| Literature DB >> 26053330 |
Wei Zhang1, Xiao-juan Luo1, Li-na Niu2, Hong-ye Yang3, Cynthia K Y Yiu4, Tian-da Wang5, Li-qun Zhou3, Jing Mao1, Cui Huang3, David H Pashley6, Franklin R Tay6.
Abstract
Limited continuous replenishment of the mineralization medium is a restriction for in-class="Chemical">situ solution-based remineralization of hypomineralized body tissues. Here, we report a process that geneEntities:
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Year: 2015 PMID: 26053330 PMCID: PMC4459175 DOI: 10.1038/srep11199
Source DB: PubMed Journal: Sci Rep ISSN: 2045-2322 Impact factor: 4.379
Figure 1a) XPS survey scan of the elemental composition of template-free MSNs. b) Infrared spectrum of template-free MSNs. The Si-O-Si vibrational mode of silica was detected around 1070, 800 and 460 cm−1. The lowest frequency mode (460 cm−1) is assigned to transverse optical rocking motions (TO1 mode). Near 800 cm−1, a weak band due to Si-O-Si symmetric stretching (TO2 mode) can be observed. The highest frequency mode around 1070 cm−1 is assigned to the anti-symmetric stretching of the Si-O-Si bonds (TO3 mode). Si-OH vibrations near 940-960 cm−1 indicates the retention of silanol groups. c) TGA of template-free MSNs. The derivative weight loss peak at 50.2 °C represents the loss of physisorbed water. d) 29Si CP-MAS NMR spectrum of template-free MSNs. Deconvoluted peaks at −89.0, −99.0 and −107.9 ppm are assigned respectively to the Q2, Q3 and Q4 units (Q-series, Si(OSi)x(OH)4-x) originating from mesoporous silica. Q4: siloxane bridges; Q3: single silanols; Q2: germinal silanols18. e) Small-angle (left) and wide-angle (right) XRD of template-free MSNs. Diffraction peaks at (100), (110) and (200) are characteristic of a 2-D hexagonal lattics (p6 mm)19. Non-crystalline scattering identified with wide-angle XRD is characteristic of the amorphous state of the mesoporous silica nanoparticles.
Figure 2a) TEM of unstained MSNs prior to amine functionalization. b) TEM of unstained AF-MSNs. Arrow: mesoporous nanochannels seen in parallel arrangement. Open arrowhead: cross-sectional view of the mesoporous nanochannels. c) Schematic illustration of the assignments of the four TGA derivative weight-loss peaks. d) TGA data shows an overall weight loss of 45.4 wt%, with 4 discernible derivative weight-loss peaks. e) STEM–EDX mapping of AF-MSNs shows elemental distribution of Si, O and N within the nanoparticles.
Figure 3a) 29Si CP-MAS NMR spectrum of AF-MSNs. b) Wide-scan XPS spectrum showing the elemental composition of AF-MSNs and the chemical bonding states of aminopropyltriethoxysilane (APTES) and mesoporous silica. c) High resolution XPS spectrum of C1s. d) High resolution XPS spectrum of N1s.
Figure 4a) Nitrogen sorption of AF-MSNs showing type IV adsorption-desorption isotherms. b) Specific surface area of AF-MSNs. c) Total micropore and mesopore volume in AF-MSNs. d) Pore size distribution in AF-MSNs.
Figure 5a) Unstained TEM image of unsectioned, template-free AF-MSNs with partially-loaded Pa-ACPs (arrowheads) revealing their mesoporous structure. b) Unstained TEM image of unsectioned AF-MSNs that were fully loaded with Pa-ACPs. c) Unstained TEM image of sectioned, epoxy resin-embedded Pa-ACP loaded AF-MSNs showing the presence of Pa-ACPs within the mesopores and around the periphery of the mesoporous silica nanoparticles (arrow). d) AFM height and phase images and three-dimensional presentation of the surface morphology AF-MSNs before and after loading of Pa-ACPs. Before loading, AF-MSNs have relative smooth surface profiles while the phase-contrast image and 3-D surface plot reveal localized regions that exhibit changes in viscoelastic properties or adhesion forces that may be contributed by anchoring of APTES on the MSN surface. After loading, the AF-MSNs have highly granular surface morphology. e) STEM-EDX mappings showing the different elements present within the loaded nanoparticles. f) Unstained TEM image showing release of Pa-ACPs (arrows) after immersion in HEPES buffer solution. Some of the Pa-ACPs were present on the surface of the AF-MSNs (arrowheads). g) Release kinetics of calcium, phosphate and silicic acid ions from Pa-ACP loaded AF-MSNs within a 10-day period after immersion in HEPES at pH 7.4.
Figure 6a–d) Unstained TEM images of collagen biomineralization in a 2-D model consisting of bovine skin collagen reconstituted on TEM grids.a) Grid placed over Pa-ACP loaded AF-MSN containing HEPES buffer for 15 min. AF-MSNs could be identified in the vicinity of the unmineralized collagen fibrils (arrowheads). b) Most of the fibrils were mineralized after 4 days. Arrows: Unmineralized portions of collagen fibrils c) High magnification of intrafibrillar (pointer) and extrafibrillar (asterisk) mineralization. Arrowhead: Pa-ACP loaded AF-MSN. d) Very high magnification showing arrangement of intrafibrillar mineral strands along the microfibrillar spaces, with no evidence of cross banding. Arrowhead: Pa-ACP loaded AF-MSN. e) Unstained TEM image of collagen biomineralization in a 3-D model consisting of natural collagen fibrils derived from rat tail tendon. Asterisk: unmineralized intrafibrillar regions after 7 days of mineralization. White circle: site from which electron diffraction was performed. f) Selected area electron diffractions of the crystalline deposition indicate that apatite crystallites are aligned along the longitudinal axis of the collagen fibril.
Figure 7a) At 24 hours, unstained collagen fibrils were partially filled with electron-dense, amorphous minerals within their intrafibrillar spaces (pointer). Open arrowhead: calcium phosphate prenucleation clusters. Bar = 100 nm. Inset: SAED taken from the collagen fibril. b) After 2 days, collagen fibrils were partially mineralized by apatite crystallites (between open arrowheads). Regions within the same fibril that were not infiltrated by polyacid-stabilized amorphous calcium phosphate (Pa-ACP) are indicated by the open arrows. Mesoporosity of the AF-MSNs became apparent again after release of Pa-ACP. Bar = 50 nm. Inset: SAED taken from the partially-mineralized region of the collagen fibril.