1. Introduction

After obtaining a unified mass theory of twelve elementary fermions [1], extravagant hopes naturally, subsequently what about the other six elementary bosons, $B=H,Z,W^{+},W^{-}$ and $\gamma ,g?!$ . May these six bosons be merged into the existing unified mass theory of twelve elementary fermions mentioned?

Ahead of us, light; Genesis of mass, light.

In this paper, we will use photon generation $\mathbf{Q}({\gamma }^{\mathrm{Q}},\xi )$ , instead of zeroth generation Zth of fermion $\mathbf{Q}(\mathrm{\Psi }(0),\xi )$ of Table 0 [1], to make a new larger Table X below, in which six elementary bosons B are included. Further, all the masses of both twelve elementary fermions and six elementary bosons of Standard Model SM could be uniformly identified.

IN Table 0, column ( $\mathbf{Q}(\mathrm{\Psi }(0),\xi )$ , $\xi (\mathrm{\Psi }(0))$ ) is the zeroth zh of generation of fermion.

IN Table X, column $(\mathbf{Q}({\gamma }^{\mathrm{Q}},\xi ),\xi ({\gamma }^{\mathrm{Q}}))$ is the generation of photon.

OR

The color representation of particle $\omega$ is defined as below. And $\xi (\omega )$ is called as mass function.

Base on ScalarProduct-Mass Equation, the mass value $M(\omega )$ of a particle $\omega$ could be obtained below

Here $\omega =F,B$ fermion, boson. CHARGE of $\omega$ rely on photon generation $\mathbf{Q}({\gamma }^{\mathrm{Q}},\xi )$ and MASS of $\omega$ relate to mass function $\xi (\omega )$ .

AND ${\mathbf{Q}}^2({\gamma }^{\mathrm{Q}},\xi )$ is the scalar product of $\mathbf{Q}({\gamma }^{\mathrm{Q}},\xi )$ that comprises four members, each one of $\mathbf{Q}({\gamma }^{\mathrm{Q}},\xi )$ with different charge: $Q({\gamma }^{\mathrm{Q}},\xi )=(0\mathrm{e},-\mathrm{e},\frac{-1\mathrm{e}}{3}\frac{-2\mathrm{e}}{3})\tilde{Q}({\gamma }^{\mathrm{Q}},\xi )=(0\mathrm{e},+\mathrm{e},\frac{-1\mathrm{e}}{3}\frac{-2\mathrm{e}}{3}).$

Analogy with what did for the masses of the twelves elementary fermions, NOW, the more detailed discussions for the masses of the six elementary bosons $\omega =H,Z,W^{+},W^{-}$ and $\gamma ,g$ are given in the next three parts Part A, Part B and Part C following

Part A and Part C are related to four neutral bosons H, Z and $\gamma g$ , that all with same charge, 0e, So, both H, Z and $\gamma g$ belong to the common photon generation members (A.1) (C.1) and (A.2) (C.2); But accompanied by the different mass function $\xi (\omega )$ : $\xi (Z)$ , $\xi (H)$ by (A.7), (A.8) and photon $\xi (\gamma )$ by (C.4), gluon $\xi (g)$ by (C.24), (C.25), ..... , (C.30), (C.31). Subsequently result in bosons Z, H massive (A.13), (A.12), and $\gamma g$ massless (C.9), (C.36). NOTICE: photon $\gamma$ is just ${\gamma }^{0e}$ .

Part B is related to two charged bosons $W^{-}$ , $W^{+}$ that with different particle charge -e, +e, So they belong to different photon generation. $W^{-}$ (B.1), $W^{+}$ (B.2); $W^{-}$ accompanied by mass function $\xi (W^{-})$ (B.13), $\xi (W^{+})$ by (B.14). BUT at last, the two particles possess the same mass valus (B.17) (B.18).

Table X is defined as ( more details see Table 2 and Table 3 Table 4 & Table 5 ) :

Before discuss Part A, Part B, Part C First, glance over Table 1, the archives of elementary fermion and elementary boson below

Decompose the color scalar products ${\mathbf{Q}}^2(B)$ of Six Bosons of the right column of Table1, into three dimensional color space $\mathbf{Q}(B)$ following

• Boson Ground States for massive particles $B=H,Z,W^{-},W^{+}$ :

• Boson Ground States for massless photon, gluon, $B=\gamma$ , $g$ :

The above six formulas $Q^2$ (0.2) (0.4) (0.6) (0.8) (0.10) will help us to use ScalarProduct-Mass Equation (00.4) (0.11) to calculate the mass $M(B)$ of the above six boson particle $\omega =B$

Later we will see the formulas $Q^2$ (0.2) (0.4) (0.6) (0.8) (0.10) are just formulas (A.13) (A.12) (B.17) (B.18) (C.9) (C.36).

1. Part A: Unified Mass Theory of Two Dirac Neutral Mass Bosons B = H, Z B = H, Z

◆ Detailed values of $\mathbf{Q}({\gamma }^0,\xi )$ of particles B=Z,H bwlow

The charges of particles $B=Z,H$ are zero

AND below

◆ Detailed values of mass function $\xi (B)$ of particles B = Z, H below

Where ${\xi }_0$ called as Color-Unit Constant that is a three dimensional colore vector, with which $\xi (\omega )$ could be limpid. see following

Expressions of the color scalar products of the above 0, 1, 2 are given below

Finally using ScalarProduct-Mass Equation (0.11): The masses of two neutral Dirac leptons Z, H are obtained by using a common color scalar product ${\mathbf{Q}}^2({\gamma }^0,\xi )$ of photon generation of particle ${\gamma }^0$ and color scalar product ${\xi }^2(Z)$ , ${\xi }^2(H)$ of mass function $\xi (Z)$ , $\xi (H)$ of particles Z, H