SWIP—RFP装置慢斜升放电的反场箍缩实验

在硅化后的良好器壁条件下，采用慢斜升放电模式，获得了具有高电流密度和较高温度的反场箍缩（ＲＦＰ）等离子体，在实验中观测到磁通长时间的持续增长，随等离子体电流增大而增大，并出现与环向磁通相伴的ＭＨＤ扰动现象，实验证实，斜升放电的ＲＦＰ等离子体存在“发电机”效应，ＲＦＰ位形维持时间长达８００μｓ，等离子体电流约１００ｋＡ，电子和离子温度分别达到７０ｅＶ和８５ｅＶ。     

Ge：SiO2的光敏缺陷的研究

研究了Ｇｅ；ＳｉＯ２光敏缺陷的特性，分别在４８８ｎｍＡｒ离子激光与１９３ｎｍＡｒ准分子激光作用下，由紫外吸收带，激光荧光的测量实验及电子自旋共振实验，发现光纤中５．１ｅＶ锗缺陷吸收带实验上是由５．０６ｅＶ可光致漂白带与５．１７ｅＶ不可漂白带组成；２９５ｎｍ的激发荧光与５．０６ｅＶ的缺氧锗缺陷对应，随５．０６ｅＶ缺陷吸收带的漂白而衰减；     

在Si衬底上异质外延GaAs薄膜变激发强度的近红外光致发光

通过对用ＭＯＣＶＤ（金属有机物化学气相沉积）方法在Ｓｉ衬底上生长的ＧａＡｓ外延薄膜，用不同激发强度下的近红外光致发光研究了液氮温度下峰值能量为１．１３ｅＶ和１．０４ｅＶ两个带谱的发光特性，表明这两个带均属于施主－受主对复合发光。由于发光带中存在着电子－声子耦合，所以应在施主－受主对复合发光能量表示式中计及Ｆｒａｎｋ－Ｃｏｎｄｏｎ位移，从而对复合发光能量表示式进行修正。通过对复合发光带能量随激发强度变化的实验曲线和理论表达式的拟合，确定了峰值为１．１３ｅＶ与１．０４ｅＶ这两个发光带深施主－受主对的束缚能之和分别为０．３００ｅＶ和０．４０１ｅＶ。     

会议消息

会议消息ＦＩＦＴＨＩＮＴＥＲＮＡＴＩＯＮＡＬＣＯＮＧＲＥＳＳＯＮＳＯＵＮＤＡＮＤＶＩＢＲＡＴＩＯＮ￥ＵｎｉｖｅｒｓｉｔｙｏｆＡｄｅｌａｉｄｅ，ＳｏｕｔｈＡｕｓｔｒａｌｉａＤｅｃ．１５～１８３１９９７第五届国际声和振动会议将于１９９７年１２月１５～１８...     

百焦耳级KrF准分子激光实验

介绍闪光Ⅱ号加速器泵浦的百焦耳级氟化氢激光研制情况，给出了激光器的构造和主要性能。在二极管电压为８４０ｋＶ，电流为２００ＫＡ条件下，获得了１５７Ｊ的最大激光能量，峰值功率为２．０ＧＷ。研究了激光输出能量随Ｆ２和Ｋｆ气体浓度的变化规律．     

一种不含自由参数的正电子吸收势

在准自由电子气模型的基础上得到一种不含自由参数的正电子吸收势，把它作为光学势的虚部，计算了能量在最小非弹性阀值到１００ｅＶ范围内正电子被Ｈｅ、Ｎｅ、Ａｒ原子散射的总截面和能量为２００ｅＶ和３００ｅＶ时的散射微分截面，计算结果与实验进行了比较。     

SG－1 FEL放大器实验初步分析

在摇摆场０．２６Ｔ，电子束能量３．３±０．１５ＭｅＶ，束流约６００Ａ时，ＳＧ－１ＦＥＬ常参数放大器实验最大功率约１０ＭＷ，指数增益约１９ｄＢ／ｍ。对实验进行了初步的分析讨论，并就实验时４ｍ长摇摆器功率未呈饱和、指数增益区右移现象与下一轮实验的改进提出了意见。     

喷气式Z箍缩等离子体装置中离子束能谱的测量

利用新研制的紧凑型汤姆生离子能谱仪（ＴｈｏｍｓｏｎＩｏｎＥｎｅｒｇｙＡｎａｌｙｚｅｒ），对喷气式Ｚ－箍缩等离子体装置中离子能谱进行了测量，在ＣＲ－３９上得到了清晰的Ａｒ＋，Ａｒ２＋，Ａｒ３＋离子抛物线轨迹，通过分析计算结果表明：离子的最大能量在１ＭｅＶ左右，离子能谱分布曲线都随其能量增加而单调下降。     

极端相对论性核碰撞中的奇异重子与QGP讯号

用带有弦集体相互作用和再散射的Ｆｒｉｔｉｏｆ程序新版，计算了Ｓ（２００ＧｅＶ／ｃ）＋Ｐｂ反应中奇异重子与反重子的比值．和的理论值和相应实验数据，在实验数据彼此偏差的范围内相符合．这表明：奇异重子与反重子的比值在强子背景下可能得到解释．     

HIRFL—CSR电子冷却系统

建议中的兰州重离子加速器冷却贮存环（ＨＩＲＦＬ－ＣＳＲ）拟采用电子冷却方法将重离子束冷却到３００ＭｅＶ／ｕ。最高电子能量为１６５ｋｅＶ，最大电子电流密度主０．２４４Ａ／ｃｍ＾２，叙述了ＣＳＲ电子冷却装置的初步方案。     

Rapidity distributions and energy densities from hydrodynamical studies at 5–200 GeV/n

3+1 dimensional relativistic calculations of the space-time evolution of heavy ion collisions at bombarding energies from 5 to 200 GeV/n are presented. Collisions with heavier projectiles seem to be more rewarding to form extended regimes of highly excited nuclear matter containing enough baryons for a sufficient time span to enable a transition of the hadron matter into a quark gluon plasma. A strong impact parameter dependence has to be taken into account when comparing the final baryon rapidity distributions with experimental results. Experimental results of the reactions¹⁶O(60, 200 GeV/n)→Pb are compared with hydrodynamical calculations.     

Charged-particle multiplicity distributions in different rapidity windows in 800 GeV proton-nucleus interactions

Multiplicity distributions of charged particles produced in interactions of 800 GeV protons with emulsion nuclei in various rapidity windows are presented. The data is also analyzed separately for the forward and the backward hemispheres, for rapidity windows of different widths. It is found that the Negative Binomial Distribution (NBD) describes well the multiplicity distribution of secondary particles in various rapidity windows and also in both the hemispheres. We have compared the NBD parameters, in both the hemispheres, at 200 GeV and 360 GeV, with those at 800 GeV. The behaviour of NBD parameters in rapidity windows of different widths and for different targets has also been studied. Received: 30 August 2001 / Accepted: 28 January 2002     

Evolution of the nuclear modification factors with rapidity and centrality in d + Au collisions at (sqrt)[N(S)N]=200 GeV

We report on a study of the transverse momentum dependence of nuclear modification factors R(dAu) for charged hadrons produced in deuteron + gold collisions at sqrt[s(NN)]=200 GeV, as a function of collision centrality and of the pseudorapidity (eta=0, 1, 2.2, 3.2) of the produced hadrons. We find a significant and systematic decrease of R(dAu) with increasing rapidity. The midrapidity enhancement and the forward rapidity suppression are more pronounced in central collisions relative to peripheral collisions. These results are relevant to the study of the possible onset of gluon saturation at energies reached at BNL RHIC.     

相对论重离子碰撞中的热解冻和纵向非均匀集体膨胀流

把非均匀纵向流模型推广到包括横向膨胀流,并计算K介子,Λ和质子的快度分布.这些模型的计算结果能较好地解释CERN/SPS 200A GeV/c能量下S-S碰撞以及158A GeV/c能量下Pb-Pb碰撞的实验结果.并且能够自然地解释实验中出现的中心下凹(centraldip)现象.     

高能不等核碰撞和弛豫时间的相对论动力论方程描述

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200A GeV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.     

Nuclear stopping in Au+Au collisions at square root of S(NN)=200 GeV

Transverse momentum spectra and rapidity densities, dN/dy, of protons, antiprotons, and net protons (p-p) from central (0%-5%) Au+Au collisions at square root of S(NN)=200 GeV were measured with the BRAHMS experiment within the rapidity range 0相似文献   

强子-强子碰撞的快度关联花样

本文利用强子-强子碰撞的PYTHIA模型, 模拟了质心系能量为s=22, 200GeV的质子-质子碰撞. 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. 结果发现, 相邻bin的快度关联在中心快度区最强, 向边缘区逐渐减弱; 固定bin和任意bin的关联在固定bin取不同快度位置时, 具有不同的花样.     

Target fragmentation in proton-nucleus and16O-nucleus reactions at 60 and 200 GeV/nucleon

Target remnants withZ<3 from proton-nucleus and¹⁶O-nucleus reactions at 60 and 200 GeV/nucleon were measured in the angular range from 30° to 160° (?1.7<η<1.3) employing the Plastic Ball detector. The excitation energy of the target spectator matter in central oxygen-induced collisions is found to be high enough to allow for complete disintegration of the target nucleus into fragments withZ<3. The average longitudinal momentum transfer per proton to the target in central collisions is considerably higher in the case of¹⁶O-induced reactions (≈300 MeV/c) than in proton-induced reactions (≈130 MeV/c). The baryon rapidity distributions are roughly in agreement with one-fluid hydrodynamical calculations at 60 GeV/nucleon¹⁶O+Au but are in disagreement at 200 GeV/nucleon, indicating the higher degree of transparency at the higher bombarding energy. Both, the transverse momenta of target spectators and the entropy produced in the target fragmentation region are compared to those attained in head-on collisions of two heavy nuclei at Bevalac energies. They are found to be comparable or do even exceed the values for the participant matter at beam energies of about 1–2 GeV/nucleon.     

Charged particle multiplicity distributions at 200 and 900 GeV c.m. energy

Multiplicity distributions of charged particles produced in non single-diffractive collisions between protons and antiprotons at centre of mass energies of 200 and 900 GeV are presented. The data were recorded in the UA5 streamer chambers at the CERN Collider, which was operated in a pulsed mode between the two energies. A new method to correct for acceptance limitations and inefficiencies based on the principle of maximum entropy has been used. Multiplicity distributions in full phase space and in intervals of pseudorapidity are presented in tabular form. The violation of KNO scaling in full phase space found by the UA5 group at an energy of 546 GeV is confirmed also at 200 and 900 GeV. The shape of the 900 GeV distribution in full phase space is narrower in the peak region than at 200 GeV but exhibits a pronounced high multiplicity tail. The negative binomial distribution fits data at 200 GeV in all pseudorapidity intervals and in small intervals at 900 GeV. In large intervals at 900 GeV, however, the negative binomial distribution. Fits to the partially coherent laser distribution are also presented as well as comparisons with predictions of the Dual Parton, the Fritiof and the Pythia models.     

Interferometry of pions and kaons in high energy collisions

A hydrodynamic model which reproduces the observed rapidity and transverse momentum spectra of mesons and baryons is applied to the study of Bose-Einstein correlations. The pion correlations are found to be strongly affected by resonance decays, except for pairs of large transverse momenta.For S+S at 200 A GeV, in the central rapidity region the effective longitudinal source radii for pions and kaons differ by a factor of 2, the transverse radii by a factor of 1.3. The lifetime of the source can be extracted from kaon interferometry.