The GAPS Programme at TNG ⋆ XXXVI. Measurement of the Rossiter-McLaughlin effect and revising the physical and orbital parameters of the HAT-P-15, HAT-P-17, HAT-P-21, HAT-P-26, HAT-P-29 eccentric planetary systems

Context. The measurement of the spin-orbit alignment of hot Jupiters, with a range of orbital and physical properties, can provide information about the evolution of the orbits of this special class of giant planets. Aims. We aim to reﬁne the orbital and physical parameters and determine the sky-projected planet orbital obliquity, λ , of ﬁve eccentric ( e and conﬁrmed that the HAT-P-26 system shows transit timing variations, which may tentatively be attributed to the presence of a third body.


Introduction
In more than 20 yr of exciting research, exoplanetary science has given many surprises for viewpoints based on our own Solar system. One major surprise came early in the development of this field: the small orbital distances and sometimes Photometric and RV data are only available at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http: //cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/664/A162 Based on observations made with the Italian Telescopio Nazionale Galileo (TNG) operated by the Fundación Galileo Galilei (FGG) of the Istituto Nazionale di Astrofisica (INAF) at the Observatorio del Roque de los Muchachos (La Palma, Canary Islands, Spain). Furthermore, the orbits of these giant planets should be roughly circular. This is because the effective frictional force, which exists for planets that are orbiting within a massive disk of gas and dust, tend to circularise any orbits, even though they are initially eccentric (see e.g. Raymond & Morbidelli 2022).
Instead, observational results show there are a lot of giant planets with eccentric orbits and located very close to their stars. These planets, which are known as hot Jupiters, are very easy to detect via transit and radial-velocity (RV) methods, and their origin has been one of the main topics of discussion in planetary science for the last 20 yr. They most likely formed at large distances from their star, as did Jupiter in the Solar system, but then, through some physical mechanism, they have migrated towards the innermost regions. Different mechanisms have been proposed that are able to shrink the orbit of a giant planet. The main ones among them are based on: (i) dynamical interactions through planet-planet scattering (Rasio & Ford 1996;Davies et al. 2014) or the Kozai mechanism (see e.g. Wu & Murray 2003), and (ii) disc-planet interaction (Lin et al. 1996;Ward 1997).
To determine which of the two theories is the correct one, or at least the most efficient, we may examine how several parameters are distributed, such as the metallicity of the parent stars (see e.g. Dawson & Murray-Clay 2013) or the eccentricity and the orientation of the planetary orbits of hot Jupiters (see e.g. Matsumura et al. 2010). For example, it is expected that scattering encounters among planets should randomise the alignments of the orbital planes. Instead, if the existence of hot Jupiters is to be primarily ascribed to disc-planet interactions, we should see many flat architectures, as this mechanism keeps the planetary orbits coplanar throughout the entire migration process. Numerical simulations support these predictions (e.g. Chatterjee et al. 2008;Marzari & Nelson 2009).
Whenever a giant planet undergoes orbital migration, the responsible mechanism is expected also to affect the eccentricity, e, and/or the angle, ψ, between the planet's orbital axis and its host star's spin. Several authors have dealt with this question based on the available data (e.g. Bonomo et al. 2017;Wang et al. 2021;Rice et al. 2021Rice et al. , 2022, but it is still not clear what the degree of correlation between these two parameters is and how much tidal interactions intervene to complicate the interpretation, as recently pointed out by Albrecht et al. (2022). Therefore, new measurements of the spin-orbit alignments are useful for enlarging the sample of exoplanetary systems in order to perform robust statistical analyses and shed new light on what the real cause of the giant-planet migration process is.
While the measurement of ψ is, unfortunately, not easy to determine, its sky-projected value, λ, can be easily measured for systems containing transiting hot Jupiters, via the observation of the Rossiter-McLaughlin (RM) effect or from star-spot tracking in consecutive transit light curves. Once λ is known, we can derive the true alignment of the projected rotational velocity of the parent star, v sin i. If its radius is also known, its rotation period can be measured as well.
The long-term observational programme GAPS (Global Architecture of Planetary Systems) utilises the HARPS-N spectrograph, at the 3.5 m Telescopio Nazionale Galileo (TNG), to execute a study of the spin-orbit alignment of a sample of known transiting exoplanetary systems for measuring the RM effect (Covino et al. 2013). We took advantage of the high spectral resolution of HARPS-N for targeting faint stars (up to V < 14 mag), for which the RM effect is harder to measure at the required level of accuracy (Esposito et al. 2014(Esposito et al. , 2017Mancini et al. 2015Mancini et al. , 2018. Photometric follow-up observations with an array of medium-class telescopes support our programme. The aim is to obtain high-quality light curves of planetary-transit events to refine the whole set of physical and orbital parameters of the planetary systems in our target list. High-quality light curves also allow us to detect possible features of the transit light curve, which can be associated with stellar activity (e.g. Mancini et al. 2017), as well as transit timing variations (TTVs).
In this work, we present new measurements of the RM effect for five exoplanetary systems. They have been selected considering the effective temperature of their parent stars, which have 5100 K < T eff < 6200 K and the eccentricity of the planetary orbits, which are 0.1 < e < 0.3. We can divide these systems in two groups. Each of the stars of the first group hosts a hot Jupiter (HAT-P-15 b, HAT-P-17 b, HAT-P-21 b and HAT-P-29 b), whose orbital eccentricity is larger than zero at 3 σ confidence level, as estimated by Bonomo et al. (2017). The second group includes only one system, in which there is a Neptune-mass planet, HAT-P-26 b, whose eccentricity was estimated larger than zero at 2 σ confidence level by Hartman et al. (2011). For the planets in the first group, we were able to measure the orbital obliquity, but we did not detect any TTVs. For HAT-P-26, we were not able to deduce a precise value for λ, but we detected a TTV.
The paper is organised as follows. In Sect. 2, we describe the systems that are the subject of this study. Spectroscopic and photometric observations and data reduction procedures are presented in Sect. 3. Section 4 is devoted to the light curve analysis. The results of the analysis of the HATNet time-series photometric data are reported in Sect. 6. An analysis of the stellar parameters, based on archival data, is performed in Sect. 7. The stellar atmospheric properties and activity of the stars, based on HARPS-N data, and the measurements of the spin-orbit alignment angle for each of the systems are presented in Sect. 8. The results of the analysis aimed at refining the physical parameters of the systems are reported in Sect. 9. Finally, Sect. 10 contains the discussion, while the main results of this work are summarised in Sect. 11.

Targets properties
In this section, we summarise the main properties of the five planetary systems that are the subject of this study. The values of the parameters were taken from the Transiting Extrasolar Planet Catalogue (TEPCat 1 ) and are also given in Tables D.1-D.5. Kovács et al. (2010) reported the discovery of HAT-P-15 b, a giant planet (M p = 1.946 ± 0.066 M Jup ; R p = 1.072 ± 0.043 R Jup ) on an eccentric orbit (e = 0.190 ± 0.019) of period P orb ∼ 10.9 days, transiting a G5 V dwarf star (V = 12.16 mag, M = 1.013 ± 0.043 M , R = 1.080 ± 0.039 R , T eff = 5568 ± 90 K). − Lucky images, which were taken with the AstraLux Norte at the Calar Alto 2.2 m telescope, show two faint objects at separation of 6.2 and 7.1 arcsec, respectively . Further observations will be needed to confirm whether these objects are physically associated with HAT-P-15. − The Gaia EDR3 catalogue (Gaia Collaboration 2016, 2021 also reports two objects at a separation of ∼7 arcsec with ∆g ∼ 7 mag; only one of them has a parallax entry that allows us to exclude it as a physical companion. − Piskorz et al. (2015) analysed NIRSPEC@Keck K-band spectra of HAT-P-15 and did not find evidence of a close redder stellar companion. Subsequent studies of this system (Bonomo et al. 2017;Stassun et al. 2017) confirmed the original estimates of its main physical parameters as reported by Kovács et al. (2010).

HAT-P-17
HAT-P-17 b is a giant planet (M p = 0.54 ± 0.02 M Jup ; R p = 1.04 ± 0.02 R Jup ) on an eccentric orbit (e = 0.3417 ± 0.0036), with period P orb ∼ 10.3 days and hosted by a relatively bright early K V dwarf star (V = 10.54 mag, M = 0.88 ± 0.04 M , R = 0.84 ± 0.01 R , T eff = 5322 ± 55 K; Howard et al. 2012). − In ∼50 HIRES-RV measurements spanning from October 2007 to August 2013 (Fulton et al. 2013;Knutson et al. 2014), evidence was found for the presence of another long period planetary companion, HAT-P-17 c, with P orb ≈ 10 to 36 yr, m sin i ≈ 3.4 M Jup , and e ≈ 0.4. Fulton et al. (2013) also measured the projected obliquity of planet b, finding λ = 19 +14 −16 , a value which is consistent with zero. − Bonomo et al. (2017) reported an additional 25 RV measurements taken with HARPS-N from October 2012 to November 2015. With a combined fit of the HIRES and HARPS-N RV data sets, they put more stringent constraints on the HAT-P-17 c parameters: P orb = 3972 +185 −146 days; e = 0.295 ± 0.021; m sin i = 2.88 ± 0.10 M Jup ; a = 4.67 ± 0.14 au. − K-band AO images, taken with the NIRC2 at Keck II (Fulton et al. 2013;Ngo et al. 2015), ruled out the existence of companions with ∆K < 7 mag for separations beyond 0.7 arcsec (65 au according to the Gaia parallax). −  observed HAT-P-17 with AstraLux Norte in the i and z passbands. They found no close companions, and reported 5σ detection limits of ∆z = 3. 84, 4.95, 6.29, 7.09 mag at 0.25, 0.5, 1.0, 2.0 arcsec, respectively. − Similar detection limits in the K s band were reported by Adams et al. (2013), who used ARIES at the MMT telescope. − Piskorz et al. (2015) used high-resolution K-band spectra, taken with NIRSPEC@KECK, to search for blended lines from cool stellar companions. They found that the spectral fit is significantly improved by the presence of a 3900 +200 −300 K companion in the HAT-P-17 system at a maximum separation of 36 au.

HAT-P-21
The exoplanet HAT-P-21 b was discovered by Bakos et al. (2011) to be a massive hot Jupiter (M p = 4.063 ± 0.161 M Jup ; R p = 1.024 ± 0.092 R Jup ) moving on a short-period and eccentric orbit (P orb ∼ 4.1 days; e = 0.228 ± 0.016) around a G3 V star (V = 11.69 mag, M = 0.947 ± 0.042 M , R = 1.105 ± 0.083 R , T eff = 5588 ± 80 K). − The values of the main physical and orbital parameters of this system reported in the discovery paper are in a good agreement with those from subsequent studies (Torres et al. 2012;Bonomo et al. 2017;Stassun et al. 2017). − For this star, 15 high-precision RV measurements were obtained with the HIRES@KECK I (from May 2009 to February 2010). K-band images, obtained with the NIRC2 at Keck II (Ngo et al. 2016), showed no evidence of bound companions. High-resolution Lucky-Imaging observations made with the AstraLux Norte camera also did not reveal the presence of any companions . − The Gaia EDR3 catalogue reports no objects close to HAT-P-21 within 10 arcsec.

HAT-P-26
The discovery of the HAT-P-26 planetary system was announced by Hartman et al. (2011). It consists of a low-density Neptunemass planet (M p = 0.059 ± 0.007 M Jup ; R p = 0.565 +0.072 −0.032 R Jup ) transiting a K1 V dwarf star (V = 11.74 mag, M = 0.816 ± 0.033 M , R = 0.788 +0.098 −0.043 R , T eff = 5011 ± 55 K) with a period of P orb ∼ 4.23 days. The orbit of this planet is also eccentric, with e = 0.124 ± 0.060. − 12 RV measurements were obtained for this star with the HIRES@KECK I between December 2009 and June 2010 . A further 11 were obtained between December 2011 and June 2012 (Knutson et al. 2014). − High-resolution Lucky-Imaging observations performed with the AstraLux Norte camera did not reveal close-in bound companions . − Indications of TTVs in the system, with an amplitude of 4 min and a periodicity of 270 epochs, were observed by von Essen et al. (2019). − Much more precise measurements of the physical parameters for this system have not been obtained by other authors (Torres et al. 2012;Mortier et al. 2013;Stassun et al. 2017). − Detailed studies of the atmosphere of HAT-P-26 b have been conducted via transmission spectroscopy Wakeford et al. 2017;MacDonald & Madhusudhan 2019). − The Gaia EDR3 catalogue reports no objects close to HAT-P-26 within 10 arcsec.

HAT-P-29
The HAT-P-29 planetary system is composed of a hot Jupiter (M p = 0.767 +0.047 −0.045 M Jup ; R p = 1.064 +0.075 −0.068 R Jup ), orbiting an F8 V star (V = 11.90 mag, M = 1.199 +0.063 −0.061 M , R = 1.237 +0.077 −0.071 R , T eff = 6115 ± 86 K) every ∼5.72 days (Buchhave et al. 2011). − 8 RV measurements were obtained for this star with the HIRES@KECK I between September and December 2010 (Buchhave et al. 2011). Joining these measurements with four others, which were taken with the same instrument between February and August 2012, Knutson et al. (2014) found a trend in the RV data and, hence, evidence for a companion in this system. −  found a stellar source 3.3 away from HAT-P-29, using the AstraLux Norte camera. − Ngo et al. (2016) confirmed the latter discovery with NIRC2 and found that this source is consistent with a bound stellar companion. − With 25 high-precision HARPS-N RVs, Bonomo et al. (2017) did not detect any significant trend that can be consistent with the RV drifts found by Knutson et al. (2014), but they found a significant (5.8σ) small eccentricity (e ≈ 0.1) for the orbit of HAT-P-29 b.
A162, page 3 of 31 A&A 664, A162 (2022) − The measurement of the orbital period of HAT-P-29 b was recalculated thanks to new transit light curves, finding that it is ≈ 17.6 s longer than the previous measurement. No statistically significant TTVs were found (Wang et al. 2018). − The Gaia EDR3 catalogue (Gaia Collaboration 2016, 2021 reports a faint (G = 17.8 mag) object at a separation of 3.43 arcsec from HAT-P-29. However, the parallax of this object indicates a distance roughly 30 times greater than that of HAT-P-29, excluding the possibility of it being a physical companion.

Observations and data reduction
In this section we present new times-series spectroscopic data of HAT-P-15, HAT-P-17, HAT-P-21, HAT-P-26 and HAT-P-29, as well as new photometric follow-up observations with TESS and ground-based telescopes.

HARPS-N spectroscopic observations
All the spectra analysed in this work were acquired with the High Accuracy Radial velocity Planet Searcher -North (HARPS-N; Cosentino et al. 2012) spectrograph at the Italian Telescopio Nazionale Galileo (TNG). The log of the HARPS-N observations is given in Table 1. HARPS-N provides high resolution spectra (R ∼ 115 000) spanning almost the entire optical range (λ = 383-690 nm), and was designed to deliver very precise stellar RVs (Cosentino et al. 2014). HARPS-N is equipped with its own Data Reduction Software (DRS) that, in addition to 1-D wavelength-calibrated spectra, provides RVs, which are calculated by cross-correlating the spectra with a numerical mask (Baranne et al. 1996;Pepe et al. 2002;Lovis & Pepe 2007) and line bisectors. The DRS also measures the Mount Wilson S index and, if the stellar B − V colour index is lower than 1.2, also the log(R HK ) chromospheric activity index (Lovis et al. 2011). Specifically, we utilised the latest version of the DRS available offline at the Italian center for Astronomical Archives (IA2) (Smareglia et al. 2014).
HAT-P-15. was observed on the night of 2015/11/16, during a planetary transit. A time series of 33 spectra covered the 5.5 h long transit from 0.9 h before ingress to 1.8 h after egress (see Table 1). With an exposure time of 900 s, the spectra have an average signal-to-noise ratio of 30 (S/N per pixel in 1-D spectra at 5500 Å). The RV measurements were obtained using the G2 numerical mask. They are reported in Table A.1 and plotted in Fig. 1.
HAT-P-17. was observed on the night of 2013/10/13, during a planetary transit. The acquisition series started before nautical twilight, while the last spectrum was taken 1.9 h after the end of the transit, when the star was at an airmass of ∼1.7. During the night ∼73% of the moon was illuminated and it was at an angular separation of ∼41 • from the target; we checked that no significant light contamination was present by analysing the spectra and the CCFs of the second fibre which was pointed at the sky. The resulted spectra have an average S/N of 60 (per pixel in 1-D spectra at 5500 Å) and a G2 mask was used to measure the RVs. They are reported in Table A.2 and plotted in Fig. 2.
HAT-P-21. was observed on the night of 2014/03/07. A timeseries of 36 spectra, lasting over 6 h, bracketed a planetary transit from ∼80 min before the ingress up to ∼40 min after the egress. With an exposure time of 600 s, the spectra have a typical S/N of 20 (per pixel in 1-D spectra at 5500 Å). However the last 2 h of observations were affected by passing clouds, so some spectra have much lower S/N and large RV uncertainties. The RV values were obtained using a G2 mask; they are reported in Table A (Fulton et al. 2013). Note that the two circled data points were considered outliers (they showed residuals larger than 4 σ and, therefore, were not considered in the modelling process). Black points are the HARPS-N RVs (this work). The best-fitting values of the systemic RVs were subtracted in order to compare the two data sets. The red line represents the best-fitting model of the RM effect; the RV residuals are plotted in the lower panel. Right-hand panels: same as left panels but with the RM effect and CB effect modelled simultaneously (green-dashed line). HAT-P-26. was observed on the night of 2015/03/26. The first spectrum was acquired about 15 min after the transit ingress, when the rising target was at an airmass of 1.6. The time series of 27 spectra stretched to ∼2 h after the transit egress. The 600 s long exposures have a typical S/N of 15 (per pixel in 1 D spectra at 5500 Å). The last 6 spectra of the series were affected by deteriorating weather conditions. The RV values were obtained using a K5 mask; they are reported in Table A.4 and plotted in Fig. 4 HAT-P-29. was observed on the night of 2013/10/16. A series of 23 spectra spanned the time interval from ∼1 h before transit ingress up to ∼1 h after egress. With a exposure time of 900 s, the spectra have an average S/N of 25 (per pixel in 1-D spectra at 5500 Å). The sky spectra acquired with the second fibre show no detectable sign of light contamination from the full Moon. The RV values were obtained using a G2 mask. They are reported in Table A.5 and plotted in Fig. 5

Photometric follow-up observations
Except for HAT-P-15, the planetary systems studied in this work were monitored with an array of medium-class telescopes with the aim of obtaining high-quality transit light curves, which can be used for refining the physical parameters of both the star and the planet, as well as checking stellar activity. As in our previous works based on photometric follow-up observations of transiting exoplanets (e.g. Southworth et al. 2012;Ciceri et al. 2013), we autoguided the telescopes and adopted the "defocussing" technique in all the observations to significantly improve the A162, page 5 of 31 precision of the photometry. The photometric data thus obtained were reduced using a modified version of the DEFOT pipeline (Southworth et al. 2014) and the light curves were extracted by performing standard aperture photometry. For the same purpose as above, we also analysed the light curves obtained by the TESS space telescope (Ricker et al. 2015).
HAT-P-15. Having an orbital period larger than 10 days, complete transits of HAT-P-15 b are difficult to catch with ground-based facilities. Unfortunately, HAT-P-15 light curves are also not available in both the TESS 2 min and 20 s cadence target list 2 for sector 19. In order to check the 30 min cadence TPF files, we went to TESScut 3 and downloaded the TPFs for the RA and DEC of HAT-P-15. Having inspected the TPFs, we realised that HAT-P-15 was not observed by TESS.
HAT-P-17. HAT-P-17 b also has an orbital period larger than 10 days, so the observation of a complete transit is difficult to achieve using ground-based telescopes. We observed one incomplete transit of HAT-P-17 b on July 2012 through a Gunn-i filter with the BFOSC (Bologna Faint Object Spectrograph & Camera) imager, which is mounted on the Cassini 1.52 m Telescope at the Astrophysics and Space Science Observatory of Bologna in Loiano (Italy). Another incomplete transit of HAT-P-17 b was observed on July 2014 with the Calar Alto (CA) Zeiss 1.23 m telescope and using a Cousins-I filter. Details of the instruments and telescopes were already reported in our previous works (see e.g. Mancini et al. 2017). Two transits were observed by TESS with the 2 min cadence during the monitoring of sector 15 of its primary mission. Continuous observations of the target star were obtained from 2019-08-23 to 2019-09-03, for a total of 2 https://tess.mit.edu/observations/target-lists/ 3 https://mast.stsci.edu/tesscut/ 892 measurements. All the transit light curves of HAT-P-17 analysed in this work are plotted in Fig. B.1.
HAT-P-21. Two complete transit events of HAT-P-21 b were observed on March 2012 with the Cassini 1.52 m and the CA 1.23 m telescopes, through a Gunn-r and a Cousins-R filter, respectively. The first data set was severely affected by clouds (Fig. B.2.). Five transits were observed by TESS with the 2 min cadence during the monitoring of sector 22 of its primary mission. Continuous observations of the target star were obtained from 2020-02-22 to 2020-03-14, for a total of 1777 measurements. All the transit light curves of HAT-P-21 analysed in this work are plotted in Fig. B.2.
HAT-P-26. Four complete and one partial transit events of HAT-P-26 b were observed with the CA 1.23 m telescope, through a Cousins-I filter, between March 2012 and February 2018. They are plotted in Fig. B.3. Again, there are no TESS data for this target. It is scheduled to be observed in March 2022 in sector 50. It was missed last time due to being close to the ecliptic, but for the extended mission the orientation of TESS has been changed to observe sections of the sky that were missed.
HAT-P-29. Four transits of HAT-P-29 b were observed with the CA 1.23 m telescope, two through a Cousins-R filter and two through a Cousins-I filter. The last two were only partially observed because they occurred much later than expected. Another two incomplete transits were observed with the DOLORES 4 instrument, mounted on the TNG, and with the IAC 80 cm telescope, through a Johnson-R and Cousins-R filter, respectively. Two complete transits were observed with the INAF-OAPd Copernico 1.82 m telescope, which is located at Cima Ekar-Asiago (Italy), using the Asiago Faint Object Spectrograph and Camera (AFOSC) and a Sloan-r filter within the long-term monitoring program of the TASTE project (Nascimbeni et al. 2011). Details on the last two telescopes were already reported in our previous works (see e.g. Covino et al. 2013;Mancini et al. 2015). Finally, four transits were observed by TESS. They are plotted in Fig. B.4.

Light curve analysis
The light curves of the transit events of HAT-P-17 b, HAT-P-21 b, HAT-P-26 b, and HAT-P-29 b (presented in the previous section) were individually modelled with the JKTEBOP code (Southworth 2013) to make a new determination of the transit parameters. This code considers stars and planets as spheres and makes use of the Levenberg-Marquardt optimisation algorithm in order to fit the parameters of the transit light curves. These are the orbital period and inclination (P orb and i), the time of transit midpoint (T 0 ), the sum and ratio of the fractional radii, i.e. r = R /a and r p = R p /a; R and R p are the radii of the star and planet, respectively, while a is the semi-major axis of the planetary orbit. For modelling the limb darkening (LD) of the star, we used a quadratic law and fitted the LD coefficients (u and v ), taking into account the differences between the atmospheric properties of the four stars as well as the filters that were used. We also took into account the eccentric orbit of the four planets, as it has a slight effect on the shape of the transit light curves (Kipping 2008). JKTEBOP allows the inclusion of the eccentricity, e, and periastron longitude, ω, as fitted parameters constrained by their known values and uncertainties (Southworth et al. 2009), which are summarised in Table 2. Finally, to mitigate the correlated (red) noise, which generally affects time-series photometry obtained by the APER routine 5 , we inflated the error bars of the photometric measurements so that each transit light curve had a reduced chi-square of χ 2 ν = 1 during the best-fitting process. The light curves and the corresponding JKTEBOP best-fitting models are reported in The uncertainties of the fitted parameters were estimated by running both a Monte Carlo and a residual-permutation algorithm. For each of the light curves, we ran 10 000 simulations for the Monte Carlo algorithm and the maximum number of simulations (which is one less than the number of data points) for the residual-permutation algorithm. We took the largest of the two 1 σ values as the uncertainty for each parameter. Finally, for each planetary system, the final values of each parameter were calculated by taking the weighted average of the values extracted from the fit of all the individual light curves; the relative 5 APER is part of the ASTROLIB subroutine library distributed by NASA.
uncertainties were used as weights. These values are shown in the Tables reported in Appendix D and are in good agreement with those available in the literature.

Orbital period determination
In the modelling of the transit light curves with JKTEBOP, we also estimated each transit mid-time and placed them on the BJD (TDB) time system. By joining these new measurements with those already published, it is possible to review and refine the orbital ephemerides for the HAT-P-17, HAT-P-21, HAT-P-26, and HAT-P-29 planetary systems, as well as search for possible TTVs due to variations in the planetary orbital period. The timings that we used for each of the four systems and their residuals for a constant period are shown in the Tables reported in Appendix C.
HAT-P-17. The few transit timings recorded for HAT-P-17 b do not allow us to perform any detailed investigations about possible TTVs. Besides the timing from the discovery paper (Howard et al. 2012), we only have two from partial transit observations and two more from TESS observations. Assuming that the orbital period is constant (linear model), we performed a weighted linear least-squares fit to the mid-transit times versus their cycle number, that is where E is the number of orbital cycles after the reference epoch  HAT-P-21. Also for HAT-P-21 b, few transit mid-times are available and we cannot investigate possible TTVs. Of the two transit light curves we have obtained, one is of low quality with large uncertainties (Fig. B.2) so was excluded from the analysis. This left us with only seven timings: one from the discovery paper , one from our observational program and five from TESS. The linear fit gives: HAT-P-26. This system is a special case for orbital period determination. Hartman et al. (2011) found a variation in the systemic velocity with a detection significance of 2.1σ. Stevenson et al. (2016) noted that there appeared to be a curvature in the diagram of the residuals from fitting a linear ephemeris to the measured times of minimum light. This was followed up by von Essen et al. (2019), who found clear evidence for a sinusoidal variation with a period of 270 epochs (1140 days) and an amplitude of 4 min. They tentatively attributed this to the presence of a third body, in agreement with the marginal detection of a variable systemic velocity.
We assembled the times of mid-transit from previous works (see the list compiled by von Essen et al. 2019) and augmented these with our own measurements. We then fitted four types of orbital ephemeris to them: linear, quadratic, cubic, and linear plus sinusoid. The last ephemeris was modelled with the equation: where P sine is the period of the sine wave (in units of the orbital period), A is the sine amplitude and φ is the phase offset with respect to T 0 . We were initially unable to find a good fit, with a best value of χ 2 ν = 2.7. A close inspection of the published timings showed that three of them have implausibly small errorbars of 0.000011 to 0.000016 days (1.0-1.4 s). These three are based on transmission spectroscopy with HST (Wakeford et al. 2017) and contain large gaps due to the low-Earth orbit: all of them fully cover the egress but have no observations during ingress.
We therefore increased the errorbars of all four timings from Wakeford et al. (2017) by a factor of 10 and refitted the full set of timings (a reanalysis of the HST data to obtain improved timings and uncertainties is outside the scope of the current work but would be useful in future studies). The factor of ten was chosen iteratively and is the factor by which the errorbars from Wakeford et al. (2017) must be increased by to get the sum of the absolute values of the residuals of these four datapoints to be equal to 4 σ (i.e. the multiplicative factor was determined from the scatter of the data around the best fit instead of the quoted errorbars).
With these revised error bars, we find decent fits for all four types of orbital ephemeris. The sinusoidal model fits the data best and is in good agreement with that from von Essen et al. (2019) and is also supported by our new transit timings. In Table 3 we provide the fitted parameters, uncertainties, and Bayesian and Akaike Information Criterion (BIC and AIC) values for the four ephemerides. The sinusoidal variation is confirmed with an amplitude significant at a level of 6σ and much better BIC and AIC values. We therefore confirm that the HAT-P-26 system shows transit timing variations (see Fig. 6).
Interpreting the oscillating O-C as a light time effect, we find a projected semi-major axis of the orbit of the star-planet system around the centre of mass with the third body a 1 sin i ∼ 0.186 ± 0.030 au and a mass function in solar units (a 1 sin i) 3 /P 2 cyc = (6.3 ± 4.3) × 10 −4 au 3 yr −2 , where P cyc = 1167 ± 39 days is the O-C modulation period. This corresponds to a minimum mass of the third body M TB ∼ 0.07 M assuming M TB M s , where M s is the mass of HAT-P-26. In the most favourable conditions, the angular separation of the third body from HAT-P-26 is only 14 mas, making its direct detection challenging, especially if it is a very faint brown dwarf as expected if it has the same age as estimated for the star. Nevertheless, the third body hypothesis is apparently in conflict with the barycentre acceleration of the HAT-P-26 system as measured by Hartman et al. (2011) because our model predicts a mean minimum acceleration of |γ| ∼ 2.2 m s −1 day −1 along the time interval of 182.69 days covered by their observations, while they gaveγ = −0.028 ± 0.014 m s −1 day −1 . An alternative hypothesis to explain the observed O-C modulation is the perturbation of the orbit of HAT-P-26 b by a distant third body as discussed in Sect. 4 of Agol et al. (2005). Their model requires an eccentric orbit of the third body which is associated with a non-sinusoidal shape of the O-C modulation. We find a minimum eccentricity e = 0.67 for the minimum third body mass as estimated from the mass function. Lower values of the eccentricity require a larger third body mass; for example, e = 0.33 requires a mass four times the minimum mass. Another kind of TTV model based on an exchange of angular momentum between the orbit and the rotation of the planet, as suggested by Lanza (2020), is disfavoured by the small moment of inertia of the planet that does not allow to store enough angular momentum to account for the amplitude of the O-C modulation.
HAT-P-26 is astrometrically well-behaved according to the Gaia EDR3 archive information (Gaia Collaboration 2016, 2021): both the values of astrometric excess noise (0.10 mas) and of renormalised unit weight error (RUWE = 1.04) indicate that a single-star solution fits well the available astrometric data. Hot-Jupiter hosts harboring known or likely long-period, massive companions typically have RUWE 1.1 (e.g. Belokurov et al. 2020), but these are not expected to be the ones responsible for the possible TTVs observed in the HAT-P-26 photometry.
We conclude that what seems to be a cyclic TTV in the HAT-P-26 system is worthy of further investigation by collecting more times of mid-transit. This will allow us to look for a non-sinusoidal shape of the modulation and to refine its period and amplitude before we can draw any sound conclusion on its origin.
HAT-P-29. Photometric follow-up of HAT-P-29 b transit events were performed by Wang et al. (2018) and Mallonn et al. (2019). In particular, Mallonn et al. (2019) recorded two incomplete transit light curves with the Stella 1.2 m telescope at the Izana Observatory, while Wang et al. (2018) reported the observations of one complete and six incomplete transit light curves with the Schmidt telescope at the Xinglong Station; these authors also observed a complete light curve with the 1 m telescope operated at the Weihai Observatory. All these light curves have point-to-point scatters larger than 2 mmag.
The two timings reported by Mallonn et al. (2019) are early by about 900 s. Since they were both based on transit events in which the egress was not observed, their reliability is reduced (e.g. Gibson et al. 2009) and we decided to exclude them from the analysis.
We joined our new timings (see Fig. B.4) with that from the discovery paper (Buchhave et al. 2011) and the eight ones from Wang et al. (2018), obtaining a total of 18 mid-transit times. We tried to model the data by using both a linear and a quadratic ephemeris, the latter taking the form: where dP orb dE is the change in the orbital period between succeeding transits. The fit of the mid-transit times with a straight line gave: T mid = BJD TDB 2 455 838.59462 (61) + 5.7233746 (32) E, (6) with a χ 2 ν = 6.4 and a root-mean-square deviation (rmsd) scatter of 244 s. The residuals are plotted in Fig. C.1. Instead, the bestfitting quadratic ephemeris gives us: with a χ 2 ν = 5.6 and rmsd = 267 s. We also estimated the Akaike Information Criterion (AIC) and the Bayesian Information Criterion (BIC). Both these criteria slightly prefer the quadratic model over the linear one. The rms is larger for the quadratic ephemeris versus the linear one only because it does not depend on the errorbars of the measured transit time. As in previous works of our series (e.g. Southworth et al. 2012;Mancini et al. 2013) such large values of the χ ν should not be interpreted as a suggestion of TTVs, but as an indication that the uncertainties in the various T 0 measurements are too small. As a matter of fact, if we exclude from the analysis the five timings measured by Wang et al. (2018) from noisy data covering only part of transits, both the fits have a lower and similar reduced chi-square. We found χ 2 ν = 3.9 and rmsd = 249.7 s for the linear model and χ 2 ν = 3.9 and rmsd = 222.0 s for the quadratic model. This time, both the AIC and BIC criteria prefer the linear model over the quadratic one.
In conclusion, considering the amount of available data and their quality, we did not find a clear indication of the existence of TTVs. Further investigation needs more photometric followup observations of transits by HAT-P-29 b. We stress that the new linear ephemeris that we determined (Eq. (6); Fig. C.1) is such that the orbital period is 16.3 ± 4.5 s longer than that of the discovery paper, in good agreement with what was found by Wang et al. (2018).

Frequency analysis of the time-series light curves
Knowledge of the stellar rotational period P rot is important for better characterisation of a star-planet system. In particular, by combining the value of P rot with those of the stellar radius, R , and projected rotational velocity v sin i , we can determine the inclination of the stellar spin axis, i . In turn, i , together with the projected spin-orbit misalignment angle λ, yields an estimation of the true obliquity angle ψ (Winn et al. 2007).
We have analysed the HATNet photometric data 6 to look for possible periodic variations induced by activity and modulated by stellar rotation. We applied the Trend Filtering Algorithm (TFA; Kovács et al. 2005) to the photometric time-series produced by the HATNet pipeline and we examined all three data sets corresponding to different apertures.
HAT-P-15. was observed on 106 different nights between September 2005 and February 2006. The typical standard deviation of photometric measurements within the same night is σ ∼ 9 mmag. Nightly averaged photometric values have very small dispersion (σ ∼ 2 mmag), indicating that the star had a low activity level (see the upper panel in Fig. 7). After removing in-transit data points (190 out of 8945), we calculated the Scargle periodogram (see the bottom panel in Fig. 7) and found that the highest peak occurs at P 1 ≡ 1/ f 1 = 9.3 days. By using the bootstrap method, we estimated for the peak at P 1 a false alarm probability (FAP) of 7.6% and concluded that it is not statistically significant.
HAT-P-17. was monitored by four different telescopes of the HAT network from June 2004 to October 2005 for a total of ∼250 nights. On the same night, photometric measurements have an average standard deviation of σ ∼ 6 mmag. We have considered first the full dataset and then, independently, the first and last longer observing seasons with red asterisks and blue circles respectively); in no case does the periodogram analysis show significant peaks. The low dispersion (σ = 1.8 mmag) of the nightly binned photometry indicates a very low activity level.
HAT-P-21. was monitored from November 2006 to June 2008, for a total of 24 633 single measurements. The power spectrum of the 288 daily means clearly shows two peaks at f = 0.063 day −1 and 2 f = 0.126 day −1 (Fig. 8, top panel). Interpreting the signal as due to the stellar rotation, we searched for the best fit by fixing simultaneously the frequency f and its harmonic 2 f , thus obtaining P rot = 15.88 ± 0.02 days. The folded light curve shows a flat part and a full-amplitude of 7.1 mmag (Fig. 8, bottom panel). Since the noise level in the power spectrum corresponds to 0.28 mmag, the signal has to be considered highly significant (S/N = 12.7).
HAT-P-26. was observed from January to August 2009, for a total of 12 223 measurements. The frequency analysis of the 150 daily means does not show any significant peak above the noise level of 0.21 mmag.

Analysis of the stellar parameters
We fit the Spectral Energy Distribution (SED) via the MESA Isochrones and Stellar Tracks (MIST) (Dotter 2016;Choi et al. 2016) through the EXOFASTv2 suite (Eastman et al. 2019). We fit the available archival magnitudes imposing Gaussian priors on T eff and [Fe/H] based on spectroscopic measurements and on parallax π based on the Gaia EDR3 astrometric measurement (Gaia Collaboration 2016, 2021; this astrometric prior helps constraining the stellar radius and improves the precision of the stellar parameters resulting from the SED fitting procedure. The stellar parameters were simultaneously constrained by the SED and the MIST isochrones, as the SED primarily constrains R and T eff , and a penalty for straying from the MIST evolutionary tracks ensures that the resulting star is physical in nature. The results are shown in the Tables reported in Appendix D and they were used for the best-modelling fit of the RM effects (Sect. 8.2) as well as for reviewing the physical parameters of the systems (Sect. 9).

Stellar atmospheric parameters
Stellar atmospheric parameters were derived using the weighted means of all HARPS-N spectra available for the five targets. We therefore measured the equivalent widths (EWs) of iron lines taken from the list by Biazzo et al. (2015), and, together with the abfind driver of the MOOG code (Sneden 1973(Sneden , version 2013 and the Castelli & Kurucz (2003) grid of model atmospheres, we obtained effective temperature (T eff ), surface gravity (log g), A162, page 10 of 31 Table 4. Stellar atmospheric parameters determined from HARPS-N spectra.
We refer to the mentioned papers (and references therein) for further details on the procedures. The final results of the spectroscopic analysis applied here to determine the stellar atmospheric parameters are listed in Table 4.

Determination of the spin-orbit alignment
The modelling and fitting of the RV measurements were performed by using a code that we developed within the MATLAB software ambient 7 . A thorough description of the code was already given in Esposito et al. (2017). In practice, we derive the best-fitting values for three parameters: the stellar projected rotational velocity, v sin i , the systemic RV, γ, and the sky-projected orbital obliquity angle, λ. The other pertinent parameters (see Esposito et al. 2017) are kept fixed to the values found in the photometric and spectroscopic analysis, while their uncertainties are propagated for determining the error bars of v sin i , γ, and λ. We upgraded the code to include the possibility to model and fit the effect of the stellar convective blueshift (CB) on the in-transit RV curve; we used a simple one-parameter model introduced by Shporer & Brown (2011). The results of the fits are summarised in Table 5, while the best-fitting RV models are shown in Figs. 1-5, superimposed on the data points.
HAT-P-15. For this target, we only have the RV time-series spanning one transit and no photometric follow-up observations. Therefore, for many relevant parameters, we had to adopt values from the literature as well as from our analysis of the stellar parameters (see Sect. 7 and Table D.1). The free parameters in our fit are λ, v sin i , and γ. Since the uncertainties on the ephemerides reported in Kovács et al. (2010) propagated to an uncertainty of 10 min on the mid-transit time at the epoch of our observations, we also included the time of periastron as a free parameter. 7 MATLAB R2015b, Optimization Toolbox 7.3 and Curve Fitting Toolbox 3.5.2, The MathWorks, Inc., Natick, Massachusetts, United States.

Notes.
Except for the first, the columns contain two values. Those on the top are from the fit in which we considered the stellar convective blueshift (CB), whereas those on the bottom did not. The preferred values are given in bold font for each target; see the text for details. Due to the low quality of the HAT-P-26 data, we were not able to well constrain λ for this system, which was merely estimated by fixing the value of v sin i .
We considered both models with and without the CB effect and show the results of the fits in Fig. 1. We used the Bayesian Information Criterion (BIC) to compare the two models. With ∆BIC = −0.95, the model with CB is only marginally better. The best fit value of CBV = −1.40 ± 0.85 km s −1 is suspiciously high for a G5 star (Dravins 1990), and we think it is driven by the first three in-transit data points. Therefore we prefer to adopt the best fit values of the model without the CB effect, for which λ = 13 • ± 6 • .
HAT-P-17. was already observed with the Keck/HIRES for detecting the RM effect, as reported by Fulton et al. (2013). Due to the slow stellar rotational velocity (v sin i = 0.56 +0.12 −0.14 km s −1 ), they estimated the amplitude of the RM effect to be only ∼7 m s −1 . As a consequence, they remarked on the need to model also the effect of the CB in order to derive a correct estimation of λ. Indeed, without the CB effect modelling, they obtained λ = 37 ± 12 deg, whereas with the CB effect they found λ = 19 +14 −16 deg, and a CB velocity parameter CBV = −0.65 ± 0.23 km s −1 .
First, we used our code to make an independent fit of the HIRES RVs. Without modelling the CB effect, we obtained λ = −28 deg and v sin i = 0.8 km s −1 ; accounting for the CB effect we derived λ = −17 deg, v sin i = 0.7 km s −1 , and CBV = −0.33 km s −1 . Provided that Fulton et al. (2013) are most likely using a different convention for the sign of λ (compare their Fig. 3 with our Fig. 2), our results are compatible with theirs: considering the CB effect results in a value of λ closer to zero. However, we obtained a significantly smaller value for CBV. Unlike Fulton et al. (2013), we rejected two of their data points as outliers (see Fig. 2) because they showed residuals larger than 4 σ. Correspondingly, we find a value for the CBV closer to zero, that is CBV = −0.33 km s −1 . Instead, by including all the data points, our best-fitting value for the CBV is −0.58 km s −1 , which is similar to the result found by Fulton et al. (2013).
Next, we analysed our HARPS-N RV data set, by using the same approach as for the HIRES data. The best-fitting values, without the CB effect, are λ = −55 deg and v sin i = 1.6 km s −1 .
A162, page 11 of 31 A&A 664, A162 (2022) By modelling also the CB effect, we obtained λ = −37 deg, v sin i = 1.1 km s −1 , and CBV = −0.57 km s −1 . Although with a marginal statistical significance, both for HIRES and HARPS-N data sets the model including the CB effect is to be preferred, as we obtain smaller BIC: ∆BIC = −0.9 and −4.1 for HIRES and HARPS-N, respectively.
Finally, we made a combined fit of the HIRES and HARPS-N RVs, and estimated the uncertainties on the best-fit parameters using the bootstrap method. The best-fit RV curve models are displayed, together with the RV data sets, in Fig. 2. The left panels show the model considering the RM effect only, whereas the model in the right panels accounts also for the CB effect. In the first case we derive v sin i = 1.00 ± 0.09 km s −1 , λ = −41.1 ± 3.6 deg, while in the second case we obtain CBV = −0.46 ± 0.11 km s −1 , v sin i = 0.84 ± 0.07 km s −1 , λ = −27.5 ± 6.7 deg. Also for the combined fit, the model that includes the CB effect is to be preferred as we obtain ∆BIC = −6.7. We adopt this latter value as our final estimation of λ for HAT-P-17 b.
HAT-P-21. For this target, we adopted all the planetary and stellar relevant parameters as obtained from the analysis of the light curves and the stellar spectra (see Table D.3). The bestfitting values of the parameters determined by the analysis of the in-transit RV curve are reported in Table 5. In particular, we obtained λ = −0.7 • ± 12.5 • .
The fit using the model that includes the CB effect gives a value of CBV very close to zero, and, correspondingly, the other fitted parameters have the same values as in the fit without CB. We notice that HAT-P-21 b has an impact parameter of b = 0.62, that is the planet never occults the central part of the stellar disk and, therefore, we expect the RV variations due to the CB effect to be small. We conclude that the data do not have the quality needed for a solid detection of the CB effect.
As we know the rotational period of its parent star (see Sect. 6), we are able to estimate the quantity i using the following equation: which gave the result of 62 • ± 16 • . Knowing i , i and λ, we can calculate the true misalignment angle via (Winn et al. 2007): cos ψ = cos i cos i + sin i sin i cos λ.
HAT-P-26. Based on published ephemerides, the first point of the HARPS-N time-series observations was taken ∼15 min after the transit had already started. Instead, the last points present a large scatter due to worsening weather conditions (see Fig. 4). Therefore, the fit of the data does not allow to constrain λ at the required precision as in the other four cases presented in this work. We made a putative estimate of λ by fixing the value of v sin i to that estimated from the spectroscopy (see Table 4) and finding λ = 18 • ± 49 • , which suggests a prograde orbit for HAT-P-26 b.
HAT-P-29. We find that the fit of the data using a model which includes the CB effect is slightly disfavoured with respect to the fit without CB (∆BIC = 3.0); given the relatively large value of v sin i = 5.2 km s −1 , we expected that the CB effect can only have a minor impact on the shape of the in-transit RV curve. Therefore, for HAT-P-29 we adopt the results of the fit without CB, that is λ = −26 • ± 16 • . However, the analysis of the fit with the CB provides us with a useful 1 σ lower limit (> −0.58 km s −1 ) to the value of CBV.

Physical parameters
Considering the new photometric data available for HAT-P-17, HAT-P-21, HAT-P-26, and HAT-P-29, we reviewed the physical properties of these planetary systems. We followed the "Homogeneous Studies" approach (Southworth et al. 2012 and references therein) and combined the parameters obtained from the light curves and spectroscopic observations, placing constraints on the properties of the host stars, which we can deduce from theoretical evolutionary models of stars. In particular, we used the following spectroscopic properties of the host stars, which we obtained from the analysis of the stellar spectra (see Sect. 8): the projected rotational velocity v sin i , the effective temperature T eff , the logarithmic surface gravity log g, and the iron abundance.
Since the HARPS-N data were collected during transit events for measuring the RM effect, we do not have new out-of-transit RV points for redetermining the velocity amplitude, K , of the RV curves. Therefore, we adopted the values from the literature; they are reported in Tables D.1-D.5, together with the other relevant parameters.
With these input parameters, as in Mancini et al. (2018), we made use of the JKTABSDIM code (Southworth et al. 2009) to make new estimates of the main physical properties of the planetary systems HAT-P-17, HAT-P-21, HAT-P-26, and HAT-P-29. By iteratively modifying the velocity amplitude of the planet, JKTABSDIM maximises the agreement between the measured T eff and R /a and with those predicted by a set of five theoretical models. A wide range of possible ages for each of the host stars was considered. The code returned five different estimates for each of the output parameters, one for each set of theoretical models, and we took the unweighted means as the final values of the parameters. The corresponding systematic uncertainties, caused by the use of theoretical models, were calculated considering the maximum deviation between the values of the final parameters and the single ones coming from the five theoretical models. Instead, statistical uncertainties were propagated from the error bars in the values of the input parameters. The final values are reported in Tables D.2-D.5, together with values taken from the literature, which are shown there for comparison purposes. Our estimations of the radii and masses for the stars and planets are all within the error bars of literature determinations, but slightly more precise.

On the spin-orbit alignment of hot Jupiters
At present (February 2022), TEPCat lists determinations of λ for roughly 170 transiting exoplanets, while ψ has been constrained for only 39. Most of them are hot Jupiters, which represents the only class for which we have a good statistical sample. What can be deduced from this collection of λ measurements for hot Jupiters is a matter of debate. So far, no convincing correlations have emerged from plotting the projected obliquity versus other parameters, such as planetary radius and mass, orbital separation, stellar age, and so on. Early studies (e.g. Winn et al. 2010;Albrecht et al. 2012;Dawson 2014;Tregloan-Reed et al. 2015), based on a smaller sample of λ measurements, have tentatively identified two populations of more or less aligned hot Jupiters based on the effective temperature of their parent stars. Considering our new data and those listed in TEPCat, we plotted the absolute values of λ of hot Jupiters (0.3 M Jup < M p < 13 M Jup and a/R < 25) versus T eff in Fig. 9. Of the more than 130 planets appearing in the diagram, only 14 have an eccentricity e > 0.1; four of them are the planets presented in this study. The separation line between the two groups is related to the Kraft break (the remarkable decrease in the rotation velocities observed in main-sequence stars later than F5, Kraft 1967), and falls somewhere between 6090 and 6300 K (see the gray zone in Fig. 9); planets orbiting stars with mostly convective (radiative) outer envelopes are on the left (right) side of this plot.
Being cooler than radiative stars, convective stars are supposed to have a rapid tidal dissipation as the convective cells produce the turbulent cascades that lead to energy loss. Instead, the radiative stars are thought to have much weaker tidal dissipation. Consequently, the orbit of hot Jupiters hosted by relatively cool stars (T eff < 6100 K) should be much more aligned with the spin of their hosts because tides limit any possible obliquity on timescales much shorter than those related to the orbital decay of hot Jupiters. Specifically, the tidal modes responsible for the damping of the obliquity may be different from those producing the orbital decay and can act on a remarkably shorter timescale producing a spin-orbit alignment without a significant decrease of the orbital semi-major axis (Lai 2012;Valsecchi & Rasio 2014;Lanza 2022). As we can see from Fig. 9, although high-obliquity hot Jupiters were found regularly above the Kraft break, there are several exceptions that challenge this theory.
In order to have a more general picture of the current situation, we refer the reader to the top panel of Fig. 10, where we made a polar plot of the measured sky-projected obliquities of all known systems hosting a planet with M p < 13 M Jup and a scaled orbital distance a/R * from the host star up to 25. Even for systems hosting smaller planets, it is difficult to see a correlation between λ and T eff .
Based on the expectations for the rotation velocities of stars with effective temperatures between 5900 and 6600 K from  Fig. 10. Top panel: sky-projected orbital obliquity of known exoplanets as a function of their scaled orbital distance a/R * from the host star. The plot includes all planets with M p < 13 M Jup and a/R < 25. They are represented by circles, whose sizes are proportional to their mass. The planets surrounded by the green circles are those examined in this work, except for HAT-P-26 b. Bottom panel: true orbital obliquity of known exoplanets. They are represented by circles, whose size are proportional to their radius. The planet surrounded by the green circle is HAT-P-21 b., which was examined in this work. Both panels: the error bars have been suppressed for clarity. Colour indicates the effective temperature of their parent stars. The data were taken from TEPCat in February 2022.  Fig. 10), in which most of the exoplanets orbiting cool stars have ψ < 30 • , whereas the four exoplanets orbiting hot stars (T eff ≥ 7650 K) have 60 • < ψ < 135 • . However, since the statistical sample is not yet significant, it is hard to make strong assertions. Finally, the diagram in Fig.11 shows the measurements of λ for all the known transiting exoplanets versus the corresponding orbital eccentricity, similar to that presented by Albrecht et al. (2022); points are coloured based on the temperature of the parent stars. No clear correlation between these two orbital parameters emerges from this plot.

Tidal-alignment timescales for the five systems of our study
An estimate of the tidal-alignment timescales in the specific cases of our four systems (HAT-P-15, HAT-P-17, HAT-P-21, and HAT-P-29), based on an adapted version of the tidal model of Leconte et al. (2010), which was already used in our previous investigations (e.g. Esposito et al. 2017), shows that only HAT-P-21 has an e-folding timescale for the damping of its obliquity of ∼0.3 Gyr. Such a timescale is shorter than the main-sequence lifetime of the star when we adopt a stellar modified tidal quality factor Q s = 10 6 , as expected for an efficient dissipation of the obliquity tides as in the model by Lai (2012). The age estimated from the observed rotation period of HAT-P-21 using gyrochronology, that is ∼1.5-2.0 Gyr, is in tension with the age estimated from the isochrone fitting (∼7.8 ± 2.6 Gyr). Its relatively fast rotation could be due to the tides produced by the close-by massive planet that tends to spin-up HAT-P-21 with a characteristic e-folding timescale of ∼4 Gyr, if we assume a stellar modified tidal quality factor Q s = 10 7 as suggested, for example, by Jackson et al. (2009). The e-folding timescale for the damping of the orbital eccentricity is ∼3.3 Gyr, when we adopt modified tidal quality factors Q s = 10 7 for the star and Q p = 10 7 for the planet, respectively. The modified tidal quality factor of the planet is obtained by scaling the value of Jupiter to the slow rotation of HAT-P-21 b assumed to be synchronised with its orbital motion (cf. Ogilvie 2014). These considerations suggest that HAT-P-21 is indeed an old star and that the planet could have migrated close to its host through an orbit of initially high eccentricity that was significantly reduced by tides during the main-sequence lifetime of the system together with any initially large obliquity.
Considering the other systems, their orbits also show a significant eccentricity. Assuming Q s = 10 7 and Q p = 10 7 as in the case of HAT-P-21 and HAT-P-21b, respectively, the e-folding timescale for the damping of the eccentricity, τ e , is comparable with the estimated age of the system only in the case of HAT-P-26 (τ e ∼ 6 Gyr), while it is longer for the other systems. The rotation of the hosts and the obliquity of the planetary orbits were not significantly affected by the tides during their main-sequence evolution, even assuming a strong interaction with Q s = 10 6 . In conclusion, these considerations suggest that (with the possible exception of HAT-P-21) the rather small spin-orbit misalignments observed in the other systems are likely to be primordial as well as their significant eccentricities. The only possible exception could be the eccentricity of HAT-P-26, which might require excitation by a third body to account for the observed values.

Summary
Within the GAPS programme, we are observing a sample of transiting-exoplanet systems, mostly hosting hot Jupiters, with  Fig. 11. Sky-projected orbital obliquity of known exoplanets as a function of their orbital eccentricity. Different colours indicate a different value of T eff : dark red are for cool hosts (T eff < 6250 K); orange are for hot hosts 6250 < T eff < 7000 K; yellow are for very hot hosts T eff < 7000 K. A number of these planets exhibiting an eccentricity equal to zero does not have horizontal error bars. The planets surrounded by the green circles are those examined in this work, except for HAT-P-26 b. The other data were taken from TEPCat in February 2022.
the HARPS-N spectrograph, supported by an array of mediumclass telescopes. The aim is to better characterise these planetary systems and get information about the degree of orbital alignment of this class of planets, according to the characteristics of their parent stars.
We divided the five targets under study in this work into two groups. In the first group, there are four hot Jupiters (HAT-P-15, HAT-P-17, HAT-P-21, and HAT-P-29), while in the second group, there is one Neptune-mass planet (HAT-P-26). Details of our new observations are reported in Tables 1 and B.1. Thanks to new spectroscopic and photometric observations that we collected, and the public data from TESS and Gaia, we were able to (i) review their physical and orbital parameters and (ii) reveal the RM effect, during transit events, and measure the spin-orbit alignment of these systems.
Our main results are as follows: -We revised most of the physical parameters of the five planetary systems. Our results are reported in Tables D.1-D.5, and are in good agreement (and, in general, slightly more accurate) with those obtained previously by other authors. -We estimated new mid-transit times for four of the systems (HAT-P-17, HAT-P-21, HAT-P-26, and HAT-P-29) and augmented them with published values to obtain lists of transit times. They are reported in Tables C.1-C.4. They were used for updating the orbital periods and expected mid-transit times of the systems. We also searched for evidence of TTVs. Our analysis shows an indication of possible TTVs in the HAT-P-29 planetary system, which must be verified with more data. We determined a new linear ephemeris with an orbital period 17 ± 4.2 s longer than that found by Buchhave et al. (2011). We also confirmed the much stronger indication of TTVs that was found by von Essen et al. (2019) for the HAT-P-26 system. This sinusoidal variation may be caused by a third body in the system. More follow-up observations are required to confirm its existence. -The frequency analysis of the HATNet photometric timeseries for HAT-P-21 highlighted a modulation caused by A162, page 15 of 31 A&A 664, A162 (2022) stellar activity, allowing us to get a measurement of the rotational period of the star of P rot = 15.88 ± 0.02 days. A similar analysis, performed for the HATNet light curves of the other four stars, did not unearth out any clear photometric modulation. -We used the HARPS-N spectrograph to monitor one transit for each of the five planets. The RM effect was completely covered for HAT-P-15, HAT-P-17, HAT-P-21, HAT-P-29 and (only partially) for HAT-P-26, which also suffered from adverse weather conditions at the end of the observations. We successfully measured the sky-projected orbital obliquity for four of the systems, obtaining λ = 13 • ± 6 • , λ = −26.3 • ± 6.7 • , λ = −0.7 • ± 12.5 • , λ = −26 • ± 16 • , for HAT-P-15 b, HAT-P-17 b, HAT-P-21 b, and HAT-P-29 b, respectively, all indicating good spin-orbit alignments within the uncertainties. Even though we were not able to constrain λ for HAT-P-26 b, the modelling of the data returns a value, λ = 18 • ± 49 • , that also suggests a prograde orbit for this planet; this is also supported by the shape of the RM effect, see Fig. 4. Finally, for the HAT-P-21 system, we were able to determine its true obliquity, obtaining ψ = 25 • ± 16 • . We also discuss the case that the sky projected spin-orbit misalignment of exoplanets, especially of hot Jupiters, can be correlated with the temperature of their parent stars. We confirm that hot Jupiters with low obliquity are regularly found orbiting convective stars, with effective temperatures below the Kraft break, which have a rapid tidal dissipation when compared with radiative stars. However, the existence of several exceptions limits the clarity we have in this regard. A further effort to enlarge the sample is required in order to shed new light on the matter.
Finally, we roughly estimated the tidal-alignment timescales of the systems under study and made some deductions about the origin of the rather small spin-orbit misalignments we measured.
Acknowledgements. This paper is based on observations collected with the following telescopes: the 3.58 m Telescopio Nazionale Galileo (TNG), operated on the island of La Palma (Spain) by the Fundación Galileo Galilei of the INAF (Istituto Nazionale di Astrofisica) at the Spanish Observatorio del Roque de los Muchachos, in the frame of the programme Global Architecture of Planetary Systems (GAPS); the Zeiss 1.23 m telescope at the Centro Astronómico Hispano Alemán (CAHA) in Calar Alto (Spain); the Cassini 1.52 m telescope at the Astrophysics and Space Science Observatory of Bologna in Loiano (Italy); the Copernico telescope (Asiago, Italy) of the INAF -Osservatorio Astronomico di Padova; the 0.82 m IAC 80 Telescope, operated on the island of Tenerife by the Instituto de Astrofísica de Canarias in the Spanish Observatorio del Teide. The HARPS-N instrument has been built by the HARPS-N Consortium, a collaboration between the Geneva Observatory (PI Institute), the Harvard-Smithonian Center for Astrophysics, the University of St. Andrews, the University of Edinburgh, the Queen's University of Belfast, and INAF. This research made use of Lightkurve, a Python package for Kepler and TESS data analysis (Lightkurve Collaboration, 2018). The other reduced light curves presented in this work will be made available at the CDS (http://cdsweb.u-strasbg.fr/). This work has made use of data from the European Space Agency (ESA) mission Gaia (https://www.cosmos.esa.int/gaia), processed by the Gaia Data Processing and Analysis Consortium (DPAC, https://www.cosmos.esa.int/web/ gaia/dpac/consortium). Funding for the DPAC has been provided by national institutions, in particular the institutions participating in the Gaia Multilateral Agreement. We thank Roberto Gualandi for his technical assistance at the Cassini telescope. We thank the support astronomers of CAHA for their technical assistance at the Zeiss telescope. L.M. acknowledges support from the "Fondi di Ricerca Scientifica d'Ateneo 2021" of the University of Rome "Tor Vergata". We acknowledge the use of the following internet-based resources: the ESO Digitized Sky Survey; the TEPCat catalogue; the SIMBAD database operated at CDS, Strasbourg, France; and the arXiv scientific paper preprint service operated by Cornell University. M.E. acknowledges the support of the DFG priority program SPP 992 "Exploring the Diversity of Extrasolar Planets" (HA 3279/12-1).

Appendix D: Revised physical parameters of the planetary systems
The tables in this appendix report the final values that we obtained for the main physical parameters of the planetary systems under study. The values obtained in this work (Sect. 9) are compared with those taken from the literature. Where two error bars are given, the first refers to the statistical uncertainties and the second to the systematic errors.