Microlensing Zone of Planets Detectable through the Channel of High-Magnification Events
arXiv:0808.3014 · doi:10.1088/0004-637X/691/1/452
Abstract
A microlensing lensing zone refers to the range of planet-star separations where the probability of detecting a planetary signal is high. Its conventional definition as the range between and 1.6 Einstein radii of the primary lens is based on the criterion that a major caustic induced by a planet should be located within the Einstein ring of the primary. However, current planetary lensing searches focus on high-magnification events to detect perturbations induced by another caustic located always within the Einstein ring very close to the primary lens (stellar caustic) and thus a new definition of a lensing zone is needed. In this paper, we determine this lensing zone. By applying a criterion that detectable planets should produce signals , we find that the new lensing zone varies depending on the planet/star mass ratio unlike the fixed range of the classical zone regardless of the mass ratio. The lensing zone is equivalent to the classical zone for a planet with a planet/star mass ratio and it becomes wider for heavier planets. For a Jupiter-mass planet, the lensing zone ranges from 0.25 to 3.9 Einstein radii, corresponding to a physical range between AU and 7.4 AU for a typical Galactic event. The wider lensing zone of central perturbations for giant planets implies that the microlensing method provides an important tool to detect planetary systems composed of multiple ice-giant planets.
6 pages, 5 figures
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- Extending the Planetary Mass Function to Earth Mass by Microlensing at Moderately High Magnification
- Planetary Lensing Signals of High-Magnification Events under Severe Finite-Source Effect
- KMT-2018-BLG-1025Lb: microlensing super-Earth planet orbiting a low-mass star
- Investigating the free-floating planet mass by Euclid observations
- Interpretation of Strong Short-Term Central Perturbations in the Light Curves of Moderate-Magnification Microlensing Events