INTEGRAL Picture Of the Month
August 2015

INTEGRAL POM
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A 'Black-Hole Scope' used by INTEGRAL and Fermi

Some of the distant quasars are occasionally situated behind a foreground galaxy. In this case the gravitational field of the galaxy bends the light from the quasar so that the entire galalaxy works as cosmic scale lense, producing multiple images of the quasar. This is the case for the quasar PKS 1830-211 in which the effect of gravitational lensing splits the image of the quasar into two images separated by the angular distance of one arcsecond. The angular resolutions of gamma-ray telescopes, like ESA's INTEGRAL and NASA's Fermi telescopes is only about a fraction of a degree, which is not sufficient to resolve the two images of the source. Still, the gamma-ray telescopes manage to separate the flux from the two images, based on the variability properties of the source. Differences in the path of photons coming from the two images lead to a delay of the signal coming from one of the images by approximately twenty days. Observing this time delay effect, astronomers have noticed a peculiarity of the source variability pattern. The advanced and delayed signals did not exactly repeat each other.

A consistent explanation of this peculiar behaviour is provided by the effect of gravitational "microlensing". This effect is produced by stars in the lensing galaxy. Each star passing through the line of sight toward the quasar works as a gravitational lens. This also leads to the appearance of the multiple images of the source, but the images are separated by only about a micro-arcsecond. This angular scale could not be resolved even by the best telescopes working in the visible domain, to say nothing about the gamma-ray telescopes. However, the gamma-ray telescopes are able to see the effect of these images on the variability of the light from the source.

The variability arises because of the motion of the stars across the line of sight. This motion effect is explained in the set of figures A-D. Left top panel A shows a simulated pattern of magnification of the source flux by many stars for different source positions. Red color indicates the positions where the effect of the microlensing is strong, blue is where the effect is moderate or absent. The "spider web" like structure is a network of the microlensing "caustics". The flux of a source situated exactly behind the caustic line is strongly magnified.

Relative motion of the stars (the caustics) and the source (the white cross in the left top panel A) causes appearance / disappearance of multiple images, as shown in the right top panel B. Appearance of the new images and their stretching leads to strong magnification of the flux at the moments when the source passes just behind the caustic. This "caustic crossing" events are visible on the red dotted lightcurve in the left bottom panel C. It is the microlensing effect which influences the exceptionally bright flare of PKS 1830-211 observed by the Fermi/LAT telescope (the data shown in the right bottom panel D). Using the microlensing effect, the authors of the Paper "Central engine of a gamma-ray blazar resolved through the magnifying glass of gravitational microlensing" have managed to constrain the size of the source of gamma-rays detected by Fermi/LAT from PKS 1830-211 and locate it very close to the black hole, at the base of the AGN jet.

The effect of the microlensing is strong only if the source is very small, much smaller than the typical caustic-to-caustic distance in the left top panel A. The lightcurve of a large source (blue lighturve in the panels C and D) does not reveal the caustic crossing episodes. Non-observation of the caustic crossings in the INTEGRAL lightcurve (shown in the right bottom panel D) shows that the hard X-ray / soft gamma-ray source is large.

This large size resolves the puzzle of how high-energy gamma-rays can actually escape from the compact source and be detected by Fermi/LAT, as otherwise the high-energy gamma-rays would produce electron positron pairs in interaction with the hard X-ray photons.

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