974 resultados para heavy ion beam


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We present the first measurements of identified hadron production, azimuthal anisotropy, and pion interferometry from Au + Au collisions below the nominal injection energy at the BNL Relativistic Heavy-Ion Collider (RHIC) facility. The data were collected using the large acceptance solenoidal tracker at RHIC (STAR) detector at root s(NN) = 9.2 GeV from a test run of the collider in the year 2008. Midrapidity results on multiplicity density dN/dy in rapidity y, average transverse momentum < p(T)>, particle ratios, elliptic flow, and Hanbury-Brown-Twiss (HBT) radii are consistent with the corresponding results at similar root s(NN) from fixed-target experiments. Directed flow measurements are presented for both midrapidity and forward-rapidity regions. Furthermore the collision centrality dependence of identified particle dN/dy, < p(T)>, and particle ratios are discussed. These results also demonstrate that the capabilities of the STAR detector, although optimized for root s(NN) = 200 GeV, are suitable for the proposed QCD critical-point search and exploration of the QCD phase diagram at RHIC.

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We present measurements of the charge balance function, from the charged particles, for diverse pseudorapidity and transverse momentum ranges in Au + Au collisions at root S-NN = 200 GeV using the STAR detector at RHIC. We observe that the balance function is boost-invariant within the pseudorapidity coverage vertical bar-1.3, 1.3 vertical bar. The balance function properly scaled by the width of the observed pseudorapidity window does not depend on the position or size of the pseudorapidity window. This scaling property also holds for particles in different transverse momentum ranges. In addition, we find that the width of the balance function decreases monotonically with increasing transverse momentum for all centrality classes. (c) 2010 Elsevier B.V. All rights reserved.

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In order to investigate the biological effects of heavy ion radiation at low closes and the different radiosensitivities of growing and non-growing plants. rice at different lift stages (dry seed, wet seed and seedling) were exposed to carbon ions at closes of 0 02, 0.2, 2 and 20 Gy. Radiobiological effects on survival, root growth and mitotic activity, as well as the induction of chromosome aberrations in root meristem. were observed The results show that radiation exposure induces a stimulatory response at lower close and an inhibitory response at higher dose on the mitotic activity of wet seeds and seedlings Cytogenetic damages are induced in both seeds and seedlings by carbon ion radiation at doses as low as 0.02 Gy Compared with seedlings. seeds are more resistant to the lethal damage and the growth rate damage by high doses of carbon ions, but are more sensitive to cytogenetic damage by low closes of irradiation Different types of radiation induced chromosome aberrations are observed between seeds and seedlings. Based on these results, the relationships between low close heavy ion-induced biological effects and the biological materials are discussed.

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The Heavy Ion Research Facility and Cooling Storage Ring (HIRFL-CSR) accelerator in Lanzhou offers a unique possibility for the generation of high density and short pulse heavy ion beams by non-adiabatic bunch compression longitudinally, which is implemented by a fast jump of the RF-voltage amplitude. For this purpose, an RF cavity with high electric field gradient loaded with Magnetic Alloy cores has been developed. The results show that the resonant frequency range of the single-gap RF cavity is from 1.13 MHz to 1.42 MHz, and a maximum RF voltage of 40 kV with a total length of 100 cm can be obtained, which can be used to compress heavy ion beams of U-238(72+) with 250 MeV/u from the initial bunch length of 200 ns to 50 ns with the coaction of the two single-gap RF cavity mentioned above.

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The 400 MeV/u C-12(6+) ion beam was successfully cooled by the intensive electron beam near 1 A in CSRe. The momentum cooling time was estimated near 15 s. The cooling force was measured in the cases of different electron beam profiles, and the different angles between the ion beam and electron beam. The lifetime of the ion beam in CSRe was over 80 h. The dispersion in the cooling section was confirmed as positive close to zero. The beam sizes before cooling and after cooling were measured by the moving screen. The beam diameter after cooling was about 1 mm. The bunch length was measured with the help of the signals from the beam position monitor. The diffusion was studied in the absence of the electron beam.

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The mirror nuclei N-12 and B-12 are separated by the Radioactive Ion Beam Line in Lanzhou (RIBLL) at HIRFL from the breakup of 78.6 MeV/u N-14 on a Be target. The total reaction cross-sections of N-12 at 34.9 MeV/u and B-12 at 54.4 MeV/u on a Si target have been measured by using the transmission method. Assuming N-12 consists of a C-11 core plus one halo proton, the excitation function of N-12 and B-12 on a Si target and a C target were calculated with the Glauber model. It can fit the experimental data very well. The characteristic halo structure for N-12 was found with a large diffusion of the protons density distribution.

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We measured the total reaction cross sections of N-12 in Si at 36.2 MeV/u. using Radioactive Ion Beam Line in Lanzhou (RIBLL) with a new method. The reaction target was installed at the intermediate focusing point T1 at RIBLL. This scheme allows us to identify particles before and after the reaction target unambiguously. The total reaction cross section (1760 +/- 78mb) of N-12 in Si is obtained. Assuming that N-12 consists of a core C-11 plus one halo proton, the excitation function of N-12 on the Si and C targets is calculated with the Glauber model and the Fermi-Fermi density distributions. It can fit the experimental data very well. A large diffusion of the protons density distribution supports the halo structure for N-12.

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The dissociative recombination of the acetaldehyde cation, CH3CHO+, has been investigated at the heavy ion storage ring CRYRING at the Manne Siegbahn Laboratory in Stockholm, Sweden. The dependence of the absolute cross section of the reaction on the relative kinetic energy has been determined and a thermal rate coefficient of k(T) = (1.5 +/- 0.2) x 10(-6) (T/300)(-0.70 +/- 0.02) cm(3) s(-1) has been deduced, which is valid for electron temperatures between similar to 10 and 1000 K. The branching fractions of the reaction were studied at similar to 0 eV relative kinetic energy and we found that breaking one of the bonds between two of the heavy atoms occurs in 72 +/- 2% of the reactions. In the remaining events the three heavy atoms stay in the same product fragment. While the branching fractions are fairly similar to the results from an earlier investigation into the dissociative recombination of the fully deuterated acetaldehyde cation, CD3CDO+, the thermal rate coefficient is somewhat larger for CH3CHO+. Astrochemical implications of the results are discussed.

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With the commissioning of HIRFL-CSR, HIRFL can provide heavy ion beams with energy covering the range of several MeV/u to 1 GeV/u. In this talk, the experiments on nuclear physics at different energies to be carried out with different experimental setups at HIRFL will be introduced.

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Collisions involving Sn-112 and Sn-124 nuclei have been calculated with the ImQMD transport model in order to place constraints on the density dependences of the nuclear symmetry energy. Consistent constraints on the symmetry energy at sub-saturation density have been obtained by comparing these transport calculations to measurements of isospin diffusion and to the ratios of neutron and proton spectra. New isospin diffusion results from E/A = 35 MeV are also presented.

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The dissociative recombination of protonated propionitrile, CH3CH2CNH+, has been investigated at the heavy ion storage ring, CRYRING, at the Manne Siegbahn Laboratory, Stockholm University, Sweden. The thermal rate coefficient has been deduced to follow k(T) = (1.5 +/- 0.2) x 10(-6) (T/300)(-0.76) (+/-) (0.02) cm(3) s(-1) for electron temperatures ranging from similar to 10 to similar to 1000 K. Measurements of the branching fractions were performed at similar to 0 eV relative kinetic energy. It has been found that in 43% +/- 2% of the reactions the four heavy atoms remain in the same product fragment. An equal portion of the reactions leads to products where one of the heavy atoms is split off from the other three and 14% +/- 1% result in a breakup into two heavy fragments containing two heavy atoms each. We discuss the significance of the data to Titan's upper atmosphere.

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目的:建立重离子束辐照结合植物组织培养技术进行植物诱变的新方法,使用该方法率先开展植物组织细胞的传能线密度(LET)生物学效应的研究,尝试重离子束辐照结合农杆菌转染及质粒微注射法转基因操作。 材料与方法:采用兰州重离子研究装置(HIRFL)加速的碳离子束辐照非洲紫罗兰、丽格海棠、新几内亚凤仙以及紫花苜蓿的外植体,测定形态学指标,计算不同外植体的相对生物学效应(RBE)。以非洲紫罗兰叶片外植体为对象研究RBE随LET的变化关系。使用氖离子束辐照烟草叶片外植体结合农杆菌转染方法进行赤霉素4(GA4)基因转染实验;使用碳离子束辐照苜蓿愈伤组织结合质粒微注射方法进行β-葡萄糖苷酸酶(GUS)基因转染实验。 结果: 1. 不同剂量的936MeV的碳离子束和8MV的X射线辐照三种花卉及一种牧草的外植体后,基于存活率的RBE值分别为2.3、1.6、2.1和4.0; 2. LET值在31~151keV/μm区间的碳离子束辐照非洲紫罗兰叶片外植体。基于鲜重增殖(FWI)的RBE值随LET的增加而增加,151keV/μm时达到最高值6.7; 3. 烟草离体叶片外植体经过5Gy的1600MeV氖离子束辐照后进行农杆菌转基因操作,最终获得转染率为3.9%,单纯农杆菌转基因的转染效率为3.2%; 4. 20Gy的936MeV的碳离子束辐照苜蓿愈伤组织后结合组织表面pBI121质粒溶液微量注射处理后,获得GUS基因瞬间表达效率高达84.6%。 结论: 1. 不同花卉植物组织培养用外植体的辐照敏感性不同,本研究发现丽格海棠的辐射敏感性最高,其次是新几内亚凤仙,非洲紫罗兰的最不敏感; 2. 不同花卉植物外植体经离子束辐照诱变处理后,得到的再生植株突变类型不尽相同,主要包括叶的突变和茎的突变; 3. RBE的随LET的增大而增加可以归因于离子在生物体中能量沉积的增加,研究发现各生物学终止点受到损伤或者抑制的程度基本上是随着LET的增大而增大; 4. 通过离子束辐照结合植物组织培养方法最终获得了非洲紫罗兰叶绿素缺失突变体,该突变体通过植物组织培养技术能够稳定遗传; 5. 中能氖离子束辐照能够略微提高烟草农杆菌转基因的转化效率,辐照能够使再生植株花期提前; 6. 中能碳离子束辐照结合苜蓿愈伤组织表面微量注射质粒溶液法进行转基因操作能获得更高的基因转染效率

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本论文主要解决CSR真空系统的控制实现与连锁保护问题。 HIRFL-CSR(Heavy Ion Research Facility at LanZhou-Cooling Storage Ring兰州重离子冷却储存环)是国家重大科学工程。为了保证CSR正常运行,超高真空系统的平均真空度必须达到6×10-9Pa,超高的真空度来之不易,CSR上任何一处真空设备发生故障,就会破坏真空度,所以CSR必须具有响应速度快、安全可靠,稳定性好的真空控制与连锁保护系统。 HIRFL-CSR真空设备有离子泵电源、分子泵、钛升华泵、阀门、真空计等。分子泵只在粗抽时使用,钛升华泵为间歇升华,因此不需要监控。需要显示和控制的设备为离子泵电源、真空计和真空阀门。通过对CSR上每个真空计的真空度数据的监测和真空阀门状态的采集,一旦真空度降低到一定阈值,立即关闭相应位置阀门(保护真空),并给出故障报警,从而实现真空系统的连锁保护。 真空控制系统以嵌入式处理器ARM、复杂可编程逻辑器件CPLD和微控制器MSP430为核心,实现了远程数据采集、数据显示和自动控制等功能。本系统可以进行现场监控与调试,也可以通过集成的100Mbps以太网接口电路进行远程监测与控制,CSR上各处真空度和真空阀门状态自动传送到中央控制中心,中控中心也可以发送命令查询当前真空设备状态和各种读数。 本文主要介绍了基于ARM、CPLD和MSP430的嵌入式真空控制系统的设计与实现。内容主要包括(1)系统各部分硬件电路设计与真空控制功能实现 ,硬件系统调试 。(2)嵌入式uClinux操作系统构建和在其上进行的应用程序,设备驱动程序,串行通信程序的开发。(3)CPLD的VHDL程序和MSP430的C430程序设计。 本文目的是解决CSR真空控制系统问题,但对于许多远程数据采集与控制等问题的解决有重要参考价值

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HIRFL-CSR(Heavy Ion Research Facility at LanZhou-Cooling Storage Ring兰州重离子冷却储存环)是国家重大科学工程,其控制系统是一个庞大的系统,由许多分控制系统组成,高频系统是其重要组成部分之一。加速器的加速过程都是由高频系统来完成的。由于高频控制系统的控制对象就是高频腔体,控制系统的稳定性和输出频率的精确性将直接影响到加速器系统的正常工作,而对于高频系统的状态回读又直接决定了对于高频系统的远程监控能力,所以高频控制系统的设计非常重要。本设计基于现场可编程逻辑门阵列FPGA和数字信号专用处理器DSP搭建, 一方面可以完成从控制中心远程控制高频腔体,另一方面也可以完成对于当前状态的读取,所经过的通道也是多样化的,包括CPCI总线通信,CANBUS总线通信或者是485总线通信。本文的内容包括了1>对于高频控制系统控制对象的分析以及各种控制参数要求。2>组成此系统的硬件部分分析选择以及硬件系统的搭建过程。3>对FPGA和DSP进行程序设计的过程和方法。本文的价值不仅在于对高频系统的控制上,对于其他数据采集系统,远程控制系统以及总线通信和数据分析算法上也有着参考价值

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HIRFL-CSR(Heavy Ion Research Facility at LanZhou-Cooling Storage Ring兰州重离子冷却储存环)是国家重大科学工程,其控制系统是一个庞大的系统,由许多分控制系统组成,磁场电源控制系统是CSR控制系统中很重要的一部分。加速器运行的所有过程都为电源所控制,所以我们的控制系统的直接控制对象就是磁场电源。为了保证CSR正常运行,控制过程波形的跟踪精度、速度和稳定度,是数字电源调节器的关键所在。电源控制系统以嵌入式处理器ARM、现场可编程门阵列FPGA为核心,实现了远程数据采集、网络通讯和自动控制等功能。本系统可以进行现场监控与调试,也可以通过集成的100Mbps以太网接口电路进行远程监测与控制,CSR上各处输出电压值和电源运行状态自动传送到中央控制中心,中控中心也可以发送命令查询当前电源设备状态和各种读数。本文主要介绍了基于ARM和FPGA的嵌入式电源控制系统的设计与实现。内容主要包括:(1)系统各部分硬件电路设计与电源控制功能实现 ,硬件系统调试 。(2)装载嵌入式Linux操作系统,测试平台接口信号,通过FPGA生成多路数字PWM波形。本文目的是解决CSR电源控制系统问题,但对于许多远程数据采集与控制等问题的解决有重要参考价值