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161.
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Toshiki Maruyama A. Bonasera M. Papa S. Chiba 《The European Physical Journal A - Hadrons and Nuclei》2002,14(2):191-197
We investigate the formation and the decay of heavy systems which are above the fission barrier. By using a microscopic simulation
of constrained molecular dynamics (CoMD) on Au + Au collision, we observe that composite states stay for a very long time
before decaying by fission.
Received: 13 December 2001 / Accepted: 19 March 2002 相似文献
164.
A. Di Pietro P. Figuera V. Scuderi F. Amorini C. Angulo G. Cardella E. Casarejos S. Cherubini J. Lu C. Marchetta A. Musumarra M. Papa M. Pellegriti R. G. Pizzone R. Raabe F. Rizzo J. L. Sida W. Tian 《Physics of Atomic Nuclei》2006,69(8):1366-1371
The present paper concerns the study of reactions induced by radioactive beams of halo and weakly bound nuclei at energies
around and above the Coulomb barrier. The results obtained for the reaction induced by the halo nucleus 6He on 64Zn have been compared with the results for the reaction induced by 4He on the same target. The results of the reaction induced by the weakly bound unstable 13N on the weakly bound 9Be have been compared with those for the reaction 10B + 12C.
The text was submitted by the authors in English. 相似文献
165.
166.
A.L.S. Angelis H.-J. Besch B.J. Blumenfeld L. Camiller T.J. Chapin R.L. Cool C. del Papa L. Di Lella Z. Dimčovski R.J. Hollebeek L.M. Lederman D.A. Levinthal J.T. Linnemann C.B. Newman N. Phinney B.G. Pope S.H. Pordes K.K. Young 《Physics letters. [Part B]》1980,97(1):163-168
A large solid-angle apparatus consisting of a superconducting solenoid magnet, cylindrical drift chambers and two arrays of lead-glass counters was used to examine particles associated with a high transverse momentum trigger in p-p collisions with three √s values at the CERN ISR. The trigger was given by energy deposition in lead-glass arrays centred at 90°. The trigger transverse momentum range covered was 3 < . Results are given for pout for both individual charged particles, and also for the sum of charged particle momenta in the hemisphere opposite to the trigger. Mean values are then deduced for the parton transverse momentum kT, and for the jet fragmentation momentum jT. 相似文献
167.
For arbitrary polynomial loading and a sufficient finite number of nodal points N, the solution for the 3D Timoshenko beam differential equations is polynomial and given as \({{\varvec \theta} = \sum_{i=1}^N I_i {\varvec \theta}_i}\) for the rotation field and \({{\bf u} = \sum_{i=1}^{N+1} J_i {\bf u}_i}\) for the displacement field, where I i and J i are the Lagrangian polynomials of order N?1 and N, respectively. It has been demonstrated in this work that the exact solution for the displacement field may be also written in a number of alternative ways involving contributions of the nodal rotations including \({{\bf u} = \sum_{i=1}^N I_i \left[ {\bf u}_i + \frac 1 N ( {\varvec \theta} - {\varvec \theta}_i ) \times {\bf R}_i \right]}\), where R i are the beam nodal positions. 相似文献
168.
169.
P. Astone M. Bassan P. Bonifazi P. Carelli E. Coccia V. Fafone A. Marini G. Mazzitelli S. M. Merkowitz Y. Minenkov I. Modena G. Modestino A. Moleti G. V. Pallottino M. A. Papa G. Pizzella F. Ronga M. Spinetti R. Terenzi M. Visco L. Votano 《Nuclear Physics B - Proceedings Supplements》1999,70(1-3)
Recently significant advancements have been made towards the realization of a large spherical gravitational wave detector. Research and development activities have already begun in several countries. We present here the main features and capabilities of a spherical gravitational wave detector. In particular, we discuss the interaction between a spherical antenna and cosmic rays that may require a large detector to be placed underground. 相似文献