Strong gravitational lensing

Part of a series of articles about

Gravitational lensing
Einstein ring
Formalism
Strong lensing
Microlensing
Weak lensing

Strong lens systems

Abell 1689 * Abell 2218]]
CL0024+17 * Bullet Cluster
QSO2237+0305 * SDSSJ0946+1006
B1359+154 * QSO 0957+561

Surveys

Strong: CLASS * SLACS (SDSS)
Micro: OGLE * Gaia
Weak: DLS * Pan-STARRS * CFHTLS * DES * LSST * SNAP * DESTINY

* v
* t
* e

Strong gravitational lensing is a gravitational lensing effect that is strong enough to produce multiple images, arcs, or Einstein rings. Generally, for strong lensing to occur, the projected lens mass density must be greater than the critical density, that is Σcr. For point-like background sources, there will be multiple images; for extended background emissions, there can be arcs or rings. Topologically, multiple image production is governed by the odd number theorem.[1]

Strong lensing was predicted by Albert Einstein's general theory of relativity and observationally discovered by Dennis Walsh, Bob Carswell, and Ray Weymann in 1979.[2] They determined that the Twin Quasar Q0957+561A comprises two images of the same object.

## Contents

* 1 Observations
* 1.1 Galaxy lensing
* 1.2 Cluster lensing
* 2 Astrophysical applications
* 2.1 Mass profiles
* 2.2 Time delays
* 3 Gallery
* 4 References

## Observations

Most strong gravitational lenses are detected by large-scale galaxy surveys.

### Galaxy lensing

A light source passes behind a gravitational lens (point mass placed in the center of the image). The aqua circle is a source as it would be seen if there was no lens, white spots are the multiple images of the source.

The foreground lens is a galaxy. When the background source is a quasar or unresolved jet, the strong lensed images are usually point-like multiple images; When the background source is a galaxy or extended jet emission, the strong lensed images can be arcs or rings. As of 2017, several hundred galaxy-galaxy (g-g) strong lenses have been observed.[3] The upcoming Vera C. Rubin Observatory and Euclid surveys are expected to discover more than 100,000 such objects.[4]

### Cluster lensing

The foreground lens is a galaxy cluster. In this case, the lens is usually powerful enough to produce noticeable both strong lensing (multiple images, arcs or rings) and weak lensing effects (ellipticity distortions). The lensing nicknamed the "Molten Ring" is an example.[5]

## Astrophysical applications

### Mass profiles

Because the strong lensing of a background source depends only on the gravitational potential of the foreground mass, this phenomenon can be used to constrain the mass model of lenses. With the constraints from multiple images or arcs, a proposed mass model can be optimized to fit to the observables. The subgalactic structures that currently interest lensing astronomers are the central mass distribution and dark matter halos.[6]

### Time delays

Since the light rays go through different paths to produce multiple images, they will get delayed by local potentials along the light paths. The time delay differences from different images can be determined by the mass model and the cosmological model. Thus, with observed time delays and constrained mass model, cosmological constants such as the Hubble constant can be inferred.[7]

## Gallery

* Gravitational lensing system SDSS J0928+2031.[8]

* SDSS J1138+2754 taken by Hubble's WFC3 camera.[9]

* Dubbed the "Molten Ring", Hubble sees strong lensing around GAL-CLUS-022058s.[10]

## References

1. ↑ Mediavilla, Evencio (2016). Astrophysical Applications of Gravitational Lensing. Cambridge University Press. ISBN 978-1-107-07854-3.
2. ↑ Bernstein, G. M.; Tyson, J. A.; Kochanek, C. S. (1993). "A large arc in the gravitational lens system 0957 + 561". The Astronomical Journal 105: 816. doi:10.1086/116474. ISSN 0004-6256. Bibcode: 1993AJ....105..816B.
3. ↑ Wang, Lin; Shu, Yiping; Li, Ran; Zheng, Zheng; Wen, Zhonglue; Liu, Guilin (2017-03-28). "SDSS J1640+1932: a spectacular galaxy–quasar strong lens system". Monthly Notices of the Royal Astronomical Society (Oxford University Press (OUP)) 468 (3): 3757–3763. doi:10.1093/mnras/stx733. ISSN 0035-8711. Bibcode: 2017MNRAS.468.3757W.
4. ↑ Collett, Thomas E. (2015). "The population of galaxy-galaxy strong lenses in forthcoming optical imaging surveys". The Astrophysical Journal 811 (1): 20. doi:10.1088/0004-637X/811/1/20. ISSN 1538-4357. Bibcode: 2015ApJ...811...20C.
5. ↑ Tuesday, Hailey Rose McLaughlin (22 December 2020). "Hubble captures a clear shot of a 'Molten Ring'" (in en). https://astronomy.com/news/2020/12/hubble-captures-a-clear-shot-of-a-molten-ring.
6. ↑ Kochanek, C. S. (2006). "Strong Gravitational Lensing". Gravitational Lensing: Strong, Weak and Micro. Saas-Fee Advanced Courses. 33. pp. 91–268. doi:10.1007/978-3-540-30310-7_2. ISBN 978-3-540-30309-1.
7. ↑ Courbin, Frédéric; Minniti, Dante (2002). Gravitational Lensing: An Astrophysical Tool. Lecture Notes in Physics. 608. doi:10.1007/3-540-45857-3. ISBN 978-3-540-44355-1.
8. ↑ "Peering into the past" (in en). https://www.spacetelescope.org/images/potw1903a/.
9. ↑ "Awesome gravity". https://www.spacetelescope.org/images/potw1837a/.
10. ↑ Jenner, Lynn (22 September 2021). "Hubble Snapshot of "Molten Ring" Galaxy Prompts New Research". https://www.nasa.gov/feature/goddard/2021/hubble-snapshot-of-molten-ring-galaxy-prompts-new-research.

0.00

(0 votes)

Original source: https://en.wikipedia.org/wiki/Strong gravitational lensing. Read more

|

Retrieved from "https://handwiki.org/wiki/index.php?title=Physics:Strong_gravitational_lensing&oldid=4106919"
*[v]: View this template
*[t]: Discuss this template
*[e]: Edit this template