As shown in
Figure 2, the DTA curve of the glass powder has been measured by a differential thermal analysis to show the glass transition temperature (T
g) and melting temperature (T
m) of the glass matrix.
Figure 2 shows that the T
g and T
m are 557℃ and 603℃, respectively. Therefore, a sintering temperature of 700℃ in this study may be suitable for the fabrication of the four-inch PiG. The photoluminescence excitation (PLE) spectrum and emission spectrum of the YAG: Ce
3+ phosphor have been measured by a fluorescence spectrometer, as shown in
Figure 3.
Figure 3 shows the excitation and emission spectrum of the YAG: Ce
3+ phosphor with peaks at 450 nm and 563 nm, respectively. The mixture of the two will present white light due to the yellow light and blue light are complementary colors in chromatics. The XRD patterns of the four-inch PiG powder at a sintering temperature of 700°C was determined by an X-ray diffraction analyzer. As shown in
Figure 4, all the diffraction peaks were in accordance with the JCPDs card no. 33-0040 pattern, indicating no crystallization of the glass phase was found.
In this study, a total of four four-inch PiG fabrication conditions were generated to develop high-performance and high-reliability four-inch YAG: Ce3+ PiG for automotive headlight applications. Through precisely adjusting the thickness of the four golden formula four-inch PiG plates to 0.08, 0.10, 0.12, and 0.15 mm, the four golden formula four-inch PiG plates have similar chromaticity and CCT, as shown in
Table 1 and
Table 2.
Table 2 lists the optical properties of the four fabricated condition four-inch PiG plates, which excited by a 450 nm blue LED chip. The high luminous efficacy was 118 lm/W for the PiG plates with a thickness of 0.08 nm.
Table 2 shows that the luminous efficacy of the four-inch PiG plates decreases as thickness increases. The luminous efficacy of the PiG plate with a thickness of 0.08 mm was about 16.83% higher than that of the PiG plate with a thickness of 0.15 mm. Therefore, the thickness of the four-inch PiG plate was significantly affecting the optical characteristics and needs further study. Based on the results in
Table 2, we performed further analysis to determine the cause of the low luminous efficacy for four-inch PiG plates with a thickness of 0.15 mm. The results are shown in
Figure 5,
Figure 6,
Figure 7 and
Table 3.
The microstructure measurements of the four-inch PiG plates are shown in
Figure 5 and
Table 3.
Figure 5 shows FE-SEM micrographs of the four-inch PiG plates with the thicknesses of (a) 0.08 mm and (b) 0.15 mm, respectively. As shown in
Table 3, the porosity of the four-inch PiG plates with the thicknesses of 0.08 mm, 0.10 mm, 0.12 mm, and 0.15 mm, estimated from the micrographs, are in the range of 1.34%, 1.37%, 1.38%, and 1.33%, respectively. From the measurement results, there was no significant difference in the porosity of the four-inch PiG plates under the four fabrication conditions. However, the number of pores increases as the thickness increases. This indicates that in the PiG plate the interaction between the pores and light increase, resulting in more light scattering, which in turn affects the optical performance of the PiG plate [
11]. This may be one of the reasons why the luminous efficacy of the PiG plate with a thickness of 0.15 mm is lower than that of the PiG plate with a thickness of 0.08 mm.
Figure 6 depicts the light emission spectrum of the four-inch PiG plates. The peak intensities of the emission spectrum at 450 nm and 563 nm decrease as the thickness of the PiG plate increases. It can be clearly seen that the luminous efficacy of the PiG plate will also decrease with the increase of the thickness of the PiG plate. As a result, the PiG plate with a thickness of 0.08 mm for vehicle headlight applications obtained significantly improved luminous efficacy due to the reduced interaction between the pores and light. This was consistent with the result of
Table 2.
Figure 7 shows the measured transmittance of the PiG plates with the thicknesses of 0.08 mm and 0.15 mm. This was due to number of pores increased as the thickness of the PiG plate increased. These induced interaction between the pores and light, resulting in more light scattering. Therefore, the transmittance value of PiG plate with a thickness of 0.08 mm was higher than that of PiG plate with a thickness of 0.15 mm. The result was consistent with the light emission spectrum of the four-inch PiG plates in
Figure 6. As shown in
Figure 8, we further measured the uniformity of the five four-inch PiG plates with a thickness of 0.08 mm using an integrating sphere measurement system, at points (A), (B), (C), (D), (E), (F), (G), (H), and (I). The measured results of a total of 45 points were shown in
Figure 9. The differences in CIE (x, y) of a total of 45 points were less than 3.9×10
-3. From the nine-point measurement results, the precisely fabricating process achieved the four-inch PiG plates with a thickness of 0.08 mm with good uniformity and excellent performance. To study the thermal stability of the PiG plate with a thickness of 0.08 mm, a thermal aging test at stress temperature of 150°C, 250°C, 350°C, and 450°C for 1008 hours were performed.
Figure 10 shows the results of the PiG plate with a thickness of 0.08 mm before and after thermal aging tests at stress temperature of 150°C, 250°C, 350°C, and 450°C for 1008 hours. The optical performance of the CIE and luminous efficacy did not significantly change before and after thermal aging. This indicates that the PiG plate with a thickness of 0.08 mm is also with high thermal stability.