General SU(2)(L) x SU(2)(R) x U(1)(EM) sigma model with external sources, dynamical breaking and spontaneous vacuum symmetry breaking

We give a general SU(2)(L) x SU(2)(R) x U(1)(EM) sigma model with external sources, dynamical breaking and spontaneous vacuum symmetry breaking, and present the general formulation of the model. It is found that sigma and pi(0) without electric charges have electromagnetic interaction effects coming front the internal structures. A general Lorentz transformation relative to external sources J(gauge) - (J(A mu) J(A mu)(kappa)) derived, using the general Lorentz transformation and the four-dimensional current of nuclear matter of the ground si ate with J(gauge) = 0, we give the four-dimensional general relations between the different currents of nuclear matter systems with J(gauge) not equal 0 and those with J(gauge) = 0. The relation of the density's coupling with external magnetic field is derived, which conforms well to dense nuclear matter in a strong magnetic field. We show different condensed effects in strong interaction about fermions and antifermions, and give the concrete scalar and pseudoscalar condensed expressions of sigma(0) and pi(0) bosons. About different dynamical breaking and spontaneous vacuum symmetry breaking, the concrete expressions of different mass spectra are obtained in field theory. This paper acquires the running spontaneous vacuum breaking value sigma'(0), and obtains the spontaneous vacuum breaking in tenus of the running sigma'(0), which make nucleon, sigma, and pi particles gain effective masses. We achieve both the effect of external sources and nonvanishing value of the condensed scalar and pseudoscalar paticles. It is deduced that the masses of nucleons, sigma and pi generally depend on different external sources.

Production cross-section of Th-236 in the interaction of U-238 with 60MeV/u O-18 Ions

The neutron-rich target-like isotope Th-236 was produced in U-238-2p multinucleon transfer reaction between a 60MeV/u O-18 beam and nature U-238 targets. The thorium activities were radiochemically separated from the mixture of uranium and reaction products. The isotope Th-236 was identified by 642.2keV, 687.6keV and 229.6keV characteristic gamma-rays. The production cross section of Th-236 has been determined to be 250 +/- 50 mu b.

Effects of annealing on the photoluminescence of He ion implanted sapphire after 230-MeV Pb ion irradiation

Single crystal sapphire (Al2O3) samples implanted with 110 keV He and irradiated at 320 K by Pb-208(27), ions with energy of 1.1 MeV/u to the fluences ranging from 1 X 10(12) to 5 X 10(14) ion/cm(2) and subsequently annealed at 600, 900 and 1100 K. The obtained PL spectra showed that emission peaks centred at 375, 390, 413, and 450 nm appeared in irradiated samples. The peak of 390 ran became very intense after 600 K annealing. The peak of 390 nm weakened and 510 nm peak started to build up at 900 K annealing, the peak of 390 nm vanished and 510 nm peak increased with the annealing temperature rising to 1100 K. Infrared spectra showed a broadening of the absorption band between 460 cm(-1), and 510 cm(-1) indicating strongly damaged regions being formed in the Al2O3 samples and position shift of the absorption band at 1000-1300 cm(-1) towards higher wavenumber after Pb irradiation.

Multi-electron processes in C-13(6+) ions with neon collisions in energy region 4.15-11.08 keV/u

The cross-section ratios of double-, triple-, quadruple-, and the total multi-electron processes to the single electron capture process sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC)) as well as the relative ratios among reaction channels in double-electron active, triple-electron active and quadruple- electron active are measured in C-13(6+) -Ne collision in the energy region of 4.15-11.08 keV/u by employing position-sensitive and time-of-flight coincident techniques. It is determined that the cross-section ratios sigma(DE)/sigma(SC), sigma(TE)/sigma(SC), sigma(QE)/sigma(SC) and sigma(ME)/sigma(SC) are approximately the constants of 0.20 +/- 0.03, 0.16 +/- 0.04, 0.06 +/- 0.02 and 0.42 +/- 0.05. These values are obviously smaller than the predictions of the molecular Coulomb over-the-barrier model (MCBM) [J. Phys. B 23 (1990) 4293], the extended classical over-the-barrier model (ECBM) [J. Phys. B 19 (1986) 2925] and the semiempirical scaling laws (SL) [Phys. Rev. A 54 (1996) 4127]. However, the relative ratios among partial processes of DE, TE and QE are found to depend on collision energy, which suggests that the collision dynamics depends on the collision velocity. The limitation of velocity-independent character of ECBM, MCBM and SL is undoubtedly shown.

单次分子镀法制备部分La系及~(238)U靶的实验研究

采用单次分子镀方法研究了异丙醇-硝酸体系中电流密度、分子镀持续时间及两极间距离对镀层性能和电沉积效率的影响,确定了制备La,Sm,Eu,Gd,Tb靶及238U靶的最佳工艺条件。因制备的靶不同,电流密度一般介于2—8mA/cm2之间,两极间最优距离为3cm,分子镀1h,用分光光度法测定各靶的沉积效率均高于85%。利用扫描电子显微镜(SEM)对部分靶的表面形貌分析后发现靶面结构均匀致密。目前制得的Gd靶和Tb靶已用于中国科学院近代物理研究所加速器SFC低能核化学终端上,利用19F束流轰击,分别产生了Ta和W的短寿命同位素,从而成功完成了Db(Z=105)及Sg(Z=106)的模型试验。

Experimental study of the U-238(S-36,3-5n)(269-271)Hs reaction leading to the observation of (270)Hs

The deformed doubly magic nucleus (270)Hs has so far only been observed as the four-neutron (4n) evaporation residue of the reaction Mg-26+Cm-248, where a maximum cross section of 3 pb was measured. Theoretical studies on the formation of (270)Hs in the 4n evaporation channel of fusion reactions with different entrance channel asymmetry in the framework of a two-parameter Smoluchowski equation predict that the reactions Ca-48+Ra-226 and S-36+U-238 result in higher cross sections due to lower reaction Q values, in contrast to simple arguments based on the reaction asymmetry, which predict opposite trends. Calculations using HIVAP predict cross sections for the reaction S-36+U-238 that are similar to those of the Mg-26+Cm-248 reaction. Here, we report on the first measurement of evaporation residues formed in the complete nuclear fusion reaction S-36+U-238 and the observation of (270)Hs, which is produced in the 4n evaporation channel, with a measured cross section of 0.8(-0.7)(+2.6) pb at 51-MeV excitation energy. The one-event cross-section limits (68% confidence level) for the 3n, 4n, and 5n evaporation channels at 39-MeV excitation energy are 2.9 pb, while the cross-section limits of the 3n and 5n channel at 51 MeV are 1.5 pb. This is significantly lower than the 5n cross section of the Mg-26+Cm-248 reaction at similar excitation energy.

80 MeV/u C-12离子诱变选育PHB高产菌株；A strain of high PHB output by mutagenesis of 80 MeV/u C-12 ions

用80MeV/u12C6+离子对一株积累聚β-羟基丁酸酯(PHB)的芽孢杆菌(BacillusP-9)进行诱变选育,最终获得PHB高产株菌G15,其PHB产量达2.93g/L,与出发菌株相比较,PHB积累量提高了1.5倍。研究结果表明,本试验辐照最佳剂量为15Gy。重离子辐照诱变育种效果显著,具有广阔的发展应用前景。

25MeV/u Kr辐照下PET薄膜的损伤机制研究；Damage Mechanism of PET Irradiated by 25 MeV/u Kr Ions

通过25MeV/u86Kr离子辐照叠层结晶聚对苯二甲酸乙二醇酯膜(PET),在不同的电子能损(3.407.25keV/nm)和离子注量(5×10113×1012ions/cm2)辐照条件下,对Kr离子在PET中引起的辐照损伤效应进行了研究。借助傅里叶变换红外光谱分析,通过对样品的红外吸收峰进行扣除基底后的Lorentz拟合,分析了与主要官能团对应的吸收峰强度的变化趋势,研究了化学结构与组分在重离子辐照下的变化规律;利用X射线衍射光谱仪测量,研究了Kr离子在PET潜径迹中引起的非晶化过程,并通过对吸光度和非晶化强度随离子注量的指数衰减规律的分析,获得了不同电子能损离子辐照PET时主要官能团的损伤截面和非晶化截面及对应的潜径迹半径。

~(12)C与~(209)Bi反应中Au同位素的产额与Q_(gg)的关系；Q_(gg)-Yield Dependence of Au Isotopes in Interaction of 47 MeV/u ~(12)C With ~(209)Bi

用47MeV/u12C离子轰击天然铋靶,通过炮弹和靶核之间的核子转移反应产生Au同位素。使用放射化学方法从大量Bi和复杂反应产物中分离、纯化Au,并制备Au的γ射线测量源。使用HPGe探测器测量放射性Au同位素的γ活性。根据照射结束时Au同位素的活度和其他相关数据,确定每个Au同位素的产生截面。分析发现,缺中子Au同位素的产生截面与Qgg值之间不遵从指数依赖关系,这可用重离子碰撞中的次级过程加以解释。

Studies of K-shell x-ray energy shifts induced by MeV/u heavy ions

This paper reports that the K x-ray spectra of the thin target 47Ag, 48Cd, 49In and 50Sn were measured by an HPGe semi-conductor detector in collisions with 84.5 MeV 6C4+ ions. Our experiment revealed the Kα x-ray energy shifts were not obvious and the Kβ1 x-ray energy shifts were about 90∼110 eV. The simple model of Burch et al has been previously used to calculate the K x-ray energy shifts due to an additional vacancy in 2p orbit. The present work extends the model of Burch to calculate the x-ray energy shifts of multiple ionized atoms induced by heavy ions with kinetic energy of MeV/u. In addition to our experimental results, many other experimental results are compared with the calculated values by using the model.

超铀核的研究

本文详细调研了超铀核研究的发展过程，总结了超铀区核素产生方法、传输方法以及分离方法。结合我国的实际，利用中国科学院高能物理研究所的质子直线加速器的质子束，轰击稀有放射性靶，通过(p，4n)反应道合成和研究了超铀区新核素~(235)Am，巧妙地利用X射线对核素进行了指定，得到了它的半衰期及合成截面，实验中没有观测到伴随~(235)Am的β~+(EC)衰变的γ跃迁，该方法发表后即被日本的实验小组采用；同时利用中国科学院近代物理研究所的SFC加速器提供的~(20)Ne束流轰击~(233)U靶，测量反应产物的α衰变，第一次观测到~(250)102的α衰变，由此得到了~(250)102的半衰期，它不同于~(250)102已知的半衰期；在实验中还观测到一个能量为17.6MeV的衰变。实验采用氦喷嘴传输技术对反应产物进行传输，并根据产物的不同衰变采用了不同的测量方法，对~(235)Am由于其半衰期长，采用了化学分离的分离方法并测量X、γ及其符合测量，而对~(250)102等采用直接测量其α衰变，利用衰变关系进行鉴别的方法。通过对实验的总结分析了利用现有条件研究更重核素的可能。

用RIMS研究低能He2+与Ar碰撞的多电子过程

用反冲离子动量谱仪研究了低能He2+与Ar碰撞的多电子交换过程。该技术的独特优势是对反冲离子末态动量的完全测量。实验上鉴别了单电子俘获SC，双电子俘获DC和转移电离TI各子过程，并得到了末态量子态布居信息，首次测量了该体系各反应道的角微分截面及直接与碰撞参数相关的信息。实验发现电子主要俘获到入射离子基态或单激发态，反冲离子处于单激发态或多激发态，并有较大几率形成空心离子。研究表明电荷交换过程中存在较强的电子-电子关联作用。角分布随反冲离子电荷态增加而变宽，并向大角度方向移动，表明碰撞参数减小，相互作用加剧。SC和DC与MCBM理论角微分截面符合很好，说明在大碰撞参数时经典近似有一定合理性。不同碰撞参数范围内反冲纵向动量分布表明，SC在碰撞参数7.2a.u.≥b≥3.6a.u.时发生机率最大，随碰撞参数减小，靶离子有不断向更高激发态过渡的趋势

12C6+重离子辐照对细胞端粒酶活性表达的影响

端粒是染色体末端由重复DNA序列和相关蛋白组成的一种特殊结构，具有稳定染色体结构及完整性的功能，会随染色体复制与细胞分裂而缩短。端粒酶是一种核糖核蛋白，能以自身RNA模板合成端粒DNA，催化合成TTAGGG重复序列，添加到染色体末端，维持端粒长度不变。端粒酶主要由hTR, TEPl和hTERT组成，一般认为hTERT是端粒酶激活的限速因素。大多数永生化细胞和恶性肿瘤细胞具有端粒酶活性，因而端粒酶目前已成为为细胞持续分裂提供遗传基础的原因。由于端粒酶与细胞衰老、肿瘤发生等关系如此密切，因此已成为肿瘤放射治疗研究热点。目的： 本文利用兰州近代物理研究所重离子研究装置（Heavy Ion Research Facility in Lanzhou,HIRFL）产生的碳离子（31MeV/u 12C6+）对人体细胞、癌细胞进行不同剂量的辐照，探索细胞中端粒酶活性的变化及与之相关的生物学信息。材料与方法： 以人肝细胞HL－7702，肝癌细胞SMMC－7721为实验对象，用不同剂量1Gy、2Gy、3Gy、4Gy的重离子分别对两种细胞进行照射，用多聚酶链式反应-银染端粒重复序列扩增法（PCR- telomeric repeat amplification protocol，TRAP-PCR）检测不同剂量下细胞端粒酶活性的变化。并提取不同剂量下的细胞转入培养皿中，培养10天，固定，染色。统计大于50个细胞的克隆数，绘制细胞存活曲线。结果与讨论： 结果显示，人肝细胞HL-7702自身没有端粒酶活性，经1Gy辐照后也没有端粒酶活性，在2、3Gy处出现端粒酶活性，4Gy处端粒酶活性又消失。肝癌细胞SMMC-7721在1－3Gy处随着剂量的增大端粒酶活性升高，在4Gy处又开始下降；在1－3Gy处随着时间的推移端粒酶活性随着时间而加强（p<0.05）。随着剂量的增大，细胞存活率呈剂量依赖型下降。分析得知，重离子辐射可以诱导人肝细胞产生端粒酶活性，也可以改变肝癌细胞的端粒酶活性。端粒酶参与细胞受辐照后DNA单链损伤的修复；辐照后DNA双链断裂导致端粒酶活性减弱。本实验与其他低LET射线相比，使重离子在辐照治疗中的优势得以体现

治癌专用离子同步加速器的物理设计

放射治疗肿瘤是利用各种放射线所携带的能量及其生物效应治疗肿瘤的一种方法。论文简要介绍了癌症的危害性和目前基本的治疗方法，回顾了国际上放射治疗肿瘤的发展历程和近年来的新动向，说明了国内放射治疗肿瘤工作的现状以及近几年的发展。为了促进国内癌症治疗的进一步发展，研究设计了国内第一台离子治癌专用装置。它由一台注入器（回旋加速器）、一台主加速器 (同步加速器)和若干治疗终端组成，能够把质子束加速到250MeV或者把碳离子束加速到430MeV/u，用于治疗人体内任意深度的肿瘤。 论文的重点是同步加速器的磁聚焦结构、注入和引出系统的设计。 商业化运行的治癌专用离子同步加速器通常采用紧凑性结构，要求操作简单，运行稳定可靠。论文根据治癌专用离子同步加速器的这些要求，研究设计了磁聚焦结构。 由于直线加速器的高流强特性，目前已有的国外离子治癌专用装置，几乎全部使用直线加速器作为同步加速器的注入器，同时采用多圈注入方式。考虑到直线加速器高的投入，借鉴大科学工程CSR束流累积的经验，论文以回旋加速器为注入器，采用剥离注入模式设计了治癌同步加速器的注入系统。另外，还对剥离注入期间离子束发射度、动量分散等参数的变化进行了较为详细的研究。 离子束治癌一般要求小剂量连续照射（1-10s），因此治癌专用离子同步加速器均采用三阶共振引出方式。论文详细阐述了三阶共振引出的基本理论与设计方法，在此基础上设计了离子束引出系统。通过磁聚焦结构、注入及引出设计的整体优化，提出了磁铁好场区和真空室孔径的参数。 最后，论文对慢引出的两种激发方式进行了理论探讨，并对纵向激发元件——磁电感应器（Betatron-core）的电流、阻抗和电压等参数的变化，以及电源纹波对引出束均匀性的影响进行了较为详细的分析计算

强子的介质效应

本论文简述了强子介质效应的研究现状，理论方法以及实验探测技术。系统的介绍了相对论平均场理论和手征有效场论。利用相对论平均场研究了Pentaquark的介质效应，利用手征有效场论研究了△(1232)共振态的介质效应。 在密度相关的平均场理论基础上，计算出的Pentaquark的有效质量随核物质密度的增加而减小。一定的Pentaquark含量导致每核子的结合能减小，这使得核物质系统更加稳定。 在手征有效场论的框架下，利用泡利不相容原理对核子传播子的修正，以及核子有效质量在核物质中的改变，通过计算△共振态一阶自能，讨论了△共振态的有效质量和衰变宽度对核物质密度的依赖关系。结果表明：△共振态的有效质量随核物质密度的增加而减小，在正常核密度下为1221MeV，而在3倍正常核密度时为1186MeV，其减小幅度与美国Lawrence Berkeley国家实验室上做的58Ni+Cu（能量为1.97GeV/u）碰撞实验给出的结果大致相符；△粒子的衰变宽度在核物质中的变化主要决定于核子以及△粒子的有效质量的变化