2-terminated films on silicon and aluminium samples by using (3-Aminopropyl)triethoxysilane (APTES) [
68]. A pulsed and remote plasma (pulsed RP-PACVD) was used in order to produce a very soft plasma polymerization process and thus promoting the growth of organic, highly ordered coatings. The plasma was ignited in the discharge tube and the generated reactive species flowed out into a second reaction tube where the substrate holder was located and the influence of the frequency, the duty cycle, t
on and t
off was investigated thoroughly. In addition to weight and spectroscopical characterizations, the Atmospheric pressure Matrix Assisted Light Desorption Ionisation (MALDI) Mass spectrometry was applied: oligomers containing up to eight APTES derived monomers (C
3H
9NO
2Si) and eight primary amine groups were undoubtedly detected and a density increases along with the duration of the t
off was observed. Among them, silsesquioxanes (cages) which are uncommon as species obtainable by plasma processes and cyclosiloxanes (rings) were clearly identified.
Fluorine containing organosilicon monomers were widely used to tune the surface water adsorption/spreading/wetting for applications such as aerospace industry, self-cleaning, heat exchangers, power generation, low-friction coatings, anti-fogging properties or oil spill clean-up processes.
Aside from the above reported example concerning the O
2 RF plasma activated functionalization by FOTS to get antifouling surfaces, Giner et al. focused on the effects of FOTS grafted, by means of a two-stepped chemical vapor deposition process (CVD) (the organosilane cross-linking, forming Si-O-Si surface bonds, was thermally promoted), on a substrate coated by HDMSO plasma polymerized films [
69], that is, composed by flat SiO
x. Actually, there is still the need to improve the analytical understanding of different states of adsorbed ultra-thin and extended water layers on nanorough substrates both for macroscopically hydrophilic and hydrophobic surfaces. Thus, this kind of surface was compared to the one consisting of SiO
x microparticles deposited from a water suspension and successively FOTS functionalized, in order to explore the combined effect of chemistry and roughness on water adhesion behaviour. The FOTS layer on the particles is more defect-rich than the one on the smooth PECVD SiO
x-film and capillary bridges are formed at the contact points between the particles: an increased water adsorption is so observed notwithstanding the presence of the water repulsive FOTS functionalization.
Finally, a double step process composed by a hexamethyldisilazane (HMDSZ) plasma polymerization (PP) step and an Acrylic Acid (AA) grafting polymerization (GP) for materials used in dental implants, titanium (Ti) [
70] and its alloys and zirconia (ZrO
2) ceramics [
71] was reported. In the former case, at first, a Micro-arc oxidation (MAO) process, also called plasma electrolytic oxidation (PEO), was applied to Ti specimens in an electrolyte containing sodium silicate pentahydrate, potassium hydroxide, and ethylenediaminetetraacetic acid) in distilled water, then a RF (13.56 MHz) LP plasma discharge in presence of HDMSZ vapours was activated to get a PP-SiO
x coating and, lastly, a O
2 plasma pre-treatment was carried out to form peroxide groups on the surface and thus facilitate the UV light-induced AA GP by liquid immersion in the precursor of the pre-treated specimens. In the latter case, the zirconia ceramic surface was coated through RF-LP plasma discharge with the PP-SiO
x which was subsequently plasma activate to promote the AA surface grafting. In both cases, the carboxylic terminations were used to immobilize biopolymers (chitosan, chitosan/poly-g-glutamic acid, and gelatin) that enhance the materials biocompatibility and cell viability assays.