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肾髓质过表达鞘氨醇1-磷酸受体1转基因可减轻醋酸脱氧皮质酮-盐诱导的高血压

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中华高血压杂志(中英文) 2024年第8期 800-800页

作者： Hu G Xie DP chen c Wang WL Li PL Ritter JK Li NJ 袁源练桂丽

前期研究表明,肾髓质鞘氨醇1-磷酸受体1(sphingosine-1-phosphate receptor 1,S1PR1)介导钠排泄,高盐摄入可增加S1PR1水平,醋酸脱氧皮质酮(deoxycorticosterone acetate,DOcA)可阻断高盐诱导的肾髓质S1PR1,在集合管中敲除S1PR1可加重DOcA盐诱导的高血压。该研究验证在肾髓质中过表达S1PR1基因是否可减轻DOcA-盐小鼠模型的钠潴留和高血压。方法:给雄性c57BL/6J小鼠肾髓质转染对照或表达S1PR1的质粒后予DOcA-盐处理。

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嗜铬细胞瘤和副神经节瘤的系统性放射性药物治疗

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中华核医学与分子影像杂志 2024年第3期44卷 187-192页

作者：席闯(译) 罗全勇(审校) 上海交通大学医学院附属第六人民医院上海200233

良性嗜铬细胞瘤和副神经节瘤通常可以通过手术切除治愈,但转移性疾病的治疗在疾病控制和症状控制方面都存在挑战。幸运的是,有几种治疗方式可用于转移性疾病的治疗,包括化疗、放射治疗和外科手术。放射性核素标记的间碘苄胍(MIBG)和生... 详细信息

良性嗜铬细胞瘤和副神经节瘤通常可以通过手术切除治愈,但转移性疾病的治疗在疾病控制和症状控制方面都存在挑战。幸运的是,有几种治疗方式可用于转移性疾病的治疗,包括化疗、放射治疗和外科手术。放射性核素标记的间碘苄胍(MIBG)和生长抑素受体显像为将这些放射性药物用作诊疗剂奠定了基础。^(131)I-MIBG治疗神经内分泌肿瘤历史悠久,美国食品与药品监督管理局最近批准将高比活度^(131)I-MIBG用于治疗转移性或不可手术的嗜铬细胞瘤或副神经节瘤,使^(131)I-MIBG的治疗应用更加广泛,并重新引起人们的兴趣。尽管已有文献报道使用90Y-或177Lu-1,4,7,10-四氮杂环十二烷-1,4,7,10-四乙酸(DOTA)偶联的生长抑素类似物对嗜铬细胞瘤和副神经节瘤进行多肽受体放射性核素治疗,但随着177Lu-DOTA-D-苯丙氨酸1-酪氨酸3-苏氨酸8-奥曲肽(DOTATATE)在美国和欧洲获批,以及美国国家综合癌症网络指南建议将其用于转移性或不可手术的嗜铬细胞瘤和副神经节瘤患者,这些药物引起了人们新的兴趣。已有证据表明这些放射性药物是对转移性或无法手术的嗜铬细胞瘤或副神经节瘤患者有效的姑息治疗方法。在该篇继续医学教育文章中,作者讨论了使用^(131)I-MIBG和90Y-或177Lu-DOTA生长抑素类似物治疗嗜铬细胞瘤和副神经节瘤。

关键词：嗜铬细胞瘤副神经节瘤生长抑素 MIBG DOATATE 多肽受体放射性核素治疗

Reduced non-cpG methylation is a potential epigenetic target after spinal cord injury

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Neural Regeneration Research 2023年第11期18卷 2489-2496页

作者： Zhourui Wu chen Li Ran Zhu Yiqiu cao Thomas c.chen Liming cheng Key Laboratory of Spine and Spinal cord Injury Repair and Regeneration(Tongji University) Ministry of EducationShanghaiChina Division of Spine Department of OrthopedicsTongji HospitalTongji University School of MedicineShanghaiChina Institute of Spinal and Spinal cord Injury Tongji University School of MedicineShanghaiChina Department of Neurosurgery Keck School of MedicalUniversity of Southern CaliforniaLos AngelesCAUSA

DNA methylation is a critical epigenetic regulator in the occurrence and development of diseases and is closely related to various functional responses in relation to spinal cord *** investigate the role of DNA methylation in spinal cord injury,we constructed a library with reduced-representation bisulfite sequencing data obtained at various time points(day 0-42)after spinal cord injury in *** DNA methylation levels,specifically non-cpG(cHG and cHH)methylation levels,decreased modestly following spinal cord *** post-spinal cord injury were classified as early(day 0-3),intermediate(day7-14),and late(day 28-42)based on similarity and hie rarchical cluste ring of global DNA methylation *** non-cpG methylation level,which included cHG and cHH methylation levels,was markedly reduced despite accounting for a minor proportion of total methylation *** multiple genomic sites,including the 5’untranslated regions,promoter,exon,intron,and 3’untranslated regions,the non-cpG methylation level was markedly decreased following spinal cord injury,whereas the cpG methylation level remained unchanged at these *** one-half of the differentially methylated regions were located in intergenic areas;the other differentially methylated regions in both cpG and non-cpG regions were cluste red in intron regions,where the DNA methylation level was *** function of genes associated with differentially methylated regions in promoter regions was also *** Gene Ontology analysis results,DNA methylation was implicated in a number of essential functional responses to spinal cord injury,including neuronal synaptic connection creation and axon ***,neither cpG methylation nor non-cpG methylation was implicated in the functional response of glial or inflammatory *** summary,our work elucidated the dynamic pattern of DNA methylation in the spinal co rd following injury and identified reduced noncpG meth

关键词： cpG methylation cytosine fraction differentially methylated regions DNA methylation DNA methyltransferases dynamic signatures Gene Ontology non-cpG methylation single-cell RNA-Seq spinal cord injury

Effects of layer interactions on instantaneous stability of finite Stokes flows

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Applied Mathematics and Mechanics(English Edition) 2024年第1期45卷 69-84页

作者： chen ZHAO Zhenli chen c.T.MUTASA Dong LI School of Aeronautics Northwestern Polytechnical UniversityXi'an 710072China

The stability analysis of a finite Stokes layer is of practical importance in flow control. In the present work, the instantaneous stability of a finite Stokes layer with layer interactions is studied via a linear stability analysis of the frozen phases of the base flow. The oscillations of two plates can have different velocity amplitudes, initial phases, and frequencies. The effects of the Stokes-layer interactions on the stability when two plates oscillate synchronously are analyzed. The growth rates of two most unstable modes when δ ckness and the half height of the channel, respectively. However, their vorticities are different. The vorticity of the most unstable mode is symmetric, while the other is asymmetric. The Stokes-layer interactions have a destabilizing effect on the most unstable mode when δ ct when δ > 0.68. However, the interactions always have a stabilizing effect on the other unstable mode. It is explained that one of the two unstable modes has much higher dissipation than the other one when the Stokes-layer interactions are strong. We also find that the stability of the Stokes layer is closely related to the inflectional points of the base-flow velocity profile. The effects of inconsistent velocity-amplitude, initial phase, and frequency of the oscillations on the stability are analyzed. The energy of the most unstable eigenvector is mainly distributed near the plate of higher velocity amplitude or higher oscillation frequency. The effects of the initial phase difference are complicated because the base-flow velocity is extremely sensitive to the initial phase.

关键词： finite Stokes layer instantaneous stability Stokes-layer interaction asynchronous oscillation

Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)

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chinese Physics c 2024年第8期48卷 6-33页

作者： M.Ablikim M.N.Achasov P.Adlarson O.Afedulidis X.c.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina I.Balossino Y.Ban H.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann H.cai X.cai A.calcaterra G.F.cao N.cao S.A.cetin J.F.chang W.L.chang G.R.che G.chelkov c.chen c.H.chen chao chen G.chen H.S.chen M.L.chen S.J.chen S.L.chen S.M.chen T.chen X.R.chen X.T.chen Y.B.chen Y.Q.chen Z.J.chen Z.Y.chen S.K.choi X.chu G.cibinetto F.cossio J.J.cui H.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich c.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici c.Q.Feng J.H.Feng Y.T.Feng K.Fischer M.Fritsch c.D.Fu J.L.Fu Y.W.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge c.Geng E.M.Gersabeck B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.c.Du S.X.Du Z.H.Duan P.Egorov Y.H.Fan J.Fang JA.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.H.Gu Y.T.Gu c.Y.Guan Z.L.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.Han T.T.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius c.H.Heinz Y.K.Heng c.Herold T.Holtmann P.c.Hong G.Y.Hou X.T.Hou Y.R.Hou Z.L.Hou B.Y.Hu H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang X.T.Huang Y.P.Huang T.Hussain F.H\"olzken N.H\"usken N.in der Wiesche M.Irshad J.Jackson S.Janchiv J.H.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang H.B.Jiang P.c.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.c.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui A.Kupsc W.K\"uhn J.J.Lane P.Larin L.Lavezzi T.T.Lei Z.H.Lei H.Leithoff M.Lellmann T.Lenz c.Li c.Li c.H.Li cheng Li D.M.Li F.Li G.Li H.Li H.B.Li H.J.Li H.N.Li Hui Li J.R.Li J.S.Li K.Li L.J.Li L.K.Li Lei Li M.H.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li W.D.Li W.G.Li X.Li X.H.Li X.L.Li X.Y.Li Y Institute of High Energy Physics Chinese Academy of SciencesBeijing 100049China Beihang University Beijing 100191China Bochum Ruhr-University D-44780 BochumGermany Budker Institute of Nuclear Physics SB RAS(BINP) Novosibirsk 630090Russia carnegie Mellon University PittsburghPennsylvania 15213USA central china Normal University Wuhan 430079China central South University Changsha 410083China china center of Advanced Science and Technology Beijing 100190China china University of Geosciences Wuhan 430074China chung-Ang University Seoul06974Republic of Korea cOMSATS University Islamabad Lahore CampusDefence RoadOff Raiwind Road54000 LahorePakistan Fudan University Shanghai 200433China GSI Helmholtzcentre for Heavy Ion Research GmbH D-64291 DarmstadtGermany Guangxi Normal University Guilin 541004China Guangxi University Nanning 530004China Hangzhou Normal University Hangzhou 310036China Hebei University Baoding 071002China Helmholtz Institute Mainz Staudinger Weg 18D-55099 MainzGermany Henan Normal University Xinxiang 453007China Henan University Kaifeng 475004China Henan University of Science and Technology Luoyang 471003China Henan University of Technology Zhengzhou 450001China Huangshan college Huangshan 245000China Hunan Normal University Changsha 410081China Hunan University Changsha 410082China Indian Institute of Technology Madras Chennai 600036India Indiana University BloomingtonIndiana 47405USA INFN Laboratori Nazionali di Frascati INFN Laboratori Nazionali di FrascatiI-00044FrascatiItaly INFN Laboratori Nazionali di Frascati INFN Sezione di PerugiaI-06100PerugiaItaly INFN Laboratori Nazionali di Frascati University of PerugiaI-06100PerugiaItaly INFN Sezione di Ferrara INFN Sezione di FerraraI-44122FerraraItaly INFN Sezione di Ferrara University of FerraraI-44122FerraraItaly Inner Mongolia University Hohhot 010021China Institute of Modern Physics Lanzhou 730000China Institute of Physics and Technology Peace Avenue 54BUlaanbaatar 13330Mongolia Instituto de A

Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1)(1260)π,D^(0)→π(1300)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both *** the obtained amplitude model,the cP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1_(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,*** branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.010_(stat.)±0.010_(syst.))%and(0.951±0.025_(stat.)±0.021_(syst.))%,*** amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the cKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay.

关键词： BESIII D^(0)meson decays amplitude analysis cP-even fraction

Reduction effect of final-pass heavy reduction rolling on the texture development,tensile property and stretch formability of ZWK100 alloy plates

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Journal of Materials Science & Technology 2022年第16期111卷 211-223页

作者： B.Q.Shi L.Y.Zhao X.L.Shang B.H.Nie D.c.chen c.Q.Li Y.Q.cheng School of Materials Science and Hydrogen Energy Foshan UniversityFoshan 528000China School of Materials and Energy Guangdong University of TechnologyGuangzhouGuangdong 510006China GD Midea Air-conditioning Equipment co. Ltd.Foshan 528311China Guangdong Key Laboratory of Hydrogen Energy Technology Foshan 528000China YunFu(Foshan)R&D center of Hydrogen Energy Standardization Yunfu 527326China

Obviously planar anisotropy due to‘TD split’orthotropic texture(TD indicates Transverse direction)always exist in the Rare-earth(RE)or ca containing Mg alloy sheets,which is likely caused by the lowreduction rolling(and annealing)as revealed in our previous *** this work,the as-cast billets of a ZWK100 alloy were subjected to final-pass heavy reduction rolling(FHRR)at 500°c with different reductions(30%-70%)after rough rolling,aiming to investigate the reduction effect on the microstructure and texture *** results show that FHRR with higher reductions above 50%is in favor of shear banding formation but has little effect on the as-deformed texture components,and the excellent formability with single-pass reduction up to 70%is mainly ascribed to the activation of prismatic *** with reduction above 50%and annealing can generate uniform grain structures of~10μm and symmetrical‘oblique-line split’texture in(0001)pole figures,with basal poles tilting by about 50°from ND(Normal direction)towards some oblique-line of TD and RD(Rolling direction)as well as uniform distribution of counter lines as an annular shape,resulting in excellent elongation to failure of~50%and ultra-low planar anisotropyΔr_of~0.1 and high stretch formability(Erichsen value:8.1).The formation‘oblique-line split’texture in(0001)pole figures is mainly correlated with the preferred growth tendency of grains with■//RD,which was suggested to relate to the high mobility of some special boundaries such as 40°-45°■.The influences of starting textures on the mechanical properties,planar anisotropy and related deformation modes,as well as their correlations with the stretch formability were comparatively investigated with the‘TD split’orthotropic texture as a counterpoint.

关键词： Magnesium alloys Texture Plane anisotropy Stretch formability Rolled sheets

cu对含Sn铁素体不锈钢的力学及耐腐蚀性能的影响

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特殊钢 2024年第3期45卷 49-55页

作者：李阳陈常勇方勇马帅张咪娜姜周华东北大学冶金学院沈阳110819 香港理工大学工业与系统工程系中国香港999077 中国科学院宁波材料技术与工程研究所宁波315201

以0.30%Sn的430铁素体不锈钢为基础,在实验钢中添加一定量的cu来研究cu对实验钢力学性能和耐腐蚀性能的影响。常温拉伸实验和高温拉伸实验结果表明,cu原子在基体中发挥固溶强化效果而增强不锈钢的抗拉强度,但同时因晶界处生成大量的富c... 详细信息

以0.30%Sn的430铁素体不锈钢为基础,在实验钢中添加一定量的cu来研究cu对实验钢力学性能和耐腐蚀性能的影响。常温拉伸实验和高温拉伸实验结果表明,cu原子在基体中发挥固溶强化效果而增强不锈钢的抗拉强度,但同时因晶界处生成大量的富cu相而相应降低不锈钢的塑性。实验钢的耐均匀腐蚀性能随着cu含量的增加而呈现先提高,后降低的趋势,且在含0.45%cu的钢中达到最佳的效果。此外,cu对实验钢的耐晶间腐蚀性能有类似的规律,且在含0.98%cu的钢中达到最佳的效果。

关键词：锡铜铁素体不锈钢力学性能耐腐蚀性能

Dynamic Event-Triggered consensus control for Input constrained Multi-Agent Systems With a Designable Minimum Inter-Event Time

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IEEE/cAA Journal of Automatica Sinica 2024年第3期11卷 649-660页

作者： Meilin Li Yue Long Tieshan Li Hongjing Liang c.L.Philip chen the School of Automation Engineering University of Electronic Science and Technology of ChinaChengdu 611731China IEEE the Yangtze Delta Region Institute University of Electronic Science and Technology of ChinaHuzhou 313000 the Laboratory of Electromagnetic Space cognition and Intelligent control Beijing 100089China the School of computer Science and Engineering South China University of TechnologyGuangzhou 510006

This paper investigates the consensus control of multi-agent systems(MASs) with constrained input using the dynamic event-triggered mechanism(ETM).consider the MASs with small-scale networks where a centralized dynamic ETM with global information of the MASs is first ***,a distributed dynamic ETM which only uses local information is developed for the MASs with large-scale *** is shown that the semi-global consensus of the MASs can be achieved by the designed bounded control protocol where the Zeno phenomenon is eliminated by a designable minimum inter-event *** addition,it is easier to find a trade-off between the convergence rate and the minimum inter-event time by an adjustable ***,the results are extended to regional consensus of the MASs with the bounded control *** simulations show the effectiveness of the proposed approach.

关键词： constrained input designable minimum inter-event time directed communication topology dynamic event-triggered mechanism MASs consensus control

Deposition law of flat fan nozzle for pesticide application in horticultural plants

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International Journal of Agricultural and Biological Engineering 2022年第4期15卷 27-38页

作者： Xiaoyi Wu Yalan Jia Bo Luo chongchong chen Yaxiong Wang Feng Kang Jiale Li School of Technology Beijing Forestry UniversityKey Lab of State Forestry Administration for Forestry Equipment and AutomationBeijing100083China Army Aviation Institute Beijing 101123China

Pesticide spraying is to protect the plants with adequate target coverage and a minimum of off-target *** the spatial distribution characteristics of spray droplets is essential for regulating pesticide deposition,in order to investigate the relationship between the two at the mechanistic level and provide an accurate basis for nozzle selection,this study compared the characteristics of the atomization field under different pressures,angles,and flow rate types by phase Doppler particle analyzer(PDPA),the unit spatial density of droplet was used as a link to explore the internal mechanism that affects the deposition efficiency by constructing a transport model and conducting actual spraying *** results showed that the cumulative distribution of droplet diameter could be perfectly fitted by the Rosin-Rammler correlation,and the deposition efficiency had a strong correlation with the peak particle size *** strawberry and chrysanthemum plants,the optimal droplet deposition particle size ranges were 250-270μm and 240-260μm,*** article explained the deposition efficiency from a single droplet dynamics mechanism and deposition of droplet cloud,which provided a new research idea for the study of precision plant protection.

关键词： pesticide transport deposition atomization field PDPA