Constraints on the time-scale of nuclear breakup from thermal hard-photon emission
arXiv:nucl-ex/0508032 · doi:10.1140/epja/i2006-09-017-2
Abstract
Measured hard photon multiplicities from second-chance nucleon-nucleon collisions are used in combination with a kinetic thermal model, to estimate the break-up times of excited nuclear systems produced in nucleus-nucleus reactions at intermediate energies. The obtained nuclear break-up time for the {Xe} + {Sn} reaction at 50{\it A} MeV is 100 -- 300 fm/ for all reaction centralities. The lifetime of the radiating sources produced in seven other different heavy-ion reactions studied by the TAPS experiment are consistent with 100 fm/, such relatively long thermal photon emission times do not support the interpretation of nuclear breakup as due to a fast spinodal process for the heavy nuclear systems studied.
arXiv comment11 pages, 9 figures, submitted to EPJA
References in corpus (9)
- A unitary isobar model for pion photo- and electroproduction on the proton up to 1 GeV
- Analysis of Pion Photoproduction Data
- First measurement of the Gerasimov-Drell-Hearn integral for Hydrogen from 200 to 800 MeV
- Multipole analysis of pion photoproduction based on fixed t dispersion relations and unitarity
- The helicity amplitudes A and A for the D resonance obtained from the reaction}
- Parameterisation of σ_{1/2}-σ_{3/2} for Q^2 \geq 0 and non-resonance contribution to the GDH sum rule
- Leading and higher twists in the proton polarized structure function at large Bjorken x
- The Drell-Hearn-Gerasimov Sum Rule
- The GDH sum rule for the deuteron