• Aucun résultat trouvé

Nuclear positioning: A matter of life

N/A
N/A
Protected

Academic year: 2021

Partager "Nuclear positioning: A matter of life"

Copied!
3
0
0

Texte intégral

Loading

Références

Documents relatifs

This time dependence, well reproduced by the Lund model [Gallmeister 2005] (see figure 3.2 ), is due to the gluon emission during the vacuum fragmentation. In order to produce a

Some Important questions are ralsed, llke : how to disentangle between the propertles of the exclted matter and the mechanism of the reactlon, what 1s the equatlon of state of

In this talk we present a description of nuclear binding in a chiral approach based on the existence of a chiral invariant scalar field associated with the generation of the

For sufficiently large coupling λ, parity symmetry is broken spontaneously at T = 0, and it becomes restored at high temperature by a second order phase transition.. The order

Secondly when we introduce confinement, i.e, when we go beyond NJL, the evolution of the nucleon mass with density, also depends on the nucleon structure through the value of

In fitting nuclear binding energies with the extended LDM formula (4), special care has to be taken with the treatment of T = 0 pairing effects (or Wigner energy)— with an

In a recent paper [4] we have proposed to identify this chiral invariant s field with the sigma meson of nuclear physics and relativistic theories of the Walecka type, or,

The module entitled Nuclear Technology: A Matter of Energy is a learning guide designed to meet all the requirements of a Second- ary IV course.. If you meet meet all the