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Robust Space-Time Adaptive Track-Before-Detect Algorithm Based on Persymmetry and Symmetric Spectrum
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作者 Xiaojing Su da xu +1 位作者 Dongsheng Zhu Zhixun Ma 《Journal of Beijing Institute of Technology》 EI CAS 2024年第1期65-74,共10页
Underwater monopulse space-time adaptive track-before-detect method,which combines space-time adaptive detector(STAD)and the track-before-detect algorithm based on dynamic programming(DP-TBD),denoted as STAD-DP-TBD,ca... Underwater monopulse space-time adaptive track-before-detect method,which combines space-time adaptive detector(STAD)and the track-before-detect algorithm based on dynamic programming(DP-TBD),denoted as STAD-DP-TBD,can effectively detect low-speed weak targets.However,due to the complexity and variability of the underwater environment,it is difficult to obtain sufficient secondary data,resulting in a serious decline in the detection and tracking performance,and leading to poor robustness of the algorithm.In this paper,based on the adaptive matched filter(AMF)test and the RAO test,underwater monopulse AMF-DP-TBD algorithm and RAO-DP-TBD algorithm which incorporate persymmetry and symmetric spectrum,denoted as PSAMF-DP-TBD and PS-RAO-DP-TBD,are proposed and compared with the AMF-DP-TBD algorithm and RAO-DP-TBD algorithm based on persymmetry array,denoted as P-AMF-DP-TBD and P-RAO-DP-TBD.The simulation results show that the four methods can work normally with sufficient secondary data and slightly insufficient secondary data,but when the secondary data is severely insufficient,the P-AMF-DP-TBD and P-RAO-DP-TBD algorithms has failed while the PSAMF-DP-TBD and PS-RAO-DP-TBD algorithms still have good detection and tracking capabilities. 展开更多
关键词 space-time adaptive detection track before detect ROBUSTNESS persymmetric property symmetric spectrum AMF test RAO test
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Bioinformatics and Activity Analysis of Antioxidant Enzymes in Wheat Seedlings under Salt Stress and Their Malondialdehyde Content Changes
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作者 da xu Mengqin WANG Yunfeng ZHANG 《Agricultural Biotechnology》 2024年第6期1-5,8,共6页
[Objectives]This study was conducted to improve crop yield and select excellent wheat varieties.[Methods]Wheat seedlings were treated with different concentrations of NaCl solution,and the activities of superoxide dis... [Objectives]This study was conducted to improve crop yield and select excellent wheat varieties.[Methods]Wheat seedlings were treated with different concentrations of NaCl solution,and the activities of superoxide dismutase(SOD)and peroxidase(POD)and the content changes of malondialdehyde(MDA)in the leaves of seedlings were determined.A control group(distilled water)and three treatment groups(NaCl concentrations of 1,2 and 3 mmol/L)were set up.When the wheat seedlings grew to two leaves and one heart,they should be treated with different concentrations of NaCl solution(the wheat seedlings grew uniformly,and 20 ml of each NaCl concentration was used for treatment of wheat).When the wheat seedlings grew to four leaves and one heart under stress,samples were taken separately,once every 2 d,for three times,with 5 g of leaves each time.The SOD and POD activities and MDA content of seedlings in the control group and treatment groups were determined,and related protein sequences were analyzed by bioinformatics,including signal peptide prediction,transmembrane domain prediction,phosphorylation prediction and protein structure prediction.[Results]Under NaCl stress,the growth rates of seedling length and root length of wheat decreased obviously,and SOD and POD in leaves decreased,while the MDA content in leaves after treatment increased compared with the control group.SOD had no signal peptide,while POD had signal peptides and a transmembrane region.SOD and POD were different in terms of secondary and tertiary structures and the number of phosphorylation sites.[Conclusions]These results lays a solid theoretical foundation and application prospect for the study on salt tolerance mechanism of wheat seedlings in the later stage. 展开更多
关键词 WHEAT Salt stress SOD activity POD activity MDA content bioinformation
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豚鼠感染模型评价胞内分枝杆菌毒力的研究
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作者 李光 何杏 +7 位作者 许达 李贞 卢坤鹏 王萍 袁昱珍 李马超 刘海灿 万康林 《中国人兽共患病学报》 CSCD 北大核心 2024年第12期1128-1133,1139,共7页
目的建立豚鼠感染模型,评价胞内分枝杆菌的毒力,为预防与治疗胞内分枝杆菌感染提供科学依据。方法培养胞内分枝杆菌CHPC 1.5701,菌悬液用0.9%氯化钠溶液分别稀释至1×10^(10) CFU/mL、1×10^(9 )CFU/mL、1×10^(8) CFU/mL、... 目的建立豚鼠感染模型,评价胞内分枝杆菌的毒力,为预防与治疗胞内分枝杆菌感染提供科学依据。方法培养胞内分枝杆菌CHPC 1.5701,菌悬液用0.9%氯化钠溶液分别稀释至1×10^(10) CFU/mL、1×10^(9 )CFU/mL、1×10^(8) CFU/mL、1×10^(7 )CFU/mL和1×10^(6) CFU/mL。筛选结核菌素纯蛋白衍生物皮肤试验呈阴性的健康Hartly豚鼠,随机分为6组,每组10只,雌雄各半。实验组豚鼠5组,分别腹腔注射5种不同浓度菌悬液1.0 mL/只,对照组豚鼠腹腔注射0.9%氯化钠溶液1.0 mL/只。观察豚鼠一般表现,每周称重,5周后解剖,取肺、脾、肝组织,分析组织病变及荷菌量。结果攻毒试验对雄性豚鼠体重无影响(P>0.05),可使雌性豚鼠体重减轻(P<0.01),攻毒试验组均观察到豚鼠肺、脾、肝组织病理改变,显微镜下可见肺泡壁肺泡上皮增生,肝脏、脾脏单核细胞浸润,炎性肉芽肿等,病变程度与攻毒剂量有关。部分脏器组织培养可分离到胞内分枝杆菌,其中脾脏荷菌量较大。结论腹腔注射胞内分枝杆菌CHPC 1.5701可影响雌性豚鼠体重,造成肺脏、肝脏、脾脏感染和病变,胞内分枝杆菌对豚鼠具有一定的毒力,属于低毒力、低致病性细菌。 展开更多
关键词 胞内分枝杆菌 豚鼠感染模型 毒力评价
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A New Two-Stage Tunable Space-Time Adaptive Detector
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作者 Xiaojing Su da xu Dongsheng Zhu 《Journal of Beijing Institute of Technology》 EI CAS 2023年第1期124-130,共7页
In order to improve the rejection capability of mismatched interferer signals,a new two-stage detector is proposed under homogeneous scenarios with unknown covariance matrix,which is obtained by cascading the adaptive... In order to improve the rejection capability of mismatched interferer signals,a new two-stage detector is proposed under homogeneous scenarios with unknown covariance matrix,which is obtained by cascading the adaptive matched filter(AMF)detector and the enhanced RAO(EnRAO)detector.The new detector has constant false alarm performance,and the closed-form expression of probability of false alarm and probability of detection is derived.The performance of the new detector is assessed,and analyzed in comparison with other detectors.The results show that,the proposed detector can provide enhanced rejection capability in the case of mismatch,but the performance of the detector is slightly lost under the condition of matching. 展开更多
关键词 adaptive detection constant false alarm rate(CFAR) two-stage tunable adaptive matched filter(AMF) enhanced RAO(EnRAO)
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Ultrathin poly(cyclocarbonate-ether)-based composite electrolyte reinforced with high-strength functional skeleton 被引量:1
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作者 Xiaojiao Zheng da xu +1 位作者 Ning Fu Zhenglong Yang 《Journal of Energy Chemistry》 SCIE EI CAS CSCD 2023年第6期603-612,I0013,共11页
Composite polymer electrolytes(CPEs)are considered to be the most promising to break through the performance and safety limitations of traditional lithium-ion batteries because of their excellent electrochemical and m... Composite polymer electrolytes(CPEs)are considered to be the most promising to break through the performance and safety limitations of traditional lithium-ion batteries because of their excellent electrochemical and mechanical properties.Aiming at the performance limitations of the most common polyether matrix such as poly(ethylene oxide)(PEO),a novel poly(cyclocarbonate-ether)polymer matrix was prepared by in-situ thermal curing,the weaker interaction between its C=O bond and Li^(+)can promote the rapid transport of Li^(+).Adding ionic liquid and active filler LLZTO to the matrix can synergistically reduce the crystallinity of matrix and promote the dissociation of lithium salts.In addition,a 3D functional skeleton made of polyacrylonitrile(PAN)and lithium fluoride(LiF)can greatly improve the mechanical strength of polymer matrix after cold pressing,and Li F is also conducive to interface stability.The thickness of the optimal sample(VP6L/CPL)was only 25μm,and its ionic conductivity,lithium ion transference number,and electrochemical stability window were as high as 7.17×10^(-4)S cm^(-1)(25℃),0.54 and 5.4 V,respectively,while the mechanical strength reaches 6.1 MPa,which can fully inhibit the growth of lithium dendrites.The excellent electrochemical performance and mechanical strength enable the assembled Li|VP6L/CPL|Li battery to be continuously charged for over 200 h and cycled stably for more than 2300 h,and Li|VP6L/CPL|LFP battery can be stably cycled for more than 400 and 550 cycles at 1 C(40℃)and 0.5 C(25℃),respectively. 展开更多
关键词 Composite polymer electrolytes Polymer matrix 3D functional skeleton PLASTICIZATION Synergistic effect
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ALTERNATING DIRECTION IMPLICIT OSC SCHEME FOR THE TWO-DIMENSIONAL FRACTIONAL EVOLUTION EQUATION WITH A WEAKLY SINGULAR KERNEL 被引量:1
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作者 Haixiang ZHANG xuehna YANG da xu 《Acta Mathematica Scientia》 SCIE CSCD 2018年第6期1689-1711,共23页
In this paper, a new kind of alternating direction implicit (ADI) Crank-Nicolson-type orthogonal spline collocation (OSC) method is formulated for the two-dimensional frac-tional evolution equation with a weakly s... In this paper, a new kind of alternating direction implicit (ADI) Crank-Nicolson-type orthogonal spline collocation (OSC) method is formulated for the two-dimensional frac-tional evolution equation with a weakly singular kernel arising in the theory of linear viscoelas-ticity. The novel OSC method is used for the spatial discretization, and ADI Crank-Nicolson-type method combined with the second order fractional quadrature rule are considered for thetemporal component. The stability of proposed scheme is rigourously established, and nearlyoptimal order error estimate is also derived. Numerical experiments are conducted to supportthe predicted convergence rates and also exhibit expected super-convergence phenomena. 展开更多
关键词 fractional equation orthogonal spline collocation scheme alternating directionimplicit stability CONVERGENCE
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Effects of Layer Thickness on the Residual Stresses of CIGS Solar Cells with Polyimide Substrate 被引量:1
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作者 Hansung Kim da xu 《Advances in Materials Physics and Chemistry》 CAS 2022年第9期195-206,共12页
In this paper, we investigate the effect of layer thickness on the residual stresses of copper indium gallium diselenide (CIGS) solar cells with polyimide substrate caused by CIGS layer deposition at 400?C and then co... In this paper, we investigate the effect of layer thickness on the residual stresses of copper indium gallium diselenide (CIGS) solar cells with polyimide substrate caused by CIGS layer deposition at 400?C and then cooling down to room temperature using the Finite Element Method (FEM). Moreover, we also examined the effect of layer thickness on residual stress of CIGS solar cells after cooling down to room temperature from the hotspot temperatures of 200?C, 300?C, and 400?C. Our simulated CIGS is composed of five layers: ZnO, CdS, CIGS, Mo, and PI substrate. We were able to quantify the effect of each layer’s thickness and hotspot temperature on the average stresses of each layer for the CIGS solar cells. We found that the PI substrate layer has the most significant effect on the residual stress of CIGS solar cells. Our simulation results reveal that the stress type (tensile vs. compressive) and the magnitude of stress of the CIGS layer (main absorber layer) can be controlled by changing the thickness of the PI substrate while applying a heat to CIGS solar cells. Quantitative analysis of relationship between layer thickness and thermo-mechanical stress of thin film solar cells can help solar cell manufacturers design more robust and reliable solar cells. For example, fabricating PI layer thickness less than 17 μm can improve the performance of CIGS solar cells by nullifying the compressive residual stress in the CIGS absorber layer. 展开更多
关键词 Thin-Film Solar Cells Residual Stress Temperature CIGS HOTSPOT
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Simulation of the influence of imperfections on dynamical decoupling of a superconducting qubit
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作者 Ying-Shan Zhang Jian-She Liu +3 位作者 Chang-Hao Zhao Yong-Cheng He da xu Wei Chen 《Chinese Physics B》 SCIE EI CAS CSCD 2019年第6期38-44,共7页
Dynamical decoupling is widely used in many quantum computing systems to combat decoherence. In a practical superconducting quantum system, imperfections can plague decoupling performance. In this work, imperfections ... Dynamical decoupling is widely used in many quantum computing systems to combat decoherence. In a practical superconducting quantum system, imperfections can plague decoupling performance. In this work, imperfections in a superconducting qubit and its control system are modeled via modified Hamiltonian and collapse operator. A master equation simulation is carried out on the qubit under 1/f environment noise spectrum. The average dephasing rate of qubit is extracted to characterize the impact of different imperfections on the decoupling from dephasing. We find that the precision of pulse position, on–off ratio, and filtering effect are most critical. Bounded pulses have weaker impact,while variation in pulse width and qubit relaxation are insignificant. Consequently, alternative decoupling protocols, jitter mitigation, cascaded mixers, and pulse shaping can be conducive to the performance of decoupling. This work may assist the analysis and optimization of dynamical decoupling on noisy superconducting quantum systems. 展开更多
关键词 dynamical DECOUPLING SUPERCONDUCTING QUBIT IMPERFECTION DEPHASING
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Observation of nonlinearity and heating-induced frequency shifts in cavity magnonics
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作者 Wei-Jiang Wu da xu +3 位作者 Jie Qian Jie Li Yi-Pu Wang Jian-Qiang You 《Chinese Physics B》 SCIE EI CAS CSCD 2022年第12期517-524,共8页
When there is a certain amount of field inhomogeneity,the biased ferrimagnetic crystal can exhibit the higher-order magnetostatic(HMS)mode in addition to the uniform-precession Kittel mode.In cavity magnonics,we show ... When there is a certain amount of field inhomogeneity,the biased ferrimagnetic crystal can exhibit the higher-order magnetostatic(HMS)mode in addition to the uniform-precession Kittel mode.In cavity magnonics,we show the nonlinearity and heating-induced frequency shifts of the Kittel mode and HMS mode in a yttrium-iron-garnet(YIG)sphere.When the Kittel mode is driven to generate a certain number of excitations,the temperature of the whole YIG sample rises and the HMS mode can display an induced frequency shift,and vice versa.This cross effect provides a new method to study the magnetization dynamics and paves a way for novel cavity magnonic devices by including the heating effect as an operational degree of freedom. 展开更多
关键词 MAGNON magnetostatic mode temperature yttrium-iron-garnet(YIG)
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Microbiome subsets determine tumor prognosis and molecular characteristics of clear-cell renal cell carcinoma:a multi-center integrated analysis of microbiome,metabolome,and transcriptome data
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作者 Wenjin Chen Xiuwu Pan +6 位作者 Wang Zhou da xu Jiaxin Chen Keqin Dong Weijie Chen Brian Rini Xingang Cui 《Frontiers of Medicine》 SCIE CSCD 2024年第2期399-402,共4页
Dear editor,Patients with clear-cell renal cell carcinoma(ccRCC)potentially have a high recurrence rate of more than 40%[1].Patients receive radical or partial nephrectomy,sometimes assisted by targeted therapies or/a... Dear editor,Patients with clear-cell renal cell carcinoma(ccRCC)potentially have a high recurrence rate of more than 40%[1].Patients receive radical or partial nephrectomy,sometimes assisted by targeted therapies or/and immune checkpoint inhibitors(ICIs),to improve overall survival(OS)[2].Large-cohort studies and large-scale human tissue sequencing have provided a series of molecular subtyping methods for precision medicine-based ccRCC risk stratification and therapeutic regimens,such as ClearCode34,the prognostic risk predictor[3],and seven subsets for ICI and angiogenesis blockade outcomes[4].However,these subtyping results are all based on human genomes without including the host microbiota,which may be non-negligible genome components. 展开更多
关键词 editor negligible characteristics
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Insulin-like growth factor 1-induced enolase 2 deacetylation by HDAC3 promotes metastasis of pancreatic cancer 被引量:6
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作者 Yan Zheng Chao Wu +16 位作者 Jimeng Yang Yue Zhao Huliang Jia Min xue da xu Feng Yang Deliang Fu Chaoqun Wang Beiyuan Hu Ze Zhang Tianen Li Shican Yan xuan Wang Peter J.Nelson Christiane Bruns Lunxiu Qin Qiongzhu Dong 《Signal Transduction and Targeted Therapy》 SCIE CSCD 2020年第1期1857-1870,共14页
Enolase 2(ENO2)is a key glycolytic enzyme in the metabolic process of glycolysis,but its potential function in pancreatic ductal adenocarcinoma(PDAC)is unclear.In this study,we observed a significant overexpression of... Enolase 2(ENO2)is a key glycolytic enzyme in the metabolic process of glycolysis,but its potential function in pancreatic ductal adenocarcinoma(PDAC)is unclear.In this study,we observed a significant overexpression of ENO2 in PDAC tissues,and its expression was correlated with metastasis and poor prognosis in PDAC patients.K394 was identified as a major acetylation site in ENO2 that regulates its enzymatic activity,cell metabolism and PDAC progression.Knockdown of ENO2 suppressed tumor growth and liver metastasis in PDAC.Re-expression of wild-type(WT)ENO2,but not the K394 acetylation mimetic mutant,could reverse the decreased tumor malignancy.We further characterized histone deacetylase 3(HDAC3)and P300/CBP-associated factor(PCAF)as the potential deacetylase and acetyltransferase for ENO2,respectively.HDAC3-mediated deacetylation was shown to lead to ENO2 activation and enhancement of glycolysis.Importantly,insulin-like growth factor-1(IGF-1)was found to decrease K394 acetylation and stimulate ENO2 activity in a dose-and time-dependent manner.The PI3K/AKT/mTOR pathway facilitated the phosphorylation of HDAC3 on S424,which promoted K394 deacetylation and activation of ENO2.Linsitinib,an oral small-molecule inhibitor of IGF-1R,could inhibit IGF-1-induced ENO2 deacetylation by HDAC3 and the PI3K/AKT/mTOR pathway.Furthermore,linsitinib showed a different effect on the growth and metastasis of PDAC depending on the overexpression of WT versus K394-mutant ENO2.Our results reveal a novel mechanism by which acetylation negatively regulates ENO2 activity in the metastasis of PDAC by modulating glycolysis.Blockade of IGF-1-induced ENO2 deacetylation represents a promising strategy to prevent the development of PDAC. 展开更多
关键词 HDAC3 METASTASIS METABOLISM
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多功能多场景应用辐射定标光源光学系统设计
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作者 刘显著 徐达 +4 位作者 李栋 李林 刘石 王宇 郑佳伟 《航空学报》 EI CAS CSCD 北大核心 2024年第19期286-294,共9页
目前空间遥感相机地面标定设备缺乏对各种谱线分布的精确模拟以及无法实现同时进行宽带和窄带的光谱辐射定标,导致空间遥感相机地面辐射定标精度低、宽带和窄带定标过程漫长复杂、无法实现多谱段光谱范围辐射定标测试。针对上述难题,提... 目前空间遥感相机地面标定设备缺乏对各种谱线分布的精确模拟以及无法实现同时进行宽带和窄带的光谱辐射定标,导致空间遥感相机地面辐射定标精度低、宽带和窄带定标过程漫长复杂、无法实现多谱段光谱范围辐射定标测试。针对上述难题,提出一种基于前置准直扩束系统凹柱面光栅的光谱辐射定标系统的设计方法,针对凹柱面光栅的场曲特性,设计了楔形场曲补偿棱镜,并通过准直扩束系统减小系统的成像视场,提高凹柱面光栅分光系统的光谱分辨率,将整个系统的光谱分辨率提升了1倍多,由5 nm提升至2 nm。最后,对系统性能进行了测试,测试结果表明在宽带模式下,实现了500~900 nm光谱范围内3 000 K、6 400 K和9 000 K色温模拟,模拟误差优于5%;在窄带模式下,系统输出光束半峰宽度小于3 nm;在多谱段模式下,等能光谱的光谱模拟误差分别为545~600 nm处1.1%、630~690 nm处2.5%、680~725 nm处1.5%。所设计的系统满足空间相机、姿态导航系统以及遥感仪器的宽带、窄带辐射定标和多功能测试标定需求。 展开更多
关键词 光谱辐射定标 光谱模拟 凹柱面光栅 辐射分光 光学设计
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Proportional Mean Residual Life Model with Varying Coefficients for Length-Biased and Right-Censored Data
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作者 da xu Yong ZHOU 《Acta Mathematica Sinica,English Series》 SCIE CSCD 2020年第5期578-596,共19页
Length-biased data are encountered in many fields,including economics,engineering and epidemiological cohort studies.There are two main challenges in the analysis of such data:the assumption of independent censoring i... Length-biased data are encountered in many fields,including economics,engineering and epidemiological cohort studies.There are two main challenges in the analysis of such data:the assumption of independent censoring is violated and the assumed model for the underlying population is no longer satisfied for the observed data.In this paper,a proportional mean residual life varyingcoefficient model for length-biased data is considered and a local pseudo likelihood method is proposed for estimating the coefficient functions in the model.Asymptotic properties are investigated for the proposed estimators.The finite sample performance of the proposed methodology is demonstrated by simulation studies.Finally,the method is applied to a real data set concerning the Academy Awards. 展开更多
关键词 Length-biased data proportional hazards MODEL mean RESIDUAL life varying-coefficient MODEL
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CEPC Technical Design Report 被引量:2
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作者 Waleed Abdallah Tiago Carlos Adorno de Freitas +1111 位作者 Konstantin Afanaciev Shakeel Ahmad Ijaz Ahmed Xiaocong Ai Abid Aleem Wolfgang Altmannshofer Fabio Alves Weiming An Rui An daniele Paolo Anderle Stefan Antusch Yasuo Arai Andrej Arbuzov Abdesslam Arhrib Mustafa Ashry Sha Bai Yu Bai Yang Bai Vipul Bairathi Csaba Balazs Philip Bambade Yong Ban Tripamo Bandyopadhyay Shou-Shan Bao Desmond P.Barber Ayse Bat Varvara Batozskaya Subash Chandra Behera Alexander Belyaev Michele Bertucci Xiao-Jun Bi Yuanjie Bi Tianjian Bian Fabrizio Bianchi Thomas Biekotter Michela Biglietti Shalva Bilanishvili Deng Binglin Denis Bodrov Anton Bogomyagkov Serge Bondarenko Stewart Boogert Maarten Boonekamp Marcello Borri Angelo Bosotti Vincent Boudry Mohammed Boukidi Igor Boyko Ivanka Bozovic Giuseppe Bozzi Jean-Claude Brient Anastasiia Budzinskaya Masroor Bukhari Vladimir Bytev Giacomo Cacciapaglia Hua Cai Wenyong Cai Wujun Cai Yijian Cai Yizhou Cai Yuchen Cai Haiying Cai Huacheng Cai Lorenzo Calibbi Junsong Cang Guofu Cao Jianshe Cao Antoine Chance xuejun Chang Yue Chang Zhe Chang Xinyuan Chang Wei Chao Auttakit Chatrabhuti Yimin Che Yuzhi Che Bin Chen danping Chen Fuqing Chen Fusan Chen Gang Chen Guoming Chen Hua-Xing Chen Huirun Chen Jinhui Chen Ji-Yuan Chen Kai Chen Mali Chen Mingjun Chen Mingshui Chen Ning Chen Shanhong Chen Shanzhen Chen Shao-Long Chen Shaomin Chen Shiqiang Chen Tianlu Chen Wei Chen Xiang Chen Xiaoyu Chen Xin Chen xun Chen xurong Chen Ye Chen Ying Chen Yukai Chen Zelin Chen Zilin Chen Gang Chen Boping Chen Chunhui Chen Hok Chuen Cheng Huajie Cheng Shan Cheng Tongguang Cheng Yunlong Chi Pietro Chimenti Wen Han Chiu Guk Cho Ming-Chung Chu Xiaotong Chu Ziliang Chu Guglielmo Coloretti Andreas Crivellin Hanhua Cui Xiaohao Cui Zhaoyuan Cui Brunella D'Anzi Ling-Yun dai Xinchen dai xuwen dai Antonio De Maria Nicola De Filippis Christophe De La Taille Francesca De Mori Chiara De Sio Elisa Del Core Shuangxue Deng Wei-Tian Deng Zhi Deng Ziyan Deng Bhupal Dev Tang Dewen Biagio Di Micco Ran Ding Siqin Dingl Yadong Ding Haiyi Dong Jianing Dong Jing Dong Lan Dong Mingyi Dong xu Dong Yipei Dong Yubing Dong Milos Dordevic Marco Drewes Mingxuan Du Mingxuan Du Qianqian Du Xiaokang Du Yanyan Du Yong Du Yunfei Du Chun-Gui Duan Zhe Duan Yahor Dydyshka Ulrik Egede Walaa Elmetenawee Yun Eo Ka Yan Fan Kuanjun Fan Yunyun Fan Bo Fang Shuangshi Fang Yuquan Fang Ada Farilla Riccardo Farinelli Muhammad Farooq Angeles Faus Golfe Almaz Fazliakhmetov Rujun Fei Bo Feng Chong Feng Junhua Feng xu Feng Zhuoran Feng Zhuoran Feng Luis Roberto Flores Castillo Etienne Forest Andrew Fowlie Harald Fox Hai-Bing Fu Jinyu Fu Benjamin Fuks Yoshihiro Funakoshi Emidio Gabrielli Nan Gan Li Gang Jie Gao Meisen Gao Wenbin Gao Wenchun Gao Yu Gao Yuanning Gao Zhanxiang Gao Yanyan Gao Kun Ge Shao-Feng Ge Zhenwu Ge Li-Sheng Geng Qinglin Geng Chao-Qiang Geng Swagata Ghosh Antonio Gioiosa Leonid Gladilin Ti Gong Stefania Gori Quanbu Gou Sebastian Grinstein Chenxi Gu Gerardo Guillermo Joao Guimaraes da Costa Dizhou Guo Fangyi Guo Jiacheng Guo Jun Guo Lei Guo Lei Guo Xia Guo Xin-Heng Guo Xinyang Guo Yun Guo Yunqiang Guo Yuping Guo Zhi-Hui Guo Alejandro Gutierrez-Rodriguez Seungkyu Ha Noman Habib Jan Hajer Francois Hammer Chengcheng Han Huayong Han Jifeng Han Liang Han Liangliang Han Ruixiong Han Yang Han Yezi Han Yuanying Han Tao Han Jiankui Hao Xiqing Hao Xiqing Hao Chuanqi He dayong He Dongbing He Guangyuan He Hong-Jian He Jibo He Jun He Longyan He Xiang He Xiao-Gang He Zhenqiang He Klaus Heinemann Sven Heinemeyer Yuekun Heng Maria A.Hernandez-Ruiz Jiamin Hong Yuenkeung Hor George W.S.Hou Xiantao Hou Xiaonan Hou Zhilong Hou Suen Hou Caishi Hu Chen Hu dake Hu Haiming Hu Jiagen Hu Jun Hu Kun Hu Shouyang Hu Yongcai Hu Yu Hu Zhen Hu Zhehao Hua Jianfei Hua Chao-Shang Huang Fa Peng Huang Guangshun Huang Jinshu Huang Ke Huang Liangsheng Huang Shuhui Huang Xingtao Huang xu-Guang Huang Yanping Huang Yonggang Huang Yongsheng Huang Zimiao Huang Chen Huanyuan Changgi Hua Jiaqi Hui Lihua Huo Talab Hussain Kyuyeong Hwang Ara loannisian Munawar Iqbal Paul Jackson Shahriyar Jafarzade Haeun Jang Seoyun Jang daheng Ji Qingping Ji Quan Ji Xiaolu Ji Jingguang Jia Jinsheng Jia xuewei Jia Zihang Ja Cailian Jiang Han Ren Jiang Houbing Jiang Jun Jiang Xiaowei Jiang Xin Jiang xuhui Jiang Yongcheng Jiang Zhongjian Jiang Cheng Jiang Ruiqi Jiao dapeng Jin Shan Jin Song Jin Yi Jin Junji Jis Sunghoon Jung Goran Kacarevic Eric Kajfasz Lidia Kalinovskaya Aleksei Kampf Wen Kang Xian-Wei Kang Xiaolin Kang Biswajit Karmakar Zhiyong Ke Rijeesh Keloth Alamgir Khan Hamzeh Khanpour Khanchai Khosonthongkee KhanchaiKhosonthongkee Bobae Kim Dongwoon Kim Mi Ran Kim Minsuk Kim Sungwon Kim On Kim Michael Klasen Sanghyun Ko Ivan Koop Vitaliy Kornienko Bryan Kortman Gennady Kozlov Shiqing Kuang Mukesh Kumar Chia Ming Kuo Tsz Hong Kwok Fran cois Sylvain Ren Lagarde Pei-Zhu Lai Imad Laktineh Xiaofei Lan Zuxiu Lan Lia Lavezzi Justin Lee Junghyun Lee Sehwook Lee Ge Lei Roy Lemmon longxiang Leng Sze Ching Leung Hai Tao Li Bingzhi Li Bo Li Bo Li Changhong Li Chao Li Cheng Li Cheng Li Chunhua Li Cui Li dazhang Li Dikai Li Fei Li Gang Li Gang Li Gang Li Gaosong Li Haibo Li Haifeng Li Hai-Jun Li Haotian Li Hengne Li Honglei Li Huijing Li Jialin Li Jingyi Li Jinmian Li Jun Li Leyi Li Liang Li Ling Li Mei Li Meng Li Minxian Li Pei-Rong Li Qiang Li Shaopeng Li Shenghe Li Shu Li Shuo Li Teng Li Tiange Li Tong Li Weichang Li Weidong Li Wenjun Li Xiaoling Li Xiaomei Li Xiaonan Li Xiaoping Li Xiaoting Li Xin Li Xinqiang Li xuekang Li Yang Li Yanwei Li Yiming Li Ying Li Ying-Ying Li Yonggang Li Yonglin Li Yufeng Li Yuhui Li Zhan Li Zhao Li Zhiji Li Tong Li Lingfeng Li Fei Li Jing Liang Jinhan Liang Zhijun Liang Guangrui Liao Hean Liao Jiajun Liao Libo Liao Longzhou Liao Yi Liao Yipu Liao Ayut Limphirat AyutLimphirat Tao Lin Weiping Lin Yufu Lin Yugen Lin Beijiang Liu Bo Liu danning Liu Dong Liu Fu-Hu Liu Hongbang Liu Huangcheng Liu Hui Liu Huiling Liu Jia Liu Jia Liu Jiaming Liu Jianbei Liu Jianyi Liu Jingdong Liu Jinhua Liu Kai Liu Kang Liu Kun Liu Mengyao Liu Peng Liu Pengcheng Liu Qibin Liu Shan Liu Shidong Liu Shuang Liu Shubin Liu Tao Liu Tao Liu Tong Liu Wei Liu Xiang Liu Xiao-Hai Liu Xiaohui Liu Xiaoyu Liu Xin Liu Xinglin Liu Xingquan Liu Yang Liu Yanlin Liu Yao-Bei Liu Yi Liu Yiming Liu Yong Liu Yonglu Liu Yu Liu Yubin Liu Yudong Liu Yulong Liu Zhaofeng Liu Zhen Liu Zhenchao Liu Zhi Liu Zhi-Feng Liu Zhiqing Liu Zhongfu Liu Zuowei Liu Mia Liu Zhen Liu Xiaoyang Liu Xinchou Lou Cai-Dian Lu Jun-xu Lu Qiu Zhen Lu Shang Lu Shang Lu Wenxi Lu Xiaohan Lu Yunpeng Lu Zhiyong Lu Xianguo Lu Wei Lu Bayarto Lubsandorzhiev Sultim Lubsandorzhiev Arslan Lukanov Jinliang Luo Tao Luo xiaoan Luo Xiaofeng Luo Xiaolan Luo Jindong Lv Feng Lyu Xiao-Rui Lyu Kun-Feng Lyu Ande Ma Hong-Hao Ma Jun-Li Ma Kai Ma Lishuang Ma Na Ma Renjie Ma Weihu Ma Xinpeng Ma Yanling Ma Yan-Qing Ma Yongsheng Ma Zhonghui Ma Zhongjian Ma Yang Ma Mousam Maity Lining Mao Yanmin Mao Yaxian Mao Aure lien Martens Caccia Massimo Luigi Maria Shigeki Matsumoto Bruce Mellado davide Meloni Lingling Men Cai Meng Lingxin Meng Zhenghui Mi Yuhui Miao Mauro Migliorati Lei Ming Vasiliki A.Mitsou Laura Monaco Arthur Moraes Karabo Mosala Ahmad Moursy Lichao Mu Zhihui Mu Nickolai Muchnoi daniel Muenstermann danielMuenstermann Pankaj Munbodh William John Murray Jerome Nanni Dmitry Nanzanov Changshan Nie Sergei Nikitin Feipeng Ning Guozhu Ning Jia-Shu Niu Juan-Juan Niu Yan Niu Edward Khomotso Nkadimeng Kazuhito Ohmi Katsunobu Oide Hideki Okawa Mohamed Ouchemhou Qun Ouyang daniele Paesani Carlo Pagani Stathes Paganis Collette Pakuza Jiangyang Pan Juntong Pan Tong Pan Xiang Pan Papia Panda Saraswati Pandey Mila Pandurovic Rocco Paparella Roman Pasechnik Emilie Passemar r Hua Pei Xiaohua Peng Xinye Peng Yuemei Peng Jialun Ping Ronggang Ping Souvik Priyam Adhya Baohua Qi Hang Qi Huirong Qi Ming Qi Sen Qian Zhuoni Qian Congfeng Qiao Guangyou Qin Jiajia Qin Laishun Qin Liqing Qin Qin Qin Xiaoshuai Qin Zhonghua Qin Guofeng Qu Antonio Racioppi Michael Ramsey-Musolf Shabbar Raza Vladimir Rekovic Jing Ren Jirgen Reuter Tania Robens Giancarlo Rossi Manqi Ruan Manqi Ruan Leonid Rumyantsev Min Sang Ryu Renat Sadykov Minjing Sang Juan Jose Sanz-Cillero Miroslav Saur Nishil Savla Michael A.Schmidt daniele Sertore Ron Settles Peng Sha Ding-Yu Shao Ligang Shao Hua-Sheng Shao Xin She Chuang Shen Hong-Fei Shen Jian-Ming Shen Peixun Shen Qiuping Shen Zhongtao Shen Shuqi Sheng Haoyu Shi Hua Shi Qi Shi Shusu Shi Xiaolei Shi Xin Shi Yukun Shi Zhan Shi Ian Shipsey Gary Shiu Chang Shu Zong-Guo Si Andrei Sidorenkov Ivan Smiljanc Aodong Song Huayang Song Jiaojiao Song Jinxing Song Siyuan Song Weimin Song Weizheng Song Zhi Song Shashwat Sourav Paolo Spruzzola Feng Su Shengsen Su Wei Su Shufang Su Yanfeng Sui Zexuan Sui Michael Sullivan Baiyang Sun Guoqiang Sun Hao Sun Hao-Kai Sun Junfeng Sun Liang Sun Mengcheng Sunl Pengfei Sun Sichun Sun Xianjing Sun Xiaohu Sun Xilei Sun Xingyang Sun Xin-Yuan Sun Yanjun Sun Yongzhao Sun Yue Sun Zheng Sun Zheng Sun Narumon Suwonjandee Elsayed Tag Eldin Biao Tan Bo Tang Chuanxiang Tang Gao Tang Guangyi Tang Jian Tang Jingyu Tang Liang Tang Ying'Ao Tang Junquan Tao Abdel Nasser Taw fik Geoffrey Taylor Valery Telnov Saike Tian Riccardo Torre Wladyslaw Henryk Trzaska Dmitri Tsybychev Yanjun Tu Shengquan Tuo Michael Tytgat Ghalib Ul Islam Nikita Ushakov German Valencia Jaap Velthuis Alessandro Vicini Trevor Vickey Ivana Vidakovic Henri Videau Raymond Volkas Dmitry Voronin Natasa Vukasinovic Xia Wan xuying Wan Xiao Wang Anqing Wang Bin Wang Chengtao Wang Chuanye Wang Ci Wang dayong Wang Dou Wang En Wang Fei Wang Fei Wang Guanwen Wang Guo-Li Wang Haijing Wang Haolin Wang Jia Wang Jian Wang Jianchun Wang Jianli Wang Jiawei Wang Jin Wang Jin-Wei Wang Joseph Wang Kechen Wang Lechun Wang Lei Wang Liguo Wang Lijiao Wang Lu Wang Meng Wang Na Wang Pengcheng Wang Qian Wang Qun Wang Shu Lin Wang Shudong Wang Taofeng Wang Tianhong Wang Tianyang Wang Tong Wang Wei Wang Wei Wang Xiaolong Wang Xiaolong Wang Xiaoning Wang Xiao-Ping Wang Xiongfei Wang xujian Wang Yaping Wang Yaqian Wang Yi Wang Yiao Wang Yifang Wang Yilun Wang Yiwei Wang You-Kai Wang Yuanping Wang Yuexin Wang Yuhao Wang Yu-Ming Wang Yuting Wang Zhen Wang Zhigang Wang Weiping Wang Zeren Simon Wang Biao Wang Hui Wang Lian-Tao Wang Zihui Wang Zirui Wang Jia Wang Tong Wang daihui Wei Shujun Wei Wei Wei Xiaomin Wei Yuanyuan Wei Yingjie Wei Liangjian Wen xuejun Wen Yufeng Wen Martin White Peter Williams Zef Wolffs William John Womersley Baona Wu Bobing Wu Guanjian Wu Jinfei Wu Lei Wu Lina Wu Linghui Wu Minlin Wu Peiwen Wu Qi Wu Qun Wu Tianya Wu Xiang Wu Xiaohong Wu Xing-Gang Wu xuehui Wu Yaru Wu Yongcheng Wu Yuwen Wu Zhi Wu Xin Wu Lei Xia Ligang Xia Shang Xia Benhou Xiang dao Xiang Zhiyu Xiang Bo-Wen Xiao Chu-Wen Xiao Dong Xiao Guangyan Xiao Han Xiao Meng Xiao Ouzheng Xiao Rui-Qing Xiao Xiang Xiao Yichen Xiao Ying Xiao Yu Xiao Yunlong Xiao Zhenjun Xiao Hengyuan Xiao Nian Xie Yuehong Xie Tianmu Xin Ye Xing Zhizhong Xing da xu Fang xu Fanrong xu Haisheng xu Haocheng xu Ji xu Miaofu xu Qingjin xu Qingnian xu Wei xu Wei xu Weixi xu Xinping xu Zhen xu Zijun xu Zehua xu Yaoyuan xu Feifei xue Baojun Yan Bin Yan Fen Yan Fucheng Yan Jiaming Yan Liang Yan Luping Yan Qi-Shu Yan Wenbiao Yan Yupeng Yan Luping Yan Haoyue Yan Dong Yang Fengying Yang Guicheng Yang Haijun Yang Jin Min Yang Jing Yang Lan Yang Li Yang Li Lin Yang Lili Yang Litao Yang Mei Yang Qiaoli Yang Tiansen Yang Xiaochen Yang Yingjun Yang Yueling Yang Zhengyong Yang Zhenwei Yang Youhua Yang Xiancong Yang De-Liang Yao Shi Yao Lei Ye Lingxi Ye Mei Ye Rui Ye Rui Ye Yecheng Ye Vitaly Yermolchyk Kai Yi Li Yi Yang Yi Di Yin Peng-Fei Yin Shenghua Yin Ze Yin Zhongbao Yin Zhang Yinhong Hwi Dong Yoo Zhengyun You Charles Young Boxiang Yu Chenghui Yu Fusheng Yu Jie-Sheng Yu Jinqing Yu Lingda Yu Zhao-Huan Yu Felix Yu Bingrong Yu Changzheng Yuan Li Yuan Xing-Bo Yuan Youjin Yuan Junhui Yue Qian Yue Baobiao Yue Un Nisa Zaib Riccardo Zanzottera Hao Zeng Ming Zeng Jian Zhai Jiyuan Zhai Xin Zhe Zhai Xi-Jie Zhan Ben-Wei Zhang Bolun Zhang Di Zhang Guangyi Zhang Hao Zhang Hong-Hao Zhang Huaqiao Zhang Hui Zhang Jialiang Zhang Jianyu Zhang Jianzhong Zhang Jiehao Zhang Jielei Zhang Jingru Zhang Jinxian Zhang Junsong Zhang Junxing Zhang Lei Zhang Lei Zhang Liang Zhang Licheng Zhang Liming Zhang Linhao Zhang Luyan Zhang Mengchao Zhang Rao Zhang Shulei Zhang Wan Zhang Wenchao Zhang Xiangzhen Zhang Xiaomei Zhang Xiaoming Zhang Xiaoxu Zhang Xiaoyu Zhang xuantong Zhang xueyao Zhang Yang Zhang Yang Zhang Yanxi Zhang Yao Zhang Ying Zhang Yixiang Zhang Yizhou Zhang Yongchao Zhang Yu Zhang Yuan Zhang Yujie Zhang Yulei Zhang Yumei Zhang Yunlong Zhang Zhandong Zhang Zhaoru Zhang Zhen-Hua Zhang Zhenyu Zhang Zhichao Zhang Zhi-Qing Zhang Zhuo Zhang Zhiqing Zhang Cong Zhang Tianliang Zhang Luyan Zhang Guang Zhao Hongyun Zhao Jie Zhao Jingxia Zhao Jingyi Zhao Ling Zhao Luyang Zhao Mei Zhao Minggang Zhao Mingrui Zhao Qiang Zhao Ruiguang Zhao Tongxian Zhao Yaliang Zhao Ying Zhao Yue Zhao Zhiyu Zhao Zhuo Zhao Alexey Zhemchugov Hongjuan Zheng Jinchao Zheng Liang Zheng Ran Zheng shanxi zheng xu-Chang Zheng Wang Zhile Weicai Zhong Yi-Ming Zhong Chen Zhou daicui Zhou Jianxin Zhou Jing Zhou Jing Zhou Ning Zhou Qi-Dong Zhou Shiyu Zhou Shun Zhou Sihong Zhou Xiang Zhou Xingyu Zhou Yang Zhou Yong Zhou Yu-Feng Zhou Zusheng Zhou Demin Zhou Dechong Zhu Hongbo Zhu Huaxing Zhu Jingya Zhu Kai Zhu Pengxuan Zhu Ruilin Zhu Xianglei Zhu Yingshun Zhu Yongfeng Zhu Xiao Zhuang xuai Zhuang Mikhail Zobov Zhanguo Zong Cong Zou Hongying Zou 《Radiation Detection Technology and Methods》 CSCD 2024年第1期I0003-I0016,1-1091,共1105页
The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by China,fostered through extensive collaboration with international partners.The complex comprises four accelerators:a 3... The Circular Electron Positron Collider(CEPC)is a large scientific project initiated and hosted by China,fostered through extensive collaboration with international partners.The complex comprises four accelerators:a 30 GeV Linac,a 1.1 GeV Damping Ring,a Booster capable of achieving energies up to 180 GeV,and a Collider operating at varying energy modes(Z,W,H,and tt).The Linac and Damping Ring are situated on the surface,while the subterranean Booster and Collider are housed in a 100 km circumference underground tunnel,strategically accommodating future expansion with provisions for a potential Super Proton Proton Collider(SPPC).The CEPC primarily serves as a Higgs factory.In its baseline design with synchrotron radiation(SR)power of 30 MW per beam,it can achieve a luminosity of 5×10^(34)cm^(-2)s^(-1)per interaction point(IP),resulting in an integrated luminosity of 13 ab^(-1)for two IPs over a decade,producing 2.6 million Higgs bosons.Increasing the SR power to 50 MW per beam expands the CEPC's capability to generate 4.3 million Higgs bosons,facilitating precise measurements of Higgs coupling at sub-percent levels,exceeding the precision expected from the HL-LHC by an order of magnitude.This Technical Design Report(TDR)follows the Preliminary Conceptual Design Report(Pre-CDR,2015)and the Conceptual Design Report(CDR,2018),comprehensively detailing the machine's layout,performance metrics,physical design and analysis,technical systems design,R&D and prototyping efforts,and associated civil engineering aspects.Additionally,it includes a cost estimate and a preliminary construction timeline,establishing a framework for forthcoming engineering design phase and site selection procedures.Construction is anticipated to begin around 2027-2028,pending government approval,with an estimated duration of 8 years.The commencement of experiments and data collection could potentially be initiated in the mid-2030s. 展开更多
关键词 initiated EXCEEDING PRECISE
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The combination of PD-1 blockade with interferon-αhas a synergistic effect on hepatocellular carcinoma 被引量:14
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作者 Ying Zhu Mo Chen +9 位作者 da xu Tian-En Li Ze Zhang Jian-Hua Li Xiang-Yu Wang Xin Yang Lu Lu Hu-Liang Jia Qiong-Zhu Dong Lun-Xiu Qin 《Cellular & Molecular Immunology》 SCIE CAS CSCD 2022年第6期726-737,共12页
Background The efficacy of immune checkpoint inhibitors(ICIs),such as programmed cell death protein-1(PD-1)or its ligand 1(PD-L1)antibody,in hepatocellular carcinoma(HCC)is limited,and it is recommended that they be c... Background The efficacy of immune checkpoint inhibitors(ICIs),such as programmed cell death protein-1(PD-1)or its ligand 1(PD-L1)antibody,in hepatocellular carcinoma(HCC)is limited,and it is recommended that they be combined with other therapies.We evaluated the combination of pegylated interferon-α(Peg-IFNα)with PD-1 blockade in HCC mouse models.Methods We analyzed the effects of Peg-IFNαon tumor-infiltrating immune cells and PD-1 expression in the HCC immune microenvironment and examined the underlying mechanism of its unique effect on the PD-1 pathway.The in vivo efficacy of anti-PD-1 and Peg-IFNαwas evaluated in both subcutaneous and orthotopic mouse models of HCC.Results The combination of Peg-IFNαwith PD-1 blockade dramatically enhanced T-cell infiltration,improved the efficacy of PD-1 antibody and prolonged mouse survival compared with PD-1 antibody monotherapy.Mechanistically,Peg-IFNαcould recruit cytotoxic CD8+T cells to infiltrate the HCC microenvironment by inducing tumor cells to secrete the chemokine CCL4.Nevertheless,the HCC microenvironment quickly overcame the immune responses by upregulating PD-1 expression in CD8+T cells via the IFNα-IFNAR1-JAK1-STAT3 signaling pathway.The combination of PD-1 blockade with Peg-IFNαcould restore the cytotoxic capacity of CD8+T cells and exerted a significant synergistic effect on HCC.Conclusion These results indicate that in addition to initiating the antitumor immune response itself,Peg-IFNαcan also generate a microenvironment favoring PD-1 blockade.Thus,the combination of Peg-IFNαand PD-1 blockade can be a promising strategy for HCC. 展开更多
关键词 Hepatocellular carcinoma Tumor microenvironment PD-1 Pegylated interferon-α T-cell exhaustion
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Spontaneous T-symmetry breaking and exceptional points in cavity quantum electrodynamics systems 被引量:5
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作者 Yu-Kun Lu Pai Peng +4 位作者 Qi-Tao Cao da xu Jan wiersig Qihuang Gong Yun-Feng Xiao 《Science Bulletin》 SCIE EI CSCD 2018年第17期1096-1100,共5页
Spontaneous symmetry breaking has revolutionized the understanding in numerous fields of modern physics. Here, we theoretically demonstrate the spontaneous time-reversal symmetry breaking in a cavity quantum electrody... Spontaneous symmetry breaking has revolutionized the understanding in numerous fields of modern physics. Here, we theoretically demonstrate the spontaneous time-reversal symmetry breaking in a cavity quantum electrodynamics system in which an atomic ensemble interacts coherently with a single resonant cavity mode. The interacting system can be effectively described by two coupled oscillators with positive and negative mass, when the two-level atoms are prepared in their excited states. The occurrence of symmetry breaking is controlled by the atomic detuning and the coupling to the cavity mode,which naturally divides the parameter space into the symmetry broken and symmetry unbroken phases.The two phases are separated by a spectral singularity, a so-called exceptional point, where the eigenstates of the Hamiltonian coalesce. When encircling the singularity in the parameter space, the quasiadiabatic dynamics shows chiral mode switching which enables topological manipulation of quantum states. 展开更多
关键词 Exceptional point Spontaneous symmetry breaking Topological singularity Cavity QED
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Ultrathin-shell epitaxial Ag@Au core-shell nanowires for high-performance and chemically-stable electronic, optical, and mechanical devices 被引量:3
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作者 Yangzhi Zhu Sanggon Kim +12 位作者 xuezhi Ma Peter Byrley Ning Yu Qiushi Liu Xiaoming Sun da xu Sangshan Peng Martin C.Hartel Shiming Zhang Vadim Jucaud Mehmet R.Dokmeci Ali Khademhosseini Ruoxue Yan 《Nano Research》 SCIE EI CSCD 2021年第11期4294-4303,共10页
Silver nanowires (AgNWs) hold great promise for applications in wearable electronics, flexible solar cells, chemical and biological sensors, photonic/plasmonic circuits, and scanning probe microscopy (SPM) due to thei... Silver nanowires (AgNWs) hold great promise for applications in wearable electronics, flexible solar cells, chemical and biological sensors, photonic/plasmonic circuits, and scanning probe microscopy (SPM) due to their unique plasmonic, mechanical, and electronic properties. However, the lifetime, reliability, and operating conditions of AgNW-based devices are significantly restricted by their poor chemical stability, limiting their commercial potentials. Therefore, it is crucial to create a reliable oxidation barrier on AgNWs that provides long-term chemical stability to various optical, electrical, and mechanical devices while maintaining their high performance. Here we report a room-temperature solution-phase approach to grow an ultra-thin, epitaxial gold coating on AgNWs to effectively shield the Ag surface from environmental oxidation. The Ag@Au core-shell nanowires (Ag@Au NWs) remain stable in air for over six months, under elevated temperature and humidity (80 °C and 100% humidity) for twelve weeks, in physiological buffer solutions for three weeks, and can survive overnight treatment of an oxidative solution (2% H2O2). The Ag@Au core-shell NWs demonstrated comparable performance as pristine AgNWs in various electronic, optical, and mechanical devices, such as transparent mesh electrodes, surface-enhanced Raman spectroscopy (SERS) substrates, plasmonic waveguides, plasmonic nanofocusing probes, and high-aspect-ratio, high-resolution atomic force microscopy (AFM) probes. These Au@Ag core-shell NWs offer a universal solution towards chemically-stable AgNW-based devices without compromising material property or device performance. 展开更多
关键词 epitaxial growth core-shell nanowire plasmonic waveguides atomic force microscopy(AFM)probe transparent electrode wearable electronics
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The Epidemiological Characteristics of Pulmonary Tuberculosis——Kashgar Prefecture,Xinjiang Uygur Autonomous Region,China,2011-2020 被引量:14
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作者 Diermulati Tusun Maiweilanjiang Abulimiti +8 位作者 Xirizhati Mamuti Zhenjiang Liu da xu Guanzhen Li Xiaowang Peng Tuerhong Abudureyimu Lijie Zhang Yanlin Zhao Xichao Ou 《China CDC weekly》 2021年第26期557-561,共5页
Introduction:National Notifiable Disease Reporting System(NNDRS)plays an important role in the early detection and control of tuberculosis(TB)in China.This study analyzed the epidemiological characteristics of pulmona... Introduction:National Notifiable Disease Reporting System(NNDRS)plays an important role in the early detection and control of tuberculosis(TB)in China.This study analyzed the epidemiological characteristics of pulmonary tuberculosis(PTB)in Kashgar Prefecture,Xinjiang Uygur Autnomous Region,China from 2011 to 2020 to provide a scientific basis for developing TB control strategies and measures in Kashgar.Methods:The data were collected from the NNDRS,which included the geographical distribution,age,sex,occupation,and pathogenic classification of reported PTB cases in 12 counties/cities of Kashgar Prefecture from 2011 to 2020.Descriptive statistics were used to describe the characteristic of PTB epidemic in Kashgar.Results:There were 189,416 PTB cases reported during 2011–2020,with a mean annual PTB case notification rate(CNR)of 451.29/100,000.A rising trend in the rate of reported PTB between 2011 and 2017(χ2 trend=26.09,P<0.01)and a declining trend between 2018 and 2020(χ2 trend=314.44,P<0.01)were observed.The months with the highest reported number of PTB cases were March to May and November to December.The mean annual rate of reported PTB was 451.88/100,000 for males and 450.67/100,000 for females.In addition,19.76%of patients were bacteriologically-confirmed(Bac+)cases(37,425/189,416),and the mean annual Bac+CNR was 89.17/100,000,rising from 64.76/100,000 in 2011 to 139.12/100,000 in 2020(χ^(2)_(trend)=74.44,P<0.01).Conclusions:The CNR of reported PTB in Kashgar showed a significant declining trend in the past three years.Males,elderly population,winter and spring,and farmers as an occupation were the main factors associated with high incidence of tuberculosis in Kashgar.Targeted prevention and treatment of TB should be strengthened in key groups in this region. 展开更多
关键词 PREVENTION XINJIANG OCCUPATION
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A Compact Difference Scheme for an Evolution Equation with a Weakly Singular Kernel 被引量:2
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作者 Hongbin Chen da xu 《Numerical Mathematics(Theory,Methods and Applications)》 SCIE 2012年第4期559-572,共14页
This paper is concerned with a compact difference scheme with the truncation error of order 3/2 for time and order 4 for space to an evolution equation with a weakly singular kernel.The integral term is treated by mea... This paper is concerned with a compact difference scheme with the truncation error of order 3/2 for time and order 4 for space to an evolution equation with a weakly singular kernel.The integral term is treated by means of the second order convolution quadrature suggested by Lubich.The stability and convergence are proved by the energy method.A numerical experiment is reported to verify the theoretical predictions. 展开更多
关键词 Evolution equation weakly singular kernel compact difference scheme STABILITY CONVERGENCE numerical experiment
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Human U Three Protein 14a Expression is Increased in Hepatocellular Carcinoma and Associated with Poor Prognosis 被引量:2
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作者 Jing-Yi Zhang da xu +3 位作者 Zhen-Zhen Liu Yuan Li Li-Jun Wang Bao-Cai Xing 《Chinese Medical Journal》 SCIE CAS CSCD 2017年第4期470-476,共7页
Background: Human U three protein 14a (hUTP 14a) promotes p53 degradation. Moreover, hUTP 14a expression is upregulated in several types of tumors. However, the expression pattern of hUTP 14a in hepatocellular carc... Background: Human U three protein 14a (hUTP 14a) promotes p53 degradation. Moreover, hUTP 14a expression is upregulated in several types of tumors. However, the expression pattern of hUTP 14a in hepatocellular carcinoma (HCC) remains unknown. The aim of this study was to investigate hUTP 14a expression and its prognostic value in HCC. Methods: The hUTP 14a expression was evaluated using immunohistochemistry (IHC) in HCC tissue specimens. The correlations between hUTP 14a expression and clinicopathological variables were analyzed. The Kaplan-Meier method was used to analyze the association between hUTP14a expression and survival. Independent prognostic factors associated with overall survival (OS) and disease-free survival (DFS) were analyzed using the Cox proportional-hazards regression model. Results: The IHC data revealed that the hUTP 14a positivity rate in HCC tissue specimens was significantly higher than that in nontumorous tissue specimens (89.9% vs. 72.7%, P 〈 0,05). The hUTP14a expression was detected in both the nucleolus and the cytoplasm. The positivity rate of nucleolar hUTP14a expression in HCC tissue specimens was higher than that in the nontumorous tissue specimens (29.3% vs. 10.1%, P 〈 0.05). No significant difference was found between HCC and nontumorous tissue specimens of cytoplasmic hUTP 14a expression (60.6% vs. 62.6%, P 〉 0.05). In addition, no significant correlation was found between nucleolar hUTP 14a expression and other clinicopathological variables. The 5-year OS and DFS rates in patients with positive nucleolar hUTP14a expression were significantly lower than those in patients with negative hUTP 14a expression (P = 0.004 for OS, P = 0.003 for DFS). Multivariate analysis showed that nucleolar hUTP 14a expression was an independent prognostic factor for OS (P = 0.004) and DFS (P 〈 0.001 ). Conclusions: The positivity rate of hUTP 14a expression was significantly higher in HCC specimens. Positive expression of nucleolar hUTP 14a might act as a novel prognostic predictor for patients with HCC. 展开更多
关键词 Hepatocellular Carcinoma Human U Three Protein 14a Poor Prognosis
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