Document consolidé. 5 pages d'origine ont été réunies ici ; les liens ci-dessous ouvrent chaque section.
Collection : 1 J.P.Petit : 1998. — ce document en fait partie.
Sommaire
- Geometrization of matter and antimatter through
- Geometrization of matter and antimatter through
- Geometrization of matter and antimatter through
- Geometrization of matter and antimatter through
Geometrization of matter and antimatter through
coadjoint action of a group on its momentum space. 1 :
Charges as additional scalar components of the momentum of a group acting on a 10d-space.
Geometrical definition of antimatter. (p2)
Geometrization of matter and antimatter through
coadjoint action of a group on its momentum space. 1 :
Charges as additional scalar components of the momentum of a group acting on a 10d-space.
Geometrical definition of antimatter. (p3)
Geometrization of matter and antimatter through
coadjoint action of a group on its momentum space. 1 :
Charges as additional scalar components of the momentum of a group acting on a 10d-space.
Geometrical definition of antimatter. (p4)
Jpe = { q , cB , cL , cm , ct , v ,Jp }
Jj= { 0 , 0 , 0 , 0 , 0 , 0 ,Jp } : photon
Jp = { 1 , 1 , 0 , 0 , 0 , vp ,Jp } : proton
Jn = { 0 , 1 , 0 , 0 , 0 , vn ,Jp } : neutron
Je = { -1 , 0 , 1 , 0 , 0 , ve ,Jp } : electron
Jne = { 0 , 0 , 1 , 0 , 0 , vne ,Jp } : electronic neutrino
Jnm = { 0 , 0 , 0 , 1 , 0 , vnm ,Jp } : m neutrino
Jnt = { 0 , 0 , 0 , 0 , 1 , vnt ,Jp } : t neutrino
......We transform a particle into the corresponding antiparticle through charge conjugation ( C-symmetry). The charges of the photon are all zero, so that it identifies with its antiparticle.
Geometrization of matter and antimatter through
coadjoint action of a group on its momentum space. 1 :
Charges as additional scalar components of the momentum of a group acting on a 10d-space.
Geometrical definition of antimatter. (p5)
Pages d'origine : a4201.htm, a4202.htm, a4203.htm, a4204.htm, a4205.htm