# First images of Antares photosphere from spectropolarimetry

Quentin Pilate, Eric Josselin, Agnès Lèbre, Arturo López Ariste, Philippe

Mathias, Alexis Lavail

► To cite this version:

Quentin Pilate, Eric Josselin, Agnès Lèbre, Arturo López Ariste, Philippe Mathias, et al. First images of Antares photosphere from spectropolarimetry. Astronomy & Astrophysics - A&A, 2025, 700, pp.A151. 10.1051/0004-6361/202555491. hal-05162368

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Submitted on 14 Aug 2025

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# First images of the Antares photosphere from spectropolarimetry

Q. Pilate<fnref n="1" />,*, E. Josselin<fnref n="2" />, A. Lèbre<fnref n="2" />, A. López Ariste<fnref n="1" />, Ph. Mathias<fnref n="3" />, and A. Lavail<fnref n="1" />

Received 12 May 2025 / Accepted 8 July 2025

## ABSTRACT

**Aims.** Antares is the closest red supergiant (RSG) to Earth. The discovery of linear polarization in the atomic lines of the star opens the path to producing direct images of the photosphere, and hence probing the dynamics at the surface.

**Methods.** We analyze this linear polarization signals following the same scheme as has been previously done for the RSG Betelgeuse, and find that they are comparable in all its details. This allows us to use the same models for the analysis of these polarization signals in both stars.

**Results.** We find that, as in Betelgeuse, the linear polarization signal of Antares is due to the depolarization of the continuum, combined with brightness inhomogeneities. This allows us to produce images of the photosphere of the star. We show that in Antares convective cells can last several months and that the largest ones can occupy roughly 30% of the stellar radius.

**Key words.** stars: individual: Antares – supergiants

## 1. Introduction

Red supergiants (RSGs) are among the brightest stars in the universe. Those cool evolved stars are able to enrich the interstellar medium through their stellar winds. However, the underlying mechanisms that trigger mass loss in RSGs are still poorly known.

Recently, a new technique to study RSGs was used for Betelgeuse. This technique consists of studying the linear polarization profile of the spectral lines of the star. This allowed Aurière et al. (2016) to map bright spots at the surface. Later on, López Ariste et al. (2018) produced images of the photosphere and followed the time evolution of its surface convection. This new technique of imaging through spectropolarimetry requires the mechanism responsible for the formation of linear polarization to be studied. In the case of Betelgeuse, the linear polarization signal was attributed to depolarization of the continuum by the atomic lines that absorb the light from a continuum polarized by Rayleigh scattering, and re-emit this light unpolarized (Aurière et al. 2016). The depolarization produces an azimuthal symmetry, so that after integration over an uniform disk, any polarization signal would be canceled out. Thus, another mechanism that is able to break the spherical symmetry was invoked through the brightness of large convective cells, present at the surface of RSGs, as was mentioned by Schwarzschild (1975) and confirmed by observations (Montargès et al. 2016) and numerical simulations (Freytag et al. 2002; Chiavassa et al. 2022).

In this article, we propose applying this spectropolarimetric technique to the RSG Antares using spectropolarimetric data obtained at the Canada-France Hawaii Telescope (CFHT). In Sect. 2 we describe Antares. In Sect. 3, we study the linear polarization profile of Antares, from the least-squares deconvolution (LSD) profiles and from the individual lines. We take a special

look at the Na I D1 and D2 lines, which are known to depolarize the continuum and produce intrinsic polarization, respectively. We also look at the signal in the lines of Fe I, Ni I, and Ca I, which also depolarize the continuum. We then produce the first images of the photosphere of Antares in Sect. 4. In Sect. 5 we conclude our work.

## 2. Antares

Antares ($\alpha$ Sco, M1.5 Iab), with Betelgeuse, is one of the prototypical RSGs, and, at ~170 pc (van Leeuwen 2007), perhaps the nearest one. Indeed, both RSGs have similar spectral types and their positions in the HR diagram are basically identical, suggesting similar temperature and surface gravity, but also similar masses (Neuhäuser et al. 2022), keeping in mind that the distance determination of RSGs may be quite uncertain (see e.g. Harper et al. 2008). Based on the reinterpretation of antique observations, Neuhäuser et al. (2022) suggest that Betelgeuse may have been yellower about 2 millennia ago, suggesting a recent evolution toward the RSG, and that is thus younger than Antares, which has been known as a red star for at least 3 millennia. However, Saio et al. (2023) propose that Betelgeuse could be in the core-carbon burning phase, and thus at the end of the RSG phase, before explosion as a supernova. At this stage, we thus just retain that Antares and Betelgeuse are similar in mass, temperature and gravity. Contrary to Betelgeuse, Antares has a wide binary companion ($\alpha$ Sco B; B2.5 V, Johnson 1879) that is a hot main-sequence star located close to 2.73" west of the RSG (Reimers et al. 2008). The orbit is seen nearly edge on, with a period of approximately 2700 years. Such binarity allows for a fairly precise determination of the mass-loss rate, $\dot{M} = 7 \ 10^{-7} M_{\odot} \text{yr}^{-1}$ (Kudritzki & Reimers 1978). Based on ALMA and VLA observations, O’Gorman et al. (2020) studied the upper atmosphere of both RSGs and found large-scale asymmetries, as well as signs

<footnote n="1">¹ Institut de Recherche en Astrophysique et Planétologie, Université de Toulouse, UPS, CNRS, IRAP/UMR 5277, 14 avenue Edouard Belin, 31400 Toulouse, France</footnote>

<footnote n="2">² LUPM, UMR5299, CNRS and Université Montpellier, Place E.Bataillon, 34090 Montpellier, France</footnote>

<footnote n="3">³ IRAP, Université de Toulouse, CNRS, UPS, CNES, 57 avenue d'Azereix, 65000 Tarbes, France</footnote>

<footnote>* Corresponding author.</footnote>
<table><caption>**Table 1.** Log of observation of Antares with ESPaDOnS.</caption><thead><tr><th>Date</th><th>Sequence</th><th><i>B</i><sub>l</sub> (G)</th></tr></thead><tbody><tr><td>20 February 2022</td><td>2Q, 2U, 9V</td><td>+1.27 ± 0.3</td></tr><tr><td>22 February 2022</td><td>4Q, 4U, 16V</td><td>+1.14 ± 0.3</td></tr><tr><td>07 July 2022</td><td>4Q, 3U, 12V</td><td>+1.87 ± 0.3</td></tr><tr><td>11 July 2022</td><td>4Q, 4U, 11V</td><td>+1.56 ± 0.3</td></tr><tr><td>14 July 2022</td><td>4Q, 4U, 11V</td><td>+2.10 ± 0.3</td></tr><tr><td>10 February 2023</td><td>5Q, 6U, 11V</td><td>-1.99 ± 0.3</td></tr><tr><td>27 May 2023</td><td>2Q, 4U, 22V</td><td>-2.10 ± 0.3</td></tr><tr><td>24 June 2023</td><td>2Q, 2U, 20V</td><td>-1.39 ± 0.3</td></tr><tr><td>27 June 2023</td><td>4Q, 3U, 21V</td><td>-0.72 ± 0.3</td></tr><tr><td>08 July 2023</td><td>2Q, 4U, 23V</td><td>-1.28 ± 0.3</td></tr></tbody></table>

of chromospheric activity. This should be linked to the super-sonic turbulent motions found in Antares by Ohnaka et al. (2017) who question a possible mechanism in addition to convection. In addition, Montargès et al. (2017) determined the size of the con- vectorive cells at the surface of the star, which can reach up to 45% of the stellar radius.

### 3. Spectropolarimetric data

#### 3.1. Observations and data reduction

Full Stokes observations of Antares were collected from Febru-ary 2022 to July 2023 with ESPaDOnS (Donati et al. 2006), mounted at the Canada-France-Hawaii Telescope (CFHT), and thus spanning 1.5 years. Each observation consisted of four sub-exposures of 2 seconds for each Stokes parameter (*Q*, *U*, and *V*), with 4 to 6 *Q* and *U* (linear polarization) and up to 23 *V* (circu-lar polarization) observations at each date (see Table 1), ensuring spectra with a signal-to noise ratio ≥10³ per velocity bin as the signal in *V* is expected to be much weaker in the case of RSGs. The observations were unevenly spaced, in order to probe short-term (day to week) to long-term (month to year) variations. The spectra were extracted with Libre-ESPRIT (Donati et al. 1997). The extracted spectra are the normalized intensity, and Stokes *Q*, *U*, *V* as a function of wavelength. Libre-ESPRIT also provides the null spectra of the polarization signals. The null spectrum is, in principle, featureless and thus serves as a diagnostic tool for detecting spurious contributions in the polarized spectrum. Additional information about the observation and data reduc-tion methods can be found in Donati et al. (1997). A summary of the observation dates, with the corresponding polarimetric sequences, is given in Table 1.

#### 3.2. Mean profiles

The study of the polarization in the individual lines of RSGs is often difficult, since the amplitude of linear polarization is roughly 10⁻⁴ times the continuum intensity and often close to noise level. In order to increase the signal to noise ratio, Donati et al. (1997) proposed summing many individual spectral lines, through the technique of LSD. By assuming that for a given Stokes parameter, *Q* or *U* for the linear polarization, and *V* for the circular polarization, the same signal up to a scale factor is present in every line, summing up will increase the signal-to-noise ratio. This leads to LSD profiles of Stokes *I* for the intensity and Stokes *Q*, *U*, and *V* for polarization.

<figure><img src="image_2.png" /><figcaption>**Fig. 1.** Top panel: LSD profile of Antares on July 7 2022. Stokes *U* is in red, Stokes *Q* in blue, Stokes *V* in green, and Stokes *I* in black. The vertical black line represents the center of the line. Bottom panel: null profiles of Stokes *Q* in blue and *U* in red. The vertical black line depicts the velocity of the star at -4.3 km s⁻¹.</figcaption></figure>

Since Betelgeuse and Antares have similar $T_{eff}$ and $log g$, we used the same mask as the one described by Aurière et al. (2016) from the Vienna Atomic Line Database (Ryabchikova et al. 2015), with an effective temperature of 3750 K, a surface gravity $log g = 0$, and a microturbulence of 4 km s⁻¹. The mask contains about 15 000 lines, with a central depth deeper than 40% of the continuum intensity. The LSD profiles for the obser-vations of July 7 2022 is presented in Fig. 1 (upper panel). The LSD profile of Stokes *Q* is represented in blue, *U* in red, *V* in green, and Stokes *I* in black. The vertical black line depicts the velocity of the star reported by Pugh & Gray (2013) for reference, at -4.3 km s⁻¹. We see a clear linear polarization signal between -30 km s⁻¹ and 20 km s⁻¹. The amplitude of linear polarization reaches up to $2 \times 10^{-4}$ the continuum intensity, while Stokes *V* only reaches $3 \times 10^{-5}$. The null profiles of both Stokes *Q* and *U* are shown in the bottom panel, with the same color code. The null profile of Stokes *V* is not represented to avoid burdening the figure but reaches an amplitude up to $1 \times 10^{-5}$.

#### 3.3. Circular polarization

The profiles have been normalized with a depth of 0.69, an equivalent Landé factor of 1.04, and an equivalent wavelength of 850 nm. Circular (Stokes *V*, green line in Fig. 1) polariza-tion was extracted with LSD method (Donati et al. 1997) and has been detected at each date. Despite the strong linear polarization signal, no significant cross-talk has been detected. Each Stokes *V* profile exhibits the typical Zeeman shape, represented as the green line in Figure 4. For clarity, the Stokes *V* profiles have been shifted down and their amplitudes have been multiplied by a factor of 5 to better see the profiles. The detection of Stokes *V* allowed us to compute the mean longitudinal magnetic field, $B_l$, which corresponds to the line-of-sight component of the mag-netic field of the star, integrated over the stellar disk. We com-puted $B_l$ using the first-order moment of the Stokes *V* Zeeman profile (see e.g Donati et al. 1997; Wade et al. 2000). We nor-malized the LSD profile using an average depth of 0.69, a mean Landé factor of $g_{eff} = 1.04$, and a mean wavelength of 850 nm. The corresponding longitudinal fields are given in Table 1.

The intensity reaches $
 \approx 2$ G, comparable to the one detected toward Betelgeuse (Mathias et al. 2018). With an
uncertainty of ~0.3 G, no significant variations on timescales ≲ a week are seen. A polarity reversal occurred around the end of 2022, suggesting a timescale of variation of ~2 years.

The generation of a magnetic field in RSGs, which are very slow rotators and thus have very high Rossby numbers is puzzling. However, (Amard et al. 2024) have shown that a genuine dynamo can occur in low-gravity, fully convective stars. The ridges of the magnetic field are then aligned with the edges of the convective cells. Furthermore, their simulations show reversals of the field on timescales of a couple of years, consistent with the reversal observed for Antares.

### 3.4. Interpretation of linear polarization

To correctly interpret the origin of those linear polarization signals, it is worth studying the polarization signal in the individual lines in the spectrum of Antares. Several mechanisms can produce linear polarization, while Stokes V is almost uniquely related to the magnetic field and is routinely used to detect and map stellar magnetic fields (e.g. Donati & Landstreet 2009). Linear polarization due to the Zeeman effect is roughly one order of magnitude smaller than Stokes V, but in Antares the linear polarization amplitude is ten times higher than the Stokes V signal (green line in Fig. 1), excluding any Zeeman origin of the linear polarization signal. Other mechanisms known to produce linear polarization in individual lines are found in the second solar spectrum (Stenflo & Keller 1997). One is the depolarization of the continuum by atomic lines. In the Sun, roughly 90% of the lines depolarize the continuum. In the case of Betelgeuse, this mechanism was found to explain the origin of all linear polarization signals in atomic lines (Aurière et al. 2016). Another mechanism is in the emission of polarized light: what we refer to as intrinsic polarization. While most of the lines are able to depolarize the continuum, only a small fraction of them can produce intrinsic polarization. This mechanism dominates the linear polarization of atomic lines in the spectrum of the Mira star χ Cyg (López Ariste et al. 2019). However, because of the similarities with Betelgeuse, we explore the continuum depolarization as the primary mechanism for the observed signals in Antares, following Aurière et al. (2016).

One way to distinguish signals due to continuum polarization from intrinsic polarization is to look at the Na I lines D1 and D2. D1 cannot produce intrinsic polarization, while D2 can (Stenflo & Keller 1997; Landi Degl'Innocenti & Landolfi 2004). In Betelgeuse, D1 and D2 clearly exhibit a similar amplitude in the linear polarization signals. Hence, Aurière et al. (2016) attributed this linear polarization signal to depolarization of the continuum. If we observe a polarization signal in D1 similar to that of D2 in the lines of Antares, the situation would be analogous to Betelgeuse. Figure 2 depicts the spectrum of Antares around the Na I doublet. The upper panel shows the intensity profile, while the lower panel shows Stokes *U* in red and Stokes *Q* in blue. The amplitude of linear polarization in the individual lines being small, we added up the observations between July 7 2022 and July 14 2022. As will be shown in Sect. 4, the LSD profiles of Stokes *Q* and *U* do not significantly change within one week, allowing us to sum the profiles. The whole set consists of an average of thirteen *Q* and *U* profiles (see log of observations in Table 1). Note that we computed the average of the polarization signal within a range of 10⁻² nm. Indeed, at those wavelengths and with the spatial resolution of ESPaDOnS being R=68 000, Δλ = λ/R ~ 10⁻² nm, which allowed us to better see the profiles. D1 and D2 seem to produce a similar polarization profile, which is above the noise level. The two profiles show a positive

<figure><img src="image_3.png" /><figcaption>**Fig. 2.** Polarized spectrum of Antares around Na I D1 and D2 lines. The upper panel depicts the intensity profile. The lower panel shows the linear polarization signal, with Stokes *Q* in blue and Stokes *U* in red. The vertical lines are the center of the lines D1 and D2, corrected from the Doppler velocity of -4.3 km s⁻¹.</figcaption></figure>

<figure><img src="image_4.png" /><figcaption>**Fig. 3.** Intensity spectra around the Fe I, Ni I, and Ca I lines (upper panel) and linear polarization spectrum in the lower panel, with Stokes *Q* in blue and Stokes *U* in red. The vertical lines represent the wavelength of the lines corrected with a Doppler shift of -4.3 km s⁻¹.</figcaption></figure>

lobe in *U* and a negative one in *Q* in the blue wing of the line, and vice versa in the red wing of the line, altogether with similar amplitudes. The Na I D1 and D2 lines have been widely studied (e.g., Belluzzi et al. 2015, and references therein), and the quantitative description of those lines is particularly hard. We thus restricted our analysis to the overall shape and amplitude of the Na I lines. From this similarity of profile shapes and amplitudes, we attribute the linear polarization in Antares to depolarization of the continuum.

To ensure that the same linear polarization signal is present in the individual lines in Antares, we followed Aurière et al. (2016) in looking at the polarization signal in lines that are known to depolarize the continuum in the Sun (Gandorfer 2000); namely, Fe I, Ni I, and Ca I at 558.7 nm, 558.8 nm, and 558.9 nm, respectively. Once again, in Betelgeuse those lines exhibit a similar shape to the one of the LSD profile. Figure 3 shows the intensity profile around those lines (upper panel) and the linear polarization in the lower panel, altogether with the center of the lines, Doppler-shifted from their rest positions. As for the D1 and D2 lines, we computed the average of linear polarization per bin of 10⁻² nm, to better see the signal. Within the confidence limits given by the signal-to-noise ratios, the signals detected for them
<figure><img src="image_5.png" /><figcaption>**Fig. 4.** LSD profiles of Stokes Q in blue and U in red. The red and blue lines represent the brightness distribution that better fits the observed profile. The observation dates are given in the bottom right of the figure. Stokes V is represented in green and has been shifted down and had its amplitude multiplied by 5 so that the profiles can be seen better. The vertical dashed lines represent, from left to right, the velocity, $v_0$, and the velocity of the star, $v_*$, adopted in our model.</figcaption></figure>

are similar and also similar to the signal extracted by the LSD procedure in Fig. 1, which justifies a posteriori our the choice of adding up the lines. Those three lines being known to depolarize the continuum, and since the shape of the LSD profile and the shape of those individual lines are the same, we conclude that the linear polarization signal present in Antares is due to the depolarization of the continuum, and that we can add up the lines, independently of their physical properties.

# 4. Imagery of the stellar photosphere

## 4.1. LSD profiles and evolution

Figure 4 shows the LSD profiles of Antares from February 2022 to July 2023. Once again, the red and blue dots represent Stokes *U* and *Q*, respectively, the green line being Stokes *V*, shifted down and having had its amplitude multiplied by 5 for clarity. The log of observations for the different dates in presented in Table 1. The solid lines are the fits of the profiles, which we describe in next subsection. The similarities of Antares with Betelgeuse continue: the LSD profiles seem to reach an amplitude between $2-4 \times 10^{-4}$ the continuum intensity, which is roughly the same order of magnitude as in Betelgeuse. The LSD profiles vary within a span of a week to a month, which is clear between May 27 2023 and June 24 2023, where the amplitude of

Stokes *Q* (blue line) is increasing in the blue wing. We also pinpoint that the shape of the LSD profiles between July 7 and July 14 2022 does not change significantly. This justifies our addition of lines in Sect. 3.4, since the same polarization signal is present in every observation. We did not represent the intensity profile in Fig. 4 to avoid overcrowding the figure. However, it is worth comparing it to the one of Betelgeuse and other RSGs. In Fig. 1, the intensity profile is narrow compared to the polarization profile. In particular, in the blue wing of the profile, around $-25 \text{ km s}^{-1}$, there is a strong polarization signal, which falls in the continuum of the line. This behavior is present in every LSD profile, but it is also present in Betelgeuse and other RSGs, such as $\mu$ Cep or CE Tau, and was attributed to velocity gradients, which narrow the intensity profile after disk integration (López Ariste et al. 2025).

## 4.2. Images of the photosphere

We found that the linear polarization signal in Antares is the same in every line. Furthermore, the polarization signal was attributed to the depolarization of the continuum by the atomic lines present in the photosphere. We recall that the depolarization of the continuum produces an azimuthal symmetry; hence, after integration over the stellar disk, any polarization signal would be canceled out. Thus, we have to introduce a mechanism
that breaks the symmetry of the disk. In RSGs, the large con-
 vective cells theorized by Schwarzschild (1975) were used by
Aurière et al. (2016) to explain the breaking of symmetry over the
disk. This allowed López Ariste et al. (2018) to produce images
of Betelgeuse. All the similarities pointed out above between
Antares and Betelgeuse lead us to apply the same models here
to produce images of the photospheric brightness distribution of
Antares. Before going any further, we recall the imaging tech-
nique. The technique involves finding the brightness distribution
that better fits the observed LSD profiles. The imaging technique
also requires the introduction of two velocities. First is the max-
imum velocity of the rising plasma. Since we assume that most
of the photons that we receive come from hot rising plasma, we
chose an ad hoc velocity, $v_0$, which is the maximum velocity of
the rising plasma. This velocity was chosen by assuming that no
polarization signal can be blueshifted compared to this veloc-
ity. We chose a value of -45 km s⁻¹, consistent with the work
of Ohnaka et al. (2017), who found a similar velocity amplitude
in the outer layers of Antares. The second velocity is the veloc-
ity of the star, $v_★$. It is tempting to choose the classical value of
-4.3 km s⁻¹ (Pugh & Gray 2013), which represents the center of
the line, and which is represented in Fig. 1. However, in RSGs,
the shape of the intensity line is not symmetric, as was pointed
out by Josselin & Plez (2007). In RSGs such as Betelgeuse, the
line exhibits the classical C-shape bisector, associated with con-
vection. The same behavior is also present in Antares. Therefore,
in RSGs, the velocity of the star lies in the red wing of the line
(López Ariste et al. 2018). Hence, we chose $v_★$ = 15 km s⁻¹,
and altogether, in the heliocentric reference frame of the LSD
profiles, $v_0$ is at -30 km s⁻¹. As is discussed in López Ariste
et al. (2018), each point in the disk was supposed to emit a Gaus-
sian profile, with a full width at half maximum of 10 km s⁻¹, to
take into account instrumental width, thermal broadening, and
macroturbulence.

Figure 5 shows the images of the photosphere of Antares,
from February 2022 to July 2023. The associated Stokes pro-
files of each image are represented with solid lines in Fig. 4,
where it is clear that the reconstructed images fit the data points
well. In every image, the brightness has been normalized. The
brightness distribution was modeled using spherical harmonics
up to $l_{max} = 5$ (López Ariste et al. 2018). As in López Ariste
et al. (2022), the brightness is correlated with velocity: 75% of
the plasma is moving upward, while 25% is falling toward the
star. The higher the brightness, the faster the plasma is moving
upward. Therefore, the dark areas in the images represent the
zones where the plasma is falling toward Antares. Looking at the
images, the brightness distribution changes with a span of a sev-
eral months. The convective cell near the disk center is consistent
with the $v_0$ that we chose, since the peak in linear polarization is
close to this velocity. The central convective cell is present for
at least one year, which is consistent with numerical simulations
(Freytag et al. 2002), in which the large convective cells have a
typical lifetime of around two years. In February 2023, another
large convective cell appears in the southwestern hemisphere.
This is consistent with the LSD profile at the same date, where a
strong polarization signal appears in Stokes Q. Since the peak is
located closer to our ad hoc velocity of the star, it appears closer
to the stellar limb. Overall, our images exhibit between one (July
2022) and three (June 2023) convective cells, once again, consis-
tent with numerical simulations and theory (Schwarzschild 1975;
Freytag et al. 2002). The convective cells reach up to 30% of the
stellar radius in size in our images. This size was estimated by
computing the area of the largest convective cell on the image

<figure><img src="image_6.png" /><figcaption>**Fig. 5.** Images of Antares. North is up, east is left. In each image, the brightness is normalized.</figcaption></figure>

obtained July 8 2023, located in the northeastern hemisphere of
the star.

As with the analogous images in Betelgeuse, a word of caution is required: one must not overinterpret those images. Linear polarization carries a 180° ambiguity; thus, every image can be rotated by 180° and the brightness distribution will still fit the observed profile. Combining both spectropolarimetry and interferometry allows us to avoid any ambiguity. Despite those ambiguities, the overall position of the convective cell should be correct, within a 180° ambiguity. To avoid any ambiguities in the reconstruction of the images, for a given day, we used the brightness distribution found in the previous observation to fit the observed linear polarization profile. This ensures continuity between the images. Such a technique was also used by López Ariste et al. (2018) to follow the surface convection of Betelgeuse.

**5. Conclusion**

The RSG Antares exhibits a strong linear polarization signal. This signal has an amplitude ten times higher than the Stokes V signal, excluding any Zeeman origin of the linear polarization. Looking at the Na I D1 and D2 lines, we have found that both lines show a clear polarization signal. The D1 line can only depolarize the continuum, while D2 can produce intrinsic polarization. By studying the three lines Fe I, Ni I, and Ca I,
which are known to depolarize the Sun's continuum (Gandorfer 2000), we have shown that a clear linear polarization appears in those lines, and that the shape of the profile is the same as the one observed in the LSD profile. Hence, we have been able to affirm that the linear polarization that we observed in Antares is due to the depolarization of the continuum by the atomic lines present in the photosphere. All these facts from Antares are perfectly comparable to those of Betelgeuse (López Ariste et al. 2018) and we were able to apply the same techniques and produce the first images of the brightness distribution in the photosphere of Antares at different epochs and track its surface convection. The velocity span observed in the linear polarization seems to be comparable to the velocity amplitude given by Ohnaka et al. (2017). The size and the number of cells are consistent with the work of Schwarzschild (1975). The technique of spectropolarimetry imaging was successfully applied to Antares, and can be extended to other RSGs, as long as their lines depolarize the continuum. This technique has to be combined with other techniques of imaging, such as interferometry, to avoid any ambiguity in the reconstructed images.

*Acknowledgements.* This work was supported by the "Programme National de Physique Stellaire" (PNPS) of CNRS/INSU co-funded by CEA and CNES. We acknowledge support from the French National Research Agency (ANR) funded project PEPPER (ANR-20-CE31-0002).

## References

* Amard, L., Brun, A. S., & Palacios, A. 2024, ApJ, 974, 311

* Aurière, M., López Ariste, A., Mathias, P., et al. 2016, A&A, 591, A119

* Belluzzi, L., Trujillo Bueno, J., & Landi Degl'Innocenti, E. 2015, ApJ, 814, 116

* Chiavassa, A., Kudritzki, R., Davies, B., Freytag, B., & de Mink, S. E. 2022, A&A, 661, L1

* Donati, J. F., & Landstreet, J. D. 2009, ARA&A, 47, 333

* Donati, J. F., Semel, M., Carter, B. D., Rees, D. E., & Collier Cameron, A. 1997, MNRAS, 291, 658

* Donati, J. F., Catala, C., Landstreet, J. D., & Petit, P. 2006, ASP Conf. Ser., 358, 362

* Freytag, B., Steffen, M., & Dorch, B. 2002, Astron. Nachr., 323, 213

* Gandorfer, A. 2000, The Second Solar Spectrum: A high spectral resolution polarimetric survey of scattering polarization at the solar limb in graphical representation. Volume I: 4625 Å to 6995 Å (Zurich: vdf ETH)

* Harper, G. M., Brown, A., & Guinan, E. F. 2008, AJ, 135, 1430

* Johnson, S. J. 1879, The Observatory, 3, 84

* Josselin, E., & Plez, B. 2007, A&A, 469, 671

* Kudritzki, R. P., & Reimers, D. 1978, A&A, 70, 227

* Landi Degl'Innocenti, E., & Landolfi, M. 2004, Polarization in Spectral Lines (Berlin: Springer), 307

* López Ariste, A., Mathias, P., Tessore, B., et al. 2018, A&A, 620, A199

* López Ariste, A., Tessore, B., Carlín, E. S., et al. 2019, A&A, 632, A30

* López Ariste, A., Georgiev, S., Mathias, P., et al. 2022, A&A, 661, A91

* López Ariste, A., Pilate, Q., Lavail, A., & Mathias, P. 2025, A&A, 699, A161

* Mathias, P., Aurière, M., López Ariste, A., et al. 2018, A&A, 615, A116

* Montargès, M., Kervella, P., Perrin, G., et al. 2016, A&A, 588, A130

* Montargès, M., Chiavassa, A., Kervella, P., et al. 2017, A&A, 605, A108

* Neuhäuser, R., Torres, G., Mugrauer, M., et al. 2022, MNRAS, 516, 693

* O'Gorman, E., Harper, G. M., Ohnaka, K., et al. 2020, A&A, 638, A65

* Ohnaka, K., Weigelt, G., & Hofmann, K. H. 2017, Nature, 548, 310

* Pugh, T., & Gray, D. F. 2013, AJ, 145, 38

* Reimers, D., Hagen, H.-J., Baade, R., & Braun, K. 2008, A&A, 491, 229

* Ryabchikova, T., Piskunov, N., Kurucz, R. L., et al. 2015, Phys. Scr, 90, 054005

* Saio, H., Nandal, D., Meynet, G., & Ekström, S. 2023, MNRAS, 526, 2765

* Schwarzschild, M. 1975, ApJ, 195, 137

* Stenflo, J. O., & Keller, C. U. 1997, A&A, 321, 927

* van Leeuwen, F. 2007, A&A, 474, 653

* Wade, G. A., Donati, J. F., Landstreet, J. D., & Shorlin, S. L. S. 2000, MNRAS, 313, 851