Fragmentation of spherical radioactive heavy nuclei as a novel probe of transient effects in fission

TL;DR

This study uses fragmentation of spherical radioactive heavy nuclei in relativistic collisions to measure transient effects in nuclear fission, revealing a consistent fission delay and nuclear dissipation strength.

Contribution

It introduces a novel experimental approach with radioactive isotopes to probe transient effects in fission, providing precise measurements of fission delay and dissipation.

Findings

Fission delay of approximately 3.3 x 10^-21 seconds for spherical nuclei.

Nuclear dissipation strength estimated at 4.5 x 10^21 s^-1.

Method effectively sheds light on previous controversies in fission dynamics.

Abstract

Peripheral collisions with radioactive heavy-ion beams at relativistic energies are discussed as an innovative approach for probing the transient regime experienced by fissile systems evolving towards quasi-equilibrium. A dedicated experiment using the advanced technical installations of GSI, Darmstadt, permitted to realize ideal conditions for the investigation of relaxation effects in the meta-stable well. Combined with a highly sensitive experimental signature, it provides a measure of the transient effects with respect to the flux over the fission barrier. Within a two-step reaction process, 45 proton-rich unstable spherical isotopes produced by projectile-fragmentation of a stable 238U beam have been used as secondary projectiles. The fragmentation of the radioactive projectiles on lead results in nearly spherical compound nuclei which span a wide range in excitation energy and fissility. The decay of these excited systems by fission is studied with a dedicated set-up which permits the detection of both fission products in coincidence and the determination of their atomic numbers with high resolution. The width of the fission-fragment nuclear charge distribution is shown to be specifically sensitive to pre-saddle transient effects and is used to establish a clock for the passage of the saddle point. The comparison of the experimental results with model calculations points to a fission delay of (3.3+/-0.7).10-21s for initially spherical compound nuclei, independent of excitation energy and fissility. This value suggests a nuclear dissipation strength at small deformation of (4.5+/-0.5).1021s-1. The very specific combination of the physics and technical equipment exploited in this work sheds light on previous controversial conclusions.