Optimization of Artificial Neural Networks models applied to the identification of images of asteroids' resonant arguments
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Abstract (arXiv)
The asteroidal main belt is crossed by a web of mean-motion and secular resonances, that occur when there is a commensurability between fundamental frequencies of the asteroids and planets. Traditionally, these objects were identified by visual inspection of the time evolution of their resonant argument, which is a combination of orbital elements of the asteroid and the perturbing planet(s). Since the population of asteroids affected by these resonances is, in some cases, of the order of several thousand, this has become a taxing task for a human observer. Recent works used Convolutional Neural Networks (CNN) models to perform such task automatically. In this work, we compare the outcome of such models with those of some of the most advanced and publicly available CNN architectures, like the VGG, Inception and ResNet. The performance of such models is first tested and optimized for overfitting issues, using validation sets and a series of regularization techniques like data augmentation, dropout, and batch normalization. The three best-performing models were then used to predict the labels of larger testing databases containing thousands of images. The VGG model, with and without regularizations, proved to be the most efficient method to predict labels of large datasets. Since the Vera C. Rubin observatory is likely to discover up to four million new asteroids in the next few years, the use of these models might become quite valuable to identify populations of resonant minor bodies.
Key facts. Cited by 1 paper in the map (data through 14 Oct 2026). Builds on 5 of its 20 references that are in the map. First posted on arXiv 28 Jul 2022.
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5 of 20 references.
References · 5
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- 2014Going Deeper with Convolutionscited by 4,241
- 2021Tails: Chasing Comets with the Zwicky Transient Facility and Deep Learningcited by 6
- 2021Artificial Neural Network classification of asteroids in the M1:2 mean-motion resonance with Marscited by 1
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