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 central rapidity region 中心快度区(1)
 中心快度区
 Dilepton Invariant Mass Distribution in Central Rapidity Region 中心快度区的双轻子不变质量分布 短句来源
 “central rapidity region”译为未确定词的双语例句
 Transport Coefficients and Viscous Hydrodynamical Evolution of Hadron Matter in the Central Rapidity Region 快度中心区强子物质输运系数和粘滞流体演化 短句来源 The transverse energy distribution in central rapidity region at both CERN and BNL energy domains are calculated. 计算了CERN和BNL两个能区的中心快度横能分布,成功地解释了高能时横能分布随靶核质量增加的加宽和低能时的饱和。 短句来源 THE CALCULATION OF TRANSVERSE ENERGY DISTRIBUTION IN CENTRAL RAPIDITY REGION AND THE STUDY OF MECHANISM OF HIGH-ENERGY HEAVY-ION COLLISIONS 中心区横能分布的多源模型计算和高能重离子碰撞机制探讨 短句来源 We predict that XcJ mesons at low transverse momentum in the central rapidity region are almost dissociated by nucleons and antinucleons in hadronic matter. So this results predict a great contribution to the total J/ suppression. 研究表明在中心快度区域，具有较小横动量的xcJ几乎完全被强子物质中的核子、反核子离解，因此对整个J/叻抑制有很大的贡献。 短句来源 The last two parts are the calculations for quantities in RHIC energy. Through calculations, the temperature is obtained to be 161MeV in central rapidity region, and baryon chemical potential to be 22MeV, strangeness chemical potential to be 4.8MeV. The net baryon density is obtained to be 0.0083fm~3. The temperature is close to the temperature in SPS energy region, but quite faraway from the former predicted temperature in RHIC energy region, so it needs further study. 在最后两部分对RHIC能量的研究中,获得中心快度温度为160MeV,重子化学势为22MeV,奇异子化学势为4.8MeV,另外获得净重子密度为0.0083/fm~3。 这个温度与在SPS能量下获得的温度相近,而和原先预测的RHIC能量下的结果(170MeV以上)相差比较远,因此需要进一步研究。 短句来源 更多
 相似匹配句对
 Dilepton Invariant Mass Distribution in Central Rapidity Region 中心快度区的双轻子不变质量分布 短句来源 On the Strategic Orientation of the Central Region 论中部地区的战略定位 短句来源 There was translocation in central optical region. 中心光学区均存在不同程度移位； 短句来源 Transport Coefficients and Viscous Hydrodynamical Evolution of Hadron Matter in the Central Rapidity Region 快度中心区强子物质输运系数和粘滞流体演化 短句来源 The transverse energy distribution in central rapidity region at both CERN and BNL energy domains are calculated. 计算了CERN和BNL两个能区的中心快度横能分布,成功地解释了高能时横能分布随靶核质量增加的加宽和低能时的饱和。 短句来源

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 central rapidity region
 Back-reaction of the partons with the field is included and a model transport equation containing a collision term is solved for the central rapidity region based on an approximation in which the partons relax to a thermal distribution. A very important question in ultrarelativistic heavy ion collisions is that of thermalization of the high energy density quark gluon plasma forud in the central rapidity region. Differential cross sections as a function of transverse momentum and Feynman's x variable are given for the central rapidity region and for transverse momenta up to pT=3.5?GeV/c. Differential cross sections as a function of rapidity and transverse momentum have been measured in the central rapidity region and for transverse momenta up to pT = 3.5?GeV/c. Our new formulae are applied to a numerical study of the pattern of $J/\psi$ suppression in the central rapidity region at RHIC/LHC energies. 更多
 By analysing the collisions of the high-energy non-equal nuclei,the author proposed a mechanism- of collisions of nucleus-nucleus,And calculated the transverse energy distribution of oxygen-nuclei col- lisions at 200A.GeV and 60 A.GeV in central rapidity region though multi-source model.The result fit the experiment date very well. 本文在深入分析高能不等核碰撞过程的基础上,提出了核—核碰撞的一种碰撞机制.并结合多源模型作计算,成功地符合了200GeV/核子和60GeV/核子的~(16)O 打不同靶核的中心快度区的横能分布. Based on a careful analysis of the mechanism of high energy non-equal mass nuclei collisions, the multisource modle is further developed. The transverse energy distribution in central rapidity region at both CERN and BNL energy domains are calculated. The saturation of transverse energy distribution at low cnergy is explained, and the minimum mass number of the target nucleus for this saturation effect (full stopping) to occur is obtained. 本文在深入分析高能不等核碰撞机制的基础上,进一步发展多源模型。计算了CERN和BNL两个能区的中心快度横能分布,成功地解释了高能时横能分布随靶核质量增加的加宽和低能时的饱和。给出了横能分布达到饱和(完全核阻止)的靶核质量。 In this paper, the time development of high energy heavy ion collision are described by the relativistic kinetic equation. The rapidity distribution of the final state particles under 200A GeV 16O and 32S particles beams are analysed in the central rapidity region. The various system relaxation time are determined. 本文用相对论动力论方程描述高能重离子碰撞时空演化，并用它分析在２００ＡＧｅＶ的１６Ｏ束流和３２Ｓ束流下，于快度中心区的末态粒子快度分布，确定了不同系统的弛豫时间． << 更多相关文摘
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