2014A&A...567A..98M


Query : 2014A&A...567A..98M

2014A&A...567A..98M - Astronomy and Astrophysics, volume 567A, 98-98 (2014/7-1)

Mid-infrared interferometry with K band fringe-tracking. I. The VLTI MIDI+FSU experiment.

MUELLER A., POTT J.-U., MERAND A., ABUTER R., DELPLANCKE-STROBELE F., HENNING T., KOEHLER R., LEINERT C., MOREL S., PHAN DUC T., POZNA E., RAMIREZ A., SAHLMANN J. and SCHMID C.

Abstract (from CDS):

A turbulent atmosphere causes atmospheric piston variations leading to rapid changes in the optical path difference of an interferometer, which causes correlated flux losses. This leads to decreased sensitivity and accuracy in the correlated flux measurement. To stabilize the N band interferometric signal in MIDI (MID-infrared Interferometric instrument), we use an external fringe tracker working in K band, the so-called FSU-A (fringe sensor unit) of the PRIMA (Phase-Referenced Imaging and Micro-arcsecond Astrometry) facility at VLTI. We present measurements obtained using the newly commissioned and publicly offered MIDI+FSU-A mode. A first characterization of the fringe-tracking performance and resulting gains in the N band are presented. In addition, we demonstrate the possibility of using the FSU-A to measure visibilities in the K band. We analyzed FSU-A fringe track data of 43 individual observations covering different baselines and object K band magnitudes with respect to the fringe-tracking performance. The N band group delay and phase delay values could be predicted by computing the relative change in the differential water vapor column density from FSU-A data. Visibility measurements in the K band were carried out using a scanning mode of the FSU-A. Using the FSU-A K band group delay and phase delay measurements, we were able to predict the corresponding N band values with high accuracy with residuals of less than 1µm. This allows the coherent integration of the MIDI fringes of faint or resolved N band targets, respectively. With that method we could decrease the detection limit of correlated fluxes of MIDI down to 0.5Jy (vs. 5Jy without FSU-A) and 0.05Jy (vs. 0.2Jy without FSU-A) using the ATs and UTs, respectively. The K band visibilities could be measured with a precision down to ≃2%.

Abstract Copyright:

Journal keyword(s): instrumentation: interferometers - techniques: interferometric - methods: observational - methods: data analysis

Simbad objects: 27

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Number of rows : 27
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 * 33 Psc RS* 00 05 20.1411719640 -05 42 27.431698821 6.52 5.65 4.61 3.83 3.29 K0III-IV 208 0
2 V* AD Cet LP? 00 14 27.6308065618 -07 46 49.903268768 8.55 6.74 5.12     M3+III 79 0
3 * iot Cet * 00 19 25.6743948847 -08 49 26.108975369 5.94 4.77 3.55 2.70 2.11 K1+IIICN0.5 180 0
4 * nu. Psc * 01 41 25.8941428289 +05 29 15.401884416 7.36 5.81 4.44 3.38 2.67 K3III 237 0
5 2MASS J02194738-1025406 TT* 02 19 47.3900001624 -10 25 40.608096780   11.80 10.72     K0e 17 0
6 * 80 Cet PM* 02 36 00.0478570968 -07 49 53.745797496   7.088 5.535     M0/1III 52 0
7 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4601 2
8 V* RY Tau Or* 04 21 57.4092550080 +28 26 35.555316612 10.82 10.34 9.30 9.67 8.87 K1IV/Ve 704 1
9 HD 27639 V* 04 22 22.7297393832 +20 49 17.087397924   7.86 5.95     M0III 52 0
10 * eps Tau ** 04 28 37.0002551195 +19 10 49.563140930 5.42 4.54 3.53     G9.5IIICN0.5 591 1
11 * 31 Ori V* 05 29 43.9820095248 -01 05 32.058334392   6.28 4.71     K4III 91 0
12 * del Ori A SB* 05 32 00.398192 -00 17 56.68527           O9.5II+B1V+B0IV 30 0
13 * bet Pic PM* 05 47 17.0876901 -51 03 59.441135 4.13 4.03 3.86 3.74 3.58 A6V 1905 1
14 * tau Pup SB* 06 49 56.1691452909 -50 36 52.339311041   4.13 2.93     K1III 105 0
15 * tet CMa PM* 06 54 11.3988612864 -12 02 19.061163780 7.20 5.51 4.08 2.95 2.17 K3/4III 218 0
16 * 23 Car V* 07 00 51.4852321368 -51 24 09.309494916   6.770 5.151     M1III 34 0
17 V* Z CMa Ae* 07 03 43.1599411656 -11 33 06.209065836 10.51 9.99 8.80     B5/8eq+F5/7 578 3
18 HD 56470 * 07 16 16.6509883752 -21 25 14.800839492   9.98 8.45     K2/3III 10 0
19 * iot Hya PM* 09 39 51.3614722468 -01 08 34.118633450 6.68 5.23 3.91 2.92 2.25 K2.5III 179 0
20 * gam Cha V* 10 35 28.1055499388 -78 36 28.038741243 7.65 5.70 4.12 2.86 1.88 K4III 79 0
21 HD 100546 Be* 11 33 25.4408872296 -70 11 41.241297948   6.71 6.30   6.64 A0VaekB8_lB 806 1
22 V* V1068 Sco LP* 16 53 42.4241880264 -43 03 03.488496048   7.71 6.06     M3II/III 29 0
23 * zet02 Sco PM* 16 54 35.0050319669 -42 21 40.737010682   4.99 3.62     K3III 77 0
24 HD 155826 ** 17 15 35.9021317723 -38 35 38.168900773   6.53 5.95     G0V 90 0
25 * alf Aql dS* 19 50 46.99855 +08 52 05.9563 1.07 0.98 0.76 0.62 0.49 A7Vn 875 1
26 V* LW Aqr LP* 23 52 47.5593324360 -12 01 00.897040632   8.90 7.48     M4III 16 0
27 * 24 Psc ** 23 52 55.5631886976 -03 09 19.733599044   7.023 5.940     K0II/III 59 0

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