Bio
Dr. ShaoXu Ren is a researcher at Tongji University, specializing in particle physics, elementary particle theory, and beyond the Standard Model physics.
Experience
Research
A Unified Mass Theory of Elementary Fermions and Elementary Bosons
Base on photon generation , a unified mass theory of elementary fermions and elementary bosons is postulated.
Quark-Colorization Of Cabibbo-Kobayashi-Maskawa Matrix CKM
This paper proposes an interesting representation VCKMïƒqRGB, ï‚®, ï™ïƒž of Cabibbo-Kobayashi-Maskawa Matrix CKM, which based on scalar products of quark color quantum numbers qR, qG, qB, or qRGB (00.1). This representation is called colorization of CKM in weak interaction. The colors of down-type quarks qw, ïƒwd, s, b in the quarkcolor scalar products of CKM are " Color-Broken, ï™ ï‚® 0 ", which results in isospin I3ïƒqw to be violated in weak interaction, further charges Qdsb CKMïƒï™rw, to be a slight deviated from 1 3 e of SM theoretical value. A short discussion of possible existence of higher-charges of quark q is given in Epilogue.
Colored Quark and Colored Gluon in Standard Model, Hadronic Constituents
In current particle physics, Color of aparticle and Spin of this particle belong to different space, and researchs on hadronic constituents are going under this guidance. In this paper base on color representation of flavor t, c, u, d, s, b of quarks and their antiquarks, color and spin are postulated to be combined into a common space STS. In this space, quark and gluon can be turned into colored quark and colored gluon directly by being colored with quark colors qR, qG, qB and antiquark colors qR, qG, qB. Along with such idea of hadronic constituents,Consequently we have: For observed baryon constituent: colored baryon particle and force-mediating coloredgluon particle. For observed meson constituent: colored meson particle and force-mediating colored gluon particle.. The above process of the color role related to hadronic constituents in this paper are much different from that of current SU(3)color. And total spin S3ïƒqqq, qqqcolor of colored baryon couldbe one-third series.And total spin S3ïƒqq, qqcolor of colored meson couldbezero,integer,evenhalf-integer.Although the phenomenons of such S3 may not beobserved. Colored pseudoscalar meson and colored vector meson separately are singlet and triplet ofspin-colorstate ïƒqq; ïŠ, ïŠïƒž, when colored gluons occupy color ground state ïƒ0, 0. Colored scalar meson and colored pseudo vector meson separately are singlet and triplet of spin-color state ïƒqq; ïŠ, ï‹ïƒž, when colored gluons transfer to color excited state ïƒï™1, ï™2, ï™ ï€½ ï™1  ï™2 ï‚® 0. The above introduction of gluon color ground state ïƒ0, 0 and gluon corlor excited state ïƒï™1, ï™2 instead of orbital angular momentums L  0 and L  1 of quarks in current theory. Possible new flovors X1, X2, X3 and Y1, Y2, Y3 are incidental to this paper. Multi quark hadrons constituents may refer this paper work too
Color of Flavor of Leptons
This paper suggests the possible existence of lepton color for charged leptons and neutral leptons as quarks possess Further lepton number conservation could be explained by lepton color scalar products. More detailsare given to search for the relationship between the broken lepton number and PMNS. And a speculation between broken lepton number and dark matter-energy.
Production and Decay of Higgs Boson, From God Particle H to Heaven Particle
This paper suggests an interesting idea: Based on quark genera (t, b), (c, s), (u, d) harmony flavor symmetry and Mass Principle Q2(ξ) – ξ2=Q2, Heaven particle Πwith M(Π)=692 Gev should instead of God particle H with M(H)=125 Gev. M(Π) as four times as heavy as ground state Q2(t) of t top quark.
Colorization of Gell-Mann-Nishijima Relation and Mass Principle, Origins of Mass; Fermions and Charges, Bosons and Color-Pairs
This paper offers color representation of Gell-mann-Nishijima Relation for quarks and leptons, in which the three quantum numbers, electrical charge, isospin and hypercharge all are colorized into three quantum colored numbers , and Y. Mass Principle is posulated to account for the mass effect of electrical charge Q. Particle mass M is suggested to be propertional to the scalar products of electrical charge Q of the particle. Further the observed twelve elementary fermion mass spectrum are given, which include those ones of three generation neutrinos. Although neutrinos are neutral particles, but their scalar products could be nonzero values. This paper presents a boson particle color mechanism about electrical charge , with which Higgs boson , and bosons could be constructed into the bound states of an elementary fermion and a anti-elementary fermion, each one with an opposite imaginary color of a Color-Pair, Further the masses of these bosons could be obtained by Mass Principle.
Force-Mediating Particle of Coupling of Spin Angular Momenta
In this paper, a hypothesis is proposed, that something similar to what happen to the puzzle of the energy losing in decay of neutron may also occur to the puzzle of the sum losing of the z-components of spin angular momenta in the synthetic course of spin coupling in Spin Topological Space. The former puzzle is related to hidden neutrial antineutrino that carries a small amount of energy away, the latter puzzle is related to hidden "constructive" zero-spin particle playing the role of a force-mediator that carries some amount of spin angular momentum, which just offsets the same amount of angular momentum losing in the formation of spin coupling.
From Majorana Neutrino and Dark Neutrino 0 to Dark Spin Particles
In current theory of particle physics, the values of Casimir Operator, that is abbreviated to CO, of spin angular momentum for elementary particles are thought to be greater than zero. Both Majorana Neutrino and Majorana Antineutrino are all with CO . Now the above limited region of CO is enlarged, this paper assumes that for the particles, the values of CO are still positive; for the antiparcles, however, the values of CO are negative. In this point of view, something similar is expected to happen in the case of Majorana Neutrino and Majorana Antineutrino . The Majorana Neutrino would be still with CO and the Majorana Antineutrino would be with CO . Further, leading to the possible existence of the so-called Dark Neutrino, DN or is with CO that is the superposition of Majorana Neutrino and Majorana Antineutrino And is the one-half spin fermion with zero-charge and zero-CO , which is a more neutral neutrino than Majorana neutrino. is one kind of Peculiar Dark Spin Particles.
