N-body light-cone mocks show 2-4 sigma deviations in third-order angular clustering between LCDM and f(R)/nDGP models at z=0.15-0.3 for halos and galaxies, with stronger signals in the dark-matter field.
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F(R)-phantom BTZ black holes satisfy the first law, undergo second-order phase transitions confirmed by Ehrenfest relations, and support stable circular orbits for massive and massless particles only in the phantom regime with negative curvature.
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Galaxy and halo angular clustering in LCDM and Modified Gravity cosmologies
N-body light-cone mocks show 2-4 sigma deviations in third-order angular clustering between LCDM and f(R)/nDGP models at z=0.15-0.3 for halos and galaxies, with stronger signals in the dark-matter field.
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Thermodynamics, Phase Transitions, and Geodesic Structure of $F(R)-$Phantom BTZ Black Holes
F(R)-phantom BTZ black holes satisfy the first law, undergo second-order phase transitions confirmed by Ehrenfest relations, and support stable circular orbits for massive and massless particles only in the phantom regime with negative curvature.