2005 APS April Meeting

Saturday–Tuesday, April 16–19, 2005; Tampa, FL

Session Z13: Nuclear Theory II

3:30 PM–4:54 PM, Tuesday, April 19, 2005
Marriott Tampa Waterside - Room 12

Sponsoring Unit: DNP
Chair: Ruprecht Machleidt, University of Idaho

Abstract: Z13.00005 : Bound nucleons have unique masses that govern elemental properties

Preview Abstract

Author:

  Eugene Pamfiloff 

It is known that measured binding energies associated with elements require equivalent energy to break the nuclear bond of a nucleus. Based upon the proposals contained in a recent published work [1] and with support from experimental high-energy data, it can be shown that a portion of listed binding energies are attributed to bound nucleons having a unique mass for every element. The figures show, relative to the hydrogen proton, that of the: a) 1.112 MeV binding energy per nucleon for ²H, 44% or 0.486 MeV represents a change in mass for the proton and neutron; b) of 5.629 MeV binding energy per nucleon for ⁷Li, 87% or 4.890 MeV represents a change of mass for each nucleon; c) likewise, ⁵⁶Fe has 8.811 MeV binding energy per nucleon and of this 92% or 8.119 MeV represents a change in mass for each nucleon; and ²³²Th has 7.639 MeV binding energy per nucleon and of this, 90% or 6.848 MeV represents a change in mass for each nucleon. This demonstrates that the nucleons of each element have unique masses. It can be shown that if three protons are removed from ₈₂Pb the result is not ₇₉Au. We conclude and predict that in addition to the Z number, elemental properties are determined by the unique proton and neutron masses for each element. [1] "The Order of the Forces''

---

---

The principle and conclusion presented in the above abstract were derived directly from the theoretical basis of the Geatron Nuclear Model (GNM). It is just one of the many important predictions that come from the model. For a comprehensive discussion of this unique nuclear model , visit the Geatron Nuclear Model at the link below. The Geatron Nuclear Model that is presented in this paper is a very straight forward model, one that identifies a single fundamental particle from which all other particles are formed and a single fundamental force from which all other forces emerge. It is the only nuclear model that explores fundamental particle physics through the interactions of the particles dominating that nuclear level.