Table 3.

Summary of radio analysis of all the diffuse radio sources in the Bullet cluster. The columns are as follows. (1) Name of the diffuse radio source, (2) Integrated flux density, (3) Integrated in-band spectral index, (4) Radio power at 1.4 GHz, (5) Largest Angular Size, and (6) Largest Linear Size.

SourceIntegrated flux density|$\alpha ^{1.1\,\rm GHz}_{1.5\,\rm GHz}$|P1.4 GHzLASLLS
(mJy)(1024 WHz−1)(arcmin)(kpc)
Halo100.7 ± 5.01.1 ± 0.234.4 ± 1.16.2 × 4.71632 × 1250
Relic region A98.6 ± 4.91.1 ± 0.140.0 ± 1.31.6432
Relic region B8.2 ± 0.41.2 ± 0.23.3 ± 0.52.1556
Relic107.0 ± 5.41.1 ± 0.243.5 ± 1.43.7988
Candidate relic1.8 ± 0.11.6 ± 0.90.6 ± 0.013.4895
SourceIntegrated flux density|$\alpha ^{1.1\,\rm GHz}_{1.5\,\rm GHz}$|P1.4 GHzLASLLS
(mJy)(1024 WHz−1)(arcmin)(kpc)
Halo100.7 ± 5.01.1 ± 0.234.4 ± 1.16.2 × 4.71632 × 1250
Relic region A98.6 ± 4.91.1 ± 0.140.0 ± 1.31.6432
Relic region B8.2 ± 0.41.2 ± 0.23.3 ± 0.52.1556
Relic107.0 ± 5.41.1 ± 0.243.5 ± 1.43.7988
Candidate relic1.8 ± 0.11.6 ± 0.90.6 ± 0.013.4895
Table 3.

Summary of radio analysis of all the diffuse radio sources in the Bullet cluster. The columns are as follows. (1) Name of the diffuse radio source, (2) Integrated flux density, (3) Integrated in-band spectral index, (4) Radio power at 1.4 GHz, (5) Largest Angular Size, and (6) Largest Linear Size.

SourceIntegrated flux density|$\alpha ^{1.1\,\rm GHz}_{1.5\,\rm GHz}$|P1.4 GHzLASLLS
(mJy)(1024 WHz−1)(arcmin)(kpc)
Halo100.7 ± 5.01.1 ± 0.234.4 ± 1.16.2 × 4.71632 × 1250
Relic region A98.6 ± 4.91.1 ± 0.140.0 ± 1.31.6432
Relic region B8.2 ± 0.41.2 ± 0.23.3 ± 0.52.1556
Relic107.0 ± 5.41.1 ± 0.243.5 ± 1.43.7988
Candidate relic1.8 ± 0.11.6 ± 0.90.6 ± 0.013.4895
SourceIntegrated flux density|$\alpha ^{1.1\,\rm GHz}_{1.5\,\rm GHz}$|P1.4 GHzLASLLS
(mJy)(1024 WHz−1)(arcmin)(kpc)
Halo100.7 ± 5.01.1 ± 0.234.4 ± 1.16.2 × 4.71632 × 1250
Relic region A98.6 ± 4.91.1 ± 0.140.0 ± 1.31.6432
Relic region B8.2 ± 0.41.2 ± 0.23.3 ± 0.52.1556
Relic107.0 ± 5.41.1 ± 0.243.5 ± 1.43.7988
Candidate relic1.8 ± 0.11.6 ± 0.90.6 ± 0.013.4895
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