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Table 1.

Properties of connecting clusters for the candidate filaments.

Filament Name Cluster Name z M500 R500 Rvir kT
(–) (1014M) (Mpc) (Mpc) (keV)
J0935+1949 1eRASS J093552.6+201132 0.1757 ± 0.0004 1 . 54 0.38 + 0.32 $ 1.54_{-0.38}^{+0.32} $ 0 . 77 0.07 + 0.05 $ 0.77_{-0.07}^{+0.05} $ 1 . 66 0.15 + 0.11 $ 1.66_{-0.15}^{+0.11} $ 1 . 66 0.53 + 2.24 $ 1.66_{-0.53}^{+2.24} $
1eRASS J093446.5+192751 0.1807 ± 0.0004 1 . 17 0.44 + 0.42 $ 1.17_{-0.44}^{+0.42} $ 0 . 7 0.1 + 0.08 $ 0.7_{-0.1}^{+0.08} $ 1 . 51 0.22 + 0.16 $ 1.51_{-0.22}^{+0.16} $ > 1.08

J0945+3418 1eRASS J094554.6+344046 0.1344 ± 0.0004 1 . 41 0.31 + 0.32 $ 1.41_{-0.31}^{+0.32} $ 0 . 76 0.06 + 0.05 $ 0.76_{-0.06}^{+0.05} $ 1 . 63 0.13 + 0.12 $ 1.63_{-0.13}^{+0.12} $ > 1.52
1eRASS J094426.2+335718 0.1306 ± 0.0004 1 . 91 0.34 + 0.4 $ 1.91_{-0.34}^{+0.4} $ 0 . 84 0.05 + 0.05 $ 0.84_{-0.05}^{+0.05} $ 1 . 81 0.12 + 0.12 $ 1.81_{-0.12}^{+0.12} $ 1 . 51 0.34 + 1.49 $ 1.51_{-0.34}^{+1.49} $

J1214+2712 1eRASS J121411.6+263822 0.1733 ± 0.0038 1 . 36 0.29 + 0.26 $ 1.36_{-0.29}^{+0.26} $ 0 . 74 0.06 + 0.04 $ 0.74_{-0.06}^{+0.04} $ 1 . 59 0.12 + 0.10 $ 1.59_{-0.12}^{+0.10} $ > 1.28
1eRASS J121259.1+272708 0.1797 ± 0.0003 3 . 36 0.29 + 0.44 $ 3.36_{-0.29}^{+0.44} $ 1 . 00 0.03 + 0.04 $ 1.00_{-0.03}^{+0.04} $ 2 . 15 0.06 + 0.09 $ 2.15_{-0.06}^{+0.09} $ 1 . 23 0.16 + 0.45 $ 1.23_{-0.16}^{+0.45} $

J2300−4534 1eRASS J230541.6−451201 0.1275 ± 0.0008 4 . 15 0.43 + 0.32 $ 4.15_{-0.43}^{+0.32} $ 1 . 09 0.04 + 0.03 $ 1.09_{-0.04}^{+0.03} $ 2 . 35 0.09 + 0.06 $ 2.35_{-0.09}^{+0.06} $ N/A (*)
1eRASS J230557.7−442221 0.1318 ± 0.0011 2 . 00 0.27 + 0.34 $ 2.00_{-0.27}^{+0.34} $ 0 . 85 0.04 + 0.05 $ 0.85_{-0.04}^{+0.05} $ 1 . 84 0.08 + 0.1 $ 1.84_{-0.08}^{+0.1} $ 0 . 38 0.05 + 0.21 $ 0.38_{-0.05}^{+0.21} $

Notes. Redshift z, mass M500, radius R500 and cluster temperature kT and corresponding 1σ errors were obtained from Bulbul et al. (2024), while Rvir is derived based on Rvir ≈ 101/3R500 given in Reiprich et al. (2013).

(*)

Temperature of 1eRASS J230541.6−451201 provided in Bulbul et al. (2024) was unrealistic.

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