Searcharxiv⌕ Search

arXiv subjects

Abhi Savaliya

Publications and source records attributed to Abhi Savaliya.

3 recordsLinked to original sources

Gravitating Tubes Beyond World Line Paradigm In General Relativity

The simplest point-particle description of classical matter is incompatible with Einstein's General Relativity because the stress-energy tensor of a point particle is distributional and concentrated on a one-dimensional worldline. For such higher-codimension sources, smooth spacetime solutions generally do not exist. This obstruction was established by Geroch and Traschen for sources of codimension $\geq2$. Motivated by this result, this thesis proposes codimension-zero tubes as a fundamental description of gravitating matter. Timelike tubes are constructed within the tubular neighbourhood of an auxiliary timelike curve. The tube interior is foliated by timelike codimension-one hypersurfaces whose dynamics are governed by a brane-like action. The resulting collective stress-energy tensor is smooth, unlike that of a point particle. For a broad class of tension and potential profiles, the strong energy condition is violated inside the tube, while the null and weak energy conditions remain satisfied. In the ultraviolet limit, where the tube radius vanishes, an appropriate rescaling of the Lagrangian density reduces the tube action to the point-particle action together with a canonical self-force-like term. The particle's rest mass then emerges as an effective quantity rather than a fundamental localized parameter. Perturbative stability is analysed at two levels. Field perturbations yield an infinite squared sound speed, showing that the foliation-generating scalar is non-dynamical and cuscuton-like. Small deformations of the leaves lead to the Jacobi equation for timelike hypersurface congruences, further constraining admissible tension and potential profiles. These results establish gravitating tubes as a geometrically and dynamically consistent description of matter that respects the Geroch--Traschen obstruction.

gr-qc↗

Dynamical Dark Energy from a Massive Vector Field in Generalized Proca Theory

In this paper, we emphasise the recent observational findings from the Dark Energy Spectroscopic Instrument Data Release 2 (DESI DR2), which provide compelling evidence for a possible deviation from the standard $Λ$CDM (Cold Dark Matter) cosmology, suggesting the presence of a dynamically evolving effective dark energy component. Motivated by this, we construct a theoretical framework in which a massive cosmological vector field, $B^μ$, couples non-minimally to the background curvature through marginal interactions, offering a controlled mechanism to realise the deviation from the $Λ$CDM model. A detailed analysis of the effective Equation of State (EoS) parameter $w(\tilde H)$ reveals a narrow region of parameter space consistent with current cosmological observations presented by DESI. The analysis yields a stringent upper bound for the coupling constant $λ$ to be $λ<2.98\times10^{-11}$, a very strong bound on mass $3.1356\times10^{-66}~\text{g} \leq m \leq 3.3627\times10^{-66}~\text{g},$ and the admissible range $-0.405 \leq \log_{10}\tildeγ\leq -0.38$ for which present-day value $w_0 = w(\tilde H = 1)$ corresponding to a deviation $δ= w_0 + 1$ that lies within the region $0.107 \leq δ\leq 0.217$. This interval reproduces the deviation inferred from the combined DESI, Cosmic Microwave Background (CMB), and Pantheon+ data, reflecting a controlled departure from the $Λ$CDM behaviour. In summary, the results suggest that the proposed framework of a massive vector field can account for the departure from $Λ$CDM behaviour highlighted by DESI in the current cosmic acceleration. Furthermore, the framework approaches the $Λ$CDM behaviour in late-time $t\gtrsim28$ Gyr, establishing a direct phenomenological link between the underlying parameters and the observed dynamical nature of dark energy.

astro-ph.CO↗

Non-Local Classical Field Theory with Fractional Operators on $\mathbb{S}^3 \times \mathbb{R}^1$ Space

We present a theoretical framework on non-local classical field theory using fractional integrodifferential operators. Due to the lack of easily manageable symmetries in traditional fractional calculus and the difficulties that arise in the formalism of multi-fractional calculus over $\mathbb{R}^{\text{D}}$ space, we introduce a set of new fractional operators over the $\mathbb{S}^3 \times \mathbb{R}^1$ space. The redefined fractional integral operator results in the non-trivial measure canonically, and they can account for the spacetime symmetries for the underlying space $\mathbb{S}^3 \times \mathbb{R}^1$ with the Lorentzian signature $(+, -, -, -, -)$. We conclude that the field equation for the non-local classical field can be obtained as the consequence of the optimisation of the action by employing the non-local variations in the field after defining the non-local Lagrangian density, namely, $\mathcal{L}(ϕ_{a}\left(x\right), \mathbbð^αϕ_{a}\left(x\right))$, as the function of the symmetric fractional derivative of the field, e.g. in the context of the kinetic term, and the field itself.

physics.class-ph↗