Theory of electroweak interactions without spontaneous symmetry breaking

نویسنده

  • Bing An Li
چکیده

A electroweak theory without spontaneous symmetry breaking is studied in this paper. A new symmetry breaking of SU(2)L × U(1), axial-vector symmetry breaking, caused by the combination of the axial-vector component of the intermediate boson and the fermion mass is found in electroweak theory. The mass of the W boson is resulted in the combination of the axial-vector symmetry breaking and the explicit symmetry breaking by the fermion masses. The Z boson gains mass from the axialvector symmetry breaking only. mW = 1 2g mt , mZ = ρm 2 W /cos θW with ρ ' 1, and GF = 1 22m2t are obtained. They are in excellent agreement with data. The 1 SU(2)L × U(1) invariant generating functional of the Green’s functions is constructed and the theory is proved to be renormalizable. The cancellation of the gauge dependent spurious poles and the ghosts is resulted in the gauge independence of the renormalized s-matrix, which is proved by using the Ward-Takahashi identity.

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

/ 99 03 31 3 v 1 1 0 M ar 1 99 9 Theory of electroweak interactions without spontaneous symmetry breaking

A electroweak theory without spontaneous symmetry breaking is studied in this paper. A new symmetry breaking of SU(2)L × U(1), axial-vector symmetry breaking, caused by the combination of the axial-vector component of the intermediate boson and the fermion mass is found in electroweak theory. The mass of the W boson is resulted in the combination of the axial-vector symmetry breaking and the ex...

متن کامل

Unitarity constraints on top quark signatures of Higgsless models

We use conditions for unitarity cancellations to constrain the couplings of the top and bottom quarks to Kaluza-Klein modes in Higgsless models of electroweak symmetry breaking. An example for the mass spectrum of quark resonances in a theory space model is given and the implications for the collider phenomenology in the top sector are discussed, comparing to signatures of Little Higgs and stro...

متن کامل

Spontaneous Symmetry Breaking as a Basis of Particle Mass

Electroweak theory joins electromagnetism with the weak force in a single quantum field theory, ascribing the two fundamental interactions—so different in their manifestations—to a common symmetry principle. How the electroweak gauge symmetry is hidden is one of the most urgent and challenging questions facing particle physics. The provisional answer incorporated in the “standard model” of part...

متن کامل

ar X iv : h ep - t h / 96 12 09 1 v 1 9 D ec 1 99 6 Electroweak theory without spontaneous symmetry breaking ∗ hep - th / 9612091

The concept of perturbative gauge invariance formulated exclusively by means of asymptotic fields is generalized to massive gauge fields. Applying it to the electroweak theory leads to an essentially complete fixing of couplings of scalar and ghost fields and of the coupling to fermionic matter, in agreement with the standard theory. The W/Z mass ratio is also determined, as well as the chiral ...

متن کامل

Nobel Lecture: The BEH mechanism and its scalar boson

CONTENTS I. Introduction: Short and long range interactions 843 II. Spontaneous Symmetry Breaking 844 A. Spontaneous symmetry breaking in phase transitions 844 B. Spontaneous symmetry breaking in field theory 845 III. The BEH Mechanism 846 A. The fate of the Nambu-Goldstone boson and vector boson masses 846 B. The fate of the massive scalar boson 847 C. Fermion masses 848 D. Why is the mechanis...

متن کامل

ذخیره 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 1999