On a Knot Model of Mesons and Baryons
نویسنده
چکیده
A quantum knot model of mesons and baryons is established. This quantum knot model is derived from a quantum gauge model which is similar to the QCD gauge model. We first establish a knot model of the π mesons. We show that the π mesons are modeled by the prime knot 41 (which is assigned with the prime number 3). We show that the knot model of the π meson gives the strong interaction for the formation of the π meson and the weak decay π → μ + νμ. We give a mass machanism for the generation of the masses of the π meson, π meson, the muon μ and the muon neutrino νμ. We then extend the knot model to the K 0 and K mesons. We show that the K and K mesons are modeled by the prime knot 61 (which is assigned with the prime number 11) while the anti-particles K and K− are modeled by the mirror image of 61. We show that the strange degree of freedom of the strange quark is from the linking of knots of the K mesons. This linking gives the strong interaction for the associated production of elementary particles with strangeness. We then extend the knot model to the basic mesons η, ρ, ω,K∗, η′, and φ. These mesons are modeled by the prime knots 62,63,63,71,72,72 respectively where 62, 63, 71, 72 are assigned with the prime numbers 13, 17, 19, 23 respectively. We then extend the knot model to the basic baryons p, n,Λ, Σ,Ξ; ∆,Σ∗,Ξ∗, Ω− and Λ∗. We show that these baryons are modeled by the prime knots 62, 62,71,71,71; 71, 71, 71,72 and 71 respectively where 62,71,72 are assigned with the prime numbers 13, 19, 23 respectively. This knot model gives a unification of the electromagnetic, the weak and the strong interactions. We show that a meson or a baryon is modeled by a representation of the form W (K)Z where W (K) denotes a quantum knot and the components of the complex vector Z represent quarks. This is as the strong interaction for forming the meson or the baryon. Then two components zi, i = 1, 2 of Z may be separated such that they are still attached to W (K) in the form that they are attached to W (K) at two different positions of the quantum knot W (K). This process of separation is identified as the weak interaction of the two quarks (or leptons) represented by zi, i = 1, 2 of Z. We show that the existing quark model is as a part of this knot model. Thus this knot model is consistent with the existing quark model. PACS numbers: 12.40.-y, 12.40.Yx, 12.10.Dm, 12.60.-i.
منابع مشابه
ترکش مزونهای سنگین در LHC
Large Hadron Collider (LHC) at CERN will provide excellent opportunity to study the production and decay of heavy mesons and baryons with high statistics. We aim at the heavy mesons in this work and calculate their fragmentation functions consistent with this machine and present their total fragmentation probabilities and average fragmentation parameters.
متن کاملOn a classification of mesons
We give a mass formula for computing the mass spectrum of mesons. By this formula we show that there are many mesons with their masses corresponding to a prime number. In particular we show that all strange mesons are with their masses corresponding to a prime number. With these prime numbers indexing the mesons we give a classification of mesons. We set up a knot model of mesons to derive this...
متن کاملمحاسبه تابع ترکش مزون B با در نظر گرفتن اثر جرم مزون
Nowadays, heavy mesons and baryons are produced and decayed at LHC in abundance. These processes are good sources to study the QCD theory, especially to study the hadron structures. Therefore, the phenomenology of heavy hadrons fragmentation function is a basic and important subject in the Particle Physics. In the present work, we replicate the calculation heavy meson fragmentation function in...
متن کاملA Computation of The Mass Spectrum of Mesons and Baryons
In this paper we give a computation of the mass spectrum of mesons and baryons. By this computation we show that there is a consecutive numbering of the mass spectrum of mesons and baryons. We show that in this numbering many stable mesons and baryons are assigned with a prime
متن کاملHeavy Baryons and Multiquark Exotics in the Large N C Limit * Typeset Using Revt E X
In the large Nc limit, one can describe normal heavy baryons Qqq and heavy pentaquarks Q̄qqqq as bound states of heavy mesons to chiral (anti)solitons. In this picture, the strong and electromagnetic decay parameters of these hadrons can be calculated from those of the constituent heavy mesons and light baryons, while the weak decay form factors can be evaluated analytically. Typeset using REVTE...
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2007