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Shadow images of Kerr-like wormholes

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arxiv 1806.07782 v2 pith:QXCEOVSU submitted 2018-06-20 gr-qc

Shadow images of Kerr-like wormholes

classification gr-qc
keywords shadowkerr-likewormholesdeviationlambdaparametercompactkerr
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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Investigations of shadows of astrophysical entities constitute a major source of insight into the evolution of compact objects. Such effects depend on the nature of the compact object and arise on account of the strong gravitational lensing that casts a shadow on the bright background. We consider the Kerr-like wormhole spacetime (Phys.\ Rev.\ D 97:024040, 2018), which is a modification of the Kerr black hole that degenerates into wormholes for nonzero values of the deviation parameter $\lambda^2$. The results suggest that the Kerr spacetime can reproduce far away from the throat of the wormhole. We obtain the shapes of the shadow for the Kerr-like wormholes and discuss the effect of the spin $a$, the inclination angle $\theta_0$, and the deviation parameter $\lambda^2$ on the size and nature of the shadow. As a consequence, it is discovered that the shadow is distorted due to the spin as well as the deviation parameter and the radius of the shadow decreases with $\lambda^2$ if the ADM mass of the Kerr-like wormholes is considered.

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Forward citations

Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. On the Cuspy Structure of Rotating Wormhole Shadows

    gr-qc 2026-02 unverdicted novelty 6.0

    Rotating wormhole shadows develop cusps above a universal critical redshift value λ_c, yielding four morphologies: smooth, cuspy, ears touching, and throat drowning.

  2. Observational Limits on Einasto Dark Matter Parameters from Event Horizon Telescope Images of Sgr A$^{*}$ and M87$^{*}$

    gr-qc 2026-07 conditional novelty 5.0

    EHT dimensionless shadow diameters plus stellar-dynamical mass priors constrain Einasto central density to ρ₀ ≲ 10^{-11} M⊙/pc³ (1σ) for Sgr A*, with weaker bounds for M87*.