2017
DOI: 10.3390/ma10121407
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Investigation of Saturation Effects in Ceramic Phosphors for Laser Lighting

Abstract: We report observations of saturation effects in a Ce:LuAG and Eu-doped nitride ceramic phosphor for conversion of blue laser light for white light generation. The luminous flux from the phosphors material increases linearly with the input power until saturation effects limit the conversion. It is shown that the temperature of the phosphor layer influences the saturation power level and the conversion efficiency. It is also shown that the correlated color temperature (CCT), phosphor conversion efficiency and co… Show more

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Cited by 38 publications
(10 citation statements)
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“…Unfortunately, even the best performing phosphors suffer from thermal quenching at high temperatures and “droop” or “saturation quenching” at high light intensities. These unwanted effects are often already observed at LED operating conditions. ,,, CASN:Eu 2+ , for example, shows a decrease in light output of about 15% when used in high-power LEDs (incident intensity approximately 1 W mm –2 ) . For applications operating at even higher powers, such as automotive head lights and projector devices (incident intensity up to 5–10 W mm –2 ), the quenching issues become even more severe. , Despite rigorous optimization efforts mainly focused on controlling the phosphor temperature, only Ce-doped garnets (e.g., YAG:Ce 3+ ) are known to have acceptable performance in such high-power applications, while no red-emitting material is available. ,,, These issues have until now limited the commercial success of phosphor-converted solid-state lighting for ultrahigh-power applications, despite impressive improvements in LED and device design. , …”
mentioning
confidence: 99%
“…Unfortunately, even the best performing phosphors suffer from thermal quenching at high temperatures and “droop” or “saturation quenching” at high light intensities. These unwanted effects are often already observed at LED operating conditions. ,,, CASN:Eu 2+ , for example, shows a decrease in light output of about 15% when used in high-power LEDs (incident intensity approximately 1 W mm –2 ) . For applications operating at even higher powers, such as automotive head lights and projector devices (incident intensity up to 5–10 W mm –2 ), the quenching issues become even more severe. , Despite rigorous optimization efforts mainly focused on controlling the phosphor temperature, only Ce-doped garnets (e.g., YAG:Ce 3+ ) are known to have acceptable performance in such high-power applications, while no red-emitting material is available. ,,, These issues have until now limited the commercial success of phosphor-converted solid-state lighting for ultrahigh-power applications, despite impressive improvements in LED and device design. , …”
mentioning
confidence: 99%
“…With the increase of the LSN PiF concentration, the higher the phosphor content in the film, the lower conversion efficiency of absorbing blue light will be seen, so the heat accumulated on the surface of the film increases. The accumulated heat will lead to the “escape” effect, and the thermal conductivity and transmittance of the fluorescent glass film will decrease; so the saturation threshold will decrease too . The saturation threshold depends largely on the thickness of the film.…”
Section: Resultsmentioning
confidence: 99%
“…The energy losses due to low quantum efficiency will increase the temperature of phosphor converters, yielding a so‐called “thermal‐run‐away effect.” [ 14,15 ] Generally, thermal quenching becomes much more serious as the average temperature of phosphor converters exceeds 200 ℃. [ 16,17 ] Optically induced luminance saturation mainly depends on the fluorescence decay time of phosphors, [ 18,19 ] and a shorter decay time is thus preferred. For instance, the Mn 4+ doped K 2 SiF 6 with a decay time of ≈8 ms only sustains a maximum blue laser power density of 0.23 W mm −2 , [ 20 ] the Eu 2+ doped CaAlSiN 3 having a decay time of ≈0.7 μs bears a maximum of 1.5 W mm −2 , [ 13 ] and the Ce 3+ doped La 3 Si 6 N 11 with a decay time of 41.5 ns withstands a blue laser power density as high as 12.91 W mm −2 .…”
Section: Introductionmentioning
confidence: 99%