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Table 2.
Parameters used to compute the acceleration efficiency.
| Cluster name | Position | 𝒞 | nd | kTd | A | Sν | ν |
|---|---|---|---|---|---|---|---|
| (cm−3) | (keV) | (π kpc2) | (mJy) | (MHz) | |||
| A2744 ( † ) | NE |
 |
1.8 × 10−4 | 12.3 | 7402 | 20 | 1400 |
| A115 | N |
 |
1.5 × 10−3 | 7.9 | 1802 | 34 | 1400 |
| El Gordo | NW |
 |
8.5 × 10−4 | 17.9 | 3502 | 28 | 610 |
| A521 | SE |
 |
3.0 × 10−4 | 7.0 | 4902 | 42 | 610 |
| A3376 | E |
 |
9.0 × 10−4 | 4.7 | 2602 | 40 | 1400 |
| Toothbrush cluster | N |
 |
5.5 × 10−4 | 8.2 | 3002 | 480 | 610 |
| Bullet cluster | E |
 |
5.0 × 10−4 | 13.5 | 2502 | 5 | 2100 |
| RXC J1314.4-2515 | W |
 |
1.0 × 10−3 | 13.5 | 3302 | 85 | 325 |
| A2146 | NW |
 |
3.5 × 10−3 | 14.5 | 1602 | 0.8 | 1500 |
| Sausage cluster | N | n.a. | 3.0 × 10−4 | 8.5 | 9002 | 337 | 610 |
Notes. Values of the downstream temperature kTd and radio flux density S are derived from the works listed in Table 1. ( † )Compression factor and downstream density taken from Eckert et al. (2016).
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