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Table 4:

The extragalactic sources with reliable RM estimates
l b $RM\pm\Delta RM$ $I_{\rm H\alpha}$ l b $RM\pm\Delta RM$ $I_{\rm H\alpha}$ l b $RM\pm\Delta RM$ $I_{\rm H\alpha}$
deg deg rad/m2 R deg deg rad/m2 R deg deg rad/m2 R
253.30 0.89 -8 $\pm$ 12 440 274.70 -2.80 420 $\pm$ 4 27 314.50 0.30 -738 $\pm$ 19 52
253.52 0.83 -50 $\pm$ 26 582 274.77 0.25 -76 $\pm$ 22 25 314.82 0.89 -507 $\pm$ 25 38
254.81 0.93 84 $\pm$ 13 501 275.02 0.82 -101 $\pm$ 25 28 317.54 -0.57 395 $\pm$ 27 24
254.95 0.63 8 $\pm$ 32 495 275.48 -0.68 248 $\pm$ 13 28 319.34 1.08 241 $\pm$ 21 37
255.16 0.24 -35 $\pm$ 16 436 275.56 1.02 16 $\pm$ 7 23 320.83 0.88 -8 $\pm$ 20 22
255.27 0.16 26 $\pm$ 23 407 275.56 -0.20 112 $\pm$ 30 31 321.48 1.02 -243 $\pm$ 8 9
255.36 -0.26 97 $\pm$ 10 456 275.83 0.16 -107 $\pm$ 7 27 321.58 -0.76 -138 $\pm$ 9 20
255.36 0.50 -115 $\pm$ 13 556 275.86 0.94 0 $\pm$ 21 23 323.15 -0.52 83 $\pm$ 25 9
256.14 0.25 44 $\pm$ 17 484 276.46 0.89 -17 $\pm$ 20 23 324.77 0.61 -66 $\pm$ 14 9
256.64 -0.22 172 $\pm$ 15 454 277.78 -0.73 -36 $\pm$ 23 21 325.81 1.08 -15 $\pm$ 31 8
257.47 0.54 23 $\pm$ 20 307 277.78 -0.81 -77 $\pm$ 3 23 325.83 -0.30 356 $\pm$ 18 11
257.71 -0.66 144 $\pm$ 20 411 279.04 -0.88 239 $\pm$ 17 32 325.93 2.92 -159 $\pm$ 28 14
257.92 0.65 76 $\pm$ 14 292 279.15 -0.63 341 $\pm$ 24 31 326.30 2.17 -357 $\pm$ 10 11
258.52 1.02 196 $\pm$ 26 342 279.15 -0.65 329 $\pm$ 20 30 326.54 2.18 -505 $\pm$ 14 12
258.77 0.08 221 $\pm$ 16 307 279.33 0.80 -157 $\pm$ 18 28 326.69 -1.16 -142 $\pm$ 22 20
259.05 -0.72 175 $\pm$ 12 295 280.62 -0.14 -112 $\pm$ 15 25 326.80 1.57 -768 $\pm$ 8 13
259.05 -0.75 150 $\pm$ 12 275 282.46 0.24 256 $\pm$ 23 30 326.94 2.40 -808 $\pm$ 29 12
260.69 -0.23 204 $\pm$ 12 829 284.30 0.81 -547 $\pm$ 25 47 327.31 0.88 -189 $\pm$ 26 14
263.50 0.17 260 $\pm$ 28 630 285.15 0.96 168 $\pm$ 31 55 327.52 2.70 -595 $\pm$ 16 15
264.24 0.88 406 $\pm$ 9 554 295.17 0.01 363 $\pm$ 22 66 327.87 1.60 -818 $\pm$ 21 12
265.69 0.85 70 $\pm$ 28 449 297.67 0.77 570 $\pm$ 11 62 328.62 1.52 -933 $\pm$ 30 12
266.14 1.08 211 $\pm$ 29 334 299.51 -1.10 315 $\pm$ 21 41 328.80 2.80 -350 $\pm$ 25 11
266.27 0.66 396 $\pm$ 18 427 300.47 -0.99 412 $\pm$ 18 59 329.20 2.83 -348 $\pm$ 11 12
267.17 0.47 323 $\pm$ 28 487 301.14 -0.09 350 $\pm$ 18 68 330.12 -1.08 -931 $\pm$ 25 31
268.62 0.58 256 $\pm$ 15 632 301.70 0.25 296 $\pm$33 75 330.35 1.81 25 $\pm$ 35 11
269.05 0.17 456 $\pm$ 16 1015 302.60 -1.17 159 $\pm$ 25 50 330.56 1.74 4 $\pm$ 11 12
269.55 0.45 137 $\pm$ 18 725 303.30 0.51 -370 $\pm$ 14 45 335.32 0.60 -138 $\pm$ 11 38
270.56 -0.85 -152 $\pm$ 23 666 304.53 1.00 40 $\pm$ 28 47 337.06 0.85 -739 $\pm$ 32 59
270.91 0.93 -149 $\pm$ 22 521 305.62 -1.16 -61 $\pm$ 28 114 339.65 -0.24 -398 $\pm$ 19 40
271.22 -0.35 215 $\pm$ 29 512 306.87 0.02 -197 $\pm$ 27 54 342.16 -0.74 127 $\pm$ 15 75
271.30 -0.06 136 $\pm$ 16 380 306.92 -0.70 52 $\pm$ 16 105 347.40 -1.04 -524 $\pm$ 36 49
271.52 -1.01 75 $\pm$ 28 602 308.64 -0.62 -133 $\pm$ 27 54 350.52 -0.73 277 $\pm$ 32 49
271.70 -0.38 -93 $\pm$ 18 600 310.20 -1.04 -584 $\pm$ 19 52 351.31 -0.53 -247 $\pm$ 15 54
272.36 0.62 -296 $\pm$ 28 506 313.96 -0.76 -480 $\pm$ 22 68 352.13 1.15 76 $\pm$ 30 43
273.46 0.68 -106 $\pm$ 19 436 313.99 0.94 -828 $\pm$ 17 64 356.57 0.87 985 $\pm$ 30 34
273.57 1.28 20 $\pm$ 25 307 314.02 1.01 -579 $\pm$ 20 54        


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