Lorentz Group Action on Ellips Space

Authors

  • Muhammad Ardhi Khalif Department of Physics, Faculty of Science and Technology, Semarang, Indonesia

DOI:

https://doi.org/10.21580/jnsmr.2015.1.2.1602

Keywords:

Physics Theory

Abstract

The ellips space E has been constructed as cartesian product R+ × R+ × [ π 2 , π 2 ]. Its elements, (a, b, θ), is called as an ellipse with eccentricity is = p1 b2/a2 if b < a and is = p1 a2/b2 if a > b. The points (a, b, π/2) is equal to (b, a, 0). The action of subgrup SOoz(3, 1) of Lorentz group SOo(3, 1), containing Lorentz transformations on xy plane and rotations about z axes, on E is defined as Lorentz transformation or rotation transformation of points in an ellipse. The action is effective since there are no rigid points in E. The action is also not free and transitive. These properties means that Lorentz transformations change any ellips into another ellips. Although mathematically we can move from an ellipse to another one with the bigger eccentrity but it is imposible physically. This is occured because we donot include the speed parameter into the definition of an ellipse in E.

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References

Wirdah, S., et. al, 2016, The change of geometrical objects due to alteration of frame of references: Circle and Ellipse, on revision

Iyer, C., Prabhu, G. M., 2007, Lorentz transformations with arbitrary line of motion, Eur. J.Phys.28 (2007) 183190

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Rosyid, M. F., 2015, Aljabar Abstrak Dalam Fisika, Gadjah Mada University Press, Yogyakarta

Tung, Wu-Ki., 1985, Group Theory in Physics, World Scientific, Philadelphia

Carmeli, M., 1977, Group Theory and General Relativity, McGraw-Hill Inc, New York

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Published

2017-08-22

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Section

Original Research Articles