Abstract:The x-ray coloration of synthetic calcium fluorophosphate (fluorapatite) crystals is shown to result from the presence of fluorine vacancy defects. Three of these defects have been studied by correlating their optical absorption bands with their electron-paramagnetic-resonance spectra, and by application of the electron-nuclear-double-resonance technique to measure the F 19 and P 31 hyperfine interactions. The models proposed for these three axially symmetric defects consist of an electron trapped at (a) an is… Show more
“…The electron-like centers are associated with F -vacancies or substituting O 2-ions in the anion column: F E(I) is an electron trapped by one of two F -vacancies separated by a substitutional O 2-ion, F E(II) is an electron trapped by an isolated F -vacancy, F E(III) is an electron trapped by two F -vacancies adjacent to a substitutional O 2-ion, and F E(IV) an electron trapped by a F -vacancy adjacent to a substitutional O 2-ion. Piper et al (1965) also reported a diamagnetic center ( F B) with two electrons trapped by two F -vacancies adjacent to a substitutional O 2-ion. Center F H(I) involves a hole trapped by a substitutional O 2-ion associated with a neighboring F -vacancy (Segall et al 1962), whereas F H(II) consists of a hole trapped by an isolated substitutional O 2-ion.…”
Section: Background Informationmentioning
confidence: 99%
“…Center F H(I) involves a hole trapped by a substitutional O 2-ion associated with a neighboring F -vacancy (Segall et al 1962), whereas F H(II) consists of a hole trapped by an isolated substitutional O 2-ion. Piper et al (1965) noted that F H(III) and F H(IV) form during the thermal conversion from F H(I) to F H(II). They interpreted F H(III) and F H(IV) to represent stable intermediate confi gurations during the progressive loss of the F -vacancy from the neighboring O 2-ion.…”
Section: Background Informationmentioning
confidence: 99%
“…For example, Piper et al (1965) and Warren (1972) reported four electron-like centers [ F E(I), F E(II), F E(III) and F E(IV)] and four hole-like centers [ F H(I), F H(II), F H(III) and F H(IV)] in X-irradiated fl uorapatite; the presuperscript denotes radiation-induced defect centers in fl uorapatite (Fig. 1).…”
Section: Background Informationmentioning
confidence: 99%
“…Electron paramagnetic resonance (EPR) spectroscopy has been proven to be particularly powerful in providing detailed structural information about dilute concentrations of paramagnetic defects in the anion column in fl uorapatite (Segall et al 1962, Piper et al 1965, Warren 1972, Pan & Fleet 2002. For example, Piper et al (1965) and Warren (1972) reported four electron-like centers [ F E(I), F E(II), F E(III) and F E(IV)] and four hole-like centers [ F H(I), F H(II), F H(III) and F H(IV)] in X-irradiated fl uorapatite; the presuperscript denotes radiation-induced defect centers in fl uorapatite (Fig.…”
Gamma-irradiated chlorapatite, synthesized from a CaCl 2 fl ux, has been investigated by powder and single-crystal electron paramagnetic resonance (EPR) spectroscopy at X-and W-band frequencies, including in situ high-T X-band EPR. The powder EPR spectra, particularly high-T X-band spectra and high-resolution W-band spectra, reveal a new hole-like center, H(III), in addition to two previously reported hole-like centers, H(I) and H(II). Center H(III) is characterized by an electron spin ½ and hyperfi ne interaction with one 35 Cl nucleus, suggesting a structural model consisting of a hole trapped by a substitutional oxygen ion adjacent to a Cl -ion vacancy in the anion column. This discovery of center H(III) also lends support to the structural model already proposed by other authors for center H(II). Single-crystal X-band EPR spectra also disclose a new electronic center, E(I). The structure model for center E(I) includes an electron trapped at an isolated Cl -ion vacancy in the anion column, corresponding to center F E(II) in fl uorapatite and similar to the well-known F center in alkali halides.
“…The electron-like centers are associated with F -vacancies or substituting O 2-ions in the anion column: F E(I) is an electron trapped by one of two F -vacancies separated by a substitutional O 2-ion, F E(II) is an electron trapped by an isolated F -vacancy, F E(III) is an electron trapped by two F -vacancies adjacent to a substitutional O 2-ion, and F E(IV) an electron trapped by a F -vacancy adjacent to a substitutional O 2-ion. Piper et al (1965) also reported a diamagnetic center ( F B) with two electrons trapped by two F -vacancies adjacent to a substitutional O 2-ion. Center F H(I) involves a hole trapped by a substitutional O 2-ion associated with a neighboring F -vacancy (Segall et al 1962), whereas F H(II) consists of a hole trapped by an isolated substitutional O 2-ion.…”
Section: Background Informationmentioning
confidence: 99%
“…Center F H(I) involves a hole trapped by a substitutional O 2-ion associated with a neighboring F -vacancy (Segall et al 1962), whereas F H(II) consists of a hole trapped by an isolated substitutional O 2-ion. Piper et al (1965) noted that F H(III) and F H(IV) form during the thermal conversion from F H(I) to F H(II). They interpreted F H(III) and F H(IV) to represent stable intermediate confi gurations during the progressive loss of the F -vacancy from the neighboring O 2-ion.…”
Section: Background Informationmentioning
confidence: 99%
“…For example, Piper et al (1965) and Warren (1972) reported four electron-like centers [ F E(I), F E(II), F E(III) and F E(IV)] and four hole-like centers [ F H(I), F H(II), F H(III) and F H(IV)] in X-irradiated fl uorapatite; the presuperscript denotes radiation-induced defect centers in fl uorapatite (Fig. 1).…”
Section: Background Informationmentioning
confidence: 99%
“…Electron paramagnetic resonance (EPR) spectroscopy has been proven to be particularly powerful in providing detailed structural information about dilute concentrations of paramagnetic defects in the anion column in fl uorapatite (Segall et al 1962, Piper et al 1965, Warren 1972, Pan & Fleet 2002. For example, Piper et al (1965) and Warren (1972) reported four electron-like centers [ F E(I), F E(II), F E(III) and F E(IV)] and four hole-like centers [ F H(I), F H(II), F H(III) and F H(IV)] in X-irradiated fl uorapatite; the presuperscript denotes radiation-induced defect centers in fl uorapatite (Fig.…”
Gamma-irradiated chlorapatite, synthesized from a CaCl 2 fl ux, has been investigated by powder and single-crystal electron paramagnetic resonance (EPR) spectroscopy at X-and W-band frequencies, including in situ high-T X-band EPR. The powder EPR spectra, particularly high-T X-band spectra and high-resolution W-band spectra, reveal a new hole-like center, H(III), in addition to two previously reported hole-like centers, H(I) and H(II). Center H(III) is characterized by an electron spin ½ and hyperfi ne interaction with one 35 Cl nucleus, suggesting a structural model consisting of a hole trapped by a substitutional oxygen ion adjacent to a Cl -ion vacancy in the anion column. This discovery of center H(III) also lends support to the structural model already proposed by other authors for center H(II). Single-crystal X-band EPR spectra also disclose a new electronic center, E(I). The structure model for center E(I) includes an electron trapped at an isolated Cl -ion vacancy in the anion column, corresponding to center F E(II) in fl uorapatite and similar to the well-known F center in alkali halides.
“…Clifford and Hill (1996) further suggested that the apatite formed in A-W systems is therefore more likely to be a mixture of fluor-and oxyapatite. Based on the pioneering electron spin resonance (ESP) studies on fluor/oxyapatites, it has been long known that O − can occupy F − sites (Segall et al, 1962;Piper et al, 1965). Nonetheless, at present, the availability of high-resolution solid-state characterization techniques such as 17 O MAS-NMR coupled with dynamic nuclear polarization (DNP) and high field 19 F MAS-NMR could provide fast and accurate elucidation of oxygen and fluorine environments in the A-W GC; however, such work is yet to be published.…”
Section: Biomedical Applications Of Apatite Glass-ceramics Orthopedicsmentioning
This article is a review of the published literature on apatite glass-ceramics (GCs). Topics covered include crystallization mechanisms of the various families of apatite GCs and an update on research and development on apatite GCs for applications in orthopedics, dentistry, optoelectronics, and nuclear waste management. Most apatite GCs crystallize through a homogenous nucleation and crystallization mechanism, which is aided by a prior liquid-liquid phase separation. Careful control of the base glass composition and heat-treatment conditions, which determine the nature and morphology of the crystal phases in the GC can produce GC materials with exceptional thermal, mechanical, optical, and biological properties. The GCs reviewed for orthopedic applications exhibit suitable mechanical properties and can chemically bond to bone and stimulate its regeneration. The most commercially successful apatite GCs are those developed for dental veneering. These materials exhibit excellent translucency and clinical esthetics and mimic the natural tooth mineral. Due to the ease of solid solution of the apatite lattice, rare earth doped apatite GCs are discussed for potential applications in optoelectronics and nuclear waste management. One of the drawbacks of the commercial apatite GCs used in orthopedics is the lack of resorbability; therefore, the review provides a direction for future research in the field.
Raman spectroscopy was used to study the radiation damage of fluorapatite single crystals and sinters. Krypton and iodine ion irradiations were performed at high energies (∼1 MeV amu −1 ) for fluences ranging between 1 × 10 11 and 5 × 10 13 cm −2 . Evolution of the symmetric stretching mode of the PO 4 3− tetrahedral building blocks (strongest Raman mode observed at 965 cm −1 ) versus ion fluence was investigated. After irradiation, this peak decreases in intensity and a second broader peak appears at lower wavenumber. The well-resolved peak has been assigned to the crystalline phase, and the broader one to the amorphous phase. The integrated intensity ratios of these two peaks versus fluence are in good agreement with the damage fractions determined by X-ray diffraction (XRD). Fits of the amorphous fraction versus fluence show that the amorphization mechanisms is dominated by a single-impact process for iodine ions and by a double-impact process for krypton ions in the case of single crystals and sinters. For both irradiations, complete amorphization could not be obtained. The amorphous fraction saturates at a maximum value of 88% for sinters and 72% for single crystals. This is attributed to a recrystallization effect which is more important in single crystals than in sinters. For both types of samples, the crystalline peak shifts slightly to a lower wavenumber with fluence, and then shifts back to its initial value for an amorphous fraction larger than 60%. This feature is attributed to a stress relaxation, as shown in the XRD data, which is accompanied by a decrease of the crystalline peak full-width at half-maximum.
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