WO2022233115A1 - 一种增强Er离子光致发光的无铅双钙钛矿及其制备方法和应用 - Google Patents
一种增强Er离子光致发光的无铅双钙钛矿及其制备方法和应用 Download PDFInfo
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- WO2022233115A1 WO2022233115A1 PCT/CN2021/128247 CN2021128247W WO2022233115A1 WO 2022233115 A1 WO2022233115 A1 WO 2022233115A1 CN 2021128247 W CN2021128247 W CN 2021128247W WO 2022233115 A1 WO2022233115 A1 WO 2022233115A1
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- C09K11/77—Luminescent materials, e.g. electroluminescent or chemiluminescent containing inorganic luminescent materials containing rare earth metals
- C09K11/7704—Halogenides
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- H10F77/45—Wavelength conversion means, e.g. by using luminescent material, fluorescent concentrators or up-conversion arrangements
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Definitions
- the present invention relates to the technical field of luminescent materials, and more particularly, to a lead-free double perovskite capable of enhancing Er ion photoluminescence and a preparation method and application thereof.
- Near-infrared light sources have good penetrability to organic matter, so they have great application potential in optoelectronics, food detection, anti-counterfeiting technology and biology.
- traditional near-infrared light sources such as tungsten filament lamps and halogen lamps are hindered from their applications due to their low quantum efficiency, high operating temperature and long response time. Therefore, we urgently need an efficient and sustainable near-infrared material for light sources. .
- Rare earth doped semiconductor materials have broad application prospects in the field of optoelectronics, so they have received keen attention.
- Modern telecommunications networks that transmit data at the speed of light worldwide are based on fiber optic cables and rely on the transmission and processing of optical signals.
- the energy level transition of 4 I 13/2 - 4 I 15/2 in Er ions results in a wavelength emission of 1.5 ⁇ m, which is just in the low-loss window in optical fiber communication, and because the luminescence of Er ions at 1.5 ⁇ m is the 4f shell of Er
- the energy position of the luminescence peak is basically not affected by the matrix material, nor does it depend on the ambient temperature. application.
- due to the ff forbidden transition of Er ion itself its quantum efficiency and absorption coefficient are low, and the emission intensity of near-infrared light cannot meet the requirements, which limits its application and must be excited with high pump power density to obtain optical gain.
- CN112480921A discloses a phosphor powder with different emission peaks doped with rare earth ions in the same host and a preparation method.
- the phosphor powder is based on NaY(MoO 4 ) 2 , and is double-doped with Dy 3+ and Er 3+ under the excitation of different wavelengths of near-infrared light and near-ultraviolet light to obtain characteristic up-conversion and down-conversion fluorescence emission, and Er 3+ green Luminescence (at 525nm and 553nm) and blue (at 479nm) and green (at 574)nm) light of Dy 3+ , real
- the above phosphors can improve the characteristic peak luminous intensity of Er 3+ by increasing the amount of Dy 3+ ion doping, but it is only aimed at the green light emission intensity at 553 nm, and cannot solve the near-infrared light emission intensity of Er ion phosphor materials. The problem of not meeting the requirements.
- the technical problem to be solved by the present invention is to overcome the defects and deficiencies that the existing rare earth Er ion light conversion materials cannot achieve strong near-infrared emission in the ultraviolet to visible light region, and provide a lead-free double perovskite that enhances Er ion photoluminescence .
- Another object of the present invention is to provide a preparation method of a lead-free double perovskite with enhanced Er ion photoluminescence.
- Another object of the present invention is to provide an application of a lead-free double perovskite that enhances Er ion photoluminescence in the fields of near-infrared LEDs, low-loss optical fiber communications and germanium-based solar cells.
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 1-xy Cr x E y Cl 6 , 0.00 ⁇ x ⁇ 1.00, 0.00 ⁇ y ⁇ 1.00.
- x and y are the molar percentages of doping ions Cr 3+ and Er 3+ respectively relative to the host ions In 3+ .
- the enhanced Er ion photoluminescence lead-free double perovskite of the present invention uses Cs 2 AgInCl 6 as a host, and Cs 2 AgInCl 6 is a direct band gap semiconductor and has excellent stability.
- the lead-free double perovskite enhancing Er ion photoluminescence of the present invention is based on the lead-free double perovskite Cs 2 AgInCl 6 , the luminescent centers are trivalent Cr 3+ and Er 3+ ions respectively, and the light conversion material is at 250 Under excitation at ⁇ 900nm , trivalent Cr 3+ ions generate infrared light with a peak at 1010 nm in the matrix, and Er 3+ ions generate infrared light with a peak at 1540 nm .
- the emission is at 1010 nm, which is close to the absorption of 4 I 15/2 ⁇ 4 I 11/2 of Er ions, which can produce efficient energy transfer, so that the luminescence of the activated ion Er is enhanced, with broadband excitation and strong excitation in the ultraviolet to visible light region.
- the advantages of NIR emission are at 1010 nm, which is close to the absorption of 4 I 15/2 ⁇ 4 I 11/2 of Er ions, which can produce efficient energy transfer, so that the luminescence of the activated ion Er is enhanced, with broadband excitation and strong excitation in the ultraviolet to visible light region.
- the Er ion photoconversion material of the present invention uses co-doping to form a sensitization method for energy transfer, and Cr 3+ ions are used as sensitizing ions, Strengthen the near-infrared luminous intensity of activated ions Er 3+ ions, increase the absorption rate by sensitizing ions, increase the quantum efficiency of Er ions near-infrared by energy transfer, and can use lower intensity or lower energy light sources (such as different wavelengths).
- the light-emitting diode (LED) to excite and modulate the light source, so as to meet the application requirements of optical fiber communication.
- the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 1-xy Cr x E y Cl 6 , 0.1 ⁇ x ⁇ 0.8, 0.1 ⁇ y ⁇ 0.8.
- the invention also specifically protects a preparation method of a lead-free double perovskite that enhances Er ion photoluminescence, comprising the following steps: mixing compounds containing Ag, In, Cr and Er, adding hydrochloric acid, stirring and dissolving, and then adding The Cs-containing compound initiates a precipitation reaction, the reaction temperature is 30-100° C., the reaction is complete, and the lead-free double perovskite is obtained by cooling, separation, cleaning, and drying.
- the reaction temperature of the present invention needs to be controlled at 30-100° C., and if the reaction temperature is too high, impurity phases will be formed, and at the same time, the luminescence of the material will be reduced.
- the reason why the temperature is controlled at 30-100 °C is that high-purity and high-performance materials can be prepared within this temperature range.
- the Cs-containing compound of the present invention is an oxide, carbonate, hydroxide, nitrate or chloride of Cs;
- Ag-containing compounds are oxides, carbonates, hydroxides, nitrates or chlorides of Ag;
- the compound containing In is an oxide, carbonate, hydroxide, nitrate or chloride of In;
- Cr-containing compounds are oxides, carbonates, hydroxides, nitrates or chlorides of Cr;
- the Er-containing compound is an oxide, carbonate, hydroxide, nitrate or chloride of Er.
- the mass percentage concentration of hydrochloric acid is 36-38%, and the hydrochloric acid is fully stirred and dissolved at 30-100 DEG C.
- the cooling is natural cooling to room temperature.
- the drying is maintained at 50-100° C. for 1-24 hours to complete drying.
- the compound containing Ag, In, Cr and Er is the chloride of Ag, In, Cr and Er.
- Chloride can provide both cations and anions required for the reaction, which can better prepare pure phases and obtain lead-free double perovskites with enhanced Er ion photoluminescence.
- the purity of the chlorides of Ag, In, Cr and Er is ⁇ 99.9%.
- the reaction temperature is 80°C.
- the luminescent properties of the material are better at this temperature.
- the function of cleaning is to remove the remaining reaction raw materials after the reaction in the product, so as not to affect the luminescence performance of the product.
- the cleaning of the present invention can use organic solvents such as isopropanol, methanol, acetone, and ethanol.
- the cleaning is ethanol flushing.
- ethanol has a low boiling point, is volatile, has low toxicity, is low in cost, and easily dissolves residual reaction raw materials.
- the washing is 1-5 times with ethanol, in order to remove the residual reaction raw materials more thoroughly.
- the lead-free double perovskite material of the present invention has superior strong near-infrared emission properties, and can be widely used in the fields of near-infrared LEDs, low-loss optical fiber communications and germanium-based solar cell materials, and the present invention especially protects the enhanced Er ion photoinduced Luminescent lead-free double perovskites for applications in near-infrared LEDs, low-loss fiber-optic communications, and germanium-based solar cells.
- the Er ion photoconversion material of the present invention obtains an emission wavelength of 1540 nm through the energy level transition of 4 I 13/2 - 4 I 15/2 in the Er ion, which is just in the low-loss window of optical fiber communication, and the excitation spectrum is the same as that of commercial 365 nm, 535nm, 620nm LED chips are matched, so it can be widely used in the field of low-loss optical fiber communication.
- the Er 3+ ion infrared emission of this material is located at about 1540 nm, which is very matched with the forbidden band width of germanium, and the excitation spectrum of this material basically covers the entire visible light region, and can emit light that can be absorbed by germanium-based solar cells.
- the near-infrared light is a potential light conversion material to improve the efficiency of germanium-based solar cells.
- the excitation wavelength of the lead-free double perovskite in the application is 250-900 nm.
- the present invention also specifically protects a germanium-based solar cell, wherein the light conversion material of the germanium-based solar cell is the lead-free double perovskite that enhances Er ion photoluminescence.
- the Er ion photoconversion material of the present invention takes Cs 2 AgInCl 6 as the host, and the luminescent centers are trivalent Cr 3+ , Er 3+ ions, Er 3+ ions generate infrared light with a peak at 1540 nm, Cr 3+ ions As sensitizing ions, the ions enhance the near-infrared luminescence intensity of the activated ions Er 3+ ions, and the quantum efficiency can reach 22.6%, which is 60 times higher than that of single-doped materials, and has stronger near-infrared light emission.
- the Er ion photoconversion material of the present invention has a very wide excitation spectrum, has effective absorption in the range of 250-900 nm, and can effectively absorb ultraviolet light and visible light.
- the Er ion photoconversion material of the present invention has strong near-infrared light emission, and the energy is just in the low-loss window of optical fiber communication, and can be widely used in the fields of near-infrared LED, low-loss optical fiber communication and germanium-based solar cell materials .
- Example 1 is the XRD patterns of the lead-free double perovskite with enhanced Er ion photoluminescence of Example 1 and the lead-free double perovskite of Comparative Examples 1-3.
- Fig. 2 is the excitation and emission spectra of the luminescent material of Comparative Example 2;
- Example 4 is an excitation and emission spectrum diagram of the luminescent material of Example 1;
- FIG. 5 is an emission spectrum diagram of the luminescent materials of Examples 1-5 and Comparative Example 3.
- FIG. 5 is an emission spectrum diagram of the luminescent materials of Examples 1-5 and Comparative Example 3.
- FIG. 6 is the infrared emission spectra of the luminescent materials doped with Er alone in Comparative Example 3 and Cr and Er co-doped in Example 5, respectively, under the excitation of 356 nm, 580 nm, and 808 nm light.
- the raw material reagents used in the examples of the present invention are conventionally purchased raw material reagents.
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.8 Cr 0.1 Er 0.1 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.6 Cr 0.1 Er 0.3 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.4 Cr 0.1 Er 0.5 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.2 Cr 0.1 Er 0.7 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite capable of enhancing Er ion photoluminescence the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.1 Cr 0.1 Er 0.8 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite the chemical formula of the lead-free double perovskite is: Cs 2 AgInCl 6 .
- the preparation method is as follows:
- a lead-free double perovskite the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.2 Cr 0.8 Cl 6 .
- the preparation method is as follows:
- CsCl cesium chloride
- a lead-free double perovskite the chemical formula of the lead-free double perovskite is: Cs 2 AgIn 0.2 Er 0.8 Cl 6 .
- the preparation method is as follows:
- Fig. 1 is the XRD patterns of the light conversion materials of Example 1 and Comparative Example 1, Comparative Example 2, and Comparative Example 3. It can be seen that the light conversion materials of Example 1 and Comparative Example 1, Comparative Example 2, and Comparative Example 3 have The XRD pattern has a face-centered cubic structure, and the phosphor powder has high crystallinity. The high crystallinity of the material will enhance the near-infrared emission.
- Fig. 2 is the excitation and emission spectra of Comparative Example 2. It can be seen from Fig. 2 that the obtained photoconversion material has near-infrared emission at 1010 nm, and the excitation spectrum presents 250-450 nm ( 4 A 2 ⁇ 4 T 1 ( 4 P )), three broadband absorptions of Cr ions at 500-650 nm ( 4 A 2 ⁇ 4 T 1 ( 4 F)), 700-900 nm ( 4 A 2 ⁇ 4 T 2 ( 4 F)).
- Figure 3 shows the excitation and emission spectra of Comparative Example 3. It can be seen from Figure 3 that the obtained phosphor has near-infrared emission at 1540 nm, and the excitation spectrum exhibits broadband matrix absorption from 250 nm to 350 nm. , 488nm, 520nm, 544nm, 650nm excitation peaks are assigned to Er ions 4 I 15/2 ⁇ 2 G 9/2 , 4 G 11/2 , 2 H 9/2 , 2 F 5/2 , 4 F 7/ 2 , 2 H 11/2 , 4 S 3/2 , 4 F 9/2 energy level absorption.
- Fig. 4 is the excitation and emission spectra of the luminescent material of Example 1. It can be seen from Fig. 4 that the obtained phosphor has near-infrared emission at 1010 nm and 1540 nm, and the excitation spectrum presents 250-450 nm ( 4 A 2 ⁇ 4 Three broadband absorptions of Cr ions at T 1 ( 4 P)), 500-650 nm ( 4 A 2 ⁇ 4 T 1 ( 4 F)), 700-900 nm ( 4 A 2 ⁇ 4 T 2 ( 4 F)).
- the quantum efficiency of the lead-free double perovskite with enhanced Er ion photoluminescence of Example 5 was measured by using the absolute photoluminescence quantum efficiency test system (Hamamatsu Photoelectric Co., Ltd., Quantaurus-QY Plus C13534-12), and the results showed that The quantum efficiency can reach 22.6%, which is about 60 times higher than that of single-doped materials.
- Example 1 achieves the following technical effects: with the addition of Cr element, the luminescent material is Under the excitation of different wavelengths, the 1540nm near-infrared light emission intensity of Er ions is greatly improved.
- the measurement method of near-infrared light emission intensity is as follows:
- Example 6 is the infrared emission spectra of the luminescent material doped with Er alone and the Cr and Er co-doped light-emitting materials of Example 5 under the excitation of 356 nm, 580 nm, and 808 nm, respectively, and Table 2 is the enhanced Er ions of Example 5
- Table 2 is the enhanced Er ions of Example 5
- the emission intensities of the photoluminescent lead-free double perovskite and the lead-free double perovskite of Comparative Example 3 it can be seen that under different excitation wavelengths, the lead-free double calcium enhanced Er ion photoluminescence of the present invention Titanites have remarkable strong Er ion photoluminescence effect.
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Abstract
Description
| 序号 | 发射强度 |
| 实施例1 | 14952.71 |
| 实施例2 | 26741.17 |
| 实施例3 | 44384.92 |
| 实施例4 | 59843.64 |
| 实施例5 | 54634.66 |
| 对比例1 | 18.63 |
| 对比例2 | 108.44 |
| 对比例3 | 1779.44 |
| 激发波长 | 实施例5发射强度 | 对比例3发射强度 |
| 356nm | 75032.71 | 1779.43 |
| 580nm | 22562.95 | 19.439 |
| 808nm | 26829.26 | 20.282 |
Claims (10)
- 一种增强Er离子光致发光的无铅双钙钛矿,其特征在于,所述无铅双钙钛矿的化学式为:Cs 2AgIn 1-x-yCr xEr yCl 6,0.00<x≤1.00,0.00<y≤1.00。
- 如权利要求1所述增强Er离子光致发光的无铅双钙钛矿,其特征在于,所述无铅双钙钛矿的化学式为:Cs 2AgIn 1-x-yCr xEr yCl 6,0.1≤x≤0.8,0.1≤y≤0.8。
- 一种权利要求1或2所述增强Er离子光致发光的无铅双钙钛矿的制备方法,其特征在于,包括如下步骤:将含Ag、In、Cr、Er的化合物混合,加入盐酸,搅拌溶解,再加入含Cs的化合物引发沉淀反应,反应温度30~100℃,反应完全,冷却、分离、清洗,干燥得到无铅双钙钛矿。
- 如权利要求3所述增强Er离子光致发光的无铅双钙钛矿的制备方法,其特征在于,所述含Ag、In、Cr、Er的化合物为Ag、In、Cr、Er的氯化物。
- 如权利要求4所述增强Er离子光致发光的无铅双钙钛矿的制备方法,其特征在于,所述Ag、In、Cr、Er的氯化物的纯度≥99.9%。
- 如权利要求3所述增强Er离子光致发光的无铅双钙钛矿的制备方法,其特征在于,所述反应温度为80℃。
- 如权利要求3所述增强Er离子光致发光的无铅双钙钛矿的制备方法,其特征在于,所述清洗为乙醇冲洗。
- 一种权利要求1或2所述增强Er离子光致发光的无铅双钙钛矿在近红外LED、低损耗光纤通信和锗基太阳能电池领域中的应用。
- 如权利要求8所述应用,其特征在于,所述应用中无铅双钙钛矿的激发波长为250~900nm。
- 一种锗基太阳能电池,其特征在于,所述锗基太阳能电池的光转换材料为权利要求1或2所述增强Er离子光致发光的无铅双钙钛矿。
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| CN117586768A (zh) * | 2023-11-22 | 2024-02-23 | 昆明理工大学 | 一种Cs2LiInCl6无铅双钙钛矿材料及其制备 |
| CN121759211A (zh) * | 2026-03-03 | 2026-03-31 | 德州学院 | 一种双钙钛矿基发光材料及其制备方法与其在发光成像或防伪中的应用 |
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| CN116694323B (zh) * | 2023-04-25 | 2024-06-18 | 广西科学院 | 一种无铅双钙钛矿黄光荧光粉及其制备方法和应用 |
| CN117186892A (zh) * | 2023-08-09 | 2023-12-08 | 西北大学 | 一类Cr3+掺杂的稀土基双钙钛矿基荧光粉及其应用 |
| CN117089343A (zh) * | 2023-08-25 | 2023-11-21 | 昆明理工大学 | 一种近红外发光的铟基双钙钛矿制备方法 |
| CN117925228A (zh) * | 2024-01-16 | 2024-04-26 | 广西大学 | 一种超宽带近红外发光无铅双钙钛矿材料及其制备方法和应用 |
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Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN117586768A (zh) * | 2023-11-22 | 2024-02-23 | 昆明理工大学 | 一种Cs2LiInCl6无铅双钙钛矿材料及其制备 |
| CN121759211A (zh) * | 2026-03-03 | 2026-03-31 | 德州学院 | 一种双钙钛矿基发光材料及其制备方法与其在发光成像或防伪中的应用 |
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| CN113372905A (zh) | 2021-09-10 |
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