894
OU-YANG ET AL.
development of a method to determine quantitatively the
spatial distribution of CO23Ϫ in mineralized tissues with IR
imaging and will enhance our understanding of the signif-
icance of carbonate in normal and diseased mineralized
tissues.
MATERIALS AND METHODS
Preparation of carbonated HA
Type B carbonate apatites were prepared following the
procedure of Penel et al.(30) Briefly, a phosphate solution
[0.216 M (NH4)2 HPO4 in 30 ml of H2O and 5 ml of
NH3 ⅐ H2O with varying levels of NaHCO3] was added very
IR spectroscopic investigations of homogenized bones
and teeth(22–24) have shown that CO23Ϫ ions generally sub-
stitute for the two anionic sites in the HA lattice for PO34Ϫ slowly over a 3-h period to a constantly stirred calcium-
containing solution [0.25 M Ca(NO3)2 ⅐ 4H2O dissolved in
30 ml of H2O and 10 ml of NH3 ⅐ H2O] at 80°C. The
precipitates were allowed to mature at 80°C for an addi-
tional 2 h. The precipitates were filtered, washed briefly
with distilled water, and dried at 60°C overnight. All re-
agents were analytical grade. Reaction conditions were kept
constant except for different levels of sodium bicarbonate.
ions (type B carbonate, the major substitution site in bone
and dentin) or for OHϪ ions (type A carbonate, which
occurs at a significant level in dental enamel). In addition to
these insertion sites, a labile carbonate species was identi-
fied and is thought to represent surface carbonate.(7) The
vibrational mode widely used for identification of these
species is the out-of-plane deformation, the v2 mode, at 879
cmϪ1 in the free ion, which undergoes substitution site-
dependent spectral shifts on insertion into the HA lattice.
The spatial distribution of the percent of each type of
carbonate substitution in bone has been reported
elsewhere.(7,8,22–24) Polarized IR studies of the v2 mode also
have provided information about the orientation of the
CO23Ϫ planes in the HA of mineralized turkey tendon.(25)
A limitation of the application of traditional IR spectros-
copy to the study of tissues is the necessity for sample
homogenization before spectral examination. This process
renders it impossible to monitor spatial variations in the
tissue constituents. Yet, spatial variations in these properties
are evidently a major determinant of biological function.
The application of IR microscopy techniques (either using
point-by-point methods or array detector-based microscopic
imaging) serves to overcome the limitations of sample ho-
mogenization. In previous publications(26,27) our laborato-
ries have established the feasibility of acquiring IR micro-
scopic images from normal and abnormal states of
mineralized tissue and cartilage. Several IR spectroscopic
parameters have been developed for molecular character-
ization of the mineral and protein components. Although
some of these parameters that measure the mineral content,
mineral crystallinity, and collagen cross-linking can be ap-
plied in both point-by-point Fourier transform infrared
(FTIR) microspectroscopy and IR imaging,(28,29) the afore-
mentioned carbonate analysis is not applicable because the
v2 mode of CO23Ϫ lies outside the operating range of the
current generation of mercury-cadmium-telluride array de-
tector elements, which have a low frequency cut-off of
ϳ900 cmϪ1. The only other CO23Ϫ mode that is currently
feasible for IR imaging is the v3 mode, which for B type
substituted CO23Ϫ, consists of a spectral doublet with com-
ponents at ϳ1419 cmϪ1 and 1450 cmϪ1. This region of the
spectrum overlaps vibrations from both the protein compo-
nents of the tissue and the embedding material (polymeth-
ylmethacrylate [PMMA]) most frequently used for section-
ing the tissue, thus rendering quantitative determination of
CO23Ϫ somewhat awkward. Nevertheless, the current study
shows the feasibility of using spectral subtraction tech-
niques to overcome spectroscopic interference in this spec-
tral region and therefore to use the v3 mode for quantitative
imaging of CO23Ϫ in bone.
FTIR and X-ray diffraction analysis
Carbonate apatite crystals were analyzed by FTIR as
potassium bromide (KBr) pellets (200:1, wt/wt) on a Matt-
son RS-1 spectrometer (Mattson, Madison, WI, USA) with
512 scans coadded at 4 cmϪ1 resolution. Interferograms
were apodized with a triangular function and Fourier-
transformed with one level of zero filling. The sample
compartment of the spectrometer was purged constantly
with dry air generated from a Whatman gas generator
(Whatman, Haverhill, MA, USA).
X-ray spectra were collected on a Siemens D-5000 Pow-
der Diffractometer with automatic sample feeder (Siemens,
Iselin, NJ, USA) using Ni-filtered Cu-K␣ (1.545 A) radia-
tion. Ground samples were scanned from 24° to 37° (2) at
0.05° intervals. Data were accumulated for 4 h to achieve
good signal/noise ratios.
Two-dimensional IR analyses
A detailed description of the two-dimensional (2D) IR
correlation spectroscopy techniques developed by Noda(31)
as applied to the study of HA crystallinity has been pub-
lished elsewhere.(32) The spectra are normalized to the in-
tegrated peak areas to compensate for 2D features arising
simply from differences in sample concentrations rather
than from alterations in spectral contours.
FTIR imaging
Iliac crest biopsy specimens were acquired as part of
routine diagnoses and provided under an Institutional Re-
view Board (IRB)-approved protocol by the Pathology De-
partment of the Hospital for Special Surgery. Samples had
been fixed in ethanol, embedded in PMMA, and were cut
into ϳ5-m-thick sections before placement between two
BaF2 windows on the instrument stage. Spectra were ac-
quired with a BioRad Sting-Ray system (BioRad, Cam-
bridge, MA, USA). In this device, a 64 ϫ 64 element
mercury-cadmium-telluride (MCT) focal plane array detec-
tor, mapped to a 400 m ϫ 400 m spot at the focal plane
of an IR microscope, is coupled to a step-scan interferom-
eter. Routinely, data from one scan of 1024 steps with 81