| An alpha particle is a heavy nucleon, which is actually the nucleus of a helium atom. |
|
| As a result of the nucleon transformations, a new proton is left behind in the nucleus and the atomic number of the atom is raised by one. |
|
| In this respect the proton and neutron are seen as different states of a single basic nucleon. |
|
| The internal structure of the nucleon is fundamental to nuclear physics. |
|
| It's not until you get into the elements heavier than lead that you find nuclei whose binding energy per nucleon is low enough that the fission fragments could tunnel apart. |
|
| This allows us to observe at this point that within each nucleon, 2 primary order attractors are in action. |
|
| The form that must be in fact, a logic relation between the properties of nucleon and the properties of fluen that form it. |
|
| The properties of this nucleon, reported to the properties of fluen aren't only compatible, but they become even naturale, coherent. |
|
| The form, the dimensions and the profile of this nucleon must be also imposed by the properties of fluen. |
|
| Also a new idea the so-called infrared regularisation, was proposed for treating heavy particles such as the nucleon in the chiral expansion. |
|
| Division of the binding energy EB by A, the mass number, yields the binding energy per nucleon. |
|
| The original cosmic ray nucleon or its fragments that stay within the nucleus still have some energy after the initial collision, which they share with the components of the residual nucleus. |
|
| It has been determined experimentally that the binding energy per nucleon is a maximum of about 1.4 10−12 joule at an atomic mass number of approximately 60 that is, approximately the atomic mass number of iron. |
|
| The binding energy of a particular nucleon to a nucleus will depend on in addition to the factors considered above the odd even character of the nucleus. |
|
| Similarly, when the nucleus of an atom of 235U fissions into two smaller nuclei, the binding energy per nucleon again increases with a concomitant release of energy. |
|
| Between the fundamental properties of the nucleon, we situate the stability in the first row, then the capacity of being bound together in order to form the atomic nucleus and the other properties. |
|
| These two possible orientations of fluen or a joint of them might offer to the nucleon properties that are bound to the polarity, but doesn't justify the great stableness and the property of association inside the nucleus. |
|
| The configuration of this nucleon must present four poles, or four zones where there can be attached other fluenic formations, situated at the entrance or exit of the two imaginary axes that might stretch the two cores. |
|
| Some of this attraction is due to the scalar diquark content of the nucleon current. |
|
| Unmatter entities inside nuclei, predicted by the Brightsen nucleon cluster model. |
|
|
|
| In theory, quarks are closely bound within a nucleon connected by gluons to create protons, neutrons and other subatomic particles. |
|
| Swift heavy ions are heavy ions with kinetic energies of the order of 1 MeV per nucleon. |
|
| Three of the papers introduce the theory and phenomenology of transverse-momentum-dependent distributions and model quark TMDs using nucleon light-cone wave functions. |
|
| Neutrinos from the supernova 1987a were detected by the Kamioka Nucleon Decay Experiment detector in Japan. |
|
| Genomic DNA was isolated from whole blood using Nucleon BACC DNA extraction kit. |
|
