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Sol–gel process
Sol–gel process
Sol–gel process
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In materials science, the sol–gel process is a method for producing solid materials from small molecules. The method is used for the fabrication of metal oxides, especially the oxides of silicon (Si) and titanium (Ti). The process involves conversion of monomers in solution into a colloidal solution (sol) that acts as the precursor for an integrated network (or gel) of either discrete particles or network polymers. Typical precursors are metal alkoxides. Sol–gel process is used to produce ceramic nanoparticles.

Stages

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Schematic representation of the different stages and routes of the sol–gel technology

In this chemical procedure, a "sol" (a colloidal solution) is formed that then gradually evolves towards the formation of a gel-like diphasic system containing both a liquid phase and solid phase whose morphologies range from discrete particles to continuous polymer networks. In the case of the colloid, the volume fraction of particles (or particle density) may be so low that a significant amount of fluid may need to be removed initially for the gel-like properties to be recognized. This can be accomplished in any number of ways. The simplest method is to allow time for sedimentation to occur, and then pour off the remaining liquid. Centrifugation can also be used to accelerate the process of phase separation.

Removal of the remaining liquid (solvent) phase requires a drying process, which is typically accompanied by a significant amount of shrinkage and densification. The rate at which the solvent can be removed is ultimately determined by the distribution of porosity in the gel. The ultimate microstructure of the final component will clearly be strongly influenced by changes imposed upon the structural template during this phase of processing.

Afterwards, a thermal treatment, or firing process, is often necessary in order to favor further polycondensation and enhance mechanical properties and structural stability via final sintering, densification, and grain growth. One of the distinct advantages of using this methodology as opposed to the more traditional processing techniques is that densification is often achieved at a much lower temperature.

The precursor sol can be either deposited on a substrate to form a film (e.g., by dip-coating or spin coating), cast into a suitable container with the desired shape (e.g., to obtain monolithic ceramics, glasses, fibers, membranes, aerogels), or used to synthesize powders (e.g., microspheres, nanospheres).[1] The sol–gel approach is a cheap and low-temperature technique that allows the fine control of the product's chemical composition. Even small quantities of dopants, such as organic dyes and rare-earth elements, can be introduced in the sol and end up uniformly dispersed in the final product. It can be used in ceramics processing and manufacturing as an investment casting material, or as a means of producing very thin films of metal oxides for various purposes. Sol–gel derived materials have diverse applications in optics, electronics, energy, space, (bio)sensors, medicine (e.g., controlled drug release), reactive material, and separation (e.g., chromatography) technology.

The interest in sol–gel processing can be traced back in the mid-1800s with the observation that the hydrolysis of tetraethyl orthosilicate (TEOS) under acidic conditions led to the formation of SiO2 in the form of fibers and monoliths. Sol–gel research grew to be so important that in the 1990s more than 35,000 papers were published worldwide on the process.[2][3][4]

Particles and polymers

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The sol–gel process is a wet-chemical technique used for the fabrication of both glassy and ceramic materials. In this process, the sol (or solution) evolves gradually towards the formation of a gel-like network containing both a liquid phase and a solid phase. Typical precursors are metal alkoxides and metal chlorides, which undergo hydrolysis and polycondensation reactions to form a colloid. The basic structure or morphology of the solid phase can range anywhere from discrete colloidal particles to continuous chain-like polymer networks.[5][6]

The term colloid is used primarily to describe a broad range of solid-liquid (and/or liquid-liquid) mixtures, all of which contain distinct solid (and/or liquid) particles which are dispersed to various degrees in a liquid medium. The term is specific to the size of the individual particles, which are larger than atomic dimensions but small enough to exhibit Brownian motion. If the particles are large enough, then their dynamic behavior in any given period of time in suspension would be governed by forces of gravity and sedimentation. But if they are small enough to be colloids, then their irregular motion in suspension can be attributed to the collective bombardment of a myriad of thermally agitated molecules in the liquid suspending medium, as described originally by Albert Einstein in his dissertation. Einstein concluded that this erratic behavior could adequately be described using the theory of Brownian motion, with sedimentation being a possible long-term result. This critical size range (or particle diameter) typically ranges from tens of angstroms (10−10 m) to a few micrometres (10−6 m).[7]

  • Under certain chemical conditions (typically in base-catalyzed sols), the particles may grow to sufficient size to become colloids, which are affected both by sedimentation and forces of gravity. Stabilized suspensions of such sub-micrometre spherical particles may eventually result in their self-assembly—yielding highly ordered microstructures reminiscent of the prototype colloidal crystal: precious opal.[8][9]
  • Under certain chemical conditions (typically in acid-catalyzed sols), the interparticle forces have sufficient strength to cause considerable aggregation and/or flocculation prior to their growth. The formation of a more open continuous network of low density polymers exhibits certain advantages with regard to physical properties in the formation of high performance glass and glass/ceramic components in 2 and 3 dimensions.[10]

In either case (discrete particles or continuous polymer network) the sol evolves then towards the formation of an inorganic network containing a liquid phase (gel). Formation of a metal oxide involves connecting the metal centers with oxo (M-O-M) or hydroxo (M-OH-M) bridges, therefore generating metal-oxo or metal-hydroxo polymers in solution.

In both cases (discrete particles or continuous polymer network), the drying process serves to remove the liquid phase from the gel, yielding a micro-porous amorphous glass or micro-crystalline ceramic. Subsequent thermal treatment (firing) may be performed in order to favor further polycondensation and enhance mechanical properties.

With the viscosity of a sol adjusted into a proper range, both optical quality glass fiber and refractory ceramic fiber can be drawn which are used for fiber optic sensors and thermal insulation, respectively. In addition, uniform ceramic powders of a wide range of chemical composition can be formed by precipitation.

Polymerization

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Simplified representation of the condensation induced by hydrolysis of TEOS

The Stöber process is a well-studied example of polymerization of an alkoxide, specifically TEOS. The chemical formula for TEOS is given by Si(OC2H5)4, or Si(OR)4, where the alkyl group R = C2H5. Alkoxides are ideal chemical precursors for sol–gel synthesis because they react readily with water. The reaction is called hydrolysis, because a hydroxyl ion becomes attached to the silicon atom as follows:

Si(OR)4 + H2O → HO−Si(OR)3 + R−OH

Depending on the amount of water and catalyst present, hydrolysis may proceed to completion to silica:

Si(OR)4 + 2 H2O → SiO2 + 4 R−OH

Complete hydrolysis often requires an excess of water and/or the use of a hydrolysis catalyst such as acetic acid or hydrochloric acid. Intermediate species including [(OR)2−Si−(OH)2] or [(OR)3−Si−(OH)] may result as products of partial hydrolysis reactions.[1] Early intermediates result from two partially hydrolyzed monomers linked with a siloxane [Si−O−Si] bond:

(OR)3−Si−OH + HO−Si−(OR)3 → [(OR)3Si−O−Si(OR)3] + H−O−H

or

(OR)3−Si−OR + HO−Si−(OR)3 → [(OR)3Si−O−Si(OR)3] + R−OH

Thus, polymerization is associated with the formation of a 1-, 2-, or 3-dimensional network of siloxane [Si−O−Si] bonds accompanied by the production of H−O−H and R−O−H species.

By definition, condensation liberates a small molecule, such as water or alcohol. This type of reaction can continue to build larger and larger silicon-containing molecules by the process of polymerization. Thus, a polymer is a huge molecule (or macromolecule) formed from hundreds or thousands of units called monomers. The number of bonds that a monomer can form is called its functionality. Polymerization of silicon alkoxide, for instance, can lead to complex branching of the polymer, because a fully hydrolyzed monomer Si(OH)4 is tetrafunctional (can branch or bond in 4 different directions). Alternatively, under certain conditions (e.g., low water concentration) fewer than 4 of the OR or OH groups (ligands) will be capable of condensation, so relatively little branching will occur. The mechanisms of hydrolysis and condensation, and the factors that bias the structure toward linear or branched structures are the most critical issues of sol–gel science and technology. This reaction is favored in both basic and acidic conditions.

Sono-Ormosil

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Sonication is an efficient tool for the synthesis of polymers. The cavitational shear forces, which stretch out and break the chain in a non-random process, result in a lowering of the molecular weight and poly-dispersity. Furthermore, multi-phase systems are very efficient dispersed and emulsified, so that very fine mixtures are provided. This means that ultrasound increases the rate of polymerisation over conventional stirring and results in higher molecular weights with lower polydispersities. Ormosils (organically modified silicate) are obtained when silane is added to gel-derived silica during sol–gel process. The product is a molecular-scale composite with improved mechanical properties. Sono-Ormosils are characterized by a higher density than classic gels as well as an improved thermal stability. An explanation therefore might be the increased degree of polymerization.[11]

Pechini process

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Main article: Pechini process

For single cation systems like SiO2 and TiO2, hydrolysis and condensation processes naturally give rise to homogenous compositions. For systems involving multiple cations, such as strontium titanate, SrTiO3 and other perovskite systems, the concept of steric immobilisation becomes relevant. To avoid the formation of multiple phases of binary oxides as the result of differing hydrolysis and condensation rates, the entrapment of cations in a polymer network is an effective approach, generally termed the Pechini process.[12] In this process, a chelating agent is used, most often citric acid, to surround aqueous cations and sterically entrap them. Subsequently, a polymer network is formed to immobilize the chelated cations in a gel or resin. This is most often achieved by poly-esterification using ethylene glycol. The resulting polymer is then combusted under oxidising conditions to remove organic content and yield a product oxide with homogeneously dispersed cations.[13]

Nanomaterials, aerogels, xerogels

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Nanostructure of a resorcinol-formaldehyde gel reconstructed from small-angle X-ray scattering. This type of disordered morphology is typical of many sol–gel materials.[14]

If the liquid in a wet gel is removed under a supercritical condition, a highly porous and extremely low density material called aerogel is obtained. Drying the gel by means of low temperature treatments (25–100 °C), it is possible to obtain porous solid matrices called xerogels. In addition, a sol–gel process was developed in the 1950s for the production of radioactive powders of UO2 and ThO2 for nuclear fuels, without generation of large quantities of dust.

Differential stresses that develop as a result of non-uniform drying shrinkage are directly related to the rate at which the solvent can be removed, and thus highly dependent upon the distribution of porosity. Such stresses have been associated with a plastic-to-brittle transition in consolidated bodies,[15] and can yield to crack propagation in the unfired body if not relieved.

In addition, any fluctuations in packing density in the compact as it is prepared for the kiln are often amplified during the sintering process, yielding heterogeneous densification. Some pores and other structural defects associated with density variations have been shown to play a detrimental role in the sintering process by growing and thus limiting end-point densities. Differential stresses arising from heterogeneous densification have also been shown to result in the propagation of internal cracks, thus becoming the strength-controlling flaws.[16][17][18][19][20]

It would therefore appear desirable to process a material in such a way that it is physically uniform with regard to the distribution of components and porosity, rather than using particle size distributions which will maximize the green density. The containment of a uniformly dispersed assembly of strongly interacting particles in suspension requires total control over particle-particle interactions. Monodisperse colloids provide this potential.[8][9][21]

Monodisperse powders of colloidal silica, for example, may therefore be stabilized sufficiently to ensure a high degree of order in the colloidal crystal or polycrystalline colloidal solid which results from aggregation. The degree of order appears to be limited by the time and space allowed for longer-range correlations to be established. Such defective polycrystalline structures would appear to be the basic elements of nanoscale materials science, and, therefore, provide the first step in developing a more rigorous understanding of the mechanisms involved in microstructural evolution in inorganic systems such as sintered ceramic nanomaterials.[22][23]

Ultra-fine and uniform ceramic powders can be formed by precipitation. These powders of single and multiple component compositions can be produced at a nanoscale particle size for dental, biomedical, agrochemical, or catalytic applications. Powder abrasives, used in a variety of finishing operations, are made using a sol–gel type process. One of the more important applications of sol–gel processing is to carry out zeolite synthesis. Other elements (metals, metal oxides) can be easily incorporated into the final product and the silicate sol formed by this method is very stable. Semi-stable metal complexes can be used to produce sub-2 nm oxide particles without thermal treatment. During base-catalyzed synthesis, hydroxo (M-OH) bonds may be avoided in favor of oxo (M-O-M) using a ligand which is strong enough to prevent reaction in the hydroxo regime but weak enough to allow reaction in the oxo regime (see Pourbaix diagram).[24]

Applications

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The applications for sol gel-derived products are numerous.[25][26][27][28][29][30] For example, scientists have used it to produce the world's lightest materials and also some of its toughest ceramics.

Protective coatings

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One of the largest application areas is thin films, which can be produced on a piece of substrate by spin coating or dip-coating. Protective and decorative coatings, and electro-optic components can be applied to glass, metal and other types of substrates with these methods. Cast into a mold, and with further drying and heat-treatment, dense ceramic or glass articles with novel properties can be formed that cannot be created by any other method.[citation needed] Other coating methods include spraying, electrophoresis, inkjet[31][32] printing, or roll coating.

Thin films and fibers

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With the viscosity of a sol adjusted into a proper range, both optical and refractory ceramic fibers can be drawn which are used for fiber optic sensors and thermal insulation, respectively. Thus, many ceramic materials, both glassy and crystalline, have found use in various forms from bulk solid-state components to high surface area forms such as thin films, coatings and fibers.[10][33] Also, thin films have found their application in the electronic field[34] and can be used as sensitive components of a resistive gas sensors.[35]

Controlled release

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Sol-gel technology has been applied for controlled release of fragrances and drugs.[36]

Opto-mechanical

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Macroscopic optical elements and active optical components as well as large area hot mirrors, cold mirrors, lenses, and beam splitters can be made by the sol–gel route. In the processing of high performance ceramic nanomaterials with superior opto-mechanical properties under adverse conditions, the size of the crystalline grains is determined largely by the size of the crystalline particles present in the raw material during the synthesis or formation of the object. Thus a reduction of the original particle size well below the wavelength of visible light (~500 nm) eliminates much of the light scattering, resulting in a translucent or even transparent material.

Furthermore, microscopic pores in sintered ceramic nanomaterials, mainly trapped at the junctions of microcrystalline grains, cause light to scatter and prevented true transparency. The total volume fraction of these nanoscale pores (both intergranular and intragranular porosity) must be less than 1% for high-quality optical transmission, i.e. the density has to be 99.99% of the theoretical crystalline density.[37][38]

See also

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References

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Further reading

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[edit]
Revisions and contributorsEdit on WikipediaRead on Wikipedia

Sol–gel process

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from Grokipedia
The sol–gel process is a versatile wet-chemical method for synthesizing inorganic materials, such as metal oxides, , and ceramics, by converting molecular precursors—typically metal —into a colloidal suspension known as a sol, which then undergoes gelation to form a three-dimensional network structure. This process primarily involves two key reactions: , where the groups react with water to produce hydroxyl groups, and , where these groups link to form metal-oxygen-metal bonds, enabling the formation of a at relatively low temperatures without requiring high-pressure . The resulting can be further processed through drying, aging, and thermal treatments like to yield dense materials, powders, fibers, or thin films with controlled microstructure and composition. Historically, the sol–gel technique traces its roots to the , with early observations of gel formation from compounds exposed to moisture, but it gained prominence in the mid-20th century as a means to overcome limitations of traditional high-temperature solid-state synthesis, allowing for atomic-level mixing and precise tailoring of material properties. Pioneering work, such as the 1968 Stöber method for producing uniform silica spheres, demonstrated its potential for , influencing subsequent advancements in hybrid organic-inorganic materials. Key factors influencing the process include the water-to-precursor ratio, solvent choice, pH, and catalysts (acidic or basic), which dictate the gel's , homogeneity, and final material . The sol–gel process offers significant advantages over conventional methods, including lower processing temperatures (often below 1000°C), scalability for thin films and coatings, and the ability to incorporate dopants or organic components for multifunctional hybrids. It is widely applied in producing optical coatings, sensors, catalysts, biomedical implants, and nanostructured materials like aerogels and quantum dots, with ongoing research focusing on sustainable precursors and energy-efficient variants.

Introduction and Fundamentals

Definition and Overview

The sol–gel process is a wet-chemical technique for producing materials, such as ceramics, , and composites, from small molecular precursors through the formation of a sol—a stable colloidal suspension of particles—and its subsequent evolution into a network of interconnected phase. This method relies on controlled chemical reactions in solution to build materials at the molecular level, enabling the creation of amorphous or crystalline structures under ambient or low-temperature conditions. Key precursors in the sol–gel process include metal alkoxides, such as (TEOS, Si(OC₂H₅)₄), and metal salts, which are typically dissolved in solvents like alcohols. These precursors facilitate and , allowing processing at temperatures far below those required for traditional methods, which often exceed 1000°C for ceramics. A simplified representation of the hydrolysis step for silica formation is: Si(OR)4+2H2O→SiO2+4ROH\text{Si(OR)}_4 + 2\text{H}_2\text{O} \rightarrow \text{SiO}_2 + 4\text{ROH} where R denotes an . The process offers several advantages, including uniform molecular mixing for high purity and homogeneity, the ability to form complex shapes like thin films, fibers, and monoliths, and precise control over nanoscale microstructure and . These features make it particularly suitable for applications requiring tailored material properties without the need for high-energy inputs.

Historical Development

The origins of the sol–gel process trace back to the mid-19th century, when French chemist Jacques-Joseph Ebelmen observed the formation of a transparent, glass-like through the slow of a , such as ethyl silicate, in 1846. This early observation laid the groundwork for understanding gel formation from alkoxide precursors like (), marking the first documented instance of sol–gel chemistry. In the 1930s, researchers at the Schott Company, including Geffcken and , advanced practical applications by developing a sol–gel method to deposit oxide layers on industrial glasses. This period also saw initial explorations in nuclear laboratories during the 1950s in the United States, where the process was adapted to produce high-density nuclear fuels, such as (UO₂) and (ThO₂) microspheres, for reactor applications without generating significant . These developments were influenced by foundational work in science, including Albert Einstein's 1905 theory of , which provided a theoretical basis for understanding the behavior of sols as stable dispersions of colloidal particles. The 1960s marked a period of growing interest, with the Stöber method (1968) demonstrating the production of uniform silica spheres, laying groundwork for nanotechnology applications, and sol–gel enabling low-temperature synthesis of homogeneous glasses that later supported advancements in optical fibers starting in the 1980s. By the 1970s, expansion into thin films gained momentum, driven by researchers like Helmut Dislich, who demonstrated sol–gel routes for borosilicate glasses and coatings at temperatures below traditional melting points, broadening its utility in optics and electronics. The 1990s witnessed an explosive growth in research, with over 35,000 publications worldwide reflecting the process's versatility, spurred by the inaugural International Workshop on Glasses and Ceramics from Gels in 1981 and the launch of the Journal of Sol-Gel Science and Technology in 1993. Post-2000, the sol–gel method has seen accelerated adoption in synthesis, fueled by breakthroughs, enabling the creation of inorganic-organic hybrids, nanocomposites, and functional structures for applications in , self-cleaning surfaces, and advanced ceramics.

Core Processes and Chemistry

Stages of the Sol-Gel Process

The sol-gel process unfolds through a series of distinct physical stages that transform a precursor solution into a solid , enabling the creation of ceramics, , and composites with controlled microstructures. Stage 1: Sol Formation
The process begins with the mixing of molecular precursors, typically metal alkoxides or salts, with a such as alcohol and to initiate the formation of a stable colloidal suspension known as a sol. This stage involves the dispersion of nanoscale particles or chains, with sizes ranging from 1 nm (10⁻⁹ ) to 1 μm (10⁻⁶ ), which remain suspended without settling due to and electrostatic or steric stabilization. The role of in this stage is to generate these reactive that assemble into the colloidal building blocks. The sol's and stability are influenced by factors like precursor concentration and polarity, setting the foundation for subsequent network development. Stage 2: Gelation
As the sol evolves, the colloidal particles or chains interconnect to form a three-dimensional network, transitioning the system from a fluid-like dispersion to a viscoelastic solid called a . This gelation is a time-dependent process, often occurring over minutes to days, where the network spans the entire volume and exhibits solid-like elasticity while retaining liquid within its pores. The rate and nature of gelation are significantly influenced by , with acidic conditions favoring linear structures and basic conditions promoting branched clusters, thereby affecting the gel's rigidity and homogeneity. At the gel point, the material loses flowability, marking a critical physical threshold in the transformation. Stage 3: Aging and Drying
Following gelation, the gel undergoes aging, during which continued interactions strengthen interparticle bonds and coarsen the pore structure through mechanisms like , enhancing mechanical integrity without altering the overall network topology. Subsequently, drying removes the pore-filling , inducing significant shrinkage due to forces that contract the gel framework; this can result in up to 90% volume loss, producing a dense xerogel under ambient conditions or a highly porous if is employed to minimize collapse. These steps critically determine the material's and surface area, with controlled drying rates preventing cracking in bulk samples. Stage 4: Densification
The final stage involves thermal treatment, or , where the dried gel is heated to 400–1000°C to promote viscous flow and eliminate residual , yielding a fully dense crystalline or . This heat-induced consolidation reduces the material's free volume and surface area, with the temperature range allowing phase transformations while avoiding of the framework. The resulting product's and microstructure depend on the heating rate and atmosphere, enabling tailored properties for applications like or . Throughout these stages, the physical evolution—from a Newtonian liquid sol to a rigid , and finally to a porous or dense solid—allows precise control over , ranging from mesoporous xerogels to ultralow-density aerogels, which is pivotal for advanced material design.

and Reactions

The sol–gel process is primarily driven by two sequential chemical reactions: and , which transform metal precursors into a three-dimensional inorganic network. involves the nucleophilic attack of on the metal–oxygen bond of the , replacing the alkoxy group (OR) with a hydroxyl group (OH), as represented by the general equation M–OR + H₂O → M–OH + ROH, where M denotes a metal atom such as (Si) or (Ti). This reaction is typically accelerated by or base catalysts, with the -to- molar playing a critical role in determining the extent of ; ratios greater than stoichiometric (e.g., >4 for tetraalkoxysilanes) promote complete to form metal hydroxides. Condensation reactions follow or occur concurrently with hydrolysis, linking hydrolyzed species through oxo- or hydroxo-bridges to form M–O–M bonds. There are two main types: alcoholysis (M–OH + M–OR → M–O–M + ROH) and aqualysis (M–OH + M–OH → M–O–M + H₂O), both of which eliminate small alcohol or molecules, respectively, and build the polymeric network. The kinetics of these reactions vary significantly with : in acid-catalyzed conditions (e.g., HCl at < 2), hydrolysis proceeds rapidly to completion while is slower, favoring a polymeric route with branched structures; conversely, base-catalyzed processes (e.g., NH₄OH at > 7) exhibit slow hydrolysis but fast , leading to a colloidal route with discrete particles. For silica specifically, full hydrolysis of tetraethoxysilane () yields Si(OR)₄ + 4H₂O → Si(OH)₄ + 4ROH, followed by such as Si(OH)₄ + Si(OH)₄ → (HO)₃Si–O–Si(OH)₃ + H₂O, which initiates network formation. Several factors influence the rates and outcomes of and . The is paramount, as it affects both reaction kinetics and species ; for silica sols, the occurs around 2, where surface charge is zero, minimizing aggregation and stabilizing the sol. accelerates both reactions but can lead to uncontrolled gelation if too high (typically 20–60°C is used), while solvents like alcohols (e.g., ) moderate rates by solvating precursors and byproducts, preventing . These parameters allow precise control over the sol's microstructure, enabling tailored material properties in applications such as coatings and ceramics.

Polymerization Mechanisms

In the sol-gel process, polymerization occurs through the sequential and of metal precursors, leading to the formation of extended inorganic networks via two primary mechanisms: the polymeric pathway and the particulate pathway. These mechanisms determine the microstructure of the resulting and, ultimately, the properties of the derived materials. The choice of pathway is governed by reaction conditions such as , water-to-precursor ratio, and catalyst type, which influence the kinetics of (conversion of M-OR to M-OH) and (formation of M-O-M bonds). The polymeric mechanism predominates under acidic conditions (typically pH 1-4) and higher water-to-alkoxide ratios, where proceeds rapidly relative to , generating silanol groups (Si-OH) that undergo . This results in the formation of linear chains that progressively branch into a three-dimensional network through siloxane (Si-O-Si) bond formation between neutral or weakly ionized . Acid catalysts, such as HCl, promote this branching by accelerating the of protonated silanols with neutral alkoxysilanes or silanols, favoring the creation of weakly to highly branched polymers with dimensions around 1.9-2.4. At low water ratios, the process can shift toward more compact structures, but the overall pathway yields entangled polymeric networks that exhibit gradual increases as the rises, reflecting the extension and interconnection of chains. In contrast, the particulate mechanism is favored under basic conditions (pH >7) and lower water-to-alkoxide ratios, where slower allows for rapid between deprotonated silanolates (Si-O⁻), leading to the and growth of discrete anionic clusters or particles (typically 5-100 nm in size). These clusters aggregate through electrostatic repulsion and van der Waals attraction to form a percolating network, rather than extensive branching. Base catalysts like promote linear growth of these particles by enhancing the rate of negatively charged species, minimizing branching and resulting in more spherical, colloidal structures. A seminal example is the , which uses -catalyzed of (TEOS) in ethanol-water mixtures to produce monodisperse silica spheres with diameters controllable from 0.1 to 2 μm, ideal for applications requiring uniform particulates. Network formation in both mechanisms is monitored by the increase in solution , which correlates with the (DP) as crosslinks form and the system transitions from a sol to a . The step, particularly the alcohol-producing reaction, drives this growth, with a rate expressed as: rate=k[\ceSi−OH][\ceSi−OR]\text{rate} = k [\ce{Si-OH}][\ce{Si-OR}] where kk is the rate constant (e.g., 0.001 L/mol·min for acid-catalyzed tetramethoxysilane systems), and the reaction yields Si-O-Si + ROH. This second-order kinetics highlights how the concentrations of reactive and alkoxysilane species dictate the pace, with higher [Si-OH] under excess accelerating network extension. The choice of mechanism significantly influences the final material properties: polymeric networks from typically yield dense, low-porosity glasses upon densification due to their branched, interpenetrating structure, while particulate networks from base catalysis produce more porous materials with larger pores (e.g., 10-50 nm) from , suitable for applications like catalysts or insulators.

Structural Formation

Particles and Polymers

In the sol–gel process, particle formation occurs primarily under basic conditions, where and lead to the rapid and growth of discrete colloidal particles, typically spherical or irregular in shape with diameters ranging from 1 to 100 nm. These particles form stable dispersions known as colloidal sols, which upon further aggregation result in particulate gels characterized by interparticle pores that arise from the packing of these primary units. The structure of such gels is often compact and non-fractal, with a mass approaching 3, reflecting dense, fully condensed clusters. In contrast, polymer formation predominates under acidic conditions, where slower favors the creation of extended (Si-O-Si) chains that branch and interconnect to form amorphous, three-dimensional networks. These polymeric structures exhibit characteristics during growth, with mass dimensions typically between 2.0 and 3.0, leading to gels with pores on the molecular scale (often <1 nm initially, expanding to 1.5–3.0 nm with aging). The resulting polymeric gels possess a more homogeneous, interconnected topology compared to their particulate counterparts. The transition from sol to gel involves the evolution of these structures into a spanning network that imparts solidity to the system, shifting from a stable dispersion of isolated particles or chains to a continuous phase that traps the liquid medium. This process often proceeds via diffusion-limited or reaction-limited cluster-cluster aggregation, yielding fractal dimensions around 2.1 in many silica systems, which influences the openness and interconnectivity of the final network. Characterization of these morphological outcomes relies on techniques such as transmission electron microscopy (TEM) and scanning electron microscopy (SEM) to visualize particle shapes, sizes, and aggregation patterns in particulate sols and gels. Rheological measurements, particularly monitoring the divergence of viscosity or the crossover of storage and loss moduli, identify the gel point where the system transitions to a viscoelastic solid. The distinct morphologies carry important property implications: particulate gels, with their interparticle porosity and high packing density of nanoscale units, achieve exceptionally high specific surface areas (often exceeding 200 m²/g), beneficial for applications requiring adsorption or catalysis. Polymeric gels, by virtue of their uniform, fractal networks lacking large scattering domains, exhibit superior optical transparency, making them suitable for thin films and optical components.

Gelation and Network Formation

Gelation in the sol-gel process marks the transition from a fluid sol to a semi-solid state, occurring at a critical conversion where the forming network spans the entire container volume, as described by percolation theory. This point is characterized by a sharp increase in the shear modulus, signaling the onset of infinite connectivity among the aggregating species. In silica systems, gelation typically happens depending on the precursor concentration and reaction conditions. Following gelation, the wet gel consists of a three-dimensional network enclosing 80-90% liquid by volume, with the solid phase forming a fragile, solvent-filled structure. During the subsequent aging phase, syneresis occurs as the gel expels solvent through continued condensation reactions, leading to network strengthening via mechanisms such as Ostwald ripening, where smaller pores dissolve and redeposit onto larger ones. This process enhances mechanical rigidity and reduces porosity over time scales of hours to days. Several factors influence the dynamics of gelation and network evolution. Temperature accelerates the reaction rates, shortening gelation times by increasing kinetic energy for hydrolysis and condensation; for instance, raising the temperature from 25°C to 60°C can reduce gelation time by orders of magnitude in alkoxide-based systems. The pH plays a crucial role, with silica gelation exhibiting a minimum rate near neutral pH (~7), where surface charge is low, favoring slower aggregation, while acidic (pH 2-4) or basic (pH 8-10) conditions promote faster network formation through charged particle repulsion or attraction. Additives, such as polymers in hybrid gels, can modify network topology by altering cross-linking density and preventing premature collapse. As the network evolves from the wet gel to the dried solid, significant shrinkage occurs due to solvent removal, with the volume shrinkage approximated by ΔV/V=1−ϕ\Delta V / V = 1 - \phi, where ϕ\phi is the initial solid volume fraction in the gel. This transformation can result in up to 90% volume loss, transitioning the material to a xerogel with a denser structure. A major challenge in this evolution is cracking during drying, induced by capillary stresses generated as the meniscus in the pores pulls on the network with forces up to several MPa, exceeding the gel's tensile strength and causing fracture propagation. These stresses are particularly severe in thicker samples or under rapid drying conditions, limiting monolithic gel sizes to millimeters without mitigation strategies.

Process Variations

Pechini Process

The Pechini process, developed by M. P. Pechini in 1967, represents a polymerizable complex variant of the sol-gel method tailored for synthesizing homogeneous multi-component metal oxides, such as perovskites, from inexpensive metal salts. This approach addresses limitations in traditional sol-gel routes by using citric acid as a chelating agent to form stable complexes with metal cations, thereby preventing selective precipitation and ensuring uniform distribution at the molecular scale. The process begins with the dissolution of metal salts (e.g., nitrates or carbonates of , strontium, or barium) in water, followed by the addition of citric acid in a molar ratio typically ranging from 2:1 to 8:1 relative to the metal ions, forming soluble chelates. is then added, often in a 4:1 molar ratio to citric acid, and the solution is heated to 130–250°C under constant stirring to drive polyesterification, yielding a transparent, viscous resin that encapsulates the metal ions homogeneously. The key esterification reaction can be represented as: Metal-citrate complex+HO-CH2CH2-OH→polymeric ester network+H2O\text{Metal-citrate complex} + \text{HO-CH}_2\text{CH}_2\text{-OH} \rightarrow \text{polymeric ester network} + \text{H}_2\text{O} This polymerization step creates a cross-linked organic matrix that maintains cation intimacy during subsequent thermal treatment. The dried resin undergoes pyrolysis at 300–600°C, which decomposes the organic components via combustion and yields fine, crystalline oxide powders with high purity and sub-micron particle sizes. For instance, this method produces phase-pure SrTiO₃ and BaTiO₃ powders suitable for capacitor dielectrics, often achieving crystallization at lower temperatures than conventional ceramic routes (e.g., 600°C versus 1000–1200°C). The process's advantages include atomic-level mixing for complex stoichiometries in perovskites, reduced synthesis costs by avoiding expensive alkoxides, and circumvention of hydrolysis control issues inherent in alkoxide-based sol-gel chemistry, leading to improved compositional homogeneity and lower contamination risks.

Sono-Ormosil

Sono-Ormosils represent a class of organically modified silicates (ORMOSILs) synthesized through the sol-gel process enhanced by sonication, enabling the incorporation of organic groups into inorganic silica networks to impart flexibility, tailored functionality, and improved processability. These hybrid materials are formed by reacting tetraethoxysilane (TEOS) with organoalkoxysilanes of the general form RSi(OR')₃, where R is an organic substituent such as alkyl, aryl, or polymeric chains, and OR' are hydrolyzable alkoxy groups. This co-hydrolysis and co-condensation create covalent bonds between organic and inorganic phases, resulting in amorphous, homogeneous structures that combine the rigidity of silica with the ductility of organics. The sonication step employs ultrasound at frequencies of 20-40 kHz to induce acoustic cavitation in the precursor solution, which consists of TEOS, the organosilane, water, and a catalyst like HCl, often without additional solvents. Cavitation generates localized high-temperature (up to 5000 K) and high-pressure (up to 1000 atm) hot spots, along with the formation of radicals such as hydroxyl (•OH), that dramatically accelerate hydrolysis and condensation reactions. This reduces gelation time from days in conventional processes to as little as 5-30 minutes, promoting rapid network formation and solventless synthesis. The acoustic energy also enhances radical-mediated polymerization, leading to finer microstructural control. Developed in the 1980s, with pioneering work on sonogels by Tarasevich using ultrasound on TEOS-water mixtures, sono-ormosils offer denser networks with lower porosity compared to traditional ORMOSILs, achieving densities above 0.98 g/cm³ and specific surface areas tuned for applications. These materials exhibit enhanced thermal stability, maintaining integrity up to 800°C due to the cross-linked hybrid structure, and superior mechanical properties, such as Vickers hardness values around 180 kg/mm². A representative example is polydimethylsiloxane (PDMS)-modified silica, where the flexible siloxane chains yield rubber-like elastomers with improved fracture toughness, making sono-ormosils suitable for protective coatings and thin films.

Other Modifications

The solvothermal modification of the sol-gel process involves pressurized heating in non-aqueous solvents to promote the formation of crystalline nanoparticles, such as anatase-phase TiO₂, under controlled conditions like 200°C for short durations without subsequent calcination. This variant enhances crystallinity and phase purity compared to standard sol-gel routes by leveraging solvent dielectric properties and elevated pressures, typically yielding nanoparticles with sizes in the 10-40 nm range. Template-assisted sol-gel methods utilize surfactants or block copolymers as structure-directing agents to create ordered mesoporous materials with uniform pore architectures. A seminal example is the discovery of MCM-41 silica in the early 1990s, synthesized via self-assembly of silicate species around cationic surfactant micelles, followed by template removal to yield hexagonally arranged pores. This approach allows precise control over pore dimensions through adjustments in surfactant chain length and synthesis pH, enabling applications in catalysis and adsorption. Epoxy-modified sol-gel processes integrate epoxy resins with inorganic precursors to form polymer-ceramic hybrids that combine the rigidity of ceramics with the flexibility of polymers, significantly improving fracture toughness. These hybrids are prepared by incorporating silane coupling agents to bridge organic and inorganic phases during hydrolysis and condensation, resulting in materials with enhanced mechanical properties suitable for coatings and composites. In the 2020s, microwave-assisted sol-gel variants have gained prominence for accelerating gelation and reducing reaction times from hours to minutes through volumetric heating, which promotes uniform nucleation and minimizes aggregation in systems like metal oxide nanoparticles. Similarly, supercritical CO₂ drying variants replace traditional solvent evaporation with low-surface-tension fluid extraction to preserve delicate gel networks, yielding high-porosity structures without collapse during processing. These modifications collectively enable tailored porosity in the mesoporous range of 2-50 nm by adjusting templating agents, solvent conditions, and drying protocols, while microwave and solvothermal approaches improve scalability for industrial production through faster processing and higher yields.

Derived Materials

Nanomaterials

The sol–gel process plays a pivotal role in the synthesis of nanomaterials, enabling precise control over particle size, morphology, and composition through hydrolysis and condensation reactions. One of the most seminal techniques for producing uniform silica nanoparticles is the Stöber method, which involves the ammonia-catalyzed hydrolysis of tetraethyl orthosilicate (TEOS) in ethanol, yielding monodisperse SiO₂ spheres typically ranging from 50 to 500 nm in diameter. This approach ensures high uniformity and colloidal stability, making it ideal for applications requiring consistent nanoscale building blocks. For metallic nanoparticles, reverse micelle systems within the sol–gel framework serve as confined reaction environments, facilitating the synthesis of gold (Au) and silver (Ag) particles with sizes below 10 nm; for instance, reduction of metal salts in AOT-based reverse micelles produces stable Au and Ag nanoparticles with narrow size distributions. Quantum dots, such as CdSe/ZnS core-shell structures, can also be incorporated or synthesized using sol–gel routes, particularly for optoelectronic applications where size-tunable emission is critical. In these systems, sol–gel processing allows for the formation of CdSe cores (2–10 nm) passivated by ZnS shells, enabling emission wavelengths from green to red through quantum confinement effects, with quantum yields exceeding 50%. This tunability arises from precise control of precursor ratios and reaction conditions during the sol–gel deposition of the shell layer. Nanocomposites represent another key advancement, where in situ sol–gel formation of silica nanoparticles within polymer matrices like poly(methyl methacrylate) (PMMA) enhances mechanical properties; for example, incorporating silica nanoparticles via TEOS hydrolysis in PMMA solutions, reinforced with carbon nanotubes, yields hybrid materials with improved scratch resistance, increasing critical load values by approximately 1.6-fold compared to unreinforced hybrids. In the 2020s, bio-inspired sol–gel approaches have emerged for self-healing nanomaterials, mimicking natural processes like mussel adhesion to create dynamic networks that autonomously repair damage through reversible covalent bonds or hydrogen bonding in silica-polymer hybrids. Similarly, high-entropy oxides (HEOs) synthesized via sol–gel methods, such as non-equiatomic mixtures of Al-Mg-Fe-Cu-Ni-Co oxides, have shown promise in catalysis, exhibiting enhanced performance for reactions like water oxidation due to configurational entropy for phase stability at the nanoscale. Recent advancements as of 2025 include rare-earth high-entropy oxides for multifunctional catalysis, leveraging high oxygen mobility in ceria-based structures. Achieving monodispersity and high purity in sol–gel nanomaterials often relies on surfactants, such as cetyltrimethylammonium bromide (CTAB) or fluorinated variants, which act as templates to direct particle growth and prevent aggregation. Gelation aspects briefly support nano-structuring by promoting uniform network interconnection during synthesis.

Aerogels and Xerogels

Xerogels are produced through ambient or low-temperature drying of sol-gel derived gels, resulting in cracked, denser porous solids due to capillary forces that cause shrinkage and fracturing during solvent evaporation. These materials typically exhibit porosities ranging from 60% to 90% and specific surface areas between 400 and 1000 m²/g, making them suitable for applications requiring robust, mesoporous structures. In contrast, aerogels are obtained by supercritical drying of the gels, which eliminates surface tension and preserves the delicate three-dimensional network formed during gelation. Supercritical drying with carbon dioxide, conducted at its critical point of 31°C and 73 bar, allows for the replacement of liquid solvents without collapsing the structure, yielding ultra-low-density materials (0.001–0.5 g/cm³) with porosities up to 99%. This process often begins with alcogels—gels in alcohol solvents—followed by solvent exchange to ensure compatibility with the supercritical fluid. The drying stage in the sol-gel process is crucial here, as it determines the final porosity and mechanical integrity of these open-cell foams. Silica aerogels, among the earliest examples, were first synthesized in 1931 by Samuel S. Kistler using a sol-gel route followed by supercritical drying, demonstrating their potential as lightweight insulators with thermal conductivities as low as 0.01 W/m·K. These translucent materials, composed of over 99% air, have been pivotal in space exploration, such as in NASA's Stardust mission launched in 1999, where silica aerogel blocks captured comet particles during hypervelocity impacts without significant fragmentation. In the 2020s, advancements have focused on carbon aerogels derived from sol-gel polymerization of resorcinol-formaldehyde precursors, followed by pyrolysis and supercritical drying, enhancing their electrical conductivity for energy-related uses. These carbon aerogels address inherent challenges like brittleness through fiber reinforcement, such as incorporation of carbon nanofibers or cloth, which improves mechanical strength while maintaining high surface areas and hierarchical porosity.

Applications

Protective Coatings and Thin Films

The sol–gel process enables the fabrication of protective coatings and thin films that safeguard substrates such as metals and glass from environmental degradation, mechanical wear, and chemical attack. These coatings form through hydrolysis and condensation reactions, yielding inorganic or hybrid organic-inorganic networks that adhere strongly to surfaces and can be tailored for specific functionalities like corrosion resistance or optical clarity. Early applications focused on anti-corrosion protection, with silica-based sol–gel coatings on aluminum alloys emerging in the 1980s as a chromate-free alternative to traditional treatments; for instance, tetraethoxysilane-derived films created dense barriers that significantly reduced pitting and uniform corrosion in aggressive electrolytes. Hybrid organically modified silicates (ormosils), such as SiO₂–TiO₂ systems, have since been applied to glass for scratch resistance, enhancing surface hardness and reducing abrasion damage by up to 50% compared to uncoated substrates through integrated polymer-silicate matrices. Deposition techniques like dip-coating and spin-coating are pivotal for achieving uniform thin films, where the substrate is immersed in or rotated with the sol precursor, followed by controlled evaporation and heat treatment. Film thickness typically ranges from 10 nm to 10 μm, adjustable via sol viscosity (often 1–100 cP), withdrawal speed in dip-coating (0.1–10 mm/s), or spin speed (500–5000 rpm); multiple layers can build thicker protective structures without cracking. Key to uniformity is precise control of sol rheology and ambient humidity, preventing defects like pinholes that compromise barrier properties. These methods are versatile for large-scale industrial application, such as roll-to-roll processing for continuous coating production. The coatings' performance stems from robust interfacial chemistry and tunable bulk properties. Adhesion is achieved via covalent siloxane (Si–O–Si) or metal–oxygen bonds formed during gelation and curing, often exceeding 10 MPa pull-off strength on pretreated surfaces like aluminum or glass, far surpassing physical adhesion in organic paints. Refractive index tuning in multilayers—ranging from ~1.2 for nanoporous silica (via controlled densification) to ~1.8 for titania-rich compositions—facilitates anti-reflective designs by gradient matching to substrates, reducing reflection losses below 1% across visible wavelengths. In practical examples, silicon-acrylic sol–gel hybrids serve as automotive clear coats, providing etch and mar resistance with pencil hardness up to 4H while maintaining >90% for aesthetic and protective finishes on vehicle exteriors. Similarly, sol–gel-derived (8 wt% Y₂O₃) forms thermal barrier coatings on turbine blades, enduring temperatures >1200°C with low thermal conductivity (~1 /m·) to extend component lifespan. As of 2025, innovations emphasize multifunctional coatings, notably self-cleaning TiO₂ films that exploit to degrade organic pollutants under UV exposure, achieving >95% removal in under 2 hours. These anatase-phase films, deposited via sol–gel dip-coating, incorporate dopants like (0.08 wt%) for enhanced visible-light activity and superhydrophilicity ( <5°), addressing urban soiling on architectural glass without mechanical cleaning. Such advancements underscore the sol–gel process's role in sustainable surface protection, balancing durability with environmental responsiveness.

Fibers and Controlled Release

The sol-gel process enables the production of oxide fibers through techniques such as and wet-spinning, where a precursor sol is spun into fibers that are subsequently gelled, dried, and calcined to form ceramic structures. In , a polymer-stabilized sol, often containing aluminum salts like aluminum nitrate, is extruded under an electric field to yield nanofibers with diameters typically ranging from 100 nm to 5 μm, followed by calcination at temperatures up to 1200°C to achieve crystalline α-alumina. Wet-spinning involves extruding the viscous sol through a spinneret into a coagulation bath to form gel fibers, which are then aged and sintered; this method is particularly suited for aerogel fibers and allows for continuous production. Alumina fibers produced via these sol-gel routes, with diameters of 100 nm to 10 μm, exhibit high porosity and thermal stability, making them ideal for applications such as high-temperature filters in environmental protection and diesel particulate traps. In controlled release systems, sol-gel-derived mesoporous silica serves as an effective matrix for drug encapsulation due to its tunable pore structure (typically 2-50 nm) formed through surfactant-templated hydrolysis and condensation of silane precursors like tetraethyl orthosilicate. For instance, ibuprofen, a model hydrophobic drug, can be loaded into these pores via solvent evaporation or incipient wetness impregnation, achieving loadings of 20-30 wt% while maintaining amorphization to enhance solubility. Release occurs primarily through diffusion governed by Fick's laws, where drug molecules desorb from pore walls and migrate via concentration gradients, with rates modulated by pore size and surface functionalization. pH-responsive variants, incorporating gatekeeping ligands like amine groups, enable triggered release in acidic environments (e.g., pH 5-6 in tumors or inflamed tissues), achieving up to 80% release over 24-48 hours compared to slower diffusion in neutral conditions. Early applications of sol-gel controlled release include fragrance delivery in cosmetics, pioneered in the 1990s through silica xerogel encapsulation of odorants like limonene and geraniol via emulsion-based sol-gel processes, which provided sustained volatilization over weeks by trapping molecules in porous silica cages. In biomedical contexts, antibiotic-releasing implants exemplify pore diffusion mechanisms; for example, vancomycin-loaded silica xerogels sustain release for up to 6 weeks, with an initial first-order phase transitioning to near-zero-order kinetics, delivering ~90% of the load (2-11 mg/g) while retaining bactericidal activity against pathogens like Staphylococcus epidermidis. Key advantages of sol-gel materials for controlled release include high biocompatibility, as silica degrades into non-toxic silicic acid, and tunable release profiles spanning days to months by adjusting porosity, particle size, or hybrid organic-inorganic compositions. These properties stem from the mild, low-temperature processing that preserves bioactive integrity. In recent developments during the 2020s, sol-gel nanofiber scaffolds, such as chitosan/nanosilica composites electrospun from hybrid sols, have been explored for wound healing, promoting sustained delivery of growth factors and achieving accelerated epithelialization in vitro and in vivo models.

Opto-Mechanical Devices

The sol–gel process enables the fabrication of optical glasses with exceptionally low scattering losses, making them suitable for waveguides in photonic devices. For instance, germano-silicate glass waveguides derived from sol–gel synthesis exhibit propagation losses as low as 0.06 dB/cm at 1550 nm, achieved through optimized annealing to minimize porosity and hydroxyl content while maintaining surface roughness below 1 nm. These low-loss properties arise from the homogeneous nanoscale structure of sol–gel materials, which reduces light scattering compared to traditional melt-quenched glasses. Dye-doped variants, such as organically modified silicates (ORMOSILs) incorporating rhodamine dyes, further extend applications to solid-state lasers, demonstrating peak optical gains up to 40 cm⁻¹ and enhanced photostability over polymeric hosts due to the rigid, transparent gel matrix. In mechanical applications, sol–gel-derived hybrids improve the toughness of silica-based ceramics, addressing the inherent brittleness of pure silica. Poly(dimethylacrylamide) (PDMA) hydrogels modified with silica nanoparticles serve as a representative example, where silica acts as physical cross-links to enhance fracture energy release rates by up to an order of magnitude compared to pure PDMA, yielding materials with high strain tolerance and no permanent damage after cyclic loading. This toughening mechanism, driven by breakable silica-polymer bonds and a broad distribution of elastic chain lengths, results in fracture toughness values significantly higher than the 0.7 MPa·m¹/² typical of unmodified silica, often reaching 2–5 MPa·m¹/² in optimized compositions. Opto-mechanical devices leverage these properties through integrated sol–gel structures, such as microelectromechanical systems (MEMS) sensors patterned from lead zirconate titanate (PZT) films. Sol–gel PZT solutions enable micrometer- and nanometer-scale patterning via soft lithography and spin coating, producing high-fidelity films with strong piezoelectric coefficients for transducers and sensors, while higher pyrolysis temperatures mitigate cracking during annealing at 650°C. Photochromic films for smart windows represent another key device, where sol–gel matrices doped with naphthopyran dyes in mesoporous organic-inorganic coatings (e.g., using glycidoxypropyltrimethoxysilane and alkyltriethoxysilane) achieve transmittance reductions of 30–60% under UV exposure, with bleaching times under 30 minutes and solar heat gain coefficients dropping to 0.78 for single-glazed units. From the 1990s onward, sol–gel materials have advanced photonic integration for circuits, evolving from early silica-titania thin films for waveguides in the 1990s—emphasizing low-cost doping with erbium for amplification—to 2020s developments in dip-coated SiO₂:TiO₂ platforms with losses comparable to chemical vapor deposition, enabling ring resonators and gratings with sensitivities up to 230 nm/RIU. Nonlinear optics benefits from χ³ tuning in these materials, where sol–gel amorphous oxide glasses (e.g., MnO₂-SiO₂ to PbO-SiO₂) exhibit third-order susceptibilities increasing from 0.48 × 10⁻¹³ esu to 2.68 × 10⁻¹³ esu via compositional adjustments that narrow bandgaps and enhance electronic polarizability through nonbridging oxygens. Fabrication often employs photolithography on UV-sensitive sol–gel films deposited on silicon, where deep UV exposure patterns ridge waveguides directly, allowing low-temperature processing and precise control over device geometry without high-vacuum equipment.

Biomedical and Energy Uses

In the biomedical field, the sol-gel process has enabled the development of bioactive glasses based on the 45S5 composition (46.1 mol% SiO₂, 24.4 mol% Na₂O, 26.9 mol% CaO, 2.6 mol% P₂O₅), which exhibit rapid hydroxyapatite formation on their surface when exposed to simulated body fluids, promoting osteoblast adhesion and bone regeneration. These glasses, synthesized via sol-gel methods to achieve higher surface area and reactivity compared to melt-derived counterparts, have been applied in particulate or scaffold forms for filling bone defects, demonstrating enhanced bone ingrowth in animal models such as rabbit calvarial defects. Sol-gel-derived scaffolds for tissue engineering typically feature interconnected porosities exceeding 90%, facilitating nutrient diffusion and vascularization essential for stem cell delivery in the 2020s. These scaffolds, often composed of silica or hybrid silica-polymer matrices, support mesenchymal stem cell proliferation and differentiation into osteoblasts, with applications in repairing critical-sized bone defects through controlled release of growth factors. For instance, silica-based aerogel scaffolds have shown compatibility with human adipose-derived stem cells, promoting osteogenic differentiation without cytotoxicity. In drug delivery, sol-gel-synthesized mesoporous silica nanoparticles (MSNs) serve as carriers for doxorubicin, achieving high loading capacities (up to 20 wt%) through electrostatic interactions and pore confinement, while leveraging the enhanced permeability and retention (EPR) effect for passive tumor targeting in cancer therapy. These nanoparticles, with tunable pore sizes of 2–10 nm, enable pH-responsive release in acidic tumor microenvironments, reducing systemic toxicity and improving efficacy in models of breast and liver cancers. For energy applications, the sol-gel process, particularly the Pechini variant, has been used to synthesize garnet-type Li₇La₃Zr₂O₁₂ (LLZO) solid-state electrolytes for lithium batteries, yielding dense pellets with ionic conductivities around 10⁻⁴ S/cm at room temperature due to the cubic phase stabilization via doping (e.g., with Al or Ta). This method allows low-temperature processing (below 1000°C), minimizing lithium loss and enabling all-solid-state batteries with improved safety over liquid electrolytes. In perovskite solar cells, sol-gel-deposited TiO₂ electron transport layers contribute to power conversion efficiencies exceeding 25% by providing compact, defect-free interfaces that enhance charge extraction and reduce recombination. Recent 2025 advances include hybrid aerogels, such as metal-organic framework (MOF)-incorporated silica variants prepared via sol-gel polycondensation, which offer high surface areas (>500 m²/g) for physisorption-based capacities up to 5 wt% at 77 K and 1 bar. Additionally, sol-gel antimicrobial coatings on implants, incorporating silver nanoparticles or antibiotics like levofloxacin in silica matrices, have demonstrated >99% reduction in bacterial adhesion (e.g., ) on surfaces, extending implant longevity. Challenges in these applications include rigorous testing per standards, which require assessments of (ISO 10993-5), implantation (ISO 10993-6), and to ensure no adverse tissue responses, as sol-gel materials may release ions affecting cell viability below 70%.

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