Jin-Da Chen
Chinese Academy of Sciences
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Featured researches published by Jin-Da Chen.
Astronomy and Astrophysics | 2004
J. Li; Juncai Ma; Xingtai Zhou; Zhongyi Jiang; Yulan Yang; Jin-Da Chen
We present CCD spectrophotometry of the nearby spiral galaxy M 33 using images obtained with National Astronomical Observatories of China (NAOC) 60/90 cm Schmidt telescope in a broad U-band and 13 intermediate-band filters from 4000 to 10 000 A. The observations cover the whole area of M 33, with a total integration of 39.08 h from September 23, 1995 to August 28, 2000. The spectral energy distributions (SEDs) for each area of M 33 are obtained. With the aid of an evolutionary synthesis model, PEGASE (Fioc & Rocca-Volmerange 1997, 2000), we compute theoretical SEDs for three kinds of star formation rate (SFR) histories. From best fits on templates of PEGASE and observed SEDs by the χ 2 -minimization procedure, we find that both the constant and exponentially decreasing (hereafter Exp, τ = 12 Gyr) SFR give good agreement between models and observations. We then obtain age distributions (when the observed stellar population formation began) and evolutionary histories of M 33 for the two models. For the constant SFR, an age gradient is clearly found between stellar populations of the central regions and of the outer regions. The stellar populations in its central regions are older than 10 Gyr; stars in the outer regions are younger, about 7 Gyr and the youngest components in the spiral arms are less than 5 Gyr. The Exp SFR gives a similar age distribution, but with absolute ages that are smaller by ∼2 Gyr. We conclude that M 33 has been forming stars continuously for most of its lifetime, with the interior having built up its stellar populations several Gyr earlier than the outer parts.
Chinese Physics C | 2016
Cheng-Ming Du; Jin-Da Chen; X. J. Zhang; Hai-Bo Yang; Ke Cheng; Jie Kong; Zheng-Guo Hu; Zhi-Yu Sun; Hong Su; Hu-Shan Xu
A new Digital Pulse Processing(DPP) module has been developed, based on a domino ring sampler version 4 chip(DRS4), with good time resolution for La Br3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes(PMTs). Two PMTs were coupled with La Br3 scintillators and placed on opposite sides of a radioactive positron22 Na source for 511 ke V γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps(FWHM), obtained by the digital constant fraction discrimination(d CFD) method,which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography(PET) with time of flight(TOF), as well as for scintillation timing measurement,such as in TOF-?E and TOF-E systems for particle identification, with picosecond accuracy timing measurement.Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronic and acquisition system to process the output signals from XP20D0 Photomultiplier Tubes (PMTs). Two PMTs were coupled with LaBr3 scintillator and placed face to face on both sides of a radioactive positron 22Na source for 511 keV gama ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-DeltaE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes (PMTs). Two PMTs were coupled with LaBr3 scintillators and placed on opposite sides of a radioactive positron 22Na source for 511 keV γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-ΔE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.
arXiv: Instrumentation and Detectors | 2015
Cheng-Ming Du; Jin-Da Chen; X. J. Zhang; Hai-Bo Yang; Ke Cheng; Zheng-Guo Hu; Zhi-Yu Sun; Hu-Shan Xu
A new Digital Pulse Processing(DPP) module has been developed, based on a domino ring sampler version 4 chip(DRS4), with good time resolution for La Br3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes(PMTs). Two PMTs were coupled with La Br3 scintillators and placed on opposite sides of a radioactive positron22 Na source for 511 ke V γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps(FWHM), obtained by the digital constant fraction discrimination(d CFD) method,which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography(PET) with time of flight(TOF), as well as for scintillation timing measurement,such as in TOF-?E and TOF-E systems for particle identification, with picosecond accuracy timing measurement.Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronic and acquisition system to process the output signals from XP20D0 Photomultiplier Tubes (PMTs). Two PMTs were coupled with LaBr3 scintillator and placed face to face on both sides of a radioactive positron 22Na source for 511 keV gama ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-DeltaE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes (PMTs). Two PMTs were coupled with LaBr3 scintillators and placed on opposite sides of a radioactive positron 22Na source for 511 keV γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-ΔE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.
arXiv: Instrumentation and Detectors | 2015
Cheng-Ming Du; Jin-Da Chen; X. J. Zhang; Hai-Bo Yang; Ke Cheng; Jie Kong; Zheng-Guo Hu; Zhi-Yu Sun; Hong Su; Hu-Shan Xu
A new Digital Pulse Processing(DPP) module has been developed, based on a domino ring sampler version 4 chip(DRS4), with good time resolution for La Br3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes(PMTs). Two PMTs were coupled with La Br3 scintillators and placed on opposite sides of a radioactive positron22 Na source for 511 ke V γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps(FWHM), obtained by the digital constant fraction discrimination(d CFD) method,which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography(PET) with time of flight(TOF), as well as for scintillation timing measurement,such as in TOF-?E and TOF-E systems for particle identification, with picosecond accuracy timing measurement.Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronic and acquisition system to process the output signals from XP20D0 Photomultiplier Tubes (PMTs). Two PMTs were coupled with LaBr3 scintillator and placed face to face on both sides of a radioactive positron 22Na source for 511 keV gama ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-DeltaE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.A new Digital Pulse Processing (DPP) module has been developed, based on a domino ring sampler version 4 chip (DRS4), with good time resolution for LaBr3 detectors, and different digital timing analysis methods for processing the raw detector signals are reported. The module, composed of an eight channel DRS4 chip, was used as the readout electronics and acquisition system to process the output signals from XP20D0 photomultiplier tubes (PMTs). Two PMTs were coupled with LaBr3 scintillators and placed on opposite sides of a radioactive positron 22Na source for 511 keV γ-ray tests. By analyzing the raw data acquired by the module, the best coincidence timing resolution is about 194.7 ps (FWHM), obtained by the digital constant fraction discrimination (dCFD) method, which is better than other digital methods and analysis methods based on conventional analog systems which have been tested. The results indicate that it is a promising approach to better localize the positron annihilation in positron emission tomography (PET) with time of flight (TOF), as well as for scintillation timing measurement, such as in TOF-ΔE and TOF-E systems for particle identification, with picosecond accuracy timing measurement. Furthermore, this module is more simple and convenient than other systems.
Journal of Physics: Conference Series | 2014
Jin-Da Chen; Zheng-Guo Hu; X. J. Zhang; Ze Chen; X. Yuan; Zhi-Yu Sun; Zy Guo; Hu-Shan Xu
In order to satisfy high precision requirement for the modern nuclear physics experiment detectors and radiologic imaging technology equipments, we do some researches in improving the resolution of the detector with LaBr3:Ce scintillator.
Science China-physics Mechanics & Astronomy | 2011
LinHui Lü; Y. Ye; D. X. Jiang; H. Hua; T. Zheng; Z. H. Li; Yu-Cheng Ge; Xiangqing Li; J. L. Lou; Z. X. Cao; Yu-Shou Song; J. Xiao; Q. Li; R. Qiao; H.B. You; R. Chen; Hu-Shan Xu; J.Z. Wang; Zy Guo; XueYing Zhang; Chen Li; Zheng-Guo Hu; R. F. Chen; Meng Wang; Zhiguo Xu; K. Yue; Bin Tang; Y. D. Zang; Xue-Heng Zhang; XiangWu Yao
Science China-physics Mechanics & Astronomy | 2011
J.J. He; Jun Hu; Shi-Wei Xu; Z. Chen; XueYing Zhang; J.Z. Wang; XiangQing Yu; LiYong Zhang; Long Li; Yan-Yun Yang; P. Ma; Xue-Heng Zhang; Zheng-Guo Hu; Zy Guo; Xing Xu; X. Yuan; Wan Lu; Y. Yu; Y. D. Zang; S.W. Tang; R.P. Ye; Jin-Da Chen; S. L. Jin; Cheng-Ming Du; Shi-Tao Wang; J.M. Ma; L. Liu; Zhen Bai; X. G. Lei; Zhi-Yu Sun
European Physical Journal A | 2011
J.J. He; Jun Hu; S. W. Xu; Z. Chen; Xiuqing Zhang; J. Wang; Hui Wang; Wendong Tian; X. Q. Yu; LiYong Zhang; Lin Li; Ying Yang; P. Ma; X.H. Zhang; J. Su; E. T. Li; Z. G. Hu; Zy Guo; X. Xu; X. Yuan; Wan Lu; Y. Yu; Y. D. Zang; Shao-Qiang Ye; R.P. Ye; Jin-Da Chen; S. L. Jin; Cheng-Ming Du; S. T. Wang; J.B. Ma
Archive | 2010
Hu-Shan Xu; Bin Tang; Zheng-Guo Hu; Zhiguo Xu; R. S. Mao; T.C. Zhao; Jin-Da Chen; Limin Duan; Zhi-Yu Sun; J.Z. Wang; Guoqing Xiao; Zy Guo; Xinjuan Rong
Nuclear Engineering and Technology | 2018
X. J. Zhang; Cheng-Ming Du; Jin-Da Chen; He-Run Yang; Jie Kong; Hai-Bo Yang; P. Ma; Guozhu Shi; Limin Duan; Zheng-Guo Hu