999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

紅色熒光粉CePO4-6LaPO4@4SiO2∶Eu3+的發光特性

2019-09-09 08:08:42王喜貴
無機化學學報 2019年9期
關鍵詞:化學科學

劉 茹 王喜貴

(內蒙古師范大學化學與環境科學學院,呼和浩特 010022)

0 Introduction

In recent years,much attention has been paid to rare earth doped various phosphors,because it has the advantages of long-term stability,long lifetime and higher luminescent efficiency,etc.And it has been studied extensively for their potential applications in light emitting devices,displays,solid state lasers,optical amplifiers,sensors and optoelectronics devices,etc[1-2].Managing the red,green and blue light to get warm white light that makes our eyes feel comfortable.The use of red phosphor has more or less defects in recent years,which directly affects the quality of white luminescence.Therefore,the investigation of red phosphor has an important theoretical significance and practical application value[3-5].

In general,phosphors are composed of luminescent center and matrix materials.The rare earth Eu3+shows red light under excitation with UV light and visible light and is an ideal red luminescence center.It is well known that due to the f-f forbidden transition of rare earth ions.The absorption efficiency is low,so it is necessary to find some methods to enhance the absorption efficiency.The method commonly used to enhance the absorption efficiency is to dope rare earth ions as an activator to select a suitable matrix.The energy absorbs from the matrix effectively transmits to the activation center(rare earth ion)to improve the luminescent efficiency.This shows that the choice of matrix is crucial.Phosphates have the advantages of charge stabilization,excellent thermal stability,high chemical stability and other excellent properties.So the phosphates have become an important matrix material.Meanwhile,the silicon dioxide have the advantages of good chemical stability,mechanical properties and low expansion coefficient.So it also becomes an excellent matrix material.But the reports about CePO4,LaPO4or SiO2as single matrix are very common[3,6-10],the reports about CePO4,LaPO4and SiO2as composite matrix are unusual.In the paper,a novel red phosphor CePO4-6LaPO4@4SiO2∶Eu3+was successfully synthesized by sol gel method and high temperature solid state method.The structure and luminescence properties of CePO4-6LaPO4@4SiO2∶Eu3+phosphors also were investigated.

1 Experimental

1.1 Synthesis of samples

Firstly,the raw solution listed in Table 1 were added to clean beaker,which were stirred for 3 min.Then NH3·H2O was added to adjust pH value to 9 and kept stirring about 2 h to get a homogeneous sol.Secondly,the sol was transferred to a dry culture dish.After 2 days,it became a gel at room temperature.Next the samples were annealed at 900℃for 17 hours.Finally,the samples were obtained.

Table 1 Experiment proportion of CePO4-6LaPO4@x SiO2∶Eu3+

1.2 Chemicals

NH3·H2O purchased from Tianjin Guangfu Fine Chemical Research Institute (98.0%),which was dissolved in distilled water to obtain La(NO3)3solution.Eu2O3was purchased from Baotou Rare Earth Institute(99.99%),which was dissolved in HCl solution to obtain EuCl3(0.16 mol·L-1).H3PO4was purchased from Tianjin Chemical Reagent Third Factory(85.0%).NH3·H2O was purchased from Tianjin Sailboat Chemical Reagent Technology Co.,Ltd.(25%~28%).CH3COOH was purchased from Tianjin Beilian Fine Chemicals Development Co.,Ltd(99.7%).

1.3 Characterization

The X-ray diffraction (XRD)pattern of powder samples were measured on a Rigaku-Dmax 2500 X diffractometer equipped with Cu Kα radiation (λ =0.154 05 nm,U=40 kV,I=30 mA,2θ=10°~80°);A 200 keV JEOL 2010 (HRTEM)micros-cope was used to record Transmission Electron Micros-copy (TEM)images;IR spectra was acquired with using a Hitachi U-4100 UV-VIS-NIR spectrometer with the KBr pellet technique;The excitation and emission spectra were measured with using a F-4500 spectrophotometer equipped with a 150 W xenon lamp as the excitation source.

2 Results and discussion

2.1 XRD study

XRD patterns of CePO4-6LaPO4∶Eu3+and CePO4-6LaPO4@4SiO2∶Eu3+phosphors were reported in Fig.1.For SiO2particles,no diffraction peak was observed,excepted for a very small broad peak at 2θ=22°,characteristic of amorphous silica[11-12].In addition,all the diffraction peaks of CePO4-6LaPO4@4SiO2∶Eu3+phosphor were agreed with the standard card(PDF No.32-0199 and No.46-1326).The indicated that a low amount of SiO2almost did not affect the crystal structure of phosphate.The above results showed that the sample was made up of crystalline state CePO4,LaPO4and amorphous state SiO2.Note that the intensity diffraction peaks of CePO4-6LaPO4@4SiO2∶Eu3+phosphor were a little improved than those of CePO4-6LaPO4∶Eu3+phosphor,suggesting that the size of the crystalline grains of phosphate on the surfaces of the silica particles in the composite was smaller than that in the pure phosphate.At the same time,no impurity peak from the third phase was detected,which indicated Eu3+entered lattice in the matrix and occupied the site of La3+and Ce3+in the matrix to form a stable solid solution without affecting the structure of host lattice.

According to previous reports[10,12],to form a new solid solution,the radius in the percentage difference(Dr)between the doped ions and the possibly substituted ion should be less than 15%,see the following formula:

Fig.1 XRD patterns of CePO4-6LaPO4∶Eu3+and CePO4-6LaPO4@4SiO2∶Eu3+

Where R1(CN)is the radius of the matrix cation and R2(CN)is the radius of the doped ions.Herein,the values of R1(CN)(Ce3+and La3+)and R2(CN)(Eu3+)are respectively 0.103,0.106 and 0.095.According to this formula,the Drvalue respectively was 7.8% and 10.4%,and less than 15%,further confirmed that the Eu3+occupied the site of the La3+and Ce3+in the matrix to form a stable solid solution without affecting the structure of the CePO4and LaPO4host lattice.

2.2 TEM stu dy

TEM image of CePO4-6LaPO4@4SiO2∶Eu3+phosphor was reported in Fig.2(a).It showed that the grain morphology was irregular shape.The grain size was measured by Nano Measure App and was 0.38 μm.According to the XRD data,the grain size was calculated by Scherrer Formula and was 0.31μm.Both results were consistent.

Fig.2(b)showed TEM image of CePO4-6LaPO4@4SiO2∶Eu3+phosphor,CePO4-6LaPO4@4SiO2∶Eu3+phosphor was further sub-jected to TEM analysis to determine the core-shell structure.The core-shell structure of the sample could be seen clearly due to the different electron penetrability of the core and shell.The core could be seen as a black irregular sphere and the shells had a gray color.

Fig.2 TEM images(a,b)and HRTEM image(c)of CePO4-6LaPO4@4SiO2∶Eu3+phosphor

The HRTEM image of CePO4-6LaPO4@4SiO2∶Eu3+phosphor was reported in Fig.2(c).It clearly showed the CePO4-6LaPO4@4SiO2lattice and lattice fringes with an inter-planar spacing of 0.191 18,0.215 28 and 0.312 30 nm,which had good match with those of the standard pattern of PDF card (LaPO4/CePO4),i.e.,spacing for(231)0.191 18 nm,(311)0.215 28 nm and(120)0.312 30 nm.

2.3 EDS study

The EDS spectrum of CePO4-6LaPO4@4SiO2∶Eu3+phosphor was reported in Fig.3.The elements of O,Si,P,La,Ce and Eu were observed in the spectrum,and the ratio of La,Ce and Si elements was 6∶1∶4,which clearly indicated the formation of CePO4-6LaPO4@4SiO2∶Eu3+phosphor.

Fig.3 EDS energy spectrum of the CePO4-6LaPO4@4SiO2∶Eu3+phosphor

2.4 IR study

IR spectra of CePO4-6LaPO4∶Eu3+and CePO4-6LaPO4@4SiO2∶Eu3+phosphor were reported in Fig.4.The absorption bands from 1 600 cm-1to 400 cm-1were observed,which had different infrared absorption peaks.In the spectra of CePO4-6LaPO4as the matrix,the three peaks at 1 089,1 063 and 1 016 cm-1were obtained by cleaving at 992 cm-1and corresponded the asymmetric stretching vibration peak of P-O,which was the characteristic of monoclinic phosphates[17].In the spectra of CePO4-6LaPO4@4SiO2as the matrix,the absorption peaks at 1 107 cm-1belonged to antistretching vibration peak of Si-O-Si.The absorption peaks located at 992,952 cm-1were observed in the region of the stretching vibration of PO43-group.The absorption peak at 797 cm-1was stretching vibration peak of Si-O-Si.The band located at 621 cm-1was observed in the region of O=P-O bending vibrations(it compared with the CePO4-6LaPO4as the matrix,the peak position occurred blue shift).The bands at 575,559 and 537 cm-1were the bending vibrations of O-PO[13-14](it compared with CePO4-6LaPO4as the matrix,the peak at 537 cm-1occurred red shift).The absorption peak at 466 cm-1was bending vibration peak of Si-OSi(it compared with CePO4-6LaPO4as matrix,the peak position occurred red shift).According to the above analysis,it showed that the sample was made up of phosphate and silicon dioxide,which was consistent with the result of XRD study.

Fig.4 IR spectra of CePO4-6LaPO4@4SiO2∶Eu3+phosphor

The polarization of Eu3+was bigger than La3+/Ce3+,Eu3+replaced La3+/Ce3+,which caused a slight change in the shape of PO43-electron cloud.So the infrared vibration peak of PO43-caused red shift and blue shift in different degrees.

2.5 Luminescence study

2.5.1 Excitation and emission spectrum of CePO4-6LaPO4@x SiO2∶Eu3+

The excitation spectra of core-shell structure CePO4-6LaPO4@x SiO2∶Eu3+were reported in Fig.5.The excitation spectrum consisted of two sharp peaks at 395 and 466 nm,and the peaks corresponded to the transitions from7F0to5L6(395 nm)and5D2(466 nm).The emission intensity was strongest at 466 nm,so 466 nm was selected as the optimum excitation wavelength.

Fig.5 Excitation spectra of CePO4-6LaPO4@x SiO2∶Eu3+

The emission spectra of core-shell structure CePO4-6LaPO4@x SiO2∶Eu3+phosphor were reported in Fig.6.The emission peaks of 588 and 615 nm corresponded to the transitions from5D0to7F1and7F2,respectively.The core shell CePO4-6LaPO4@x SiO2∶Eu3+had a luminous intensity that increased first and then decreased with the increased of SiO2in the matrix,and there is an optimal core-shell ratio.The shell thickness was measured by the molar ratio of core to the element contained in the shell[18],when the core shell ratio was 1∶4,the sample had the brightest red light at 615 nm.Because a large amount of Eu3+was surrounded by SiO2and even diffuses into the SiO2network structure,greatly reducing the possibility of Eu3+being in the surface state.That is to say,the appearance of the core-shell structure increased the distance between Eu3+and the surface,thus changing the surrounding matrix environment of Eu3+near the original surface(from unevenness to relatively uniform),which hindered the energy transfer of the original Eu3+and surface states,so that improved luminous intensity of the sample.When the core shell ratio was more than 1∶4,the luminescence intensity gradually decreased.As the thickness of the shell continued to increase,the thicker shell provided a uniform matrix environment.But the loss of light through the more,which led to the excitation light could be finally utilized became less,so that causing the emitted light to weaken.The above results indicated that the optimum ratio of phosphate to SiO2was 1∶4.

Fig.6 Emission spectra of CePO4-6LaPO4@x SiO2∶Eu3+

2.5.2 Luminescence study of CePO4-6LaPO4@4SiO2∶Eu3+and CePO4-6LaPO4∶Eu3+phosphors

The emission spectra of CePO4-6LaPO4@4SiO2∶Eu3+were reported in Fig.7.Before the addition of SiO2,the main peak of CePO4-6LaPO4∶Eu3+phosphor was located at 588 nm.After the addition of SiO2,the main peak of CePO4-6LaPO4@4SiO2∶Eu3+phosphor was located at 615 nm.The showed that the addition of SiO2effectively increased red light intensity of the sample.

The sample emitted orange light and red light,which was closely related to the crystallographic position of Eu3+[15-16]. The transition5D0→7F1was dominant when Eu3+occupied the lattice site with inversion center,and the sample emitted orange light(the main peak was located at 588 nm).The transition5D0→7F2was dominant when Eu3+occupied the lattice site without inversion center,and the sample emitted red light(the main peak was located at 615 nm).In the experiment,the Eu3+of CePO4-6LaPO4∶Eu3+phosphor occupied the lattice site with inversion center,so the sample emitted orange light;the Eu3+of CePO4-6LaPO4@4SiO2∶Eu3+phosphor occupied the lattice site without inversion center,so the sample emitted red light.It as shown as Fig.8.The intensity pattern of the emission lines demonstrate that the Eu3+was successfully doped in the sample.In addition,the formation of core-shell structure was also beneficial to red luminescence[18-19].

Fig.7 Emission spectra of CePO4-6LaPO4∶Eu3+and CePO4-6LaPO4@4SiO2∶Eu3+

Fig.8 Energy level diagram

3 Conclusions

The CePO4-6LaPO4@x SiO2∶Eu3+red phosphors were synthesized by sol gel method and high temperature solid statue method.The results showed that the optimal excitation wavelength of the phosphor was 466 nm and the optimum ratio of phosphate to SiO2was 1∶4.And the appearance of core-shell structure CePO4-6LaPO4@4SiO2was more conducive to the doping of Eu3+and improved the red light of the sample.It indicated that CePO4-6LaPO4@4SiO2∶Eu3+could be a good candidate as red phosphor or it combined with blue and green phosphor to get ideal quality warm WLED.

猜你喜歡
化學科學
點擊科學
點擊科學
科學大爆炸
小小藝術家(2019年6期)2019-06-24 17:39:44
奇妙的化學
奇妙的化學
奇妙的化學
奇妙的化學
奇妙的化學
科學
科學拔牙
主站蜘蛛池模板: 欧洲亚洲一区| 日韩欧美成人高清在线观看| 1024你懂的国产精品| 免费国产高清视频| 久久久久夜色精品波多野结衣| 欧美激情视频一区二区三区免费| 亚洲无限乱码| 激情乱人伦| 99热这里只有精品在线播放| 99ri国产在线| 国产亚洲欧美在线人成aaaa| 69av免费视频| 亚洲欧美成aⅴ人在线观看| 国产91丝袜| 婷婷五月在线| 国产真实乱子伦视频播放| 国产高清免费午夜在线视频| 国产精品亚洲а∨天堂免下载| 久久不卡精品| 亚洲an第二区国产精品| 国产精品视频观看裸模| 国产精品偷伦在线观看| 精品国产一二三区| 特黄日韩免费一区二区三区| 国产一区免费在线观看| 高清无码手机在线观看| 亚洲综合亚洲国产尤物| 成人永久免费A∨一级在线播放| 中文字幕在线永久在线视频2020| 91福利免费视频| 99re在线免费视频| 国产美女自慰在线观看| 中文字幕在线永久在线视频2020| 欧美笫一页| 亚洲最大看欧美片网站地址| 四虎永久在线视频| 五月天久久婷婷| 伊伊人成亚洲综合人网7777| 制服丝袜一区二区三区在线| 日韩欧美国产另类| 91在线日韩在线播放| 国产福利拍拍拍| 午夜a视频| 日韩精品一区二区三区免费| 国产精品无码作爱| 久久精品人人做人人综合试看 | 久久国产精品国产自线拍| 国产激情第一页| 极品国产在线| 亚洲视频免费在线看| 中文字幕乱码中文乱码51精品| 国产在线视频自拍| 亚洲色图欧美在线| 亚洲一级色| 亚洲区欧美区| 亚洲人在线| 精品国产欧美精品v| 伊人久久福利中文字幕| 国产毛片久久国产| 日韩一区二区三免费高清| 91丝袜在线观看| 亚洲成肉网| 香蕉国产精品视频| 91小视频在线观看免费版高清| 91亚洲精品国产自在现线| 国产精品亚洲一区二区三区在线观看| 一本大道香蕉久中文在线播放| 国产在线日本| 激情综合网址| 国模私拍一区二区三区| 91原创视频在线| 91成人在线观看| 久久精品国产精品一区二区| 日本亚洲国产一区二区三区| 天堂av高清一区二区三区| 经典三级久久| 久久人体视频| 亚洲伦理一区二区| 成人精品区| 婷婷亚洲视频| 日韩一级毛一欧美一国产| 成·人免费午夜无码视频在线观看 |