Open Access

Tab1e A.1

Targets observed as part of the ES0 SupJup Survey (Program ID: 1110.C-4264, PI: Sne11en), sorted by right ascension.

System Name 0n-S1it Targets d (pc) BANYAN Σ(1) Age (Myr) SpType mJ (mag) mK (mag) M (MJup) a (″/AU) 0bs. Date Setting A0 S1it Exp. Time
HD 1160 HD 1160B, 120.9±0.5(2) FIELD (99.9%) 10-20<3> M5.5(4), 15.83±0.10, 14.12±0.05, 20(3), 0.78/80, 2022 11 01 K2166 Yes 0.4 45×300s = 3h45m
HD 1160C M3.5(5) 13.31±0.04(5) 12.18±0.06(5) 231±42(3) 5.15/530(5)

LSPM J0036+1821 LSPM J0036 8.74±0.01(2) FIELD (99.9%) - L3.5(6) 12.47±0.03(7) 11.06±0.02(7) - - 2022 11 03 K2166 No 0.2 10×300s = 0h50m
2022 11 04 J1226 No 0.2 14×300s = 1h10m
2h00m

2MASS J01033563-5515561 2M 0103AB, 12.86±1.97(8) THA (99.3%) 45±4 M5.5, 10.16±0.02(7), 9.24±0.02(7), 199/178±21, 1.72/84(10) 2022 11 04 K2166 No 0.4 34×300s = 2h50m
2M 0103(AB)b L(10) 15.4±0.3(10) 13.6±0.2(10) 13+1(10)

2MASS J01225093-2439505 2M 0122A, 33.74±0.03(2) ABDMG (98.4%) 14919+51$149_{ - 19}^{ + 51}$(9) M3.5(11), 10.02±0.03, 9.17±0.03, 419±52, 1.45/52±6(12) 2022 11 02 K2166 Yes 0.4 49×300s = 4h05m
2M 0122B L4-6(12) 16.81±0.14(12) 14.53±0.05(12) 23-27(12)
2022 11 03 K2166 Yes 0.4 42×300s = 3h30m
7h35m

2MASS J01415823-4633574 2M 0141 36.65±0.59(2) THA (99.9%) 45±49 L0(13) 14.83±0.04(7) 13.10±0.03(7) - - 2023 01 03 K2166 No 0.4 12×300s = 1h00m

2MASS J02192210-3925225 2M 0219A, 40.2±0.1(2) THA (99.9%) 45±49 M6, 11.32±0.03, 10.44±0.03, 113±12, 3.96/156±10(14) 2022 11 01 K2166 No 0.4 26×300s = 2h10m
2M 0219B L4(14) 15.54±0.10(14) 13.82±0.10(14) 13.9±1.1(14)
2022 11 03 K2166 No 0.4 16×300s = 1h20m
2022 11 04 K2166 No 0.4 32×300s = 2h40m
6h10m

DENIS J025503.3-470049 DENIS J0255 4.868±0.004(2) FIELD (99.9%) - L9(15) 13.24±0.03(7) 11.56±0.02(7) - - 2022 11 02 K2166 No 0.2 12×300s = 1h00m

2MASS J03552337+1133437 2M 0355 9.16±0.04(2) ABDMG (99.9%) 149+51(9) L5(13) 14.05±0.02(7) 11.53±0.02(7) - - 2022 11 02 K2166 No 0.2 10×300s = 0h50m

FU Tau FU Tau A, 127.6±1.2(2) TAU (96.6%) ļ.2(16) M7.25, 10.78±0.03, 9.32±0.02, 52.4, 5.7/800(17) 2023 01 01 K2166 No 0.4 24×300s = 2h00m
FU Tau B M9.25(17) 15.04±0.12(7) 13.33±0.10(7) 15.7(17)

DH Tau DH Tau A, 133.4±0.5(2) TAU (99.8%) 1_2(i6) M0.5, 9.77±0.02, 8.18±0.03, 670±42(19), 2.34/328.2±0.4(21) 2022 12 31 K2166 No 0.4 16×300s = 1h20m
DH Tau B L2 (18) 15.71±0.05(18) 14.19±0.02(15) 8-22(20)
2023 01 01 K2166 No 0.4 14×300s = 1h10m
2h30m

2MASS J04341527+2250309 2M 0434 163±10(2) TAU (87.8%) 1-2(16) M7(22) 13.74±0.03(7) 11.85±0.02(7) - - 2022 12 31 K2166 No 0.4 1×300s = 0h05m
2023 02 01 K2166 No 0.4 22×300s = 1h50m
2023 02 01 J1226 No 0.4 10×300s = 50m
2h45m

2MASS J05002100+0330501 2M 0500 13.23±0.05(2) FIELD (99.9%) - L4(23) 13.67±0.02(7) 12.06±0.02(7) - - 2023 02 27 K2166 No 0.4 18x300 = 1h30m

2MASS J05012406-0010452 2M 0501 20.9±0.3(2) FIELD (99.9%) - L4(13) 14.98±0.04(7) 12.96±0.04(7) - - 2022 12 31 K2166 No 0.4 3×300s = 0h15m
2023 02 01 K2166 No 0.4 12×300s = 1h00m
1h15m

2MASS J05233822-1403022 2M 0523 12.73±0.02(2) FIELD (99.9%) - L2.5(24) 13.08±0.02(7) 11.638±0.03(7) - - 2023 01 03 K2166 No 0.4 12×300s = 1h00m

β Pic β Pic b 19.44±0.05(2) β PMG (99.9%) 24±3<"> L2(25) 14.00±0.08(25) 12.30±0.15(25) 11.903.04+2.93$11.90_{ - 3.04}^{ + 2.93}$ ~0.5/10.6±0.5(27) 2023 01 02 K2166 Yes 0.2 210×120s = 7h00m

2MASS J05591914-1404488 2M 0559 10.50±0.08(2) FIELD (99.9%) - T4.5(28) 13.80±0.02(7) 13.58±0.05(7) - - 2023 02 01 K2166 No 0.4 16×300s = 1h20m
2023 02 01 J1226 No 0.4 4×300s = 0h20m
1h40m

DENIS J060852.8-275358 2M 0608 44.2±0.3(2) FIELD (99.9%) - M9.6(29) 13.60±0.03(7) 12.37±0.03(7) - - 2023 02 26 K2166 No 0.4 24×300s = 2h00m

CD-35 2722 CD-35 2722A, 22.36±0.01(2) ABDMG (99.9%) 14919+51$149_{ - 19}^{ + 51}$(9) M1(30), 7.86±0.03, 7.03±0.05, 419±52, 3.14/67±4(31) 2022 12 31 K2166 No 0.4 8×300s = 0h40m
CD-35 2722B L4(31) 13.63±0.11(31) 12.01±0.07(31) 31±8(31)
2023 01 03 K2166 No 0.4 24×300s = 2h00m
2023 01 31 J1226 No 0.4 7×300s = 0h35m
3h15m

AB Pic AB Pic b 50.14±0.03(2) CAR (99.7%) 13.30.6+1.1$13.3_{ - 0.6}^{ + 1.1}$(32) L0-1(33) 16.18±0.10(34) 14.14±0.08(34) 10±1(35) 5.4/273±2(34) 2022 11 01 K2166 Yes 0.4 22×300s = 1h50m
2022 11 02 K2166 Yes 0.4 12×300s = 1h00m
2022 11 03 K2166 Yes 0.4 16×300s = 1h20m
2022 11 04 K2166 Yes 0.4 14×300s = 1h10m
5h20m

2MASS J06244595-4521548 2M 0624 12.19±0.05(2) ARG (93.5%) 40-50(36) L6.5(15) 14.48±0.03(7) 12.60±0.03(7) - - 2023 02 27 K2166 No 0.4 15×300 = 1h15m

SSSPM J0829-1309 2M 0829 11.68±0.02(2) FIELD (99.9%) - L2(37) 12.80±0.03(7) 11.30±0.02(7) - - 2023 01 03 K2166 No 0.4 12×300s = 1h00m

2MASS J08354256-0819237 2M 0835 7.23±0.01(2) FIELD (95.1%) - L6.5(15) 13.17±0.02(7) 11.136±0.02(7) - - 2023 01 01 K2166 No 0.4 4×300s = 0h20m

HR 3549 HR 3549B 94.8±0.3(2) FIELD (92.1%) 100-150(38) L0(38) 15.94±0.06(38) - 40-50(38) 0.9/80(39) 2023 01 01 K2166 Yes 0.2 26×300s = 2h10m

2MASS J08561384-1342242 2M 0856 53.8±0.4(2) FIELD (96.2%) - M8(23) 13.60±0.03(7) 12.49±0.02(7) - - 2023 03 04 K2166 No 0.4 18×300s = 1h30m

2MASSI J0953212-101420 2M 0953 35.7±0.3(2) FIELD (63.5%) - L0.0(29) 13.47±0.03(7) 12.14±0.02(7) - - 2023 03 04 K2166 No 0.4 18×300s = 1h30m

Luhman 16 Luhman 16A, 2.02±0.15(2) ARG (94.1 %) 40-50(36) L7.5, 11.53±0.04, 9.44±0.07, 33.5±0.3, 1.5/3.12±0.25(40) 2022 12 31 K2166 No 0.2 4×300s = 0h20m
Luhman 16B T0.5(41) 11.22±0.04(41) 9.73±0.09(41) 28.6±0.3(42)
2023 01 01 K2166 No 0.4 4×300s = 0h20m
2023 01 01 J1226 No 0.4 4×300s = 0h20m
1h00m

TWA 28 TWA 28 59.2±0.4(2) TWA (99.6%) 10±3(9) M8.3(43) 13.03±0.02(7) 11.89±0.02(7) - - 2023 03 03 K2166 No 0.4 14×300s = 1h10m

CD-33 7795 TWA 5A, 49.6±0.1(2) TWA (99.9%) 10±3(9) M1.5, 8.40±0.07, 7.39±0.04, ~419(45), 1.9/86±4(46) 2023 02 26 K2166 Yes 0.2 16×300s = 1h20m
TWA 5B M8.5(44) 12.6±0.2(18) 11.4±0.2(18) 2520+120$25_{ - 20}^{ + 120}$(46)

2MASS J11553952-3727350 2M 1155 11.80±0.02(2) FIELD (99.9%) - L2(47) 12.81 ±0.02(7) 11.46±0.02(7) - - 2023 02 01 K2166 No 0.4 4×300s = 0h20m
2023 02 01 J1226 No 0.4 2×300s = 0h10m
0h30m

2MASS J12003792-7845082 2M 1200 101.6±0.7(2) EPSC (99.8%) 3.71.4+4.6$3.7_{ - 1.4}^{ + 4.6}$(48) M6(49) 12.52±0.02(7) 11.60±0.02(7) - - 2023 03 04 K2166 No 0.4 8×300s = 0h40m

HIP 64892 HIP 64892B Π9.6±0.7(2) LCC (74.0%) 15±3(50) M9(51) 14.85±0.15(51) 13.50±0.17(51) 33±4(51) 1.27/159±12(51) 2023 02 26 K2166 Yes 0.2 12×300s = 1h00m
2023 03 03 K2166 Yes 0.2 5×300s = 0h25m
2023 03 04 K2166 Yes 0.2 18×300s = 1h30m
2h55m

YSES 1 YSES 1b, 94.2±0.1(2) LCC (99.1%) 15±3(50) L0(52), 15.73±0.38(52), 14.70±0.14(52), 14±3(52), 1.71/162(52), 2023 02 26 K2166 Yes 0.2 22×600s = 3h40m
YSES 1c L7.5(53) 21.50±0.13(53) 18.13±0.13(53) 6±1(53) 3.37/320(53)
2023 02 27 K2166 Yes 0.2 10×600s = 1h40m
5h20m

2MASS J14252798-3650229 2M 1425 11.85±0.04(2) ABDMG (99.9%) 14919+51$149_{ - 19}^{ + 51}$(9) L4(23) 13.75±0.03(7) 11.81±0.03(7) 2023 02 01 K2166 No 0.4 12×300s = 1h00m
2023 02 01 J1226 No 0.4 4×300s = 0h20m
1h20m

GQ Lup GQ Lup A, 154.1 ±0.7(2) UCL (99.4%) 16±2(50) K7(54), 8.69±0.04, 7.10±0.02, 1079±52(56), 0.7/105(18) 2023 02 27 K2166 Yes 0.2 61×180s = 3h03m
GQ Lup b L1(55) 14.90±0.11(18) 13.34±0.13(18) ~30(57)

R0Xs 12 R0Xs 12A, 138.6±0.3(2) USC0 (97.6%) 10±3(50) M0, 10.28±0.02, 9.10±0.03, 911 ±84, 1.75/210±20(59) 2023 03 03 K2166 No 0.4 2×450s = 0h15m
R0Xs 12b L0(58) 15.82±0.03(58) 14.14±0.03(58) 16±4(59)
2023 03 04 K2166 No 0.4 22×600s = 3h40m
3h55m

PZ Tel PZ Tel B 47.25±0.05(2) βPMG (97.2%) 24±3(9) M7(60) 12.26±0.14(61) 11.42±0.15(61) 279+25$27_{ - 9}^{ + 25}$(62) 0.48/~25(60) 2022 11 02 K2166 Yes 0.2 8×300s = 0h40m
PZ Tel A, G9(63), 6.86±0.02(7), 6.38±0.02(7), H84±3l(64), 0.48/~25(60) 2022 11 03 K2166 Yes 0.2 22×150s = 0h55m
PZ Tel B M7(60) 12.26±0.14(61) 11.42±0.15(61) 279+25$27_{ - 9}^{ + 25}$(62)
1h35m

36 systems 49 on-slit,
19 companions

Notes. As a consequence of the degeneracy between the ages and masses of isolated, field sub-stellar objects, these parameters are not listed. The BANYAN Σ association (Gagné et al. 2018) with the highest membership probability (in parentheses) is shown. The full names of these identifiers are field (FIELD), Tucana-Horologium association (THA), AB Doradus (ABDMG), Taurus (TAU), β Pictoris (βPMG), Carina (CAR), Argus (ARG), TW Hya (TWA), є Chamaeleontis (EPSC), Lower Centaurus Crux (LCC), Upper Centaurus Lupus (UCL), and Upper Scorpius (USCO).

References. (1) Gagné et al. (2018); (2) Gaia Collaboration (2020); (3) Mesa et al. (2020); (4) Garcia et al. (2017); (5) Nielsen et al. (2012); (6) Reid et al. (2000); (7) Cutri et al. (2003); (8) Riedel et al. (2014); (9) Bell et al. (2015); (10) Delorme et al. (2013); (11) Riaz et al. (2006); (12) Bowler et al. (2013); (13) Cruz et al. (2009); (14) Artigau et al. (2015); (15) Burgasser et al. (2006); (16) Kenyon & Hartmann (1995); (17) Luhman et al. (2009); (18) Patience et al. (2012); (19) Xuan et al. (2020); (20) Luhman et al. (2006); (21) Itoh et al. (2005); (22) Monin et al. (2010); (23) Gagné et al. (2015); (24) Cruz et al. (2003); (25) Chilcote et al. (2017); (26) Lacour et al. (2021); (27) GRAVITY Collaboration et al. (2020); (28) Geballe et al. (2002); (29) Bardalez Gagliuffi et al. (2014); (30) Torres et al. (2006); (31) Wahhaj et al. (2011); (32) Booth et al. (2021); (33) Bonnefoy et al. (2010); (34) Chauvin et al. (2005); (35) Palma-Bifani et al. (2023); (36) Zuckerman (2019); (37) Scholz & Meusinger (2002); (38) Mesa et al. (2016); (39) Mawet et al. (2015); (40) Luhman (2013); (41) Burgasser et al. (2013); (42) Lazorenko & Sahlmann (2018); (43) Faherty et al. (2016); (44) Lowrance et al. (1999); (45) Faherty et al. (2010); (46) Neuhäuser et al. (2010); (47) Gizis (2002); (48) Murphy et al. (2013); (49) Schutte et al. (2020); (50) Pecaut & Mamajek (2016); (51) Cheetham et al. (2018); (52) Bohn et al. (2020a); (53) Bohn et al. (2020b); (54) Herbig (1977); (55) Lavigne et al. (2009); (56) MacGregor et al. (2017); (57) Stalker et al. (2021); (58) Bowler et al. (2017); (59) Kraus et al. (2014); (60) Maire et al. (2016); (61) Biller et al. (2010); (62) Franson & Bowler (2023); (63) Stalker et al. (2020); (64) Jenkins et al. (2012)

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