×ばつ {10}<SUP>15</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> dominates the weak-lensing signal. This cluster is likely to be undergoing a merger with one (or more) subcluster whose mass is approximately a factor of 10 lower. One candidate is the subcluster of mass {M}<SUB>200{{c</SUB>}}={1.16}<SUB>-0.13</SUB><SUP>+0.15</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> located ∼ 400 {kpc} to the SE. The location of this subcluster suggests that its interaction with the primary cluster could be the source of the NW radio relic. Another subcluster is detected ∼ 2 Mpc to the SE of the X-ray peak with mass {M}<SUB>200{{c</SUB>}}={1.68}<SUB>-0.20</SUB><SUP>+0.22</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>. This SE subcluster is in the vicinity of the SE radio relic and may have created the SE radio relic during a past merger with the primary cluster. The fourth subcluster, {M}<SUB>200{{c</SUB>}}={1.87}<SUB>-0.22</SUB><SUP>+0.24</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>, is NW of the X-ray peak and beyond the NW radio relic."> ×ばつ {10}<SUP>15</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> dominates the weak-lensing signal. This cluster is likely to be undergoing a merger with one (or more) subcluster whose mass is approximately a factor of 10 lower. One candidate is the subcluster of mass {M}<SUB>200{{c</SUB>}}={1.16}<SUB>-0.13</SUB><SUP>+0.15</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> located ∼ 400 {kpc} to the SE. The location of this subcluster suggests that its interaction with the primary cluster could be the source of the NW radio relic. Another subcluster is detected ∼ 2 Mpc to the SE of the X-ray peak with mass {M}<SUB>200{{c</SUB>}}={1.68}<SUB>-0.20</SUB><SUP>+0.22</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>. This SE subcluster is in the vicinity of the SE radio relic and may have created the SE radio relic during a past merger with the primary cluster. The fourth subcluster, {M}<SUB>200{{c</SUB>}}={1.87}<SUB>-0.22</SUB><SUP>+0.24</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>, is NW of the X-ray peak and beyond the NW radio relic."> ×ばつ {10}<SUP>15</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> dominates the weak-lensing signal. This cluster is likely to be undergoing a merger with one (or more) subcluster whose mass is approximately a factor of 10 lower. One candidate is the subcluster of mass {M}<SUB>200{{c</SUB>}}={1.16}<SUB>-0.13</SUB><SUP>+0.15</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB> located ∼ 400 {kpc} to the SE. The location of this subcluster suggests that its interaction with the primary cluster could be the source of the NW radio relic. Another subcluster is detected ∼ 2 Mpc to the SE of the X-ray peak with mass {M}<SUB>200{{c</SUB>}}={1.68}<SUB>-0.20</SUB><SUP>+0.22</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>. This SE subcluster is in the vicinity of the SE radio relic and may have created the SE radio relic during a past merger with the primary cluster. The fourth subcluster, {M}<SUB>200{{c</SUB>}}={1.87}<SUB>-0.22</SUB><SUP>+0.24</SUP&g×ばつ {10}<SUP>14</SUP> {h}<SUB>70</SUB><SUP>-1</SUP> {M}<SUB>☉ </SUB>, is NW of the X-ray peak and beyond the NW radio relic."/>
[フレーム]
Now on home page

ADS

MC2: Subaru and Hubble Space Telescope Weak-lensing Analysis of the Double Radio Relic Galaxy Cluster PLCK G287.0+32.9

Abstract

The second most significant detection of the Planck Sunyaev-Zel’dovich survey, PLCK G287.0+32.9 (z = 0.385), boasts two similarly bright radio relics and a radio halo. One radio relic is located ∼ 400 {kpc} NW of the X-ray peak and the other ∼ 2.8 Mpc to the SE. This large difference suggests that a complex merging scenario is required. A key missing puzzle for the merging scenario reconstruction is the underlying dark matter distribution in high resolution. We present a joint Subaru Telescope and Hubble Space Telescope weak-lensing analysis of the cluster. Our analysis shows that the mass distribution features four significant substructures. Of the substructures, a primary cluster of mass {M}200{{c}}={1.59}-0.22+0.25×ばつ {10}15 {h}70-1 {M} dominates the weak-lensing signal. This cluster is likely to be undergoing a merger with one (or more) subcluster whose mass is approximately a factor of 10 lower. One candidate is the subcluster of mass {M}200{{c}}={1.16}-0.13+0.15×ばつ {10}14 {h}70-1 {M} located ∼ 400 {kpc} to the SE. The location of this subcluster suggests that its interaction with the primary cluster could be the source of the NW radio relic. Another subcluster is detected ∼ 2 Mpc to the SE of the X-ray peak with mass {M}200{{c}}={1.68}-0.20+0.22×ばつ {10}14 {h}70-1 {M}. This SE subcluster is in the vicinity of the SE radio relic and may have created the SE radio relic during a past merger with the primary cluster. The fourth subcluster, {M}200{{c}}={1.87}-0.22+0.24×ばつ {10}14 {h}70-1 {M}, is NW of the X-ray peak and beyond the NW radio relic.


Publication:
The Astrophysical Journal
Pub Date:
December 2017
DOI:

10.3847/1538-4357/aa998c

10.48550/arXiv.1710.02527

arXiv:
arXiv:1710.02527
Bibcode:
2017ApJ...851...46F
Keywords:
  • cosmology: observations;
  • dark matter;
  • galaxies: clusters: individual: PLCK G287.0+32.9;
  • gravitational lensing: weak;
  • X-rays: galaxies: clusters;
  • Astrophysics - Cosmology and Nongalactic Astrophysics
E-Print:
19 pages, 14 figures
full text sources
IOP
Preprint
Related Materials (1)
🌓

AltStyle によって変換されたページ (->オリジナル) /