Abstract

The debiased absolute-magnitude and orbit distributions as well as source regions for near-Earth objects (NEOs) provide a fundamental frame of reference for studies of individual NEOs and more complex population-level questions. We present a new four-dimensional model of the NEO population that describes debiased steady-state distributions of semimajor axis, eccentricity, inclination, and absolute magnitude H in the range 17 < H < 25. The modeling approach improves upon the methodology originally developed by Bottke et al. (2000, Science 288, 2190–2194) in that it is, for example, based on more realistic orbit distributions and uses source-specific absolute-magnitude distributions that allow for a power-law slope that varies with H. We divide the main asteroid belt into six different entrance routes or regions (ER) to the NEO region: the ν6, 3:1J, 5:2J and 2:1J resonance complexes as well as Hungarias and Phocaeas. In addition we include the Jupiter-family comets as the primary cometary source of NEOs. We calibrate the model against NEO detections by Catalina Sky Surveys’ stations 703 and G96 during 2005–2012, and utilize the complementary nature of these two systems to quantify the systematic uncertainties associated to the resulting model. We find that the (fitted) H distributions have significant differences, although most of them show a minimum power-law slope at H ∼ 20. As a consequence of the differences between the ER-specific H distributions we find significant variations in, for example, the NEO orbit distribution, average lifetime, and the relative contribution of different ERs as a function of H. The most important ERs are the ν6 and 3:1J resonance complexes with JFCs contributing a few percent of NEOs on average. A significant contribution from the Hungaria group leads to notable changes compared to the predictions by Bottke et al. in, for example, the orbit distribution and average lifetime of NEOs. We predict that there are 962−56+52 (802−42+48×103) NEOs with H < 17.75 (H < 25) and these numbers are in agreement with the most recent estimates found in the literature (the uncertainty estimates only account for the random component). Based on our model we find that relative shares between different NEO groups (Amor, Apollo, Aten, Atira, Vatira) are (39.4,54.4,3.5,1.2,0.3)%, respectively, for the considered H range and that these ratios have a negligible dependence on H. Finally, we find an agreement between our estimate for the rate of Earth impacts by NEOs and recent estimates in the literature, but there remains a potentially significant discrepancy in the frequency of Tunguska-sized and Chelyabinsk-sized impacts.

Highlights

  • 1 B612 Asteroid Institute and DIRAC Institute Postdoctoral FellowM

  • NEOs are classified as potentially hazardous objects (PHOs) when their minimum orbital intersection distance (MOID) with respect to the Earth is less than 0.05 au and H < 22

  • Bottke et al (2002a) are unable to reproduce the NEO, and in particular Aten, inclination distribution (Greenstreet and Gladman, 2013). These shortcomings are most readily explained by the limited number of detections that the model was calibrated with, but may be explained by an unrealistic initial inclination distribution for the test asteroids which were used for computing the orbital steady-state distributions, or by not accounting for Yarkovsky drift when populating the so-called intermediate source regions in the main asteroid belt (MAB)

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Summary

B612 Asteroid Institute and DIRAC Institute Postdoctoral Fellow

703 AICc CSS ER G96 HFD IMC JFC MAB MBO ML MMR MPC MOID NEO PHO RMS SR YORP Amor Apollo Aten Atira Vatira a e i ω. Fitting a model with three escape routes from the MAB, that is, the ν6 secular resonance (SR), the intermediate Mars crossers (IMC), and the 3:1J mean-motion resonance (MMR) with Jupiter, to 138 NEOs detected by the Spacewatch survey, Bottke et al (2000) estimated that there are 910+−110200 NEOs with H < 18. Bottke et al (2002a) are unable to reproduce the NEO, and in particular Aten, inclination distribution (Greenstreet and Gladman, 2013) These shortcomings are most readily explained by the limited number of detections that the model was calibrated with, but may be explained by an unrealistic initial inclination distribution for the test asteroids which were used for computing the orbital steady-state distributions, or by not accounting for Yarkovsky drift when populating the so-called intermediate source regions in the MAB.

Theory and methods
Estimation of observational selection effects
Orbit integrator
Estimation of model parameters
Distribution of NEOs as observed by CSS
Observational selection effects of CSS
Identification of ERs in the MAB
Orbital evolution of NEOs originating in the MAB
Debiased NEO orbit and absolute-magnitude distributions
Selecting the preferred combination of steady-state orbit distributions
10 ERs 23 ERs 44600
The best-fit model with 7 ERs
Sensitivity to variations in orbit distributions
Sensitivity to observational data
Uniqueness
Comparison to other population estimates
Extrapolation to larger and smaller NEOs
Completeness of the current inventory of NEOs
Flux of NEOs from different ERs
NEAs on retrograde orbits
Findings
Collision rate on terrestrial planets
Conclusions
Full Text
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