Gasdynamic model of intermediate energy heavy ion collisions and high-energy particle emission
Description
Emission of high-energy particles is investigated for cases of collision of heavy ions of intermediate energies in the framework of gasdynamic model. Nonequilibrium equation of state corresponding to fermi-ellipsoid is used in calculations. In the process of collision the smaller nucleus makes ''a tube of nuclear matter'' in the target nucleus. The process of nucleus colllision with the tube is performed in two stages: initial compression and the following relaxation. Results of calculations of compression degree on the collision energy for nucleon are presented, as well as maximum velocity in the process of system expansion for Brakner interaction and Skyrme interactiion. Spectra of neutrons in the 12C+158Gd reaction and proton spectra in the 16O+197Au reaction are calculated
Additional details
Additional titles
- Original title (Russian)
- Газодинамическая модел' столкновений тяжелых ионов промежуточных энергий и энымиссия высокоэнергетичх частиц
Publishing Information
- Imprint Title
- International school-seminar on heavy ion physics
- Journal Page Range
- p. 349-353.
- Report number
- JINR-D--7-83-644
Conference
- Title
- International school-seminar on heavy ion physics.
- Dates
- 14-21 Apr 1983.
- Place
- Alushta (USSR).
INIS
- Country of Publication
- USSR
- Country of Input or Organization
- USSR
- INIS RN
- 16029400
- Subject category
- S73: NUCLEAR PHYSICS AND RADIATION PHYSICS;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- CARBON 12 REACTIONS; COHERENT TUBE MODEL; EQUATIONS OF STATE; GADOLINIUM 158 TARGET; GOLD 197 TARGET; HEAVY ION REACTIONS; MEV RANGE 100-1000; NEUTRON SPECTRA; OXYGEN 16 REACTIONS; PROTON SPECTRA; SKYRME POTENTIAL
- Descriptors DEC
- ENERGY RANGE; EQUATIONS; MATHEMATICAL MODELS; MEV RANGE; NUCLEAR REACTIONS; NUCLEON-NUCLEON POTENTIAL; POTENTIALS; SPECTRA; TARGETS
Optional Information
- Notes
- Imprint:Mezhdunarodnaya shkola-seminar po fizike tyazhelykh ionov.