Stephan’s Quintet (SQ, co-moving radial distance = 85 ± 6 Mpc, taken from the NASA/IPAC Extragalactic Database (NED)1) is unique among compact groups of galaxies2,3,4,5,6,7,8,9,10,11,12. Observations have previously shown that interactions between multiple members, including a high-speed intruder galaxy currently colliding into the intragroup medium, have probably generated tidal debris in the form of multiple gaseous and stellar filaments6,8,13, the formation of tidal dwarfs7,14,15 and intragroup-medium starbursts16, as well as widespread intergalactic shocked gas5,10,11,17. The details and timing of the interactions and collisions remain poorly understood because of their multiple nature18,19. Here we report atomic hydrogen (H i) observations in the vicinity of SQ with a smoothed sensitivity of 1σ = 4.2 × 1016 cm−2 per channel (velocity bin-width Δv = 20 km s−1; angular resolution = 4′), which are about two orders of magnitude deeper than previous observations8,13,20,21. The data show a large H i structure (with linear scale of around 0.6 Mpc) encompassing an extended source of size approximately 0.4 Mpc associated with the debris field and a curved diffuse feature of length around 0.5 Mpc attached to the south edge of the extended source. The diffuse feature was probably produced by tidal interactions in early stages of the formation of SQ (>1 Gyr ago), although it is not clear how the low-density H i gas (NH i ≲ 1018 cm−2) can survive the ionization by the intergalactic ultraviolet background on such a long time scale. Our observations require a rethinking of properties of gas in outer parts of galaxy groups and demand complex modelling of different phases of the intragroup medium in simulations of group formation.
Atomic hydrogen (H i) is the least bound component of galaxies and is therefore the easiest (and hence first) to be stripped off and spread around during interactions. Thus, the distribution of the very diffuse H i and its velocity field can provide new information about th earliest interactions. To study the diffuse H i associated with Stephan’s Quintet (SQ), we carried out deep mapping observations of the 21 cm H i emission over a region of around 30′ × 30′ centred on SQ (Fig. 1) using the 19-beam receiver of Five-hundred-meter Aperture Spherical Telescope (FAST). The FAST observations and data reduction are described in the Methods. As shown illustratively in Fig. 2, the final data cube includes 304 spectra in Δv = 20 km s−1 channels covering the velocity range of 4,600–7,600 km s−1, with an average root-mean-square (r.m.s.) noise of 0.16 mJy per beam and an average beam size of 2.9′. The mapping satisfies the Nyquist sampling criterion with beams separated by 1.4′ in the right ascension direction and 1.2′ in the declination direction. The original data cube has a H i column-density sensitivity of 1σ = 1.2 × 1017 cm−2 per channel, which is improved to 1σ = 4.2 × 1016 cm−2 per channel when smoothed to 4′. Results of the analysis of the whole data cube will be presented elsewhere. In this Article we report only the discovery of a large H i structure in the velocity range of 6,550–6,750 km s−1.
Figure 3a presents the integrated H i emission map in the velocity range of 6,550–6,750 km s−1 overlaid on the deep MegaCam optical colour image12. The map has an angular resolution of 4.0′ and Δv = 200 km s−1 (ten times the channel width) with an H i column-density error of 1σ = 1.34 × 1017 cm−2. The base contour starts from NH i = 7.4 × 1017 cm−2 (at a 5.5σ level). The map shows a large H i structure of around 0.6 Mpc in size, which has two parts: an extended source centred on SQ and a diffuse feature attached to the south edge of the source. The extended source encompasses the previously detected 6,600 km s−1 H i component associated with the debris field8,13. As shown by the cyan contours in Fig. 3a, the high-resolution (beam = 19.4″ × 18.6″) Very Large Array (VLA) observations8 detected only the high- density part of the 6,600 km s−1 component (NH i ≥ 5.8 × 1019 cm−2), which is confined to the central region (D ≈ 0.1 Mpc) of the extended source. Most of the high-density H i gas traces the optically detected inner and outer tails6 plus a compact cloud (north-west of NGC 7319) coincident with the intragroup-medium starburst SQ-A16. Single-dish H i mapping observations by the Arecibo Telescope and the Green Bank Telescope, which detected lower density H i gas at NH i ≈ 5 × 1018 cm−2 albeit with lower angular resolutions (>3′), have found evidence for this component to be extended on a scale of around 0.2 Mpc (refs. 20,21). Our deeper FAST map shows an even larger size with a diameter of around 0.4 Mpc. The diffuse feature has a characteristic column density of approximately 7 × 1017 cm−2 in an elongated and curved structure of around 0.5 Mpc in length. It appears at the bottom of the FAST mapping and therefore may well reach beyond the map. The faint optical halo (the yellowish diffuse light around SQ in the optical colour image) discovered previously12 lies inside the extended source and has no spatial overlap with the newly discovered diffuse feature. The first moment map in Fig. 3b shows that in the velocity field the diffuse feature is linked smoothly with the extended source. The two green boxes marked by characters A and B in Fig. 3a cover the entire diffuse H i feature. The sum of all spectra in these two boxes provides a good measure of the spectrum of the diffuse feature, which is presented in Fig. 3c. The spectrum has a flux-density-weighted mean velocity of 6,633 km s−1 and a rather narrow line width of ΔV20 = 160 km s−1 (ΔV20 is the line width measured at 20% of the peak). The integrated flux is 0.42 ± 0.03 Jy km s−1, corresponding to an H i mass of (7.1 ± 0.5) × 108M⨀, which is only around 3% of the total H i mass of SQ (2.45 × 1010M⨀)21. It is worth noting that, although the Green Bank Telescope mapping observations found 65% more H i than the VLA observations, SQ is still slightly deficient in H i abundance compared with normal galaxies (by a factor of around 1.3)4,21. The very diffuse H i (NH i < 3 × 1018 cm−2) discovered in this work does not change this H i deficiency significantly.
Two new detections of unresolved sources can also be found in Fig. 3a. NGC 7320a, detected with the signal-to-noise ratio S/N = 36, has an H i mass of MH i = (6.3 ± 0.2) × 108M⨀ and a vH i = 6,702 ± 24 km s−1. The other source Anon 7, a 4.4σ detection, has an H i velocity of 6,654 ± 16 km s−1 and an H i mass of (2.2 ± 0.5) × 108M⨀. More discussions about these two sources are given in the Methods.
We examine in Fig. 4 the individual spectra in box A and box B to investigate the physical nature of the diffuse feature. No diffuse stellar radiation is detected in these regions down to the limit of the deep MegaCam image. Spectra of beams with detections of S/N > 4 are marked by pink boxes and those with 3 < S/N ≤ 4 by green boxes. Galaxies brighter than the r-band magnitude r = 20 mag found in the SDSS photometric redshift (photo-z) catalogue22 are also marked in Fig. 4. Only two of them have photo-z < 0.1 (marked by red circles) and the remaining 28 have photo-z ≥ 0.1 (orange circles). Given the 1σ error of the photo-z (δz/(1 + z) = 0.02)22 and the redshift of SQ (z = 0.02), galaxies with photo-z ≥ 0.1 are very unlikely to be at the same redshift of SQ (probability < 0.001). We can rule out with high confidence the possibility of the diffuse feature being associated with a collection of gas-rich galaxies (even including those fainter than r = 20 mag), because it needs at least four such galaxies to cover all beams with significant detections of S/N > 4 (one for those in the upper-left corner of box A, two for those in the right half of box A and one for that in box B) and the probability that they happen to have about the same radial velocity is extremely low.
H i clouds without stellar counterparts have been found in and around many galaxy groups/clusters23,24,25,26. Most of them, as the authors of ref. 27 have argued, can be explained by tidal debris of galaxy interaction involving very extended H i disks instead of ‘dark’ or ‘almost dark’ galaxies. Given its location and velocity, the diffuse feature is most likely to be related to the debris field. A hypothetical scenario for the formation of the diffuse feature is that NGC 7320a (v = 6,702 km s−1 and currently around 300 kpc away from the SQ centre) passed through the SQ centre approximately 1.5 Gyr ago (assuming a relative transverse velocity of 200 km s−1) and pulled out from one of the core member galaxies of SQ a tidal tail, which developed into the diffuse feature we see now. Another possibility is that, like the large Leo Ring (D ≈ 0.25 Mpc)28, the diffuse feature could be the product of a high-speed head-on collision between another old intruder and one of the core members of SQ. In this scenario, the collision triggers an expanding density wave that pushes gas in an extended H i disk of the target galaxy outwards to form a very large ring, of which the diffuse feature is the high-density part. A candidate for such an intruder could be Anon 4 (v = 6,057 km s−1, MH i = 1.1 × 109M⨀)8, which spatially coincides with optical galaxy LEDA 141041 (B band magnitude B = 18.4 mag). It has a relative radial velocity of around 600 km s−1 and a projected distance of approximately 0.2 Mpc from the SQ centre. If the relative transverse velocity is around 200 km s−1, it would have taken approximately 1 Gyr for Anon 4 to move to the current position after the collision. Both scenarios proposed above suggest a formation time of the diffuse feature of more than 1 Gyr ago. They are both based on analogies to cases studied in simulations in the literature, which demonstrate that diffuse H i features without a stellar component can be produced in galaxy–galaxy interations27,28. However, two questions remain to be answered: (1) Can the tidal feature in either of the scenarios survive the subsequent interactions that triggered the formation of the inner and outer tails of SQ about (3–8) × 108 years ago18,19? (2) Can H i structures with column density as low as NH i ≲ 1018 cm−2 exist on timescales of around 1 Gyr? These questions can only be answered by more sophisticated models that are built upon the existing simulations for the formation and evolution of SQ18,19. It has been argued that cold gas of NH i ≤ 2 × 1019 cm−2 cannot stay neutral in the intergalactic ultraviolet background radiation for more than 500 Myr (refs. 21,29). A plausible solution for this problem is the physical mechanism involving the transition between ionized and neutral phases due to thermal instabilities in the low-density gas30,31. New simulations, which are beyond the scope of this Article, shall explore this mechanism.
The deep H i mapping observations were carried out in September and October of 2021 using the FAST 19-beam receiver in the standard ON–OFF mode with the total observation time of 22.4 h including overheads (Extended Data Table 1). The FAST 19-beam L-band Array is currently the largest multibeam feed array for H i observations in the world. Details about its properties and performance can be found in ref. 32. The 19 beams are arranged in a hexagonal configuration with the neighbouring beams separated by 5.7′. The observations have a central frequency of 1,391.64 MHz and a frequency coverage of 1,050–1,450 MHz with a resolution of 7.63 kHz (Δv = 1.65 km s−1). For the 19 beams, the average half-power beam-width at 1,391 MHz is 2.9′ (Extended Data Table 2). To meet the Nyquist sampling criterion and fill the gaps between beams in the focal plane, we carried out 16 pointings in a 4 × 4 rectangular grid in the north-up orientation (Fig. 1). The final mapping covers a region of around 30′ × 30′ centred on SQ with 304 sky pixels (beam positions in the sky), and the separation between the nearest pixels is 1.4′ in the right ascension direction and 1.2′ in the declination direction. The 1σ pointing error of individual beams is 7.9′′ (ref. 32). At each pointing, six cycles of ON–OFF integrations were conducted, with the OFF position at 40′ southeast from the ON position. Each ON or OFF took 300 s integration with a sampling frequency of 1 Hz. The total on-target time for each pixel was 1,800 s (Extended Data Table 1). To minimize the effects of standing waves and sidelobes, all observations were confined within the zenith angle of 20°.
Compared with the scan-mapping mode, which is more suitable for large sky surveys such as the FAST Extragalactic HI Survey33, our observational strategy provides an alternative for deep and small maps (≤30′), which can take advantage of the ON–OFF mode in more accurately removing various systematic effects such as the standing waves and baseline wobbling.
Data reduction and calibration
For each sky pixel observed by a given beam, we reduced the spectral data following a similar procedure to that presented in ref. 34. The spectra of the two polarizations were reduced separately (and eventually combined after the consistency check). The data were grouped in ON–OFF cycles. Each ON (or OFF) has 300 samplings which were averaged and calibrated (that is, converted from digital counts to kelvin), resulting in a single raw spectrum. During the observations, a calibration signal of 10 K was injected for a duration of 20 s at the beginning of every ON–OFF cycle, and these data were used to calibrate the antenna temperature Ta. The calibration error is on the order of 10%. Repeating this, we obtained a raw spectrum for every ON or OFF. As examples, the upper panel of Extended Data Fig. 1 presents the individual raw ON–OFF spectra obtained by the M01 beam during the first pointing observation (the P1 pixel in Fig. 1). The mean of these spectra is presented in the middle panel of Extended Data Fig. 1. It is affected significantly by the standing waves, which can be well fitted by a sine function locally. The spectrum has been converted from Ta (in K) to flux density (in mJy). The gain factor that converts Ta to flux density (in the units of K Jy−1) depends on the frequency and varies from beam to beam. The values for individual beams at 1,391 MHz, derived by interpolating values at other frequencies adopted from ref. 32, are presented in Extended Data Table 2. The next step was to remove the standing waves together with the baseline from the spectrum. The bottom panel of Extended Data Fig. 1 presents the final spectrum at sky pixel P1 after the subtraction of a baseline modelled by a sinusoidal (representing the standing waves) plus a polynomial (for the baseline gradient). We converted the frequency to velocity by adopting the optical redshift convention and the local standard of rest reference frame and rebinned the spectrum into bins of Δv = 20 km s−1. The above process was carried out repeatedly for every sky pixel observed in our observations.
It is worth noting that, if the standing waves and baseline vary significantly during a given observation, it is better to carry out the removal of the standing waves and baseline for spectra of individual ON–OFFs instead of doing it for their mean. However, in a test in which we did the standing waves and baseline subtraction for each ON–OFF and then used the median of the baseline-subtracted spectra of ON–OFFs as the final spectrum at a given pixel, we got a noisier product. It seems that the wavelength of the standing waves (in the frequency domain) in a given observation is rather constant (although the phase changes from cycle to cycle). Consequently, the effect of the standing waves in the mean of the spectra of individual ON–OFFs is still a well-defined sinusoidal with the same wavelength, which can be easily removed. Hence, because the mean spectrum is less noisy than individual spectra and therefore a more accurate model for the standing waves and the baseline can be obtained, subtracting the baseline model from the mean spectrum can achieve a better result.
The final data cube was constructed from the 304 individual spectra obtained using this technique, with a velocity coverage of 4,600–7,600 km s−1 in 20 km s−1 bins. A uniform half-power beam-width of 2.9′ was adopted for all spectra, neglecting the small variation of the beam size among different beams.
The actual half-power beam-width of individual beams at 1,391 MHz, derived from interpolations of values adopted from ref. 2, are listed in Extended Data Table 2. The units of the flux density of the spectra in the cube are mJy per beam. To find the flux density in units of mJy for a given spectrum, a factor of A = (B/2.9′)2 should be multiplied to the value taken from the cube, where B is the half-power beam-width (in arcmin) of the beam with which the spectrum was observed.
In the 16-pointing observations, each of the 19 beams covered 16 adjacent sky pixels. The mean and the standard deviation of the measured r.m.s. noise of these 16 spectra are also listed in Extended Data Table 2. The r.m.s. noise of each spectrum was measured in the two velocity intervals of 4,700–5,000 km s−1 and 7,000–7,500 km s−1, where no H i signal was detected. Beam M16 stands out as the noisiest beam in the array, with a mean r.m.s. of 0.26 mJy per beam and a standard deviation of 0.14 mJy beam. The false colour map of the r.m.s. noise in the left panel of Extended Data Fig. 2 shows that indeed pixels in the top-right corner that were covered by beam M16 have higher noise than others. The histogram of the distribution of the r.m.s. noise at all sky pixels is shown in the right panel of Extended Data Fig. 2. The mean of the r.m.s. is 0.16 mJy per beam with a standard deviation of 0.05 mJy per beam. It is worth noting that strong radio frequency interference (RFI) in the frequency range of our observations was a serious issue in the early stages of this project. The operation team of FAST did excellent work in discovering and removing the source of the RFI in a relatively short time. All of our observations were carried out after the removal of the RFI source. Consequently, our observations were not affected by any significant RFI.
The H i data cube obtained above is highly redundant in the sense that a sky area of the size of a single beam (D = 2.9') is covered by multiple beams (beam separation 1.4' x 1.2'). When making channel maps and integrated emission maps from the data cube, applying a Gaussian-kernel convolution (that is, smoothing) makes good use of this redundancy. This minimizes the noise due to the signal fluctuations in adjacent beams and results in significant improvement in the H i column-density sensitivity. The only disadvantage is a slight degradation in the angular resolution. For single-channel maps, the mean r.m.s. of 0.16 mJy per beam corresponds to a H i column-density sensitivity of 1σ = 1.2 × 1017 cm−2 per channel (Δv = 20 km s−1). When a smoothing with a Gaussian kernel of full-width at half-maximum (FWHM) = 2.8′ is applied, the H i column-density sensitivity is improved by a factor of 2.9 to 1σ = 4.2 × 1016 cm−2 per channel whereas the angular resolution is degraded only slightly (by a factor 1.4) to 4.0′. The improvement in the H i column-density sensitivity is particularly important for the exploration of diffuse extended emission. In Extended Data Fig. 3 we present the contour map of the integrated H i emission in the velocity range of 6,550–6,750 km s−1 before the smoothing. Compared with the map after the smoothing (Fig. 3a), the low H i column-density features in Extended Data Fig. 3 are more fragmented mainly because of the signal fluctuations in adjacent beams. On a linear scale the pre- and after-smoothing resolutions are 72.5 kpc and 100 kpc, respectively, which is not a significant difference given that we are searching for extended diffuse H i gas on a linear scale of a few 100 kpc.
The data cube is corrected for the sidelobes using the images of individual beams of the 19-beam receiver32, which provide information about the point spread functions of the beams. For each beam, a ‘sidelobe responsivity function’ is defined by the difference between the point spread function and the ‘main beam’, the latter being approximated by a two-dimensional Gaussian with the FWHM equal to the half-power beam-width. In the calculation of the sidelobe corrections, we consider only the effects due to the central extended source associated with the SQ group. The FAST observations also detected numerous other H i sources in the SQ neighbourhood in the velocity range of 5,500–7,000 km s−1. They are much fainter than the central SQ source and therefore their contributions to the sidelobes are neglected.
The first step is to estimate the sidelobe contribution to the map of integrated H i emission in the velocity range of 6,550–6,750 km s−1, which encompasses the peak of the H i spectrum of SQ21. The original integrated H i emission map (the observed map) is first deconvolved with the main beam of M01 (the central beam of the 19-beam receiver). Then all pixels outside a circular aperture of D = 10.6′, within which the central extended source is located, are masked. The result is then taken as our approximation for the ‘truth map’. The sidelobe contribution to any given pixel in the observed map is estimated by the following equation: Fsidelobe (xi, yj) = ∑m∑nT(xm, yn) × Rk (xm − xi, yn − yj), where xi and yj are the coordinates of the pixel centre, T(xm, yn) is the flux in the truth map in the pixel at xm and yn, Rk is the sidelobe responsivity function of the beam that is pointed at the pixel (xi, yj), and ∑m and ∑n are summations along the x and y directions, respectively. Extended Data Figure 4 presents the map of the sidelobe contribution estimated using this method overlaid by contours of the map of integrated H i emission in the velocity range of 6,550–6,750 km s−1 (without the sidelobe correction, smoothed by a Gaussian kernel of FWHM = 2.8′). It shows that the sidelobes contribute significantly at the edge of the debris field but have a minimal effect on the diffuse feature in the south.
Neglecting the frequency dependencies of the shapes of both the sidelobes and the central SQ source, we estimate the sidelobe contribution to each channel in the data cube by scaling the map in Extended Data Fig. 4 with a factor of Cv = Sv /S6,550–6,750, where Sv (in mJy) is the flux density of SQ in the given channel and S6,550–6,750 (in mJy km s−1) is the integrated flux of SQ in the velocity range of 6,550–6,750 km s−1. Finally, we obtain the sidelobe corrected data cube by subtracting the estimated sidelobe contribution from every channel map in the cube. The 304 spectra in the resulting data cube are presented illustratively in Fig. 2.
Detections of two new H i sources in the SQ neighbourhood
In the velocity range of 6,550–6,750 km s−1 we detected two new unresolved H i sources in the SQ neighbourhood (Extended Data Table 3). Their H i spectra are presented in Extended Data Fig. 5. The spectrum of the source associated with NGC 7320a shows a typical double-horn profile consistent with the highly edge-on optical morphology of the galaxy. To confirm the association of the H i source and the optical galaxy, we made a long-slit optical spectroscopic observation (1 h exposure) for NGC 7320a on the night of 21 December 2021 using the 2.4 m telescope at Lijiang Observatory. The optical spectrum is presented in Extended Data Fig. 6. The radial velocity obtained from the optical spectrum is 6,729 ± 59 km s−1, which is consistent with the H i velocity (6,702 ± 24 km s−1). The other source is a 4.4σ detection without obvious optical counterpart and therefore we name it Anon 7 following the convention in the literature8,13.
The Python and IDL code for the data reduction pipeline is available at https://www.scidb.cn/s/jiIfee.
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This work is supported by the National Key R&D Programme of China No. 2017YFA0402704 and National Natural Science Foundation of China (NSFC) No. 11873055 and sponsored (in part) by the Chinese Academy of Sciences (CAS) through a grant to the CAS South America Center for Astronomy. C.K.X. acknowledges NSFC grant No. 11733006. C.C. acknowledges NSFC grant No. 11803044 and 12173045. N.-Y.T. is supported by the National key R&D program of China under grant no. 2018YFE0202900 and the Cultivation Project for FAST Scientific Payoff and Research Achievement of CAMS-CAS. J.-S.H. acknowledges NSFC grant No. 11933003. U.L. acknowledges support from project PID2020-114414GB-100, financed by MCIN/AEI/10.13039/501100011033, from project P20_00334 financed by the Junta de Andalucia and from FEDER/Junta de Andalucía-Consejería de Transformaciòn Econòmica, Industria, Conocimiento y Universidades/Proyecto A-FQM-510-UGR20. F.R. acknowledges support from the Knut and Alice Wallenberg Foundation. This work made use of data from FAST, a Chinese national mega-science facility built and operated by the National Astronomical Observatories, CAS. We thank P. Jiang, L. Hou, C. Sun and other FAST operation team members for supports in the observations and data reductions, and H.-C. Feng and Y. Huang for helping with the optical spectroscopic observation of NGC 7320a. Support of the staff from the Lijiang 2.4 m telescope is acknowledged. Funding for the Lijiang 2.4 m telescope has been provided by the CAS and the People’s Government of Yunnan Province. This research has made use of the NASA/IPAC Extragalactic Database, which is operated by the Jet Propulsion Laboratory, California Institute of Technology, under contract with the National Aeronautics and Space Administration. We dedicate this Article to the memory of Y. Gao, a coauthor of the Article who passed away recently.
The authors declare no competing interests.
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Extended data figures and tables
Upper Panel: Individual ON-OFF spectra obtained by beam M01 in Pointing 1 observation (i.e. the data obtained at the pixel P1 in Figure 1). An offset of 0.2 K is added to every spectrum relative to the previous one in order to make them separated from each other. Middle Panel: The mean of the ON-OFF spectra in the upper panel. The units of the flux density are converted from K to mJy using the gain factor taken from Extended Data Table 2. The red line shows the baseline model derived by fitting the parts of the spectrum free of signals (marked by orange color) using a sinusoidal (representing standing waves) plus a polynomial (for baseline gradient). Bottom Panel: The spectrum after the baseline removal. The frequency is converted to radial velocity in the optical convention relative to the local standard rest reference frame (LSR). The orange line presents the rebinned spectrum with the velocity bin-width of 20 km s−1.
Left: The false color image of the r.m.s. noise at different sky pixels. Right: Histogram of the distribution of the r.m.s. noise.
Contour map of integrated HI emission (unsmoothed) in the velocity range of 6550–6750 km s−1 overlaid on the composite color image (u, g, r) of the deep CFHT MegaCam observation. The red circle at bottom-right illustrates the angular resolution (FWHM =2.9') of the FAST map (unsmoothed). The contours start from NHI = 7.4 × 1017 cm−2 (at 2-σ level) with an increment of a factor of 2. The red lines delineate the boundary of the FAST observations. The cyan contours in the center are adopted from the VLA observations for the 6600 component of SQ8, with angular resolution of 19.4"×18.6". They have the base level at NHI = 5.8 × 1019 cm−2 and the increment of a factor of 2. The same Box A and Box B that mark the location of the diffuse feature in Figure 3a are plotted here to facilitate the comparison between the two figures.
Extended Data Fig. 4 Sidelobe contribution to the integrated HI emission in the velocity range of 6550–6750 km s−1.
False color image of the sidelobe contribution overlaid by the contour map of integrated HI emission in the velocity range of 6550–6750 km s−1 (before the sidelobe correction and after the convolution by a Gaussian kernel of FWHM = 2.8'). The contours start from 20 mJy km s−1 beam−1 (corresponding to NHI = 7.4 × 1017 cm−2 for the original beam of FWHM = 2.9') with an increment of a factor of 2.
HI spectra of two newly detected HI sources (NGC 7320a and Anon 7) in the SQ neighborhood.
Optical spectrum of NGC 7320a obtained at Lijiang 2.4 meter telescope. The vertical dotted lines mark the positions of corresponding emission/absorption lines redshifted according to the best-fit redshift z = 0.02243 (v = 6729 km s−1).
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Xu, C.K., Cheng, C., Appleton, P.N. et al. A 0.6 Mpc H i structure associated with Stephan’s Quintet. Nature 610, 461–466 (2022). https://doi.org/10.1038/s41586-022-05206-x