1992
DOI: 10.1086/116051
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Binary star observations with the Hubble Space Telescope fine guidance sensors. II - Bright Hyades

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Cited by 19 publications
(16 citation statements)
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“…Figure 5 shows the transfer functions of GJ 54AB, LHS 224AB, and the single star HIP 28355, measured along orthogonal axes of FGS1r. These X and Y transfer functions track the visibility of the broadband fringes as the stars are scanned across the Koester's prism (Franz et al 1992). The transfer functions of a single star (left panels of Figure 5) are generally antisymmetric about the zero scan position that denotes alignment between the incoming wavefront and the optical axis.…”
Section: Gj 54ab and Lhs 224abmentioning
confidence: 95%
“…Figure 5 shows the transfer functions of GJ 54AB, LHS 224AB, and the single star HIP 28355, measured along orthogonal axes of FGS1r. These X and Y transfer functions track the visibility of the broadband fringes as the stars are scanned across the Koester's prism (Franz et al 1992). The transfer functions of a single star (left panels of Figure 5) are generally antisymmetric about the zero scan position that denotes alignment between the incoming wavefront and the optical axis.…”
Section: Gj 54ab and Lhs 224abmentioning
confidence: 95%
“…The FGS astrometer offers many observation capabilities (Nelan et al 1998) that have already been used in the past for binary stars (Franz et al 1991(Franz et al , 1992Bernacca et al 1993Bernacca et al , 1995Schneider et al 1998), extended Miras (Lattanzi et al 1994(Lattanzi et al , 1997 and AGN (Hook et al 2000). For such objects the fringe pattern or S -curve changes with respect to that of a point-like source.…”
Section: Effects Of Size and Duplicitymentioning
confidence: 99%
“…The FGS is used in TRANS mode by scanning the instantaneous field of view (IFOV) across the star and recording the difference in photometric counts from pairs of photomultiplier tubes in two orthogonal directions (denoted X and Y). The resulting transfer function (TF) measures the interference pattern between detectors, and in the case of a binary star, the observed TF is a convolution of the TF for a single star with two ␦ functions representing the projected separation and magnitude difference of the pair (Franz et al 1992;Lattanzi et al 1992). The binary separations are then measured by fitting the observations with a composite TF formed by co-addition of two shifted and weighted single-star TFs.…”
Section: Hst͞fgs Astrometry and Astrometric Orbitmentioning
confidence: 99%