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Relations between SMBH Parameters and Jet Generation and Efficiency in Blazars 被引量:5
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作者 H.Zhang h.j.zhang 《Research in Astronomy and Astrophysics》 SCIE CAS CSCD 2023年第11期67-83,共17页
We analyzed the relationship between several basic parameters describing supermassive black holes such as jet power,black hole spin,accretion disk magnetic field,black hole mass,etc.We found that there is a general co... We analyzed the relationship between several basic parameters describing supermassive black holes such as jet power,black hole spin,accretion disk magnetic field,black hole mass,etc.We found that there is a general correlation between these parameters,such as jet power is significantly positively correlated with black hole spin,while black hole mass is significantly negatively correlated with black hole spin.To apprehend these relationships,we consider the Blandford–Znajek model to be superior to the Blandford–Payne model.It is also found that the intrinsic gamma luminosity of the FSRQs has a positive correlation with the accretion disk magnetic field,while the intrinsic gamma luminosity of the BL Lacs has a negative correlation with the accretion disk magnetic field.A feedback effect may exist between accretion disk accretion rate and magnetic field,which may be the key to the evolution between BL Lacs and FSRQs.There is no significant difference in the jet power and jet generation efficiency of FSRQs and BL Lacs,which suggests that the jets are generated by the same mechanism.The contribution rate of accretion rate to jet generation efficiency is high,while the contribution rate of accretion rate to jet power is very low. 展开更多
关键词 galaxies:evolution galaxies:fundamental parameters galaxies:jets
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Reducing the tension-compression yield asymmetry of extruded Mg-Zn-Ca alloy via equal channel angular pressing 被引量:11
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作者 L.B.Tong M.Y.Zheng +4 位作者 S.Kamado D.P.Zhang J.Meng L.R.Cheng h.j.zhang 《Journal of Magnesium and Alloys》 SCIE EI CAS 2015年第4期302-308,共7页
The influence of equal channel angular pressing on the tension-compression yield asymmetry of extruded Mg-5.3 Zn-0.6 Ca(weight percent)alloy has been investigated.The microstructure was obviously refined by the large ... The influence of equal channel angular pressing on the tension-compression yield asymmetry of extruded Mg-5.3 Zn-0.6 Ca(weight percent)alloy has been investigated.The microstructure was obviously refined by the large strain during the equal channel angular pressing,accompanied with very fine Ca_(2)Mg_(6)Zn_(3) phases with average diameter of 70 nm.The weak tension-compression yield asymmetry after equal channel angular pressing is mainly attributed to the reduced volume fraction of extension twinning during the compression,because the slope(k)of twinning in Hall-Petch relationship is higher than that of dislocation slip,and the twinning deformation is difficult to take place with decreasing grain size.The basal slip is more active in the alloy after equal channel angular pressing,due to the non-basal texture components,which hinders the twinning activation and reduces the yield asymmetry.Furthermore,the presence of fine precipitate restricts the twinning activation,which also contributes to the reduction of yield asymmetry. 展开更多
关键词 Mg-Zn-Ca alloy Yield asymmetry Equal channel angular pressing TWINNING PRECIPITATES
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A comparison study of Ce/La and Ca microalloying on the bio-corrosion behaviors of extruded Mg-Zn alloys 被引量:8
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作者 J.H.Chu L.B.Tong +4 位作者 Z.H.Jiang D.N.Zou Q.J.Wang S.F.Liu h.j.zhang 《Journal of Magnesium and Alloys》 SCIE EI CAS 2020年第4期1269-1280,共12页
The influences of Ca and Ce/La microalloying on the microstructure evolution and bio-corrosion resistances of extruded Mg-Zn alloys have been systematically investigated in the current study.Compared with single Ca or... The influences of Ca and Ce/La microalloying on the microstructure evolution and bio-corrosion resistances of extruded Mg-Zn alloys have been systematically investigated in the current study.Compared with single Ca or Ce/La addition,the Ca-Ce/La cooperative microalloying results in an outstanding grain refinement,because the fine secondary phase particles effectively hinder the recrystallized grain growth.The coarse Ca2Mg6Zn3 phases promote the formation of Ca3(PO4)2 or hydroxyapatite particles during the immersion process and accelerate the dissolution of the corrosion product film,which destroys its integrity and results in the deterioration of anti-corrosive performance.The Ce/La elements can be dispersed within the conventional Mg7Zn3 phases,which reduce the internal galvanic corrosion between Mg matrix and the secondary phases,leading to an obvious improvement of corrosion resistance.Therefore,the Ca-Ce/La cooperative microalloying achieves a homogenous fine-grained microstructure and improves the protective ability of surface film,which will pave a new avenue for the design of biomedical Mg alloys in the coming future. 展开更多
关键词 Extruded Mg-Zn alloy Ca and Ce/La microalloying Microstructure evolution Bio-corrosion behaviors
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伊豆—小笠原俯冲带板片的形态与形变研究
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作者 h.j.zhang F.Wang +3 位作者 R.Myhill H.Guo 刘思青(译) 常利军(校) 《世界地震译丛》 2020年第5期566-577,共12页
地震层析成像方法为俯冲板片的形态、形变与流变(间接)提供了独特的约束条件。本文利用远震双差P波成像技术对伊豆—小笠原板片的复杂结构进行了非常清晰的成像,结果显示位于26.5°N^28°N之间的地幔过渡带(MTZ)中存在一个板片... 地震层析成像方法为俯冲板片的形态、形变与流变(间接)提供了独特的约束条件。本文利用远震双差P波成像技术对伊豆—小笠原板片的复杂结构进行了非常清晰的成像,结果显示位于26.5°N^28°N之间的地幔过渡带(MTZ)中存在一个板片撕裂。撕裂以北,板片在MTZ发生折叠,在褶皱枢纽的正上方,剪切带内初期的黏性耗散形成了P波衰减区。撕裂以南,在MTZ底部板片发生翻转且平铺于MTZ的底部。2015年小笠原地震(M W约为7.9)的震源深度约为680km,该地震发生在翻转板片的最北端。伊豆—小笠原板片的局部撕裂、剪切和屈曲表明,其经过上地幔和地幔过渡带后仍然保持了较高的黏滞性。 展开更多
关键词 地震层析成像 地幔过渡带 震源深度 褶皱枢纽 俯冲带 剪切带 远震 上地幔
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高频波形匹配反演震源机制解及其在小震级诱发地震中的应用
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作者 J.L.Li h.j.zhang +4 位作者 H.S.Kuleli M.N.Toksoz 许鑫(译) 李振月(译) 万永革(校) 《世界地震译丛》 2020年第5期494-508,共15页
本文给出了一种利用稀疏地表台阵记录的高频全波形信息得到近震小震震源机制解的方法。波形反演中,除同时使观测波形与模拟波形之间震相和振幅的匹配度最大外,还利用了P波初动及平均S/P振幅比来更好地约束模拟和观测波形之间的匹配度。... 本文给出了一种利用稀疏地表台阵记录的高频全波形信息得到近震小震震源机制解的方法。波形反演中,除同时使观测波形与模拟波形之间震相和振幅的匹配度最大外,还利用了P波初动及平均S/P振幅比来更好地约束模拟和观测波形之间的匹配度。本文构建了一个包含四种约束的目标函数,并利用优化的网格搜索法在震源参数(走向、倾角和滑动角)的可能取值范围内搜索。为加快计算速度,预先计算了所有可能的震源位置上各地震矩张量分量对应的格林函数,形成一个格林函数库。另外对滤波和互相关部分进行了优化,以进一步加快网格搜索法。本文用由5个地表台站组成的用于监测油田诱发地震活动的台网对新方法进行了测试。人工实验的结果表明,仅使用3~9Hz频率范围的垂直向地震波分量来确定震源机制解时,新方法具有有效性和稳健性。将新方法应用于确定多个诱发地震事件的震源机制解,显示出观测和模拟地震波形之间较为满意的匹配度,并且大多数地震的走向与区域内NE-SW向的主断层平行。正断型震源机制占主要比例,表明垂直向应力大于水平向应力。 展开更多
关键词 震源观测 地震活动和构造 体波 波的传播
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STUDY ON PREPARATION, COMPLEX PERMITTIVITY,PERMEABILITY AND MICROWAVE PROPERTIES OF BaZnzCo(2-z)Fe16O27/SiO2 MICROCRYSTALLINE GLASS CERAMICS
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作者 h.j.zhang X.L.Jia +1 位作者 X.Yao L.Y.Zhang 《Acta Metallurgica Sinica(English Letters)》 SCIE EI CAS CSCD 2003年第6期421-427,共7页
BaZnzCo2-zFe16O27/SiO2 microcrystalline glass ceramics with Z=0.0, 0.5, 0.8 and 1.1 were prepared at temperature 1200℃ for 5h by citrate sol-gel process. The complex dielectric constant and complex permeability of Ba... BaZnzCo2-zFe16O27/SiO2 microcrystalline glass ceramics with Z=0.0, 0.5, 0.8 and 1.1 were prepared at temperature 1200℃ for 5h by citrate sol-gel process. The complex dielectric constant and complex permeability of BaZnzCo2-zFe16 O27/SiO2-paraffin wax composites had been measured. Both the complex dielectric constant and dielectric loss exhibit almost no variation with frequency in 0.1-6.0GHz. The real part of permeability decreases with increasing frequency for all samples, and the imaginary part of permeability exhibits a clear resonance peak at 1.44GHz for Co2 W/SiO2, 1.32GHz for Zn0.5Co1.5 W/SiO2, 1.20GHz for Zn0.8Co1.2W/SiO2, and 1.08GHz for Zn1.1 Co0.9 W/SiO2. It is also showed that the content of zinc has a close effect on the magnetic properties of BaZnzCo2-zFe16O27/SiO2 microcrystalline glass ceramics, the greater the zinc content, the higher the values of imaginary part of permeability and magnetic loss. 展开更多
关键词 BaZnz Co2-zFe16O27/SiO2 microcrystalline glass ceramics sol-gel microwave property
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中国四川省2008年汶川M S8.0地震区域三维速度结构
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作者 S.P.Pei J.R.Su +7 位作者 h.j.zhang Y.S.Sun M.N.Toksz Z.Wang X.Gao J.Liu-Zeng J.K.He 薛晓添 《世界地震译丛》 2018年第3期243-251,共9页
我们利用2008年汶川M_S8.0地震的余震给出了中国四川龙门山断裂带区域纵波速度(VP)、剪切波速度(VS)和波速比(VP/VS)的三维(3D)模型。该速度和波速比模型是利用双差地震层析成像程序的一个新版本tomoDDPS(Zhang,2003)获得的,这个版本可... 我们利用2008年汶川M_S8.0地震的余震给出了中国四川龙门山断裂带区域纵波速度(VP)、剪切波速度(VS)和波速比(VP/VS)的三维(3D)模型。该速度和波速比模型是利用双差地震层析成像程序的一个新版本tomoDDPS(Zhang,2003)获得的,这个版本可以同时反演VP,VS,VP/VS,以及地震的位置。用于反演的数据来自位于一个东北到西南长400km、西北到东南宽200km的区域内的63个固定台站和临时台站,包括了73 013条P波到时、62 287条S波到时,以及61 823条S-P波走时差。速度模型显示了沿着断层和穿过断层的不均匀性。总体而言,速度模型和当地地质特征一致,老的岩石波速高,而年轻的岩石波速低。龙门山断裂带是VP,VS和VP/VS的一个明显分界。基本上在15km以上,断层西部呈现高VP,VS和低VP/VS,对应着松潘—甘孜褶皱系;而在断层东部则呈现低VP,VS和高VP/VS,对应着四川盆地。沿着断层方向,速度结构和多个破裂滑移模型比较吻合,两个高速体恰好对应着两个较大滑移距离的区域。这显示了速度结构控制着沿断层面的滑移分布。 展开更多
关键词 汶川地震 双差层析成像 速度和波速比结构 余震
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STCF conceptual design report (Volume 1): Physics & detector 被引量:2
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作者 M.Achasov X.C.Ai +457 位作者 L.P.An R.Aliberti Q.An X.Z.Bai Y.Bai O.Bakina A.Barnyakov V.Blinov V.Bobrovnikov D.Bodrov A.Bogomyagkov A.Bondar I.Boyko Z.H.Bu F.M.Cai H.Cai J.J.Cao Q.H.Cao X.Cao Z.Cao Q.Chang K.T.Chao D.Y.Chen H.Chen H.X.Chen J.F.Chen K.Chen L.L.Chen P.Chen S.L.Chen S.M.Chen S.Chen S.P.Chen W.Chen X.Chen X.F.Chen X.R.Chen Y.Chen Y.Q.Chen H.Y.Cheng J.Cheng S.Cheng T.G.Cheng J.P.Dai L.Y.Dai X.C.Dai D.Dedovich A.Denig I.Denisenko J.M.Dias D.Z.Ding L.Y.Dong W.H.Dong V.Druzhinin D.S.Du Y.J.Du Z.G.Du L.M.Duan D.Epifanov Y.L.Fan S.S.Fang Z.J.Fang G.Fedotovich C.Q.Feng X.Feng Y.T.Feng J.L.Fu J.Gao Y.N.Gao P.S.Ge C.Q.Geng L.S.Geng A.Gilman L.Gong T.Gong B.Gou W.Gradl J.L.Gu A.Guevara L.C.Gui A.Q.Guo F.K.Guo J.C.Guo J.Guo Y.P.Guo Z.H.Guo A.Guskov K.L.Han L.Han M.Han X.Q.Hao J.B.He S.Q.He X.G.He Y.L.He Z.B.He Z.X.Heng B.L.Hou T.J.Hou Y.R.Hou C.Y.Hu H.M.Hu K.Hu R.J.Hu W.H.Hu X.H.Hu Y.C.Hu J.Hua G.S.Huang J.S.Huang M.Huang Q.Y.Huang W.Q.Huang X.T.Huang X.J.Huang Y.B.Huang Y.S.Huang N.Hüsken V.Ivanov Q.P.Ji J.J.Jia S.Jia Z.K.Jia H.B.Jiang J.Jiang S.Z.Jiang J.B.Jiao Z.Jiao H.J.Jing X.L.Kang X.S.Kang B.C.Ke M.Kenzie A.Khoukaz I.Koop E.Kravchenko A.Kuzmin Y.Lei E.Levichev C.H.Li C.Li D.Y.Li F.Li G.Li G.Li H.B.Li H.Li H.N.Li H.J.Li H.L.Li J.M.Li J.Li L.Li L.Li L.Y.Li N.Li P.R.Li R.H.Li S.Li T.Li W.J.Li X.Li X.H.Li X.Q.Li X.H.Li Y.Li Y.Y.Li Z.J.Li H.Liang J.H.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.Liao C.X.Lin D.X.Lin X.S.Lin B.J.Liu C.W.Liu D.Liu F.Liu G.M.Liu H.B.Liu J.Liu J.J.Liu J.B.Liu K.Liu K.Y.Liu K.Liu L.Liu Q.Liu S.B.Liu T.Liu X.Liu Y.W.Liu Y.Liu Y.L.Liu Z.Q.Liu Z.Y.Liu Z.W.Liu I.Logashenko Y.Long C.G.Lu J.X.Lu N.Lu Q.F.Lü Y.Lu Y.Lu Z.Lu P.Lukin F.J.Luo T.Luo X.F.Luo Y.H.Luo H.J.Lyu X.R.Lyu J.P.Ma P.Ma Y.Ma Y.M.Ma F.Maas S.Malde D.Matvienko Z.X.Meng R.Mitchell A.Nefediev Y.Nefedov S.L.Olsen Q.Ouyang P.Pakhlov G.Pakhlova X.Pan Y.Pan E.Passemar Y.P.Pei H.P.Peng L.Peng X.Y.Peng X.J.Peng K.Peters S.Pivovarov E.Pyata B.B.Qi Y.Q.Qi W.B.Qian Y.Qian C.F.Qiao J.J.Qin J.J.Qin L.Q.Qin X.S.Qin T.L.Qiu J.Rademacker C.F.Redmer H.Y.Sang M.Saur W.Shan X.Y.Shan L.L.Shang M.Shao L.Shekhtman C.P.Shen J.M.Shen Z.T.Shen H.C.Shi X.D.Shi B.Shwartz A.Sokolov J.J.Song W.M.Song Y.Song Y.X.Song A.Sukharev J.F.Sun L.Sun X.M.Sun Y.J.Sun Z.P.Sun J.Tang S.S.Tang Z.B.Tang C.H.Tian J.S.Tian Y.Tian Y.Tikhonov K.Todyshev T.Uglov V.Vorobyev B.D.Wan B.L.Wang B.Wang D.Y.Wang G.Y.Wang G.L.Wang H.L.Wang J.Wang J.H.Wang J.C.Wang M.L.Wang R.Wang R.Wang S.B.Wang W.Wang W.P.Wang X.C.Wang X.D.Wang X.L.Wang X.L.Wang X.P.Wang X.F.Wang Y.D.Wang Y.P.Wang Y.Q.Wang Y.L.Wang Y.G.Wang Z.Y.Wang Z.Y.Wang Z.L.Wang Z.G.Wang D.H.Wei X.L.Wei X.M.Wei Q.G.Wen X.J.Wen G.Wilkinson B.Wu J.J.Wu L.Wu P.Wu T.W.Wu Y.S.Wu L.Xia T.Xiang C.W.Xiao D.Xiao M.Xiao K.P.Xie Y.H.Xie Y.Xing Z.Z.Xing X.N.Xiong F.R.Xu J.Xu L.L.Xu Q.N.Xu X.C.Xu X.P.Xu Y.C.Xu Y.P.Xu Y.Xu Z.Z.Xu D.W.Xuan F.F.Xue L.Yan M.J.Yan W.B.Yan W.C.Yan X.S.Yan B.F.Yang C.Yang H.J.Yang H.R.Yang H.T.Yang J.F.Yang S.L.Yang Y.D.Yang Y.H.Yang Y.S.Yang Y.L.Yang Z.W.Yang Z.Y.Yang D.L.Yao H.Yin X.H.Yin N.Yokozaki S.Y.You Z.Y.You C.X.Yu F.S.Yu G.L.Yu H.L.Yu J.S.Yu J.Q.Yu L.Yuan X.B.Yuan Z.Y.Yuan Y.F.Yue M.Zeng S.Zeng A.L.Zhang B.W.Zhang G.Y.Zhang G.Q.Zhang h.j.zhang H.B.Zhang J.Y.Zhang J.L.Zhang J.Zhang L.Zhang L.M.Zhang Q.A.Zhang R.Zhang S.L.Zhang T.Zhang X.Zhang Y.Zhang Y.J.Zhang Y.X.Zhang Y.T.Zhang Y.F.Zhang Y.C.Zhang Y.Zhang Y.Zhang Y.M.Zhang Y.L.Zhang Z.H.Zhang Z.Y.Zhang Z.Y.Zhang H.Y.Zhao J.Zhao L.Zhao M.G.Zhao Q.Zhao R.G.Zhao R.P.Zhao Y.X.Zhao Z.G.Zhao Z.X.Zhao A.Zhemchugov B.Zheng L.Zheng Q.B.Zheng R.Zheng Y.H.Zheng X.H.Zhong H.J.Zhou H.Q.Zhou H.Zhou S.H.Zhou X.Zhou X.K.Zhou X.P.Zhou X.R.Zhou Y.L.Zhou Y.Zhou Y.X.Zhou Z.Y.Zhou J.Y.Zhu K.Zhu R.D.Zhu R.L.Zhu S.H.Zhu Y.C.Zhu Z.A.Zhu V.Zhukova V.Zhulanov B.S.Zou Y.B.Zuo 《Frontiers of physics》 SCIE CSCD 2024年第1期1-154,共154页
The superτ-charm facility(STCF)is an electron–positron collider proposed by the Chinese particle physics community.It is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of... The superτ-charm facility(STCF)is an electron–positron collider proposed by the Chinese particle physics community.It is designed to operate in a center-of-mass energy range from 2 to 7 GeV with a peak luminosity of 0.5×10^(35) cm^(–2)·s^(–1) or higher.The STCF will produce a data sample about a factor of 100 larger than that of the presentτ-charm factory—the BEPCII,providing a unique platform for exploring the asymmetry of matter-antimatter(charge-parity violation),in-depth studies of the internal structure of hadrons and the nature of non-perturbative strong interactions,as well as searching for exotic hadrons and physics beyond the Standard Model.The STCF project in China is under development with an extensive R&D program.This document presents the physics opportunities at the STCF,describes conceptual designs of the STCF detector system,and discusses future plans for detector R&D and physics case studies. 展开更多
关键词 electron–positron collider tau-charm region high luminosity STCF detector conceptual design
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Passive Q-switching and Q-switched mode-locking operations of 2 μm Tm:CLNGG laser with MoS2 saturable absorber mirror 被引量:17
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作者 L.C.Kong G.Q.Xie +4 位作者 P.Yuan L.J.Qian S.X.Wang H.H.Yu h.j.zhang 《Photonics Research》 SCIE EI 2015年第2期47-50,共4页
With MoS2 as saturable absorber, passive Q-switching and Q-switched mode-locking operations of a Tm-doped calcium lithium niobium gallium garnet(Tm:CLNGG) laser were experimentally demonstrated. The Q-switched laser... With MoS2 as saturable absorber, passive Q-switching and Q-switched mode-locking operations of a Tm-doped calcium lithium niobium gallium garnet(Tm:CLNGG) laser were experimentally demonstrated. The Q-switched laser emitted a maximum average output power of 62 mW and highest pulse energy of 0.72 μJ. Q-switched mode locking was also obtained in the experiment. The research results will open up applications of MoS2 at the mid-infrared wavelength. 展开更多
关键词 mode RATE m Tm:CLNGG laser with MoS2 saturable absorber mirror Passive Q-switching and Q-switched mode-locking operations of 2 TM
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