Cluster Structure Calculations Research Articles

Elastic scattering andαproduction in theBe9+Y89system

Elastic scattering measurement for the $^{9}\mathrm{Be}+^{89}\mathrm{Y}$ system has been carried out at near-barrier energies with the aim of investigating the effect of breakup on the elastic channel. The energy dependence of the optical model potential for the system gives an indication of the breakup threshold anomaly (BTA) for the system. An overall repulsive real part of the dynamic polarization potential (DPP) generated due to continuum couplings using the $\ensuremath{\alpha}+^{5}\mathrm{He}$ cluster structure for $^{9}\mathrm{Be}$ is consistent with the BTA behavior observed for the system. In contrast, an attractive real part of the DPP, at all energies, is observed for similar calculations carried out using the $^{8}\mathrm{Be}+n$ cluster structure. Coupling of the 1$n$ transfer channel in addition to continuum couplings does not have a significant effect on the elastic scattering angular distributions. The experimental 1$n$ transfer cross sections show better agreement with the corresponding values obtained using the $^{8}\mathrm{Be}+n$ cluster structure calculations. Inclusive breakup-$\ensuremath{\alpha}$ cross sections are observed to form a large fraction of the reaction cross sections, especially at below-barrier energies, suggesting the dominance of the breakup channel at these energies. This also supports the BTA behavior observed for the system, reflected as the presence of a reaction channel and thus the persistence of the imaginary potential at below-barrier energies.

Parallelization of the global extremum searching process

The parallel algorithm for searching the global extremum of the function of several variables is designed. The algorithm is based on the method of nonuniform coverings proposed by Yu.G. Evtushenko for functions that comply with the Lipschitz condition. The algorithm is realized in the language C and message passing interface (MPI) system. To speed up computations, auxiliary procedures for founding the local extremum are used. The operation of the algorithm is illustrated by the example of atomic cluster structure calculations.

Calculation of Cluster Structure of Melts, Its Effect on Formation of Nanoamorphous Solid Phases and Their Structural Relaxation in Subsequent Heating

Calculation of Cluster Structure of Melts, Its Effect on Formation of Nanoamorphous Solid Phases and Their Structural Relaxation in Subsequent Heating