On the Koide-like Relations for the Running Masses of Charged Leptons, Neutrinos and Quarks

نویسنده

  • Zhi-zhong Xing
چکیده

Current experimental data indicate that the Koide relation for the pole masses of charged leptons, which can be parametrized as Q l = 2/3, is valid up to the accuracy of O(10−5). We show that the running masses of charged leptons fail in satisfying the Koide relation (i.e., Ql(μ) 6= 2/3), but the discrepancy between Ql(μ) and Q pole l is only about 0.2% at μ = MZ . The Koide-like relations for the running masses of neutrinos (1/3 < Qν(MZ) < 0.6), up-type quarks (QU(MZ) ∼ 0.89) and down-type quarks (QD(MZ) ∼ 0.74) are also examined from MZ up to the typical seesaw scale MR ∼ 1014 GeV, and they are found to be nearly stable against radiative corrections. The approximate stability ofQU(μ) andQD(μ) is mainly attributed to the strong mass hierarchy of quarks, while that of Ql(μ) and Qν(μ) is essentially for the reason that the lepton mass ratios are rather insensitive to radiative corrections. E-mail: [email protected] E-mail: [email protected] 1 1 Thanks to the precise measurements of three charged lepton masses [1], me = (0.510998918± 0.000000044) MeV , mμ = (105.6583692± 0.0000094) MeV , mτ = (

برای دانلود 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

Mass generation of the lepton sector

We discuss the necessity of a right-handed Weyl neutrino due to the vector-like phenomenon of the regularized Standard Model. It is shown that this right-handed neutrino is decoupled from low energies as a free particle, and Dirac neutrino masses are very small. We suggest gauge-invariant couplings between down quarks and charged leptons so that charged leptons acquire masses without extra Golt...

متن کامل

Mixing of Charge −1/3 Quarks and Charged Leptons with Exotic Fermions in E6

A way is suggested to understand why the average masses of (d, s, b) quarks are smaller than those of (u, c, t) quarks. In contrast to previously proposed mechanisms relying on different Higgs boson vacuum expectation values or different Yukawa couplings, the mass difference is explained as a consequence of mixing of (d, s, b) with exotic quarks implied by the electroweak-strong unification gro...

متن کامل

Possible reason why leptons are lighter than quarks.

The minimal model of spontaneously broken leptonic colour and discrete quarklepton symmetry predicts that charged leptons have the same masses as their partner charge +2/3 quarks up to small radiative corrections. By invoking a different pattern of symmetry breaking, a similar model can be constructed with the structural feature that charged leptons have to be lighter than their partner quarks ...

متن کامل

DSF 94/59 INFN NA IV 94/59 A Geometric Picture for Fermion Masses

We describe a geometric picture for the pattern of fermion masses of the three generations which is invariant with respect to the renormalization group below the electroweak scale. Moreover, we predict the upper limit for the ratio between the Dirac masses of the and neutrinos, m =m (9:6 0:6) 10 . The Standard Model [1, 2] of strong and electroweak interactions describes accurately all the obse...

متن کامل

X iv : h ep - p h / 05 05 22 0 v 1 2 5 M ay 2 00 5 The strange formula of Dr . Koide Alejandro Rivero

We present a short historical and bibliographical review of the lepton mass formula of Yoshio Koide, as well as some speculations on its extensions to quark and neutrino masses, and its possible relations to more recent theoretical developments. A subjective slice of history At the end of 1981 Yoshio Koide, working on some composite models of quarks and leptons, had the good or bad fortune of s...

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

برای دانلود 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

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2006