1) Quick Algorithm
快度算法
2) rapidity
快度
1.
Particle Rapidity and Pseudorapidity Distributions in Ideal Gas Model;
理想气体模型中粒子的快度与赝快度分布
2.
The change of rapidity distribution after particles identification is found.
发现了粒子鉴别前后两种实验事件快度分布的变化。
3.
It has been found that the neighboring bin correlations are the strongest at the central rapidity region and become weaker and weaker toward the two side rapidity regions; while the fixed-to-arbitrary bin correlations vary from one fixed bin to another.
研究了快度空间中末态粒子在固定bin和任意bin中,以及相邻bin中的关联花样。
3) rapidity distribution
快度分布
1.
The rapidity distribution of protons produced in nucleus-nucleus collisions at the Alternating Gradient Synchrotron (AGS) and the Super Proton Synchrotron(SPS) energies are analyzed by the three-fireball model.
用三火球模型分析了核-核以AGS(the Alternating Gradient Synchrotron)和SPS(the Super Proton Synchrotron)能量碰撞中产生质子的快度分布。
2.
It is shown that the rapidity distribution at RHIC-LHC energy region for the cases with and without phase transition will be much different in shapes This result suggests that the shape of rapidity distribution may be used as a possible signal for quark matter formation.
用流体动力学模型研究一维流体的集体效应和相变对末态粒子分布的影响，结果表明：在ＲＨＩＣ－ＬＨＣ能区有相变和无相变时的末态快度分布形状是很不相同的，预计快度分部的形状可作为夸克物质形成的信号。
3.
The △ resonance effects on the rapidity distributions of proton and pion and on the transverse mass distribution of proton are investigared.
研究了共振态对质子π的快度分布以及质子横质量分布的影响。
4) Pseudorapidity
赝快度
1.
Particle Rapidity and Pseudorapidity Distributions in Ideal Gas Model;
理想气体模型中粒子的快度与赝快度分布
2.
Pseudorapidity Distribution of Charged Particles in High-Energy Nucleus-Nucleus Collisions;
高能核-核碰撞中带电粒子的赝快度分布(英文)
3.
Measurement of Pseudorapidity Distributions and Study of Particle Number Densities in pp Collisions at 400 GeV/c;
400GeV／c pp碰撞赝快度分布测量和粒子数密度的研究
5) rapidity cut
快度截断
1.
Using the rapidity cut techniqu at fixed multiplicity N the p ⊥/〈 p ⊥〉 distribution at S =5?GeV is coincided with that of a hadrom source at S =1?800?GeV,where -2γ B (g R )=0.
非微扰（短距离） 量子场论的横动量标度分布Ｑ－ ｖ⊥ Ｋν（β⊥ Ｑ⊥／〈Ｑ⊥〉） 与实验数据（ Ｓ＝ ５ ～１ ８００ＧｅＶ）符合得很好，在固定多重数Ｎ 用快度截断技术后的质量证认数据（ 单个强子源， Ｓ＝ １ ８００ ＧｅＶ） 与低能ｐ⊥－ 分布重合（ Ｓ＝ ５ＧｅＶ） ，低能ｐ⊥－ 分布反常的困难消失。
6) large rapidity gap (LRG)
大快度gap
参考词条
补充资料：快堆(见快中子增殖堆)
快堆(见快中子增殖堆)
fast-breeder reactor
l快堆堆。(fast一breeder reaetor)见快中子增殖
说明：补充资料仅用于学习参考，请勿用于其它任何用途。