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Table 3:

H-band and mass limits obtained from the observations.
Object $H_{\rm lim} \pm 1\sigma$a ZPb $SE-2MASS-\rm limits$c Lo Curto et al. (2007) Mass-limitd
  [mag] [mag] [mag] [mag] [Jupiter masses]
PSR J0108-1431 $21.42 \pm 0.16$ 24.66 $21.5 \pm 1.5$ $\cdots$ -
RX J0420.0-5022 $21.84 \pm 0.16$ 24.61 $21.5 \pm 0.6$ 21.7 $\cdots$
Gemingae $22.66 \pm 0.14$ 24.66 $^{\rm ep2}$ $22.0 \pm 0.4$ $\cdots$ 12
RX J0720.4-3125 $23.07 \pm 0.11$ 24.63 $^{\rm ep2}$ $22.3 \pm 0.4$ 22.7 15
RX J0806.4-4123 $22.64 \pm 0.16$ 24.59 $22.6\pm 0.4$ 22.9 $\cdots$
RX J1856.6-3754 $21.54 \pm 0.24$ 24.65 $^{\rm ep2}$ $22.1 \pm 0.4$ 21.5 11
PSR J1932+1059 $20.31 \pm 0.18$ 23.49 $\cdots$ $\cdots$ 42
RBS 1774 $22.04 \pm 0.16$ 24.67 $21.6 \pm 1.0$ 22.1 $\cdots$
a $H_{\rm lim}$ indicates the faintest H-magnitude with a detection SNR of three measured close to the position of the neutron star; The $1 \sigma$ error is a result of the StarFinder photometric error, the zeropoint error, and an estimated/assumed error from comparison with 2MASS; b ZP states the magnitude of the zeropoints, which were obtained in the frame of ESO's calibration plan; $^{\rm ep2}$ indicates that two epochs have been used; c SE-2MASS-limits lists the Source Extractor limits if using relative 2MASS photometry; d The mass-limit is according to Sect. 5.1, $\cdots$ notes that the found objects are interesting for a second epoch observation, - states the opposite; e Geminga has been detected in a deeper HST ${\it F160W}$ observation with roughly 24.1 mag (Shibanov et al. 2006).

Source LaTeX | All tables | In the text

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