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南昌大学材料科学研究所, 江西, 南昌, 330047
纸质出版日期:2000-5-30,
收稿日期:1999-9-23,
修回日期:2000-12-16,
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江风益, 李述体, 王立, 熊传兵, 彭学新, 辛勇, 姚冬敏. MOCVD生长GaN:Si单晶膜的研究[J]. 发光学报, 2000,21(2): 120-124
JIANG Feng-yi, LI Shu-ti, WANG Li, XIONG Chuan-bing, PENG Xue-xin, XIN Yong, YAO Dong-min. GaN:Si Single Crystal Films Grown on Sapphire Substrates by MOCVD[J]. Chinese Journal of Luminescence, 2000,21(2): 120-124
江风益, 李述体, 王立, 熊传兵, 彭学新, 辛勇, 姚冬敏. MOCVD生长GaN:Si单晶膜的研究[J]. 发光学报, 2000,21(2): 120-124 DOI:
JIANG Feng-yi, LI Shu-ti, WANG Li, XIONG Chuan-bing, PENG Xue-xin, XIN Yong, YAO Dong-min. GaN:Si Single Crystal Films Grown on Sapphire Substrates by MOCVD[J]. Chinese Journal of Luminescence, 2000,21(2): 120-124 DOI:
获得高质量的n型GaN单晶膜是制作GaN基光电子器件的关键之一。采用立式MOCVD系统生长GaN:Si单晶膜
通过优化生长工艺
获得了电子载流子浓度高达210
19
cm
-3
迁移率达120cm
2
/V.s的n型GaN:Si单晶膜;并有效地抑制了GaN中由深能级引起的黄带发射
大大提高带边发光强度。研究结果还表明:随着Si掺杂量的增大
GaN:Si单晶膜的电子载流子浓度增加
迁移率下降
X光双晶衍射峰半高宽增大。首次报道了随掺Si量增大
GaN:Si单晶膜的生长速率显著下降的现象。
Si-doped GaN was grown by MOCVD method using a home-made vertical reactor operating at atmospheric pressure.To prevent parasitic reactions in the gas phase
reagents were mixed at 20mm before reaching the substrate.The growth was carried out on(0001)oriented sapphire substrates using Trimethylgallium(TMGa)and blue-ammonia(NH
3
)as Ga and N sources
respectively.The doping reagents was the diluted silane(SiH
4
).The mixed gases of hydrogen and nitrogen were used as the carrier gases.A thin buffer layer with thickness of about 15um was grown at 520℃ and recrystallized at 1060℃ for 6 minutes.The Sidoped GaN films were grown at 1060℃with the [V]/[Ⅲ]
ratio of 1000: 1 The growth time was an hour with the growth rate in the rage of 1.8-4.0um/h.The photoluminescence(PL)
the Van der Pauw Hall method
and the double-crystal X-ray diffraction(DXRD)were used to measure the optical
electrical
and structural data of these films at room temperature.Table 1 is the characterization data of the Si-doped GaN films.Fig.1 shows the electron carrier concentration and mobility of Si-doped GaN as a function of SiH
4
/TMGa ratio.The carrier concentration varies between 110
17
and 410
19
cm
-3
.The relationship between the carrier concentration and the flow rate ratio of SiH
4
/TMGa is approximately linear.Fig.2 shows the photoluminescence(PL)spectra of Si-doped GaN as a function of the SiH
4
/TMGa ratio at 300K.The excitation-source was a 15mW He-Cd laser.The band-edge emission and deep-level emission were observed around 370um and 550um
respectively.Very strong band-edge emission without yellow band(limited by the apparatus)was observed in Fig.2-D.Fig.3 shows the intensity of band-edge emission
the intensity ratio between band-edge emission and deep-level emission as a function of the carrier concentration of Si-doped GaN films.The intensity of bandedge emission was highly enhanced and the intensity of yellow emission was restrained with the increasing ofcarrier concentration.As shown in Fig.3
Si-doped GaN films
with carrier concentration of 210
19
cm
-3
were obtained.For this kind of film
the intensity of band edge emission is as high as one hundred times of that of unintentional doped GaN and no yellow luminescence can be found.Fig.4 shows the relationships between the SiH
4
/TMGa ratio and the FWHM of double-crystal x-ray diffraction(DXRD)and the growth rate of Si-doped GaN films.The FWHM of DXRD of GaN films became wider when SiH
4
/TMGa ratio increased.However
the growth rate decreased from 4um/h to 1.7um/h with increasing SiH
4
/TMGa ratio.This phenomenon has not been reported to our knowledge.In this paper
Si-doped GaN films with carrier concentration of 210
19
cm
-3
electron mobility of 120.m
2
/V.s can be obtained.FOr this kind of film
FWHM of the band edge emission at room temperature is only 60meV
and no yellow emission can be observed.In this work
the optimum flow ratio of SiH
4
/TMGa was 210
-4
.
MOCVDGaN光致发光X射线双晶衍射Hall测量
MOCVDGaNphotoluminescencethe double-crystal X-ray diffraction(DXRD)the Van der Pauw Hall method
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