999 resultados para RICH NUCLEI


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Within the hadronic transport model IBUU04, we investigate the effect of density-dependent symmetry energy on double neutron/proton (n/p) ratio of free nucleons in heavy ion collisions by taking four isotopic Sn+Sn reaction systems. Especially the entrance-channel asymmetry and impact-parameter dependence of the effect of symmetry energy are discussed. It is found that in both central and semi-central collisions the sensitivity of the double n/p ratio to the density-dependent symmetry energy is more pronounced in neutron-richer systems. Our results also indicate clearly that the effect of symmetry energy is stronger in central collisions than that in semi-central collisions.

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The longitudinal momentum distribution (P-//) of fragments after one-proton removal from Al-23 and reaction cross sections (sigma(R)) for Al-23,Al-24 on carbon target at 74A MeV have been measured simultaneously. An enhancement in sigma(R) is observed for Al-23 compaxed with Al-24. The full width at half maximum of the P-// distribution for Mg-22 fragments has been determined to be 232 +/- 28 MeV/c. Analysis of P-// using the Few-Body Glauber Model indicates a dominant d-wave configuration for the valence proton in the ground state of Al-23. The exotic structure in Al-23 is discussed.

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The differential isospin-fractionation (IsoF) during the liquid-gas phase transition in dilute asymmetric nuclear matter is studied as a function of nucleon momentum. Within a self-consistent thermal model it is shown that the neutron/proton ratio of the gas phase becomes smaller than that of the liquid phase for energetic nucleons, although the gas phase is overall more neutron-rich. Clear indications of the differential IsoF consistent with the thermal model predictions are demonstrated within a transport model for heavy-ion reactions. Future comparisons with experimental data will allow us to extract critical information about the momentum dependence of the isovector strong interaction.

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We measured fragmentation cross sections produced using the primary beam of Kr-86 at 64 MeV/nucleon on Be-9 and Ta-181 targets. The cross sections were obtained by integrating the momentum distributions of isotopes with 25 <= Z <= 36 measured using the RIPS fragment separator at RIKEN. The cross-section ratios obtained with the Ta-181 and Be-9 targets depend on the fragment masses, contrary to the simple geometrical models. We compared the extracted cross sections to EPAX; an empirical parametrization of fragmentation cross sections. Predictions from current EPAX parametrization severely overestimate the production cross sections of very neutron-rich isotopes. Attempts to obtain another set of EPAX parameters specific to the reaction studied here to extrapolate the neutron-rich nuclei more accurately have not been very successful, suggesting that accurate predictions of production cross sections of nuclei far from the valley of stability require information of nuclear properties that are not present in EPAX.

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Within a transport model it is shown that the neutron/proton ratio of squeezed-out nucleons perpendicular to the reaction plane, especially at high transverse momenta, in heavy-ion reactions induced by high energy neutron-rich nuclei can be a useful tool for studying the high density behavior of the nuclear symmetry energy.

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The double neutron-proton differential transverse flow taken from two reaction systems using different isotopes of the same element is studied at incident beam energies of 400 and 800 MeV/nucleon within the framework of an isospin- and momentum-dependent hadronic transport model IBUU04. The double differential flow is found to retain about the same sensitivity to the density dependence of the nuclear symmetry energy as the single differential flow in the more neutron-rich reaction. Because the double differential flow reduces significantly both the systematic errors and the influence of the Coulomb force, it is thus more effective probe for the high-density behavior of the nuclear symmetry energy.

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Radium was radiochemically separated from natural thorium. Thin Ra-228 ->beta Ac-228 sources were prepared and exposed to mica fission track detectors, and measured by an HPGe gamma-ray detector. The beta-delayed fission events of Ac-228 were observed and its beta-delayed fission probability was found to be (5 +/- 2)x10(-12).

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Based on the isospin- and momentum-dependent hadronic transport model IBUU04, effects of the nuclear symmetry energy on the single and double pi(-)/pi(+) ratios in central reactions of Sn-132+Sn-124 and Sn-112+Sn-112 at a beam energy of 400 MeV/nucleon are studied. It is found that around the Coulomb peak of the single pi(-)/pi(+) ratio the double pi(-)/pi(+) ratio taken from the two isotopic reactions retains about the same sensitivity to the density dependence of nuclear symmetry energy. Because the double pi(-)/pi(+) ratio can significantly reduce the systematic errors, it is thus a more effective probe for the high-density behavior of the nuclear symmetry energy.

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The double neutron/proton ratio of nucleon emissions taken from two reaction systems using four isotopes of the same element, namely, the neutron/proton ratio in the neutron-rich system over that in the more symmetric system, has the advantage of reducing systematically the influence of the Coulomb force and the normally poor efficiencies of detecting low energy neutrons. The double ratio thus suffers less systematic errors. Within the IBUU04 transport model the double neutron/proton ratio is shown to have about the same sensitivity to the density dependence of nuclear symmetry energy as the single neutron/proton ratio in the neutron-rich system involved. The double neutron/proton ratio is therefore more useful for further constraining the symmetry energy of neutron-rich matter.

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Based on the isospin-dependent transport model IBUU and on the scaling model according to nucleon effective mass, effects of elastic and inelastic NN scattering cross-sections on pi(-)/pi(+) in the neutron-rich reaction Ca-48 + Ca-48 at a beam energy of 400MeV/nucleon are studied. It is found that cross-section effects of both NN elastic and inelastic scatterings affect Delta(1232), pi(-) and pi(+) productions as well as the value of pi(-)/pi(+).

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The Coulomb dissociation of the proton-rich nuclei Cl-31 was studied experimentally using Cl-31 beams at 58 MeV/nucleon with a lead target. The relative energy between the reaction products, S-30 and proton, was obtained. The first excited state in Cl-31 was observed which is relevant to the resonant capture of stellar S-30(p, gamma)Cl-31 reaction

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Using a transport model coupled with a phase-space coalescence after-burner we study the triton-He-3 relative and differential transverse flows in semi-central Sn-132 + Sn-124 reactions at a beam energy of 400 MeV/nucleon. We find that the triton-He-3 pairs carry interesting information about the density dependence of the nuclear symmetry energy. The t-He-3 relative flow can be used as a particularly powerful probe of the high-density behavior of the nuclear symmetry energy.

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本文概述了 A > 170 质量区重丰中子同位素研究的主要工作和意义;介绍了 A > 170 重丰中子同位素合成、分离和鉴别方法;详细论述了激光离子源的原理、设计及其同传统离子源相比所具有的优越性;在文章结尾,设计了一个物理实验,实验目的在于:1)寻找 ~(181)Yb新核素;2)揭示天体物理学中~(180m)Ta 的产生问题。我们对反应截面进行了分析,并对产额进行了估计,证明了此实验设计的合理性,进而说明了带激光离子源的同位素分离器适用于产生截面很低的新核素和衰变研究。本文重点讨论了激光离子源的各方面问题:介绍了激光多步共振电离原理和激光离子源原理;具体分析了热毛细管式激光离子源元素选择性的产生及其影响的因素;讨论了在设计、加工过程中的具体问题;描述了所使用的激光技术;通过在线实验验证了热毛细管式激光离子源的元素选择性和分离效率。

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核反应总截面是表征原子核反应基本特征的一个基本量,从实验测得的核反应总截面中可以得到有关核反应、核结构和核内核子分布的信息。在由放射性束流所产生奇的结构与各种反应机制研究中,反应总截面的测量更是具有特殊的重要性,具有奇异晕核结构的核的一个典型的物理现象就是其反应总截面要比稳定核大很多,Tanihata等人最早就是通过对放射性束流的相互作用截面的测量发现了具有奇异结构的核,即中子晕核。这次实验结果得出的跟放射性奇异核性质等有关的一些有趣现象,为放射性束核物理的研究注入了新的活力。我们采用能量为80MeV/u的初级~(20)Ne束轰击3mm厚的初级Be靶,在RIBLL上测量了由初级靶上产生碎裂反应所得到的次级~(12)N, ~(17)F和~(17)Ne等质子滴线核在硅靶上的中能核反应总截面,从而进一步补充了现有的中能区奇异核反应总截面测量的空白,并对现有的数据进行了检验。由于~(12)N, ~(17)F和~(17)Ne都是有争议的可能具有奇异质子结构(质子晕或质子皮)的核,测量它们在中能区的核反应总截面,可以对上述说法的成立与否提供实验上的验证。在与相邻同位素核的反应截面测量结果的比较中,发现实验得出的这些奇异核的截面值都偏大,而且由相对论平均场(RMF)计算得到的它们的质子密度分布明显比中子分布松散的多,因此推断它们可能具有奇异质子分布结构。并且基于库仑修正后的微观Glauber模型的理论计算出这些奇异核反应截面的结果同我们得出的实验数据吻合得很好。为了更精确地进行奇异核反应总截面的测量,研制了两种双维位置灵敏平行板雪崩电离室(PPAC),可以放在待测硅靶前,用来选择小于一定入射角的次级束粒子,有助于得到更准确的结果。该PPAC的有效探测面积为50 * 50mm~2,分别采用电荷分除法和延迟线读出的方法确定入射粒子的位置,并具有结构简单、价格便宜的特点。用三组分α源(5.155Mev~(239)Pu, 5.486 Mev~(241)Am, 5.806Mev~(244)Cm) 对探测器进行了测试,由阴极电荷分除读出法得到的位置分辨(FWHM)约为1.5mm。

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我们首先用Woods-Saxon势对一些丰中子核进行了系统的计算.计算表明在Woods-Saxon势中考虑一个对称能项,Woods-Saxon势就能够很好的描述丰中子核的密度分布,单粒子能级结构和中子质子的均方根半径.用Woods Saxon势的计算结果表明中子皮是丰中子远离β稳定线核的普遍现象。2S1/2轨道与1d 5/2轨道的交又和2s1d壳与1p壳的壳崩渍是中子晕形成的重要原因,也是中子晕与中子皮的一个重要区别.壳模型的计算能够很好的再现9《A《14和3《Z《5丰中子核的许多性质,这表明了,改进壳模型的有效相互作用,壳模型可能能够描述远离核的性质. 我们208Ti一类核和206Pb的一些性质进行了系统的壳模型计算.计算结果表明,K-H和SDI等有效相互作用对描述208Ti一类核和206Pb的高激发态仍然是有效的,计算结果也表明,如果208Hg可供利用的β衰变能比206Hg小,则可以预计208Hg的半寿命比206Hg要长.计算还证实了在反应209Bi(ρ,a )206Pb中激发的206Pb激发态结构,与205Tl低激发态结构相似,即这些态可以用h9/2轨道上的一个质子与205T1的低激发态的弱耦合来描述,此即所谓的对应的相似多重态的概念. 最后,我们对11Li等中子晕核的束缚机制提出了一种新的关联机制和讨论了用壳模型描述集体运动的方法.