2019
DOI: 10.1103/physrevd.99.103002
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Classification of a black hole spin out of its shadow using support vector machines

Abstract: We use Support Vector Machines (SVMs) to classify the spin of a black hole. The SVMs are trained and tested with a catalog of numerically generated images of black holes, assuming disk and spherical matter models with monochromatic emission with wavelength of 4mm. We determine the accuracy of the SVM to classify the spin in terms of the image resolution, for which we consider three resolutions of 16 2 , 32 2 and 64 2 pixels. Our approach is applied to the specific mass of the Supermassive Black Hole (SMBH) at … Show more

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Cited by 4 publications
(6 citation statements)
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“…Support Vector Machines (Cortes & Vapnik 1995) is one of the most well-established methods used in a wide range of topics. Some indicative examples include classification problems for variable stars (Pashchenko et al 2018), black hole spin (González & Guzmán 2019), molecular outflows (Zhang et al 2020), and supernova remnants (Kopsacheili et al 2020). The method searches for the line or the hyperplane (in two or multiple dimensions, respectively) that separates the input data (features) into distinct classes.…”
Section: Selected Algorithmsmentioning
confidence: 99%
“…Support Vector Machines (Cortes & Vapnik 1995) is one of the most well-established methods used in a wide range of topics. Some indicative examples include classification problems for variable stars (Pashchenko et al 2018), black hole spin (González & Guzmán 2019), molecular outflows (Zhang et al 2020), and supernova remnants (Kopsacheili et al 2020). The method searches for the line or the hyperplane (in two or multiple dimensions, respectively) that separates the input data (features) into distinct classes.…”
Section: Selected Algorithmsmentioning
confidence: 99%
“…The normal vector to Σ t at each point of the space-time is given by n µ = g µν n ν , where n ν = (−α, 0, 0, 0) is the 1-form measuring the density of hypersurfaces along the normal direction. We consider the matter to be a perfect fluid whose stressenergy tensor for a general space-time with metric g µν is T µν = ρ 0 hu µ u ν + pg µν , (2) where each volume element has rest mass density ρ 0 , specifi enthalpy h = 1 + e + p/ρ 0 , internal energy e, pressure p and 4-velocity u µ . With this metric one can construct expressions of the 4velocity of a flui element u µ = (u 0 , u i ) in terms of the velocities according to Eulerian observers:…”
Section: Hydrodynamics Equations On a Spherically Symmetric Space-timementioning
confidence: 99%
“…Formally the areal radius of the apparent horizon is R AH = γ θθ (t, r AH ), located where the outermost zero of Θ is found. Then we calculate the area of the AH as that of the corresponding 2-sphere A AH = 4πR 2 AH and the AH mass [22,23]. In our case, we are enforcing the condition γ θθ = r 2 , and therefore r AH = R AH .…”
Section: Apparent Horizonmentioning
confidence: 99%
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“…Basically, the cross-validation separates the training set into a fixed number of subsets and, sequentially, each one of those subsets is used to test the accuracy of the decision function obtained using the rest of the subsets. For a detailed explanation of the methods the reader can consult [21, 22] and for a specific setup of our implementation in a similar analysis [23]. Instead of implementing our own version of the support vector machine, we use the library libSVM [22].…”
Section: Direct and Inverse Problemsmentioning
confidence: 99%