nuclear shell model

Also in the nuclear shell model angular momentum coupling is ubiquitous.

Article on the "nuclear shell model," giving nuclear shell filling for the various elements.

Its four stable isotopes have 82 protons, a magic number in the nuclear shell model of atomic nuclei.

In order to get these numbers, the nuclear shell model starts from an average potential with a shape something between the square well and the harmonic oscillator.

While working at Argonne in 1948, she developed the "nuclear shell model" to explain how neutrons and protons within atomic nuclei are structured.

He exploited the nuclear shell model and the collective, or unified, model, and also worked extensively on muonic atoms.

Ca is the lightest nucleus known to undergo double beta decay and the only one simple enough to be analyzed with the sd nuclear shell model.

Superimposed on this classical picture, however, are quantum-mechanical effects, which can be described using the nuclear shell model, developed in large part by Maria Goeppert-Mayer.

The nuclear shell model does just this and assumes that the individual neutrons and protons move in an average spherical or deformed (spheroidal) potential field.

In atomic nuclei, the spin-orbit interaction is much stronger than for atomic electrons, and is incorporated directly into the nuclear shell model.

This effect is not only experimentally observed, but is included to the semi-empirical mass formula and explained by some other nuclear models, such as nuclear shell model.

Maria Goeppert-Mayer was the second female Nobel Prize winner in Physics, for proposing the nuclear shell model of the atomic nucleus.

Jensen shared half of the 1963 Nobel Prize for Physics with Maria Göppert-Mayer for their proposal of the nuclear shell model.

This picture of the nucleus is called the nuclear shell model to obtain the information from experimental data and use it to calculate and predict energies which have not been measured.

The more sophisticated nuclear shell model is needed to mechanistically explain the route to the more energetically favorable outcome, in which one fission product is slightly smaller than the other.

Later D. Ivanenko and E. Gapon proposed the idea of the shell distribution of protons and neutrons in the nucleus (nuclear shell model).

An island of inversion is a region of the chart of nuclides that contains isotopes with a non-standard ordering of single particle levels in the nuclear shell model.

According to the nuclear shell model, radioactive nuclei that would decay into isotopes of these elements have closed neutron shells near the neutron drip line, where more neutrons cannot be added.

The hypothesis is based upon Nuclear shell model, which implies that the atomic nucleus is built up in "shells" in a manner similar to the structure of the much larger electron shells in atoms.

A model derived from the nuclear shell model is the alpha particle model developed by Henry Margenau, Edward Teller, J. K. Pering, T.H. Skyrme.

This circumstance explains in part why the nuclear isomeric shift was not discovered earlier: the appropriate nuclear theory and in particular the nuclear shell model were developed only in the late 1940s and early 1950s.

Among other things, these data showed abundance peaks for strontium, barium, and lead, which, according to quantum mechanics and the nuclear shell model, are particularly stable nuclei, much like the noble gases are chemically inert.

In nuclear physics and nuclear chemistry, the nuclear shell model is a model of the atomic nucleus which uses the Pauli exclusion principle to describe the structure of the nucleus in terms of energy levels.

According to the nuclear shell model there exists a class of isomers for which, in a first approximation, it is sufficient to consider one single nucleon, called the "optical" nucleon, to get an estimate of the difference between the charge distributions of the two isomer states, the rest of the nucleons being filtered out.