Related Experiment Video
Updated: Dec 17, 2025

Rapid Mix Preparation of Bioinspired Nanoscale Hydroxyapatite for Biomedical Applications
Published on: February 23, 2017
Characterization of Synthetic Hydroxyapatite Fibers Using High-Resolution, Polarized Raman Spectroscopy
1Department of Biomaterials, Sahlgrenska Academy, University of Gothenburg, Gothenburg, Sweden.
Abstract:
In the Raman spectrum of B-type carbonated apatites, the ν1 CO32- mode (at ∼1070 cm-1) overlaps the ν3 PO43- band. The latter is readily observed where the CO32- content is low (up to ∼3 wt%). The CO32- content of bone is considerably higher (∼7-9 wt%). As a result, the ν3 PO43- band becomes completely obscured. The 1000-1100 cm-1 spectral range of carbonated apatite is frequently considered a combined ν3 PO43- and ν1 CO32- region. Here, high-resolution polarized Raman spectroscopy (step size of 0.74 ± 0.04 cm-1) provides new insights into synthetic hydroxyapatite (HAp) obtained as micrometer-sized fibers. Compared to bone mineral (deproteinized bovine bone), spectral features of HAp fibers are highly resolved. In particular, the ν3 PO43- band resolves into nine distinct sub-components: 1028, 1032, 1040, 1043, 1047, 1053, 1055, 1062, and 1076 cm-1. Parameters including full width half-maximum, intensity, area fraction, intensity ratio, and area fraction ratio vary between parallel and perpendicular polarized configurations. It is likely that the ν1 CO32- band of B-type carbonated apatites may contain a small but not insignificant contribution from the 1076 cm-1 sub-component of the ν3 PO43- band. Furthermore, the 1076 cm-1/1047 cm-1 ratio changes between parallel and perpendicular scattering configurations, suggesting that the contribution of the 1076 cm-1 sub-component may vary as a function of local orientation of bone mineral, thus skewing the ν1 CO32- band and compromising accurate estimation of carbonate-to-phosphate ratios in B-type CO32- substituted apatite.
More Related Videos
Related Concept Videos
Raman Spectroscopy: Overview
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
Raman Spectroscopy Instrumentation: Overview
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
Attenuated Total Reflectance (ATR) Infrared Spectroscopy: Overview
The ATR process begins by directing a beam...

