Table A.1
VLT/SPHERE observations of the system HD 120326
Epoch | Instr. Filt. | Nexp | DIT | Δπ | seeing | τ0 | airmass | strehl | PI | ESO program |
---|---|---|---|---|---|---|---|---|---|---|
(s) | (°) | (") | (ms) | (RTC) | ||||||
2015-04-09 | IRDIS H23 | 13 | 16 | 1.7 | - | - | 3.3 | - | Bonnefoy | 095.C-0607(A) |
2015-04-09 | IFS YJ | 3 | 16 | 0.3 | 3.3 | - | Bonnefoy | 095.C-0607(A) | ||
2015-08-01 | Zimpol IPRIM | 48a | 28 × 5 | - | 0.65±0.10 | 3.2±0.5 | 1.1 | - | Booth | 095.C-0487(A) |
2016-04-05 | IRDIS H23 (†) | 128 | 32 | 37 | 1.06±0.13 | 3.4±0.6 | 1.12 | 0.63 | Bonnefoy | 097.C-0060(A) |
2016-04-05 | IFS YJ | 64 | 64 | 0.63 | Bonnefoy | 097.C-0060(A) | ||||
2016-06-03 | IRDIS H23 (†) | 80 | 32 | 22 | 0.72±0.14 | 3.1±0.5 | 1.11 | - | Hinkley | 097.C-0949(A) |
2016-06-03 | IFS YJ | 40 | 64 | - | Hinkley | 097.C-0949(A) | ||||
2016-06-13 | IRDIS J23 | 80 | 64 | 44.7 | 1.18±0.17 | 2.1±0.4 | 1.11 | 0.54 | GTO | 097.C-0865(F) |
2018-06-01 | IRDIS Pol. BBH (‡) | 80 | 64 | - | 0.51±0.06 | 4.4±0.8 | 1.11 | 0.69 | Boccaletti | 0101.C-0128(D) |
2019-06-26 | IRDIS BBH | 56 | 32 | 36 | 1.76±0.26 | 2.1±0.3 | 1.13 | 0.53 | Bonnefoy | 0101.C-0016(A) |
2019-06-26 | IFS YJ | 28 | 64 | 0.53 | Bonnefoy | 0101.C-0016(A) | ||||
2019-07-09 | IRDIS BBH (‡) | 224 | 32 | 58 | 0.63±0.07 | 3.1±0.4 | 1.13 | 0.60 | Bonnefoy | 0101.C-0016(A) |
2019-07-09 | IFS YJ (‡) | 112 | 64 | 0.60 | Bonnefoy | 0101.C-0016(A) |
Notes. The results from this work are mainly based on the high-quality observations acquired on 2018-06-01 (polarized intensity) and on 2019-07-09 (total intensity), highlighted via (‡). We also successfully detect the disk in the SPHERE/IRDIS total intensity observations of 2016-04-05 and 2016-06-03 (†; see Fig. 2). The other datasets are of poorer quality with for some no (2015-08-01) or almost no (2016-06-13, 2019-06-26) recovery of disk signal. The observation acquired in 2015-04-09 is not exploitable because the focal plane mask was missing during the observation sequence. (α) The 48 exposures correspond to twelve HWP cycles, resulting in a total time on source of Nexp × DIT. GTO stands for Guaranteed Time Observations (PI: Beuzit).
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