2013
DOI: 10.1007/s10773-013-1948-x
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Invariances and Conservation Laws Based on Some FRW Universes

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Cited by 11 publications
(7 citation statements)
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“…Since then the group classification problem has been studied intensely for fundamental equations arising from models in engineering and physics, e.g. the symmetry classification of the geodesic equations of Riemannian spaces [3,4], the symmetry classification of the two and three dimensional Newtonian systems [5,6,7,8] and many others [9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25]. Furthermore, a symmetry analysis of wave equation in a power-law Bianchi III spacetime spacetime can be found in [26] and a symmetry analysis of the wave equation on static spherically symmetric spacetimes, with higher symmetries, was recently carried out in [27] In [28], it was proved that for a linear, in the derivatives, second order partial differential equation (PDE) the Lie point symmetries are related with the conformal algebra of the geometry defined by the PDE.…”
Section: Introductionmentioning
confidence: 99%
“…Since then the group classification problem has been studied intensely for fundamental equations arising from models in engineering and physics, e.g. the symmetry classification of the geodesic equations of Riemannian spaces [3,4], the symmetry classification of the two and three dimensional Newtonian systems [5,6,7,8] and many others [9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25]. Furthermore, a symmetry analysis of wave equation in a power-law Bianchi III spacetime spacetime can be found in [26] and a symmetry analysis of the wave equation on static spherically symmetric spacetimes, with higher symmetries, was recently carried out in [27] In [28], it was proved that for a linear, in the derivatives, second order partial differential equation (PDE) the Lie point symmetries are related with the conformal algebra of the geometry defined by the PDE.…”
Section: Introductionmentioning
confidence: 99%
“…Here we note that it is only found one Noether symmetry in Reference [19] which is X 2 given in (24), and the remaining ones are not appeared in this reference. It follows from E L = 0 that a = 0, that is, a(t) = a 0 = constant, which is the Minkowski spacetime recovered in vacuum and so I 2 = I 3 = 0, I 4 = 4 f 0 a 3 0 and I 5 = 8 f 0 a 3/2 0 by (28).…”
Section: Vacuum Casementioning
confidence: 73%
“…Firstly, one can consider a strict Noether symmetry approach [18][19][20][21] which yields £ X L = 0, where £ X is the Lie derivative operator along X. On the other side, one could use the classical Noether symmetry approach with a functional term [22][23][24][25] which is a generalization of the strict Noether symmetry approach in the sense that the Noether symmetry equation includes a divergence of a functional boundary term. The classical Noether symmetry approach was originally established by Emmy Noether [26] and it gives a connection between a Noether symmetry and the existence of a first integral expressed in a simple form.…”
Section: Introductionmentioning
confidence: 99%
“…First, one can take a strict Noether symmetry approach [4][5][6], which results in £ X L = 0, where £ X is the Lie derivative operator along X. On the other hand, one can employ the Noether symmetry approach with a gauge term [7][8][9][10][11][12][13], a generalization of the strict Noether symmetry approach where the Noether symmetry equation includes the gauge term. Noether symmetries with a gauge term are equally valuable in addressing a variety of problems in physics and applied mathematics.…”
Section: Introductionmentioning
confidence: 99%