{
  "id": "astro-ph/9611134",
  "version": "v1",
  "published": "1996-11-18T12:42:49.000Z",
  "updated": "1996-11-18T12:42:49.000Z",
  "title": "Discovering Galactic Planets by Gravitational Microlensing: Magnification Patterns and Light Curves",
  "authors": [
    "Joachim Wambsganss"
  ],
  "comment": "8 pages Latex plus 10 Figures (partly in GIF/JPEG format due to size constraints). High quality Postscript figures can be obtained electronically at the URL: http://www.aip.de:8080/~jkw/planet_figures.html . Hardcopies of figures can be obtained on request. To appear in MNRAS (Jan.1, 1997, Volume 284, pp.172-188)",
  "categories": [
    "astro-ph"
  ],
  "abstract": "The current searches for microlensing events towards the galactic bulge can be used to detect planets around the lensing stars. Their effect is a short-term modulation on the smooth lightcurve produced by the main lensing star. Current and planned experiments should be sensitive enough to discover planets ranging from Jupiter mass down to Earth mass. For a successful detection of planets, it is necessary to accurately and frequently monitor a microlensing event photometrically, once it has been \"triggered\". We present a large variety of two-dimensional magnification distributions for systems consisting of an ordinary star and a planetary companion. We cover planet/star mass ratios from $m_{pl}/M_* = 10^{-5}$ to $ 10^{-3}$. These limits correspond roughly to $M_{Earth}$ and $M_{Jup}$, for a typical lens mass of $M_* = 0.3 M_{\\odot}$. We explore a range of star-planet distances, with particular emphasis on the case of \"resonant lensing\", a situation in which the planet is located at or very near the Einstein ring of the lensing star. We show a wide selection of light curves - one dimensional cuts through the magnification patterns - to illustrate the broad range of possible light curve perturbations caused by planets. The strongest effects are to be expected for caustic crossings. But even tracks passing outside the caustics can have considerable effects on the light curves. The easiest detectable (projected) distance range for the planets is between about 0.6 and 1.6 Einstein radii. Planets in this distance range produce caustics inside the Einstein ring of the star. For a lensing star with a mass of about $0.3 M_{\\odot}$ at a distance of 6 kpc and a source at 8 kpc, this corresponds to physical distances between star and planet of about 1 to 3 AU.",
  "revisions": [
    {
      "version": "v1",
      "updated": "1996-11-18T12:42:49.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "light curve",
      "discovering galactic planets",
      "magnification patterns",
      "lensing star",
      "gravitational microlensing"
    ],
    "tags": [
      "journal article"
    ],
    "publication": {
      "doi": "10.1093/mnras/284.1.172"
    },
    "note": {
      "typesetting": "LaTeX",
      "pages": 8,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 436936
    }
  }
}