2 may be produced on the surface of detectors, using two commercial YAG dye pulse lasers supplied only with 10KW source. The latent effects of some practical nonideal reasons on the photo-produced stress are analysed and discussed. The realizatoin is also reached that the energy expending of the damage effect resulting from the coherent Raman phonons is less than that of the same effect resulting from thermal effects.]]> 2014/1/3 16:01:27 Lu Qisheng,Jiang Zhiping and Liu Zejing 93true 2013/11/18 15:33:03 Chen Jinbao,Zhao Yijun,Liu Zejin and Shu Bohong 92true 3-YBCO superconductor is illuminated by laser(CW-CO₂ laser, CW-YAG and plused-YAG laser). The influence of laser on supconducting critical electric current density Jc is studied.]]> 2013/11/18 15:30:59 CHENG Xiangai,YU Banmei,CHEN Jingbao,SHU Bohong,AI Jie,DENG Qinghua,HU xin and ZHONG Huihuang 91true 3 from 5mg to 10mg are added respectively. AII sampIes are prepared by solid state reaction method. From the superconductor transit temperature（Tc），transit width ΔT，critical electric current density Jc，SEM and XRD chart，we can draw the conclusion that Tc of abundant 123 phase samples is above 90K（ΔT=1～3K）；20mg BaCO₃ is propitious to growth of 123 phase；some abundant BaCO₃ help to improve Jc.]]> 2013/11/18 15:30:58 CHENG Xiangai,YU Banmei,DENG Qinghua,AI Jie,ZHONG Huihuang and HU xin 90true 2013/11/18 0:00:00 ZHANG Xiaoping,ZHOU Jinjuan,LI Xiangsheng,ZHANG Jiande and LI Chuanlu 89true C was measured. The experimental results show that proper microwave radiation can improve the critical current density J_C of samples, samples radiated once in comparison with non-radiated samples, the value of J_C increases one order.]]> 2013/11/18 0:00:00 YU Banmei,CHENG Xiangai,HU Xin,XUE Xiaodong and ZHONG Huihuang 88true 2013/4/27 3:07:23 QIU Zhiqiang,LU Hongwei,ZHANG Xiaohu and YU Qifeng 87true 2013/4/8 11:10:35 YANG Hanwu,WANG Yong,ZHANG Jiande and ZHAO Yansong 86true 11mode converter. The mode conversion processes of the mode converter were reviewed, and the reflective characteristics were studied by analyzing the waveguide discontinuousness. It is revealed that, the reflection modes of the mode converter are TEM mode and TE₁₁mode, the reflection TE₁₁ mode can be canceled by choosing the right radii of the coaxial waveguide, and the reflection TEM mode can be diminished by setting matching poles and properly designing the cone at the end of inner conductor.]]> 2013/4/8 11:10:35 1,LIU Qingxiang² and ZHONG Huihuang¹]]> YUAN Chengwei¹,LIU Qingxiang² and ZHONG Huihuang¹ 85true -10T is obtained in this system.]]> 2013/4/8 11:09:48 ZHANG Xueliang,NI Ming,MENG Zhou and HU Yongming 84true 2013/3/14 10:39:54 YUAN Baolun and RAO Guyin 83true 2013/3/14 10:39:12 ZHANG Xiaohu,DI Hui,ZHOU Jian,SHANG Yang,LI Lichun and YU Qifeng 82true 2013/3/14 10:39:12 DI Hui and YU Qifeng 81true 2013/3/25 4:43:53 TANG Litie,QIU Zhiqiang and LU Qisheng 80true 2013/2/28 5:09:21 HU Xiaojun,ZHENG Ziwen,DAI Yifan and LI Shengyi 79true 2013/2/28 5:09:21 YAN Baozhu,YUAN Shengfu and LU Qisheng 78true 2013/2/28 5:09:09 1,LUO Jianshu¹ and LI Chuanlu²]]> NI Guyan¹,LUO Jianshu¹ and LI Chuanlu² 77true 2013/2/28 5:08:14 LIU Jianping,MENG Zhipeng,CAO Shengguang and LI Da 76true 2012/12/7 2:58:05 LI Lan,HUA Weihong,YUAN Shengfu and JIANG Zongfu 75true 2012/12/7 2:57:23 GONG Changchao,ZENG Xinwu,ZHAO Yun and XU Wei 74true 2012/11/8 3:52:03 XUN Tao,YANG Hanwu,ZHANG Jiande and WANG Yong 73true 2012/11/8 3:52:58 WANG Xiaowei,LI Quan,WANG Yangui,CHEN Wei and HU Xiaojing 72true 2012/11/8 3:52:58 GAO Jingming,LIU Yonggui,YANG Jianhua,ZHOU Xiang and LONG Xiafeng 71true 2012/8/28 16:33:33 YUAN Shengfu,LIU Wenguang,HUA Weihong,YAN Baozhu and LIU Zejin 70true 2012/9/19 9:01:24 1,2,TAN Jichun³,ZHENG Guangwei¹,HE Yanlan³,ZHENG Haobin³,RUAN Yi¹ and LIU Yixing³]]> LIU Li^1,2,TAN Jichun³,ZHENG Guangwei¹,HE Yanlan³,ZHENG Haobin³,RUAN Yi¹ and LIU Yixing³ 69true 2012/9/19 9:01:24 ZHANG Qinghua,HU Shaomin and LONG Xingwu 68true 2 flow rate, the changing of the chemiluminescence in visible range in the optical cavity flow field of discharge driven HF laser was observed and recorded, and the spectrum of the chemiluminescence on the optic axis was measured. The component particle of the gas in the optical cavity was analyzed theoretically, and the high order overtone spectral line of HF molecule was computed. It was found that the spectral line of the transition from 3 order vibration excited state to ground state was in infrared region. The measured spectrum of the chemiluminescence and the spectral line of the particle was compared, discovering that the yellow-green chemiluminescence was formed by the radiation of the excited F, He, H, N, HF and other particle, which corrected the explanation in some classic literature that the yellow-green chemiluminescence was formed by the 3,4,5 order overtone radiation of HF molecule. This further explains the color forming of the chemiluminescence on the optic axis.]]> 2012/9/12 11:15:11 LUO Wei,YUAN Shengfu,YAN Baozhu and LU Qisheng 67true 2012/9/12 11:15:11 CHEN Minsun,JIANG Houman and LIU Zejin 66true 2012/8/28 11:51:54 1,JIANG Guangwen¹,FU Sihua¹ and YU Qifeng²]]> CHAO Zhichao¹,JIANG Guangwen¹,FU Sihua¹ and YU Qifeng² 65true 2012/8/28 11:51:54 YANG Yujie,HU Biru and WU Wenjian 64true 2012/8/28 10:30:13 1,XI Xiaoming¹,SUN Guilin^1,2,Xu Zhongnan¹,HOU Jing¹ and JIANG Zongfu¹]]> CHEN Zilun¹,XI Xiaoming¹,SUN Guilin^1,2,Xu Zhongnan¹,HOU Jing¹ and JIANG Zongfu¹ 63true 2012/8/28 10:30:13 ZHANG Bin,HOU Jing and JIANG Zongfu 62true 2012/8/28 10:30:13 1,2,CHENG Xiangai¹,LI Li¹,ZHENG Xin¹,JIANG Houman¹,LU Qisheng¹,TIAN Hong³ and BIAN Jing³]]> JIANG Tian^1,2,CHENG Xiangai¹,LI Li¹,ZHENG Xin¹,JIANG Houman¹,LU Qisheng¹,TIAN Hong³ and BIAN Jing³ 61true 3gas was injected, the plasma necking phenomenon occurred in all three discharge tubes. For the laser which used the 20mm diameter discharge tube, the plasma necking phenomenon was the weakest, the total consume of working gas was the least, the output power and the electro-optic transfer efficiency were the highest, and the laser output power promotion effect by secondary He was the most outstanding. Through comparison, it is suggested that the stability and volume of the plasma are two intuitionistic parameters for judging the performance of discharge tubes.]]> 2012/8/28 10:30:13 LUO Wei,YUAN Shengfu,LU Qisheng and YAN Baozhu 60true 2012/8/28 10:30:13 1,YANG Zining¹,LIU Liang¹,GUO Shaofeng¹,XU Xiaojun¹,ZHAO Yijun¹,LIU Wenbing²,JIANG Benxue² and PAN Yubo²]]> LI Xiao¹,YANG Zining¹,LIU Liang¹,GUO Shaofeng¹,XU Xiaojun¹,ZHAO Yijun¹,LIU Wenbing²,JIANG Benxue² and PAN Yubo² 59true 2012/8/28 10:30:13 YAN Baozhu,YUAN Shengfu,LU Qisheng,LI Lan and JIN Donghuan 58true 2012/8/28 10:30:13 CHEN Minsun,JIANG Houman and LIU Zejin 57true 2012/8/28 10:30:14 HAN Kai,XU Xiaojun,ZHOU Pu,MA Yanxing and WANG Xiaolin 56true 2012/8/28 10:30:14 WU Saicheng,QIN Shiqiao,WANG Xingshu and HU Chunsheng 55true 3-D₂-He reaction system were calculated by combining minimum Gibbs' free energy method and mass flux conservation principle. Mole flux of F atom as a new parameter that can be used to express yield of F atom was presented. The effect of changing fuels' mass flow rates on combustor's characteristics was analyzed with emphasis. When the compositions proportion in combustor was maintained constant, increasing of mass flow rate of F atom and total pressure of combustor was in proportion to the increasing of total mass flow rate. Changing of total pressure had no obvious impact on adiabatic flame temperature, degree of F₂ dissociation, and mole fraction of F atom. The changing of mass flow rates of NF₃ or D₂ was able to adjust the oxidizer excess factor. In comparison with changing mass flow rate of D₂, changing mass flow rate of NF₃ could acquire much higher mole fraction and mole flux of F atom, much smaller fluctuating amplitude of combustor's total pressure. Increasing mass flow rate of He decreased adiabatic flame temperature and mole fraction of F atom observably. Whereas degree of F₂ dissociation and mole flux of F atom maintained a high level still when primary diluent ratio was less than 15.]]> 2012/8/28 10:30:14 JIN Donghuan,LIU Wenguang,CHEN Xing and LU Qisheng 54true 2012/8/29 10:50:39 JIN Donghuan,LIU Wenguang,CHEN Xing,LU Qisheng and ZHAO Yijun 53true 2012/8/29 10:50:39 ZHANG Wei,CHEN Yuzhong and HU Yongming 52true 2013/1/11 4:19:31 1,2,HAI Yulin³,SUN Xiangyi¹ and ZHANG Xiaohu¹]]> ZHOU Jian^1,2,HAI Yulin³,SUN Xiangyi¹ and ZHANG Xiaohu¹ 51true 2013/1/11 4:19:31 1,2,YU Qifeng^1,2,LEI Zhihui^1,2 and HOU Wang^1,2]]> LIU Xiaochun^1,2,YU Qifeng^1,2,LEI Zhihui^1,2 and HOU Wang^1,2 50true 2012/9/12 9:00:49 1,ZENG Xinwu²,WANG Yibo² and CAI Qingyu²]]> ZHANG Zhenfu¹,ZENG Xinwu²,WANG Yibo² and CAI Qingyu² 49true 2012/8/28 10:27:55 NIE Yongming,LI Xiujian,QI Junli,YANG Jiankun,LIAO Jiali,HU Wenhua and LUO Shishang 48true 2012/8/27 9:46:17 CHEN Shengping,CHEN Hongwei,WANG Jianhua,CHEN Zilun,HOU Jing,XU Xiaojun,CHEN Jinbao and LIU Zejin 47true 2012/8/27 9:46:17 LIU Wenguang and QIU Weicheng 46true 2012/8/27 9:46:17 HUANG Shengyang,XI Fengjie,NING Yu,LIU Changhai and JIANG Zongfu 45true 2012/8/27 9:46:17 SUN Ke,JIANG Houman and CHENG Xiangai 44true 4, will cause excessive absorption of acoustic energy due to its chemical relaxation. Starting from a modified equation of state, with special consideration of the relaxation absorption of MgSO₄ in seawater, a new wave propagation equation of intensive acoustic pulse was deduced. Combined with the numerical algorithm, the propagation process of the pulse was simulated and the effects of MgSO₄ relaxation on waveform and spectrum were analyzed. The results indicate that relaxation process will flatten and smooth the steep pulse waveform, and reduce the acoustic energy to low frequency end. The chemical relaxation effects will cause extra loss of the pulse energy, in addition to the geometric spreading effects of pulse wavefront. ]]> 2012/8/27 9:46:17 ZHANG Jun,ZENG Xinwu,WANG Yibo and CHEN Dan 43true 2012/8/27 9:46:17 LI Xiao,CAO Jianqiu,ZHOU Pu,CHEN Zilun,XU Xiaojun and ZHAO Yijun 42true 2012/8/27 9:46:17 WU Huiyun,WU Wuming,XU Xiaojun,CHEN Jinbao and ZHAO Yijun 41true 2012/8/27 9:46:17 WANG Xiaolin,ZHOU Pu,MA Yanxing,MA Haotong,LI Xiao,XU Xiaojun and ZHAO Yijun 40true 2012/8/27 9:46:18 MA Yanxing,SI Lei,ZHOU Pu,WANG Xiaolin,ZHANG Kan,ZHAO Haichuan,XU Xiaojun and ZHAO Yijun 39true 2013/8/22 16:54:28 1,ZHU Zhaokun¹,CHEN Shengyi¹,GUO Jinhu² and ZHANG Xiaohu¹]]> ZHU Zunshang¹,ZHU Zhaokun¹,CHEN Shengyi¹,GUO Jinhu² and ZHANG Xiaohu¹ 38true 2013/5/21 9:27:56 ZHANG Wei,CAI Yingbo and WEI Xuetong 37true 2013/5/21 9:27:56 HOUWang,ZHONG Lijun,ZHANG Xiaohu,LEI Zhihui and YANG Xia 36true 2015/1/22 16:38:31 LU Jun and PENG Zhongtao 35true 2015/1/22 16:38:31 GUAN Banglei,CAO Yu,YANG Xia,ZHOU Langming and ZHANG Xiaohu 34true 2014/7/17 17:22:22 YANG Mingye,SONG Zhangqi,ZHANG Xueliang and CHEN Yuzhong 33true 2014/5/14 17:10:49 1,2, GONG Wenquan², SU Ang¹, ZHANG Yueqiang¹, ZHANG Xiaohu¹]]> XU Yuhua^1,2, GONG Wenquan², SU Ang¹, ZHANG Yueqiang¹, ZHANG Xiaohu¹ 32true 2014/5/14 17:10:49 1,2, DING Shaowen^1,2, TIAN Zunhua^1,2, ZHANG Hongliang^1,2, ZHANG Xiaohu^1,2]]> GUO Pengyu^1,2, DING Shaowen^1,2, TIAN Zunhua^1,2, ZHANG Hongliang^1,2, ZHANG Xiaohu^1,2 31true 2015/12/31 10:11:11 1,2, DAI Yifan^1,2, GUAN Chaoliang^1,2 and WANG Guilin^1,2]]> ZHU Dengchao^1,2, DAI Yifan^1,2, GUAN Chaoliang^1,2 and WANG Guilin^1,2 30true 2015/11/9 16:21:59 1, CHEN Weiyi¹ and XU Zhongsheng²]]> LIU Hongliang¹, CHEN Weiyi¹ and XU Zhongsheng² 29true 2015/5/16 9:33:23 ZHANG Cunbo, ZHANG Jiande, WANG Honggang and DU Guangxing 28true 2015/5/16 9:33:23 1, SONG Zuyin², YUAN Yunhua², QIN Shu², CHEN Dongqun¹ and LIU Jinliang¹]]> ZHANG Tianyang¹, SONG Zuyin², YUAN Yunhua², QIN Shu², CHEN Dongqun¹ and LIU Jinliang¹ 27true 2015/5/16 9:33:24 LI Song, GAO Jingming, YANG Hanwu and QIAN Baoliang 26true 2015/5/16 9:33:24 1, LIU Lie¹, JU Jinchuan¹ and WANG Xiao²]]> CAI Dan¹, LIU Lie¹, JU Jinchuan¹ and WANG Xiao² 25true 2015/5/16 9:33:24 ZHU Danni, ZHANG Jun, ZHONG Huihuang and QI Zumin 24true 2015/5/16 9:33:24 JIANG Tao, HE Juntao, ZHANG Jiande, LI Zhiqiang and LING Junpu 23true 2015/5/16 9:33:24 WU Dapeng, SHU Ting and ZHANG Hua 22true 10 mode was investigated. This magnetron with 6 resonant cavities operates at πmode and can well transit between resonant cavities and rectangular output waveguide through the structure design of 4 cavities axial output, which realizes the microwave output of rectangular TE₁₀ mode. Compared with the magnetron with diffraction output (MDO), this design not only makes both the diameter and the axial length of the magnetron minimized so that the whole system can be more compact, but also provides a much purer output mode of a low order in the output waveguide. The operating performance of the magnetron has been analyzed and optimized by using particle-in-cell simulation software. Simulation results show that the power conversion efficiency can reach to 25.0%, corresponding to the output power of 10GW and the working frequency of 2.58GHz, under the condition of the applied voltage of 500kV and the applied magnetic field of 0.5T.]]> 2015/5/16 9:33:24 SHI Difu, QIAN Baoliang, WANG Honggang and LI Wei 21true 0n modes, it has high energy conversion efficiency, but it can′t ensure the purity of output modes. However, it is necessary for high radiation efficiency that the microwave input to the radiation terminal is certain single and pure. So it is hard to put these HPM sources into application. In order to solve this problem, a design method for compact hybrid modes converter of purifying TM_0n mixed modes was proposed. With this method, the TM₀₁,TM₀₂ and TM₀₃ mixed modes can be converted into pure circular waveguide TM₀₁ mode efficiently on the condition of high power capacity and wide wave band. This method also reduces the modes purification difficulty in the design of the HPM sources.]]> 2015/5/16 9:33:24 PENG Shengren, YUAN Chengwei, SHU Ting, ZHANG Qiang and WU Dapeng 20true 01 mode high power microwave phase shifter is proposed which is composed of two crossed circularly polarized TE₁₁ mode converter. The phase of the output microwave can be adjustable in a range of 0°~360°. The electromagnetic behaviors of the circularly polarized TE₁₁ mode converter and the phase shifter are simulated by the software CST. The results show that the output microwave can be adjustable in a range of 0°~360°at the frequency of 1.75GHz with the error is not more than 1 °, the transmission efficiency in this range is larger than 97%, and the power capacity is larger than 4.3GW.]]> 2015/5/16 9:33:24 ZHAO Xuelong, YUAN Chengwei, LIU Lie, PENG Shengren, BAI Zhen and CAI Dan 19true 2016/7/7 11:14:22 XIE Yuanping, YU Xudong, WEI Guo, LONG Xingwu, LUO Hui, HUANG Yun and WAN Zhiyi 18true 2016/3/7 9:21:22 1,2, YANG Li¹, FAN Chunli¹, SHI Hongchen¹ and ZHAO Xiaolong¹]]> CHEN Lin^1,2, YANG Li¹, FAN Chunli¹, SHI Hongchen¹ and ZHAO Xiaolong¹ 17true 2016/3/7 9:21:23 LI Geng, ZHANG Pengfei and LONG Xingwu 16true 2018/1/16 17:02:02 CHEN Yuzhong, SONG Zhangqi and ZHANG Xueliang 15true 2017/11/7 15:44:04 1, WANG Mi¹, JIN Shuying¹, PAN Jun¹, WANG Yan² and ZHANG Biao²]]> FAN Chengcheng¹, WANG Mi¹, JIN Shuying¹, PAN Jun¹, WANG Yan² and ZHANG Biao² 14true 2+NF₃+He)+D₂ and (C₂H₄+NF₃+He)+D₂, when the primary dilution He is preheated to (1100 K,1300 K), the available specific output power is improved by (21%, 24%) and (46%, 56%) respectively; and at the same time, the fuel consumption in the combustor is reduced by (255%, 29%) and (32%, 36%) respectively. In practical application, the primary dilution He can be heated to 800℃(1100 K) successfully. Therefore, preheating the primary dilution He is a feasible and effective method to improve the laser output characteristics, which can facilitate the development of more compact chemical lasers with higher efficiency.]]> 2019/1/17 15:43:46 FANG Xiaoting, YUAN Shengfu and HUA Weihong 13true 2018/9/17 0:00:00 NIE Jinsong and HU Yuze 12true 2 OPO (optical parametric oscillation) pumped by a 2.7 μm laser. Experimental results were analyzed in detail. The pump source was a 2.7 μm KTiOPO₄ OPO laser pumped by a 1064 nm Nd:YAG laser, and the KTiOPO₄ OPO was singly resonated. Two identical KTiOPO₄ crystals were placed with opposite optical axis to compensate the walk off effect. The KTiOPO₄ crystals were cut asΦ=0°,θ=62° to generate 2.7 μm wave band laser. To utilize the large effective nonlinear coefficient, the phase matching was based on type Ⅱ(B) (o→o+e). The ZnGeP₂ OPO was singly resonated too. To output narrow linewidth laser, the phase matching is based on typeⅡ(B) (o→o+e).The ZnGeP₂ crystal was cut as Φ=0°,θ=68° to generate 4.3 μm laser. The energy of the 2.7 μm laser is 7.5 mJ with a pulse of 8.6 ns and line-width 12 nm.The pulse energy of 2.12 mJ at 4.26 μm with an optical-optical conversion efficiency of 28.3% and a slop efficiency of 32.6% is obtained, and the pulse width is 8.7 ns, the line-width is 30 nm. The beam qualities M² of horizontal and vertical directions are 6.2 and 13.5, respectively.]]> 2018/9/17 0:00:00 BIAN Jintian, YE Qing and SUN Xiaoquan 11true 4 K level in the laser pulse irradiation moment. And then the energy is released slowly to lattice and the thermal equilibrium is reached until 10 ns order of magnitude. The electron has two rapid warming processes. The first one starts from the free-carrier absorption, and stops at the electron-lattice energy coupling; the second one starts from the single photon and two photon absorption, and ends at the end of the pulse. It is found that the higher the temperature and density of electron are, the bigger the pulse energy is and the shorter the pulse duration is.]]> 2018/9/17 0:00:00 DOU Xianan, SUN Xiaoquan and XU Haiping 10true 4 crystal is chosen as 12 mm, the transmissivity of the output mirror is fixed to 10%, and the Q-switching frequency is selected as 50 kHz, the average output power of the fundamental wave is 18.98 W, and the average power of the output of secondharmonic wave is 2.22 W. ]]> 2018/9/17 0:00:00 1, FAN Yisong^1,2, WANG Lei¹ and BIAN Jintian¹]]> YE Qing¹, FAN Yisong^1,2, WANG Lei¹ and BIAN Jintian¹ 9true 2 under the photovoltage effect, and 2.23 μJ/cm² under the space charge effect. An experimental investigation of the saturation effect of multi-alkali photocathode irradiated with 266 nm laser is conducted, and the saturation threshold laser energy density is about 2 μJ/cm², which indicates that the space charge effect is the main factor limiting its photoelectron emission capability. ]]> 2018/9/17 0:00:00 XIE Yuntao, SUN Xiaoquan, WANG Xi and ZHANG Yujun 8true 2018/9/17 0:00:00 WU Yunlong, SUN Xiaoquan and NIE Jinsong 7true 2018/9/17 0:00:00 LIU Yang, CHENG Li, WANG Jiachun, YUAN Zhongcai and SHI Jiaming 6true -3lux), the LLL image has the characteristics of low signaltonoise ratio and low contrast, so that the target is difficult to be identified, thus seriously affecting the observation effect. In order to improve the LLL image quality, a convolutional autoencoder deep neural network for image enhancement was designed. In view of the fact that the traditional mean square error loss function cannot meet the human visual perception characteristics, several loss functions including perceptual loss were studied and a novel, differentiable loss function was proposed in combination with the existing full reference image quality evaluation index. Experimental results show that the proposed loss function can improve the detail information of the image while improving the signaltonoise ratio and contrast ratio of the lowlight level image when the network structure does not change. ]]> 2018/9/17 0:00:00 1,2, ZHANG Xiaohui¹ and HU Qingping¹]]> LIU Chao^1,2, ZHANG Xiaohui¹ and HU Qingping¹ 5true 2018/9/17 0:00:00 1,2, ZHANG Xiaohu^1,2, WANG Jie^1,2 and SHI Zhongchen^1,2]]> DING Shaowen^1,2, ZHANG Xiaohu^1,2, WANG Jie^1,2 and SHI Zhongchen^1,2 4true 2018/9/17 0:00:00 1,2, DAI Yifan^1,2, NING Yu³, GUAN Chaoliang^1,2, LIU Junfeng^1,2 and FU Tianyang³]]> FAN Zhanbin^1,2, DAI Yifan^1,2, NING Yu³, GUAN Chaoliang^1,2, LIU Junfeng^1,2 and FU Tianyang³ 3true 2019/9/30 15:58:02 ZHANG Lin, YANG Li and FAN Chunli 2true 2019/4/24 14:24:49 1,2,3, PENG Rencan^2,3 and DONG Jian^2,3]]> ZHOU Wei^1,2,3, PENG Rencan^2,3 and DONG Jian^2,3 1true