60AGeV 16 O诱发乳胶核反应α射弹碎片发射研究

对60AGeV^16O诱发乳胶核反应射弹α碎片的发射进行了研究，得到α射弹碎片多重数分布服从KNO标度无关性。在边缘作用下，α射弹碎片的产生与靶核碎片的产生存在线性关联，靶核碎片平均多重数随α射弹碎片数的增加线性减小，它可以很好地利用核作用几何模型来解释。     

60AGeV 16O诱发乳胶核反应α射弹碎片发射研究

对60AGeV 16 O诱发乳胶核反应射弹α碎片的发射进行了研究,得到α射弹碎片多重数分布服从KNO标度无关性. 在边缘作用下,α射弹碎片的产生与靶核碎片的产生存在线性关联,靶核碎片平均多重数随α射弹碎片数的增加线性减小,它可以很好地利用核作用几何模型来解释.     

60 A GeV16O原子核在核乳胶中的电磁离解

对60 A GeV16O在原子核乳胶中的电磁离解现象首次进行了高统计的研究,得到电磁离解截面随束流能量的增加而增加,射弹碎片电荷分布和200 A GeV16O在乳胶中电磁离解的电荷分布一致,但电荷为3≤Z≤5的射弹碎片的发射概率低于200 A GeV能区,这些特点和Weiszacker和Williams的经典电磁理论模型计算结果一致.60 A GeV16O电磁离解下各反应道出现的概率和200 A GeV能区结果基本一致,但同14.6 A GeV能区的结果不同,在60 A GeV能区16O电磁离解主要是由电偶及电四激发引起的巨偶极和巨四极共振及准氘核效应过程所致,这一点可以通过电磁离解下质子的多重数分布得到定性解释.电磁离解下α射弹碎片的分布同非弹核作用下α碎片的分布规律不同,说明α碎片的产生机制不同.     

60 A GeV16O原子核在核乳胶中的电磁离解

对60 A GeV¹⁶O在原子核乳胶中的电磁离解现象首次进行了高统计的研究,得到电磁离解截面随束流能量的增加而增加,射弹碎片电荷分布和200 A GeV¹⁶O在 乳胶中电磁离解的电荷分布一致,但电荷为3≤Z≤5的射弹碎片的发射概率低于200 A GeV能 区,这些特点和Weiszacker和Williams的经典电磁理论模型计算结果一致.60 A GeV¹⁶ O电磁离解下各反应道出现的概率和200 A GeV能区结果基本一致,但同14.6 关键词： 电磁离解 射弹碎片 碎裂     

核乳胶中1.4A GeV~(84)Kr的相互作用自由程和射弹α-碎片多重数分布

本文报告了关于1.4A GeV ~(84)Kr与乳胶核碰撞的相互作用自由程分布和射弹α-碎片多重数分布的初步测量结果.     

核乳胶中1.4A GeV 84Kr的相互作用自由程和射弹α-碎片多重数分布

本文报告了关于1.4A GeV ⁸⁴Kr与乳胶核碰撞的相互作用自由程分布和射弹α-碎片多重数分布的初步测量结果.     

30MeV/u 40Ar+natAg反应中中等质量碎片的发射时标

采用强度干涉技术,研究了30MeV/u ⁴⁰Ar+^angAg反应中IMF-IMF关联的实验结果.利用三体弹道模型从约化速度关联函数提取了中等质量碎片的发射时间.中等质量碎片的平均发射时间随其能量而变化,从低能时的约300fm/c下降到高能时的约100fm/c.扣除类弹碎片的贡献后,得到此反应发射中途中等质量碎片的平均发射时间约为250fm/c,表明此反应发射的中等质皇碎片主要来自于相继两体衰变.     

全浸水带间隙发射高速射弹的入水冲击载荷分析

全浸水带间隙发射方式可以将发射环境由水介质转化为气体介质。为了研究高速射弹在此条件下的入水冲击载荷,建立了射弹入水冲击载荷的理论模型。针对射弹在入水速度、头部锥角和入水攻角不同情况下的入水冲击载荷进行了计算,分析了入水速度、射弹头部参数和入水攻角对冲击载荷的影响。研究结果对全水下高速射弹入水冲击载荷的预测和射弹头部结构的设计具有重要意义。     

一种针对高速小目标的偏航角测算方法

射弹偏航角是影响电磁轨道发射装置发射精度的关键参数,为实时、高精度测量射弹偏航角,提升电磁轨道发射装置发射精度,基于双目视觉原理提出一种无需目标速度的射弹偏航角测算方法。利用高速射弹轨迹图像,通过构建像机线性成像模型解算高速射弹图像坐标,实现目标偏航角的测量。分析了光学系统参数对测量精度的影响,理论误差约为14.5 μrad。偏航角测量实验结果表明该方法能够实时、准确测算射弹偏航角,测算量偏差平均值为0.58 mrad。     

30MeV/u~(40)Ar ~(159)Tb反应中中等质量碎片的发射时标与发射机制

报道３０ＭｅＶ／ｕ４０Ａｒ＋１５９Ｔｂ反应中碎片碎片关联函数的实验结果．利用三体弹道模型从关联函数提取了中等质量碎片发射时间．中等质量碎片的平均发射时间随碎片能量而变化，从低能时的约５００ｆｍ／ｃ下降至高能时的约１００ｆｍ／ｃ．中等质量碎片发射时间随束流能量的升高而下降，表明随着束流能量的升高中等质量碎片发射机制逐渐从相继两体衰变向多重碎裂发射过渡．对于４０Ａｒ＋１５９Ｔｂ反应，此过渡能区在３５—４５ＭｅＶ／ｕ之间     

Top quark mediated Higgs boson decay into hadrons to order alphas5

We present in analytic form the O(alphas5) correction to the H-->gg partial width of the standard-model Higgs boson with an intermediate mass MH<2Mt. Its knowledge is useful because the O(alphas4) correction is sizable (around 20%). For MH=120 GeV, the resulting QCD correction factor reads 1+(215/12)alphas(5)(MH)/pi+152.5[alphas(5)(MH)/pi]2+381.5[alphas(5)(MH)/pi]3 approximately 1+0.65+0.20+0.02. The new four-loop correction increases the total Higgs-boson hadronic width by a small amount of order 1 per thousand and stabilizes significantly the residual scale dependence.     

Order alphas4 QCD corrections to Z and tau decays

Using recently developed methods for the evaluation of five-loop amplitudes in perturbative QCD, corrections of order alphas4 for the nonsinglet part of the cross section for electron-positron annihilation into hadrons and for the decay rates of the Z boson and the tau lepton into hadrons are evaluated. The new terms lead to a significant stabilization of the perturbative series, to a reduction of the theory uncertainly in the strong coupling constant alphas, as extracted from these measurements, and to a small shift of the central value, moving the two central values closer together. The agreement between two values of alphas measured at vastly different energies constitutes a striking test of asymptotic freedom. Combining the results from Z and tau decays we find alphas(MZ)=0.1198+/-0.0015 as one of the most precise and presently only result for the strong coupling constant in order alphas4.     

Strong-coupling constant with flavor thresholds at five loops in the modified minimal-subtraction scheme

We present in analytic form the matching conditions for the strong-coupling constant alphas(nf) (mu) at the flavor thresholds to four loops in the modified minimal-subtraction scheme. Taking into account the present knowledge on the coefficient beta4 of the Callan-Symanzik beta function of quantum chromodynamics, we thus derive a five-loop formula for alphas(nf) (mu) together with appropriate relationships between the asymptotic scale parameters Lamda(nf) for different numbers of flavors nf.     

Radial diffusion of toroidally trapped particles induced by lower hybrid and fast waves

The paper brings analytical estimates of induced radial diffusion of alphas and ions, caused by their interaction with lower hybrid and fast waves.     

Two source emission behavior of projectile fragments alpha in 84Kr interactions at around 1 GeV per nucleon

The emission of projectile fragments alpha has been studied in ⁸⁴Kr interactions with nuclei of the nuclear emulsion detector composition at relativistic energy below 2 GeV per nucleon. The angular distribution of projectile fragments alpha in terms of transverse momentum could not be explained by a straight and clean-cut collision geometry hypothesis of Participant — Spectator (PS) Model. Therefore, it is assumed that projectile fragments alpha were produced from two separate sources that belong to the projectile spectator region differing drastically in their temperatures. It has been clearly observed that the emission of projectile fragments alpha are from two different sources. The contribution of projectile fragments alpha from contact layer or hot source is a few percent of the total emission of projectile fragments alphas. Most of the projectile fragments alphas are emitted from the cold source.     

The third particle in deep inelastic collisions

Angular correlations between charged reaction products have been measured for the reaction¹⁴N+²⁷A1 at 70 and 100 MeV. Light particle evaporation from the heavy recoil is shown to be the dominant process. In addition, however fast alphas are observed for all reaction channels. From the three-body kinematics we conclude that these alphas are emitted from the contact zone between the two heavy ions. A comparison of the results forE _Lab=70 and 100 MeV excludes an explanation of this process by the recently suggested “Piston” or “hot-spot” models.     

Detection of fusion alphas from D2-T2 gas targets

Detectors for recording alphas from fusions in D₂–T₂ gas targets require protection against diffusion of tritium into the detector medium. Tests have been carried out on surface barrier detectors to determine the feasibility of using thin coatings of oxide and metal for this purpose. The results show that a layer of 0.5 m aluminium oxide plus 0.2 m gold provides effective protection for at least 280 h, without impairing the transmission of 2 MeV alphas into the detector. Tests of an alternative detector, a phoswich of thin film plastic and lithium-glass scintillators, are also described.     

Coherent dissociation of oxygen into four alphas in photoemulsion at 4.5 A GeV/c

The search for and study of the coherent dissociation reaction ¹⁶O → 4 have been made at 4.5 GeV/c per nucleon in emulsion. The momentum and correlation characteristics of alphas cannot be described by the statistical model of prompt fragmentation. The decay “temperature” is considerably smaller than one for the usual multifragmentation of relativistic projectiles.     

稳态托卡马克堆中的自举电流

在稳态托卡马克堆的燃烧阶段,当感应电流下降后,新经典输运产生的自举电流便成为维持稳定电流的最好手段。本文根据α粒子新经典自举电流的最新结果,计算了感应电流消失阶段,稳态堆中α粒子、电子和离子的自举电流。     

Inclusive and exclusive measurements in the projectile breakup of 7Li

The inclusive and exclusive measurements were carried out for ⁷Li projectile breakup on ²⁷Al target at 48 MeV. In the inclusive data we have observed a broad peak around the beam velocity for alphas and tritons. The exclusive data for alpha-triton coincidences show good agreement with the post-form DWBA theory of breakup reactions.