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TELKOMNIKA Telecommunication, Computing, Electronics and Control
Vol. 18, No. 5, October 2020, pp. 2385~2390
ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018
DOI: 10.12928/TELKOMNIKA.v18i5.13860  2385
Journal homepage: http://journal.uad.ac.id/index.php/TELKOMNIKA
Sr[Mg3SiN4]Eu2+ phosphor: solution for enhancing the optical
properties of the 5600K remote-packaging WLEDs
Phu Tran Tin1
, Duy Hung Ha2
, Minh Tran3
1,2
Wireless Communications Research Group, Faculty of Electrical and Electronics Engineering,
Ton Duc Thang University, Vietnam
3
Optoelectronics Research Group, Faculty of Electrical and Electronics Engineering,
Ton Duc Thang University, Vietnam
Article Info ABSTRACT
Article history:
Received Aug 10, 2019
Revised Feb 25, 2020
Accepted Mar 18, 2020
In the last decade, light-emitting diodes (LEDs), which based on spontaneous
light emission in semiconductors can be considered as the main light sources
for civil and industrial purposes. In this paper, we presented and investigated
the effect of the Sr[Mg3SiN4]Eu2+
concentration on the optical properties of
the 5600K remote-packaging WLEDs (RP-WLEDs). We use the Mat Lab
and the LightTool software to investigate the effect of the Sr[Mg3SiN4]Eu2+
concentration on the CRI, CQS, D-CCT and LO of the 5600K RP-WLEDs.
From the result, we can state that the concentration of the Sr[Mg3SiN4]Eu2+
influenced on the CRI, CQS, D-CCT and LO of the RP-WLEDs. The red
Sr[Mg3SiN4]Eu2+
phosphor can be considered as the novel recommendation
for LEDs industry.
Keywords:
CQS
CRI
D-CCT
LO
Optical properties
Red-emitting phosphor
RP-WLEDs
This is an open access article under the CC BY-SA license.
Corresponding Author:
Phu Tran Tin,
Wireless Communications Research Group,
Faculty of Electrical and Electronics Engineering,
Ton Duc Thang University,
Ho Chi Minh City, Vietnam.
Email: phutrantin@tdtu.edu.vn
1. INTRODUCTION
In the last decade, light-emitting diodes (LEDs can be considered as the main light sources for civil
and industrial purposes. In comparison with conventional lamps, LEDs with the excellent advantages such as
superior lifetime, efficiency, and reliability can be considered as the promising solution for significant
reductions in power consumption and pollution from fossil fuel power plants [1-8]. In order to improve
the performance of LEDs, a lot of issues such as chip processing, light extraction efficiency, heat sink
structures, resin materials, reliability, life test, etc. is necessary to investigate. Phosphor coating is the most
critical fluid flow problem in LED packaging since the coating process determines the phosphor thickness,
location, distribution, and morphology in LED packaging [9-15].
In this paper, we presented and investigated the effect of the Sr[Mg3SiN4]Eu2+
phosphor on
the optical properties of the 5600K remote-packaging WLEDs (RP-WLEDs). We use the Mat Lab and
the light tool software to investigate the effect of the Sr[Mg3SiN4]Eu2+
concentration on the CRI, CQS,
D-CCT, and LO of the 5600K RP-WLEDs. From the result, we can state that the concentration of
the Sr[Mg3SiN4]Eu2+
influenced on the CRI, CQS, D-CCT and LO of the RP-WLEDs. The rest of this paper
can be drawn as the following section. In the second section, the physical model and the mathematical
 ISSN: 1693-6930
TELKOMNIKA Telecommun Comput El Control, Vol. 18, No. 5, October 2020: 2385 - 2390
2386
scattering model is presented. Next, the results and some discussions are provided in third section. Finally,
some conclusions are convinced in the last section.
2. RESEARCH METHOD
Explaining research chronological, including research design, research procedure (in the form of
algorithms, Pseudocode or other), how to test and data acquisition [1-3]. The description of the course of
research should be supported references, so the explanation can be accepted scientifically [2, 4].
We conducted the physical model of the 5600K RP-WLEDs using Light Tool software with the primary
parameters as:
− We set the depth as 2.07 mm, the inner and outer radius of the reflector as 8 mm and 9.85 mm,
respectively.
− LED chips are covered with a fixed thickness of 0.08 mm and 2.07 mm.Each blue chip has a dimension
of 1.14 mm by 0.15mm, the radiant flux of 1.16 W (Figure 1) [15-20].
(a)
(b)
Figure 1. (a) The RP- WLEDs; (b) The physical model
The scattering processes in the phosphor layer can be analyzed by using the Mie-scattering theory,
as shown in [20-27]. The scattering coefficient μsca(λ).
𝜇 𝑠𝑐𝑎(𝜆) = ∫ 𝑁(𝑟)𝐶𝑠𝑐𝑎(𝜆, 𝑟)𝑑𝑟 (1)
Anisotropy factor g(λ)
𝑔(𝜆) = 2𝜋 ∫ ∫ 𝑝(𝜃, 𝜆, 𝑟)𝑓(𝑟) 𝑐𝑜𝑠 𝜃
1
−1
𝑑 𝑐𝑜𝑠 𝜃 𝑑𝑟 (2)
Reduced scattering coefficient δsca(λ)
𝛿 𝑠𝑐𝑎 = 𝜇 𝑠𝑐𝑎(1 − 𝑔) (3)
TELKOMNIKA Telecommun Comput El Control 
Sr[Mg3SiN4]Eu2+
phosphor: solution for enhancing the optical properties… (Phu Tran Tin)
2387
qhere N(r) and f(r) can be defined as
𝑓(𝑟) = 𝑓𝑑𝑖𝑓(𝑟) + 𝑓𝑝ℎ𝑜𝑠(𝑟) (4)
𝑁(𝑟) = 𝑁 𝑑𝑖𝑓(𝑟) + 𝑁𝑝ℎ𝑜𝑠(𝑟) = 𝐾 𝑁. [𝑓𝑑𝑖𝑓(𝑟) + 𝑓𝑝ℎ𝑜𝑠(𝑟)] (5)
where c is the phosphor concentration can be calculated by
𝑐 = 𝐾 𝑁 ∫ 𝑀(𝑟)𝑑𝑟 (6)
The mass distribution M(r) (milligrams) can be defined as the below equation
𝑀(𝑟) =
4
3
𝜋𝑟3
[𝜌 𝑑𝑖𝑓 𝑓𝑑𝑖𝑓(𝑟) + 𝜌 𝑝ℎ𝑜𝑠 𝑓𝑝ℎ𝑜𝑠(𝑟)] (7)
In Mie theory, Csca can be calculated as
𝐶𝑠𝑐𝑎 =
2𝜋
𝑘2
∑ (2𝑛 − 1)(|𝑎 𝑛|2
+ |𝑏 𝑛|2
)∞
0 (8)
where an and bn can be calculated by the below equations
𝑎 𝑛(𝑥, 𝑚) =
𝜓 𝑛
′ (𝑚𝑥)𝜓 𝑛(𝑥)−𝑚 𝜓 𝑛(𝑚𝑥)𝜓 𝑛
′ (𝑥)
𝜓 𝑛
′ (𝑚𝑥)𝜉 𝑛(𝑥)−𝑚 𝜓 𝑛(𝑚𝑥)𝜉 𝑛
′
(𝑥)
(9)
𝑎 𝑛(𝑥, 𝑚) =
𝑚𝜓 𝑛
′ (𝑚𝑥)𝜓 𝑛(𝑥)−𝜓 𝑛(𝑚𝑥)𝜓 𝑛
′ (𝑥)
𝑚𝜓 𝑛
′ (𝑚𝑥)𝜉 𝑛(𝑥)−𝜓 𝑛(𝑚𝑥)𝜉 𝑛
′
(𝑥)
(10)
Here, the phase function 𝑝(𝜃, 𝜆, 𝑟) can be defined as the following
𝑝(𝜃, 𝜆, 𝑟) =
4𝜋𝛽(𝜃,𝜆,𝑟)
𝑘2 𝐶𝑠𝑐𝑎(𝜆,𝑟)
(11)
where 𝛽(𝜃, 𝜆, 𝑟) is the dimensionless scattering function, which can be calculated as the followings
𝛽(𝜃, 𝜆, 𝑟) =
1
2
[|𝑆1(𝜃)|2
+ |𝑆2(𝜃)|2
] (12)
𝑆1 = ∑
2𝑛+1
𝑛(𝑛+1)
∞
𝑛=1 [
𝑎 𝑛(𝑥, 𝑚)𝜋 𝑛(𝑐𝑜𝑠 𝜃)
+𝑏 𝑛(𝑥, 𝑚)𝜏 𝑛(𝑐𝑜𝑠 𝜃)
] (13)
𝑆2 = ∑
2𝑛+1
𝑛(𝑛+1)
∞
𝑛=1 [
𝑎 𝑛(𝑥, 𝑚)𝜏 𝑛(𝑐𝑜𝑠 𝜃)
+𝑏 𝑛(𝑥, 𝑚)𝜋 𝑛(𝑐𝑜𝑠 𝜃)
] (14)
In (13) and (14), 𝜋 𝑛(𝑐𝑜𝑠 𝜃) and 𝜏 𝑛(𝑐𝑜𝑠 𝜃) are the angular dependent functions.
3. RESULTS AND ANALYSIS
In this section, we use the Mat Lab and Light Tool software to investigate the influence of
the Sr[Mg3SiN4]Eu2+
concentration on the optical properties in terms of D-CCT, CRI, CQS, and LO.
As shown in Figure 2, the D-CCT has a considerable increase with the rising of the Sr[Mg3SiN4]Eu2+
concentration. The D-CCT increases from 1000 K to 5000K when we vary the Sr[Mg3SiN4]Eu2+
concentration from 0% to 16%. From the results, we can state that the more Sr[Mg3SiN4]Eu2+
added to
the phosphor compounding, the more D-CCT can be obtained. The excellent value of the D-CCT can be
obtained with the lowest concentration of the Sr[Mg3SiN4]Eu2+
. It can be observed that the Sr[Mg3SiN4]Eu2+
takes part in the scattering processes in the phosphor layer.
Furthermore, the influence of the Sr[Mg3SiN4]Eu2+
concentration on the CQS and CRI of the 5600K
RP-WLEDs is drawn in Figures 3 and 4, respectively. From Figure 3, we can see that the CQS increases
while the Sr[Mg3SiN4]Eu2+
concentration rises from 0% to 12% and has a massive decrease with
the Sr[Mg3SiN4]Eu2+
concentration from12% to 16 %. The optimal value of the CQS is76, with 12% red
phosphor concentration. In the same way, the CRI rises when the Sr[Mg3SiN4]Eu2+
concentration increases
 ISSN: 1693-6930
TELKOMNIKA Telecommun Comput El Control, Vol. 18, No. 5, October 2020: 2385 - 2390
2388
from 0% to 10% and then decreases significantly while the Sr[Mg3SiN4]Eu2+
concentration varies from 10%
to 16%. The CRI has the maximum value as 87 with 10% Sr[Mg3SiN4]Eu2+
concentration, as illustrated
in Figure 4.
Figure 2. D-CCT
Figure 3. CQS
Figure 4. CRI
TELKOMNIKA Telecommun Comput El Control 
Sr[Mg3SiN4]Eu2+
phosphor: solution for enhancing the optical properties… (Phu Tran Tin)
2389
From these results, we can state that the Sr[Mg3SiN4]Eu2+
concentration has a significant impact on
the CQS and CRI of the 5600K RP-WLEDs. Finally, the impact of the Sr[Mg3SiN4]Eu2+
concentration on
the LO of the 5600K RP-WLEDs is presented in Figure 5. Here, we varied the Sr[Mg3SiN4]Eu2+
concentration from 0% to 16% and investigated the influence of the Sr[Mg3SiN4]Eu2+
concentration on
the LO. As shown in Figure 5, the Lo has a massive fall with the rising of the Sr[Mg3SiN4]Eu2+
concentration
to convince the influence of the Sr[Mg3SiN4]Eu2+
concentration on the LO of the 5600K RP-WLEDs.
Figure 5. LO
4. CONCLUSION
In this paper, we presented and investigated the effect of the red Sr[Mg3SiN4]Eu2+
phosphor
concentration on the optical properties of the 5600K RP-WLEDs. We use the Mat Lab and the Light Tool
Software to investigate the effect of the red phosphor concentration on the CRI, CQS, D-CCT, and LO of
the 5600K RP-WLEDs. From the result, we can state that the concentration of the red phosphor influenced
on the CRI, CQS, D-CCT and LO of the RP-WLEDs. This research can be proposed the novel
recommendation for LEDs manufacturing in the near future.
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Sr[Mg3SiN4]Eu2+ phosphor: solution for enhancing the optical properties of the 5600K remote-packaging WLEDs

  • 1. TELKOMNIKA Telecommunication, Computing, Electronics and Control Vol. 18, No. 5, October 2020, pp. 2385~2390 ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018 DOI: 10.12928/TELKOMNIKA.v18i5.13860  2385 Journal homepage: http://journal.uad.ac.id/index.php/TELKOMNIKA Sr[Mg3SiN4]Eu2+ phosphor: solution for enhancing the optical properties of the 5600K remote-packaging WLEDs Phu Tran Tin1 , Duy Hung Ha2 , Minh Tran3 1,2 Wireless Communications Research Group, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, Vietnam 3 Optoelectronics Research Group, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, Vietnam Article Info ABSTRACT Article history: Received Aug 10, 2019 Revised Feb 25, 2020 Accepted Mar 18, 2020 In the last decade, light-emitting diodes (LEDs), which based on spontaneous light emission in semiconductors can be considered as the main light sources for civil and industrial purposes. In this paper, we presented and investigated the effect of the Sr[Mg3SiN4]Eu2+ concentration on the optical properties of the 5600K remote-packaging WLEDs (RP-WLEDs). We use the Mat Lab and the LightTool software to investigate the effect of the Sr[Mg3SiN4]Eu2+ concentration on the CRI, CQS, D-CCT and LO of the 5600K RP-WLEDs. From the result, we can state that the concentration of the Sr[Mg3SiN4]Eu2+ influenced on the CRI, CQS, D-CCT and LO of the RP-WLEDs. The red Sr[Mg3SiN4]Eu2+ phosphor can be considered as the novel recommendation for LEDs industry. Keywords: CQS CRI D-CCT LO Optical properties Red-emitting phosphor RP-WLEDs This is an open access article under the CC BY-SA license. Corresponding Author: Phu Tran Tin, Wireless Communications Research Group, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam. Email: phutrantin@tdtu.edu.vn 1. INTRODUCTION In the last decade, light-emitting diodes (LEDs can be considered as the main light sources for civil and industrial purposes. In comparison with conventional lamps, LEDs with the excellent advantages such as superior lifetime, efficiency, and reliability can be considered as the promising solution for significant reductions in power consumption and pollution from fossil fuel power plants [1-8]. In order to improve the performance of LEDs, a lot of issues such as chip processing, light extraction efficiency, heat sink structures, resin materials, reliability, life test, etc. is necessary to investigate. Phosphor coating is the most critical fluid flow problem in LED packaging since the coating process determines the phosphor thickness, location, distribution, and morphology in LED packaging [9-15]. In this paper, we presented and investigated the effect of the Sr[Mg3SiN4]Eu2+ phosphor on the optical properties of the 5600K remote-packaging WLEDs (RP-WLEDs). We use the Mat Lab and the light tool software to investigate the effect of the Sr[Mg3SiN4]Eu2+ concentration on the CRI, CQS, D-CCT, and LO of the 5600K RP-WLEDs. From the result, we can state that the concentration of the Sr[Mg3SiN4]Eu2+ influenced on the CRI, CQS, D-CCT and LO of the RP-WLEDs. The rest of this paper can be drawn as the following section. In the second section, the physical model and the mathematical
  • 2.  ISSN: 1693-6930 TELKOMNIKA Telecommun Comput El Control, Vol. 18, No. 5, October 2020: 2385 - 2390 2386 scattering model is presented. Next, the results and some discussions are provided in third section. Finally, some conclusions are convinced in the last section. 2. RESEARCH METHOD Explaining research chronological, including research design, research procedure (in the form of algorithms, Pseudocode or other), how to test and data acquisition [1-3]. The description of the course of research should be supported references, so the explanation can be accepted scientifically [2, 4]. We conducted the physical model of the 5600K RP-WLEDs using Light Tool software with the primary parameters as: − We set the depth as 2.07 mm, the inner and outer radius of the reflector as 8 mm and 9.85 mm, respectively. − LED chips are covered with a fixed thickness of 0.08 mm and 2.07 mm.Each blue chip has a dimension of 1.14 mm by 0.15mm, the radiant flux of 1.16 W (Figure 1) [15-20]. (a) (b) Figure 1. (a) The RP- WLEDs; (b) The physical model The scattering processes in the phosphor layer can be analyzed by using the Mie-scattering theory, as shown in [20-27]. The scattering coefficient μsca(λ). 𝜇 𝑠𝑐𝑎(𝜆) = ∫ 𝑁(𝑟)𝐶𝑠𝑐𝑎(𝜆, 𝑟)𝑑𝑟 (1) Anisotropy factor g(λ) 𝑔(𝜆) = 2𝜋 ∫ ∫ 𝑝(𝜃, 𝜆, 𝑟)𝑓(𝑟) 𝑐𝑜𝑠 𝜃 1 −1 𝑑 𝑐𝑜𝑠 𝜃 𝑑𝑟 (2) Reduced scattering coefficient δsca(λ) 𝛿 𝑠𝑐𝑎 = 𝜇 𝑠𝑐𝑎(1 − 𝑔) (3)
  • 3. TELKOMNIKA Telecommun Comput El Control  Sr[Mg3SiN4]Eu2+ phosphor: solution for enhancing the optical properties… (Phu Tran Tin) 2387 qhere N(r) and f(r) can be defined as 𝑓(𝑟) = 𝑓𝑑𝑖𝑓(𝑟) + 𝑓𝑝ℎ𝑜𝑠(𝑟) (4) 𝑁(𝑟) = 𝑁 𝑑𝑖𝑓(𝑟) + 𝑁𝑝ℎ𝑜𝑠(𝑟) = 𝐾 𝑁. [𝑓𝑑𝑖𝑓(𝑟) + 𝑓𝑝ℎ𝑜𝑠(𝑟)] (5) where c is the phosphor concentration can be calculated by 𝑐 = 𝐾 𝑁 ∫ 𝑀(𝑟)𝑑𝑟 (6) The mass distribution M(r) (milligrams) can be defined as the below equation 𝑀(𝑟) = 4 3 𝜋𝑟3 [𝜌 𝑑𝑖𝑓 𝑓𝑑𝑖𝑓(𝑟) + 𝜌 𝑝ℎ𝑜𝑠 𝑓𝑝ℎ𝑜𝑠(𝑟)] (7) In Mie theory, Csca can be calculated as 𝐶𝑠𝑐𝑎 = 2𝜋 𝑘2 ∑ (2𝑛 − 1)(|𝑎 𝑛|2 + |𝑏 𝑛|2 )∞ 0 (8) where an and bn can be calculated by the below equations 𝑎 𝑛(𝑥, 𝑚) = 𝜓 𝑛 ′ (𝑚𝑥)𝜓 𝑛(𝑥)−𝑚 𝜓 𝑛(𝑚𝑥)𝜓 𝑛 ′ (𝑥) 𝜓 𝑛 ′ (𝑚𝑥)𝜉 𝑛(𝑥)−𝑚 𝜓 𝑛(𝑚𝑥)𝜉 𝑛 ′ (𝑥) (9) 𝑎 𝑛(𝑥, 𝑚) = 𝑚𝜓 𝑛 ′ (𝑚𝑥)𝜓 𝑛(𝑥)−𝜓 𝑛(𝑚𝑥)𝜓 𝑛 ′ (𝑥) 𝑚𝜓 𝑛 ′ (𝑚𝑥)𝜉 𝑛(𝑥)−𝜓 𝑛(𝑚𝑥)𝜉 𝑛 ′ (𝑥) (10) Here, the phase function 𝑝(𝜃, 𝜆, 𝑟) can be defined as the following 𝑝(𝜃, 𝜆, 𝑟) = 4𝜋𝛽(𝜃,𝜆,𝑟) 𝑘2 𝐶𝑠𝑐𝑎(𝜆,𝑟) (11) where 𝛽(𝜃, 𝜆, 𝑟) is the dimensionless scattering function, which can be calculated as the followings 𝛽(𝜃, 𝜆, 𝑟) = 1 2 [|𝑆1(𝜃)|2 + |𝑆2(𝜃)|2 ] (12) 𝑆1 = ∑ 2𝑛+1 𝑛(𝑛+1) ∞ 𝑛=1 [ 𝑎 𝑛(𝑥, 𝑚)𝜋 𝑛(𝑐𝑜𝑠 𝜃) +𝑏 𝑛(𝑥, 𝑚)𝜏 𝑛(𝑐𝑜𝑠 𝜃) ] (13) 𝑆2 = ∑ 2𝑛+1 𝑛(𝑛+1) ∞ 𝑛=1 [ 𝑎 𝑛(𝑥, 𝑚)𝜏 𝑛(𝑐𝑜𝑠 𝜃) +𝑏 𝑛(𝑥, 𝑚)𝜋 𝑛(𝑐𝑜𝑠 𝜃) ] (14) In (13) and (14), 𝜋 𝑛(𝑐𝑜𝑠 𝜃) and 𝜏 𝑛(𝑐𝑜𝑠 𝜃) are the angular dependent functions. 3. RESULTS AND ANALYSIS In this section, we use the Mat Lab and Light Tool software to investigate the influence of the Sr[Mg3SiN4]Eu2+ concentration on the optical properties in terms of D-CCT, CRI, CQS, and LO. As shown in Figure 2, the D-CCT has a considerable increase with the rising of the Sr[Mg3SiN4]Eu2+ concentration. The D-CCT increases from 1000 K to 5000K when we vary the Sr[Mg3SiN4]Eu2+ concentration from 0% to 16%. From the results, we can state that the more Sr[Mg3SiN4]Eu2+ added to the phosphor compounding, the more D-CCT can be obtained. The excellent value of the D-CCT can be obtained with the lowest concentration of the Sr[Mg3SiN4]Eu2+ . It can be observed that the Sr[Mg3SiN4]Eu2+ takes part in the scattering processes in the phosphor layer. Furthermore, the influence of the Sr[Mg3SiN4]Eu2+ concentration on the CQS and CRI of the 5600K RP-WLEDs is drawn in Figures 3 and 4, respectively. From Figure 3, we can see that the CQS increases while the Sr[Mg3SiN4]Eu2+ concentration rises from 0% to 12% and has a massive decrease with the Sr[Mg3SiN4]Eu2+ concentration from12% to 16 %. The optimal value of the CQS is76, with 12% red phosphor concentration. In the same way, the CRI rises when the Sr[Mg3SiN4]Eu2+ concentration increases
  • 4.  ISSN: 1693-6930 TELKOMNIKA Telecommun Comput El Control, Vol. 18, No. 5, October 2020: 2385 - 2390 2388 from 0% to 10% and then decreases significantly while the Sr[Mg3SiN4]Eu2+ concentration varies from 10% to 16%. The CRI has the maximum value as 87 with 10% Sr[Mg3SiN4]Eu2+ concentration, as illustrated in Figure 4. Figure 2. D-CCT Figure 3. CQS Figure 4. CRI
  • 5. TELKOMNIKA Telecommun Comput El Control  Sr[Mg3SiN4]Eu2+ phosphor: solution for enhancing the optical properties… (Phu Tran Tin) 2389 From these results, we can state that the Sr[Mg3SiN4]Eu2+ concentration has a significant impact on the CQS and CRI of the 5600K RP-WLEDs. Finally, the impact of the Sr[Mg3SiN4]Eu2+ concentration on the LO of the 5600K RP-WLEDs is presented in Figure 5. Here, we varied the Sr[Mg3SiN4]Eu2+ concentration from 0% to 16% and investigated the influence of the Sr[Mg3SiN4]Eu2+ concentration on the LO. As shown in Figure 5, the Lo has a massive fall with the rising of the Sr[Mg3SiN4]Eu2+ concentration to convince the influence of the Sr[Mg3SiN4]Eu2+ concentration on the LO of the 5600K RP-WLEDs. Figure 5. LO 4. CONCLUSION In this paper, we presented and investigated the effect of the red Sr[Mg3SiN4]Eu2+ phosphor concentration on the optical properties of the 5600K RP-WLEDs. We use the Mat Lab and the Light Tool Software to investigate the effect of the red phosphor concentration on the CRI, CQS, D-CCT, and LO of the 5600K RP-WLEDs. From the result, we can state that the concentration of the red phosphor influenced on the CRI, CQS, D-CCT and LO of the RP-WLEDs. This research can be proposed the novel recommendation for LEDs manufacturing in the near future. REFERENCES [1] Sheng Liu Xiaobing Luo, “LED Packaging for Lighting Applications: Design of LED Packaging Applications-Chapter 6,” pp. 215-315, 2011. doi:10.1002/9780470827857. [2] Gibney Elizabeth, “Nobel for Blue LED That Revolutionized Lighting,” Nature, vol. 514, no. 7521, pp. 152-153, 2014. doi:10.1038/514152a. [3] Winkler, Holger, Quang Trinh, Peter Bodrogi, and Tran Quoc Khanh, “LED Lighting:Technology and Perception,” Weinheim: Wiley-VCH, 2015. [4] Luo Xiaobing, Run Hu, Sheng Liu, and Kai Wang, “Heat and Fluid Flow inHigh-Power LED Packaging and Applications.” Progress in Energy and Combustion Science, vol. 56, pp. 1-32, 2016. [5] Hu Run, Xiaobing Luo, and Sheng Liu, “Effect of the Amount of Phosphor Silicone Gel on Optical Property of White Light-Emitting Diodes Packaging,” 2011 12th International Conference on Electronic Packaging Technology and High Density Packaging, 2011. doi:10.1109/icept.2011.6067015. [6] Phu Tran Tin, N. H. K. Nhan, Minh Tran, T. T. Trang, Tan N. Nguyen and Miroslav Voznak, “Co-Doping Red-Emitting Sr2si5n8:Eu2+ Into Yellow-EmittingPhosphor-Packaging For Enhancing The Optical Properties Of The 8500 K Remote-Phosphor Packaging Wleds,” Digest Journal of Nanomaterials and Biostructures, vol. 13, no. 4, pp. 1027-1034, 2018. [7] Phu Tran Tin, N. H. K. Nhan, T. H. Q. Minh, Miroslav Voznak, Tan N. Nguyen and Tran Thanh Trang, “Sr2Si5N8:Eu2+ phosphor:a novel recommendation for improving the lighting performance of the 7000 K remote- packaging white LEDs,” Proceedings of the Estonian Academy of Sciences, vol. 67, no. 4, pp. 337-341, 2018. [8] Sommer, Christian, Franz-Peter Wenzl, Paul Hartmann, Peter Pachler, Marko Schweighart, Stefan Tasch, and Günther Leising, “Tailoring of the Color Conversion Elements in Phosphor-Converted High-Power LEDs by Optical Simulations,” IEEE Photonics Technology Letters, vol. 20, no. 9, pp. 739-741, 2008. [9] Li Shuiming, Kai Wang, Fei Chen, Shuang Zhao, Zhili Zhao, and Sheng Liu, “Angular Color Uniformity Enhancement of Phosphor Converted White LEDs Integrated with Compact Modified Freeform TIR Components,” 2012 13th International Conference on Electronic Packaging Technology and High Density Packaging, 2012. [10] Liu Zongyuan, Sheng Liu, Kai Wang, and Xiaobing Luo, “Analysis of Factors Affecting Color Distribution of White LEDs,” 2008 International Conference on Electronic Packaging Technology and High Density Packaging, 2008. doi:10.1109/icept.2008.4607013.
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