Rogerio Deienno, Larry Denneau, David Nesvorný, David Vokrouhlický, William F. Bottke, Robert Jedicke, Shantanu Naidu, Steven R. Chesley, Davide Farnocchia, Paul W. Chodas
{"title":"The Debiased Near-Earth Object Population from ATLAS Telescopes","authors":"Rogerio Deienno, Larry Denneau, David Nesvorný, David Vokrouhlický, William F. Bottke, Robert Jedicke, Shantanu Naidu, Steven R. Chesley, Davide Farnocchia, Paul W. Chodas","doi":"arxiv-2409.10453","DOIUrl":null,"url":null,"abstract":"This work is dedicated to debias the Near-Earth Objects (NEO) population\nbased on observations from the Asteroid Terrestrial-impact Last Alert System\n(ATLAS) telescopes. We have applied similar methods used to develop the\nrecently released NEO model generator (NEOMOD), once debiasing the NEO\npopulation using data from Catalina Sky Survey (CSS) G96 telescope. ATLAS is\ncomposed of four different telescopes. We first analyzed observational data\nfrom each of all four telescopes separately and later combined them. Our\nresults highlight main differences between CSS and ATLAS, e.g., sky coverage\nand survey power at debiasing the NEO population. ATLAS has a much larger sky\ncoverage than CSS, allowing it to find bright NEOs that would be constantly\n\"hiding\" from CSS. Consequently, ATLAS is more powerful than CSS at debiasing\nthe NEO population for H $\\lesssim$ 19. With its intrinsically greater\nsensitivity and emphasis on observing near opposition, CSS excels in the\ndebiasing of smaller objects. ATLAS, as an all sky survey designed to find\nimminent hazardous objects, necessarily spends a significant fraction of time\nlooking at places on the sky where objects do not appear, reducing its power\nfor debiasing the population of small objects. We estimate a NEO population\ncompleteness of $\\approx$ 88%$^{+3\\%}_{-2\\%}$ for H $<$ 17.75 and $\\approx$\n36%$^{+1\\%}_{-1\\%}$ for H $<$ 22.25. Those numbers are similar to previous\nestimates (within error bars for H $<$ 17.75) from CSS, yet, around 3% and 8%\nsmaller at their face values, respectively. We also confirm previous finding\nthat the $\\nu_6$ secular resonance is the main source of small and faint NEOs\nat H = 28, whereas the 3:1 mean motion resonance with Jupiter dominates for\nlarger and brighter NEOs at H = 15.","PeriodicalId":501209,"journal":{"name":"arXiv - PHYS - Earth and Planetary Astrophysics","volume":"18 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Earth and Planetary Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10453","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
This work is dedicated to debias the Near-Earth Objects (NEO) population
based on observations from the Asteroid Terrestrial-impact Last Alert System
(ATLAS) telescopes. We have applied similar methods used to develop the
recently released NEO model generator (NEOMOD), once debiasing the NEO
population using data from Catalina Sky Survey (CSS) G96 telescope. ATLAS is
composed of four different telescopes. We first analyzed observational data
from each of all four telescopes separately and later combined them. Our
results highlight main differences between CSS and ATLAS, e.g., sky coverage
and survey power at debiasing the NEO population. ATLAS has a much larger sky
coverage than CSS, allowing it to find bright NEOs that would be constantly
"hiding" from CSS. Consequently, ATLAS is more powerful than CSS at debiasing
the NEO population for H $\lesssim$ 19. With its intrinsically greater
sensitivity and emphasis on observing near opposition, CSS excels in the
debiasing of smaller objects. ATLAS, as an all sky survey designed to find
imminent hazardous objects, necessarily spends a significant fraction of time
looking at places on the sky where objects do not appear, reducing its power
for debiasing the population of small objects. We estimate a NEO population
completeness of $\approx$ 88%$^{+3\%}_{-2\%}$ for H $<$ 17.75 and $\approx$
36%$^{+1\%}_{-1\%}$ for H $<$ 22.25. Those numbers are similar to previous
estimates (within error bars for H $<$ 17.75) from CSS, yet, around 3% and 8%
smaller at their face values, respectively. We also confirm previous finding
that the $\nu_6$ secular resonance is the main source of small and faint NEOs
at H = 28, whereas the 3:1 mean motion resonance with Jupiter dominates for
larger and brighter NEOs at H = 15.