中国科学院机构知识库网格
Chinese Academy of Sciences Institutional Repositories Grid
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浏览/检索结果: 共11条,第1-10条 帮助

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Electrically pumped organic laser device with a coupled microcavity structure (EI CONFERENCE) 会议论文  OAI收割
Organic Light Emitting Materials and Devices XVI, August 12, 2012 - August 15, 2012, San Diego, CA, United states
作者:  
Li Y.;  Li Y.;  Li Y.;  Li Y.;  Lin J.
收藏  |  浏览/下载:21/0  |  提交时间:2013/03/25
The optical gain and radiative current density of GaInNAs/GaAs/AlGaAs separate confinement heterostructure quantum well lasers 期刊论文  OAI收割
Journal of Applied Physics, 2010, 卷号: 107, 期号: 1
S. D. Wu, Y. G. Cao, S. Tomic and F. Ishikawa
收藏  |  浏览/下载:20/0  |  提交时间:2012/11/02
Metamorphic InGaAs Quantum Well Laser Diodes at 1.5 mu on GaAs Grown by Molecular Beam Epitaxy 期刊论文  OAI收割
chinese physics letters, 2009, 卷号: 26, 期号: 1, 页码: art. no. 014214
Wang HL; Wu DH; Wu BP; Ni HQ; Huang SS; Xiong YH; Wang PF; Han Q; Niu ZC; Tangring I; Wang SM
收藏  |  浏览/下载:183/53  |  提交时间:2010/03/08
1310 nm GaInNAs triple quantum well laser with 13 GHz modulation bandwidth 期刊论文  OAI收割
electronics letters, 2009, 卷号: 45, 期号: 7, 页码: 356-u23
Zhao H; Haglund A; Westburgh P; Wang SM; Gustavsson JS; Sadeghi M; Larsson A
收藏  |  浏览/下载:91/31  |  提交时间:2010/03/08
A novel bottom-emitting vcsel's one-dimension array (EI CONFERENCE) 会议论文  OAI收割
Optoelectronic Materials and Devices III, October 27, 2008 - October 30, 2008, Hangzhou, China
作者:  
Wang L.;  Wang L.;  Wang L.;  Liu Y.;  Liu Y.
收藏  |  浏览/下载:23/0  |  提交时间:2013/03/25
A novel 980nm bottom-emitting VCSELs array with high power density and good beam property of Gaussian far-field distribution is reported. This array is composed of 5 symmetrically-arranged elements of 200m  150m and 100m-diameter  with the center spacings of 300m and 250m respectively. The maximum power is 880mW at a current of 4A  corresponding to lKW/cm2 average optical power density. The differential resistance is 0.09 with a threshold of 0.56A. The novel array is compared with a 300m-aperture-size single device and a 44 2-D array with 50m element aperture size and 250m centre spacing. The three devices have the same lasing area. The conclusion is that the novel array is better in the property of output power  threshold current  lasing spectra  far-field distribution etc. 2008 SPIE.  
A 1.5 mu m n-type InGaAsP/InGaAsP modulation-doped multiple quantum well DFB laser by MOCVD 期刊论文  OAI收割
semiconductor science and technology, 2006, 卷号: 21, 期号: 3, 页码: 306-310
Zhang RY; Wang W; Zhou F; Wang BJ; Wang LF; Bian J; Zhao LJ; Zhu HL; Jian SS
收藏  |  浏览/下载:58/0  |  提交时间:2010/04/11
Fabrication and electron emission of carbon microtubes (EI CONFERENCE) 会议论文  OAI收割
Technical Digest of the 18th International Vacuum Nanoelectronics Conference, IVNC 2005, July 10, 2005 - July 14, 2005, Oxford, United kingdom
作者:  
Liu L.;  Liu L.;  Wang W.;  Wang W.
收藏  |  浏览/下载:38/0  |  提交时间:2013/03/25
Carbon nanotubes have been attracting attention because of their unique physical properties and their application potential for field emission cathode. Carbon nanotubes possess the following properties favorable for field emission material  such as a high aspect ratio and sharp tip  high chemical stability  high mechanical strength  stable at high temperature. Some research works on carbon nanotubes field emitter and field emission display have been reported. Here  a kind of carbon microtubes and its field emission properties are introduced. They have some different properties with carbon nanotubes  and the density is lower than carbon nanotubes bundles. These carbon microtubes are directly synthesized by liquidoid epitaxy method on silicon substrates at low temperature. The field emission properties of carbon microtubes are reported too. Carbon microtubes film is synthesized in liquid by electrolysis. The graphite plate is as anode  and n-silicon substrate with resistivity of 4-8 cm is as cathode. The electrolysis current is about 5-8mA/cm2  and applied voltage is 800-1500V. Temperatures of the methanol base solution is maintained at 60C in process of deposition of carbon microtubes. Carbon microtubes film is observed by scanning electron microscopy(SEM)  as shown in fig.1(a  b). The wall's thickness of carbon microtube is about 60nm. The diameter of carbon microtube is about 0.8 m. Raman spectrum of carbon microtubes film shows the two peaks at 1342and 1560cm-1. The field emission properties of carbon microtubes are measured in high vacuum chamber(10-5Pa). The emission area of carbon microtubes is 0.5cm 0.5cm. The threshold of field emission of the carbon microtubes film is about 3.6V/ m. Field emission property of carbon microtubes film is shown in fig.2. Another  when the electric field between anode and cathode is 10V/ m  the electric field distribution on single carbon microtube is also given after calculation according to electric field theory. Fig 3 shows that electric field distribution vertical section on the of single carbon microtube top with 2 m of highness. These results may help us to understand field emission properties of carbon microtubes. According to research results  it is found that liquidoid synthesis is simple method to produce carbon microtubes cold cathode material  and the carbon microtubes have better field emission properties. 2005 IEEE.  
High-power InGaAs/GaAs VCSEL's two-dimension arrays (EI CONFERENCE) 会议论文  OAI收割
ICO20: Lasers and Laser Technologies, August 21, 2005 - August 26, 2005, Changchun, China
作者:  
Liu Y.;  Wang L.-J.;  Wang L.-J.;  Liu Y.;  Liu Y.
收藏  |  浏览/下载:26/0  |  提交时间:2013/03/25
Selectively oxidized InGaAs/GaAs vertical -cavity surface-emitting lasers (VCSEL) array at an emission wavelength of 980nm was reported. A 16 elements array with 200m aperture size (250m center spacing) of individual elements shows a CW output power of 1.21 W at room temperature  resulting in 1 KW/cm2 average optical power density. The device threshold current is 1.32A The lasing peak wavelength is 981.9 nm  the full width at half-maximum is 0.7 nm  and the far-field divergence angle is about 17.The characteristics of a single device with a active region diameter of 800m is compared with that of a 2-D array with active region diameter of individual clement of 200m. These two kinds of devices have the same total lasing area. At the same current injection  the single device has a higher threshold and a higher output power than the array. The red shift of single device is more obvious than that of the array's.  
High-power InGaAs VCSEL's single devices and 2-D arrays (EI CONFERENCE) 会议论文  OAI收割
Optoelectronic Materials and Devices for Optical Communications, November 7, 2005 - November 10, 2005, Shanghai, China
作者:  
Sun Y.;  Wang L.;  Wang L.;  Wang L.;  Liu Y.
收藏  |  浏览/下载:21/0  |  提交时间:2013/03/25
Low threshold current density 1.5 mu m strained-mqw laser by n-type modulation-doping 期刊论文  iSwitch采集
Pricm 5: the fifth pacific rim international conference on advanced materials and processing, pts 1-5, 2005, 卷号: 475-479, 页码: 1663-1667
作者:  
Zhang, RY;  Wang, W;  Zhou, F;  Bian, J;  Zhao, LJ
收藏  |  浏览/下载:25/0  |  提交时间:2019/05/12