Authors: Angel Garcés Doz
The last neutron life-time experiments using the bottle method rule out possible experimental errors and possible sources of interference; mainly the interaction of the neutrons with the material of the walls of the bottle. Therefore, the discrepancy between the lifetimes of the neutron by experiments of the beam and the bottle require a theoretical explanation.The main and crucial difference between the beam and bottle experiments is the different topology of the experiments. While in the beam experiment the neutrons are not confined; in the experiment of the bottle a confinement takes place. In our theoretical approach we postulate the existence of a type of Casimir effect that due to the different geometry-topology of the experiments; it produces an induction-polarization of the vacuum by the confinement and the existence of the trapped neutrons; in such a way that there is an increase in the density of the quarks u, d, gluons and the virtual W and Z bosons. This density increase, mainly, of the neutral Z bosons; would be responsible for the increased probability of the decay of a neutron in a proton; and therefore of the shortening of the decay time of the neutron in the experiment of the bottle; of 877.7 seconds.
Comments: 9 Pages. Corrected Feynman diagram writing error
Unique-IP document downloads: 25 times
Vixra.org is a pre-print repository rather than a journal. Articles hosted may not yet have been verified by peer-review and should be treated as preliminary. In particular, anything that appears to include financial or legal advice or proposed medical treatments should be treated with due caution. Vixra.org will not be responsible for any consequences of actions that result from any form of use of any documents on this website.
Add your own feedback and questions here:
You are equally welcome to be positive or negative about any paper but please be polite. If you are being critical you must mention at least one specific error, otherwise your comment will be deleted as unhelpful.