Xiaofeng Sai
Chinese Academy of Sciences
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Publication
Featured researches published by Xiaofeng Sai.
Photonics and Optoelectronics Meetings (POEM) 2011: Optoelectronic Sensing and Imaging | 2011
Qiurong Yan; Baosheng Zhao; Hao Yang; Yongan Liu; Lizhi Sheng; Yonglin Wei; Xiaofeng Sai
The Long Slit Spectrograph is one of instruments onboard The World Space Observatory-Ultraviolet. Both the FUV (102-1700nm) and NUV (160-320nm) channels of LSS choose micro-channel plates (MCP) detector with anode readout in the focal plane. The MCP detectors with anode readout are typically used to provide photon counting imaging. According to the desired performance of LSS, the Vernier anode may be the optimum readout scheme. The Vernier anode is famous for its high spatial resolution, however, the original decode algorithms of the Vernier anode is susceptible to wrongly decode, when the charge acquisition is not precise enough and the footprint size of charge cloud collected by Vernier anode is not small enough and eventually results in the deterioration of photon counting image. In this paper, the causes leading to image deterioration is analyzed. The least-squares method was used to calculate the phase value to correct imaging distortions caused by charge measurement accuracy. The area ratio of each electrode covered by charge cloud is accurately calculated to improving the imaging results. The corrected algorithms are verified by experimental results and the results show that the correction methods can obviously improve the quality of the original photon counting image.
International Symposium on Photoelectronic Detection and Imaging 2011: Space Exploration Technologies and Applications | 2011
Yongan Liu; Baosheng Zhao; Yonglin Wei; Xiaofeng Sai; Qiurong Yan; Lizhi Sheng
In the World Space Observatory-Ultraviolet (WSO-UV) mission, the Long Slit Spectrograph (LSS) instrument will provide low resolution spectra in the range 102-320nm. Both the NUV (160-320nm) and the FUV (102-170nm) channels of LSS use microchannel plates (MCP) working in photon-counting modes as detectors. In this paper, the progress and parameters of NUV and FUV photon-counting imaging detectors were described. For the NUV detector, we developed the detector based on a sealed MCP-image intensifier which comprises input window, photocathode, MCP stack, Ge-layer and its ceramic substrate. To maximize the quantum efficiency, we adopted a Caesium Telluride (Cs2Te) photocathode, which was deposited on input window and mounted close to the MCP. For the FUV detector, because of the lower cut-off wavelength, there are no suitable window materials in this band and the open-faced design should be used to meet the requirements of the detection. Therefore, a Caesium Iodide (CsI) photocathode deposited on the input surface of the MCP was used to optimize detector efficiency. By using an existing wedge and strip anode (WSA), the imaging performance of the NUV and FUV detectors was tested respectively. Experimental results show that the quantum efficiency of Cs2Te is 12.1% (at 230nm), the spatial resolution of NUV and FUV detectors is better than 110μm, the dark count rate of NUV and FUV detectors is about 10.5- and 2.3-counts/s*cm2 respectively.
Chinese Optics Letters | 2010
Feifei Zhao; Baosheng Zhao; Xiaofeng Sai; Xinghua Zhang; Yonglin Wei; Wei Zou
Compared with the traditional image intensifier with phosphor screen readout, the photon-counting imaging detector with charge induction readout is more beneficial in several aspects (e.g., good imaging properties and time resolution) to astronomy, reconnaissance, bioluminescence, and materials research. However, the annealing temperature during the tube-making process can affect the properties of the Ge film, and consequently impair the performance of the detector. Therefore, the influence of annealing temperature on Ge film and on the detector is studied in order to determine the crucial parameters. The Ge films are prepared on ceramic and quartz glass by the use of an electron gun. They are analyzed by scanning electron microscope (SEM), high-resistance meter, and X-ray diffraction (XRD). The results show that the optimum substrate and annealing temperature are ceramic plate and 250 ?, respectively.
Archive | 2011
Ding Chen; H. M. Hu; Xiaofeng Sai; Lizhi Sheng; Baosheng Zhao
Archive | 2012
Lizhi Sheng; Baosheng Zhao; Feng Zhou; Yongan Liu; Qiurong Yan; Xiaofeng Sai; Yonglin Wei
Archive | 2009
Xiaofeng Sai; Baosheng Zhao; Jinshou Tian; Junfeng Wang; Wei Zou
Archive | 2007
Xiaofeng Sai; Baosheng Zhao; Xibin Cao; Junfeng Wang; Yonglin Wei; Wei Zou; Gaiyun Dong
Archive | 2012
Baosheng Zhao; Qiurong Yan; Yongan Liu; Hao Yang; Xiangping Zhu; Yonglin Wei; Xiaofeng Sai; Feifei Zhao; Mei Li
Archive | 2012
Qiurong Yan; Baosheng Zhao; Yongan Liu; Lizhi Sheng; Yonglin Wei; Xiaofeng Sai
Archive | 2012
Qiurong Yan; Baosheng Zhao; Yongan Liu; Lizhi Sheng; Yonglin Wei; Xiaofeng Sai