Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries

Abstract The present article investigates the existence of Noether and Noether gauge symmetries of flat Friedman–Robertson–Walker universe model with perfect fluid matter ingredients in a generalized scalar field formulation namely $$f(R,Y,\phi )$$ f ( R , Y , ϕ ) gravity, where R is the Ricci scala...

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Main Authors: Saira Waheed, Iqra Nawazish, M. Zubair
Format: Article
Language:English
Published: SpringerOpen 2021-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-021-08917-z
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spelling doaj-f70c11bfeb38481d84032fcb27989fd12021-02-14T12:44:31ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-02-0181212710.1140/epjc/s10052-021-08917-zIsotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetriesSaira Waheed0Iqra Nawazish1M. Zubair2Prince Mohammad Bin Fahd UniversityDepartment of Mathematics, COMSATS University IslamabadDepartment of Mathematics, COMSATS University IslamabadAbstract The present article investigates the existence of Noether and Noether gauge symmetries of flat Friedman–Robertson–Walker universe model with perfect fluid matter ingredients in a generalized scalar field formulation namely $$f(R,Y,\phi )$$ f ( R , Y , ϕ ) gravity, where R is the Ricci scalar and Y denotes the curvature invariant term defined by $$Y=R_{\alpha \beta }R^{\alpha \beta }$$ Y = R α β R α β , while $$\phi $$ ϕ represents scalar field. For this purpose, we assume different general cases of generic $$f(R,Y,\phi )$$ f ( R , Y , ϕ ) function and explore its possible forms along with field potential $$V(\phi )$$ V ( ϕ ) by taking constant and variable coupling function of scalar field $$\omega (\phi )$$ ω ( ϕ ) . In each case, we find non-trivial symmetry generator and its related first integrals of motion (conserved quantities). It is seen that due to complexity of the resulting system of Lagrange dynamical equations, it is difficult to find exact cosmological solutions except for few simple cases. It is found that in each case, the existence of Noether symmetries leads to power law form of scalar field potential and different new types of generic function. For the acquired exact solutions, we discuss the cosmology generated by these solutions graphically and discuss their physical significance which favors the accelerated expanding eras of cosmic evolution.https://doi.org/10.1140/epjc/s10052-021-08917-z
collection DOAJ
language English
format Article
sources DOAJ
author Saira Waheed
Iqra Nawazish
M. Zubair
spellingShingle Saira Waheed
Iqra Nawazish
M. Zubair
Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
European Physical Journal C: Particles and Fields
author_facet Saira Waheed
Iqra Nawazish
M. Zubair
author_sort Saira Waheed
title Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
title_short Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
title_full Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
title_fullStr Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
title_full_unstemmed Isotropic exact solutions in $$F(R,Y,\phi )$$ F ( R , Y , ϕ ) gravity via Noether symmetries
title_sort isotropic exact solutions in $$f(r,y,\phi )$$ f ( r , y , ϕ ) gravity via noether symmetries
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2021-02-01
description Abstract The present article investigates the existence of Noether and Noether gauge symmetries of flat Friedman–Robertson–Walker universe model with perfect fluid matter ingredients in a generalized scalar field formulation namely $$f(R,Y,\phi )$$ f ( R , Y , ϕ ) gravity, where R is the Ricci scalar and Y denotes the curvature invariant term defined by $$Y=R_{\alpha \beta }R^{\alpha \beta }$$ Y = R α β R α β , while $$\phi $$ ϕ represents scalar field. For this purpose, we assume different general cases of generic $$f(R,Y,\phi )$$ f ( R , Y , ϕ ) function and explore its possible forms along with field potential $$V(\phi )$$ V ( ϕ ) by taking constant and variable coupling function of scalar field $$\omega (\phi )$$ ω ( ϕ ) . In each case, we find non-trivial symmetry generator and its related first integrals of motion (conserved quantities). It is seen that due to complexity of the resulting system of Lagrange dynamical equations, it is difficult to find exact cosmological solutions except for few simple cases. It is found that in each case, the existence of Noether symmetries leads to power law form of scalar field potential and different new types of generic function. For the acquired exact solutions, we discuss the cosmology generated by these solutions graphically and discuss their physical significance which favors the accelerated expanding eras of cosmic evolution.
url https://doi.org/10.1140/epjc/s10052-021-08917-z
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