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Microstructure evolution and shape memory behaviors of Ni_(47)Ti_(44)Nb_(9)alloy subjected to multistep thermomechanical loading with different prestrain levels 被引量:3
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作者 Y.H.Zhang h.li +2 位作者 Z.W.Yang X.Liu Q.F.Gu 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2024年第4期80-93,共14页
Ni_(47)Ti_(44)Nb_(9)shape memory alloy(SMA)is a promising material in the aerospace field due to its wide transformation hysteresis.The application of shape memory effect depends on multistep thermomechan-ical loading... Ni_(47)Ti_(44)Nb_(9)shape memory alloy(SMA)is a promising material in the aerospace field due to its wide transformation hysteresis.The application of shape memory effect depends on multistep thermomechan-ical loading,viz.,low-temperature deformation and subsequent heating to recovery.Low-temperature deformation prestrain plays a pivotal role in shape memory properties tailoring of SMA components.However,microstructure evolution and deformation mechanisms of Ni_(47)Ti_(44)Nb_(9)SMA subjected to vari-ous prestrain levels are still unclear.To this end,microstructure evolution and shape memory behaviors of Ni_(47)Ti_(44)Nb_(9)alloy subjected to multistep thermomechanical loading with prestrain levels of 8%-16%at-28℃(M_(s)+30℃)were investigated.The results demonstrate that the stress-strain curve of the specimen exhibits four distinct stages at a maximal prestrain of 16%.Whereas stageⅡand stageⅢend at prestrains of∼8%and∼12%,respectively.In stageⅡ,the stress-induced martensitic transformation is accompanied by the dislocation slip of the NiTi matrix andβ-Nb inclusions.In stageⅢ,in addition to the higher density of dislocations and further growth of stress-induced martensite variants(SIMVs),(001)compound twins are introduced as a result of the(001)deformation twinning in stress-induced martensite.More{20-1}martensite twins are gradually introduced in stageⅣ.Correspondingly,after subsequent unloading and heating,a higher density of{114}austenite twins form in the specimen with a larger prestrain of 16%.With increasing prestrain from 8%to 16%,the recoverable strainε_(re)^(T)upon heating increases first and then decreases.Theε_(re)^(T)obtains a maximum of 7.03%at 10%prestrain and de-creases to 6.17%at 16%prestrain.The increase ofε_(re)^(T)can be attributed to the formation of new SIMVs,the further growth of existing SIMVs,and the recoverable(001)compound twins.While the decrease ofε_(re)^(T)is mainly associated with the irrecoverable strain by{20−1}martensite twins.The effect ofβ-Nb inclusions on the evolution of SIMVs is also found herein that deformedβ-Nb inclusions can significantly hinder the growth and recoverability of adjacent stress-induced martensite. 展开更多
关键词 Ni_(47)Ti_(44)Nb_(9)shape memory alloy Wide transformation hysteresis Thermomechanical loading Microstructure evolution Shape memory behaviors Stress-induced martensitic transformation Deformation twinning
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Shear band evolution and mechanical behavior of cold-rolled Zr-based amorphous alloy sheets:An in-situ study 被引量:1
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作者 C.Y.Zhang Z.W.Zhu +5 位作者 S.T.Li Y.Y.Wang Z.K.Li h.li G.Yuan H.F.Zhang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2024年第14期115-127,共13页
Cold rolling process can regulate the microstructure and mechanical properties of amorphous alloys,but it is still a challenging task to reveal their microscopic mechanism.Here,we designed an in-situ SEM observation d... Cold rolling process can regulate the microstructure and mechanical properties of amorphous alloys,but it is still a challenging task to reveal their microscopic mechanism.Here,we designed an in-situ SEM observation device for the cold rolling process of amorphous alloy,and visually observed the formation and evolution of shear bands during single-pass and multi-pass rolling process of the Zr_(55)Cu_(30)Al_(10)Ni_(5)amorphous alloy sheets.It is found that the evolution process of shear bands in the rolling process of amorphous alloy shows heritability,which is mainly reflected in two aspects:one is that the shear band formation pattern in the single-pass rolling process is more inclined to inherit the previous shear band formation pattern;the other is that the shear deformation is more likely to occur in the pre-existing shear bands in the multi-pass rolling process.This rule can be used to guide the controlled genera-tion of shear bands in amorphous alloys.Moreover,we emphasized the importance of pre-existing shear band orientations and systematically investigated the mechanical behavior of the amorphous alloys with pre-existing shear bands by in-situ SEM observation.It is found that the mechanical properties of the as-rolled amorphous alloys are determined by the competition between the work-softening of the pre-existing shear band itself and the work-hardening caused by the blocking effect of the pre-existing shear bands on the shear deformation.Based on this,we enhance the tensile fracture strength and the tensile ductility of the amorphous alloy by adjusting the orientation of the pre-existing shear bands parallel to the tensile stress axis so that the pre-existing shear bands prevent the linear propagation and destruction of the new shear bands. 展开更多
关键词 Amorphous alloy Cold rolling Shear band Mechanical behavior In-situ study PLASTICITY
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Multi-scale defects in powder-based additively manufactured metals and alloys 被引量:39
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作者 J.Fu h.li +1 位作者 X.Song M.W.Fu 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2022年第27期165-199,共35页
Defect formation is a critical challenge for powder-based metal additive manufacturing(AM).Current understanding on the three important issues including formation mechanism,influence and control method of metal AM def... Defect formation is a critical challenge for powder-based metal additive manufacturing(AM).Current understanding on the three important issues including formation mechanism,influence and control method of metal AM defects should be updated.In this review paper,multi-scale defects in AMed metals and alloys are identified and for the first time classified into three categories,including geometry related,surface integrity related and microstructural defects.In particular,the microstructural defects are further divided into internal cracks and pores,textured columnar grains,compositional defects and dislocation cells.The root causes of the multi-scale defects are discussed.The key factors that affect the defect formation are identified and analyzed.The detection methods and modeling of the multi-scale defects are briefly introduced.The effects of the multi-scale defects on the mechanical properties especially for tensile properties and fatigue performance of AMed metallic components are reviewed.Various control and mitigation methods for the corresponding defects,include process parameter control,post processing,alloy design and hybrid AM techniques,are summarized and discussed.From research aspect,current research gaps and future prospects from three important aspects of the multi-scale AM defects are identified and delineated. 展开更多
关键词 Metal additive manufacturing Multi-scale defects Detection and modeling Mechanical properties Defect control and mitigation
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Diffusion behavior at void tip and its contributions to void shrinkage during solid-state bonding 被引量:5
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作者 C.Zhang M.Q.Li h.li 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2018年第8期1449-1454,共6页
Solid-state diffusion bonding is an advanced joining technique, which has been widely used to join similar or dissimilar materials. Generally, it is easy to observe the diffusion behavior during dissimilar bonding, bu... Solid-state diffusion bonding is an advanced joining technique, which has been widely used to join similar or dissimilar materials. Generally, it is easy to observe the diffusion behavior during dissimilar bonding, but for similar bonding the diffusion behavior has yet been observed via experiments. In this study, the diffusion behavior at void tip was firstly observed during similar bonding of stainless steel. Scanning electron microscopy with energy dispersive spectroscopy was used to examine the interface charac- teristic and diffusion behavior. The results showed that a diffusion region was discovered at void tip. Element concentrations of diffusion region were more than those of void region, but less than those of bonded region. This behavior indicated that the diffusion was ongoing at void tip, but the perfect bond has yet formed. The diffusion region was attributed to the interface diffusion from adjacent region to void tip due to the stress gradient along bonding interface. The mass accumulation at void tip transformed the sharp void tip into smooth one at the beginning of void shrinkage, and then resulted in shorter voids. 展开更多
关键词 Stainless steel Micro-void morphology Solid-state bonding Void tip Element diffusion
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New ductile laminate structure of Ti-alloy/Ti-based metallic glass composite with high specific strength 被引量:4
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作者 D.Li Z.W.Zhu +4 位作者 A.M.Wang H.M.Fu h.li H.W.Zhang H.F.Zhang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2018年第4期708-712,共5页
Bulk laminate structure of Ti-alloy/Ti-based metallic glass composite (MGC) was prepared by melting a preform of alternate stack-up foils in the high vacuum atmosphere. The composite demonstrates a good combination ... Bulk laminate structure of Ti-alloy/Ti-based metallic glass composite (MGC) was prepared by melting a preform of alternate stack-up foils in the high vacuum atmosphere. The composite demonstrates a good combination of yield strength (-1618MPa), plasticity (-4.3%) and specific fracture strength (384 × 10^3 N m kg^-1 ) in compression. The maintained yield strength results from the unique microstruc- ture composed of the Ti layer, the solution layer with gradient structure and the MGC layer. Such a multilayer structure effectively inhibits the propagation of shear band, leading to the enhanced plastic- ity. Those extraordinary properities suggest that combining ductile lamella with brittle metallic glass (MG) by such a lay-up method can be an effective way to improve mechanical properties of MG. 展开更多
关键词 Laminate composite Metallic glass Specific strength PLASTICITY
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Large deformation and wrinkling analyses of bimodular structures and membranes based on a peridynamic computational framework 被引量:3
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作者 h.li Y.G.Zheng +2 位作者 Y.X.Zhang H.F.Ye H.W.Zhang 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2019年第6期1226-1240,共15页
In this paper,the quasi-static large deformation,wrinkling and fracture behaviors of bimodular structures and membranes are studied with an implicit bond-based peridynamic computational framework.Firstly,the constant ... In this paper,the quasi-static large deformation,wrinkling and fracture behaviors of bimodular structures and membranes are studied with an implicit bond-based peridynamic computational framework.Firstly,the constant and tangential stiffness matrices of the implicit peridynamic formulations for the nonlinear problems are derived,respectively.The former is con structed from the linearization of the bond strain on the basis of the geometric approximation while the latter is established according to the linearization of the pairwise force by using first-order Taylor’s expansion.Then,a bimodular material model in peridynamics is developed,in which the tensile or compressive behavior of the material at each point is conveniently described by the tensile or compressive states of the bonds in its neighborhood.Moreover,the bimodular material model is extended to deal with the wrinkling and fracture problems of membranes by setting the compressive micro-modulus to be zero.In addition,the incremental-iterative algorithm is adopted to obtain the convergent solutions of the nonlinear problems.Finally,several representative numerical examples are presented and the results demonstrate the accuracy and efficiency of the proposed method for the large deformation,wrinkling and fracture analyses of bimodular structures and membranes. 展开更多
关键词 Bimodular structures Wrinkling membranes Fracture problems PERIDYNAMICS Implicit numerical algorithm
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The Lobster Eye Imager for Astronomy Onboard the SATech-01 Satellite 被引量:2
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作者 Z.X.Ling X.J.Sun +123 位作者 C.Zhang S.L.Sun G.Jin S.N.Zhang X.F.Zhang J.B.Chang F.S.Chen Y.F.Chen Z.W.Cheng W.Fu Y.X.Han h.li J.F.Li Y.Li Z.D.Li P.R.Liu Y.H.Lv X.H.Ma Y.J.Tang C.B.Wang R.J.Xie Y.L.Xue A.L.Yan Q.Zhang C.Y.Bao H.B.Cai H.Q.Cheng C.Z.Cui Y.F.Dai D.W.Fan H.B.Hu J.W.Hu M.H.Huang Z.Q.Jia C.C.Jin D.Y.Li J.Q.Li H.Y.Liu M.J.Liu Y.Liu H.W.Pan Y.L.Qiu M.Sugizaki H.Sun W.X.Wang Y.L.Wang Q.Y.Wu X.P.Xu Y.F.Xu H.N.Yang X.Yang B.Zhang M.Zhang W.D.Zhang Z.Zhang D.H.Zhao X.Q.Cong B.W.Jiang L.h.li X.B.Qiu J.N.Sun D.T.Su J.Wang C.Wu Z.Xu X.M.Yang S.K.Zhang Z.Zhang N.Zhang Y.F.Zhu H.Y.Ban X.Z.Bi Z.M.Cai W.Chen X.Chen Y.H.Chen Y.Cui X.L.Duan Z.G Feng Y.Gao J.W.He T.He J.J.Huang F.Li J.S.Li T.J.Li T.T.Li H.Q.Liu L.Liu R.Liu S.Liu N.Meng Q.Shi A.T.Sun Y.M.Wang Y.B.Wang H.C.Wu D.X Xu Y.Q Yang Y.Yang X.S.Yu K.X.Zhang Y.L.Zhang Y.H.Zhang Y.T.Zhang H.Zhou X.C.Zhu J.S.Cheng L.Qin L.Wang Q.L.Wang M.Bai R.L.Gao Z.Ji Y.R.Liu F.L.Ma Y.J.Shi J.Su Y.Y.Tan J.Z.Tong H.T.Xu C.B.Xue G.F.Xue W.Yuan 《Research in Astronomy and Astrophysics》 SCIE CAS CSCD 2023年第9期66-78,共13页
The Lobster Eye Imager for Astronomy(LEIA),a pathfinder of the Wide-field X-ray Telescope of the Einstein Probe mission,was successfully launched onboard the SATech-01 satellite of the Chinese Academy of Sciences on20... The Lobster Eye Imager for Astronomy(LEIA),a pathfinder of the Wide-field X-ray Telescope of the Einstein Probe mission,was successfully launched onboard the SATech-01 satellite of the Chinese Academy of Sciences on2022 July 27.In this paper,we introduce the design and on-ground test results of the LEIA instrument.Using stateof-the-art Micro-Pore Optics(MPO),a wide field of view of 346 square degrees(18.6°×18.6°)of the X-ray imager is realized.An optical assembly composed of 36 MPO chips is used to focus incident X-ray photons,and four large-format complementary metal-oxide semiconductor(CMOS)sensors,each of size 6 cm×6 cm,are used as the focal plane detectors.The instrument has an angular resolution of 4’-8’(in terms of FWHM)for the central focal spot of the point-spread function,and an effective area of 2-3 cm^(2) at 1 keV in essentially all the directions within the field of view.The detection passband is 0.5-4 keV in soft X-rays and the sensitivity is2-3×10^(-11) erg s^(-1) cm^(-2)(about 1 milliCrab)with a 1000 s observation.The total weight of LEIA is 56 kg and the power is 85 W.The satellite,with a design lifetime of 2 yr,operates in a Sun-synchronous orbit of 500 km with an orbital period of 95 minutes.LEIA is paving the way for future missions by verifying in flight the technologies of both novel focusing imaging optics and CMOS sensors for X-ray observation,and by optimizing the working setups of the instrumental parameters.In addition,LEIA is able to carry out scientific observations to find new transients and to monitor known sources in the soft X-ray band,albeit with limited useful observing time available. 展开更多
关键词 instrumentation detectors-space vehicles instruments-telescopes-X-rays GENERA
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Distribution of Be in a Ti-Based Bulk Metallic Glass Composite Containing B-Ti 被引量:6
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作者 L.Zhang W.Q.Li +6 位作者 Z.W.Zhu H.M.Fu h.li Z.K.Li H.W.Zhang A.M.Wang H.F.Zhang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2017年第7期708-711,共4页
In order to obtain a glassy matrix during quenching, Be is often selected as a constituent of the compositions of Ti/Zr-based bulk metallic glass composites(BMGCs). The in situ formed β phase in Be-bearing BMGCs wa... In order to obtain a glassy matrix during quenching, Be is often selected as a constituent of the compositions of Ti/Zr-based bulk metallic glass composites(BMGCs). The in situ formed β phase in Be-bearing BMGCs was reported to be Be-free. However, a thorough investigation of the distribution of Be in BMGCs is still missing to date. In this work, the distribution of Be in a Ti_(47.5)Zr_(33)Cu_(5.8)Co_3Be_(12.5)(at.%) BMGC was studied by the secondary ion mass spectrometry(SIMS) and the electron energy loss spectroscopy(EELS).It is found that Be almost totally dissolves in the glassy matrix, but a very weak intensity of Be in β phase is still detectable by SIMS, and the content of Be in β-Ti is estimated to be about 0.3 at.%. Based on the recently established two-phase quasi-equilibrium of BMGCs, the distinct solubility of Be in the glassy matrix and in β-Ti has been explained. 展开更多
关键词 Bulk metallic glass(BMG) Metallic glass composite Beryllium Quasi-equilibrium
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Modeling biomembranes and red blood cells by coarse-grained particle methods 被引量:1
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作者 h.li H.Y.CHANG +3 位作者 J.YANG L.LU Y.H.TANG G.LYKOTRAFITIS 《Applied Mathematics and Mechanics(English Edition)》 SCIE EI CSCD 2018年第1期3-20,共18页
In this work, the previously developed coarse-grained (CG) particle models for biomembranes and red blood cells (RBCs) are reviewed, and the advantages of the CG particle methods over the continuum and atomistic s... In this work, the previously developed coarse-grained (CG) particle models for biomembranes and red blood cells (RBCs) are reviewed, and the advantages of the CG particle methods over the continuum and atomistic simulations for modeling biological phenomena are discussed. CG particle models can largely increase the length scale and time scale of atomistic simulations by eliminating the fast degrees of freedom while preserving the mesoscopic structures and properties of the simulated system. Moreover, CG particle models can be used to capture the microstructural alternations in diseased RBCs and simulate the topological changes of biomembranes and RBCs, which are the major challenges to the typical continuum representations of membranes and RBCs. The power and versatility of CG particle methods are demonstrated:through simulating the dynamical processes mvolving significant topological .changes e.g. lipid self-assembly vesicle fusion and membrane budding. 展开更多
关键词 coarse-grained molecular dynamics lipid bilayer red blood cell membrane membrane fusion
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Effects of concurrent grain boundary and surface segregation on the final stage of sintering: the case of Lanthanum doped yttriastabilized zirconia 被引量:2
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作者 M.M.Gong S.Dey +4 位作者 L.J.Wu C.H.Chang h.li R.H.R.Castro F.Liu 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2017年第3期251-260,共10页
Dopants play a critical role in tailoring the microstructure during sintering of compacts. These dopants may form solid solution within the bulk, and/or segregate to the grain boundaries(GBs) and the solidvapor inte... Dopants play a critical role in tailoring the microstructure during sintering of compacts. These dopants may form solid solution within the bulk, and/or segregate to the grain boundaries(GBs) and the solidvapor interfaces(free surfaces), each causing a distinct energetic scenario governing mass transports during densification and grain growth. In this work, the forces controlling the dopant distribution, in particular the possibility of concurrent segregation at both surfaces and GBs, are discussed based on the respective enthalpy of segregation. An equation is derived based on the minimum Gibbs energy of the system to determine enthalpy of segregation from experimental interface energy data, and the results applied to depict the role of La as a dopant on the interface energetics of yttria stabilized zirconia during its final stage of sintering. It is shown that La substantially decreases both GB and surface energies(differently)as sintering progresses, dynamically affecting its driving forces, and consequent grain growth and densification in this stage. 展开更多
关键词 Grain boundary(GB) segregation Surface segregation Enthalpy of segregation GB energy Surface energy
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由灌溉引起的阶地边缘黄土滑坡 被引量:2
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作者 D.MA S.ZHAO +1 位作者 h.li 曾康 《四川水利》 1998年第4期63-64,共2页
关键词 滑坡 阶地边缘 黄土滑坡 灌溉 漫灌
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Observation of an EPIR Effect in Nd_(1-x)Sr_xMnO_3 Ceramics with Secondary Phases
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作者 S.S.Chen X.J.Luo +2 位作者 D.W.Shi h.li C.P.Yang 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2013年第8期737-741,共5页
Nd1-xSrxMnO3 (x : 0.3, 0.5) ceramics containing a secondary phase are synthesized by high-energy ball milling and post heat-treatment method. The 4-wire and 2-wire measuring modes are used to investigate the transp... Nd1-xSrxMnO3 (x : 0.3, 0.5) ceramics containing a secondary phase are synthesized by high-energy ball milling and post heat-treatment method. The 4-wire and 2-wire measuring modes are used to investigate the transport character of the grain/phase boundary (inner interface) and electrode-bulk interface (outer interface), respectively, and the results indicate that there is a similar nonlinear I-V behaviour for both of the inner and outer interfaces, however, the electric pulse induced resistance change (EPIR) effect can only be observed at the outer interface. 展开更多
关键词 Electric pulse induced resistance change (EPIR) Space charge layer NONLINEARITY MANGANITE High-energy ball milling
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深部地壳的氧同位素变异——加拿大安大略省Wawa-Kapuskasing地壳断面
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作者 h.li H.P.Schwarcz +1 位作者 D.M.Shaw 于介江 《世界地质》 CAS CSCD 1992年第4期34-37,共4页
我们已经研究了安大略中部苏必利尔省内100km断面域内岩石的氧同位素组成。代表性构造单元有kapuskasing构造带的较浅部地体,Wawa片麻岩地体和Michipicoten绿岩带。这些岩石的年龄介于2.76~2.60 Ga之间,并且与约20km厚的地壳断面相对... 我们已经研究了安大略中部苏必利尔省内100km断面域内岩石的氧同位素组成。代表性构造单元有kapuskasing构造带的较浅部地体,Wawa片麻岩地体和Michipicoten绿岩带。这些岩石的年龄介于2.76~2.60 Ga之间,并且与约20km厚的地壳断面相对应。在每个地壳层次,相同的岩石类型具有类似的δ^(18)O数值范围。英云闪长质到花岗闪长质岩石:6.4~9.5‰;闪长质到斜长质岩石:5.5~7.6‰;镁铁质片麻岩:组1(主体):5.7~7.1‰;组2:8.1~9.5‰。δ^(18)O值与SiO_2值具有明显的相关性,这与相同成分未蚀变深成岩的观测结果类似。副片麻岩具有相当高的δ^(18)O值;9.3~12.2‰。与kapuskasing构造带和Wawa片麻岩地体中的高级变质岩相比,Michipicoten绿岩带中的低级变火山岩和变沉积岩富含^(18)O。镁铁质到长英质变火山岩的δ^(18)O值为:7.4~13.3‰;碎屑沉积岩的δ^(18)O值为:11.4~14.7‰。共存矿物表现出与平衡作用相一致的^(18)O分馏作用,这与整个断面内均一的同位素温度(约553~584℃)相符。这一温度比最高级地体(Kapuskasing构造带)中推断的变质温度要低。Kapuskasing构造带,Wawa片麻岩地体和Michipicoten绿岩带中相同岩石类型之间无明显的同位素差异,这表明随地壳深度的变化δ^(18)O值没有明显的变化。镁铁质片麻岩的主体(组1)或是作为近地表的喷出岩或侵入的岩床产出,或是(可能性更小)作为水下喷发物产出,后者遭受了高温热液蚀变作用。不太多的组2中的镁铁质岩石具有遭受海水低温蚀变的绿岩的δ^(18)O值,并且在同位素组成上,它们类似于Michipicoten和Abitibi带中的低级变质岩。总之,在麻粒岩相交质作用过程中,全岩同位素组成没有大的变化,这就意味着有限的水和CO_2熔剂的存在。在高级变质岩中,δ^(18)O和SiO_2之间的连续的线性梯度并不是由于镁铁质源区岩浆分异作用造成的。关于幔源镁铁质岩浆和富含^(18)O的地壳物质组合的一个成因模式与氧同位素和稀土元素资料更吻合。 展开更多
关键词 地壳 同位素 变异
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STCF conceptual design report (Volume 1): Physics & detector 被引量:5
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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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Whole‑genome analyses and metabolic modification of Mycobacterium sp.LY‑1 to enhance yield of 9α‑OH‑AD 被引量:1
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作者 W.Liu h.li +5 位作者 J.X.Zhang Y.N.Xu X.M.Zhang J.S.Shi M.A.G.Koffas Z.H.Xu 《Systems Microbiology and Biomanufacturing》 2024年第1期127-137,共11页
With the increasing application of steroid drugs as therapeutics,the demand for steroid drugs is increasing.In recent years,biological synthesis has become the standard approach to produce steroid intermediates,while ... With the increasing application of steroid drugs as therapeutics,the demand for steroid drugs is increasing.In recent years,biological synthesis has become the standard approach to produce steroid intermediates,while this method still faces some problems such as unclear metabolic pathway and low yield.Mycobacterium sp.LY-1 can convert phytosterols into 9α-hydroxyandrost-4-ene-3,17-dione(9α-OH-AD)which is a key intermediate for the synthesis of steroid drugs with long effective time and significant pharmacological activity.In this work,the whole-genome sequence of the Mycobacterium sp.LY-1 was analyzed,and the side-chain degradation pathway of phytosterols in Mycobacterium sp.LY-1 was proposed.Meanwhile,the related key enzymes of phytosterol metabolism were identified through qRT-PCR.Through overexpressing the key enzymes including KshA2,KshB,and HsdB,the yield of 9α-OH-AD increased by 12.7%compared to that of the control.Furthermore,by optimizing the medium and culture conditions,the yield of 9α-OH-AD reached 50.4%.The maxi-mum yield was 30.7%higher than that of the original strain.The results are of significance for the industrial production of 9α-OH-AD using metabolic engineering methods. 展开更多
关键词 Mycobacterium sp.LY-1 Phytosterols 9α-Hydroxyandrost-4-ene-3 17-dione BIOTRANSFORMATION
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Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)
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作者 M.Ablikim M.N.Achasov +642 位作者 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.G.Li Z.J.Li Z.X.Li C.Liang h.liang h.liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao Y.P.Liao J.Libby A.Limphirat D.X.Lin T.Lin B.J.Liu B.X.Liu C.Liu C.X.Liu F.Liu F.h.liu Feng Liu G.M.Liu h.liu H.B.Liu H.h.liu H.M.Liu Huihui Liu J.B.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu L.C.Liu Lu Liu M.h.liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu X.Liu Y.Liu Y.Liu Y.B.Liu Z.A.Liu Z.D.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.Ma H.L.Ma J.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma X.T.Ma X.Y.Ma Y.Ma Y.M.Ma F.E.Maas M.Maggiora S.Malde A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo B.Moses N.Yu.Muchnoi J.Muskalla Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Q.L.Niu W.D.Niu Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak P.Patteri Y.P.Pei M.Pelizaeus H.P.Peng Y.Y.Peng K.Peters J.L.Ping R.G.Ping S.Plura V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian C.F.Qiao J.J.Qin L.Q.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu Z.H.Qu C.F.Redmer K.J.Ren A.Rivetti M.Rolo G.Rong Ch.Rosner S.N.Ruan N.Salone A.Sarantsev Y.Schelhaas K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen W.H.Shen X.Y.Shen B.A.Shi H.C.Shi J.L.Shi J.Y.Shi Q.Q.Shi R.S.Shi S.Y.Shi X.Shi X.D.Shi J.J.Song T.Z.Song W.M.Song Y.J.Song Y.X.Song S.Sosio S.Spataro F.Stieler Y.J.Su G.B.Sun G.X.Sun H.Sun H.K.Sun J.F.Sun K.Sun L.Sun S.S.Sun T.Sun W.Y.Sun Y.Sun Y.J.Sun Y.Z.Sun Z.Q.Sun Z.T.Sun C.J.Tang G.Y.Tang J.Tang Y.A.Tang L.Y.Tao Q.T.Tao M.Tat J.X.Teng V.Thoren W.H.Tian Y.Tian Z.F.Tian I.Uman Y.Wan S.J.Wang B.Wang B.L.Wang Bo Wang D.Y.Wang F.Wang H.J.Wang J.P.Wang K.Wang L.L.Wang M.Wang Meng Wang N.Y.Wang S.Wang S.Wang T.Wang T.J.Wang W.Wang W.Wang W.P.Wang X.Wang X.F.Wang X.J.Wang X.L.Wang X.N.Wang Y.Wang Y.D.Wang Y.F.Wang Y.L.Wang Y.N.Wang Y.Q.Wang Yaqian Wang Yi Wang Z.Wang Z.L.Wang Z.Y.Wang Ziyi Wang D.Wei D.H.Wei F.Weidner S.P.Wen Y.R.Wen U.Wiedner G.Wilkinson M.Wolke L.Wollenberg C.Wu J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Y.H.Wu Y.J.Wu Z.Wu L.Xia X.M.Xian B.H.Xiang T.Xiang D.Xiao G.Y.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao C.Xie X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu H.Y.Xu Q.J.Xu Q.N.Xu W.Xu W.L.Xu X.P.Xu Y.C.Xu Z.P.Xu Z.S.Xu F.Yan L.Yan W.B.Yan W.C.Yan X.Q.Yan H.J.Yang H.L.Yang H.X.Yang T.Yang Y.Yang Y.F.Yang Y.F.Yang Y.X.Yang Z.W.Yang Z.P.Yao M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu T.Yu X.D.Yu C.Z.Yuan J.Yuan L.Yuan S.C.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng S.H.Zeng X.Zeng Y.Zeng Y.J.Zeng Y.J.Zeng X.Y.Zhai Y.C.Zhai Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.C.Zhang H.H.Zhang H.H.Zhang H.Q.Zhang H.Y.Zhang J.Zhang J.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang L.M.Zhang Lei Zhang P.Zhang Q.Y.Zhang S.H.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Y.M.Zhang Yan Zhang Z.D.Zhang Z.H.Zhang Z.L.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Y.Zhao J.Z.Zhao L.Zhao Lei Zhao M.G.Zhao R.P.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng W.J.Zheng Y.H.Zheng B.Zhong X.Zhong H.Zhou J.Y.Zhou L.P.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.Zhu L.X.Zhu S.H.Zhu S.Q.Zhu T.J.Zhu W.D.Zhu Y.C.Zhu Z.A.Zhu J.H.Zou J.Zu 《Chinese Physics C》 SCIE CAS CSCD 2024年第8期6-33,共28页
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... 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 channels.With 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.))%,respectively.The 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.))%,respectively.The 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. 展开更多
关键词 BESIII D^(0)meson decays amplitude analysis CP-even fraction
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Measurements of the center-of-mass energies of e^(+)e^(-)collisions at BESIII 被引量:1
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作者 M.Ablikim M.N.Achasov +511 位作者 P.Adlarson S.Ahmed M.Albrecht R.Aliberti A.Amoroso M.R.An Q.An X.H.Bai Y.Bai O.Bakina R.Baldini Ferroli I.Balossino Y.Ban K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi J.Bloms A.Bortone I.Boyko R.A.Briere H.Cai X.Cai A.Calcaterra G.F.Cao N.Cao S.A.Cetin J.F.Chang W.L.Chang G.Chelkov D.Y.Chen G.Chen H.S.Chen M.L.Chen S.J.Chen X.R.Chen Y.B.Chen Z.J.Chen W.S.Cheng G.Cibinetto F.Cossio X.F.Cui H.L.Dai X.C.Dai A.Dbeyssi R.E.de Boer D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori Y.Ding C.Dong J.Dong L.Y.Dong M.Y.Dong X.Dong S.X.Du Y.L.Fan J.Fang S.S.Fang Y.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng M.Fritsch C.D.Fu Y.Gao Y.Gao Y.Gao Y.G.Gao I.Garzia P.T.Ge C.Geng E.M.Gersabeck A Gilman K.Goetzen L.Gong W.X.Gong W.Gradl M.Greco L.M.Gu M.H.Gu Y.T.Gu C.Y Guan A.Q.Guo L.B.Guo R.P.Guo Y.P.Guo A.Guskov T.T.Han W.Y.Han X.Q.Hao F.A.Harris K.L.He F.H.Heinsius C.H.Heinz T.Held Y.K.Heng C.Herold M.Himmelreich T.Holtmann G.Y.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang L.Q.Huang X.T.Huang Y.P.Huang Z.Huang T.Hussain N Husken W.Ikegami Andersson W.Imoehl M.Irshad S.Jaeger S.Janchiv Q.Ji Q.P.Ji X.B.Ji X.L.Ji Y.Y.Ji H.B.Jiang X.S.Jiang J.B.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing T.Johansson N.Kalantar-Nayestanaki X.S.Kang R.Kappert M.Kavatsyuk B.C.Ke I.K.Keshk A.Khoukaz P.Kiese R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc M.G.Kurth W.Kuhn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi Z.H.Lei H.Leithoff M.Lellmann T.Lenz C.Li C.h.li Cheng Li D.M.Li F.Li G.Li h.li h.li H.B.Li H.J.Li J.L.Li J.Q.Li J.S.Li Ke Li L.K.Li Lei Li P.R.Li S.Y.Li W.D.Li W.G.Li X.h.li X.L.Li Xiaoyu Li Z.Y.Li h.liang h.liang h.liang Y.F.Liang Y.T.Liang G.R.Liao L. Z. Liao J.Libby C.X.Lin B.J.Liu C.X.Liu D.Liu F.h.liu Fang Liu Feng Liu H.B.Liu H.M.Liu Huanhuan Liu Huihui Liu J.B.Liu J.L.Liu J.Y.Liu K.Liu K.Y.Liu L.Liu M.h.liu P.L.Liu Q.Liu Q.Liu S.B.Liu Shuai Liu T.Liu W.M.Liu X.Liu Y.Liu Y.B.Liu Z.A.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.D.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu C.L.Luo M.X.Luo P.W.Luo T.Luo X.L.Luo X.R.Lyu F.C.Ma H.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma R.T.Ma X.X.Ma X.Y.Ma F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri T.J.Min R.E.Mitchell X.H.Mo N.Yu.Muchnoi H.Muramatsu S.Nakhoul Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak A.Pathak P.Patteri M.Pelizaeus H.P.Peng K.Peters J.Pettersson J.L.Ping R.G.Ping S.Pogodin R.Poling V.Prasad H.Qi H.R.Qi K.H.Qi M.Qi T.Y.Qi S.Qian W.B.Qian Z.Qian C.F.Qiao L.Q.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu K.H.Rashid K.Ravindran C.F.Redmer A.Rivetti V.Rodin M.Rolo G.Rong Ch.Rosner M.Rump H.S.Sang A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio D.C.Shan W.Shan X.Y.Shan J.F.Shangguan M.Shao C.P.Shen H.F.Shen P.X.Shen X.Y.Shen H.C.Shi R.S.Shi X.Shi X.D Shi J.J.Song W.M.Song Y.X.Song S.Sosio S.Spataro K.X.Su P.P.Su F.F.Sui G.X.Sun H.K.Sun J.F.Sun L.Sun S.S.Sun T.Sun W.Y.Sun W.Y.Sun X Sun Y.J.Sun Y.K.Sun Y.Z.Sun Z.T.Sun Y.H.Tan Y.X.Tan C.J.Tang G.Y.Tang J.Tang J.X.Teng V.Thoren W.H.Tian Y.T.Tian I.Uman B.Wang C.W.Wang D.Y.Wang H.J.Wang H.P.Wang K.Wang L.L.Wang M.Wang M.Z.Wang Meng Wang W.Wang W.H.Wang W.P.Wang X.Wang X.F.Wang X.L.Wang Y.Wang Y.Wang Y.D.Wang Y.F.Wang Y.Q.Wang Y.Y.Wang Z.Wang Z.Y.Wang Ziyi Wang Zongyuan Wang D.H.Wei F.Weidner S.P.Wen D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg J.F.Wu L.H.Wu L.J.Wu X.Wu Z.Wu L.Xia H.Xiao S.Y.Xiao Z.J.Xiao X.H.Xie Y.G.Xie Y.H.Xie T.Y.Xing G.F.Xu Q.J.Xu W.Xu X.P.Xu Y.C.Xu F.Yan L.Yan W.B.Yan W.C.Yan Xu Yan H.J.Yang H.X.Yang L.Yang S.L.Yang Y.X.Yang Yifan Yang Zhi Yang M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu J.S.Yu T.Yu C. Z. Yuan L.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar X.Zeng Zeng Y.Zeng A.Q.Zhang B.X.Zhang Guangyi Zhang H.Zhang H.H.Zhang H.H.Zhang H.Y.Zhang J.J.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang Jiawei Zhang L.M.Zhang L.Q.Zhang Lei Zhang S.Zhang S.F.Zhang Shulei Zhang X.D.Zhang X.Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Yan Zhang Yao Zhang Z.Y.Zhang G.Zhao J.Zhao J.Y.Zhao J.Z.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng Y.H.Zheng B.Zhong C.Zhong L.P.Zhou Q.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou A.N.Zhu J.Zhu K.Zhu K.J.Zhu S.H.Zhu T.J.Zhu W.J.Zhu W.J.Zhu Y.C.Zhu Z.A.Zhu B.S.Zou J.H.Zou 《Chinese Physics C》 SCIE CAS CSCD 2021年第10期7-15,共9页
During the 2016-17 and 2018-19 running periods,the BESIII experiment collected 7.5 fb of e^(+)e^(-)collision data at center-of-mass energies ranging from 4.13 to 4.44 GeV.These data samples are primarily used for the ... During the 2016-17 and 2018-19 running periods,the BESIII experiment collected 7.5 fb of e^(+)e^(-)collision data at center-of-mass energies ranging from 4.13 to 4.44 GeV.These data samples are primarily used for the study of excited charmonium and charmoniumlike states.By analyzing the di-muon process e^(+)e^(-)→(γISR=FSR)μ^(+)μ^(-),we measure the center-of-mass energies of the data samples with a precision of 0.6 MeV.Through a run-by-run study,we find that the center-of-mass energies were stable throughout most of the data-collection period. 展开更多
关键词 center-of-mass ENERGY e^(+)e^(-) ANNIHILATION BESIII
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Construction and optimization of boldenone synthesis from androstenedione catalyzed by a dual-enzyme system
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作者 Y.Liang h.li +6 位作者 W.Liu L.Y.Xu J.X.Zhang L.Y.Chen S.L.Wang J.S.Shi Z.H.Xu 《Systems Microbiology and Biomanufacturing》 2024年第2期783-793,共11页
Boldenone is a protein-assimilating androgen steroid that can promote protein synthesis,support nitrogen storage,and enhance renal erythropoietin release.The industrial production of boldenone mainly relies on chemica... Boldenone is a protein-assimilating androgen steroid that can promote protein synthesis,support nitrogen storage,and enhance renal erythropoietin release.The industrial production of boldenone mainly relies on chemical synthesis,which has various problems,such as a complex conversion process,excessive byproducts,and serious environmental pollution.There-fore,it is of great significance to explore a new biosynthetic route.Recently,the enzymatic synthesis of steroid compounds has been performed more frequently than in the past.In this work,boldenone was produced from androstenedione(AD)in two steps by a dual-enzyme cascade of 17β-hydroxysteroid dehydrogenase(17β-HSD)and 3-sterone-Δ^(1)-dehydrogenase(KstD).The conversion efficiency of three isoenzymes of 17β-HSD from Mycobacterium sp.LY-1 for substrate AD was first analyzed.After that,the 17β-HSD2 with high selectivity and specificity for AD was screened and co-expressed with KstD3 in Escherichia coli BL21 to construct a dual-enzyme catalytic system.The results showed that the synthesis of boldenone from AD could be achieved by constructing the dual-enzyme expression system of 17β-HSD and KstD,as we determined that the concentration of boldenone reached 24.3 mg/L.To further improve the synthesis efficiency of boldenone,the expression conditions of the dual-enzyme system were optimized,and the concentration of boldenone reached 31.9 mg/L.The explora-tion of this route will provide a foundation for the efficient enzymatic synthesis of boldenone. 展开更多
关键词 BOLDENONE Dual-enzyme catalytic system 17β-HSD KstD Escherichia coli Heterologous expression
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Measurement of integrated luminosities at BESⅢ for data samples at center-of-mass energies between 4.0 and 4.6 GeV
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作者 M.Ablikim M.N.Achasov +561 位作者 P.Adlarson S.Ahmed M.Albrecht R.Aliberti A.Amoroso M.R.An Q.An X.H.Bai Y.Bai O.Bakina R.Baldini Ferroli I.Balossino Y.Ban V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi J.Bloms 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.Chelkov C.Chen G.Chen H.S.Chen M.L.Chen S.J.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Z.J.Chen W.S.Cheng X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.Ede Boer D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong S.X.Du P.Egorov Y.L.Fan J.Fang S.S.Fang W.X.Fang Y.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng K Fischer M.Fritsch C.Fritzsch C.D.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge C.Geng E.M.Gersabeck A Gilman K.Goetzen L.Gong W.X.Gong W.Gradl M.Greco M.H.Gu C.Y Guan A.Q.Guo L.B.Guo R.P.Guo Y.P.Guo A.Guskov T.T.Han W.Y.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold M.Himmelreich T.Holtmann G.Y.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang L.Q.Huang X.T.Huang Y.P.Huang Z.Huang T.Hussain N Husken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv Q.Ji Q.P.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia H.B.Jiang S.S.Jiang X.S.Jiang Y.Jiang J.B.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing T.Johansson N.Kalantar-Nayestanaki X.S.Kang R.Kappert M.Kavatsyuk B.C.Ke I.K.Keshk A.Khoukaz P.Kiese R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kuhn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi 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.li H.B.Li H.J.Li H.N.Li J.Q.Li J.S.Li J.W.Li Ke Li L.J Li L.K.Li Lei Li M.h.li P.R.Li S.X.Li S.Y.Li T.Li W.D.Li W.G.Li X.h.li X.L.Li Xiaoyu Li Z.Y.Li h.liang h.liang h.liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao J.Libby A.Limphirat C.X.Lin D.X.Lin T.Lin B.J.Liu C.X.Liu D.Liu F.h.liu Fang Liu Feng Liu G.M.Liu h.liu H.M.Liu Huanhuan Liu Huihui Liu J.B.Liu J.L.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu M.h.liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu Y.Liu Y.B.Liu Z.A.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma R.T.Ma X.Y.Ma Y.Ma F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo N.Yu.Muchnoi H.Muramatsu Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak A.Pathak M.Pelizaeus H.P.Peng K.Peters J.Pettersson J.L.Ping R.G.Ping S.Plura S.Pogodin R.Poling V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian Z.Qian C.F.Qiao J.J.Qin L.Q.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu S.Q.Qu K.H.Rashid C.F.Redmer K.J.Ren A.Rivetti V.Rodin M.Rolo G.Rong Ch.Rosner S.N.Ruan H.S.Sang A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen X.Y.Shen B.-A.Shi H.C.Shi J.Y.Shi R.S.Shi X.Shi X.D Shi J.J.Song W.M.Song Y.X.Song S.Sosio S.Spataro F.Stieler K.X.Su P.P.Su Y.-J.Su G.X.Sun H.Sun H.K.Sun J.F.Sun L.Sun S.S.Sun T.Sun W.Y.Sun X Sun Y.J.Sun Y.Z.Sun Z.T.Sun Y.H.Tan Y.X.Tan C.J.Tang G.Y.Tang J.Tang L.Y Tao Q.T.Tao J.X.Teng V.Thoren W.H.Tian Y.Tian I.Uman B.Wang B.L.Wang D.Y.Wang F.Wang H.J.Wang H.P.Wang K.Wang L.L.Wang M.Wang M.Z.Wang Meng Wang S.Wang T.Wang T.J.Wang W.Wang W.H.Wang W.P.Wang X.Wang X.F.Wang X.L.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.Q.Wang Ying Wang Z.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Z.Wu L.Xia T.Xiang D.Xiao H.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu Q.J.Xu S.Y.Xu X.P.Xu Y.C.Xu F.Yan L.Yan W.B.Yan W.C.Yan H.J.Yang H.L.Yang H.X.Yang L.Yang S.L.Yang Tao Yang Y.X.Yang Yifan Yang M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu T.Yu C.Z.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng X.Zeng Y.Zeng Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.H.Zhang H.H.Zhang H.Y.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang Jiawei Zhang L.M.Zhang L.Q.Zhang Lei Zhang P.Zhang Q.Y.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang X.Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Yan Zhang Yao Zhang Z.H.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Zhao J.Y.Zhao J.Z.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng Y.H.Zheng B.Zhong C.Zhong X.Zhong H.Zhou L.P.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.J.Zhu Y.C.Zhu Z.A.Zhu B.S.Zou J.H.Zou Y.T.Gu H.B.Liu 《Chinese Physics C》 SCIE CAS CSCD 2022年第11期53-63,共11页
The integrated luminosities of data samples collected in the BESⅢ experiment in 2016-2017 at centerof-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by analyzing large-angle Bhab... The integrated luminosities of data samples collected in the BESⅢ experiment in 2016-2017 at centerof-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by analyzing large-angle Bhabha scattering events.The integrated luminosities of old datasets collected in 2010-2014 are updated by considering corrections related to detector performance,offsetting the effect of newly discovered readout errors in the electromagnetic calorimeter,which can haphazardly occur. 展开更多
关键词 integrated luminosity e^(+)e^(-)annihilation Bhabha scattering
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Luminosities and energies of e^(+)e^(−) collision data taken between √s=4.61 GeV and 4.95 GeV at BESⅢ
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作者 M.Ablikim M.N.Achasov +558 位作者 P.Adlarson M.Albrecht R.Aliberti A.Amoroso M.R.An Q.An X.H.Bai Y.Bai O.Bakina R.Baldini Ferroli I.Balossino Y.Ban V.Batozskaya D.Becker K.Begzsuren N.Berger M.Bertani D.Bettoni F.Bianchi J.Bloms 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.Chelkov C.Chen G.Chen H.S.Chen M.L.Chen S.J.Chen T.Chen X.R.Chen X.T.Chen Y.B.Chen Z.J.Chen W.S.Cheng X.Chu G.Cibinetto F.Cossio J.J.Cui H.L.Dai J.P.Dai A.Dbeyssi R.Ede Boer D.Dedovich Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong S.X.Du P.Egorov Y.L.Fan J.Fang S.S.Fang W.X.Fang Y.Fang R.Farinelli L.Fava F.Feldbauer G.Felici C.Q.Feng J.H.Feng K Fischer M.Fritsch C.Fritzsch C.D.Fu H.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge C.Geng E.M.Gersabeck A Gilman K.Goetzen L.Gong W.X.Gong W.Gradl M.Greco M.H.Gu C.Y Guan A.Q.Guo L.B.Guo R.P.Guo Y.P.Guo A.Guskov T.T.Han W.Y.Han X.Q.Hao F.A.Harris K.K.He K.L.He F.H.Heinsius C.H.Heinz Y.K.Heng C.Herold M.Himmelreich T.Holtmann G.Y.Hou Y.R.Hou Z.L.Hou H.M.Hu J.F.Hu T.Hu Y.Hu G.S.Huang K.X.Huang L.Q.Huang L.Q.Huang X.T.Huang Y.P.Huang Z.Huang T.Hussain N Husken W.Imoehl M.Irshad J.Jackson S.Jaeger S.Janchiv Q.Ji Q.P.Ji X.B.Ji X.L.Ji Y.Y.Ji Z.K.Jia H.B.Jiang S.S.Jiang X.S.Jiang Y.Jiang J.B.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing T.Johansson N.Kalantar-Nayestanaki X.S.Kang R.Kappert M.Kavatsyuk B.C.Ke I.K.Keshk A.Khoukaz P.Kiese R.Kiuchi R.Kliemt L.Koch O.B.Kolcu B.Kopf M.Kuemmel M.Kuessner A.Kupsc W.Kuhn J.J.Lane J.S.Lange P.Larin A.Lavania L.Lavezzi 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.li H.B.Li H.J.Li H.N.Li J.Q.Li J.S.Li J.W.Li Ke Li L.J Li L.K.Li Lei Li M.h.li P.R.Li S.X.Li S.Y.Li T.Li W.D.Li W.G.Li X.h.li X.L.Li Xiaoyu Li Z.Y.Li h.liang h.liang h.liang Y.F.Liang Y.T.Liang G.R.Liao L.Z.Liao J.Libby A.Limphirat C.X.Lin D.X.Lin T.Lin B.J.Liu C.X.Liu D.Liu F.h.liu Fang Liu Feng Liu G.M.Liu h.liu H.M.Liu Huanhuan Liu Huihui Liu J.B.Liu J.L.Liu J.Y.Liu K.Liu K.Y.Liu Ke Liu L.Liu M.h.liu P.L.Liu Q.Liu S.B.Liu T.Liu W.K.Liu W.M.Liu X.Liu Y.Liu Y.B.Liu Z.A.Liu Z.Q.Liu X.C.Lou F.X.Lu H.J.Lu J.G.Lu X.L.Lu Y.Lu Y.P.Lu Z.H.Lu C.L.Luo M.X.Luo T.Luo X.L.Luo X.R.Lyu Y.F.Lyu F.C.Ma H.L.Ma L.L.Ma M.M.Ma Q.M.Ma R.Q.Ma R.T.Ma X.Y.Ma Y.Ma F.E.Maas M.Maggiora S.Maldaner S.Malde Q.A.Malik A.Mangoni Y.J.Mao Z.P.Mao S.Marcello Z.X.Meng J.G.Messchendorp G.Mezzadri H.Miao T.J.Min R.E.Mitchell X.H.Mo N.Yu.Muchnoi H.Muramatsu Y.Nefedov F.Nerling I.B.Nikolaev Z.Ning S.Nisar Y.Niu S.L.Olsen Q.Ouyang S.Pacetti X.Pan Y.Pan A.Pathak A.Pathak M.Pelizaeus H.P.Peng K.Peters J.Pettersson J.L.Ping R.G.Ping S.Plura S.Pogodin R.Poling V.Prasad F.Z.Qi H.Qi H.R.Qi M.Qi T.Y.Qi S.Qian W.B.Qian Z.Qian C.F.Qiao J.J.Qin L.Q.Qin X.P.Qin X.S.Qin Z.H.Qin J.F.Qiu S.Q.Qu S.Q.Qu K.H.Rashid C.F.Redmer K.J.Ren A.Rivetti V.Rodin M.Rolo G.Rong Ch.Rosner S.N.Ruan H.S.Sang A.Sarantsev Y.Schelhaas C.Schnier K.Schoenning M.Scodeggio K.Y.Shan W.Shan X.Y.Shan J.F.Shangguan L.G.Shao M.Shao C.P.Shen H.F.Shen X.Y.Shen B.-A.Shi H.C.Shi J.Y.Shi R.S.Shi X.Shi X.D Shi J.J.Song W.M.Song Y.X.Song S.Sosio S.Spataro F.Stieler K.X.Su P.P.Su Y.-J.Su G.X.Sun H.Sun H.K.Sun J.F.Sun L.Sun S.S.Sun T.Sun W.Y.Sun X Sun Y.J.Sun Y.Z.Sun Z.T.Sun Y.H.Tan Y.X.Tan C.J.Tang G.Y.Tang J.Tang L.Y Tao Q.T.Tao J.X.Teng V.Thoren W.H.Tian Y.Tian I.Uman B.Wang B.L.Wang D.Y.Wang F.Wang H.J.Wang H.P.Wang K.Wang L.L.Wang M.Wang M.Z.Wang Meng Wang S.Wang T.Wang T.J.Wang W.Wang W.H.Wang W.P.Wang X.Wang X.F.Wang X.L.Wang Y.D.Wang Y.F.Wang Y.H.Wang Y.Q.Wang Ying Wang Z.Wang Z.Y.Wang Ziyi Wang D.H.Wei F.Weidner S.P.Wen D.J.White U.Wiedner G.Wilkinson M.Wolke L.Wollenberg J.F.Wu L.H.Wu L.J.Wu X.Wu X.H.Wu Y.Wu Z.Wu L.Xia T.Xiang D.Xiao H.Xiao S.Y.Xiao Y.L.Xiao Z.J.Xiao X.H.Xie Y.Xie Y.G.Xie Y.H.Xie Z.P.Xie T.Y.Xing C.F.Xu C.J.Xu G.F.Xu Q.J.Xu S.Y.Xu X.P.Xu Y.C.Xu F.Yan L.Yan W.B.Yan W.C.Yan H.J.Yang H.L.Yang H.X.Yang L.Yang S.L.Yang Tao Yang Y.X.Yang Yifan Yang M.Ye M.H.Ye J.H.Yin Z.Y.You B.X.Yu C.X.Yu G.Yu T.Yu C.Z.Yuan L.Yuan S.C.Yuan X.Q.Yuan Y.Yuan Z.Y.Yuan C.X.Yue A.A.Zafar F.R.Zeng X.Zeng Y.Zeng Y.H.Zhan A.Q.Zhang B.L.Zhang B.X.Zhang D.H.Zhang G.Y.Zhang H.Zhang H.H.Zhang H.H.Zhang H.Y.Zhang J.L.Zhang J.Q.Zhang J.W.Zhang J.X.Zhang J.Y.Zhang J.Z.Zhang Jianyu Zhang Jiawei Zhang L.M.Zhang L.Q.Zhang Lei Zhang P.Zhang Q.Y.Zhang Shulei Zhang X.D.Zhang X.M.Zhang X.Y.Zhang X.Y.Zhang Y.Zhang Y.T.Zhang Y.H.Zhang Yan Zhang Yao Zhang Z.H.Zhang Z.Y.Zhang Z.Y.Zhang G.Zhao J.Zhao J.Y.Zhao J.Z.Zhao Lei Zhao Ling Zhao M.G.Zhao Q.Zhao S.J.Zhao Y.B.Zhao Y.X.Zhao Z.G.Zhao A.Zhemchugov B.Zheng J.P.Zheng Y.H.Zheng B.Zhong C.Zhong X.Zhong H.Zhou L.P.Zhou X.Zhou X.K.Zhou X.R.Zhou X.Y.Zhou Y.Z.Zhou J.Zhu K.Zhu K.J.Zhu L.X.Zhu S.H.Zhu T.J.Zhu W.J.Zhu Y.C.Zhu Z.A.Zhu B.S.Zou J.H.Zou 《Chinese Physics C》 SCIE CAS CSCD 2022年第11期64-75,共12页
From December 2019 to June 2021,the BESⅢ experiment collected approximately 5.85 fb^(−1) of data at center-of-mass energies between 4.61 and 4.95 GeV.This is the highest collision energy BEPCⅡ has reached to date.Th... From December 2019 to June 2021,the BESⅢ experiment collected approximately 5.85 fb^(−1) of data at center-of-mass energies between 4.61 and 4.95 GeV.This is the highest collision energy BEPCⅡ has reached to date.The accumulated e^(+)e^(−) annihilation data samples are useful for studying charmonium(-like)states and charmed-hadron decays.By adopting a novel method of analyzing the production of A_(c)^(+)A_(c)^(-) pairs in e^(+)e^(−) annihilation,the center-of-mass energies are measured with a precision of 0.6 MeV.Integrated luminosities are measured with a precision of better than 1% by analyzing the events of large-angle Bhabha scattering.These measurements provide important inputs to analyses based on these data samples. 展开更多
关键词 LUMINOSITY center-of-mass energy BESⅢdetector
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