论文标题
$ f(\ Mathbb {t},\ Mathcal {t})$ fravatars
Gravastars in $f(\mathbb{T},\mathcal{T})$ gravity
论文作者
论文摘要
我们在$ f(\ mathbb {t},\ mathcal {t})$重力下提出了一个恒星模型,因为Mazur-Mottola的猜想[Mazur(2001),Mazur(2004)]被称为Graverastar,通常被认为是Black Black Hole的可行替代品。 Grastar由三个区域组成,即(I)内部区域,(II)中间壳区域和(iii)外部区域。假定内核区域内的压力等于恒定的负物质能量密度,该密度在薄壳区域提供了恒定的排斥力。 The shell is assumed to be made up of fluid of ultrarelativistic plasma and following the Zel'dovich's conjecture of stiff fluid [Zeldovich (1972)] it is also assumed that the pressure which is directly proportional to the matter-energy density according to Zel'dovich's conjecture, does cancel the repulsive force exerted by the interior region.外部区域是完全真空的,可以通过Schwarzschild溶液来描述。在所有这些规格下,我们找到了一组省长的精确和无奇异性解决方案,在替代性重力的框架内呈现了几个物理有效的特征$ \ mathbb {t} $和能量量张量$ \ mathcal {t} $的跟踪。
We propose a stellar model under the $f(\mathbb{T},\mathcal{T})$ gravity following Mazur-Mottola's conjecture [Mazur (2001), Mazur (2004)] known as gravastar which is generally believed as a viable alternative to black hole. The gravastar consists of three regions, viz., (I) Interior region, (II) Intermediate shell region, and (III) Exterior region. The pressure within the interior core region is assumed to be equal to the constant negative matter-energy density which provides a constant repulsive force over the thin shell region. The shell is assumed to be made up of fluid of ultrarelativistic plasma and following the Zel'dovich's conjecture of stiff fluid [Zeldovich (1972)] it is also assumed that the pressure which is directly proportional to the matter-energy density according to Zel'dovich's conjecture, does cancel the repulsive force exerted by the interior region. The exterior region is completely vacuum and it can be described by the Schwarzschild solution. Under all these specifications we find out a set of exact and singularity-free solutions of the gravastar presenting several physically valid features within the framework of alternative gravity, namely $f(\mathbb{T},\mathcal{T})$ gravity [Harko (2014)], where the part of the gravitational Lagrangian in the corresponding action is taken as an arbitrary function of torsion scalar $\mathbb{T}$ and the trace of the energy-momentum tensor $\mathcal{T}$.