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In ImQMD model, each nucleon is represented by a coherent state of a Gaussian wave packet. The time evolution of the coordinate and momentum of each nucleon is determined by the mean field part which is described by Hamiltonian equations and the nucleon-nucleon collision part. The Hamiltonian includes kinetic energy, nuclear potential energy and the Coulomb energy. The nuclear potential energy is an integration of the Skyrme type potential energy density functional, which reads
where
$ \rho = \rho_{\rm n}+\rho_{\rm p} $ is the nucleon density and$ \delta = (\rho_{\rm n}-\rho_{\rm p})/(\rho_{\rm n}+\rho_{\rm p}) $ .$ \rho_{\rm n} $ ,$ \rho_{\rm p} $ are neutron and proton density, respectively. The Coulomb energy in the Hamiltonian is written as a sum of the direct and the exchange contribution:In the collision term, the isospin-dependent in-medium nucleon-nucleon scattering cross sections are applied, and the Pauli blocking effects are treated as in Ref. [30]. The phase space occupation number constraint method[37] is adopted in this model. The model parameters as those used in Ref. [31] are listed in Table 1. More detailed description of the ImQMD model and its applications can be found in Refs. [31, 33-34].
Parameter Values Parameter Values α/MeV –356 $g_{\tau}$/MeV 12.5 β/MeV 303 $\eta$ 2/3 $\gamma$ 7/6 $c_{\rm s}$/MeV 32 g0/(MeV·fm2) 7.0 $\kappa_{\rm s}$/fm2 0.08 $\rho_0$/fm–3 0.165 Table 1. The model parameters.
In this work, the binding energy per nucleon and deformation of 136Xe and 208Pb are taken from Ref. [38]. The orientations of the initial projectile and target in all events are sampled randomly with an equal probability. The cross section for the primary fragment with charge number
$ Z $ , mass number$ A $ , excitation energy$ E^* $ , angular momentum$ J $ is calculated byHere
$ b $ is the impact parameter,$ N_{\rm{frag}}(Z,A,b,E^*,J) $ is the number of events in which a fragment$ (Z,A,E^*,J) $ is formed at a given impact parameter$ b. $ The excitation energy$ E^* $ for the fragment with charge number$ Z $ and mass number$ A $ is obtained by subtracting the corresponding ground-state energy[38] from the total energy of the excited fragment in its rest frame. The total energy of the fragment is calculated by the Hamiltonian. Angular momentum$ J $ of primary fragment is calculated by the coordinates and momentums of all nucleons in the rest frame of fragment. Both excitation energy and angular momentum of primary fragment are related with incident energy, impact parameters and nucleons transfer, etc.$ N_{\rm{tot}}(b) $ is the total event number at a given impact parameter$ b $ . The maximum impact parameter is taken to be$ b_{\rm{max}} $ =13 fm, and the impact parameter step is$ \Delta{b} $ =0.1 fm. The initial distance between the centers of mass of projectile and target is taken to be 30 fm. 10 000 events for each impact parameter are simulated in this work.The system 136Xe+208Pb is special because of the closed neutron shell in projectile and doubly magic target. The structure effect of two interacting nuclei, which may be partly missed in ImQMD model, should be significant in the reaction. For simply considering this effect,
$ Q $ -value is proposed to be considered in ImQMD model from the point of view based on the experimental results, in which the exponential dependence of the cross sections for products on$ Q $ -value was observed in multinucleon transfer reactions 232Th, 197Au+16O[39]. In ImQMD model, the motion of each nucleon can be tracked. In the small time step of simulation, the transfer of only several nucleons occurs in the area of neck. The neck area is defined by the density configuration of system. The experimentally observed dependence of transfer of several nucleons on$ Q $ -value is introduced in the process of nucleons transfer. In this work, whether the motion of transferred nucleons in neck area will be affected by$ Q $ -value is determined by the probability distribution of$ Q $ -value$P_i=f_i[Q^{(i)}_{\rm gg}]/\sum\limits_if_i[Q^{(i)}_{\rm gg}]$ for all possible transfer of nucleons. Here$ f_i[Q^{(i)}_{\rm gg}] $ =$ C_i\exp[Q^{(i)}_{\rm gg}] $ . The momentum component along the axis connecting the centers-of-mass of two interacting nuclei for each transferred nucleon changes to the opposite direction while the$ P_i $ is not selected by the random number. That is, the transfer of nucleons with larger$ Q $ -value is more likely to happen.$ Q^{(i)}_{\rm gg} $ is the mass difference between before and after nucleons transfer to produce$ i $ -th combination of projectile-like and target-like parts.$ C_i $ should be related with many factors, such as the structure properties, the deformation and the excitation of system, etc. It is still unclear and needs to be studied further. Here we simply set$C_i$ =1. Therefore, the motion of nucleons are determined by Hamiltonian equations, nucleon-nucleon collision part and the effect of$ Q $ -value. It is named ImQMD+$ Q $ .Multinucleon transfer reaction 136Xe+208Pb at
$ E_{\rm{c.m.}} $ =617 MeV is simulated by ImQMD and ImQMD+$ Q $ . The incident energy is about 40 percent over Bass barrier[40]. For comparing with experimental data deduced from different measured distributions[1], the angles of primary fragments are calculated according to the momenta of fragments in ImQMD and ImQMD+$ Q $ . The decays of primary fragments are considered by statistical evaporation model (HIVAP code)[41-42]. The matching time to apply HIVAP code is determined by the decay process of primary fragments calculated in ImQMD model. Over a period of time after the separation of composite system, the probability of forming a fragment decreases with a constant slope, which means that the fragment almost completely enters into the statistical decay stage. We take this time as the matching time to calculate the decay of primary fragments by HIVAP code. In the de-excitation of primary fragments through evaporation of$ \gamma $ , n, p and$ \alpha $ particle, we assume that the emitting angle of the fragments remains unchanged. The corresponding coincident binary fragments over experimentally detected angular range 25°~70° in the laboratory frame are identified. The distributions of total kinetic energy lost calculated by ImQMD and ImQMD+$ Q $ are plotted and compared with experimental data in Fig. 1(a). TKEL is normalized to the count number or cross sections at TKEL=0 for comparison. The open and solid circles represent the calculation results of ImQMD and ImQMD+$ Q $ , respectively. The data denoted by the solid squares are generally better reproduced by the results of ImQMD+$ Q $ .$ Q $ -value effect significantly decreases the contribution of larger TKEL in comparing with those of ImQMD. The effects of$ Q $ -value on TKEL from different impact parameters are shown in panels (b~d). The difference between the results of ImQMD and ImQMD+$ Q $ mainly occurs in the events at lower impact parameters ($ b\leqslant $ 6 fm). The energy transfer from collective motion to internal excitation decreases due to the effect of$ Q $ -value. It leads to a larger probability of producing primary fragments with smaller excitation energies.Figure 1. (color online)TKEL distribution of 136Xe+ 208Pb for binary events at
$E_{\rm{c.m.}}$ =617 MeV. Open and solid circles are the results of ImQMD and ImQMD+$Q$ , respectively. The data denoted by solid squares are taken from Ref. [1]. The calculated TKEL are compared with the data in panel (a). Panels (b~d) represent the contributions to TKEL from different impact parameters.The primary fragments produced in the binary events in Fig. 1 are selected with energy losses greater than 40 MeV. Mass distributions of those fragments are plotted in Fig. 2(a) for comparing with experimental data[1]. The open and solid circles represent the same meanings as Fig. 1. The experimental data denoted by solid squares are also better generally reproduced by the results of ImQMD+
$ Q $ than those of ImQMD. ImQMD provides a larger cross section in massive transfer between two nuclei. The effect of$ Q $ -value in ImQMD+$ Q $ leads to the suppression in the transfer of more than ten nucleons. The peaks of experimental mass distribution and the mass number of projectile and target are denoted by arrows and dashed lines, respectively. The peaks of mass distribution in ImQMD locate at the mass number of projectile and target. A large number of primary fragments in ImQMD+$ Q $ drift away from the entrance channel mass-asymmetry to the peaks of experimental mass distribution. It can be understood by positive$ Q $ -value in the maximum$ Q $ -value$ Q_{\rm gg} $ for each mass number of fragments in panel (b). The transfer of less than about ten nucleons are obviously driven by the effect of$ Q $ -value.Figure 2. (color online) Mass distribution and
$Q_{\rm{gg}}$ distribution of 136Xe+208Pb. (a) Mass distribution for binary events with energy losses greater than 40 MeV. Open and solid circles are the results of ImQMD and ImQMD+$Q$ , respectively. The data denoted by solid squares are taken from Ref. [1]. The peak positions in experimental data and two colliding nuclei are represented by arrows and dashed lines, respectively. (b) Distribution of maximum$Q_{\rm{gg}}$ for all possible mass transfers.$Q_{\rm{gg}}$ =$M_{\rm{P}}$ +$M_{\rm{T}}$ –$M_{\rm{PLF}}$ –$M_{\rm{TLF}}$ , where$M_{\rm{P}}$ and$M_{\rm{T}}$ are the masses of projectile and target.$M_{\rm{PLF}}$ and$M_{\rm{TLF}}$ are the masses of the projectile-like and target-like fragments.Multinucleon transfer and the energy transfer from collective motion to internal excitation are strongly related with the lifetime of composite system. The comparison between the average lifetimes of composite system calculated by ImQMD and ImQMD+
$ Q $ for different impact parameters is shown in Fig. 3. With increasing the impact parameters, the larger angular momentum decreases the average lifetime of composite system. The effect of$ Q $ -value obviously decreases the average lifetime of composite system at lower impact parameters$ b\leqslant $ 5 fm. It explains the increase of lower TKEL at lower impact parameters in Fig. 1 and the suppression of cross sections for the fragments produced in the transfer of massive nucleons in Fig. 2. The smaller lifetime of composite system caused by the effect of$ Q $ -value provides the smaller probability for multinucleon transfer.Figure 3. (color online) The average lifetime of composite system calculated by ImQMD and ImQMD+
$Q$ for different impact parameters. The meaning of the symbols is the same as Fig. 1.The system 136Xe+208Pb has aroused a great interest in the production of more neutron-rich nuclei with neutron number
$ N $ =126. The effect of$ Q $ -value on the production of these primary isotopes is shown in Fig. 4. ImQMD+$ Q $ provides larger cross sections for neutron-rich isotopes produced in protons transfer from target to projectile. It originates from the effect of$ Q $ -value in the comparison between the results of ImQMD and ImQMD+$ Q $ .$ Q $ -value describes the properties of nuclei in their ground states. The result implies that the production of those isotopes is still related with$ Q $ -value effect (or quantum effect) in 136Xe+208Pb even at 40 percent over bass barrier.Figure 4. (color online) The cross sections for primary isotopes with neutron number
$N$ =126 in ImQMD and ImQMD+$Q$ . The meaning of the symbols is the same as Fig. 1.
Effect of Q-value on Multinucleon Transfer Reaction 136Xe+208Pb
doi: 10.11804/NuclPhysRev.37.2020022
- Received Date: 2020-03-21
- Rev Recd Date: 2020-04-21
- Publish Date: 2020-07-15
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Key words:
- multinucleon transfer reaction /
- Q-value effect /
- ImQMD model
Abstract: Multinucleon transfer reaction 136Xe+208Pb at
Citation: | Kai ZHAO, Zhengtong XIA, Jizheng DUAN. Effect of Q-value on Multinucleon Transfer Reaction 136Xe+208Pb[J]. Nuclear Physics Review, 2020, 37(2): 160-165. doi: 10.11804/NuclPhysRev.37.2020022 |