Open Access Article
Wenkai Liang,
Nai Wang
* and
Yingrui Gan
School of Gemmology, China University of Geosciences, Beijing, 100083, China. E-mail: 2003011807@cugb.edu.cn
First published on 26th August 2025
Blue, yellow and green are common colors of apatite, and its mineralogical characteristics and fluorescence properties have attracted the attention of many researchers and scholars. In this paper, the structure, composition, spectroscopic features and fluorescence characteristics of three different colors of apatite are investigated to further compare and explore their mineralogical characteristics and fluorescence properties. The results show that the three colors of apatite that belong to fluorapatite, blue apatite and green apatite are in medium oxidation state, and yellow apatite is in oxidation state. Some samples of blue and green apatite showed the homogeneous substitution of [CO3]2− for [PO4]3−. Yellow apatite fluoresces orange, green and blue apatite fluoresce blue–violet, and all three colors of apatite show strong emission peaks at 400 nm at an excitation wavelength of 320 nm, attributed to: the jump of Ce3+: (5d)5D3/2 → 2F7/2(4f) to (5d)5D3/2 → 2F5/2(4f), and the jump of Eu2+: 4f65d1 → (4f)8S7/2; The emission peaks at 585 nm and 600 nm are attributed to the leaps of 4G5/2 → 6H7/2 for Sm3+ with 1D2 → 3H4 for Pr3+. A comparative analysis of the relationship between luminescence intensity and temperature in samples of yellow and blue apatite was conducted. The findings of this analysis indicated that yellow apatite exhibits greater thermal stability in comparison to blue apatite.
In the field of mineralogy, apatite is a prevalent by-mineral in a variety of igneous, metamorphic, and sedimentary rocks. Its structural and compositional characteristics yield substantial insights into petrogenesis and mineralization processes. Extensive research has been conducted on various aspects, including dating methods, low-temperature pyroclastic studies, isotope tracing, and deposit geochemistry.5 Apatite is characterized by its abundance of primary and trace elements, with its original information being more effectively preserved post-formation. For instance, the SO3 composition of apatite can be used to estimate the sulfur content in the magma of the ore-forming host rock. The halogen content can be used to estimate the F, Cl, and H2O content in the fluids and melts, and trace elements (Mn, Ce, Eu, etc.) can indicate the redox state of the ore-forming rocks. Finally, Sr-Nd isotopes can trace the origin and evolution of the ore-forming magma or hydrothermal fluids.6 Apatite has long been recognized as a crucial instrument in the field of mineralogical research.
Due to its multiple lattice sites and variable crystal field environment, apatite has been widely studied in the field of mineral luminescence and is considered a perfect fluorescence mechanism.7 The fluorescent properties of apatite are widely used, and apatite-structured compounds are practical matrices,8,9 and numerous apatite-type luminescent materials have been prepared by some researchers and scholars in the past few years.10–12 Fluorapatite is the most luminescent subspecies within the apatite mineral group, and its dual luminescence mechanism, involving phosphorescence and fluorescence, its capacity for rare earth elements to regulate, and its stable crystal structure, all render it indispensable in the domains of gem identification and luminescent materials research. There is a wealth of research information on the luminescent properties of natural and synthetic apatite phosphors, and the research techniques are mainly laser-induced photoluminescence spectroscopy,13,14 and Laser-induced delayed luminescence (LIDL). Reisfeld et al. detected the luminescent centers of Pr3+, Eu3+, Er3+, Tm3+ and Yb3+ in apatite using laser-induced luminescence;13 Gaft et al. utilized laser-induced luminescence to detect the long-decay luminescence center of Eu3+ and to identify high symmetry position of Ca(1) in the Eu3+- substituted apatite.15 This was soon followed by the detection of the Pr3+ luminescence center using the aforementioned technique. It was ascertained that the different spectral properties of Pr3+ were related to its structural position of Ca within the apatite;16 A group of scholars conducted a study in which they examined the apatite of varying rock types utilizing steady-state fluorescence spectroscopy. They further characterized the luminescence characteristics of Ce3+ and Eu2+ in apatite. Their findings revealed that Ce in apatite attains two distinct wavelength ranges at two distinct Ca crystalline locations: 340 to 380 nanometers (nm) for Ca(I) and 420 to 450 nm for Ca(II);17 M. Czaja et al. detected luminescence spectra in apatite attributable to Sm3+, Pr3+, and Eu3+, in addition to the presence of Ce3+ and Eu2+ ions, as detected by selective excitation of steady-state fluorescence.18 The fluorescence behavior of different color apatite varies significantly. Specifically, blue–violet fluorescence is mostly triggered by Ce3+, Dy3+, and Eu2+, while orange–red fluorescence is associated with Pr3+ and Sm3+19. The underlying mechanisms behind the fluorescence phenomena exhibited by different colored apatite remain to be fully elucidated. Therefore, a comparative analysis of the fluorescence properties across diverse apatite colors is imperative to comprehensively understand their respective fluorescence characteristics.
Consequently, natural apatite samples in blue, yellow, and green colors were selected in this paper, and their chemical compositions, crystal structures, spectral characteristics, and fluorescence properties were discussed comprehensively. This study innovatively utilizes fluorescence spectroscopy and variable temperature fluorescence spectroscopy to analyze apatite. The aim is to explore the fluorescence characteristics of three colors of apatite and the effect of temperature on the fluorescence changes, and to broaden the potential applications of apatite in the field of luminescence.
The composition of apatite was tested using an EPMA-1720 electron microprobe from Shimadzu, Japan, with a detection limit of 500 ppm. Voltage set to 15 kV, carbon coated before testing.
Trace element testing was performed using an Analytik Jena Plasma Quant MS, (Jena, Germany) laser-ablation inductively coupled plasma mass spectrometer (LA-ICP-MS). The laser stripping system was a quasi-molecular laser with a resolution of 193 nm, and high-purity helium was used as the carrier gas for the experiment. The single-point analysis time was 85 s, of which the blank background acquisition time was 20 s, the continuous stripping acquisition time was 45 s, the cleaning of the injection system time was 40 s, and the sample acquisition data point size was 100 μm.
Infrared spectroscopy, Raman spectroscopy and UV-visible absorption spectroscopy were carried out at the Gem Testing Laboratory, the School of Gemology, China University of Geosciences (Beijing). Infrared spectroscopic data were acquired utilizing a TENSOR 27 Fourier transform infrared spectrometer manufactured in Germany. The measurements were conducted in reflectance method with a spectral scanning range spanning from 200 cm−1 to 4000 cm−1 Raman spectra were acquired using an HR Evolution micro-Raman spectrometer (HORIBA, Japan). The experimental voltage was 220 V, the current was 10 A, the laser wavelength was 532 nm, and the scanning range was 100–4000 cm−1. UV-vis absorption spectra were recorded using a UV-3600 UV-vis spectrophotometer (Shimadzu, Japan). The experimental conditions were as follows: the sampling interval was 2 s; the testing method was diffuse reflection method; the measuring wavelength range was 200–900 nm.
A Hitachi F-4700 fluorescence spectrophotometer equipped with a temperature control unit was used to obtain photoluminescence spectra, photoluminescence excitation spectra, and variable-temperature photoluminescence spectra of the samples. The scanning rate was 1200 nm min−1, the detection voltage was 500 V, and the warming rate of variable-temperature fluorescence was 0.17 K s−1, with a warming range of 300–575 K. The temperature range of the fluorescence was from 300 to 575 K, and the temperature range of the fluorescence was 0.17 K s−1.
| Date | APY-5 | APY-3 | APY-1 | APG-5 | APG-4 | APG-2 | APB-5 | APB-3 | APB-1 |
|---|---|---|---|---|---|---|---|---|---|
| CaO | 52.94 | 52.09 | 51.80 | 54.40 | 52.48 | 52.88 | 54.00 | 54.13 | 54.52 |
| P2O5 | 41.05 | 40.57 | 40.43 | 40.13 | 40.45 | 39.96 | 40.41 | 40.22 | 40.25 |
| SO3 | 0.20 | 0.42 | 0.42 | 0.98 | 0.85 | 0.99 | 0.90 | 0.70 | 0.56 |
| SiO2 | 0.20 | 0.43 | 0.42 | 1.02 | 0.89 | 1.13 | 1.21 | 1.04 | 1.18 |
| Na2O | 0.20 | 0.21 | 0.26 | 0.18 | 0.06 | 0.17 | 0.01 | 0.00 | 0.00 |
| MgO | 0.12 | 0.11 | 0.04 | 0.00 | 0.00 | 0.00 | 0.00 | 0.00 | 0.01 |
| Al2O3 | 0.01 | 0.00 | 0.00 | 0.00 | 0.00 | 0.02 | 0.01 | 0.02 | 0.02 |
| FeO | 0.06 | 0.12 | 0.06 | 0.00 | 0.00 | 0.00 | 0.00 | 0.03 | 0.00 |
| MnO | 0.13 | 0.08 | 0.09 | 0.00 | 0.00 | 0.00 | 0.03 | 0.03 | 0.10 |
| SrO | 0.24 | 0.21 | 0.17 | 0.35 | 0.34 | 0.24 | 0.05 | 0.04 | 0.13 |
| La2O3 | 0.30 | 0.30 | 0.31 | 0.37 | 0.21 | 0.37 | 0.10 | 0.13 | 0.21 |
| TiO2 | 0.00 | 0.01 | 0.03 | 0.03 | 0.00 | 0.00 | 0.00 | 0.06 | 0.02 |
| Ce2O3 | 0.87 | 0.74 | 0.89 | 0.65 | 0.71 | 0.82 | 0.22 | 0.35 | 0.45 |
| Nd2O3 | 0.27 | 0.21 | 0.32 | 0.21 | 0.21 | 0.23 | 0.16 | 0.01 | 0.14 |
| As2O3 | 0.00 | 0.01 | 0.00 | 0.01 | 0.00 | 0.00 | 0.06 | 0.00 | 0.00 |
| F | 2.16 | 2.72 | 2.41 | 3.37 | 3.71 | 2.24 | 3.29 | 3.30 | 3.67 |
| Cl | 1.30 | 1.22 | 1.21 | 0.32 | 0.20 | 0.34 | 0.19 | 0.16 | 0.14 |
| Ca/P | 1.63 | 1.63 | 1.62 | 1.72 | 1.64 | 1.68 | 1.69 | 1.71 | 1.72 |
| Mn/Fe | 2.47 | 0.65 | 1.55 | 0.00 | 0.00 | 0.00 | 0.00 | 0.98 | 0.00 |
| F/Cl | 1.67 | 2.23 | 2.00 | 10.54 | 18.82 | 6.61 | 17.42 | 20.89 | 26.79 |
| Total | 100.05 | 99.44 | 98.83 | 102.01 | 100.11 | 99.37 | 100.64 | 100.22 | 101.39 |
Three of each color sample were selected for calculation of their crystal chemical formulas by the oxygen atom method. In the blue, yellow and green series apatite, Ca2+ was partially replaced by ions such as Na+, Ce3+, Sr2+, Fe2+/Fe3+ and Mn2+ were observed, whereas [PO4]3− anionic groups were replaced by [SiO4]4−, and [SO4]2− isomorphic substitution occurred more frequently in apatite, indicating that the crystal structure has a certain degree of flexibility that can be replaced by a variety of cations and anions. By calculation, it can be found that the content of F− in the general formula of apatite of the three colors is greater than the content of Cl− and OH−, so the additional anions of the end elements are dominated by F−, and it can be determined that all the apatite samples in this test are fluorapatite.
As Fig. 3 and Table 2 show, the three colors of apatite exhibit a consistent “rightward shift” in the distribution of rare earth elements. This trend is characterized by an enrichment of light rare earth elements and a deficiency of heavy rare earth elements. It should also be noted that the elements Eu and Ce are present. Through the formula
;
, where a positive anomaly is defined as δ > 1 and a negative anomaly as δ < 1, it can be determined that the blue apatite sample has a δEu value of 0.43 and a δCe value of 0.84, indicating a negative Eu anomaly. Additionally, Ce exhibits a negative anomaly, though it is not pronounced; The green apatite sample has a δEu of 0.40 and a δCe of 0.84, exhibiting a negative Eu anomaly, while Ce also shows a negative anomaly but it is not significant; The yellow apatite sample has a δEu of 0.66 and a δCe of 0.85, exhibiting a moderate negative Eu anomaly, while Ce shows a negative anomaly but it is not significant. The magmatic evolution process is accompanied by changes in oxygen fugacity, and in apatite Eu and Ce are two widely differing elements with opposite distribution characteristics, so this property is an important indication for identifying the oxidation state of apatite.24,25 Under the same conditions of temperature, pressure, and magma composition, apatite crystals from highly oxidized magmas have higher levels of Eu, V, and As and lower levels of Mn, Ce, and Ga compared to apatite crystals from less oxidized magmas.25 However, the redox state of apatite cannot be determined by the valence and content of a single element because feldspathic deviation results in a lower level of Eu. Therefore, conclusions regarding the redox state of this apatite sample must be drawn in conjunction with further research.
| Samples | APB1-5 | APG1-5 | APY1-5 |
|---|---|---|---|
| Total rare earth elements (ΣREE) range (μg g−1) | 7852.12–9361.13 | 12978.76–23730.23 | 14197.93–18619.40 |
| Light rare earth elements (LREE) mean (μg g−1) | 8447.77 | 17127.90 | 15817.89 |
| Heavy rare earth elements (HREE) mean (μg g−1) | 301.86 | 477.27 | 930.25 |
| δEu | 0.43 | 0.40 | 0.66 |
| δCe | 0.84 | 0.84 | 0.85 |
From the IR transmission and reflection results, in addition to the weak [CO3]2− characteristic peaks observed in the blue and green apatite samples, it is clear that the characteristic peaks appearing in the vibrational spectra of the three colored apatite samples are mainly caused by the vibrations of the phosphorus–oxygen tetrahedra. The vibration of infrared reflection and transmission spectra of different color apatite has no significant change, only in the intensity of the peaks have been affected by the polarization rate and elemental content.
There were four distinct absorption peaks in the range of 400 to 2200 cm−1 and one distinct absorption peak in the range of 3200 to 3600 cm−1. Comparing the laser Raman spectra of the three colors of apatite, the vibrational peaks of phosphate were mainly appeared, and the symmetric vibration of V1 of [PO4]3− showed the strongest vibrational peak at 959–962 cm−1; the bending vibrational peak of V2 was weaker and was located in the range of 430–450 cm−1; the asymmetric telescopic vibrational absorption peak, V3, showed the weak vibration at the location of 1050 cm−1; and the V4 asymmetric bending vibration peak, with weak vibration at the range of 577∼603 cm−1. In the range of 3200–3600 cm−1, the samples all showed absorption peaks at 3480 cm−1, which was caused by the O–H stretching vibration, and also showed a weak absorption peak at 3296 cm−1. The vibrational mode of [CO3]2− in the Raman spectrum is a symmetric vibration at 1070 cm−1, and the other vibrational peaks of [CO3]2− in the Raman spectrum are not obvious due to the asymmetric telescopic vibration V3 of [PO4]3− is located at 1050 cm−1, which is easy to overlap. In combination with the infrared transmission spectra of the samples and the XRD analysis of the composition, it is hypothesized that the blue and green apatite samples show a substitution of [CO3]2−for [PO4]3−. In addition, a weak absorption peak at 3296 cm−1 was detected. This peak is probably caused by water in apatite.29
Comparing the UV-visible spectra of the three colors of apatite, the three colors of apatite absorb strongly in the blue-violet region, and the absorption of the yellow and green series samples is larger than that of the blue series samples, and the absorption in the blue-violet range is mainly related to Ce.33 In the yellow series apatite, there is no absorption band of 600–750 nm, and there is an absorption peak belonging to Nd3+, so the coloring mechanism of yellow apatite is mainly related to Nd3+. Green apatite, there is an absorption band of 600–750 nm, and the absorption peak belongs to Nd3+, which is the reason why the green series apatite has a yellow hue. The coloring mechanism of blue apatite is mainly related to MnO3− and SO3−.Comparing the Nd content, the Nd content of APY-1 > Nd content of APG-1 > Nd content of APB-1 is presumed to be related to the wavelength redshift of the sample colors, because the absorption peaks induced by Nd3+ were observed in all the three colors of apatite, and there was a deviation in the position of the absorption peaks. The absorption bands at 610–720 nm of each color of apatite have different contributions, and the absorption band of APY-1 is weak, which is caused by the influence of transition metals Mn and Fe, while the absorption bands of APG-1 and APB-1 have not only the contribution of transition metals, but also the contribution of Th element, which can be used as a marker for the presence of SO3− and SiO3− radicals, and the content of Th in the blue series of apatite is much higher than that of the remaining two colors. Th content of blue series apatite is much higher than that of the other two colors.
The fluorescence spectra of the three colored apatite samples show that the blue and green samples have similar fluorescence spectra, while the yellow sample has a different luminescence behavior, as shown in Fig. 8a. Fluorescence emission peaks were found at 400 nm for all three colors samples and also at 585 and 600 nm for the yellow series. As shown in Fig. 8b, a Gaussian fit was performed on the 400 nm fluorescence emission peak. Three small peaks at 393 nm, 409 nm and 434 nm were fitted to the emission peak. The emission peaks at 400 nm can be attributed to the leaps of Ce3+: (5d)5D3/2 → 2F7/2(4f) as well as (5d)5D3/2 → 2F5/2(4f) and Eu2+: 4f65d1 → (4f)8S7/2, which are a combined effect of the jumps of the two rare earth ions.34,35 LA-ICP-MS test results showed that the Eu content in apatite samples ranged from 31.34 to 101.88 ppm. Previous studies have shown that strong blue-violet fluorescence can be produced at a wavelength36 of 266 nm when the Eu content is 20 × 10−6, and that Ce3+ can act as a sensitizer for other rare earth ions.19 The two elements work together to produce fluorescence. The emission peaks of the green and blue samples showed different degrees of redshift at 400 nm with respect to the emission peaks of the yellow samples, and the phenomenon of peak shift was generally investigated by the previous researchers using the crystal field intensity analysis method37 according to the crystal field intensity calculation formula:
![]() | ||
| Fig. 8 (a) Fluorescence spectra of three color apatite samples (b) Gaussian fitting of 400 nm emission peaks under 320 nm excitation for some samples of three different color apatite. | ||
Among these, Dq refers to energy level splitting; z is the charge of the anion ligand; e is the electron charge; r is the radius of the d wave function; and R is the bond length. In apatite samples, since the values of d, z, e, and r are identical, the energy level splitting (Dq) is inversely proportional to R. According to the results of Electron probe microanalysis (EPMA) data test, all three color samples contain Na and Mg ions, so there will be the phenomenon of Na, Mg into the Ca site, the degree of substitution: yellow series > green series > blue series, because the ionic radius of Na, Mg is smaller than the ionic radius of Ca, so Na, Mg ions into the crystal lattice to replace ions larger than their own ionic radius. Based on the above equations, the entry of sodium and magnesium ions into the crystal lattice causes R to decrease, the crystal field splitting energy to increase, and the emission peak to exhibit a red shift phenomenon. However, as shown in Fig. 8, the actual situation is exactly the opposite. Therefore, for naturally occurring apatite minerals with more complex compositions, calculations of crystal field strength contribute little to explaining changes in peak positions. It is therefore speculated that the red shift observed in the fluorescence spectra of the three colored apatite samples is due to the different lattice positions of the luminescent centers Ce and Eu at an excitation wavelength of 320 nm, resulting in a red shift of the 400 nm emission peak.
The emission peaks at 585 nm and 600 nm are attributed to the leaps of Sm3+ and Pr3+, respectively, in the mode of 4G5/2 → 5H7/2 for Sm3+ and 1D2 → 3H4 for Pr3+. Pr3+ displaces the Ca(I) position in natural fluorapatite and produces a brick-red fluorescence around 610 nm.18,38 In fluorescence phenomena, Pr3+ sensitizes other rare earth elements more than it sensitizes its own emission, if Pr3+ and Sm3+ have similar characteristic jump energies.38,39 The emission intensity is strong for the yellow sample, weak for the green sample, and no corresponding emission peaks are observed for the blue sample. Comparing the Sm content of the three colored apatite samples, the average Sm content in the yellow sample was 730.76 ppm, the average Sm contant in the green sample was 431.42 ppm, and the average Sm content in the blue sample was 248.87 ppm, and the yellow sseries had the highest Sm content, so the yellow apatite showed a stronger emission peak at 585 nm, and Sm3+ had a Pr3+ sensitizing effect. When Sm and Pr ions are in close proximity, the Sm ions emit fluorescence when externally excited, while the Pr ions can receive this emission energy and become excited, enhancing the fluorescence emission of the Pr ions. This is due to the suitable coordination environment and energy matching of rare earth ions Sm and Pr at the same lattice position. When the Sm ion is in a higher excited state, the sensitization effect causes the Pr ion to also be in a higher excited state.34 The effect can be observed through changes in the fluorescence spectrum, in which the emission peak intensity of Pr ions increases and the fluorescence intensity correspondingly enhances. Thus the intensity of the emission peak at 600 nm is also stronger for both the yellow apatite sample than for the green and blue apatite samples.
Supplementary information include S-1 and S-2. S-1 is LA-ICP-MS results for three colors of apatite. S-2 is globular meteorite fossil standardization results for three colors of apatite. See DOI: https://doi.org/10.1039/d5ra03299g.
| This journal is © The Royal Society of Chemistry 2025 |