Next Article in Journal / Special Issue
The Applicability of Nanostructured Materials in Regenerating Soft and Bone Tissue in the Oral Cavity—A Review
Previous Article in Journal
Biped Robots Control in Gusty Environments with Adaptive Exploration Based DDPG
Previous Article in Special Issue
Radiographic Study of Transcrestal Sinus Floor Elevation Using Osseodensification Technique with Graft Material: A Pilot Study
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Review

Biological Surface Layer Formation on Bioceramic Particles for Protein Adsorption

Department of Materials Science and Bioengineering, Nagaoka University of Technology, Kamitomioka 1603-1, Nagaoka 940-2188, Japan
*
Author to whom correspondence should be addressed.
Biomimetics 2024, 9(6), 347; https://doi.org/10.3390/biomimetics9060347
Submission received: 13 May 2024 / Revised: 28 May 2024 / Accepted: 5 June 2024 / Published: 8 June 2024

Abstract

:
In the biomedical fields of bone regenerative therapy, the immobilization of proteins on the bioceramic particles to maintain their highly ordered structures is significantly important. In this review, we comprehensively discussed the importance of the specific surface layer, which can be called “non-apatitic layer”, affecting the immobilization of proteins on particles such as hydroxyapatite and amorphous silica. It was suggested that the water molecules and ions contained in the non-apatitic layer can determine and control the protein immobilization states. In amorphous silica particles, the direct interactions between proteins and silanol groups make it difficult to immobilize the proteins and maintain their highly ordered structures. Thus, the importance of the formation of a surface layer consisting of water molecules and ions (i.e., a non-apatitic layer) on the particle surfaces for immobilizing proteins and maintaining their highly ordered structures was suggested and described. In particular, chlorine-containing amorphous silica particles were also described, which can effectively form the surface layer of protein immobilization carriers. The design of the bio-interactive and bio-compatible surfaces for protein immobilization while maintaining the highly ordered structures will improve cell adhesion and tissue formation, thereby contributing to the construction of social infrastructures to support super-aged society.

1. Introduction

The population in the world is aging rapidly, and urgent action should be taken to extend healthy life expectancy. In order to improve this situation, the development of medical technology is necessary, especially drug delivery system (DDS), which has become an efficient bone regenerative therapy technology. When bone growth factor protein drugs are immobilized on DDS carriers, the collapse of the highly ordered protein structure often occurs, resulting in the loss of drug function. To ameliorate the problem, it is important to functionalize the carrier surfaces that could maintain the protein interaction structures. Therefore, in the present review, the structures and characteristics of the representative bioceramic particles such as hydroxyapatite (HA) and amorphous silica were summarized, and the novel protein immobilization techniques on bioceramics such as hydroxyapatite (HA) and amorphous silica hosts were highlighted and investigated by mimicking the steric adsorption states of proteins in vivo. Furthermore, the research on surface functionalization of bioceramic particles for protein immobilization was reviewed to construct the novel research field of surface hydration layer formation and protein interaction states.

2. Protein Immobilization Phenomena on Biological Bone

The illustration of biological bone is shown in Figure 1. In introducing the bone from the outside, the layers of the periosteum, cortical bone, trabecular bone, and bone marrow can be observed. The cortical bone is a thin bone layer called Haber’s lamina that surrounds the channels of blood vessels (i.e., Haber’s canal) like the annual ring structure [1]. Here, the Haber’s lamina is composed of the hybrid bioceramic system of HA with organic/polymeric materials. In particular, collagen is artificially used as the backbone structure and HA fills the structural spaces, and the interfacial collagen-HA binding is effectively attributed to the non-collagen protein medication [2].
The highly ordered structures of proteins are closely related to their functions, and the non-collagen proteins maintain their highly ordered structures and effectively bind with HA, enabling them to perform bone formation and functions. It is known that non-collagen proteins involved in binding to collagen are osteocalcin and osteonectin [2]. The functional molecular part of the non-collagen proteins would be γ-carboxyglutamic acid (Gla) residues with two carboxylate ions, which interact electrostatically with the calcium ions of HA in biological bone mineralization. As a specific behavior, old biological bone is exposed to the acidic environment of osteoclasts, resulting in its dissolution into calcium and phosphate ions. Subsequently, osteoblasts release non-collagen proteins and then precipitate HA on their carboxylate ions as the nucleation sites, indicating the inorganic–organic binding interfaces in vivo. However, there have been few studies that mimic the mechanism of biological bone mineralization, which is important for novel research on the surface modification of bioceramics and the formation of their interactive interfaces with proteins.

3. Bioceramic Particles and Surface Function

3.1. Hydroxyapatite Particles

3.1.1. Features

HA, which has higher biocompatibility, is one of the bioceramics and the main component of biological bone. For the crystalline structure (Figure 2), HA is hexagonal, the space group is classified into P63/m, and the lattice constants are a = 0.94 nm and c = 0.68 nm. The ten Ca ions in HA can be divided into two different locations: four Ca ions are Ca(I) (columnar Ca) and are arranged in a single column along the c-axis, while the other Ca ions are Ca(II) (axis Ca) and form the equilateral triangles around the c-axis at the four corners of the HA unit cell, which are rotated by 60° and stacked along the c-axis direction. The hydroxyl groups are stacked and arranged along the c-axis direction in the region surrounded by Ca(II), and these Ca(I) and Ca(II) are surrounded by oxygen atom of PO43− [4]. The a-plane (m-plane) is positively charged with many Ca2+ ions, whereas the c-plane with many PO43− ions is negatively charged. Moreover, the hydrophilic OH and PO43− in the HA structure form hydrogen bonds with the functional groups of proteins, making it easy to immobilize proteins. Furthermore, HA also has higher ion exchange ability. For example, various elemental ions are substituted and introduced into HA in the biological hard tissues, depending on their concentrations and species, thereby causing changes in the crystal lattice, bone metabolism, and bone formation in vivo. The cationic substitutions with Ca2+ and the anionic substitutions with PO43− and OH of different elemental ions will affect the lattice constant, crystallinity, surface charge, and morphology of HA. Na+ and K+ are abundant in vivo and also exist in the biological bones, whereas the substitution elements change the lattice parameters of HA due to factors such as the loss of OH and Ca2+ and the increase in ionic diameters. For example, it has been reported that Na+ and CO32− (type B) substitutions decrease the a-axis and increase the c-axis, Cl substitution increases the a-axis and decreases the c-axis, and K+ substitution decreases the a- and c-axes [5].
HA has been applied to biomedical devices such as artificial bones and implants and to the chromatographic stationary phase due to its high protein adsorption ability [6,7]. Currently, research is being conducted using HA as a drug delivery carrier due to its biocompatibility and protein adsorption ability [8,9]. HA exists in vivo as the Ca-deficient hydroxyapatite (CDHA) and carbonate-containing hydroxyapatite (CHA) structures [10], which can be artificially synthesized and controlled for biomimicry, and interest in the crystalline phases is growing.

3.1.2. Ca-Deficient Hydroxyapatite

CDHA is a type of apatite, and its chemical formula is shown below.
Ca 10 x HPO 4 x PO 4 6 x OH 2 x
The Ca/P molar ratio of CDHA is 1.33–1.67, making it more bioabsorbable than the case in the stoichiometric (Ca/P molar ratio of 1.67) HA, which is more similar to the apatite in biological bone. The formation of CDHA is largely related to the dissociation state of the phosphate ions [11,12]. Specifically, it has been reported that HA is formed under a higher proportion of PO43− in solution, whereas CDHA is formed under a higher proportion of HPO42− in solution [13]. With increasing pH during the synthesis, phosphate ions dissociate in the form of H3PO4→H2PO4→HPO42−→PO43−, indicating that HA and CDHA are formed under the higher (pH > 10) and lower (pH 6–8) pH conditions, respectively. The crystal structure of CDHA is shown in Figure 3. The comparison between Figure 2 and Figure 3 indicates that the crystal structure of CDHA is almost identical to that of HA [14]. Specifically, the Ca(I) sites of HA become the vacancies, and part of the PO43− becomes HPO42−, so the crystal structure remains almost unchanged compared to the case in HA. It has been reported that the phase transitions occur to form β-phase tricalcium phosphate (β-TCP) at 650–750 °C and to form α-TCP at 1180 °C [15,16]. Moreover, CDHA can also be synthesized by the hydrolysis of α-TCP. These characteristics have significantly promoted the research of CDHA particulation, which is applied to the DDS nanocarriers [17,18]. These reports are related to the CDHA/organic interface hybrid design, suggesting that organic molecules are immobilized on the CDHA surface.

3.1.3. Carbonate-Substituted Hydroxyapatite

CHA represents all HA structures containing carbonate ions. In this case, the carbonate ions are present through adsorption on the HA surfaces and substitution within the crystal structure. CHA has been known to exhibit higher solubility than HA at lower pH (pH < 7) and has been applied to bone replacement materials [19]. CHA is stable at higher pH (pH > 10). Thus, there are various carbonate ion contents, with biological bone containing approximately 2.3–8 wt% of carbonate ions, and many studies have been conducted in this concentration range [20,21]. The apatite with the carbonate ions substituted within the crystal structures is called carbonate apatite. The carbonate apatite is classified into three types: HA with the carbonate ions substituted with the OH site, as shown in Figure 4, is called type A CHA, and its chemical formula is expressed as follows.
Ca 10 PO 4 6 OH 2 2 x CO 3 x
Type A CHA can be synthesized by heating HA at around 1000 °C in a carbon dioxide atmosphere and does not precipitate in most lower-temperature synthesis in the wet process [22]. With increasing CO32− content, an increase in the a-axis and a decrease in the c-axis of the lattice constants have been observed. When the substitution of CO32− reaches the maximum content of 4.4 wt%, the a-axis increases by 0.0025 nm for every 1 wt% increase [23].
The apatite with carbonate ions substituted at the PO43− site is called type B CHA, and its chemical formula is expressed as follows.
Ca 10 x / 2 PO 4 6 x CO 3 x OH 2
Type B CHA can be synthesized by wet process at lower temperatures (≈body temperature at around 40 °C) [24], with the loss of Ca2+ and OH through the substitution of CO32− for the charge compensation, and CO32− is eventually replaced by HPO42−. For each 1 wt% substitution of CO32−, the a-axis decreases by 0.00006 nm and the c-axis increases in length, and it has been reported that the substitution amount of CO32− can be as high as 22.2 wt% [25]. The substitutions at both sites are called type AB CHA [26]. CHA and CDHA particles have been investigated as nanocarriers for DDS based on the CHA/organic interface design [27,28].

3.2. Amorphous Silica Particles

3.2.1. Features

Silica is the generic term for silicon dioxide, in which oxygen and silicon are abundant elements on the earth [29]. Especially, silica particles exist in various forms as crystalline [30] and amorphous states [31]. In particular, amorphous silica particles are usually converted into the high-purity quartz glass, sol, gel and fumed silica, and then have a wide range of applications such as semiconductor encapsulation fillers, liquid crystal display materials [32,33,34,35,36], reinforcing fillers for elastomers and polymers, and key materials in the biomedical field [37,38]. The representative production methods include the melting method [39], the sol-gel method [40] as the liquid-phase method, and the Vapor-Phase-Axial-Deposition (VAD) method as the gas-phase method [41] (Figure 5).
In the melting method to obtain the amorphous silica particles, quartz powder as the starting material is filled in carbon cases and melted using electricity or flames (Figure 5a) [43]. In the electric melting, the particles are melted by electric resistance heating using carbon electrodes [44]. In flame melting, the particles are obtained by melting with an oxygen-hydrogen flame. The sol-gel method is the direct synthesis of the particles using solutions of inorganic and organic metal salts as the starting materials through hydrolysis and condensation polymerization reactions [45,46]. The reactions proceed to form the sol, which then undergoes further reactions to form the gel. The gel is dried at 40–120 °C, then heated and sintered at 900–1200 °C to produce amorphous silica particles (Figure 5b) [47]. The VAD method uses silicon tetrachloride (SiCl4) as the starting material and supplies oxygen-hydrogen gas from the burner to obtain the porous matrix, on which the amorphous silica particles formed in the flame are deposited (Figure 5c) [48,49]. Since the process is carried out through a porous matrix, the quality of the synthesized particles can be controlled depending on the sintering process and the presence or absence of the matrix modification process. For example, it is possible to obtain the halogen-containing particles by adding halogen elements to the sintering atmosphere [50,51]. Moreover, the porous matrix is sintered in the atmosphere with a lower moisture content, resulting in the synthesis of particles with lower concentrations of silanol groups and impurities. Thus, the structure and surface properties of the particles depend on the synthetic method, and the selection is important for the applications.

Structure and Surfaces

The silica network of the amorphous silica particles consists of the structures in which the SiO4 tetrahedral units are irregularly connected to each other through the O atom [52,53,54,55]. There are two main functional groups of the siloxane bond (≡Si–O–Si≡) and the silanol group (≡Si–OH) (Figure 6) [56,57,58].
Siloxane bonds are present from the interior to the top of the particles and are the main chains of the network. Their bond angle range is 120–180° [59,60,61], which allows for a variety of ring structures, including three-, four-, six-, and eight-membered rings [62,63,64,65]. Depending on the bond angles and bond distortions, there are stable or unstable ring structures. Particularly, the planar three-membered ring structure is unstable and is easily hydrolyzed by water molecules [66].
Silanol groups are generally numerous on the amorphous silica particles and can be classified as single, geminal, and triple types when the number of OH groups attached to the Si atom is one, two, or three, respectively [67,68,69]. There are also vicinal silanol groups, which are present with two or more silanol groups in close contact to form hydrogen bonds with each other [70]. Particularly, the presence of silanol groups is an important parameter that determines the physicochemical properties of the particles (e.g., the molecular adsorption sites). Silanol groups interact with polar molecules such as water molecules, which form hydrogen bonds with silanol groups and with other molecules that exhibit hydrogen bond-forming ability [71,72,73,74]. The pH environment causes the different dissociation behaviors of the protons from the silanol groups on the particles, resulting in the changes in surface charge [75,76]. The isoelectric point of amorphous silica particles is around pH 2.0, and in biological fluids at pH 7.4, they have dispersibility due to their electrostatic repulsion of negative charges around −50 mV [77,78]. The higher surface reactivity of silanol groups is an important parameter for applications in biomedical fields [79,80,81,82,83].

3.2.2. Biofunctionalization

The surface functions of amorphous silica particles as bioceramics are given in this section. First, bioglasses (e.g., Na2O-CaO-SiO2-P2O5) containing amorphous silica particles (<50 mol%) have been known to show osteoconductive properties [84,85,86,87]. In the biological fluid, Na+, Ca2+, and phosphate ions are first eluted from the bioglass. Subsequently, the amorphous silica particles on the bioglass form a gel layer, which is the starting point for the adsorption of Ca2+ ions. As a result, HA is efficiently precipitated and adhered to biological bone, which has been used as the bone replacement material. Then, amorphous silica particles could induce the production of nutrients for all organs in vivo and have been developed for use in supplemental food products [88,89,90,91]. For example, they promote collagen production in vivo and improve the bonding between collagen and elastin in skin and bone [92,93,94]. Amorphous silica particles have attracted attention as cosmetic ingredients because of their activation of fibroblast functions. For the applications, the protein adsorption form in vivo on surface functions such as silanol groups of amorphous silica particles should be important for the biofunctions in biomedical fields. However, the immobilization states of amorphous silica particles have not yet been clarified. If the immobilization states can be clarified, a wide range of biological and medical applications can be achieved.

3.2.3. Application for Antibody Protein Immobilization

With the biomedical applications of amorphous silica particles, the antibody test kits and the carriers for the immobilization in immunochromatography can be proposed [95,96]. In the applications, the immobilization of antibody proteins on the particles should be considered to improve their functions. Immunoglobulins are known as antibody proteins with immune functions (Figure 7a) [97,98]. The antibody proteins consist of two heavy chains (H chain: 50–77 kDa) and two light chains (L chain: 25 kDa), which are connected to each other by disulfide bonds and form the Y-shape [99,100,101]. They recognize and specifically bind to antigen (i.e., antigen–antibody reactions) [102,103,104]. The V-shaped part of the Y-shaped arm is termed as Fab (Fragment antigen binding) domain, and the body part is known as the Fc (Fragment crystallizable) domain [100]. Immunity is acquired when phagocytes recognize the antibodies that have interacted with antigens through binding of the Fc region to phagocyte receptors, resulting in the production of large amounts of antibody proteins in biological fluids [105,106,107]. The variable site of the antibody that recognizes the antigen has been called the antigenic determinant (epitope) and consists of several amino acids [108,109]. The most numerous antibody protein in human blood and biological fluids is immunoglobulin G (IgG), which accounts for about 80% of the total and is approximately [110] 14.5 nm × 8.5 nm × 4.0 nm in size [111]. Immunoassays using these antibody proteins are used for antibody testing [112,113]. Immunochromatography and ELISA are the two main types of immunoassays [114,115,116]. Immunoassays are characterized by the immobilization of antibody proteins on particulate substrates. If the antibody proteins are denatured due to immobilization, it becomes difficult to form binding between the antibody protein and the target antigen, thus adversely affecting the sensitivity of the test (Figure 7b) [117,118]. The orientation of IgG at immobilization is important for immunoassay efficiency. Specifically, it has been reported that by coating glass with n-butyl methacrylate, the adsorbed orientation was controlled by the temperature [119]. Furthermore, in the case of bioceramics, the zirconia particles modified with phosphate groups enable the selective adsorption of amino groups from the Fab and Fc regions via electrostatic interactions, suggesting astate where only one Fab region is exposed on the surface [120]. Accordingly, the controlled orientation of the IgG on the amorphous silica particles will be the future challenge. In recent years, the use of amorphous silica particles as immobilization carriers for antibody proteins has been investigated. In conventional particles, the direct interactions with silanol groups on the particles are thought to result in denaturation, leading to lower sensitivity of the immunoassays [121,122]. In fact, there have been cases where IgG has been adsorbed on hydrophilic silica glass, and the subsequent immune response has been investigated. However, the immobilized IgG might have been denatured, as the phagocytic response was completely inhibited [123]. In other words, the challenge for applications such as antibody test kits is to immobilize antibody proteins (IgG) sterically, with a focus on inhibiting direct interactions with the surface of amorphous silica particles.

4. The Surface Layer Formed on the Bioceramic Particles

4.1. Formation of the Surface Layer in Biological Fluids

When considering the immobilization states of antibody proteins on bioceramic particles (e.g., amorphous silica particles), the hydration layer formed at the interfaces between the particles and proteins is very important [124,125]. The hydration layer is formed by the adsorption of water molecules and ions on the bioceramics in biological fluids (Figure 8). Various factors contribute to the formation of the hydration layer, which is mediated between ions and bioceramic surfaces through electrostatic interactions and hydrogen bonding. The hydration layer is composed of three types (i.e., non-freezing water, intermediate water, and free water) [126], which have been mainly investigated in the biopolymers, and this theory has recently also been applied to the bioceramics. Non-freezing water and intermediate water showed direct interactions with bioceramics, reducing the hydrogen bonds between water molecules, resulting in enhanced and maintained dynamics of water molecules with decreasing temperature. In free water, hydrogen bonds are formed between water molecules below 0 °C, and the molecular motion stops and freezing occurs. The differences are due to the strength of interactions acting on the bioceramic surfaces, resulting in different kinetic properties, which can be evaluated by differential scanning calorimetry (DSC) and 1H-NMR [127]. According to the DSC measurement, non-freezing water does not freeze at −100 °C, and intermediate water has been reported to be cold recrystallized at lower temperatures below 0 °C with increasing temperature [128]. Free water is the water that melts from its frozen state at 0 °C and interacts weakly with bioceramic surfaces and non-freezing water. The hydration layer shows the recombination behavior from femtoseconds to picoseconds to form the amorphous structures in a very short time and shows the randomness of the liquid on a longer time scale. Therefore, the relaxation times (τc) of non-freezing water, intermediate water, and free water obtained by 1H-NMR are 10−8–10−6, 10−10–10−9, and 10−12–10−11 s, respectively. When stronger interactions with the bioceramic surface are observed, the kinetics will be lowered [129]. According to the FT-IR spectra, the absorption bands (vIR) of the stretching vibrations of hydroxyl groups corresponding to non-freezing water, intermediate water, and free water are observed at 3600 cm−1, 3400 cm−1 and 3200 cm−1, respectively. The vIR has been evaluated by the spectral deconvolution and separation techniques [129,130].

4.2. Formation of the Surface Layer in Biological Fluids

After the hydration layer is formed on the bioceramics, the protein immobilization layer is formed by recognizing the hydration layer states [132]. In order to consider the protein immobilization states, it is necessary to consider the balance of the hydration layer components composed of non-freezing, intermediate, and free waters (Figure 9). The importance of the balance was supported by the fact that the denaturation of proteins in vivo was observed on the biopolymer without intermediate water in the hydration layer. The relationship between the adsorbed proteins and the hydration layers has recently been applied to bioceramics. For example, our research group has reported that the fibrinogen was sterically adsorbed on the elliptical HA nanocrystals due to the reduced proportion of non-freezing water components [133]. When the silicate ion-containing HA (SiHA) was immersed in biological fluid, the proportion of free water components effectively increased due to the enhanced elution of carbonate ions from the surfaces [134]. Then, the fibrillation of the adsorbed collagen on SiHA was inhibited due to the repulsion between the intermediate waters, thus inducing the steric adsorption of collagen molecules on the surfaces [135]. Therefore, the control of the proportion of hydration layer components is important for the steric adsorption of proteins such as immunoglobulins. Therefore, the sterility of protein immobilization is largely affected by the fraction of each hydration layer component. Furthermore, the immobilization, which maintains the highly ordered structure of the proteins, also affects subsequent cell adhesion. For example, cell adhesion is promoted on the fibronectin adsorbed while maintaining its highly ordered structure on the HA surfaces [136]. Also, the cell-adhesive proteins adsorbed on citric acid-modified HA films, maintaining their higher-order structure, enhanced the growth of the osteoblasts [135]. Thus, the adsorbed state of proteins effectively determines the functions of adhered cells.

4.3. Formation of the Non-Apatitic Layer and Protein Immobilization Ability

The non-apatitic layer has been investigated by FT-IR and NMR spectra, etc. In the FT-IR spectra, the absorption band corresponding to the non-apatitic layer is usually observed at 680−480 cm−1, which has been assigned to phosphate ions (e.g., PO43− and HPO42−) [137,138]. In terms of the coordination environment and interactions of phosphate ions, 2D solid-state NMR has demonstrated that the HA nanocrystal surfaces were composed of a non-apatitic layer composed of amorphous calcium phosphate (Figure 10) [139,140,141]. The exposed ions on the non-apatitic layer were strongly bound with the O atoms of the H2O molecules, partially forming the lewis acidity, indicating the highly reactive surfaces of the non-apatitic layer [142,143]. The ions on the non-apatitic layer were stabilized by the hydration layer, effectively constructing the hydrogen bonding network [143,144]. The non-apatitic layers are involved in the growth and ion exchange of the inner HA nanocrystal core as well as the adsorption of organic ions [145]. For example, the interfacial phenomena between non-apatitic layers and biological fluids are induced in vivo, resulting in the calcification of teeth and bones [146,147,148,149,150]. It is thought that the interfacial phenomena are effectively caused by the ions contained in the non-apatitic layer (i.e., the state of the hydration layer), leading to the protein adsorption states. The ions contained in the non-apatitic layer are important in this sequence of interfacial mechanisms. The silicate and carbonate ions contained in the non-apatitic layer cause the structural defects in the HA nanocrystals, thereby increasing the solubility of the ions in vivo [151,152,153]. The increased solubility of the ions expands the hydrogen bonding network and changes the proportion of the hydration layer component, thus controlling the adsorption states of the protein. Moreover, it has been reported that the presence of ions in the non-apatitic layer on HA nanocrystals facilitates the elution of carbonate ions from the non-apatitic layer, increasing the proportion of free water components in the hydration layer [133]. Therefore, ions in the non-apatitic layer are thought to alter the hydration layer state and affect the protein immobilization state.
The immobilization of proteins on HA nanocrystals is affected by the interactions between the ions in the non-apatitic layer and the functional groups of the proteins. For example, it has been reported that the immobilization of pepsin on the spherical HA nanocrystals modified with cetylpyridinium chloride caused the denaturation due to the Cl ion diffusion into pepsin [154]. Thus, the ions in the non-apatitic layer can affect the protein immobilization states. Therefore, the non-apatitic layer is thought to be involved in the steric properties of organic molecules and proteins adsorbed on HA nanocrystals, and the protein immobilization states affect the biological functions. For example, the ionic species on the surfaces of HA nanocrystals can control the orientation (i.e., steric state) of adsorption and immobilization of anionic porphyrins [155]. It has also been reported that the adsorbed state of human serum albumin (HSA) on HA nanocrystals with carbonate ions in the non-apatitic layer has a lower proportion of the random coils in the protein secondary structures as compared to the case in HSA in the native state [156]. Furthermore, the steric immobilization of bone morphogenetic protein (BMP-2) and antibody proteins involved in the immunization has also been reported on pure HA nanocrystals [157,158].
As described above, the non-apatitic layer on the HA nanocrystal core surface can sterically immobilize nucleic acids and proteins, which can be applied to the surface modification of protein chromatography columns [159,160]. Therefore, water molecules and ions in the non-apatitic layer would induce the steric immobilization states, although further detailed investigation is needed.

4.4. Amorphous Silica Particles for the New Layer Formation

As mentioned above, the formation of a surface layer consisting of water molecules and ions similar to the non-apatitic layer leads to the steric immobilization of proteins. Among the ions contained in the non-apatitic layer, phosphate, Na+, and Cl ions play important roles in biological reactions. Phosphate ions are the main component of the HA nanocrystal, and it is believed that the adsorption states of ions on HA during the nucleation stage are important [5]. Na+ ions in the non-apatitic layer provide excellent osteoconductivity to activate osteoblast growth [161]. In fact, there have been reports on the alkaline treatment of the titania surfaces to improve their reactivity with simulated body fluid (SBF). Surface treatment with 10 mM NaOH resulted in the formation of a sodium titanate layer on the surface. The Na+ ion contained in this layer caused the exchange with H3O+ ions in SBF, and the interfaces might be involved in inducing the steric immobilization of proteins [162,163,164,165]. Cl ions are also contained in the non-apatitic layer, showing excellent osteoconductivity [166]. The inclusion of various ions will improve the reactivity of amorphous silica particles, promote the adsorption of water molecules and ions in biological fluids, and facilitate the steric immobilization of proteins.
In order to form a surface layer composed of water molecules and ions similar to the non-apatitic layer, surface reactivity can be effectively improved by including chlorine in amorphous silica particles. The inclusion of chlorine into silica glass decreases the total amount of silanol groups, subsequently reducing transmission losses and improving the refractive index in the near-infrared light region (λ > 1064 nm) [167]. In the VAD method, chlorine can be contained in amorphous silica particles. In particular, the porous matrix is heat-treated in a mixed atmosphere of chlorine compound vapors with inert gases such as H2, Ne, and N2 to resultantly achieve inclusion [168]. Here, the two main types of chlorine compound vapors are silicon tetrachloride and chlorine gases. The concentration of chlorine content in silicon tetrachloride gas is higher than that in chlorine gas. In the case of silicon tetrachloride gas, the inclusion concentration of chlorine in the base material can be proportional to 1/4 of the added silicon tetrachloride concentration. It has been reported that the reaction proceeds according to the following chemical equilibrium (Equation (1)).
SiCl4 + 3SiO2 ⇆ 4SiO1.5Cl
where SiO2 indicates the porous matrix. Furthermore, when chlorine is contained in amorphous silica particles, the chemical formula is SiO1.5Cl [169]. When chlorine gas is used, the inclusion concentration of chlorine in amorphous silica particles is low. Considering this and (Equation (2)), the reaction between the porous matrix and chlorine is required to use silicon tetrachloride. Therefore, the introduction of chlorine components into amorphous silica particles with the chlorine gas are the following two-step reactions.
2Cl2 + SiO2 ⇆ SiCl4 + O2
SiCl4 + 3SiO2 ⇆ 4SiO1.5Cl
Here, when chlorine gas is used, the presence of oxygen in the heat treatment makes it difficult to generate silicon tetrachloride according to chemical equilibrium. Thus, it is necessary to reduce the oxygen concentration in the reaction furnace.
Chlorine has been reported to be contained in amorphous silica particles in various forms, as shown in Figure 11. Among them, the ≡Si–Cl bond (Figure 11a) is considered to be the most common structure [170]. Here, the ≡Si–Cl bond has been reported to form the weak hydrogen bond, which was observed in the FT-IR spectra at 2810 cm−1 [171,172].
The molecular Cl2 in the interstitial lattice (Figure 11b) [173], the complexes consisting of the four ≡Si–Cl bonds known as the defect centers (Figure 11c) [174], the atomic Cl in the interstitial lattice (Figure 11d) [174], and the SiCl2 bond defects formed by the bonding to the two-coordinated silicon atoms (Figure 11e) [175] have been reported. Particularly, the ≡Si–Cl bonds on the surfaces can enhance the adsorption of water molecules and ions in biological fluids. Specifically, the ≡Si–Cl bonds are highly electronegative and can form weak hydrogen bonds. Then, the adsorption of Na+ and phosphate ions from biological fluids is thought to enhance the formation of the surface layer (Figure 12) [171,172]. As a result, the adsorption of water molecules and ions would be enhanced as compared to the case in conventional amorphous silica particles, leading to the formation of a surface layer similar to the non-apatitic layer and a steric immobilization state of proteins. In fact, the surface layer composed of water molecules and ions formed on the chlorine-containing silica particles in our group, leading to an increase in the amount of immobilized protein. Additionally, the protein was successfully immobilized while preserving its highly ordered structure [42].

5. Conclusions

In this review article, the research on the surface design of bioceramic particles is described and highlighted. The studies on the relationship between the surface properties of bioceramic particles and the protein immobilization states were deepened. We hope that the surfaces of bioceramic particles can effectively act on proteins and cells, which can be applied to DDS and achieve the phenomenon of ultra-early tissue regeneration. Furthermore, this technology can also be applied to the surface design of bioceramics for bone regenerative therapy. Particularly, osteoblasts recognize and adhere to the pre-immobilized cell-adhesive proteins in maintaining their highly ordered structures, indicating the importance of the studies on the interfacial properties between the bioceramic particle surfaces and proteins. In the future, research on surface design with positive effects on biological tissues is expected to contribute to the construction of social infrastructure that promotes health and vitality.

Author Contributions

Conceptualization, R.K. and M.T.; Writing of the manuscript, R.K., D.N. and R.A.; review and editing, Z.L. and W.S.; Visualization, D.N. and W.S.; Supervision, M.T. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflicts of interests.

References

  1. Olszta, M.J.; Cheng, X.; Jee, S.S.; Kumar, R.; Kim, Y.-Y.; Kaufman, M.J.; Douglas, E.P.; Gower, L.B. Bone Structure and Formation: A New Perspective. Mater. Sci. Eng. R Rep. 2007, 58, 77–116. [Google Scholar] [CrossRef]
  2. Sasaki, S. Non-Collagenous Proteins in Bone. J. Bone Miner. Metab. 1981, 4, 323–326. [Google Scholar]
  3. Chai, Y.; Zhou, Y.; Tagaya, M. Rubbing-Assisted Approach for Fabricating Oriented Nanobiomaterials. Micromachines 2022, 13, 1358. [Google Scholar] [CrossRef] [PubMed]
  4. Kay, M.I.; Young, R.A.; Posner, A.S. Crystal Structure of Hydroxyapatite. Nature 1964, 204, 1050–1052. [Google Scholar] [CrossRef] [PubMed]
  5. Ratnayake, J.T.B.; Mucalo, M.; Dias, G.J. Substituted Hydroxyapatites for Bone Regeneration: A Review of Current Trends. J. Biomed. Mater. Res. B Appl. Biomater. 2017, 105, 1285–1299. [Google Scholar] [CrossRef] [PubMed]
  6. Kawasaki, T. Theory of Chromatography on Hydroxyapatite Columns with Small Loads. J. Chromatogr. A 1978, 157, 7–42. [Google Scholar] [CrossRef]
  7. Brown, W.E.; Eidelman, N.; Tomazic, B. Octacalcium Phosphate as a Precursor in Biomineral Formation. Adv. Dent. Res. 1987, 1, 306–313. [Google Scholar] [CrossRef]
  8. Shinto, Y.; Uchida, A.; Korkusuz, F.; Araki, N.; Ono, K. Calcium Hydroxyapatite Ceramic Used as a Delivery System for Antibiotics. J. Bone Joint Surg. Br. 1992, 74-B, 600–604. [Google Scholar] [CrossRef]
  9. Otsuka, M.; Matsuda, Y.; Yu, D.; Wong, J.; Fox, J.L.; Higuchi, W.I. A Novel Skeletal Drug Delivery System for Anti-Bacterial Drugs Using Self-Setting Hydroxyapatite Cement. Chem. Pharm. Bull. 1990, 38, 3500–3502. [Google Scholar] [CrossRef]
  10. Zapanta LeGeros, R. Apatites in Biological Systems. Prog. Cryst. Growth Charact. 1981, 4, 1–45. [Google Scholar] [CrossRef]
  11. Ishikawa, K.; Ducheyne, P.; Radin, S. Determination of the Ca/P Ratio in Calcium-Deficient Hydroxyapatite Using X-ray Diffraction Analysis. J. Mater. Sci. Mater. Med. 1993, 4, 165–168. [Google Scholar] [CrossRef]
  12. Dorozhkina, E.I.; Dorozhkin, S.V. Mechanism of the Solid-State Transformation of a Calcium-Deficient Hydroxyapatite (CDHA) into Biphasic Calcium Phosphate (BCP) at Elevated Temperatures. Chem. Mater. 2002, 14, 4267–4272. [Google Scholar] [CrossRef]
  13. Shen, Y.; Semon, J.A.; Brow, R.K. Conversion of Borate Glass Microspheres to Hollow Biphasic Calcium Phosphate Ceramic Microspheres for Bone Defects. J. Am. Ceram. Soc. 2022, 105, 7211–7227. [Google Scholar] [CrossRef]
  14. Camire’, C.L.; Jegou Saint-Jean, S.; Hansen, S.; McCarthy, I.; Lidgren, L. Hydration Characteristics of Alpha-Tricalcium Phosphates: Comparison of Preparation Routes. J. Appl. Biomater. Biomech. 2005, 3, 106–111. [Google Scholar] [CrossRef] [PubMed]
  15. Bohner, M.; Santoni, B.L.G.; Döbelin, N. β-Tricalcium Phosphate for Bone Substitution: Synthesis and Properties. Acta Biomater. 2020, 113, 23–41. [Google Scholar] [CrossRef] [PubMed]
  16. Carrodeguas, R.G.; De Aza, S. α-Tricalcium Phosphate: Synthesis, Properties and Biomedical Applications. Acta Biomater. 2011, 7, 3536–3546. [Google Scholar] [CrossRef] [PubMed]
  17. LIU, T.; CHEN, S.; LIU, D.; LIOU, S. On the Study of BSA-Loaded Calcium-Deficient Hydroxyapatite Nano-Carriers for Controlled Drug Delivery. J. Control. Release 2005, 107, 112–121. [Google Scholar] [CrossRef] [PubMed]
  18. Al-Kattan, A.; Girod-Fullana, S.; Charvillat, C.; Ternet-Fontebasso, H.; Dufour, P.; Dexpert-Ghys, J.; Santran, V.; Bordère, J.; Pipy, B.; Bernad, J.; et al. Biomimetic Nanocrystalline Apatites: Emerging Perspectives in Cancer Diagnosis and Treatment. Int. J. Pharm. 2012, 423, 26–36. [Google Scholar] [CrossRef] [PubMed]
  19. Ishikawa, K.; Hayashi, K. Carbonate Apatite Artificial Bone. Sci. Technol. Adv. Mater. 2021, 22, 683–694. [Google Scholar] [CrossRef]
  20. Bigi, A.; Cojazzi, G.; Panzavolta, S.; Ripamonti, A.; Roveri, N.; Romanello, M.; Noris Suarez, K.; Moro, L. Chemical and Structural Characterization of the Mineral Phase from Cortical and Trabecular Bone. J. Inorg. Biochem. 1997, 68, 45–51. [Google Scholar] [CrossRef]
  21. Driessens, F.C.M. The Mineral in Bone, Dentin and Tooth Enamel. Bull. Sociétés Chim. Belg. 2010, 89, 663–689. [Google Scholar] [CrossRef]
  22. Young, R.A.; Bartlett, M.L.; Spooner, S.; Mackie, P.E.; Bonel, G. Reversible High Temperature Exchange of Carbonate and Hydroxyl Ions in Tooth Enamel and Synthetic Hydroxyapatite. J. Biol. Phys. 1981, 9, 1–26. [Google Scholar] [CrossRef]
  23. Young, R.A. Biological Apatite vs Hydroxyapatite at the Atomic Level. Clin. Orthop. Relat. Res. 1975, 113, 249–262. [Google Scholar] [CrossRef] [PubMed]
  24. Bel Hadj Yahia, F.; Jemal, M. Synthesis, Structural Analysis and Thermochemistry of B-Type Carbonate Apatites. Thermochim. Acta 2010, 505, 22–32. [Google Scholar] [CrossRef]
  25. LeGeros, R.Z.; Trautz, O.R.; Klein, E.; LeGeros, J.P. Two Types of Carbonate Substitution in the Apatite Structure. Experientia 1969, 25, 5–7. [Google Scholar] [CrossRef] [PubMed]
  26. Combes, C.; Cazalbou, S.; Rey, C. Apatite Biominerals. Minerals 2016, 6, 34. [Google Scholar] [CrossRef]
  27. Kataoka, T.; Samitsu, S.; Okuda, M.; Kawagoe, D.; Tagaya, M. Highly Luminescent Hydroxyapatite Nanoparticles Hybridized with Citric Acid for Their Bifunctional Cell-Labeling and Cytostatic Suppression Properties. ACS Appl. Nano Mater. 2020, 3, 241–256. [Google Scholar] [CrossRef]
  28. Kataoka, T.; Hashimoto, T.; Shi, W.; Tagaya, M. Investigation of the Surface Elution Mechanism of Citric Acid-Coordinated Hydroxyapatite Nanoparticles in Biological Solutions. Ind. Eng. Chem. Res. 2022, 61, 10915–10921. [Google Scholar] [CrossRef]
  29. Heyde, M.; Shaikhutdinov, S.; Freund, H.J. Two-Dimensional Silica: Crystalline and Vitreous. Chem. Phys. Lett. 2012, 550, 1–7. [Google Scholar] [CrossRef]
  30. Weissenrieder, J.; Kaya, S.; Lu, J.L.; Gao, H.J.; Shaikhutdinov, S.; Freund, H.J.; Sierka, M.; Todorova, T.K.; Sauer, J. Atomic Structure of a Thin Silica Film on a Mo(112) Substrate: A Two-Dimensional Network of SiO4 Tetrahedra. Phys. Rev. Lett. 2005, 95, 076103. [Google Scholar] [CrossRef]
  31. Cho, W.S.; Choi, M.; Han, B.S.; Cho, M.; Oh, J.H.; Park, K.; Kim, S.J.; Kim, S.H.; Jeong, J. Inflammatory Mediators Induced by Intratracheal Instillation of Ultrafine Amorphous Silica Particles. Toxicol. Lett. 2007, 175, 24–33. [Google Scholar] [CrossRef]
  32. Boissière, C.; Kümmel, M.; Persin, M.; Larbot, A.; Prouzet, E. Spherical MSU-1 Mesoporous Silica Particles Tuned for HPLC. Adv. Funtional Mater. 2001, 11, 129–135. [Google Scholar] [CrossRef]
  33. Liu, C.C.; Maciel, G.E. The Fumed Silica Surface: A Study by NMR. J. Am. Chem. Soc. 1996, 118, 5103–5119. [Google Scholar] [CrossRef]
  34. Smith, D.M.; Scherer, G.W.; Anderson, J.M. Shrinkage during Drying of Silica Gel. J. Non-Cryst. Solids 1995, 188, 191–206. [Google Scholar] [CrossRef]
  35. Feuston1, B.P.; Garofalini, S.H. Oligomerization in Silica Sols. J. Phys. Chem. 1990, 94, 5351–5356. [Google Scholar] [CrossRef]
  36. Saito, K.; Ikushima, A.J. Reduction of Light-Scattering Loss in Silica Glass by the Structural Relaxation of “‘Frozen-in’” Density Fluctuations. Appl. Phys. Lett. 1997, 70, 3504–3506. [Google Scholar] [CrossRef]
  37. Merget, R.; Bauer, T.; Küpper, H.; Philippou, S.; Bauer, H.; Breitstadt, R.; Bruening, T. Health Hazards Due to the Inhalation of Amorphous Silica. Arch. Toxicol. 2002, 75, 625–634. [Google Scholar] [CrossRef]
  38. David, L. Griscom And Fission-Reactor Radiation Effects on the Visible-Range Transparency of Aluminum-Jacketed, All-Silica Optical Fibers. J. Appl. Phys. 1996, 80, 2142–2155. [Google Scholar]
  39. Kikuchi, Y.; Sudo, H.; Kuzuu, N. Thermal Expansion of Vitreous Silica: Correspondence between Dilatation Curve and Phase Transitions in Crystalline Silica. J. Appl. Phys. 1997, 82, 4121–4123. [Google Scholar] [CrossRef]
  40. Singh, L.P.; Bhattacharyya, S.K.; Kumar, R.; Mishra, G.; Sharma, U.; Singh, G.; Ahalawat, S. Sol-Gel Processing of Silica Nanoparticles and Their Applications. Adv. Colloid. Interface Sci. 2014, 214, 17–37. [Google Scholar] [CrossRef] [PubMed]
  41. Koilketsu, N.; Awazu, K.; Wape, H.; Ypmne, B. Llminescence Centers in SiO2 and SiO2: Geop Vad Rods Si-under Reducing or Oxidizing Conditions. J. Non Cryst. Solids 1987, 95, 679–684. [Google Scholar] [CrossRef]
  42. Kimura, R.; Chatani, S.; Inui, M.; Motozuka, S.; Liu, Z.; Tagaya, M. Control of Biological Surface States on Chlorine-Doped Amorphous Silica Particles and Their Effective Absorptive Ability for Antibody Protein. Langmuir 2024, 40, 8939–8949. [Google Scholar] [CrossRef]
  43. Kuzuu, N.; Horikoshi, H.; Nishimura, T.; Kokubo, Y. Effects of Heat Treatment on Absorption Bands in OH-Free and OH-Contalning Fused Quartz. J. Appl. Phys. 2003, 93, 9062–9071. [Google Scholar] [CrossRef]
  44. Brockner, R. Properties and structure of vitreous silica. I. J. Non-Cryst. Solids 1970, 5, 123–175. [Google Scholar] [CrossRef]
  45. Sacks, M.D.; Sheu, R.-S. Rheological properties of silica sol-gel materials. J. Non-Cryst. Solids 1987, 92, 383–396. [Google Scholar] [CrossRef]
  46. Kobayashi, Y.; Correa-Duarte, M.A.; Liz-Marzán, L.M. Sol-Gel Processing of Silica-Coated Gold Nanoparticles. Langmuir 2001, 17, 6375–6379. [Google Scholar] [CrossRef]
  47. Ciriminna, R.; Sciortino, M.; Alonzo, G.; De Schrijver, A.; Pagliaro, M. From Molecules to Systems: Sol-Gel Microencapsulation in Silica-Based Materials. Chem. Rev. 2011, 111, 765–789. [Google Scholar] [CrossRef]
  48. Horender, S.; Lipowsky, J.; Sommerfeld, M.; Schwerin, M.; Badeke, K.U. Deposition of SiO2 Nanoparticles Produced in a Turbulent H2/O2 Flame. Aerosol Sci. Technol. 2008, 42, 873–883. [Google Scholar] [CrossRef]
  49. Sekiya, E.H.; Torikai, D.; Gusken, E.; Ogata, D.Y.; Cuevas, R.F.; Suzuki, C.K. Crystalline and Amorphous Phases of GeO 2 in VAD Silica±germania Soot Preform. J. Non-Cryst. Solids 2000, 273, 228–232. [Google Scholar] [CrossRef]
  50. Butov, O.V.; Golant, K.M.; Tomashuk, A.L.; Van Stralen, M.J.N.; Breuls, A.H.E. Refractive Index Dispersion of Doped Silica for Fiber Optics. Opt. Commun. 2002, 213, 301–308. [Google Scholar] [CrossRef]
  51. Hammond, C.R.; Norman, S.R. Silica Based Binary Glass Systems-Refractive Index Behaviour and Composition in Optical Fibres. Opt. Quantum Electron. 1977, 9, 399–409. [Google Scholar] [CrossRef]
  52. Pereira, J.C.G.; Catlow, C.R.A.; Price, G.D. Silica Condensation Reaction: An Ab Initio Study. Chem. Commun. 1998, 13, 1387–1388. [Google Scholar] [CrossRef]
  53. **ao, Y.; Lasaga, A.C. Quantum Mechanical Studies of the Kinetics and Mechanisms of Silicate Dissolution: H + ( H30’) Catalysis. Geochim. Cosmochlmica Acta 1994, 58, 5379–5400. [Google Scholar] [CrossRef]
  54. Feya, O.D.; Wang, Q.; Lepeshkin, S.V.; Baturin, V.S.; Uspenskii, Y.A.; Oganov, A.R. Tetrahedral Honeycomb Surface Reconstructions of Quartz, Cristobalite and Stishovite. Sci. Rep. 2018, 8, 11947. [Google Scholar] [CrossRef]
  55. Loy, D.A.; Carpenter, J.P.; Alam, T.M.; Shaltout, R.; Dorhout, P.K.; Greaves, J.; Small, J.H.; Shea, K.J. Cyclization Phenomena in the Sol-Gel Polymerization of α,ω- Bis(Triethoxysilyl)Alkanes and Incorporation of the Cyclic Structures into Network Silsesquioxane Polymers. J. Am. Chem. Soc. 1999, 121, 5413–5425. [Google Scholar] [CrossRef]
  56. Pelmenschikov, A.; Strandh, H.; Pettersson, L.G.M.; Leszczynski, J. Lattice Resistance to Hydrolysis of Si-O-Si Bonds of Silicate Minerals: Ab Initio Calculations of a Single Water Attack onto the (001) and (111) β-Cristobalite Surfaces. J. Phys. Chem. B 2000, 104, 5779–5783. [Google Scholar] [CrossRef]
  57. Hair, M.L. Hydroxyl groups on silica surface. J. Non-Cryst. Solids 1975, 19, 299–309. [Google Scholar] [CrossRef]
  58. Cypryk, M.; Apeloig, Y. Mechanism of the Acid-Catalyzed Si-O Bond Cleavage in Siloxanes and Siloxanols. A Theoretical Study. Organometallics 2002, 21, 2165–2175. [Google Scholar] [CrossRef]
  59. Le Page, Y.; Calvert, L.D.; Gabe, E.J. Parameter variation in low-quartz between 94 and 298KtS. Phys. Chem. Solids 1980, 41, 721–725. [Google Scholar] [CrossRef]
  60. Lisovskii, I.P.; Litovchenko, V.G.; Lozinskii, V.G.; Steblovskii, G.I. IR Spectroscopic Investigation of SiO2 Film Structure. Thin Solid. Films 1992, 213, 164–169. [Google Scholar] [CrossRef]
  61. Janes, N.; Oldfield, E. Prediction of Silicon-29 Nuclear Magnetic Resonance Chemical Shifts Using a Group Electronegativity Approach: Applications to Silicate and Aluminosilicate Structures. J. Am. Chem. Soc. 1985, 107, 6769–6775. [Google Scholar] [CrossRef]
  62. Sharma, S.K.; Mammone, J.F.; Nicol, M.F. Raman Investigation of Ring Configurations in Vitreous Silica. Nature 1981, 292, 140–141. [Google Scholar] [CrossRef]
  63. Walrafen, G.E.; Hokmabadi, M.S.; Holmes, N.C.; Nellis, W.J.; Henning, S. Raman Spectrum and Structure of Silica Aerogel. J. Chem. Phys. 1985, 82, 2472–2476. [Google Scholar] [CrossRef]
  64. Pasquarello, A.; Car, R. Identification of Raman Defect Lines as Signatures of Ring Structures in Vitreous Silica. Phys. Rev. Lett. 1998, 80, 5145–5147. [Google Scholar] [CrossRef]
  65. Wallace, S.; West, J.K.; Hench, L.L. Interactions of Water with Trisiloxane Rings. I. Experimental Analysis. J. Non-Cryst. Solids 1993, 152, 101–108. [Google Scholar] [CrossRef]
  66. Vigil, G.; Xu, Z.; Steinberg, S.; Israelachvili, J. Interactions of Silica Surfaces. J. Colloid. Interface Sci. 1994, 165, 367–385. [Google Scholar] [CrossRef]
  67. Morrow, B.A.; Mcfarlan, A.J. Surface Vibrational Modes of Silanol Groups on Silica. J. Phys. Chem. 1992, 96, 1395–1400. [Google Scholar] [CrossRef]
  68. Warring, S.L.; Beattie, D.A.; McQuillan, A.J. Surficial Siloxane-to-Silanol Interconversion during Room-Temperature Hydration/Dehydration of Amorphous Silica Films Observed by ATR-IR and TIR-Raman Spectroscopy. Langmuir 2016, 32, 1568–1576. [Google Scholar] [CrossRef]
  69. Zhuravlev, L.T. The Surface Chemistry of Amorphous Silica. Zhuravlev Model. Colloids Surf. A Physicochem. Eng. Asp. 2000, 173, 1–38. [Google Scholar] [CrossRef]
  70. Dalstein, L.; Potapova, E.; Tyrode, E. The Elusive Silica/Water Interface: Isolated Silanols under Water as Revealed by Vibrational Sum Frequency Spectroscopy. Phys. Chem. Chem. Phys. 2017, 19, 10343–10349. [Google Scholar] [CrossRef] [PubMed]
  71. Smirnova, I.; Mamic, J.; Arlt, W. Adsorption of Drugs on Silica Aerogels. Langmuir 2003, 19, 8521–8525. [Google Scholar] [CrossRef]
  72. Kosmulski, M. Adsorption of Trivalent Cations on Silica. J. Colloid. Interface Sci. 1997, 195, 395–403. [Google Scholar] [CrossRef] [PubMed]
  73. Krysztafkiewicz, A.; Binkowski, S.; Jesionowski, T. Adsorption of Dyes on a Silica Surface. Appl. Surf. Sci. 2002, 199, 31–39. [Google Scholar] [CrossRef]
  74. Hair, M.L.; Hertl, W. Adsorption on Hydroxylated Silica Surfaces. J. Phys. Chem. 1969, 73, 4269–4276. [Google Scholar]
  75. De Keizer, A.; Van Der Ent, E.M.; Koopal, L.K. Surface and Volume Charge Densities of Monodisperse Porous Silicas. Colloids Surf. A Physicochem. Eng. Asp. 1998, 142, 303–313. [Google Scholar] [CrossRef]
  76. Kobayashi, M.; Juillerat, F.; Galletto, P.; Bowen, P.; Borkovec, M. Aggregation and Charging of Colloidal Silica Particles: Effect of Particle Size. Langmuir 2005, 21, 5761–5769. [Google Scholar] [CrossRef] [PubMed]
  77. Antonio Alves Júnior, J.; Baptista Baldo, J. The Behavior of Zeta Potential of Silica Suspensions. New J. Glass Ceram. 2014, 04, 29–37. [Google Scholar] [CrossRef]
  78. Franks, G.V. Zeta Potentials and Yield Stresses of Silica Suspensions in Concentrated Monovalent Electrolytes: Isoelectric Point Shift and Additional Attraction. J. Colloid. Interface Sci. 2002, 249, 44–51. [Google Scholar] [CrossRef] [PubMed]
  79. Tang, F.; Li, L.; Chen, D. Mesoporous Silica Nanoparticles: Synthesis, Biocompatibility and Drug Delivery. Adv. Mater. 2012, 24, 1504–1534. [Google Scholar] [CrossRef] [PubMed]
  80. Arcos, D.; Vallet-Regí, M. Sol-Gel Silica-Based Biomaterials and Bone Tissue Regeneration. Acta Biomater. 2010, 6, 2874–2888. [Google Scholar] [CrossRef]
  81. Jones, J.R. New Trends in Bioactive Scaffolds: The Importance of Nanostructure. J. Eur. Ceram. Soc. 2009, 29, 1275–1281. [Google Scholar] [CrossRef]
  82. Zhang, K.; Yan, H.; Bell, D.C.; Stein, A.; Francis, L.F. Effects of Materials Parameters on Mineralization and Degradation of Sol-Gel Bioactive Glasses with 3D-Ordered Macroporous Structures. J. Biomed. Mater. Res. A 2003, 66, 860–869. [Google Scholar] [CrossRef]
  83. Manzano, M.; Vallet-Regí, M. Mesoporous Silica Nanoparticles for Drug Delivery. Adv. Funct. Mater. 2020, 30, 1902634. [Google Scholar] [CrossRef]
  84. Wilson, J.; Pigott, G.H.; Schoen, F.J.; Hench, L.L. Toxicology and Biocompatibility of Bioglasses. J. Biomed. Mater. Res. 1981, 15, 805–817. [Google Scholar] [CrossRef] [PubMed]
  85. Ogino, M.; Ohuchi, F.; Hench, L.L. Compositional Dependence of the Formation of Calcium Phosphate Films on Bioglass. J. Biomed. Mater. Res. 1980, 14, 55–64. [Google Scholar] [CrossRef] [PubMed]
  86. Xynos, I.D.; Hukkanen, M.V.J.; Batten, J.J.; Buttery, L.D.; Hench, L.L.; Polak, J.M. Bioglass ®45S5 Stimulates Osteoblast Turnover and Enhances Bone Formation In Vitro: Implications and Applications for Bone Tissue Engineering. Calcif. Tissue Int. 2000, 67, 321–329. [Google Scholar] [CrossRef] [PubMed]
  87. Li, R.; Clark, A.E.; Hench, L.L. An Investigation of Bioactive Glass Powders by Sol-Gel Processing. J. Appl. Biomater. 1991, 2, 231–239. [Google Scholar] [CrossRef]
  88. Peters, R.; Kramer, E.; Oomen, A.G.; Herrera Rivera, Z.E.; Oegema, G.; Tromp, P.C.; Fokkink, R.; Rietveld, A.; Marvin, H.J.P.; Weigel, S.; et al. Presence of Nano-Sized Silica during In Vitro Digestion of Foods Containing Silica as a Food Additive. ACS Nano 2012, 6, 2441–2451. [Google Scholar] [CrossRef]
  89. Mojsiewicz-Pie, N.; Nkowska, K.; Łukasiak, J. Analytical Fractionation of Silicon Compounds in Foodstuffs. Food Control 2003, 14, 153–162. [Google Scholar] [CrossRef]
  90. Napierska, D.; Thomassen, L.C.J.; Lison, D.; Martens, J.A.; Hoet, P.H. The Nanosilica Hazard: Another Variable Entity. Part. Fibre Toxicol. 2010, 7, 39. [Google Scholar] [CrossRef]
  91. Winkler, H.C.; Suter, M.; Naegeli, H. Critical Review of the Safety Assessment of Nano-Structured Silica Additives in Food. J. Nanobiotechnol. 2016, 14, 44. [Google Scholar] [CrossRef] [PubMed]
  92. Liu, M.; Shafiq, M.; Sun, B.; Wu, J.; Wang, W.; EL-Newehy, M.; EL-Hamshary, H.; Morsi, Y.; Ali, O.; Khan, A.U.R.; et al. Composite Superelastic Aerogel Scaffolds Containing Flexible SiO2 Nanofibers Promote Bone Regeneration. Adv. Healthc. Mater. 2022, 11, 2200499. [Google Scholar] [CrossRef]
  93. Desimone, M.F.; Hélary, C.; Rietveld, I.B.; Bataille, I.; Mosser, G.; Giraud-Guille, M.M.; Livage, J.; Coradin, T. Silica-Collagen Bionanocomposites as Three-Dimensional Scaffolds for Fibroblast Immobilization. Acta Biomater. 2010, 6, 3998–4004. [Google Scholar] [CrossRef]
  94. Hwang, C.; Min, Y.J.; Seong, Y.J.; Kim, D.E.; Kim, H.E.; Jeong, S.H. Enhanced Biolubrication on Biomedical Devices Using Hyaluronic Acid-Silica Nanohybrid Hydrogels. Colloids Surf. B Biointerfaces 2019, 184, 110503. [Google Scholar] [CrossRef]
  95. Tsai, C.-P.; Chen, C.-Y.; Hung, Y.; Chang, F.-H.; Mou, C.-Y. Monoclonal Antibody-Functionalized Mesoporous Silica Nanoparticles (MSN) for Selective Targeting Breast Cancer Cells. J. Mater. Chem. 2009, 19, 5737–5743. [Google Scholar] [CrossRef]
  96. Wang, X.; Wang, Y.; Xu, H.; Shan, H.; Lu, J.R. Dynamic Adsorption of Monoclonal Antibody Layers on Hydrophilic Silica Surface: A Combined Study by Spectroscopic Ellipsometry and AFM. J. Colloid. Interface Sci. 2008, 323, 18–25. [Google Scholar] [CrossRef]
  97. Kontermann, R.E.; Brinkmann, U. Bispecific Antibodies. Drug Discov. Today 2015, 20, 838–847. [Google Scholar] [CrossRef] [PubMed]
  98. Scott, A.M.; Wolchok, J.D.; Old, L.J. Antibody Therapy of Cancer. Nat. Rev. Cancer 2012, 12, 278–287. [Google Scholar] [CrossRef] [PubMed]
  99. Mylvaganam, S.E.; Paterson, Y.; Getzoff, E.D. Structural Basis for the Binding of an Anti-Cytochrome c Antibody to Its Antigen: Crystal Structures of FabE8-Cytochrome c Complex to 1.8 A Ê Resolution and FabE8 to 2.26 A Ê Resolution. J. Mol. Biol. 1998, 281, 301–322. [Google Scholar] [CrossRef]
  100. Javkhlantugs, N.; Bayar, H.; Ganzorig, C.; Ueda, K. Computational Study on the Interactions and Orientation of Monoclonal Human Immunoglobulin G on a Polystyrene Surface. Int. J. Nanomed. 2013, 8, 2487–2496. [Google Scholar] [CrossRef]
  101. Harris, L.J.; Skaletsky, E.; Mcpherson, A. Crystallographic Structure of an Intact IgG1 Monoclonal Antibody. J. Mol. Biol. 1998, 275, 861–872. [Google Scholar] [CrossRef]
  102. Sheriff, S.; Silverton, E.W.; Padlan, E.A.; Cohen, G.H.; Smith-Gillt, S.J.; Finzelt, B.C.; Davies, D.R. Three-Dimensional Structure of an Antibody-Antigen Complex (Immunoglobulins/Epitope/X-ray Crystallography/Complementarity/Lysozyme). Proc. Natl. Acad. Sci. USA 1987, 84, 8075–8079. [Google Scholar] [CrossRef]
  103. Sundberg, E.J.; Mariuzza, R.A. Molecular Recognition in Antibody-Antigen Complexes. Adv. Protein Chem. 2003, 61, 119–157. [Google Scholar]
  104. Davies, D.R.; Padlan, E.A.; Sheriff, S. Antibody-antigen complexes. Annu. Rev. Biochem. 1990, 59, 439–473. [Google Scholar] [CrossRef]
  105. Iyonaga, K.; Takeya, M.; Yamamoto, T.; Ando, M.; Takahashi, K. A Novel Monoclonal Antibody, RM-4, Specifically Recognizes Rat Macrophages and Dendritic Cells in Formalin-Fixed, Paraffin- Embedded Tissues. Histochem. J. 1997, 29, 105–116. [Google Scholar] [CrossRef] [PubMed]
  106. Kraal, G.; Rep, M.; Janse, M. Macrophages in T and B Cell Compartments and Other Tissue Macrophages Recognized by Monoclonal Antibody MOMA-2. Scand. J. Immunol. 1987, 26, 653–661. [Google Scholar] [CrossRef] [PubMed]
  107. Hirsch, S.; Gordon, S. The Use and Limitation of Monoclonal Antibodies Against Mononuclear Phagocytes. Immunobiology 1982, 161, 298–307. [Google Scholar] [CrossRef] [PubMed]
  108. Sharma, O.P.; Das, A.A.; Krishna, R.; Suresh Kumar, M.; Mathur, P.P. Structural Epitope Database (SEDB): A Web-Based Database for the Epitope, and Its Intermolecular Interaction along with the Tertiary Structure Information. J. Proteomics Bioinform. 2012, 5, 84–89. [Google Scholar] [CrossRef]
  109. Sanchez-Trincado, J.L.; Gomez-Perosanz, M.; Reche, P.A. Reche Fundamentals and Methods for T- and B-Cell Epitope Prediction. J. Immunol. Res. 2017, 2017, 2680160. [Google Scholar] [CrossRef]
  110. van de Bovenkamp, F.S.; Hafkenscheid, L.; Rispens, T.; Rombouts, Y. The Emerging Importance of IgG Fab Glycosylation in Immunity. J. Immunol. 2016, 196, 1435–1441. [Google Scholar] [CrossRef]
  111. Amit, A.G.; Mariuzza, R.A.; Phillips, S.E.V.; Poljak, R.J. Three-Dimensional Structure of an Antigen-Antibody Complex at 2.8 Å Resolution. Science 1986, 233, 747–753. [Google Scholar] [CrossRef] [PubMed]
  112. Selby, C. Interference in Immunoassay. Ann. Clin. Biochem. 1999, 36, 704–721. [Google Scholar] [CrossRef] [PubMed]
  113. Bernard, A.; Michel, B.; Delamarche, E. Micromosaic Immunoassays. Anal. Chem. 2001, 73, 8–12. [Google Scholar] [CrossRef] [PubMed]
  114. Umeki, K.; Yasuda, A.; Umekita, K.; Megumi, R.; Nomura, H.; Kawaguchi, T.; Matsuda, M.; Takajo, I.; Shimojima, M.; Okayama, A. Detection of Anti-SFTSV Nuclear Protein Antibody in the Acute Phase Sera of Patients Using Double-Antigen ELISA and Immunochromatography. J. Virol. Methods 2020, 285, 113942. [Google Scholar] [CrossRef] [PubMed]
  115. Niloofa, R.; Fernando, N.; De Silva, N.L.; Karunanayake, L.; Wickramasinghe, H.; Dikmadugoda, N.; Premawansa, G.; Wickramasinghe, R.; De Silva, H.J.; Premawansa, S.; et al. Diagnosis of Leptospirosis: Comparison between Microscopic Agglutination Test, IgM-ELISA and IgM Rapid Immunochromatography Test. PLoS ONE 2015, 10, e129236. [Google Scholar] [CrossRef] [PubMed]
  116. Khamrin, P.; Nguyen, T.A.; Phan, T.G.; Satou, K.; Masuoka, Y.; Okitsu, S.; Maneekarn, N.; Nishio, O.; Ushijima, H. Evaluation of Immunochromatography and Commercial Enzyme-Linked Immunosorbent Assay for Rapid Detection of Norovirus Antigen in Stool Samples. J. Virol. Methods 2008, 147, 360–363. [Google Scholar] [CrossRef] [PubMed]
  117. Cho, I.-H.; Park, J.-W.; Lee, T.G.; Lee, H.; Paek, S.-H. Biophysical Characterization of the Molecular Orientation of an Antibody-Immobilized Layer Using Secondary Ion Mass Spectrometry. Analyst 2011, 136, 1412–1419. [Google Scholar] [CrossRef]
  118. Welch, N.G.; Madiona, R.M.T.; Scoble, J.A.; Muir, B.W.; Pigram, P.J. ToF-SIMS and Principal Component Analysis Investigation of Denatured, Surface-Adsorbed Antibodies. Langmuir 2016, 32, 10824–10834. [Google Scholar] [CrossRef] [PubMed]
  119. Awsiuk, K.; Stetsyshyn, Y.; Raczkowska, J.; Lishchynskyi, O.; Dąbczyński, P.; Kostruba, A.; Ohar, H.; Shymborska, Y.; Nastyshyn, S.; Budkowski, A. Temperature-Controlled Orientation of Proteins on Temperature-Responsive Grafted Polymer Brushes: Poly(Butyl Methacrylate) vs. Poly(Butyl Acrylate): Morphology, Wetting, and Protein Adsorption. Biomacromolecules 2019, 20, 2185–2197. [Google Scholar] [CrossRef]
  120. Hirano, A.; Wada, M.; Kitamura, M.; Kasahara, S.; Kato, K. Interactions between Amino Acids and Zirconia Modified with Ethylenediaminetetra(Methylenephosphonic Acid): Mechanistic Insights into the Selective Binding of Antibodies. Langmuir 2021, 37, 1605–1612. [Google Scholar] [CrossRef]
  121. Jönsson, U.; Lundström, I.; Rönnberg, I. Immunoglobulin G and Secretory Fibronectin Adsorption to Silica The Influence of Conformational Changes on the Surface. J. Colloid. Interface Sci. 1987, 117, 127–138. [Google Scholar]
  122. Tosaka, R.; Yamamoto, H.; Ohdomari, I.; Watanabe, T. Adsorption Mechanism of Ribosomal Protein L2 onto a Silica Surface: A Molecular Dynamics Simulation Study. Langmuir 2010, 26, 9950–9955. [Google Scholar] [CrossRef] [PubMed]
  123. Liu, L.; Elwing, H.; Karlsson, A.; Nimeri, G.; Dahlgren, C. Surface-Related Triggering of the Neutrophil Respiratory Burst. Characterization of the Response Induced by IgG Adsorbed to Hydrophilic and Hydrophobic Glass Surfaces. Clin. Exp. Immunol. 2003, 109, 204–210. [Google Scholar] [CrossRef]
  124. Frauenfelder, H.; Fenimore, P.W.; Mcmahon, B.H. Hydration, Slaving and Protein Function. Biophys. Chem. 2002, 98, 35–48. [Google Scholar] [CrossRef]
  125. Tsuruta, T. On the Role of Water Molecules in the Interface between Biological Systems and Polymers. J. Biomater. Sci. Polym. Ed. 2010, 21, 1831–1848. [Google Scholar] [CrossRef] [PubMed]
  126. Tanaka, M.; Mochizuki, A. Effect of Water Structure on Blood Compatibility— Thermal Analysis of Water in Poly(Meth)Acrylate. J. Biomed. Mater. Res. A 2004, 68A, 684–695. [Google Scholar] [CrossRef]
  127. Tanaka, M.; Mochizuki, A.; Ishii, N.; Motomura, T.; Hatakeyama, T. Study of Blood Compatibility with Poly(2-Methoxyethyl Acrylate). Relationship between Water Structure and Platelet Compatibility in Poly(2-Methoxyethylacrylate-Co-2-Hydroxyethylmethacrylate). Biomacromolecules 2002, 3, 36–41. [Google Scholar] [CrossRef]
  128. Tanaka, M.; Motomura, T.; Ishii, N.; Shimura, K.; Onishi, M.; Mochizuki, A.; Hatakeyama, T. Cold Crystallization of Water in Hydrated Poly(2-Methoxyethyl Acrylate) (PMEA). Polym. Int. 2000, 49, 1709–1713. [Google Scholar] [CrossRef]
  129. Tanaka, M.; Sato, K.; Kitakami, E.; Kobayashi, S.; Hoshiba, T.; Fukushima, K. Design of Biocompatible and Biodegradable Polymers Based on Intermediate Water Concept. Polym. J. 2015, 47, 114–121. [Google Scholar] [CrossRef]
  130. Morita, S.; Tanaka, M.; Ozaki, Y. Time-Resolved In Situ ATR-IR Observations of the Process of Sorption of Water into a Poly(2-Methoxyethyl Acrylate) Film. Langmuir 2007, 23, 3750–3761. [Google Scholar] [CrossRef]
  131. Sugimoto, K.; Zhou, Y.; Galindo, T.G.P.; Kimura, R.; Tagaya, M. Investigation of Surface Layers on Biological and Synthetic Hydroxyapatites Based on Bone Mineralization Process. Biomimetics 2023, 8, 184. [Google Scholar] [CrossRef] [PubMed]
  132. Tagaya, M. In Situ QCM-D Study of Nano-Bio Interfaces with Enhanced Biocompatibility. Polym. J. 2015, 47, 599–608. [Google Scholar] [CrossRef]
  133. Sugimoto, K.; Mikami, K.; Kimura, R.; Tagaya, M. Synthesis of Tetraethoxysilane-Reacted Hydroxyapatite Nanoparticles and Their Stabilization in Phosphate-Buffered Saline. Langmuir 2023, 39, 9431–9438. [Google Scholar] [CrossRef] [PubMed]
  134. Yamada, S.; Chai, Y.; Tagaya, M. PEG Functionalization Effect of Silicate-Containing Hydroxyapatite Particles on Effective Collagen Fibrillation with Hydration Layer State Change. Phys. Chem. Chem. Phys. 2022, 24, 6788–6802. [Google Scholar] [CrossRef] [PubMed]
  135. Liu, Z.; Kawagoe, D.; Tagaya, M. Nanospacial Effect of Citric Acid-Coordinated Hydroxyapatite Nanoparticle Films on Protein Adsorption and Cell Adhesion States. J. Mater. Chem. B 2022, 10, 9599–9606. [Google Scholar] [CrossRef] [PubMed]
  136. Peñaflor Galindo, T.G.; Tagaya, M. Interfacial Effect of Hydration Structures of Hydroxyapatite Nanoparticle Films on Protein Adsorption and Cell Adhesion States. ACS Appl. Bio Mater. 2019, 2, 5559–5567. [Google Scholar] [CrossRef] [PubMed]
  137. Rey, C.; Collins, B.; Goehl, T.; Dickson, I.R.; Glimcher, M.J. The Carbonate Environment in Bone Mineral: A Resolution-Enhanced Fourier Transform Infrared Spectroscopy Study. Calcif. Tissue Int. 1989, 45, 157–164. [Google Scholar] [CrossRef] [PubMed]
  138. Combes, C.; Rey, C.; Mounic, S. Identification and Evaluation of HPO4 Ions in Biomimetic Poorly Crystalline Apatite and Bone Mineral. Key Eng. Mater. 2001, 192–195, 143–146. [Google Scholar]
  139. Jarlbring, M.; Sandström, D.E.; Antzutkin, O.N.; Forsling, W. Characterization of Active Phosphorus Surface Sites at Synthetic Carbonate-Free Fluorapatite Using Single-Pulse 1H, 31P, and 31P CP MAS NMR. Langmuir 2006, 22, 4787–4792. [Google Scholar] [CrossRef]
  140. Aue, W.P.; Roufosse, A.H.; Glimcher, M.J.; Griffin, R.G. Solid-State Phosphorus-31 Nuclear Magnetic Resonance Studies of Synthetic Solid Phases of Calcium Phosphate: Potential Models of Bone Mineral. Biochemistry 1984, 23, 6110–6114. [Google Scholar] [CrossRef]
  141. Roufosse, A.H.; Aue, W.P.; Roberts, J.E.; Glimcher, M.J.; Griffin, R.G. Investigation of the Mineral Phases of Bone by Solid-State Phosphorus-31 Magic Angle Sample Spinning Nuclear Magnetic Resonance. Biochemistry 1984, 23, 6115–6120. [Google Scholar] [CrossRef] [PubMed]
  142. Delgado-López, J.M.; Iafisco, M.; Rodríguez, I.; Tampieri, A.; Prat, M.; Gómez-Morales, J. Crystallization of Bioinspired Citrate-Functionalized Nanoapatite with Tailored Carbonate Content. Acta Biomater. 2012, 8, 3491–3499. [Google Scholar] [CrossRef]
  143. Bolis, V.; Busco, C.; Martra, G.; Bertinetti, L.; Sakhno, Y.; Ugliengo, P.; Chiatti, F.; Corno, M.; Roveri, N. Coordination Chemistry of Ca Sites at the Surface of Nanosized Hydroxyapatite: Interaction with H2O and CO. Philos. Trans. R. Soc. A 2012, 370, 1313–1336. [Google Scholar] [CrossRef]
  144. Lin, T.-J.; Heinz, H. Accurate Force Field Parameters and PH Resolved Surface Models for Hydroxyapatite to Understand Structure, Mechanics, Hydration, and Biological Interfaces. J. Phys. Chem. C 2016, 120, 4975–4992. [Google Scholar] [CrossRef]
  145. Mann, S. Molecular Recognition in Biomineralization. Nature 1988, 332, 119–124. [Google Scholar] [CrossRef]
  146. Palmer, L.C.; Newcomb, C.J.; Kaltz, S.R.; Spoerke, E.D.; Stupp, S.I. Biomimetic Systems for Hydroxyapatite Mineralization Inspired by Bone and Enamel. Chem. Rev. 2008, 108, 4754–4783. [Google Scholar] [CrossRef]
  147. Boyan, B.D.; Schwartz, Z.; Swain, L.D.; Khare, A. Role of Lipids in Calcification of Cartilage. Anat. Rec. 1989, 224, 211–219. [Google Scholar] [CrossRef] [PubMed]
  148. Loveridge, N. Bone: More than a Stick. J. Anim. Sci. 1999, 77, 190–196. [Google Scholar] [CrossRef]
  149. Gómez-Morales, J.; Iafisco, M.; Delgado-López, J.M.; Sarda, S.; Drouet, C. Progress on the Preparation of Nanocrystalline Apatites and Surface Characterization: Overview of Fundamental and Applied Aspects. Prog. Cryst. Growth Charact. Mater. 2013, 59, 1–46. [Google Scholar] [CrossRef]
  150. Vallet-Regí, M.; González-Calbet, J.M. Calcium Phosphates as Substitution of Bone Tissues. Progress Solid. State Chem. 2004, 32, 1–31. [Google Scholar] [CrossRef]
  151. Porter, A.E.; Patel, N.; Skepper, J.N.; Best, S.M.; Bonfield, W. Comparison of in Vivo Dissolution Processes in Hydroxyapatite and Silicon-Substituted Hydroxyapatite Bioceramics. Biomaterials 2003, 24, 4609–4620. [Google Scholar] [CrossRef] [PubMed]
  152. Tang, P.F.; Li, G.; Wang, J.F.; Zheng, Q.J.; Wang, Y. Development, Characterization, and Validation of Porous Carbonated Hydroxyapatite Bone Cement. J. Biomed. Mater. Res. B Appl. Biomater. 2009, 90 B, 886–893. [Google Scholar] [CrossRef]
  153. Qiu, Z.Y.; Noh, I.S.; Zhang, S.M. Silicate-Doped Hydroxyapatite and Its Promotive Effect on Bone Mineralization. Front. Mater. Sci. 2013, 7, 40–50. [Google Scholar] [CrossRef]
  154. Kadu, K.; Kowshik, M.; Roy Ramanan, S. Does the Nanoparticle Morphology Influence Interaction with Protein: A Case Study with Hydroxyapatite Nanoparticles. Mater. Today Commun. 2021, 26, 102172. [Google Scholar] [CrossRef]
  155. Noda, D.; Saito, N.; Yamada, I.; Tagaya, M. Investigation of Adsorptive Orientation State Change of Anionic Porphyrin with the Hydrolysis Reaction of α-Tricalcium Phosphate. CrystEngComm 2022, 24, 4008–4012. [Google Scholar] [CrossRef]
  156. Iafisco, M.; Sabatino, P.; Lesci, I.G.; Prat, M.; Rimondini, L.; Roveri, N. Conformational Modifications of Serum Albumins Adsorbed on Different Kinds of Biomimetic Hydroxyapatite Nanocrystals. Colloids Surf. B Biointerfaces 2010, 81, 274–284. [Google Scholar] [CrossRef] [PubMed]
  157. Dong, X.; Wang, Q.; Wu, T.; Pan, H. Understanding Adsorption-Desorption Dynamics of BMP-2 on Hydroxyapatite (001) Surface. Biophys. J. 2007, 93, 750–759. [Google Scholar] [CrossRef] [PubMed]
  158. Iafisco, M.; Varoni, E.; Di Foggia, M.; Pietronave, S.; Fini, M.; Roveri, N.; Rimondini, L.; Prat, M. Conjugation of Hydroxyapatite Nanocrystals with Human Immunoglobulin G for Nanomedical Applications. Colloids Surf. B Biointerfaces 2012, 90, 1–7. [Google Scholar] [CrossRef] [PubMed]
  159. Tibbetts, C.; Pettersson, U.; Johansson, K.; Philpson, L. Relationship of MRNA from Productively Infected Cells to the Complementary Strands of Adenovirus Type 2 DNA. J. Virol. 1974, 13, 370–377. [Google Scholar] [CrossRef]
  160. Kawasaki, T.; Takahashi, S.; Ideda, K. Hydroxyapatite High-Performance Liquid Chromatography: Column Performance for Proteins. Eur. J. Biochem. 1985, 152, 361–371. [Google Scholar] [CrossRef]
  161. Sang Cho, J.; Um, S.H.; Su Yoo, D.; Chung, Y.C.; Hye Chung, S.; Lee, J.C.; Rhee, S.H. Enhanced Osteoconductivity of Sodium-Substituted Hydroxyapatite by System Instability. J. Biomed. Mater. Res. B Appl. Biomater. 2014, 102, 1046–1062. [Google Scholar] [CrossRef]
  162. Kim, H.S.; Bugli, G.; Djéga-Mariadassou, G. Preparation and Characterization of Niobium Carbide and Carbonitride. J. Solid. State Chem. 1999, 142, 100–107. [Google Scholar] [CrossRef]
  163. Kim, H.M.; Miyaji, F.; Kokubo, T.; Nakamura, T. Effect of Heat Treatment on Apatite-Forming Ability of Ti Metal Induced by Alkali Treatment. J. Mater. Sci. Mater. Med. 1997, 8, 341–347. [Google Scholar] [CrossRef]
  164. Kokubo, T.; Miyaji, F.; Kim, H.-M.; Nakamura, T. Spontaneous Formation of Bonelike Apatite Layer on Chemically Treated Titanium Metals. J. Am. Ceram. Soc. 1996, 79, 1127–1129. [Google Scholar] [CrossRef]
  165. Kim, H.-M.; Miyaji, F.; Kokubo, T.; Nakamura, T. Preparation of Bioactive Ti and Its Alloys via Simple Chemical Surface Treatment. J. Biomed. Mater. Res. 1996, 32, 409–417. [Google Scholar] [CrossRef]
  166. Cho, J.S.; Yoo, D.S.; Chung, Y.C.; Rhee, S.H. Enhanced Bioactivity and Osteoconductivity of Hydroxyapatite through Chloride Substitution. J. Biomed. Mater. Res. A 2014, 102, 455–469. [Google Scholar] [CrossRef]
  167. Saito, K.; Ikushima, A.J. Structural Relaxation Enhanced by Cl Ions in Silica Glass. Appl. Phys. Lett. 1998, 73, 1209–1211. [Google Scholar] [CrossRef]
  168. Sanada, K.; Shiota, T.; Inada, K. Studies of the Chemical Kinetics on the Vapor Phase Axial Deposition Method. J. Non Cryst. Solids 1995, 188, 275–284. [Google Scholar] [CrossRef]
  169. Shinji, I.; Masashi, O. Method of Making Synthetic Silica Glass. U.S. Patent No. 6,116,055, 12 September 2000. [Google Scholar]
  170. Awazu, K.; Kawazoe, H.; Muta, K.; Ibuki, T.; Tabayashi, K.; Shobatake, K. Characterization of Silica Glasses Sintered under Cl2 Ambients. J. Appl. Phys. 1991, 69, 1849–1852. [Google Scholar] [CrossRef]
  171. Hepburn, R.W.; Tomozawa, M. Diffusion of Water in Silica Glasses Containing Different Amounts of Chlorine. J. Non-Cryst. Solids 2001, 281, 162–170. [Google Scholar] [CrossRef]
  172. Davis, K.M.; Tomozawa, M. An Infrared Spectroscopic Study of Water-Related Species in Silica Glasses. J. Non-Cryst. Solids 1996, 201, 177–198. [Google Scholar] [CrossRef]
  173. Awazu, K.; Harada, K.; Kawazoe, H.; Muta, K. Structural Imperfections in Silica Glasses with an Optical Absorption Peak at 3.8 EV. J. Appl. Phys. 1992, 72, 4696–4699. [Google Scholar] [CrossRef]
  174. Griscom, D.L.; Friebele, E.J. Fundamental Radiation-Induced Defect Centers in Synthetic Fused Silicas: Atomic Chlorine, Delocalized E’ Centers, and a Triplet State. Phys. Rev. B 1986, 34, 7524–7533. [Google Scholar] [CrossRef] [PubMed]
  175. Bogart, K.H.A.; Donnelly, V.M. Composition of Trench Sidewalls and Bottoms for SiO2-Masked Si(100) Etched in Cl2 Plasmas. J. Appl. Phys. 2000, 87, 8351–8360. [Google Scholar] [CrossRef]
Figure 1. Schematic diagram of the living bone structures. Adapted from Ref. [3].
Figure 1. Schematic diagram of the living bone structures. Adapted from Ref. [3].
Biomimetics 09 00347 g001
Figure 2. Crystal structure of HA. Here, the grey parts indicate phosphate ions.
Figure 2. Crystal structure of HA. Here, the grey parts indicate phosphate ions.
Biomimetics 09 00347 g002
Figure 3. Crystal structure of CDHA. Here, the grey and white parts indicate phosphate ions and Ca(I) sites, respectively.
Figure 3. Crystal structure of CDHA. Here, the grey and white parts indicate phosphate ions and Ca(I) sites, respectively.
Biomimetics 09 00347 g003
Figure 4. Crystal structure of CHA. Here, the white circles, grey and brown parts indicate oxygen atoms, phosphate ions, and carbonate ions, respectively.
Figure 4. Crystal structure of CHA. Here, the white circles, grey and brown parts indicate oxygen atoms, phosphate ions, and carbonate ions, respectively.
Biomimetics 09 00347 g004
Figure 5. Illustrations of the manufacturing method for the amorphous silica particles, which are (a) fusion, (b) sol-gel, and (c) vapor-axial-phase-deposition methods, respectively. Adapted with permission from Ref. [42]. Copyright 2024 American Chemical Society.
Figure 5. Illustrations of the manufacturing method for the amorphous silica particles, which are (a) fusion, (b) sol-gel, and (c) vapor-axial-phase-deposition methods, respectively. Adapted with permission from Ref. [42]. Copyright 2024 American Chemical Society.
Biomimetics 09 00347 g005
Figure 6. Illustration of the formation mechanism and the surface structure of the amorphous silica particles.
Figure 6. Illustration of the formation mechanism and the surface structure of the amorphous silica particles.
Biomimetics 09 00347 g006
Figure 7. Illustration of the (a) antibody protein structure and the (b) immobilization state on the conventional amorphous silica particle surfaces.
Figure 7. Illustration of the (a) antibody protein structure and the (b) immobilization state on the conventional amorphous silica particle surfaces.
Biomimetics 09 00347 g007
Figure 8. Classification of hydration layers, which were analyzed by relaxation time (τc) of the water molecule motion measured by solid-state NMR and IR adsorption wavenumber νIR. Adapted from Ref. [131].
Figure 8. Classification of hydration layers, which were analyzed by relaxation time (τc) of the water molecule motion measured by solid-state NMR and IR adsorption wavenumber νIR. Adapted from Ref. [131].
Biomimetics 09 00347 g008
Figure 9. Illustration of the surface layer on bioceramics for protein immobilization.
Figure 9. Illustration of the surface layer on bioceramics for protein immobilization.
Biomimetics 09 00347 g009
Figure 10. Illustration of the surface layers of HA nanocrystal core in vivo. Adapted from Ref. [131].
Figure 10. Illustration of the surface layers of HA nanocrystal core in vivo. Adapted from Ref. [131].
Biomimetics 09 00347 g010
Figure 11. Illustration of the presence states of chlorine (indicated in red) in the amorphous silica particles, which are classified into (a) Si–Cl arrangement (main product), (b) interstitial molecular Cl2, (c) complex consisting of four Si–Cl groups, (d) interstitial atomic chlorine, and (e) SiCl2 arrangement. Reprinted with permission from Ref. [42]. Copyright 2024 American Chemical Society.
Figure 11. Illustration of the presence states of chlorine (indicated in red) in the amorphous silica particles, which are classified into (a) Si–Cl arrangement (main product), (b) interstitial molecular Cl2, (c) complex consisting of four Si–Cl groups, (d) interstitial atomic chlorine, and (e) SiCl2 arrangement. Reprinted with permission from Ref. [42]. Copyright 2024 American Chemical Society.
Biomimetics 09 00347 g011
Figure 12. Illustration of the adsorption processes of the hydration layer on bioceramics and subsequent protein adlayer on the surface.
Figure 12. Illustration of the adsorption processes of the hydration layer on bioceramics and subsequent protein adlayer on the surface.
Biomimetics 09 00347 g012
Disclaimer/Publisher’s Note: The statements, opinions and data contained in all publications are solely those of the individual author(s) and contributor(s) and not of MDPI and/or the editor(s). MDPI and/or the editor(s) disclaim responsibility for any injury to people or property resulting from any ideas, methods, instructions or products referred to in the content.

Share and Cite

MDPI and ACS Style

Kimura, R.; Noda, D.; Liu, Z.; Shi, W.; Akutsu, R.; Tagaya, M. Biological Surface Layer Formation on Bioceramic Particles for Protein Adsorption. Biomimetics 2024, 9, 347. https://doi.org/10.3390/biomimetics9060347

AMA Style

Kimura R, Noda D, Liu Z, Shi W, Akutsu R, Tagaya M. Biological Surface Layer Formation on Bioceramic Particles for Protein Adsorption. Biomimetics. 2024; 9(6):347. https://doi.org/10.3390/biomimetics9060347

Chicago/Turabian Style

Kimura, Reo, Daichi Noda, Zizhen Liu, Wanyu Shi, Ryota Akutsu, and Motohiro Tagaya. 2024. "Biological Surface Layer Formation on Bioceramic Particles for Protein Adsorption" Biomimetics 9, no. 6: 347. https://doi.org/10.3390/biomimetics9060347

Article Metrics

Back to TopTop