# Optimization of LaPO4:Bi3+ Single-Phased White-Emitting Phosphor Luminescence Properties by Li+/Na+ Doping

Authors: Taoli Deng; Qiuyun Zhang
Journal: International Journal of Optics
 (2019)

---

## Abstract

LaPO4:Bi3+ single-phased white-emitting phosphors doped with both Li+/Na+ ions were successfully prepared by a conventional solid-state reaction technique. Microstructures were analyzed by both X-ray diffraction and high-resolution scanning electron microscopy experiments. Under the excitation of 335 nm, the L
a
0.97
P
O
4
:
B
i
3
+
0.03 phosphor showed four emission bands with maxima at 460 nm, 487 nm (blue), 530 nm (yellow), and 637 nm (red); these can be successfully combined to form pure white light in a single host lattice only by simple activator Bi3+ ion. It was found that changing the concentration of dopant (Li+, Na+ ions) did not produce a change in shape or location of the emission peaks, but the value of the emission intensity increased; this was particularly evident in the red emission, which could optimize the white light emitting performance of the phosphors. When the Na+ doping concentration was 0.02, the CIE chromaticity coordinate of phosphor L
a
0.95
P
O
4
:
B
i
3
+
0.03, N
a
+
0.02 was (0.3008, 0.3203), close to that of the standard white light.


---

## Body

## 1. Introduction

In recent years, white light-emitting diodes (WLEDs) have attracted significant attention as a promising general illumination source, due to their small volume, low energy consumption, high luminous efficiency, good safety record, and long lifetime [1–3].At present, there are two alternative approaches to WLED assembly. The main strategy in producing white light is to combine a blue LED chip with a YAG: Ce yellow phosphor. However, it is of note that several defects have been identified in this method. Firstly, blue light LEDs have low luminescence efficiency, and as device color is changed by a combination of the working temperature, voltage, and the phosphor coating thickness, this makes the white light emission unstable. Secondly, a lack of red light components results in white light which has both a high color temperature and poor color rending index. An alternative approach in the generation of white light is to use the UV chip coated with blend of tri-chromatic phosphors, which is considered more competitive in terms of color uniformity, color rendition, and long-term color stability. However, the blue emission efficiency is still poor in this white light LED system, due to the strong reabsorption of blue light by the green and red phosphors [4–7]. Therefore, the development of a series of single-phased white light phosphors is very important, which is with tunable emissions to enhance the luminous efficiency and color rendering index. It has been shown that nonrare trivalent bismuth (Bi3+) can exhibit emission in UV, emitting in the blue, green, yellow, and red regions; depending on the susceptibility of the 6s electrons to the surrounding field [8], this results in a tunable emission band from the Bi3+ ions in various doped host phosphors [9–12].LaPO4 is an excellent phosphor host, exhibiting remarkable chemical and thermal stability, having a monoclinic structure, in a single crystallographic position (P 21/n group), which is available for trivalent ions [13]. Photoluminescence properties of LaPO4 as the host material have been extensively researched in the literature [14–18]. Few single-component white-emitting phosphors codoping Bi3+/Eu3+ ions have been reported [19, 20]. However, the white-emitting phosphor LaPO4:Bi3+ of single host lattice only by simple activator Bi3+ ion is a new research, in which the white light emitting performance can be optimized by Li+/Na+ doping.


## 2. Experimental

### 2.1. Sample Preparation

Powder samplesL
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x
=
0.00,0.01,0.02,0.03) and L
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y
=
0.00,0.01,0.02,0.03) were synthesized by a conventional solid-state reaction technique [21]. Stoichiometric amounts of La2O3 (99.99%), Bi2O3 (99.99%), Li2CO3 (>99.0%), Na2CO3 (>99.0%), and NH4H2PO4 (>99.0%) were thoroughly mixed and ground in an agate mortar, before addition of a 2% excess of (NH4)2HPO4 to compensate for the evaporation of phosphorus species during high-temperature solid state reactions. The mixture was subsequently calcined successively in air at 800°C for 1 h and then at 1200°C for 8 h. After cooling to room temperature, the calcined samples were prepared for measurement by crushing


### 2.2. Characterization

The phase purity of the phosphors was checked by advance X-ray diffractometry (D/MAX-2200) with Cu Kα radiation (λ = 0.154056 nm) operated at 40 mA and 40 kV. The phosphors morphology was investigated by scanning electron microscope (EGA 3 SBU). The photoluminescence excitation (PLE) and emission (PL) spectra of the phosphors were recorded using spectrofluorimetry (PE LS55) at room temperature.


## 2.1. Sample Preparation

Powder samplesL
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x
=
0.00,0.01,0.02,0.03) and L
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y
=
0.00,0.01,0.02,0.03) were synthesized by a conventional solid-state reaction technique [21]. Stoichiometric amounts of La2O3 (99.99%), Bi2O3 (99.99%), Li2CO3 (>99.0%), Na2CO3 (>99.0%), and NH4H2PO4 (>99.0%) were thoroughly mixed and ground in an agate mortar, before addition of a 2% excess of (NH4)2HPO4 to compensate for the evaporation of phosphorus species during high-temperature solid state reactions. The mixture was subsequently calcined successively in air at 800°C for 1 h and then at 1200°C for 8 h. After cooling to room temperature, the calcined samples were prepared for measurement by crushing


## 2.2. Characterization

The phase purity of the phosphors was checked by advance X-ray diffractometry (D/MAX-2200) with Cu Kα radiation (λ = 0.154056 nm) operated at 40 mA and 40 kV. The phosphors morphology was investigated by scanning electron microscope (EGA 3 SBU). The photoluminescence excitation (PLE) and emission (PL) spectra of the phosphors were recorded using spectrofluorimetry (PE LS55) at room temperature.


## 3. Results and Discussion

### 3.1. Crystal Structure and Morphology Analysis

Figures1 and 2 present the representative XRD patterns of the L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) samples. Each phosphor spectral pattern has been successfully assigned and shows a match with standard data single phase for monoclinic LaPO4 (JCPD#35-0731) [22], with no other impurities detected. This indicates that Bi3+, Li+, and Na+ ions have been successfully incorporated into the LaPO4 host lattices. When compared to the pattern of L
a
0.97
P
O
4
:
B
i
3
+
0.03 phosphor, the spectral peaks of the phosphors have shifted to larger diffraction following Li+ and Na+ doping. This proves that Li+ and Na+ ions were incorporated into LaPO4 host crystal, by substitution of the La3+. Due to the fact that the ionic radii of Li+ (0.076nm, CN=8) and Na+ (0.102nm, CN=8) are smaller than that of La3+ (1.172 nm, CN=8) [23], incorporation of Li+/Na+ ions into LaPO4 is observed, resulting in the contraction of the host lattice. When the concentration of Li+ and Na+ ions is increased to 0.03, the diffraction peaks no longer shift to larger diffraction, implying that dopant ions may now be in the interstitial position rather than substituting the lattice ions [24].Figure 1
XRD patterns ofL
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x
=
0.00,0.01,0.02,0.03) samples calcined at 1200°C for 8 h.Figure 2
XRD patterns ofL
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y
=
0.00,0.01,0.02,0.03) samples calcined at 1200°C for 8 h.The average sizes of the crystallites were estimated by Scherrer’s equation [25]:(1)
D
=
0.89
λ
β
cos
⁡
θwhere D is the average crystallite size, λ is the wavelength of the Cu Kα line, θ is the Bragg angle, and β is the full-width at half maximum in radians. The strongest peak at 28.6° (β=0.064) was used to estimate the crystallite size by the Scherrer equation. Using this procedure gave an average crystallite size of 2.44 nm, for the prepared phosphor particles.SEM analysis ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 (Figure 3), calcined at 1200°C for 8 h, and then cooling to room temperature by crushing, indicates that the phosphors exhibit a quasi-spherical morphology with a size range of 0.5 μm-1 μm, with the prepared phosphor particles showing good dispersity.Figure 3
SEM images ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 samples after calcination at 1200°C for 8 h.


### 3.2. PL and PLE Analysis

Figure4 shows PL and PLE spectra of L
a
0.97
P
O
4
:
B
i
3
+
0.03. By monitoring of the emission at 637 nm, the PLE spectrum shows a weak band with maxima at 380 nm and a strong band at 335 nm, respectively. The strong excitation peak belongs to the 1S0→3P1 transition of Bi3+ ions. The PL spectrum excited by 335 nm radiation shows four emission bands with maxima at 460 nm, 487 nm (blue), 530 nm (yellow), and 637 nm(red). Interestingly, the emission spectrum covers the entire visible region from 400 nm to 700 nm, and these three emission bands can be successfully combined to form pure white light, in the single host lattice containing a simple activator Bi3+ ion. As we know, the electronic configuration of trivalent bismuth (Bi3+) is [Xe]-4f145d106s2, its ground state is 1S0, and the excited states of 6s 6p configuration in an increasing energy order can be split into 3P0, 3P1, 3P2, and 1P1 levers. The transitions of 1S0→3P0 and 1S0→3P2 are parity forbidden, but the transitions of 1S0→3P1 or 1P1 are parity allowed due to spin orbit coupling [26]. According to the energy levels of Bi3+, the red, yellow, and blue emissions are due to 3P1→1S0 transition depending on the susceptibility of its 6s electrons to the surrounding field.Figure 4
PL and PLE spectra ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 phosphor.


### 3.3. Discussions on the Tunable Emissions

In order to optimize the white light emitting performance of the phosphors, a series of samples with different doping concentration of Li+ and Na+ were synthesized and their PL spectra were investigated. Figures 5 and 6 showed the emission spectra of phosphors L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) and the emissions intensities at 487 nm (blue), 530 nm (yellow), and 637 nm (red) on Li+ and Na+ doping concentration. Figure 5(a) shows that the emission intensity at 637 nm is relatively unaffected by increasing Li+ doping concentration and reached maximum intensity at x=0.01. Conversely, the emissions intensity at 487 nm and 530 nm increased slowly as shown in Figure 5(b).Figure 5
Emission spectra (λ
e
x=335nm) of L
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x = 0.00, 0.01, 0.02, 0.03) phosphors (a). The emissions intensity of 487 nm (blue), 530 nm (yellow), and 637 nm (red) as function of Li+ doping concentration (red) (b).
(a)
(b)Figure 6
Emission spectra (λ
e
x = 335nm) of L
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y=0.00, 0.01, 0.02, 0.03) phosphors (a). The emissions intensity of 487 nm (blue), 530 nm (yellow), and 637 nm (red) as function of Na+ doping concentration (red) (b).
(a)
(b)A marked improvement in the emission spectra is observed when the Na+ doping concentration is increased (Figure 6(a)); the red emission intensity at 637 nm increased significantly and reached the highest a dope concentration of 0.02, with the emissions intensity at 487 nm and 530 nm still being increased slowly as shown in Figure 6(b), which indicated that the intensity of red emission at 637 nm is strongly influenced by the surrounding environment around the Bi3+. Since Li+ and Na+ ions were incorporated into the LaPO4 host crystal, by substitution of the La3+ in the interstitial position of host crystal, reducing the symmetry of the matrix materials and favoring for release of the forbidden parity, and promoting the f-f electronic transitions, which in turn increases the intensity of the red emission. Meanwhile, doping of Li+ and Na+ ions creates a charge imbalance between the phosphor systems, enhancing the activity of oxygen vacancies which can be subsequently used as a sensitizer to transfer energy to rare earth luminescent ions via charge transfer, again increasing red emission intensity [27].Different doping concentration of Li+ and Na+ ions does not produce a change in shape or location of the emission peaks, but the value of emission intensity changes especially for the red emission effecting a movement of the CIE coordinates (x, y). Table 1 shows the CIE coordinates (x, y) of various concentrations of the samples and correlated color temperature (CCT) and Figure 7 represents the corresponding CIE chromaticity diagram of the phosphors LaPO4:Bi3+ by doping Li+/Na+ ions. All the CIE coordinates shown in Table 1 of the L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors fall into the nearly white light region in the CIE diagram, which makes it suitable for the fabrication of white light emitting LEDs [28, 29].Table 1
The color coordinates of various color concentrations of the samples and correlated color temperature.
Samples
CIE coordinates (x,y)
CCTs
La0.97PO4:0.03Bi3+ (a)
(0.2778, 0.3278)
8708k
La0.96PO4:0.03Bi3+, 0.01Li+ (b)
(0.2956, 0.3221)
7520K
La0.95PO4:0.03Bi3+, 0.02Li+ (c)
(0.2775, 0.3280)
8725K
La0.94PO4:0.03Bi3+, 0.03Li+ (d)
(0.2798, 0.3226)
8699K
La0.96PO4:0.03Bi3+, 0.01Na+ (e)
(0.2821, 0.3228)
8528K
La0.95PO4:0.03Bi3+, 0.02Na+ (f)
(0.3008, 0.3203)
7302K
La0.94PO4:0.03Bi3+, 0.03Na+ (g)
(0.2797, 0.3252)
8640KFigure 7
CIE chromaticity coordinates ofL
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors.It has been proven that the red emission intensity increases with the Li+/Na+ ions doping; then, changing Li+/Na+ ions concentrations can adjust the CIE and CCT. In L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors by varying concentration of Li+/Na+ from 0 to 0.03 mol, the corresponding color tone shifted from the blue-green to white region as shown in Figure 6 (point a→b→c→d, a→e→f→g). When the Na+ doping concentration is 0.02, the CIE chromaticity coordinates of phosphor L
a
0.95
P
O
4
:
B
i
3
+
0.03, N
a
+
0.02 are (0.3008, 0.3203), close to that of the standard white light. Low CCT value implies warmer light, while the high CCT indicates colder tones [30]. For all the prepared phosphor samples, the CCT values are found to be above 5000 K, which can be regarded as a cool white light for commercial applications [31].


## 3.1. Crystal Structure and Morphology Analysis

Figures1 and 2 present the representative XRD patterns of the L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) samples. Each phosphor spectral pattern has been successfully assigned and shows a match with standard data single phase for monoclinic LaPO4 (JCPD#35-0731) [22], with no other impurities detected. This indicates that Bi3+, Li+, and Na+ ions have been successfully incorporated into the LaPO4 host lattices. When compared to the pattern of L
a
0.97
P
O
4
:
B
i
3
+
0.03 phosphor, the spectral peaks of the phosphors have shifted to larger diffraction following Li+ and Na+ doping. This proves that Li+ and Na+ ions were incorporated into LaPO4 host crystal, by substitution of the La3+. Due to the fact that the ionic radii of Li+ (0.076nm, CN=8) and Na+ (0.102nm, CN=8) are smaller than that of La3+ (1.172 nm, CN=8) [23], incorporation of Li+/Na+ ions into LaPO4 is observed, resulting in the contraction of the host lattice. When the concentration of Li+ and Na+ ions is increased to 0.03, the diffraction peaks no longer shift to larger diffraction, implying that dopant ions may now be in the interstitial position rather than substituting the lattice ions [24].Figure 1
XRD patterns ofL
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x
=
0.00,0.01,0.02,0.03) samples calcined at 1200°C for 8 h.Figure 2
XRD patterns ofL
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y
=
0.00,0.01,0.02,0.03) samples calcined at 1200°C for 8 h.The average sizes of the crystallites were estimated by Scherrer’s equation [25]:(1)
D
=
0.89
λ
β
cos
⁡
θwhere D is the average crystallite size, λ is the wavelength of the Cu Kα line, θ is the Bragg angle, and β is the full-width at half maximum in radians. The strongest peak at 28.6° (β=0.064) was used to estimate the crystallite size by the Scherrer equation. Using this procedure gave an average crystallite size of 2.44 nm, for the prepared phosphor particles.SEM analysis ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 (Figure 3), calcined at 1200°C for 8 h, and then cooling to room temperature by crushing, indicates that the phosphors exhibit a quasi-spherical morphology with a size range of 0.5 μm-1 μm, with the prepared phosphor particles showing good dispersity.Figure 3
SEM images ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 samples after calcination at 1200°C for 8 h.


## 3.2. PL and PLE Analysis

Figure4 shows PL and PLE spectra of L
a
0.97
P
O
4
:
B
i
3
+
0.03. By monitoring of the emission at 637 nm, the PLE spectrum shows a weak band with maxima at 380 nm and a strong band at 335 nm, respectively. The strong excitation peak belongs to the 1S0→3P1 transition of Bi3+ ions. The PL spectrum excited by 335 nm radiation shows four emission bands with maxima at 460 nm, 487 nm (blue), 530 nm (yellow), and 637 nm(red). Interestingly, the emission spectrum covers the entire visible region from 400 nm to 700 nm, and these three emission bands can be successfully combined to form pure white light, in the single host lattice containing a simple activator Bi3+ ion. As we know, the electronic configuration of trivalent bismuth (Bi3+) is [Xe]-4f145d106s2, its ground state is 1S0, and the excited states of 6s 6p configuration in an increasing energy order can be split into 3P0, 3P1, 3P2, and 1P1 levers. The transitions of 1S0→3P0 and 1S0→3P2 are parity forbidden, but the transitions of 1S0→3P1 or 1P1 are parity allowed due to spin orbit coupling [26]. According to the energy levels of Bi3+, the red, yellow, and blue emissions are due to 3P1→1S0 transition depending on the susceptibility of its 6s electrons to the surrounding field.Figure 4
PL and PLE spectra ofL
a
0.97
P
O
4
:
B
i
3
+
0.03 phosphor.


## 3.3. Discussions on the Tunable Emissions

In order to optimize the white light emitting performance of the phosphors, a series of samples with different doping concentration of Li+ and Na+ were synthesized and their PL spectra were investigated. Figures 5 and 6 showed the emission spectra of phosphors L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) and the emissions intensities at 487 nm (blue), 530 nm (yellow), and 637 nm (red) on Li+ and Na+ doping concentration. Figure 5(a) shows that the emission intensity at 637 nm is relatively unaffected by increasing Li+ doping concentration and reached maximum intensity at x=0.01. Conversely, the emissions intensity at 487 nm and 530 nm increased slowly as shown in Figure 5(b).Figure 5
Emission spectra (λ
e
x=335nm) of L
a
0.97
-
x
P
O
4
:
B
i
3
+
0.03, L
i
+
x (x = 0.00, 0.01, 0.02, 0.03) phosphors (a). The emissions intensity of 487 nm (blue), 530 nm (yellow), and 637 nm (red) as function of Li+ doping concentration (red) (b).
(a)
(b)Figure 6
Emission spectra (λ
e
x = 335nm) of L
a
0.97
-
y
P
O
4
:
B
i
3
+
0.03, N
a
+
y (y=0.00, 0.01, 0.02, 0.03) phosphors (a). The emissions intensity of 487 nm (blue), 530 nm (yellow), and 637 nm (red) as function of Na+ doping concentration (red) (b).
(a)
(b)A marked improvement in the emission spectra is observed when the Na+ doping concentration is increased (Figure 6(a)); the red emission intensity at 637 nm increased significantly and reached the highest a dope concentration of 0.02, with the emissions intensity at 487 nm and 530 nm still being increased slowly as shown in Figure 6(b), which indicated that the intensity of red emission at 637 nm is strongly influenced by the surrounding environment around the Bi3+. Since Li+ and Na+ ions were incorporated into the LaPO4 host crystal, by substitution of the La3+ in the interstitial position of host crystal, reducing the symmetry of the matrix materials and favoring for release of the forbidden parity, and promoting the f-f electronic transitions, which in turn increases the intensity of the red emission. Meanwhile, doping of Li+ and Na+ ions creates a charge imbalance between the phosphor systems, enhancing the activity of oxygen vacancies which can be subsequently used as a sensitizer to transfer energy to rare earth luminescent ions via charge transfer, again increasing red emission intensity [27].Different doping concentration of Li+ and Na+ ions does not produce a change in shape or location of the emission peaks, but the value of emission intensity changes especially for the red emission effecting a movement of the CIE coordinates (x, y). Table 1 shows the CIE coordinates (x, y) of various concentrations of the samples and correlated color temperature (CCT) and Figure 7 represents the corresponding CIE chromaticity diagram of the phosphors LaPO4:Bi3+ by doping Li+/Na+ ions. All the CIE coordinates shown in Table 1 of the L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors fall into the nearly white light region in the CIE diagram, which makes it suitable for the fabrication of white light emitting LEDs [28, 29].Table 1
The color coordinates of various color concentrations of the samples and correlated color temperature.
Samples
CIE coordinates (x,y)
CCTs
La0.97PO4:0.03Bi3+ (a)
(0.2778, 0.3278)
8708k
La0.96PO4:0.03Bi3+, 0.01Li+ (b)
(0.2956, 0.3221)
7520K
La0.95PO4:0.03Bi3+, 0.02Li+ (c)
(0.2775, 0.3280)
8725K
La0.94PO4:0.03Bi3+, 0.03Li+ (d)
(0.2798, 0.3226)
8699K
La0.96PO4:0.03Bi3+, 0.01Na+ (e)
(0.2821, 0.3228)
8528K
La0.95PO4:0.03Bi3+, 0.02Na+ (f)
(0.3008, 0.3203)
7302K
La0.94PO4:0.03Bi3+, 0.03Na+ (g)
(0.2797, 0.3252)
8640KFigure 7
CIE chromaticity coordinates ofL
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors.It has been proven that the red emission intensity increases with the Li+/Na+ ions doping; then, changing Li+/Na+ ions concentrations can adjust the CIE and CCT. In L
a
0.97
-
x
-
y
P
O
4
:
B
i
3
+
0.03, L
i
+
x, N
a
+
y (x
=
0.00,0.01,0.02,0.03
,
y
=
0.00,0.01,0.02,0.03) phosphors by varying concentration of Li+/Na+ from 0 to 0.03 mol, the corresponding color tone shifted from the blue-green to white region as shown in Figure 6 (point a→b→c→d, a→e→f→g). When the Na+ doping concentration is 0.02, the CIE chromaticity coordinates of phosphor L
a
0.95
P
O
4
:
B
i
3
+
0.03, N
a
+
0.02 are (0.3008, 0.3203), close to that of the standard white light. Low CCT value implies warmer light, while the high CCT indicates colder tones [30]. For all the prepared phosphor samples, the CCT values are found to be above 5000 K, which can be regarded as a cool white light for commercial applications [31].


## 4. Conclusions

The luminescence properties of LaPO4:Bi3+ single-phased white-emitting phosphors were optimized by Li+/Na+ doping, prepared by conventional solid-state reaction techniques. The prepared phosphor particles show good dispersity with a size range of 0.5μm-1μm. It was found that the PL spectrum excited by 335 nm radiation shows four emission bands with maxima at 460 nm, 487 nm (blue), 530 nm (yellow), and 637 nm (red), covering the entire visible region from 400 nm to 700 nm. These color emission bands can be successfully combined to form pure white light in the single host lattice only by simple activator Bi3+ ion. The phosphor emission intensity at 637 nm hardly increases with Li+ and Na+ doping, making the corresponding color tone shifted from the blue-green to white region. Finally, for the LaPO4:Bi3+ single-phased phosphors optimized by doping with Li+/Na,+ when the Na+ doping concentration is 0.02, the CIE chromaticity coordinates is (0.3008, 0.3203), which has been close to that of the standard white light, and can be regarded as a cool white light for commercial applications.



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*Source: 4530978-2019-03-03.xml*