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Generalized Extended Uncertainty Principle Black Holes: Shadow and Lensing in the Macro- and Microscopic Realms
by
Pantig, Reggie C.
, Lobos, Nikko John Leo S.
in
black hole
/ Black holes
/ Deflection
/ Gauss–Bonnet theorem
/ generalized extended uncertainty principle
/ Principles
/ shadow cast
/ Shadows
/ Spacetime
/ strong gravitational lensing
/ Uncertainty principles
/ weak gravitational lensing
2022
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Generalized Extended Uncertainty Principle Black Holes: Shadow and Lensing in the Macro- and Microscopic Realms
by
Pantig, Reggie C.
, Lobos, Nikko John Leo S.
in
black hole
/ Black holes
/ Deflection
/ Gauss–Bonnet theorem
/ generalized extended uncertainty principle
/ Principles
/ shadow cast
/ Shadows
/ Spacetime
/ strong gravitational lensing
/ Uncertainty principles
/ weak gravitational lensing
2022
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Do you wish to request the book?
Generalized Extended Uncertainty Principle Black Holes: Shadow and Lensing in the Macro- and Microscopic Realms
by
Pantig, Reggie C.
, Lobos, Nikko John Leo S.
in
black hole
/ Black holes
/ Deflection
/ Gauss–Bonnet theorem
/ generalized extended uncertainty principle
/ Principles
/ shadow cast
/ Shadows
/ Spacetime
/ strong gravitational lensing
/ Uncertainty principles
/ weak gravitational lensing
2022
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Generalized Extended Uncertainty Principle Black Holes: Shadow and Lensing in the Macro- and Microscopic Realms
Journal Article
Generalized Extended Uncertainty Principle Black Holes: Shadow and Lensing in the Macro- and Microscopic Realms
2022
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Overview
Motivated by the recent study about the extended uncertainty principle (EUP) black holes, we present in this study its extension called the generalized extended uncertainty principle (GEUP) black holes. In particular, we investigated the GEUP effects on astrophysical and quantum black holes. First, we derive the expression for the shadow radius to investigate its behavior as perceived by a static observer located near and far from the black hole. Constraints to the large fundamental length scale, L*, up to two standard deviations level were also found using the Event Horizont Telescope (EHT) data: for black hole Sgr. A*, L*=5.716×1010 m, while for M87* black hole, L*=3.264×1013 m. Under the GEUP effect, the value of the shadow radius behaves the same way as in the Schwarzschild case due to a static observer, and the effect only emerges if the mass, M, of the black hole is around the order of magnitude of L* (or the Planck length, lPl). In addition, the GEUP effect increases the shadow radius for astrophysical black holes, but the reverse happens for quantum black holes. We also explored GEUP effects to the weak and strong deflection angles as an alternative analysis. For both realms, a time-like particle gives a higher value for the weak deflection angle. Similar to the shadow, the deviation is seen when the values of L* and M are close. The strong deflection angle gives more sensitivity to GEUP deviation at smaller masses in the astrophysical scenario. However, the weak deflection angle is a better probe in the micro world.
Publisher
MDPI AG
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