共查询到16条相似文献,搜索用时 156 毫秒
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36Ar+112,124Sn反应中小角关联出射的中等质量碎片(IMF)约化速度关联函数. 结果表明36Ar+124Sn反应系统中的约化速度关联函数在小约化速度处的反关联程度比36Ar+112Sn反应系统中的强, 表现出明显的入射道依赖性. 考察出射粒子对的单核子总动量时, 发现这种差异主要来自于高动量粒子对的贡献. 用三体弹道理论模型MENEKA分别计算了两个系统的IMF发射时标, 在36Ar+112Sn反应系统中约为150fm/c, 而在36Ar+124Sn反应系统中, 约为120fm/c. 同位旋相关的量子分子动力学计算表明, 36Ar+124Sn系统中IMF的发射时间谱比36Ar+112Sn系统略有前移, 相应地, 其中心密度从最高点随时间的下降亦比36Ar+112Sn系统略快. 相似文献
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30MeV/u 40Ar+159Tb反应中中等质量碎片发射的时空演化 总被引:1,自引:1,他引:0
报道了30MeV/u 40Ar+159Tb反应中中等质量碎片发射时间随空间大小的演化规律.实验结果表明,发射空间大小对IMF关联函数的影响主要来自于发射源的核物质密度,而几乎不依赖于源的质量数,对于发射时间较短(≤100fm/c)的高能碎片,较小的核物质密度导致提取的发射时间变小.在正常核物质密度参数下提取的发射时间可作为其上限值,对于发射时间较长的中低能碎片,发射时间不随空间大小变化,提取的发射时间值即为其实际值. 相似文献
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在25MeV/u 40Ar+115In反应的在平面和出平面大角度关联测量中,提取了碎片和α粒子之间的方位角关联函数和方位角非对称性因子.φ=90°时,方位角关联函数呈现为最小值,表明在集体类转动效应影响下,反应产生的轻带电粒子和碎片优先在反应平面内发射.随着关联对质量的增加,在平面关联粒子的发射相对于束流轴不对称性逐渐增大.随着关联对质量的增加,相继衰变和粒子末态相互作用对φ=0°的关联粒子对方位角关联函数值的影响逐渐降低并直至消失,同时集体转动效应增强,方位角非对称性增加. 相似文献
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用13单元望远镜探测器阵列测量了30MeV/u 40Ar +112,124Sn反应中小角关联粒子,由两体符合事件提取了αα关联函数.用三体弹道理论模型MENEKA计算本底关联函数,用Monte Carlo方法计算探测效率函数,在扣除本底产额并考虑探测效率的修正后,对不同同位旋反应系统40Ar +112Sn和40Ar+124Sn提取的相对态布居核温度分别是4.18±0.25 0.21MeV和4.10±0.22 0.20MeV ;考察态布居核温度和粒子能量的关系时,观察到两个系统的发射温度均随着粒子能量的增加而降低,缺中子系统40Ar +112Sn中由低能时的5.13±0.30 0.2 6MeV降低到高能时的3.87±0.37 0.29MeV ,丰中子系统40Ar+124Sn中由低能时的5.39±0.30 0.26MeV降低到高能时的3.32±0.28 0.23MeV .用激发热核衰变过程的同位旋选择性对这种同位旋相关性进行了解释. 相似文献
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在25MeV/u 40Ar+natAg、209Bi反应中,用4个PPAC和11组望远镜完成了关联裂变碎片与发射轻粒子的符合测量,角关联描绘为两个被探测到碎片折叠角θff的函数,线性动量转移〈LMT〉由测量到的角关联推出.将符合测量得到的对应于不同窗的后角轻带电粒子能谱用Maxwell分布来拟合其谱的后沿,经过一些修正,由能谱得到热核的初始温度Tint,在考虑反应Q值和预平衡发射的修正之后,可以得到不同窗所对应的激发能.实验结果表明,在40Ar+natAg、209Bi反应的中心碰撞中激发能分别为4.2、2.4MeV/u,而温度达6.1、5.5MeV,在半中心碰撞中激发能为3.5、1.9MeV/u,温度可达5.8、4.8MeV. 相似文献
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Emission Time Measurements of Light Particles from 40Ar+197Au Collisions in Intermediate Energies 下载免费PDF全文
He Zhiyong Duan Limin Li Zuyu Jin Genming Luo Qingzheng Wu Heyu Zhang Baoguo Wen Wanxin Qi Yujin Dang Bingrong Dai Guangxi 《中国物理C(英文版)》1996,20(1):8-12
Particle-particle correlation functions have been measured for 40Ar+197Au collisions at E=25 MeV/u.Emission time of light particles has been extracted from correlation functions using the three-body trajectory model.The average emission time varies with the energy of particles. It decreases from about 300 fm/c for low energy particles to about 100fm/c for energetic particles. 相似文献
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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
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Li Zuyu Wang Hongwei He Zhiyong Dun Limin Zhang Baoguo Dai Guangxi Fu Yanbiao Jin Genming 《中国物理C(英文版)》1998,22(8):684-689
Fragment-fragment conelation functions have been measured in E/A=30 MeV 40Ar+natAg reaction via the technique of intensity interferometry. Emission times of intermediate mass fragments have been extracted from reduced velocity correlation functions by using the threebody trajectory model. The average emission time of intermediate mass fragments varies with the energy of fragments. It decreases from about 300fm/c for low energy fragments to about 80fm/c for energetic fragments. After subtmcting the contribution of projectile-like fragments, average emission times of mid-rapidity fragments are of the order of 250fm/c for this reaction.It indicates that intermediate mass fragments emitted in this reaction mainly come from sequential binary decays. 相似文献
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报道了25MeV/u40Ar+197Au反应中从两粒子相对动量关联函数提取的发射时间随空间大小演化的规律.结果表明,即使发射源质量数减小50%,对计算的关联函数及提取的发射时间影响仍然很小.在短发射时间(τ≤100fm/c)情况下,较小的核物质密度,导致提取的发射时间变小.因此,在正常核物质密度参数下提取的τ值可作为发射时间的上限值.在长发射时间(τ≥300fm/c)情况下发射时间不随空间大小变化,提取的τ即为实际的发射时间.
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Fan Sheng Li Zhuxia Zhao Zhixiang Ding Dazhao 《The European Physical Journal A - Hadrons and Nuclei》1999,4(1):61-68
The double differential cross section of emitting particles, the mass and charge distribution of the residual nuclei from
proton-induced reaction on 208Pb with incident energy 590 MeV and 322 MeV have been analyzed by the quantum molecular dynamics (QMD). The time scale of
the change of reaction mechanism in the process of reaction is investigated. The reaction process can be divided into three
stages i.e., the direct, the cascade and the evaporation stage with the corresponding time scale of about <30 fm/c, 30–100
fm/c and >100 fm/c, respectively.
Received: 16 January 1998 / Revised version: 17 September 1998 相似文献
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Afanasiev S Aidala C Ajitanand NN Akiba Y Alexander J Al-Jamel A Aoki K Aphecetche L Armendariz R Aronson SH Averbeck R Awes TC Azmoun B Babintsev V Baldisseri A Barish KN Barnes PD Bassalleck B Bathe S Batsouli S Baublis V Bauer F Bazilevsky A Belikov S Bennett R Berdnikov Y Bjorndal MT Boissevain JG Borel H Boyle K Brooks ML Brown DS Bucher D Buesching H Bumazhnov V Bunce G Burward-Hoy JM Butsyk S Campbell S Chai JS Chernichenko S Chiba J Chi CY Chiu M Choi IJ Chujo T Chung P Cianciolo V 《Physical review letters》2008,100(23):232301
A three-dimensional correlation function obtained from midrapidity, low p(T), pion pairs in central Au+Au collisions at sqrt[s(NN)]=200 GeV is studied. The extracted model-independent source function indicates a long range tail in the directions of the pion pair transverse momentum (out) and the beam (long). A proper breakup time tau(0) ~ 9 fm/c and a mean proper emission duration Delta tau ~ 2 fm/c, leading to sizable emission time differences ({|Delta t(LCM)|} approximately 12 fm/c), are required to allow models to be successfully matched to these tails. The model comparisons also suggest an outside-in "burning" of the emission source reminiscent of many hydrodynamical models. 相似文献