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Table A.2.

Published and new spectroscopic solutions of the SB1 systems and candidates in the MONOS sample. T0 corresponds to the periastron passage for the eccentric orbits. The orbits derived in this work are marked as TP. Errors in parentheses corresponds to the last digit. An ”f” means that the parameter was fixed for that solution. An asterisk after the mass function indicates that the value was calculated by us with the parameters of the orbital solution. We denote ellipsoidal systems with an ”†” after the SBS classification. For the rotational velocities (v sini) measured in this work, we used the IACOB-BROAD tool.

Name SBS Class. Period T0 e ω K1 γ1 f(m) v sin i Ref
MONOS II d JD−2 400 000 degrees km s−1 km s−1  M km s−1
HD 164 438 SB1 10.249 74(17) 55 501.114(74) 0.296(13) 220.7(26) 27.78(40) -14.4(25) 0.019 8(9) 55(3) TP. HeI
... ... 10.249 73(26) 55 501.148(114) 0.302(20) 222.3(41) 27.11(57) -15.95(39) 0.018 3(12) 55(3) TP. CC
... ... 10.250 42(40) 55 501.050(60) 0.310(13) 218.5(25) 26.90(40) -8.00(30) 0.017 8(8) 89(2) Ma17
V479 Sct SB1 3.906 09(12) 55 017.468(240) 0.272(107) 263.5(270) 19.73(243) 26.52(185) 0.002 77(105) 157(8) TP. OIII
... ... 3.906 06(7) 55 017.133(208) 0.282(113) 232.9(246) 21.73(288) 10.61(165) 0.003 67(151) 157(8) TP. HeII
... ... 3.906 00(f) 55 017.080(60) 0.240(80) 237.3(218) 23.60(400) 3.90(130) 0.004 90(60) ... Sa11
... ... 3.906 08(10) 52 825.985(53) 0.337(36) 236.0(58) 19.74(86) 4.01(31) 0.002 61(36) ... Ar09
... ... 3.906 03(17) 51 943.090(100) 0.350(40) 225.8(33) 25.20(140) 17.20(70) 0.005 30(90) 113(8) Ca05
... ... 4.426 70(50) 52 756.490(70) 0.480(60) 268.0(100) 17.60(130) 4.10(80) 0.001 70(50) 140(8) Mc04
... ... 4.117 00(1100) 51 822.120(90) 0.410(50) 217.0(90) 14.70(90) 4.60(50) 0.001 03(20) 131(6) Mc01
9 Sge Single 78.740(f) 44 075.770(1130) 0.556(44) 262.00(4000) 11.45(112) 17.0(4) 0.007 00 ... Un95
... ... 32.514 4817.201 0.600 356.22 9.00 11.0 0.001 25 ... As92
... ... 78.300 44 073.630 0.380 164.00 9.00 13.6 0.005 70 ... As84
Cyg X-1 SB1E 5.599 754(37) 56 796.219(12) 0.0(f) 83.79(130) 2.84(125) 0.3408(161) 95(5) TP. HeII
... ... 5.599 742(35) 56 796.781(11) 0.0(f) ... 77.55(118) 7.42(115) 0.2701(124) 95(5) TP. OIII
... ... 5.599 664(86) 56 793.040(29) 0.0(f) ... 74.25(271) -14.70(252) 0.2371 95(5) TP. HeI
... ... 5.599 829(f) 41 163.529(9) 0.018(3) 307.6(53) ... ... 0.2256 * 95(6) Or11
... ... 5.599 829(f) 52 872.788(9) 0.0(f) ... 73.00(70) ... 0.2257 * ... Gi08
... ... 5.599 829(f) 51 730.449(8) 0.0(f) ... 75.60(70) ... 0.2510(70) ... Gi03
... ... 5.599 829(16) 41 874.707(9) 0.0(f) ... 74.93(56) ... 0.2440 ... Br99
... ... 5.601 700(100) 5869.170(10) 0.0(f) ... 75.00(10) -4.44(50) 0.2248 * 94.3(5) Ni87
... ... 5.599 740(80) 5869.110(14) 0.0(f) ... 74.60(130) -0.90(100) 0.2420(90) ... Gi82
... ... 5.607 500 41 166.060 0.0(f) ... 64.00 ... 0.1200 100(2) We72
BD +36 4063 SB1E 4.812 17(3) 58 381.04(2) 0.01(1) 22.(83) 160.(3) 0.5(18) 2.06(10) 96(5) TP. comb. HeII
... ... 4.812 60(40) 52 448.60(8) 0.0(f) ... 163.(3) -17.0(30) 2.18(12) 126(15) Wi09
HDE 229 234 SB1E 3.510 395(12) 56 527.114(13) 0.04(1) 56.0(20) 49.9(6) -29.6(5) 0.0451(16) 95(5) TP. comb. HeI
... ... 3.510 590(1750) 54 714.326(11) 0.0(f) ... 48.5(11) -16.3(8) 0.0420(30) ... Mh13
... ... 3.510 420(50) 50 892.400(10) 0.0(f) 0.0(f) 50.9(8) -15.0(6) 0.0480(20) 103(2) Bo04
HD 192 281 Single 5.480(6) 45 922.469 0.19(11) 26.9(400) 16.8(24) -54.5(27) 0.002 55 270 Ba93
HDE 229 232 AB Single 6.2(2) 54 790.6(1) 0.0(f) ... 15.6(12) -46.6(8) 0.002(1) 273(19) Wi13
ALS 15 133 SB1 unc. 2 259.0(460) 53 355.0(1340) 0.34(11) 157.9(260) 9.0(10) -13.0(10) 0.1419 * ... Ko12
Cyg OB2-A11 SB1 15.4428(25) 55 761.47(99) 0.136(59) 47.0(240) 23.4(14) -18.58(99) 0.0199(37) 100(7) TP. comb. HeI
... ... 15.5110(560) 55 745.70(80) 0.210(70) 37.0(190) 24.0(20) -13.00(100) 0.0208 * ... Ko12

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