Bipolar jets ejected from KX And in the emission lines [OIII] (reddish), Hα (greenish), and [SII] (bluish). The image reveals fine details and shows two jets with an apparent length of about 20′, with the northern jet ending in a bright tip. That structure appears to be the outer end of a cigar-shaped shell. The bright source in the image is KX And. It remains visible after continuum subtraction because the brighter companion of this binary system is an emission-line star.
The jets were only detected in Hα and [SII], while the shell is also visible in [OIII]. This points to different ionization processes. The shell may be rendered visible through shock ionization of the surrounding interstellar medium, whereas the gas in the jets may be ionized by the B3pe component of KX And. (The latter process probably cannot provide sufficient energy to doubly ionize oxygen, resulting in the absence of [OIII] emission.) See also the interactive image below for a direct comparison of the emission lines.
Two structures appear to lie outside the cigar-shaped shell. A diffuse arc crossing the southern jet is visible in Hα and [SII] light (cyan). To the west (right) of KX And, there is a faint cloud that can be detected only in the [SII] channel (blue), which is highly unusual. However, no artifacts that might explain this observation — such as filter issues or flat-field problems — could be identified, and the object itself appears to exhibit some structure. If this object is real, its nature remains a mystery.
A fraction of the material that falls to the accreting star is ejected in the form of jets which are aligned perpendicular to the accretion disk. The jets cannot be detected in [OIII] and are likely ionized by the B3pe component of KX And. The elongated shell, including the bright tip at the end of the northern jet, is probably formed by the interaction of the ejected gas with the interstellar medium and may be rendered visible through shock ionization. Parts of the shell are visible at all observed wavelengths.
The apparent length of the northern jet (with the bright tip) is 19.9′, while the southern jet is 20.3′ long. With a distance of 760±10 pc (Gaia Collaboration et al., 2023) and an inclination to the line of sight of the binary system (and thus of the accretion disc) of about 50° (Berdyugin et al., 1998), this corresponds to a true length of about 19 light-years (5.8 pc) for each jet.
Another class of mass-transferring systems is X-ray binaries, which consist in a mass donating star and an accreting neutron star or black hole. The infalling material releases energy as X-rays, giving these binaries their name. The most famous example is Cyg X-1, a binary consisting in a black hole and the supergiant HD 226868 of spectral class O7Iab (Sota et al., 2011). It is assumed that this star does not overflow its Roche lobe (Ziolkowski, 2014), i.e. mass is transferred through stellar wind.
In optical wavelengths, only one jet becomes visible indirectly due to the interaction of high-energy particles with surrounding interstellar medium. The apparent separation between the resulting shockwave and the binary is 10.9′ (measured in own images). Assuming the jet ends at the bow shock, distance measurements from Gaia DR3 (2255±80 pc) and a inclination of about 27.5° for the binary system (Zdziarski et al., 2024) result in a true length of about 51 light-years. The authors of the latter publication also discuss the possibility of a tilted inner accretion disc with a inclination of 39°, which would result in a length of 37 light-years.
Although the jet of this reference X-ray binary appears to be significantly more energetic, the size of the newly discovered jets from KX And is on the same order of magnitude as that of the jet ejected from Cyg X-1.
| Position (J2000): | RA: 23h07m06.21s; DEC: 50°11′32.5″ (centered on KX And) | ||||||||||
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| Image width × height: | 40′ × 30′ | ||||||||||
| Orientation: | North is oriented upward, but rotated 3.5° toward east (left) | ||||||||||
| Date: | Oct. 25 to Feb. 2026 | ||||||||||
| Location: | Pulsnitz, Germany | ||||||||||
| Instrument: | 400mm Newton at f=1520mm | ||||||||||
| Camera Sensor: | Sony IMX455 | ||||||||||
| Total exposure times: |
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The individual exposures were aligned and intensity-calibrated to sources form Gaia DR3 using synthetic photometry. The Stacking was performed with weights based on noise estimation in order to maximize the final signal-to-noise ratio.
Emission line images are obtained from the stacked results through continuum subtraction. To avoid artifacts around stars, this was done in two steps. First, the stars are subtracted by extracting their positions and intensities from the continuum image. Then, the (starless) residuals are subtracted. This procedure prevents small structures, such as the knots in the jets, from being misinterpreted as stars and therefore removed. Another consequence (of determination the star brightness from the continuum images) is that the emission-line star KX And is only partially subtracted in Hα.
The continuum-subtracted images are then deconvolved and denoised. These results are used to create both color and monochrome images. For the color images, a luminance image is first created by a linear combination of the emission line channels, then tonal curve adjusted, and finally colorized using the linear emission line channels. The last step is designed to preserve luminance, i.e. if one color channel becomes saturated, the intensities in the other channels are increased to maintain the luminance. This prevents loss of detail in saturated regions and is also the reason why KX And appears white rather than green, even though this emission-line star is mainly visible in Hα.
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