World-line condition for a spinning particle in superspace

1984 ◽  
Vol 82 (1) ◽  
pp. 17-28 ◽  
Author(s):  
J. Gomis ◽  
P. Mato ◽  
M. Novell
1995 ◽  
Vol 351 (1-3) ◽  
pp. 200-205 ◽  
Author(s):  
Myriam Mondragón ◽  
Lukas Nellen ◽  
Michael G. Schmidt ◽  
Christian Schubert

1983 ◽  
Vol 13 (3) ◽  
pp. 385-393 ◽  
Author(s):  
E. C. G. Sudarshan ◽  
N. Mukunda

1985 ◽  
Vol 31 (2) ◽  
pp. 314-318 ◽  
Author(s):  
F. Marquès ◽  
V. Iranzo ◽  
A. Molina ◽  
A. Montoto ◽  
J. Llosa
Keyword(s):  

2019 ◽  
Vol 1 (2) ◽  
pp. 181-192 ◽  
Author(s):  
Florio Maria Ciaglia ◽  
Fabio Di Cosmo ◽  
Alberto Ibort ◽  
Giuseppe Marmo

In this paper, a generalized form of relativistic dynamics is presented. A realization of the Poincaré algebra is provided in terms of vector fields on the tangent bundle of a simultaneity surface in R 4 . The construction of this realization is explicitly shown to clarify the role of the commutation relations of the Poincaré algebra versus their description in terms of Poisson brackets in the no-interaction theorem. Moreover, a geometrical analysis of the “eleventh generator” formalism introduced by Sudarshan and Mukunda is outlined, this formalism being at the basis of many proposals which evaded the no-interaction theorem.


2015 ◽  
Vol 30 (21) ◽  
pp. 1550101 ◽  
Author(s):  
Alexei A. Deriglazov ◽  
Walberto Guzmán Ramírez

Interaction of spin with electromagnetic field yields an effective metric along the world-line of spinning particle with anomalous magnetic moment. If we insist to preserve the usual special relativity definitions of time and distance, critical speed which the particle cannot overcome during its evolution in electromagnetic field differs from the speed of light. Instead, we can follow the general relativity prescription to define time and distance. With these definitions, critical speed coincides with the speed of light. But intervals of time and distance probed by the particle in the presence of electromagnetic field slightly differ from those in empty space. Effective metric arises also when spin interacts with gravitational field.


Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter discusses the kinematics of point particles undergoing any type of motion. It introduces the concept of proper time—the geometric representation of the time measured by an accelerated clock. It also describes a world line, which represents the motion of a material point or point particle P, that is, an object whose spatial extent and internal structure can be ignored. The chapter then considers the interpretation of the curvilinear abscissa, which by definition measures the length of the world line L representing the motion of the point particle P. Next, the chapter discusses a mathematical result popularized by Paul Langevin in the 1920s, the so-called ‘Langevin twins’ which revealed a paradoxical result. Finally, the transformation of velocities and accelerations is discussed.


1995 ◽  
Vol 36 (4) ◽  
pp. 1602-1615 ◽  
Author(s):  
T. Boudjedaa ◽  
A. Bounames ◽  
L. Chetouani ◽  
T. F. Hammann ◽  
Kh. Nouicer

1952 ◽  
Vol 8 (6) ◽  
pp. 670-672
Author(s):  
R. C. Majumdar ◽  
S. P. Pandya ◽  
S. Gupta

Sign in / Sign up

Export Citation Format

Share Document