Reviews
Expert reviews and annotations of scientific papers.
On the Origin of Chaos in the Asteroid Belt
It is showed that many three-body resonances involving the longitude of Saturn are chaotic. They gave simple expressions for the width of the chaotic region and the associated Lyapunov time.
— IŽ
It is showed that many three-body resonances involving the longitude of Saturn are chaotic. They gave simple expressions for the width of the chaotic region and the associated Lyapunov time.
— IŽ
BYORP and Dissipation in Binary Asteroids: Lessons from DART
Their findings suggest that for relatively spheroidal bodies composed of small-scale debris, such as Dimorphos, the BYORP effect may be significantly weaker and more sensitive to the object's size than earlier models predicted.
— IŽ
Their findings suggest that for relatively spheroidal bodies composed of small-scale debris, such as Dimorphos, the BYORP effect may be significantly weaker and more sensitive to the object's size than earlier models predicted.
— IŽ
Rotational breakup as the origin of small binary asteroids
While the origin of similar binaries (primary and satellite) in these two dynamically different populations (MB and NEA) was previously unknown, here is showed that they form via YORP-induced spin-up of 'rubble pile' asteroids.
— IŽ
While the origin of similar binaries (primary and satellite) in these two dynamically different populations (MB and NEA) was previously unknown, here is showed that they form via YORP-induced spin-up of 'rubble pile' asteroids.
— IŽ
Dancing with Venus in the shadow of the Earth: a pair of genetically related near-Earth asteroids trapped in a mean-motion resonance
They demonstrate that the Near-Earth Asteroids 2017 SN16 and 2018 RY7 currently follow an orbital path where their relative mean longitude remains stable. This lack of long-term drift is a direct result of the stabilizing influence of the 3:5 MMR with Venus.
— IŽ
They demonstrate that the Near-Earth Asteroids 2017 SN16 and 2018 RY7 currently follow an orbital path where their relative mean longitude remains stable. This lack of long-term drift is a direct result of the stabilizing influence of the 3:5 MMR with Venus.
— IŽ
Asteroid pairs: A complex picture
Authors derived and estimated many astrometric and physical parameters about 93 genetically connected asteroid pairs.
— IŽ
Authors derived and estimated many astrometric and physical parameters about 93 genetically connected asteroid pairs.
— IŽ
The Strength and Shapes of Contact Binary Objectcts
This research examines how strong the material of 'contact binary' asteroids must be to allow them to fuse into a single object.
— IŽ
This research examines how strong the material of 'contact binary' asteroids must be to allow them to fuse into a single object.
— IŽ
Astrometric detection of binary asteroids
This study explores the detection of binary systems via the astrometric shift of the photocenter relative to the barycenter. By utilizing this "wobble," we can probe regions of the binary asteroid phase-space that remain challenging for standard observational techniques to reach.
— IŽ
This study explores the detection of binary systems via the astrometric shift of the photocenter relative to the barycenter. By utilizing this "wobble," we can probe regions of the binary asteroid phase-space that remain challenging for standard observational techniques to reach.
— IŽ
Asteroid Systems: Binaries, Triples, and Pairs
Observational data confirms that binaries smaller than 20 km typically originate from rotational fission, a process driven by the YORP effect. This suggests a comprehensive framework where rotational fission and subsequent dynamical evolution account for the creation of small-scale binary, triple, and paired asteroid systems.
— IŽ
Observational data confirms that binaries smaller than 20 km typically originate from rotational fission, a process driven by the YORP effect. This suggests a comprehensive framework where rotational fission and subsequent dynamical evolution account for the creation of small-scale binary, triple, and paired asteroid systems.
— IŽ
Binary asteroid candidates in <i>Gaia</i> DR3 astrometry
This study details a specialized period-detection algorithm and presents its application to the Gaia DR3 catalog. The technique identifies periodic signatures by analyzing the post-fit residuals of the calculated orbits.
— IŽ
This study details a specialized period-detection algorithm and presents its application to the Gaia DR3 catalog. The technique identifies periodic signatures by analyzing the post-fit residuals of the calculated orbits.
— IŽ
The functional relation between three-body mean motion resonances and Yarkovsky drift speeds
Here are devised two equations that approximately describe the functional relation between the average time dtr spent in the three-body resonance, the strength of the resonance SR, and the semimajor axis drift speed da/dt (positive and negative) with the orbital eccentricities of asteroids in the range (0, 0.1).
— IŽ
Here are devised two equations that approximately describe the functional relation between the average time dtr spent in the three-body resonance, the strength of the resonance SR, and the semimajor axis drift speed da/dt (positive and negative) with the orbital eccentricities of asteroids in the range (0, 0.1).
— IŽ
The functional relation between mean motion resonances and Yarkovsky force on small eccentricities
Here is derived a functional relation that accurately describes dependence between the average time lead/lag dtr in mean motion resonances, the strength of the resonance SR, and the semimajor axis drift speed da/dt with asteroids’ orbital eccentricities in the range (0.1, 0.2).
— IŽ
Here is derived a functional relation that accurately describes dependence between the average time lead/lag dtr in mean motion resonances, the strength of the resonance SR, and the semimajor axis drift speed da/dt with asteroids’ orbital eccentricities in the range (0.1, 0.2).
— IŽ
The relationship between the `limiting' Yarkovsky drift speed and asteroid families' Yarkovsky V-shape
The main conclusion of this study is: the location of the inverse of the ‘limiting’ diameter 1/D(limit) (derived from the ‘limiting’ Yarkovsky drift speed, 7 × 10^(−5) au/Myr) is exactly at the place of changing the V-shape slope of the border in an old asteroid family which are crossed in the same side by relatively strong mean motion resonance, very close to the parent body, in the (a, 1/D) plane.
— IŽ
The main conclusion of this study is: the location of the inverse of the ‘limiting’ diameter 1/D(limit) (derived from the ‘limiting’ Yarkovsky drift speed, 7 × 10^(−5) au/Myr) is exactly at the place of changing the V-shape slope of the border in an old asteroid family which are crossed in the same side by relatively strong mean motion resonance, very close to the parent body, in the (a, 1/D) plane.
— IŽ
The specific property of motion of resonant asteroids with very slow Yarkovsky drift speeds
This paper has presented a new description on the orbital behavior of resonant asteroids with very small Yarkovsky drift speeds. The conclusion is the boundary value of da/dt in the motion of resonant main belt asteroids under the influence of the Yarkovsky effect is at |−7| ×10^(−5) au/Myr. Below this value, asteroids typically quickly jump across the mean motion resonances, and this is especially the case in strong resonances, such as 9:4, 8:3 and 13:6 with Jupiter.
— IŽ
This paper has presented a new description on the orbital behavior of resonant asteroids with very small Yarkovsky drift speeds. The conclusion is the boundary value of da/dt in the motion of resonant main belt asteroids under the influence of the Yarkovsky effect is at |−7| ×10^(−5) au/Myr. Below this value, asteroids typically quickly jump across the mean motion resonances, and this is especially the case in strong resonances, such as 9:4, 8:3 and 13:6 with Jupiter.
— IŽ
Interaction between Yarkovsky force and mean-motion resonances: Some specific properties
It would be easy to calculate the average time that an object spent inside an mean-motion resonance, with given the resonance’s strength, the Yarkovsky drift speed and an object’s eccentricity (0.025<e<0.4). The derived modified Laplace statistical distribution could be used for generating the average time for certain number of asteroids with a particular Yarkovsky drift speed in mean motion resonances.
— IŽ
It would be easy to calculate the average time that an object spent inside an mean-motion resonance, with given the resonance’s strength, the Yarkovsky drift speed and an object’s eccentricity (0.025<e<0.4). The derived modified Laplace statistical distribution could be used for generating the average time for certain number of asteroids with a particular Yarkovsky drift speed in mean motion resonances.
— IŽ
THE ROLE OF MEAN-MOTION RESONANCES IN SEMIMAJOR AXIS MOBILITY OF ASTEROIDS
This Letter presents a novel view on the interaction between mean-notion resonances and the Yarkovsky effect, describing for the first time the functional relationship between the average time spent inside a resonance, the strength of the resonance, and the semimajor axis drift speed.
— IŽ
This Letter presents a novel view on the interaction between mean-notion resonances and the Yarkovsky effect, describing for the first time the functional relationship between the average time spent inside a resonance, the strength of the resonance, and the semimajor axis drift speed.
— IŽ
The three principal secular resonances ν5, ν6, and ν16 in the asteroidal belt
A simple analytical model for the secular resonance ν6 in the asteroidal belt
The main secular resonances ν6, vs and ν16 in the asteroid belt
The positions of secular resonance surfaces
Chaotic Evolution of the Solar System
The chaotic motion of the solar system: A numerical estimate of the size of the chaotic zones
Discovery of a young subfamily of the (221) Eos asteroid family
SECULAR RESONANCE SWEEPING OF THE MAIN ASTEROID BELT DURING PLANET MIGRATION
Secular resonances in the asteroid belt: Theoretical perturbation approach and the problem of their location
The Secular Resonances in the Solar System
Secular perturbation theory and computation of asteroid proper elements
Implementation of secular resonance support in the open-source python package "resonances"
If you need to identify whether or not an asteroid is trapped in secular resonance, this is the package for you.
— ES
If you need to identify whether or not an asteroid is trapped in secular resonance, this is the package for you.
— ES
On the Erigone family and the z2 secular resonance
The (not so) peculiar case of the Padua family
The peculiar case of the Agnia asteroid family
Yarkovsky footprints in the Eos family
Machine learning classification of new asteroid families members
The quest for young asteroid families: new families, new results
Asteroid Proper Elements and the Dynamical Structure of the Asteroid Main Belt
A frequency approach to identifying asteroid families
The resonant population of asteroids in librating states of the ν6 linear secular resonance
Contains a list of specific asteroids that are in secular resonances. Useful for comparison or software testing.
— ES
Contains a list of specific asteroids that are in secular resonances. Useful for comparison or software testing.
— ES
The asteroid population in g-type non-linear secular resonances
Secular resonances from 2 to 50 AU
Asteroid proper elements and secular resonances
Asteroid families interacting with secular resonances
Secular Resonance Maps
Complete list of secular resonances by order with unified notation
— ES
Complete list of secular resonances by order with unified notation
— ES
Survey of secular resonances in the asteroid belt
A comprehensive overview of existing secular resonances and their classification by dynamic zones. An excellent start for understanding!
— ES
A comprehensive overview of existing secular resonances and their classification by dynamic zones. An excellent start for understanding!
— ES
Deep learning identification of asteroids interacting with g-s secular resonances
On the identification of the first two young asteroid families in g-type non-linear secular resonances
Identification of asteroid groups in the z1 and z2 nonlinear secular resonances through genetic algorithms
Dynamical evolution of NEAs: Close encounters, secular perturbations and resonances
Interesting to isolate encounters vs. secular/MMR resonance effects.
— VC
Interesting to isolate encounters vs. secular/MMR resonance effects.
— VC
V‐type near‐Earth asteroids: Dynamics, close encounters and impacts with terrestrial planets
Interesting for learning about close encounters and impacts of V-type asteroids with terrestrial planets, but a bit niche.
— VC
Interesting for learning about close encounters and impacts of V-type asteroids with terrestrial planets, but a bit niche.
— VC
Origin and dynamics of Near Earth Objects
A dynamical steady-state model links NEO orbits to asteroid-belt resonances, highlighting Yarkovsky drift as the key resupply mechanism. A bit outdated.
— VC
A dynamical steady-state model links NEO orbits to asteroid-belt resonances, highlighting Yarkovsky drift as the key resupply mechanism. A bit outdated.
— VC
Identification and analysis of interior and exterior resonant orbits in the Sun–Venus system
Interesting paper to learn about the dynamics of mmr with Venus in the CR3BP model. Advanced, require some background in celestial mechanics.
— VC
Interesting paper to learn about the dynamics of mmr with Venus in the CR3BP model. Advanced, require some background in celestial mechanics.
— VC
Planar near-Earth asteroids in resonance with the Earth
Useful to learn about what mmr with Earth may be relevant for NEOs. Quite advanced, not an easy reading.
— VC
Useful to learn about what mmr with Earth may be relevant for NEOs. Quite advanced, not an easy reading.
— VC