Disclosure of Invention
Therefore, an object of the present invention is to provide a nitride light emitting material. The nitride luminescent material can be effectively excited by light with the wavelength range of 350-500nm and efficiently emits in a visible light region, and is an ideal luminescent material.
In order to achieve the purpose, the invention adopts the following technical scheme:
a nitride light emitting material comprising an inorganic compound of the formula [ I ],
MmAbXyDz [I]
wherein
M is one or the combination of more than two of La, Lu, Gd and Y,
a is one or two of Si and Ge,
x is N, or N and F,
d is one or the combination of more than two of Dy, Ce and Pr, wherein Pr and/or Dy must be contained, and
2. ltoreq. m.ltoreq.4, m being, for example, 2.2, 2.4, 2.5, 2.55, 2.63, 2.7, 2.9, 3.1, 3.3, 3.5, 3.7, 3.85, 3.9, etc.,
b is 5-7, b is, for example, 5.2, 5.4, 5.5, 5.55, 5.63, 5.7, 5.9, 6.1, 6.3, 6.5, 6.7, 6.85, 6.9, etc.,
y is 10.5-11.5, such as 10.6, 10.8, 10.9, 11.0, 11.15, 11.22, 11.3, 11.35, 11.4, 11.45, etc
0 < z.ltoreq.0.5, and z is, for example, 0.02, 0.04, 0.06, 0.08, 0.1, 0.15, 0.2, 0.22, 0.26, 0.32, 0.36, 0.4, 0.42, 0.43, 0.45, 0.48, or the like. Preferably, the luminescent material has a structure similar to La3Si6N11The same crystal structure.
Dy singly doped3+After being excited, the light emitting diode can respectively emit blue-green light and yellow-orange light, and the combination forms white light, so that the problem of low luminous efficiency caused by the mutual absorption action easily existing among various activator ions is solved. In addition, doped with Pr3+Light emitted by blue excitation after ionization can be used for backlight display to improve color gamut. With La3Si6N11The crystal structure is used as a substrate, and a luminescent material with high thermal stability can be further prepared, so that the method can be suitable for a device excited by high energy density.
In the nitride luminescent material, the crystal structure is constructed by an M-A polyhedron, and luminescent materials with different structures can be obtained by linking M and A-N tetrahedrons in an angle-angle or edge-edge manner. In order to make the nitride luminescent material of the invention have La3Si6N11The nitride luminescent material has the same crystal structure, and other mixed phases are not introduced, so that when the M element is one or the combination of more than two of the trivalent rare earth elements La, Lu, Y and Gd in the nitride luminescent material, the strict growth of the crystal lattice of the luminescent material can be ensured, and the high-stability luminescent material can be obtained. However, the amount of the above elements should be appropriate, and when m < 2, pure phase cannot be generated due to the difference of the element ratio during the firing process, resulting in deterioration of the performance of the light emitting material; when m > 4, the excess of the raw material remains to influence the generation of a pure phase of the luminescent material as well, and the temperature characteristics of the luminescent material are also deteriorated, and therefore, it is necessary to define: m is more than or equal to 2 and less than or equal to 4.
X is N element, which enables the luminescent material synthesized by the selected elements and La3Si6N11The same crystal structure. When y is less than 10.5 or y is more than 11.5, the valence in the crystal is unbalanced due to the difference of the element ratio, the instability of the structure is caused, and the ideal luminescent material is not easy to obtain, therefore, the following limitations are required: y is more than or equal to 10.5 and less than or equal to 11.5.
In the nitride luminescent material, D ions are used as activator ions, and after a plurality of experiments, the optimal effect is achieved when the limiting range of the concentration of the activator is more than 0 and less than or equal to 0.5. When the content of D is more than 0.5, on one hand, the structure instability is increased and even a mixed phase is generated due to mismatching of the ion radius after the D enters the crystal lattice, on the other hand, too many D ions generate a concentration quenching effect due to too small ion distance, and the luminous brightness is reduced along with the increase of the D ions.
According to the nitride luminescent material, the peak position of the excitation wavelength and the peak wavelength of the emission wavelength are different according to the selected specific element types and dosage ratios.
Preferably, D is Dy.
Preferably, a is Si.
Preferably, M is La.
Preferably, the peak wavelength of the excitation spectrum of the luminescent material is 380-390 nm, the peak wavelength of the main emission peak is 570-580 nm, and the secondary peak wavelength is 470-480 nm.
Preferably, D is Pr.
Preferably, a is Si.
Preferably, M is La.
Preferably, the peak wavelength of the excitation spectrum of the luminescent material is 450-470 nm, the peak wavelength of the main emission peak is 660-670 nm, and the secondary peak wavelength is 500-510 nm.
Preferably, the luminescent material may be one or a combination of two or more of powder, ceramic, and crystal.
The preparation method of the nitride light emitting material of the present invention can be prepared by methods known in the art, such as a high temperature solid phase method.
In a preferred embodiment of the present invention, the raw materials and their proportions of the elements required in the general formula of the nitride luminescent material according to the present invention are uniformly mixed and then calcined at high temperature; and (3) taking out the furnace after calcining and sintering, and carrying out post-treatment steps including grinding, acid washing, sieving, drying and the like on the powder.
The raw materials of the elements are preferably simple substances or compounds of various metal and nonmetal elements, and the compound is preferably a nitride.
Preferably, the calcination is carried out in a reducing atmosphere or an inert atmosphere, preferably in a high-pressure or atmospheric furnace protected by a reducing atmosphere or an inert atmosphere, in order to ensure a low oxygen content of the environment.
Preferably, the reducing atmosphere or inert atmosphere is one or a combination of two or more of nitrogen, hydrogen or CO gas.
Nitrides, because of their stable covalent bonds, require higher temperatures to facilitate product synthesis. Preferably, according to theory and experiment, the temperature of the high-temperature calcination is 1400-1800 ℃, preferably 1600 ℃, the calcination time is 20min-24h, if the holding time is too short, the reaction is not sufficient, and the excessive time causes abnormal growth of crystal grains, preferably 6-15 h.
It is also an object of the present invention to provide a light-emitting device comprising the luminescent material of the present invention.
Preferably, the light-emitting device further comprises a radiation source. Preferably, the radiation source is a laser light source or a semiconductor light source.
Wherein the laser light source includes but is not limited to vacuum ultraviolet emission source, purple light emission source or blue light emission source; semiconductor light sources include, but are not limited to, ultraviolet LEDs, violet LEDs, blue LEDs, and the like.
Preferably, the light-emitting device further comprises another light-emitting material excited by the radiation source.
Preferably, the other luminescent material is one or a combination of two or more of the following fluorescent substances: (Y, Gd, Lu, Tb)3(Al,Ga)5O12:Ce3+、β-SiAlON:Eu2+、(Ca,Sr)AlSiN3:Eu2+、(Li,Na,K)2(Ti,Zr,Si,Ge)F6:Mn4+、(Ca,Sr,Ba)MgAl10O17:Eu2+。
The invention adjusts M: a: the proportion of D can form La taking D ions as luminescent centers3Si6N11Crystal structure, which makes the activator center obtain higher transition energy under the action of Si-N tetrahedral field, thereby obtaining high-efficiency emission, and La3Si6N11The crystal structure is used as a matrix, so that a luminescent material with high thermal stability is prepared, and the luminescent material can be suitable for a device excited by high energy density.
Detailed Description
For the purpose of facilitating an understanding of the present invention, the present invention will now be described by way of examples. It should be understood by those skilled in the art that the examples are only for the purpose of facilitating understanding of the present invention and should not be construed as specifically limiting the present invention.
In the following examples, the XRD patterns were subjected to X-ray diffraction using a Co target (λ 1.78892 nm). The emission spectrum is acquired by a high-sensitivity integrated fluorescence spectrometer of FluoroMax-4 model of Horiba company.
Comparative example 1
According to the formula Y2.9Al5O11:Dy0.1The raw materials are weighed according to the mixture ratio. Grinding the raw material mixture in an agate mortar uniformly, putting the mixture into a corundum crucible, roasting the mixture at 1400 ℃ for 4 hours at the heating speed of 5 ℃/min by taking carbon monoxide as a reducing atmosphere, and cooling the mixture to room temperature. And grinding the obtained sintered product, and performing post-treatment processes such as ball milling and grinding to obtain a sample.
Comparative example 2
According to the formula Y2.91Al5O11:Pr0.09The raw materials are weighed according to the mixture ratio. Grinding the raw material mixture in an agate mortar uniformly, putting the mixture into a corundum crucible, roasting the mixture at 1400 ℃ for 4 hours at the heating speed of 5 ℃/min by taking carbon monoxide as a reducing atmosphere, and cooling the mixture to room temperature. And grinding the obtained sintered product, and performing post-treatment processes such as ball milling and grinding to obtain a sample.
The samples prepared in comparative examples 1 and 2 were commercially available YAG phosphors.
Example 1
By mixing the following La2.9Si6N11:Dy0.1LaN, CeN and Si weighed according to stoichiometric ratio3N4And mixing the DyN powder in a mortar uniformly, keeping the temperature of 1600 ℃ for 3 hours in a reducing atmosphere, crushing the obtained product, washing with water to remove impurities, sieving and drying to obtain the product.
The XRD pattern of the sample prepared in this example is shown in FIG. 1, demonstrating the formation of La2.9Si6N11Phase (1); the emission spectrum under 387nm excitation is shown in fig. 2, demonstrating that a spectrum according to our design is obtained. It was measured that comparative example 1 was selected as a comparison, and the relative luminous intensity of this sample was 145%. When the temperature is raised to 150 ℃, the luminous intensity can still be kept at 87%, which shows the good stability of the product of the invention. The products of examples 2-22 maintained greater than 83% luminous intensity when raised to 150 ℃.
Examples 2 to 14
Examples 2-14 have a similar synthesis to example 1. In examples 2-14, the emission spectra are similar to those of FIG. 2. The chemical formulas of examples 2 to 14 and the relative luminescence intensities thereof are shown in Table 1, and the relative luminescence intensities in Table 1 are compared with those of comparative example 1.
TABLE 1
Name (R)
|
Chemical composition
|
Relative luminescence intensity (%)
|
Example 2
|
La2Dy0.01Si6.35N10.5 |
110
|
Example 3
|
Dy0.01Gd2.71Si5Ge0.835N10.5 |
105
|
Example 4
|
Dy0.11La2.89Si6N11 |
137
|
Example 5
|
Dy0.066Y2.1Si7N11.5 |
102
|
Example 6
|
Dy0.15La2Si6.41N10.7 |
104
|
Example 7
|
Dy0.07La2.93Si6N11 |
112
|
Example 8
|
Dy0.386Gd2.834Si4.5Ge1.46N11F0.5 |
105
|
Example 9
|
Dy0.07La2.93Si6N11 |
125
|
Example 10
|
Dy0.06La4Si5N10.5F0.68 |
130
|
Example 11
|
Dy0.5Sc2.33Si6.5N11.5 |
112
|
Example 12
|
Dy0.04La3.3Si5.24N10F1.02 |
105
|
Example 13
|
Lu4Dy0.33Si4.5Ge0.5N11 |
133
|
Example 14
|
Dy0.05Ce0.02La2.93Si6N11 |
132 |
Example 15
By mixing the following La2.91Si6N11:Pr0.09Respectively weighing LaN, CeN and Si in stoichiometric ratio3N4And uniformly mixing the PrN powder in a mortar, and carrying out heat preservation for 3 hours at 1600 ℃ in a reducing atmosphere, and crushing, washing and removing impurities, sieving and drying the obtained product to obtain the product.
The emission spectrum of the sample prepared in this example under the excitation of 460nm light is similar to that of FIG. 3. This sample was measured to have a luminous intensity of 150% by comparison with comparative example 2.
Examples 16 to 22
Examples 16-22 have a similar synthesis to example 15. In examples 16 to 22, the emission spectra are shown in FIG. 3. The chemical formulas of examples 16 to 22 and their relative luminous intensities are shown in Table 2, and the relative luminous intensities in Table 2 are compared with those of comparative example 2.
TABLE 2
Name (R)
|
Chemical composition
|
Relative luminescence intensity (%)
|
Example 16
|
Pr0.5Lu4Ge5.25N11.5 |
145
|
Example 17
|
Pr0.4La3.93Si5N11 |
146
|
Example 18
|
Pr0.45Lu2.9Ge6N10F1.01 |
122
|
Example 19
|
Lu0.02Pr0.07La3.23Si5.91N11.2 |
112
|
Example 20
|
Y0.016Pr0.1Lu2.05Ge7N11.5 |
148
|
Example 21
|
Dy0.03Ce0.02Lu1.45Pr0.35Gd2.115Si5.649N11.5 |
115
|
Example 22
|
Dy0.2Lu0.8Pr0.01La1.2Si3.13Ge3N10F1.15 |
112 |
It should be understood that the above examples are only for clarity of illustration and are not intended to limit the embodiments. Other variations and modifications will be apparent to persons skilled in the art in light of the above description. And are neither required nor exhaustive of all embodiments. And obvious variations or modifications therefrom are within the scope of the invention.