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1.
An isoratio method is proposed to study the chemical potential of neutrons (protons) from the yield ratio of isotopes (isotones) differing in neutron-excess (I = N-Z). The measured fragments in the 140 A MeV40,48 Ca and 58,64 Ni + 9 Be reactions, as well as those in the simulated 58,64 Ni + 9Be reactions by using the antisymmetric molecular dynamics (AMD) model plus the secondary decay model gemini, have been adopted to perform the isoratio analysis. The results of the isoratio method verify that they are similar to that of the well known isoscaling method. The isoratio scaling phenomenon suggested by the isoratio method has also been found in the measured data and the fragments simulated by the AMD + gemini models.  相似文献   

2.
The heavy fragments in heavy-ion collisions are finally formed after the hot prefragments undergo sequential decay,of whom the temperature should be much lower than that of prefragments.Using the double ratio(DR) method,the isotopic thermometer(Tiso) for heavy fragment is constructed using the yield of heavy isotopes.T iso of heavy fragment is obtained by analyzing the measured data in the 1A GeV124,136Xe and 140A MeV 48Ca/64Ni reactions.Result shows that T iso varies from 0.5 MeV to 10 MeV.But most T iso is around 1±0.5 MeV,which is much lower than temperature of light particles.Result also indicates that the difference between T iso of heavy fragments in different reactions is very small,and T iso is independent on the size of the reaction system,the incident energy and the neutron-richness of the projectile.  相似文献   

3.
徐文霞  杨永成  邓联忠 《中国物理 B》2017,26(5):53702-053702
We theoretically investigate the production of cold CN molecules by photodissociating ICN precursors in a brute-force field. The energy shifts and adiabatic orientation of the rotational ICN precursors are first investigated as a function of the external field strength. The dynamical photofragmentation of ICN precursors is numerically simulated for cases with and without orienting field. The CN products are compared in terms of their velocity distributions. A small portion of the CN fragments are recoiled to near zero speed in the lab frame by appropriately selecting the photo energy for dissociation. With a precursor ICN molecular beam of ~ 1.5 K in rotational temperature, the production of low speed CN fragments can be improved by more than 5 times when an orienting electrical field of 100 k V/cm is present. The corresponding production rate for decelerated fragments with speeds ≤ 50 m/s is simulated to be about ~2.1×10~(-4) and CN number densities of 10~(8) –10~(10) cm~(-3) can be reached with precursor ICN densities of ~10~(12) –10~(14) cm~(-3) from supersonic expansion.  相似文献   

4.
提出一个经验公式,预测散裂反应中同位素产生的截面值,并且利用现有GSI-FRS实验测量的300,500,750,1 000和1 500 MeV/u能量下p+56Fe散裂反应产物的实验结果进行验证。发现此经验公式预测的同位素截面值与实验值的符合度比较好,但随着质量数与能量的改变,同位素产生截面的计算值与实验值的差距也在变大。通过引入质量与能量修正可使此经验公式计算出的同位素截面值的精确度更高,与实验值的符合程度更好。An empirical formula is proposed to predict the isotopic cross section in spallation reactions. The measured fragments in the 300, 500, 750, 1 000 and 1 500 MeV/u p+56Fe spallation reactions have been adopted to perform the analysis. The cross sections of isotopes predicted by the proposed empirical formula have been compared to the experimental results, which shows that the empirical formula can predict the results well. But with the change of the mass and incident energy, the difference between the calculated results and experimental data is larger. The proposed empirical formula is found to predict the isotopic cross sections better, by incorporating the incident energy and mass dependents of fragments.  相似文献   

5.
中国锦屏地下实验室(CJPL)坐落于四川省锦屏山中,利用水电站修建的隧道建成。由于其本底环境极低,非常适合开展低本底实验测量。一台基于ECR源的400 kV强流加速器将安装在CJPL中,其可以为核天体物理实验提供流强为12 emA的质子束流,6 emA的He+束流和2.5 emA的He2+束流。拟通过非共振反应12C(p,γ)13N以及一系列的共振反应27Al(p,γ)28Si等,对加速器的束流能量进行精确刻度,对束流的能量展宽以及长期稳定性进行测量。由于该加速器正在中国原子能科学研究院进行地面调试,我们利用中国科学院近代物理研究所的320 kV研究平台,进行了12C(p,γ)13N和27Al(p,γ)28Si反应的测试实验。测量结果表明,在质子束流能量为224 keV时,束流的能量展宽约为1.0 keV,束流能量在连续4小时的测量期间,其晃动幅度远小于±200 eV。China JinPing underground Laboratory (CJPL) was established inside the tunnels piercing Jinping Mountain in Sichuan Province, China, which can provide an ideal environment for low background experiment. A new 400 kV accelerator, with high current based on an ECR source, will be placed at this underground laboratory for nuclear astrophysics experiment. The beam characteristics of this accelerator, like absolute energy, energy spread, and long-term energy stability, will be determined by several wellknown resonance and non-resonance reactions. Due to the new accelerator still being under construction, the resonance reaction of 27Al(p, γ)28Si and non-resonance 12C(p, γ)13N were studied at the 320 kV highvoltage platform in Institute Modern Physics of CAS in Lanzhou. The energy spread of proton beam is about 1.0 keV at proton energy Ep=224 keV and the long-term energy stability of proton beam is much better than 200 eV during 4 hours measurement.  相似文献   

6.
A new technique has been applied to coincidence measurements between fission fragments (FF) and intermediate mass fragments (IMF) emitted from the composite system 149 65Tb at an excitation energy of 224 MeV. The method permits simultaneous observation of IMF emissions along and normal to the FF separation axes. For the integrated total of 0.10± 0.02 IMF emitted per fission, we find no significant correlation with FF direction, suggesting that IMFs associated with fission reactions are predominantly emitted from the system prior to fission.  相似文献   

7.
Excitation functions, angular distributions and differential ranges were measured for the 26Mg(18O, 16O)28Mg reaction at 18O beam energies of 20–45 MeV. Excitation functions only were measured for the reactions 14C(18O, 19O)13C, 14C(18O, 16O)16C, 14C(18O, 20O)12C, 14C(18O, 15N)17N and 18O(18O, 19O)17O, 18O(18O, 16O)20O, 18O(18O, 15N)21F at 18O beam energies of 13–41 MeV. We have identified these as direct reactions in which a single neutron, a two-neutron cluster, a deuteron and a triton are transferred between projectile and target.

The cross sections for two-neutron transfer reactions were found to be relatively high and those for the 18O+18O and the 14C+18O reactions were higher than the ones of single-neutron transfers over most of the energy range.

Attempts were made to apply the theory of Buttle and Goldfarb for single-neutron transfer to the case of two-neutron transfer in the 26Mg(18O, 16O)28Mg reaction below the Coulomb barrier. It is shown that for those reactions for which the assumptions, implicit in the model, are valid, good agreement is obtained with experiment. We also tried to apply the diffraction model of Dar and Kozlovsky to the calculation of the angular distribution of these reactions. A good fit to the experimental results could be obtained if quite different sets of parameters were used in the calculations for the two bombarding energies.  相似文献   


8.
The dynamical cluster-decay model (DCM) is employed to investigate the decay of 68,70Ge* compound nuclei formed respectively via tightly (4He) and loosely (6He) bound projectiles, using 64Zn target. The study is carried out over a wide energy range (Ec.m.~5 MeV to 16 MeV) by including the quadrupole deformations (β2i) and optimum orientations (θiopt) of the decaying fragments. The fusion cross-sections, obtained by adding various evaporation channels show nice agreement with the experimental data for 4He+64Zn reaction. The contribution from competing compound inelastic scattering channel is also analyzed particularly for 68Ge* nucleus at above barrier energies. On the other hand, the decrement in the fusion cross-sections of 70Ge* nuclear system is addressed by presuming that 65Zn ER is formed via two different modes:(i) the αn evaporation of 70Ge* nucleus, and (ii) 1n-evaporation of 66Zn* nuclear system, formed via breakup and 2n-transfer channels due to halo structure of the 6He projectile. Besides this, the suppression in 2np evaporation cross-sections suggests the contribution of another breakup and transfer process of 6He i.e. 4He+64Zn. The contribution of breakup+transfer channels for 6He+64Zn reaction is duly addressed by applying relevant energy corrections due to the breakup of " 6He" projectile into 2n and 4He. In addition to this, the barrier lowering, angular momentum and energy dependence effects are also explored in view of the dynamics of chosen reactions.  相似文献   

9.
By using a new reaction model for light nuclei, the double-differential cross section of total outgoing neutron with LUNF code for n+^16O reactions at En=14.1 MeV and 18 MeV have been calculated and analyzed. In this paper the opened reaction channels, which have contribution to emitting the neutrons, are listed in detail. To improve the fitting results the direct inelastic scattering mechanism is involved. The calculating results agree fairly well with the experimental data at E,~ = 14.1 MeV and the deviation from calculated results and experimental data in low energy region at En= 18 MeV has been analyzed. Since the possibility of 5He has been affirmed theoretically [J.S. Zhang, Sci. Chin. G 47 (2004) 137], so 5He emission from n+ ^16O reaction is taken into account, which plays an important role at the region of the outgoing neutron energy εn〈3 MeV in total outgoing neutron energy-angular spectrum. The calculated results indicate that the pre-equilibrium mechanism dominates the whole reaction processes, and the recoil effect in light nuclear reactions is essentially important.  相似文献   

10.
本文采用由自由核子,α粒子及平均重核组成的核统计平衡模型描述由自由核子和许多种类原子核组成的系铣。由半径验核质量及核激发态熵公式描述核的性质,给定系统温度、密度及电子浓度ye,由系统自由能在电中性及强子数守恒约束下求极小得我们的物态方程EOS(Ⅰ),并与E1 Eid等物态方程(在密度ρ~109-1012g cm-3)和与Lgmb等物态方程(在ρ~1012-1014g cm-3,ye=0.3,σ=1.5k)作了比较,符合程度较好。本文对电子俘获率也作了更细致的考虑。  相似文献   

11.
A twin crystal of Ga was investigated in the temperature and field ranges of 0.5 to 10 mK and 60 to 250 mT, respectively. In these fields the magnetic interaction is too large to be treated as a perturbation of the quadrupolar interaction. Therefore, the eigenvalues of the Schrödinger equation were calculated numerically, and then used to determine the crystalline axes by pulsed NMR on 69Ga and 71Ga. The temperature dependence of the NMR line intensities was measured using 195Pt-NMR for thermometry. The observed intensities do not follow the theoretical expectations for a spin system of low nuclear polarization. In addition, a temperature-dependent frequency shift was observed. These results suggest that the effect of interactions between the spins, as well as more complicated spin dynamics, need to be considered in order to use gallium as an absolute thermometer at temperatures below 1 mK.  相似文献   

12.
We have studied the interaction of low-energy (5–50 eV) electrons with nanoscale (10 ML) ice films by probing the yields and quantum-state distributions of the neutral dissociation products using laser resonance-enhanced multiphoton ionization spectroscopy. In particular, we have observed the electron-stimulated desorption (ESD) of D (2S), O (3P2) and O (1D2) from amorphous D2O films. These products are observed at threshold energies (relative to the vacuum level) between 6.5–7 eV and desorb with low kinetic energies (60–85 meV) which are independent of the incident electron energy. We associate the ESD of atomic fragments from ice with dissociation of Frenkel-type excitons of 4a1 character which are near the bottom of the ice conduction band. These excitons are created either directly or via electron-ion recombination. Changing the surface temperature from 88 to 145 K results in an increase in the thermal component of the time-of-flight (kinetic energy) distributions and an overall increase in the neutral fragment yield. We suggest that the change in neutral yield with substrate temperature results from a combination of: (1) increased electron-ion recombination; (2) exciton transport to the near-surface region; and (3) dissociation followed by inelastic scattering and desorption.  相似文献   

13.
The proton transfer reactions (d, n) and (τ, d) on 42Ca have been studied. The reaction 42Ca(d, n)43Sc has been studied by the time-of-flight method at deuteron energies between 5.0 and 6.05 MeV. The reaction 42Ca(τ, d)43Sc has been studied at 18.0 MeV with a magnetic spectrograph. Altogether 54 levels in 43Sc up to an excitation energy of 6.92 MeV have been identified including states at 4.234 and 6.145 MeV which are analogues of the ground state and the 2.048 MeV state respectively in 43Ca. The l-values and spectroscopic strengths have been determined for 31 transitions. Within the errors of the experiments and the DWBA analyses, the spectroscopic strengths derived from the (d, n) and the (τ, d) experiments are in agreement for both and states, i.e. there are no T-dependent discrepancies. Similar agreement is found in the strengths of the s- and d-hole transitions which reflect the degree of particle-hole impurity in the 42Cag,s. wave function. A second state is indicated at 2.657 MeV. It appears a likely candidate for the head of a second band of 6p-3h character as proposed by Johnstone.  相似文献   

14.
N. Ohtsuka 《Nuclear Physics A》1981,370(3):431-444
The energy spectra of neutrons emitted following muon capture in 16O and 12C are investigated using the continuum shell model. Nuclear wave functions, which have been shown by Ohtsubo and the author to describe the radiative pion capture reaction in the above nuclei well, are adopted. The calculated neutron energy spectra explain well the observed main peaks, at 5 MeV for 16O and 4 MeV for 12C, which are considered to be the giant resonances excited in the muon capture reaction. These peaks are interpreted as the 2 state at 20.3 MeV for 16O and the 1 state at 22.5 MeV for 12C. Comparisons with photon spectra in radiative pion capture reactions are also made. The calculated total capture rates exceed the experimental values by a factor of 2.5 for 16O and by 30–40% for 12C.  相似文献   

15.
16.
The energy spectra of deuterons, tritons and 3He particles from the reactions 3He(p, d)2p, 4He(p, t)2p and 4He(p, 3He)pn have been measured at angles between 6° and 60° lab. The 3He(p, d)2p reaction was studied at both 30.5 and 49.5 MeV incident proton energies, while the other two reactions were studied at 49.5 MeV only. The energy spectra are compared with calculations based on the Watson-Migdal model of final-state interactions.  相似文献   

17.
The excited states of the deformed odd-proton nucleus 161Ho have been studied in the reactions 159Tb(, 2n), 161Dy(d, 2n) and 161Dy(p, n). Gamma-ray spectra in single and coincidence modes as well as angular distributions and excitation functions of the transitions were measured. The proposed level scheme of 161Ho contains besides of the ground state band [523] the bands +[404], +[411], +[411] and [541] (band heads at 252.7, 298.7, 211.2 and 423.9 keV, respectively). An attempt was made to estimate the influence of Coriolis coupling between the bands + [411] and + [411], which are very close in energy. The + [404] band was found to de-excite by very fast E1 transitions to the ground state band [523]. Nilsson retardation factors of about 0.03 for these transitions were deduced using the E2/E1 branching ratios. An investigation has also been made of the independent feeding of the levels from high-lying states.  相似文献   

18.
The 12C(γ,pn) and 12C(γ,pp) reactions have been studied using tagged photons of energy Eγ = 150–400 MeV. Recoil momentum distributions are compared to the results of Monte Carlo calculations based on a two-nucleon photon absorption model and two different phase space models. The 12C(γ,pn) data at low missing energy are consistent with absorption on 1p2 and 1s1p nucleon pairs.  相似文献   

19.
A novel scheme for measuring the cross section of the 7Be(p,γ)8B reaction, the major source of high energy neutrinos from the sun, is presented. The scheme involves a strictly uniform particle beam and overcomes some of the recognized experimental uncertainties of previous measurements. A new measurement of σ[7Li(d,p)8Li] has been carried out using this setup, and the present value of σ[7Li(d,p)8Li] = 155(8) mb at the top of the Ed(lab.) = 776 keV resonance is compared with previous measurements. A new issue regarding both the (d,p) and (p,γ) reactions has been examined: reaction-product nuclei which are backscattered out of the target. Measurements and simulations carried out in the course of this investigation are presented and discussed in the context of possible effects on the measured cross sections of these reactions.  相似文献   

20.
核子-核子碰撞截面(σNN)是描述原子核反应模型中的重要物理量。 核子-核子碰撞截面包括质子-质子碰撞截面(σpp)、中子-中子碰撞截面(σNN)和中子 质子碰撞截面(σnp), 它们随着核子能量与核物质密度的改变而变化。人们在目前研究中提出了多种核子-核子碰撞截面关于能量和核物质密度的参数化公式,通过计算12C+12C的完全反应截面,比较了不同入射能量下使用各种核子-核子碰撞截面参数化公式对12C完全反应截面的影响。 The nucleus-nucleus cross sections(σNN) include the proton-proton cross section, neutron-neutron cross section, and neutron-proton cross section. σNN change with the variations of the incident energies and the densities. Some parameterizations of σNNas a function of incident energy and density have been proposed in the theoretical and experimental study of nuclear reactions. Through the calculation of reaction cross sections of 12C+12C at different energies, the effect of different σNN parameterizations in the reaction cross sections of 12 are studied.   相似文献   

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