Radiationless Condition and Renormalization

Details Radiationless Condition and Renormalization Radiationless Condition and Renormalization

Jul 1966

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1966pthph..36..175h&link_type=abstract

Progress of Theoretical Physics, Vol. 36, No. 1, pp. 175-180

Physics

1

Scientific paper

The space-time behavior of the n-th elementary particle is represented by a trajectory with changing direction of time, the distance between adjacent kinks of the trajectory being L/n where L is the classical electron radius. L is numerically the distance between charge irregularities of the universe R/sqrt[]{N_e}, where N_e is the number of electrons in the universe of radius R. The radiationless condition for a point charge moving along this trajectory gives Nambu's mass formula. Another consequence of the radiationless condition is to cut off short wavelength components of self-action virtual quanta at sim L and guarantee a finite mass correction. It is also seen that the short wavelength ( < L) components are the very components that concentrate the charge (particle) within a small spatial distance sim L and give rise to the major part of the observed mass.

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