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Table B.1.

Results of fitting the BLR model to the line profiles.

ID Model Tied? HαRBLR [ld] β ϵ i [°] θ0 [°] κ γ ξ fflow fellip θe [°] Δϕpeak
× 10−3
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14) (15)
1 F - 2442 1582 + 1123 $ 2442_{-1582}^{+1123} $ 1.36 0.21 + 0.18 $ {1.36}_{-0.21}^{+0.18} $ + 4.20 8.27 + 0.69 $ {+4.20}_{-8.27}^{+0.69} $ 55 27 + 23 $ {55}_{-27}^{+23} $ 25 6 + 23 $ {25}_{-6}^{+23} $ 0.39 0.02 + 0.74 $ {-0.39}_{-0.02}^{+0.74} $ 3.92 1.81 + 0.48 $ {3.92}_{-1.81}^{+0.48} $ 0.45 0.31 + 0.33 $ {0.45}_{-0.31}^{+0.33} $ 0.43 0.27 + 0.26 $ {0.43}_{-0.27}^{+0.26} $ 0.17 0.08 + 0.27 $ {0.17}_{-0.08}^{+0.27} $ 19 7 + 35 $ {19}_{-7}^{+35} $ 9.3 7.9 + 7.3 $ {9.3}_{-7.9}^{+7.3} $
2 C - 1128 554 + 457 $ 1128_{-554}^{+457} $ 1.86 0.31 + 0.07 $ {1.86}_{-0.31}^{+0.07} $ 0.34 0.56 + 0.45 $ {-0.34}_{-0.56}^{+0.45} $ 43 19 + 16 $ {43}_{-19}^{+16} $ 61 24 + 17 $ {61}_{-24}^{+17} $ 4.6 2.5 + 4.2 $ {4.6}_{-2.5}^{+4.2} $
3 C - 348 229 + 248 $ 348_{-229}^{+248} $ 1.56 0.92 + 0.20 $ {1.56}_{-0.92}^{+0.20} $ 0.22 1.34 + 0.74 $ {0.22}_{-1.34}^{+0.74} $ 53 27 + 24 $ {53}_{-27}^{+24} $ 67 43 + 12 $ {67}_{-43}^{+12} $ 0.3 0.3 + 1.2 $ {0.3}_{-0.3}^{+1.2} $
4 C - 597 373 + 400 $ 597_{-373}^{+400} $ 1.83 0.48 + 0.03 $ {1.83}_{-0.48}^{+0.03} $ 0.12 0.55 + 0.46 $ {-0.12}_{-0.55}^{+0.46} $ 25 10 + 20 $ {25}_{-10}^{+20} $ 50 23 + 18 $ {50}_{-23}^{+18} $ 0.9 0.6 + 1.9 $ {0.9}_{-0.6}^{+1.9} $
5 F - 1899 1175 + 974 $ 1899_{-1175}^{+974} $ 1.76 0.21 + 0.13 $ {1.76}_{-0.21}^{+0.13} $ + 0.91 1.84 + 1.09 $ {+0.91}_{-1.84}^{+1.09} $ 37 20 + 27 $ {37}_{-20}^{+27} $ 49 23 + 28 $ {49}_{-23}^{+28} $ 0.01 0.34 + 0.36 $ {-0.01}_{-0.34}^{+0.36} $ 2.69 1.12 + 1.48 $ {2.69}_{-1.12}^{+1.48} $ 0.48 0.31 + 0.37 $ {0.48}_{-0.31}^{+0.37} $ 0.35 0.24 + 0.38 $ {0.35}_{-0.24}^{+0.38} $ 0.41 0.27 + 0.34 $ {0.41}_{-0.27}^{+0.34} $ 36 25 + 35 $ {36}_{-25}^{+35} $ 3.6 2.7 + 3.4 $ {3.6}_{-2.7}^{+3.4} $
6 C Y 1552 335 + 1316 $ 1552_{-335}^{+1316} $ 1.76 0.21 + 0.13 $ {1.76}_{-0.21}^{+0.13} $ 0.11 0.23 + 0.21 $ {-0.11}_{-0.23}^{+0.21} $ 33 9 + 20 $ {33}_{-9}^{+20} $ 50 11 + 24 $ {50}_{-11}^{+24} $ 9.6 4.2 + 9.4 $ {9.6}_{-4.2}^{+9.4} $
7 C - 905 378 + 1058 $ 905_{-378}^{+1058} $ 1.48 0.32 + 0.35 $ {1.48}_{-0.32}^{+0.35} $ 0.05 0.88 + 1.07 $ {-0.05}_{-0.88}^{+1.07} $ 37 14 + 33 $ {37}_{-14}^{+33} $ 53 25 + 25 $ {53}_{-25}^{+25} $ 6.2 4.3 + 9.5 $ {6.2}_{-4.3}^{+9.5} $
8 C - 1492 632 + 1074 $ 1492_{-632}^{+1074} $ 1.56 0.28 + 0.28 $ {1.56}_{-0.28}^{+0.28} $ 0.32 0.55 + 0.54 $ {-0.32}_{-0.55}^{+0.54} $ 38 16 + 23 $ {38}_{-16}^{+23} $ 56 21 + 23 $ {56}_{-21}^{+23} $ 7.7 4.9 + 8.6 $ {7.7}_{-4.9}^{+8.6} $
9 C Y 2931 1089 + 2272 $ 2931_{-1089}^{+2272} $ 1.80 0.28 + 0.11 $ {1.80}_{-0.28}^{+0.11} $ 0.23 0.36 + 0.55 $ {-0.23}_{-0.36}^{+0.55} $ 34 12 + 22 $ {34}_{-12}^{+22} $ 52 17 + 24 $ {52}_{-17}^{+24} $ 25.3 16.4 + 19.0 $ {25.3}_{-16.4}^{+19.0} $
10 C Y 5199 2373 + 3995 $ 5199_{-2373}^{+3995} $ 1.87 0.29 + 0.07 $ {1.87}_{-0.29}^{+0.07} $ 0.44 0.68 + 0.68 $ {-0.44}_{-0.68}^{+0.68} $ 33 14 + 18 $ {33}_{-14}^{+18} $ 48 17 + 25 $ {48}_{-17}^{+25} $ 21.5 14.0 + 30.0 $ {21.5}_{-14.0}^{+30.0} $
11 C - 525 339 + 955 $ 525_{-339}^{+955} $ 1.23 0.76 + 0.50 $ {1.23}_{-0.76}^{+0.50} $ 0.50 2.50 + 2.93 $ {-0.50}_{-2.50}^{+2.93} $ 53 6 + 29 $ {53}_{-6}^{+29} $ 44 26 + 33 $ {44}_{-26}^{+33} $ 1.1 0.9 + 4.2 $ {1.1}_{-0.9}^{+4.2} $
12 C - 252 161 + 338 $ 252_{-161}^{+338} $ 0.94 0.45 + 0.80 $ {0.94}_{-0.45}^{+0.80} $ 0.06 2.18 + 1.67 $ {-0.06}_{-2.18}^{+1.67} $ 37 10 + 39 $ {37}_{-10}^{+39} $ 70 50 + 7 $ {70}_{-50}^{+7} $ 0.9 0.7 + 2.6 $ {0.9}_{-0.7}^{+2.6} $
13 C N 1354 717 + 1017 $ 1354_{-717}^{+1017} $ 1.64 0.31 + 0.22 $ {1.64}_{-0.31}^{+0.22} $ 0.28 0.54 + 0.37 $ {-0.28}_{-0.54}^{+0.37} $ 34 16 + 21 $ {34}_{-16}^{+21} $ 53 22 + 23 $ {53}_{-22}^{+23} $ 6.3 3.7 + 10.2 $ {6.3}_{-3.7}^{+10.2} $
14 C - 330 220 + 423 $ 330_{-220}^{+423} $ 1.39 0.77 + 0.38 $ {1.39}_{-0.77}^{+0.38} $ 0.14 1.98 + 2.14 $ {-0.14}_{-1.98}^{+2.14} $ 48 23 + 27 $ {48}_{-23}^{+27} $ 59 40 + 18 $ {59}_{-40}^{+18} $ 1.0 1.0 + 1.2 $ {1.0}_{-1.0}^{+1.2} $
15 C Y 1273 664 + 776 $ 1273_{-664}^{+776} $ 1.68 0.35 + 0.13 $ {1.68}_{-0.35}^{+0.13} $ 0.65 0.80 + 0.39 $ {0.65}_{-0.80}^{+0.39} $ 35 16 + 28 $ {35}_{-16}^{+28} $ 60 29 + 19 $ {60}_{-29}^{+19} $ 6.1 4.1 + 6.8 $ {6.1}_{-4.1}^{+6.8} $
16 C Y 2339 1202 + 2263 $ 2339_{-1202}^{+2263} $ 1.46 0.27 + 0.39 $ {1.46}_{-0.27}^{+0.39} $ 0.51 0.80 + 0.78 $ {-0.51}_{-0.80}^{+0.78} $ 41 19 + 27 $ {41}_{-19}^{+27} $ 59 29 + 19 $ {59}_{-29}^{+19} $ 8.9 6.1 + 17.4 $ {8.9}_{-6.1}^{+17.4} $
17 C Y 1151 533 + 718 $ 1151_{-533}^{+718} $ 1.44 0.28 + 0.33 $ {1.44}_{-0.28}^{+0.33} $ 0.53 0.77 + 0.59 $ {-0.53}_{-0.77}^{+0.59} $ 39 18 + 18 $ {39}_{-18}^{+18} $ 53 18 + 25 $ {53}_{-18}^{+25} $ 5.8 2.9 + 5.8 $ {5.8}_{-2.9}^{+5.8} $
18 C Y 2746 1140 + 1645 $ 2746_{-1140}^{+1645} $ 1.79 0.20 + 0.11 $ {1.79}_{-0.20}^{+0.11} $ 0.07 0.30 + 0.26 $ {-0.07}_{-0.30}^{+0.26} $ 32 12 + 12 $ {32}_{-12}^{+12} $ 47 14 + 18 $ {47}_{-14}^{+18} $ 15.6 6.8 + 16.4 $ {15.6}_{-6.8}^{+16.4} $
19 C - 1072 1140 + 1645 $ 1072_{-1140}^{+1645} $ 1.56 0.98 + 0.22 $ {1.56}_{-0.98}^{+0.22} $ + 0.95 2.93 + 4.44 $ {+0.95}_{-2.93}^{+4.44} $ 36 10 + 40 $ {36}_{-10}^{+40} $ 53 32 + 24 $ {53}_{-32}^{+24} $ 3.8 3.1 + 18.6 $ {3.8}_{-3.1}^{+18.6} $
20 C Y 1150 620 + 1150 $ 1150_{-620}^{+1150} $ 1.40 0.55 + 0.40 $ {1.40}_{-0.55}^{+0.40} $ 1.60 1.22 + 1.20 $ {-1.60}_{-1.22}^{+1.20} $ 42 20 + 26 $ {42}_{-20}^{+26} $ 51 25 + 25 $ {51}_{-25}^{+25} $ 3.6 2.5 + 10.6 $ {3.6}_{-2.5}^{+10.6} $
21 C Y 5510 3670 + 2999 $ 5510_{-3670}^{+2999} $ 1.69 0.44 + 0.18 $ {1.69}_{-0.44}^{+0.18} $ 0.05 0.64 + 0.51 $ {-0.05}_{-0.64}^{+0.51} $ 40 23 + 13 $ {40}_{-23}^{+13} $ 55 31 + 17 $ {55}_{-31}^{+17} $ 19.8 12.8 + 35.1 $ {19.8}_{-12.8}^{+35.1} $
22 C Y 1776 946 + 956 $ 1776_{-946}^{+956} $ 1.79 0.19 + 0.14 $ {1.79}_{-0.19}^{+0.14} $ 0.004 0.292 + 0.296 $ {-0.004}_{-0.292}^{+0.296} $ 37 18 + 22 $ {37}_{-18}^{+22} $ 55 23 + 22 $ {55}_{-23}^{+22} $ 12.8 7.8 + 12.8 $ {12.8}_{-7.8}^{+12.8} $
23 C Y 333 162 + 297 $ 333_{-162}^{+297} $ 1.61 0.45 + 0.22 $ {1.61}_{-0.45}^{+0.22} $ 0.33 0.55 + 0.75 $ {-0.33}_{-0.55}^{+0.75} $ 38 16 + 31 $ {38}_{-16}^{+31} $ 55 25 + 22 $ {55}_{-25}^{+22} $ 1.5 1.1 + 3.7 $ {1.5}_{-1.1}^{+3.7} $
24 C Y 4651 1185 + 1307 $ 4651_{-1185}^{+1307} $ 1.65 0.11 + 0.11 $ {1.65}_{-0.11}^{+0.11} $ 0.26 0.19 + 0.17 $ {-0.26}_{-0.19}^{+0.17} $ 40 9 + 9 $ {40}_{-9}^{+9} $ 54 10 + 14 $ {54}_{-10}^{+14} $ 25.4 7.8 + 14.2 $ {25.4}_{-7.8}^{+14.2} $
25 C Y 4252 2029 + 4221 $ 4252_{-2029}^{+4221} $ 1.79 0.49 + 0.11 $ {1.79}_{-0.49}^{+0.11} $ 0.15 0.66 + 0.67 $ {-0.15}_{-0.66}^{+0.67} $ 33 13 + 26 $ {33}_{-13}^{+26} $ 54 26 + 22 $ {54}_{-26}^{+22} $ 21.1 13.3 + 28.6 $ {21.1}_{-13.3}^{+28.6} $
26 C - 606 430 + 518 $ 606_{-430}^{+518} $ 1.48 0.96 + 0.26 $ {1.48}_{-0.96}^{+0.26} $ 0.55 2.63 + 3.29 $ {-0.55}_{-2.63}^{+3.29} $ 48 22 + 28 $ {48}_{-22}^{+28} $ 61 41 + 16 $ {61}_{-41}^{+16} $ 0.6 0.5 + 1.7 $ {0.6}_{-0.5}^{+1.7} $
27 C Y 2112 1083 + 2855 $ 2112_{-1083}^{+2855} $ 1.61 0.68 + 0.21 $ {1.61}_{-0.68}^{+0.21} $ 0.08 0.98 + 0.89 $ {0.08}_{-0.98}^{+0.89} $ 38 16 + 33 $ {38}_{-16}^{+33} $ 69 41 + 9 $ {69}_{-41}^{+9} $ 11.1 7.1 + 35.5 $ {11.1}_{-7.1}^{+35.5} $
28 C Y 351 277 + 515 $ 351_{-277}^{+515} $ 1.56 1.07 + 0.21 $ {1.56}_{-1.07}^{+0.21} $ 0.02 2.09 + 1.56 $ {-0.02}_{-2.09}^{+1.56} $ 35 14 + 30 $ {35}_{-14}^{+30} $ 43 18 + 33 $ {43}_{-18}^{+33} $ 0.3 0.3 + 1.9 $ {0.3}_{-0.3}^{+1.9} $
29 C N 436 256 + 359 $ 436_{-256}^{+359} $ 1.73 0.52 + 0.12 $ {1.73}_{-0.52}^{+0.12} $ + 23.32 0.73 + 0.41 $ {+23.32}_{-0.73}^{+0.41} $ 44 18 + 33 $ {44}_{-18}^{+33} $ 51 42 + 25 $ {51}_{-42}^{+25} $ 1.1 0.8 + 3.7 $ {1.1}_{-0.8}^{+3.7} $

Note: The columns show (1) the ID number, (2) the model used (C for circular, F for full), (3) whether the central wavelength of Hβ and Hγ was tied to that of Hα whenever the other Balmer lines are available, (4) the Hα BLR size in ld, (5) the shape parameter of the radial cloud distribution, (6) the amount of shift on the central wavelength of the Balmer line(s), (7) inclination angle, (8) position angle, (9) anisotropy parameter, (10) vertical distribution of clouds, (11) midplane obscuration, (12) binary switch for inflowing (fflow < 0.5) and outflowing (fflow > 0.5) radial motion, (13) fraction of clouds in circular/bound orbits, (14) angular location for radial orbit distribution, and (15) the peak expected differential phase. All errors are 1σ uncertainties. More details about the BLR model parameters are discussed in Sect. 5, while the calculation of the peak expected differential phase is shown in Sect. 6.

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