Journal Article 1 Mention
Free-floating Planet Mass Function from MOA-II 9 yr Survey toward the Galactic Bulge
T. Sumi2023
Naoki KoshimotoD. P. Bennett
Top 1% · 99th Percentile
81 citations · Astronomy and Astrophysics
Open Access重力マイクロレンズを用いた地球質量の系外惑星、浮遊惑星及びブラックホールの探査Revealing the Planet Mass Function beyond the Snow LineSearch for free-floating planets by using gravitational microlensingOUR PROPOSAL INVOLVES FOLLOW-UP OBSERVATIONS OF MORE THAN 60 PLANETARY AND STELLAR BINARY MICRO LENSING EVENTS IN AN ATTEMPT TO IDENTIFY AND MEASURE THE BRIGHTNESS OF THE LENS STARS FOR THESE MICROLENSING EVENTS. THE KECK DATA WILL INCLUDE LASER GUIDE STAR ADAPTIVE OPTICS (AO) IMAGES FROM THE NIRC2 AND OSIRIS INFRARED CAMERAS. THIS PROJECT WILL BE MANAGED BY THE P.L. DAVID BENNETT WHO WILL LEAD THE LIGHT CURVE MODELING EFFORT TO DETERMINE WHICH EVENTS TO OBSERVE AS A FUNCTION OF OBSERVING CONDITIONS. HE WILL BE RESPONSIBLE FOR SELECTING THE TARGETS TO BE OBSERVED AND TO DETERMINE THE OBSERVING PLANS. THE DATA REDUCTION FOR THIS DATA WILL BE THE RESPONSIBILITY OF POSTDOC DR. APAMA BHATTACHARYA WITH THE HELP OF CO-I'S J.-P. BEAULIEU AND JESSICA LU (WHO ARE NOT FUNDED BY THIS PROPOSAL). BOTH BEAULIEU AND LU HAVE EXTENSIVE EXPERIENCE ANALYZING KECK DATA AND THEIR METHODS AND SOFTWARE WILL BE USED FOR BOTH THE OBSERVATIONS AND THE ANALYSIS. WE EXPECT THAT THIS ANALYSIS WILL LEAD TO A LARGE NUMBER OF PAPERS AND WE EXPECT THAT THE INFORMATION PROVIDED IN THESE PAPERS ON THE MAGNITUDES AND RELATIVE PROPER MOTIONS OF THE SOURCE AND LENS STARS WILL BE THE PRIMARY INPUTS FOR FUTURE WORK ON THESE EVENTS. IN ADDITION TO THESE PUBLICATIONS AND ASSOCIATED HIGH LEVEL DATA PRODUCTS WE WILL ALSO PROVIDE CALIBRATED CO-ADDED IMAGES OF EACH TARGET THAT IS OBSERVED WITH A GOOD AO CORRECTION TO THE NASA EXOPLANET ARCHIVE. IN MOST CASES TARGETS WILL BE OBSERVED IN MULTIPLE PASSBANDS AND WE WILL USUALLY OBTAIN DEEP HIGH RESOLUTION IMAGES (WITH THE NIRC-2 NARROW CAMERA) AND SHALLOWER WIDER ANGLE IMAGES (WITH THE NIRC-2 WIDE CAMERA) TO AID IN CALIBRATION TO 2MASS OR VVV STANDARD STARS. WE WILL PROVIDE A SINGLE CO-ADDED IMAGE IN EACH PASSBAND WITH EACH CAMERA THAT WAS USED TO THE NASA EXOPLANET ARCHIVE. THE PUBLICATIONS DESCRIBING THE ANALYSIS OF EACH EVENT WILL PROVIDE DETAILS ON THE LOCATION OF THE SOURCE STAR BASED ON DIFFERENCE IMAGES TAKEN CLOSE TO MAXIMUM MICROLENSING MAGNIFICATION AND IFWE OBTAIN PERMISSION FROM THE MICROLENSING OBSERVING GROUPS THAT OWN THESE DATA WE WILL ALSO ADD THESE TO THE NASA EXOPLANET ARCHIVE. WE PLAN TO SUBMIT THIS DATA TO THE NASA EXOPLANET ARCHIVE ON A ROLLING BASIS AS EACH EVENT IS ANALYZED AND IMAGES FOR ALL THE EVENTS WITH GOOD DATA WILL BE SUBMITTED BY FEBRUARY 28 2021.近赤外線重力マイクロレンズ観測による冷たい系外惑星・浮遊惑星の形成過程の解明

TLDR

The Milky Way may contain many more planets wandering without stars than planets orbiting far from stars. Most could be small, but the estimate remains uncertain because it relies on only a handful of brief signals.

Summary

1 Study Aim

The authors aimed to measure the mass function of free-floating planets (planets without detectable host stars) using nine years of observations. They also included planets on extremely wide orbits, whose stars would not appear in the data. The study tested whether brief gravitational microlensing events (temporary brightening caused by a foreground object bending starlight) require a planetary population beyond known stars and brown dwarfs. The study asks whether short, faint lensing signals reveal a large population of small planets.

2 Study Design

The research analyzed 3,535 carefully selected single-lens events from the MOA-II survey toward the Galactic bulge, collected from 2006 through 2014. The authors modeled each event using its Einstein-radius crossing time (how long the lensing signal lasts) and, when available, its angular Einstein radius (the lensing scale seen in the sky). The sample included 10 events lasting under one day and 13 with finite-source effects (changes caused by the source star’s size). Image-level simulations measured detection efficiency across both measurements. The team then used a Galactic population model and Markov Chain Monte Carlo (MCMC, repeated random sampling) likelihood analysis to fit planetary and known-object populations. The researchers combined thousands of ordinary events with a small, carefully modeled set of very brief events.

3 Findings

The study identifies six likely planetary events lasting under 0.5 days. The shortest lasted 0.057 days and had an angular Einstein radius of 0.90 microarcseconds. The authors find a power-law mass function (a rule describing how object numbers change with mass) with slope 0.96, though uncertainty is large. It implies 21^{+23}_{-13} free-floating or very wide-orbit planets per star from 0.33 to 6,660 Earth masses, totaling 80^{+73}_{-47} Earth masses per star. These objects may outnumber wide-orbit bound planets by 19^{+23}_{-13} times, while holding similar total mass. The authors argue that ejection from planetary systems could explain this pattern. A broken power law gives consistent but less precise results. The study predicts Roman could detect about 988 such objects down to Mars mass. It recommends better measurements of low-magnification events around ordinary stars. The results point to a large population of small wandering planets, but future surveys must test how many truly exist.

Abstract

Abstract We present the first measurement of the mass function of free-floating planets (FFPs), or very wide orbit planets down to an Earth mass, from the MOA-II microlensing survey in 2006–2014. Six events are likely to be due to planets with Einstein radius crossing times t E < 0.5 days, and the shortest has t E = 0.057 ± 0.016 days and an angular Einstein radius of θ E = 0.90 ± 0.14 μ as. We measure the detection efficiency depending on both t E and θ E with image-level simulations for the first time. These short events are well modeled by a power-law mass function, dN 4 / d log M = ( 2.18 − 1.40 + 0.52 ) × ( M / 8 M ⊕ ) − α 4 dex −1 star −1 with α 4 = 0.96 − 0.27 + 0.47 for M / M ⊙ < 0.02. This implies a total of f = 21 − 13 + 23 FFPs or very wide orbit planets of mass 0.33 < M / M ⊕ < 6660 per star, with a total mass of 80 − 47 + 73 M ⊕ star −1 . The number of FFPs is 19 − 13 + 23

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