Magnetized Anisotropic Bianchi Type-VI Cosmological Model Containing Dark Energy
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1 IOSR Journal of pplied Physics (IOSR-JP) e-issn: Volume 0, Issue Ver II (Jan eb 08), PP 3-35 wwwiosrjournalsorg Magnetized nisotropic Bianchi Type-VI Cosmological Model Containing Dark Energy Mukunda Dewri (Department of Mathematical Sciences, Bodoland University, India) Corresponding uthor: Mukunda Dewri bstract : The paper summarizes the Bianchi Type VI cosmological model with electromagnetic field Taking exponential scale factor and variable Lambda parameter the exact solutions of the field equations and different cosmological parameters have been found Magnetized anisotropic model with dark energy has been found Keywords: Bianchi Type VI, Electromagnetic field, Dark energy, Variable Lambda, ccelerated expansion Date of Submission: Date of acceptance: I Introduction The observational data obtained from various experiments like SNeIa, the CMB radiation anisotropies, LSS and X-ray experiments [-8] indicates the discovery of accelerated expansion of the present day universe Study of Bianchi type models shows that the models contain isotropic special cases and they permit arbitrarily small anisotropic levels at some instant of cosmic times Bianchi type cosmological models are important due to their homogenous and anisotropic nature, from the theoretical point of view also, anisotropic universe has a general significance than isotropic models The simplicity of the field equation made Bianchi space time useful in construction models of spatially homogenous and anisotropic cosmologies Ellis and Mac Callum [9] obtained solutions of Einstein's field equations for a Bianchi type VI space-time in the case of a stiff-fluid Collins [0] and Ruban [] have also presented some exact solutions of Bianchi type VI for perfect fluid distributions satisfying specific equations of state Some Bianchi VI cosmological models with gravitational field of the magnetic type has been studied by many authors [-4] Patel and Koppar [5] obtained some Bianchi type VI viscous fluid cosmological models Bali, Pradhan and Hassan [6-7] are some researchers who studied Bianchi type VI magnetized string cosmological models in General Relativity Pradhan and Bali [8-9] presented Bianchi type VI universe with decaying vacuum energy density Bali, Banerjee and Banerjee [0] studied some LRS Bianchi type VI cosmological models with special free Gravitational fields sgar and nsari [] investigated spatially homogeneous and totally anisotropic Bianchi type-vi bulk viscous cosmological models in Lyra geometry bdel-megied and Hegazy [] studied Bianchi type VI cosmological model in the presence of electromagnetic field with variable magnetic permeability in the framework of Lyra geometry In this paper, taking exponential scale factor and variable Lambda parameter Bianchi Type VI cosmological model with electromagnetic field has been studied II Metric nd ield Equations We consider Bianchi type- VI metric in the form ds = dt + dx + B e ax dy + C e ax dz () where, B and C are function of cosmic time t and a is a constant parameter The Einstein s field equations (with 8πG 4 = ) is given by c R i j gi j R + gi j Λ = Ti j () The energy momentum tensor for perfect fluid with electromagnetic field has the form T j i = ρ + p u i u j + pg i j + Ei j (3) Here ρ and p denote density and pressure respectively lso u i is the four velocity vector satisfying u i u i = In Eq (3), E j i is the electromagnetic field given by Lichnerowicz [3] E j i = μ h l h l u i u j + gi j hi h j, (4) where μ is the magnetic permeability and h i the magnetic flux vector defined by h i = μ ji u j, (5) where the dual electromagnetic field tensor ji is defined by Synge [4] DOI: 09790/ wwwiosrjournalsorg 3 Page
2 g Magnetized nisotropic Bianchi Type-VI Cosmological ji = ε ij kl kl (6) Here ij is the electromagnetic field tensor and ε ijkl is the Levi-Civita tensor density In the present model, the comoving coordinates are taken as u i = 0, 0, 0, (7) The incident magnetic field is taken along z-axis so that h = 0 = h = h 4, h 3 0 (8) The first set of Maxwell s equations [ij ;k] = 0, (9) μ ij ;j = J i (0) Require that is the function of x alone and the magnetic permeability is the function of x and t both Here semicolon represents a covariant differentiation Equation (9) leads to = constant () Here 3 = 3 = 4 = 0, 0 due to assumption of infinite electromagnetic conductivity The only nonvanishing component of ij is The non-vanishing components of E i j are μ E = = B e ax E = E 3 3 = E 4 4 () Now using equation (3)-(), the Einstein field equations () for the metric () reduces to following set of equations + Λ = p μ B e ax (3) B + B C + C + a B BC C + C C + C C a + B + B B B + C B B a + B C a C BC + Λ = p μ B e ax (4) + Λ = p + μ B e ax (5) + Λ = ρ + μ B e ax (6) B C = 0 (7) B C The proper volume V and average scale factor S for Bianchi type-vi Space time is V = S 3 = BC (8) The generalized mean Hubble parameter H is given by H = 3 H + H + H 3 (9) where H =, H = B, H B 3 = C are directional Hubble parameters in x, y, z directions C The scalar expansion Θ, shear scalar σ, anisotropy parameter Δ and the declaration parameter q have the following expressions Θ = 3H (0) σ = 3 i= H i 3H () 3 H i H Δ = 3 i= H () q = SS S (3) III Solution Of The ield Equations rom equation (7) we get B = C (3) Now let us assume, proper volume as V = S 3 = BC = c ( t c ) e t (3) where c, c > 0 DOI: 09790/ wwwiosrjournalsorg 3 Page
3 igure : Graph of proper volume with respect to time for c = c = To find a determinate solution, we first assume that Θ = constant This leads to = σ Cn (33) Then using (3) and (33) in (3) we get B = c ( t c ) e t C = c ( t c ) e t = c ( t c ) e t n + n + n n + Bianchi type- VI metric for this model is found to be in the form n ds = dt + c ( t c ) e t n + dx + c ( t c ) e t n + e ax dy + e ax dz (37) On solving the field equations with the help of (34)-(36), we obtain following parameter values p = n +n+ (n+) t c +4 t( t c ) ρ = n+ t c +4 (n+) t( t c ) Λ = a c ( t c ) e t n n + n+ t c +4 t t c + t 3 n+ 4t μ (n +) c ( t c ) e t n + e ax μ c ( t c ) e t (34) (35) (36) ( t c ) (38) (n +) n + e ax (39) (30) Hubble parameter and Scalar expansion are given by H = t c +4 6 t( t c ) Θ = t c +4 t( t c ) (3) (3) Shear scalar and nisotropy parameter are obtained as σ = (n ) 3(n+) t c +4 t( t c ) Deceleration parameter is obtained as q = + (33) = n (n+) (34) t ( t c ) t ( t c ) t 6 t + 3 ( t c ) t (35) DOI: 09790/ wwwiosrjournalsorg 33 Page
4 igure : Graph of deceleration parameter with respect to time for c = IV Conclusion In this paper, the proper volume is considered as V = c ( t c ) e t which is an exponential function of time t rom igure, it is observed that the proper volume increases at very high rate as time increases The proper volume of the model increases exponentially as t ; that is, the model is expanding with the increase of time The model (37) starts expansion with a big-bang singularity from t = and it goes on expanding as t Hubble s parameter and scalar expansion tend to zero as time tends to infinity The value of deceleration parameter tends to as time tends to infinity rom Eq (39), it is found that ρ is a decreasing function of time and ρ > 0 for all times The pressure is found to be negative in this model universe, which gives us a dark energy model with accelerated expansion of the universe or n, Θ σ 0 which indicates that the model does not approach isotropy rom Eq (30), it is found that the value of Λ for the model is large at initial stage and tends to small positive value as time increases, which is supported by the results from various observational data from Cosmological Projects (Perlmutter et al [6], Riess et al [7,7], Garnavich et al [5,6], Schmidt et al [8]) With 0, a magnetized Bianchi Type VI dark energy model with decaying energy density has been found References [] J K delman-mccarthy et al, The Sixth Data Release of the Sloan Digital Sky Survey, strophysjsupplser,75, 008, 97 [] P stier et al, The Supernova Legacy Survey: measurement of Ω M, Ω Λ and w from the first year data set, stron strophys,447, 006, 3 [3] P de Bernadis et al, flat Universe from high- resolution Maps of the cosmic microwave background radiation Nature, 404,000, 955 [4] C L Bennett et al,irst year Wilkinson Microwave nisotropy Probe (WMP) observation : Preliminary Maps and Basis Result strophysjsupplser,48,003, [5] E Komatsu et al, ive-year Wilkinson Microwave nisotropy Probe (WMP) observations: Cosmological Interpretation, strophysjsuppl,80,009,330 [6] S Permutter et al, Measurements of Omega and Lambda from 4 High- Redshift Supernova, strophys J, 57,999,565 [7] G Riess etal, Observational Evidence from Supernova for an ccelerating Universe and a Cosmological Constant, stron, J, 6,998,009 [8] U Seljak et al,cosmological parameter analysis including SDDS Ly-alpha forest and galaxy bias: constraints on the primordial spectrum of fluctuations, neutrino mass, and dark energy, Phys Rev D, 7, 005, 0355 [9] G R Ellis and M H Mac Callum, Class of Homogeneous Cosmological models, Communications in Mathematical Physics,, 969, 08-4 [0] C B Collins, More Qualitative Cosmology, Communications in Mathematical Physic3(), 97, [] Ruban, Preprint No 4, Leningrade Institute of Nuclear Physics, B P Konstrantinova, Preprint, 978 [] K Dunn and B O J Tupper, Class of Bianchi Type VI Cosmological Models with Electromagnetic ield, strophysical Journal, 04( ), 976, 3-39 [3] S R Roy and J P Singh, Some Bianchi VI Cosmo- logical Models with ree Gravitational ield of the agnetic Type, cta Phys ustriaca, 55(), 983, [4] B M Ribeiro and K Sanyal, Bianchi-VI Viscous luid Cosmology with Magnetic ield, Journal of Mathematical Physics, 8(3), 987, [5] L K Patel and S S Koppar, Some Bianchi Type VI Viscous luid Cosmological Models, J ustral Math Soc Ser B 33, 99, [6] R Bali, Pradhan and Hassan, Bianchi Type VI Magnetized Barotropic Bulk Viscous luid Massive String Universe in General Relativity, International Journal of Theoretical Physics 47(0), 008, [7] R Bali, R Banerjee and S K Banerjee, Bianchi Type VI Bulk Viscous Massive String Cosmological Models in General Relativity, 37(-), 008, -6 [8] Pradhan and R Bali, Magnetized Bianchi Type VI Barotropic Massive String Universe with Decaying Vacuum Energy Density Λ, EJTP 5(9), 008, 9-04 DOI: 09790/ wwwiosrjournalsorg 34 Page
5 [9] Pradhan, P Yadav and K Jotania, New Class of LRS Bianchi Type VI Universe with ree Gravitational ield and Decaying Vacuum Energy Density, 009, arxiv: [gr-qc] [0] R Bali, R Banerjee and S K Banerjee, Some LRS Bianchi Type VI Cosmological Models with Special ree Gravitational ields, EJTP 6, No 6,,009, [] sgar, M nsari, ccelerating Bianchi type VI bulk viscous cosmological models in Lyra geometry J Theor ppl Phys 8, 04, 9-4 [] M bdel-megied, E Hegazy, Bianchi type VI cosmological model with electromagnetic field in Lyra geometry Canadian Journal of Physics,, 94(0), 06, [3] Lichnerowica, Relativistic Hydrodynamics and Magneto hydrodynamics, W Benjamin Inc, New York, p93 (967) [4] J L Synge, Relativity: The General Theory, North-Holland Publ Co, msterdam, p 356 (960) [5] P M Garnavich et al, Constraints on cosmological models from Hubble Space Telescope Observations of High-Z Supernovae, strophys J 493, 998, L53 [6] P M Garnavich et al, Supernova Limits on the Cosmic equations of State, strophys J 509, 998, 74 [7] G Riess et al, Type I Supernova Discoveries at Z > from the Hubble Space Telescope: Evidence for past deceleration and constraints on Dark Energy Evolution, strophys J 607, 004, 665 [8] P Schmidt et al, The High-Z Supernova Search: Measuring Cosmic deceleration and global curvature of the universe using type I Supernova, strophys J 507, 998, 46 Mukunda Dewri "Magnetized nisotropic Bianchi Type-Vi Cosmological Model Containing Dark Energy IOSR Journal of pplied Physics (IOSR-JP), vol 0, no, 08, pp 3-35 DOI: 09790/ wwwiosrjournalsorg 35 Page
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