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S Dalal, F Rescigno, M Cretignier, A Anna John, F Z Majidi, L Malavolta, A Mortier, M Pinamonti, L A Buchhave, R D Haywood, A Sozzetti, X Dumusque, F Lienhard, K Rice, A Vanderburg, B Lakeland, A S Bonomo, A Collier Cameron, M Damasso, L Affer, W Boschin, B Cooke, R Cosentino, L Di Fabrizio, A Ghedina, A Harutyunyan, D W Latham, M López-Morales, C Lovis, A F Martínez Fiorenzano, M Mayor, B Nicholson, F Pepe, M Stalport, S Udry, C A Watson, T G Wilson, Correction to: Trio of super-Earth candidates orbiting K-dwarf HD 48948: a new habitable zone candidate, Monthly Notices of the Royal Astronomical Society, Volume 534, Issue 3, November 2024, Pages 2410–2411, https://doi.org/10.1093/mnras/stae2228
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This is an erratum to the paper titled ‘Trio of super-Earth candidates orbiting K-Dwarf HD 48948: a new habitable zone candidate’, published in MNRAS 531, 4464–4481 (2024) with 10.1093/mnras/stae1367. We have identified and corrected errors in table 3 of the original publication. The incident flux and temperature values for the three planetary candidates were incorrectly calculated due to a mathematical error. Additionally, we discovered a typographical mistake in the eccentricity values for candidates c and d in the tweaks analysis. The accurate and updated values are provided in the Table 1. While these errors do not alter the overall conclusions of the paper, the corrected values provide a more accurate representation of the data and should be used for reference in future research.
The table displays the results of three Keplerian models, as discussed in sections 7.1, 7.2, and 7.3. The values and uncertainties of each parameter are derived from their respective posterior distributions, with the 50|$^{\rm {th}}$| percentile representing the central value and the 16|$^{\rm {th}}$| to 84|$^{\rm {th}}$| percentile range indicating 1σ uncertainty. Additionally, the derived parameters, as explained in section 7.3, are also included in this table. The maximum equilibrium temperature is calculated assuming an albedo (A|$_{B}$|) of 0 and isotropic re-emission and uniform equilibrium temperature.
Parameter . | Symbol . | Unit . | HD48948 b . | HD48948 c . | HD48948 d . |
---|---|---|---|---|---|
Three Keplerians-only analysis on YV2 RVs | |||||
Orbital period | P | days | |$7.33982_{-0.00085}^{+0.00082}$| | |$37.998_{-0.019}^{+0.018}$| | |$151.12_{-0.49}^{+0.56}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$1.35_{-0.17}^{+0.18}$| | |$1.71_{-0.22}^{+0.20}$| | |$1.09\pm 0.19$| |
Eccentricity | e | |$0.06_{-0.05}^{+0.10}$| | |$0.06_{-0.05}^{+0.09}$| | |$0.10_{-0.09}^{+0.18}$| | |
Argument of periastron | |$\omega$| | rad | |$0.83_{-1.28}^{+1.27}$| | |$-1.06_{-1.00}^{+1.24}$| | |$-1.02_{-1.11}^{+1.43}$| |
|$\sqrt{e}\cos \omega$| | |$0.07_{-0.16}^{+0.19}$| | |$0.04_{-0.20}^{+0.15}$| | |$0.04_{-0.30}^{+0.17}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.09_{-0.15}^{+0.20}$| | |$-0.11_{-0.19}^{+0.13}$| | |$-0.14_{-0.27}^{+0.18}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456574.05_{-1.49}^{+1.53}$| | |$2456570.22_{-7.11}^{+5.98}$| | |$2456564.06_{-31.89}^{+18.67}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$3.18\pm 0.41$| | |$6.97_{-0.89}^{+0.82}$| | |$6.93_{-1.24}^{+1.21}$| |
One-dimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34012_{-0.00046}^{+0.00052}$| | |$37.99_{-0.22}^{+0.16}$| | |$150.28\pm 0.69$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.07_{-0.17}^{+0.15}$| | |$1.06\pm 0.69$| | |$1.55_{-0.38}^{+0.35}$| |
Eccentricity | e | |$0.08_{-0.05}^{+0.06}$| | |$0.23_{-0.19}^{+0.14}$| | |$0.15_{-0.10}^{+0.17}$| | |
Argument of periastron | |$\omega$| | rad | |$0.55_{-0.92}^{+0.95}$| | |$-0.48_{-1.40}^{+1.81}$| | |$-1.05{-0.79}^{+0.96}$| |
|$\sqrt{e}\cos \omega$| | |$0.16_{-0.18}^{+0.13}$| | |$0.13_{-0.40}^{+0.34}$| | |$0.10_{-0.33}^{+0.20}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.11_{-0.18}^{+0.14}$| | |$-0.11_{-0.33}^{+0.46}$| | |$-0.25_{-0.20}^{+0.23}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456573.74_{87}^{+1.05}$| | |$2456571.71_{-9.80}^{+10.5}$| | |$2456571.52\pm 15.3$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.86_{-0.39}^{+0.35}$| | |$3.94_{-2.85}^{+3.02}$| | |$9.72_{-2.56}^{+2.26}$| |
Multidimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34013_{-0.00040}^{+0.00040}$| | |$37.920_{-0.024}^{+0.026}$| | |$150.95_{-0.41}^{+0.45}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.11\pm 0.13$| | |$1.75\pm 0.25$| | |$1.72\pm 0.22$| |
Eccentricity | e | |$0.078_{-0.050}^{+0.058}$| | |$0.22_{-0.11}^{+0.10}$| | |$0.12_{-0.08}^{+0.12}$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
|$\sqrt{e}\cos \omega$| | |$0.17_{-0.18}^{+0.13}$| | |$-0.08_{-0.22}^{+0.23}$| | |$0.01\pm 0.24$| | ||
|$\sqrt{e}\sin \omega$| | |$0.14_{-0.17}^{+0.13}$| | |$0.41_{-0.21}^{+0.13}$| | |$0.21_{-0.19}^{+0.25}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2459003.44 _{ -0.83 }^{+ 1.06}$| | |$2459019.8 _{ -2.7 }^{+ 3.5}$| | |$2459107 _{ -42 }^{+ 24}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.96\pm 0.32$| | |$6.9\pm 1.0$| | |$11.0\pm 1.5$| |
tweaksanalysis ontweaksRVs | |||||
Orbital period | P | days | |$7.34013 \pm 0.00040$| | |$38.06 \pm 0.06$| | |$151.92 \pm 0.44$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.28\pm 0.15$| | |$1.48\pm 0.39$| | |$1.55\pm 0.34$| |
Eccentricity | e | |$0.055 \pm 0.043$| | |$0.11 \pm 0.08$| | |$0.13 \pm 0.11$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
Time of periastron | |$t_{\rm p}$| | BJD | |$2456567.026 \pm 1.72$| | |$2456557.14 \pm 12.5$| | |$2456494.34 \pm 20.1$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$5.43\pm 0.30$| | |$6.33\pm 1.6$| | |$10.05\pm 2.27$| |
Derived parameters | |||||
Semimajor axis | a | au | |$0.0652\pm 0.0005$| | |$0.1951\pm 0.0016$| | |$0.4894\pm 0.0042$| |
Semimajor axis | a | arcsec | 0.0039 | 0.0116 | 0.0291 |
Scaled semimajor axis | |$a/R_\star$| | |$20.65\pm 0.21$| | |$61.79\pm 0.62$| | |$154.97\pm 1.61$| | |
Incident flux | |$F_{\rm inc}$| | |$F_{\rm inc,{\oplus }}$| | |$43.33\pm 2.41$| | |$4.84\pm 0.27$| | |$0.77\pm 0.04$| |
Equilibrium temperature | |$T_{\rm eq}$| | K | |$715\pm 10$| | |$413\pm 6$| | |$261\pm 4$| |
Parameter . | Symbol . | Unit . | HD48948 b . | HD48948 c . | HD48948 d . |
---|---|---|---|---|---|
Three Keplerians-only analysis on YV2 RVs | |||||
Orbital period | P | days | |$7.33982_{-0.00085}^{+0.00082}$| | |$37.998_{-0.019}^{+0.018}$| | |$151.12_{-0.49}^{+0.56}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$1.35_{-0.17}^{+0.18}$| | |$1.71_{-0.22}^{+0.20}$| | |$1.09\pm 0.19$| |
Eccentricity | e | |$0.06_{-0.05}^{+0.10}$| | |$0.06_{-0.05}^{+0.09}$| | |$0.10_{-0.09}^{+0.18}$| | |
Argument of periastron | |$\omega$| | rad | |$0.83_{-1.28}^{+1.27}$| | |$-1.06_{-1.00}^{+1.24}$| | |$-1.02_{-1.11}^{+1.43}$| |
|$\sqrt{e}\cos \omega$| | |$0.07_{-0.16}^{+0.19}$| | |$0.04_{-0.20}^{+0.15}$| | |$0.04_{-0.30}^{+0.17}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.09_{-0.15}^{+0.20}$| | |$-0.11_{-0.19}^{+0.13}$| | |$-0.14_{-0.27}^{+0.18}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456574.05_{-1.49}^{+1.53}$| | |$2456570.22_{-7.11}^{+5.98}$| | |$2456564.06_{-31.89}^{+18.67}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$3.18\pm 0.41$| | |$6.97_{-0.89}^{+0.82}$| | |$6.93_{-1.24}^{+1.21}$| |
One-dimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34012_{-0.00046}^{+0.00052}$| | |$37.99_{-0.22}^{+0.16}$| | |$150.28\pm 0.69$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.07_{-0.17}^{+0.15}$| | |$1.06\pm 0.69$| | |$1.55_{-0.38}^{+0.35}$| |
Eccentricity | e | |$0.08_{-0.05}^{+0.06}$| | |$0.23_{-0.19}^{+0.14}$| | |$0.15_{-0.10}^{+0.17}$| | |
Argument of periastron | |$\omega$| | rad | |$0.55_{-0.92}^{+0.95}$| | |$-0.48_{-1.40}^{+1.81}$| | |$-1.05{-0.79}^{+0.96}$| |
|$\sqrt{e}\cos \omega$| | |$0.16_{-0.18}^{+0.13}$| | |$0.13_{-0.40}^{+0.34}$| | |$0.10_{-0.33}^{+0.20}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.11_{-0.18}^{+0.14}$| | |$-0.11_{-0.33}^{+0.46}$| | |$-0.25_{-0.20}^{+0.23}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456573.74_{87}^{+1.05}$| | |$2456571.71_{-9.80}^{+10.5}$| | |$2456571.52\pm 15.3$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.86_{-0.39}^{+0.35}$| | |$3.94_{-2.85}^{+3.02}$| | |$9.72_{-2.56}^{+2.26}$| |
Multidimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34013_{-0.00040}^{+0.00040}$| | |$37.920_{-0.024}^{+0.026}$| | |$150.95_{-0.41}^{+0.45}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.11\pm 0.13$| | |$1.75\pm 0.25$| | |$1.72\pm 0.22$| |
Eccentricity | e | |$0.078_{-0.050}^{+0.058}$| | |$0.22_{-0.11}^{+0.10}$| | |$0.12_{-0.08}^{+0.12}$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
|$\sqrt{e}\cos \omega$| | |$0.17_{-0.18}^{+0.13}$| | |$-0.08_{-0.22}^{+0.23}$| | |$0.01\pm 0.24$| | ||
|$\sqrt{e}\sin \omega$| | |$0.14_{-0.17}^{+0.13}$| | |$0.41_{-0.21}^{+0.13}$| | |$0.21_{-0.19}^{+0.25}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2459003.44 _{ -0.83 }^{+ 1.06}$| | |$2459019.8 _{ -2.7 }^{+ 3.5}$| | |$2459107 _{ -42 }^{+ 24}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.96\pm 0.32$| | |$6.9\pm 1.0$| | |$11.0\pm 1.5$| |
tweaksanalysis ontweaksRVs | |||||
Orbital period | P | days | |$7.34013 \pm 0.00040$| | |$38.06 \pm 0.06$| | |$151.92 \pm 0.44$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.28\pm 0.15$| | |$1.48\pm 0.39$| | |$1.55\pm 0.34$| |
Eccentricity | e | |$0.055 \pm 0.043$| | |$0.11 \pm 0.08$| | |$0.13 \pm 0.11$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
Time of periastron | |$t_{\rm p}$| | BJD | |$2456567.026 \pm 1.72$| | |$2456557.14 \pm 12.5$| | |$2456494.34 \pm 20.1$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$5.43\pm 0.30$| | |$6.33\pm 1.6$| | |$10.05\pm 2.27$| |
Derived parameters | |||||
Semimajor axis | a | au | |$0.0652\pm 0.0005$| | |$0.1951\pm 0.0016$| | |$0.4894\pm 0.0042$| |
Semimajor axis | a | arcsec | 0.0039 | 0.0116 | 0.0291 |
Scaled semimajor axis | |$a/R_\star$| | |$20.65\pm 0.21$| | |$61.79\pm 0.62$| | |$154.97\pm 1.61$| | |
Incident flux | |$F_{\rm inc}$| | |$F_{\rm inc,{\oplus }}$| | |$43.33\pm 2.41$| | |$4.84\pm 0.27$| | |$0.77\pm 0.04$| |
Equilibrium temperature | |$T_{\rm eq}$| | K | |$715\pm 10$| | |$413\pm 6$| | |$261\pm 4$| |
The table displays the results of three Keplerian models, as discussed in sections 7.1, 7.2, and 7.3. The values and uncertainties of each parameter are derived from their respective posterior distributions, with the 50|$^{\rm {th}}$| percentile representing the central value and the 16|$^{\rm {th}}$| to 84|$^{\rm {th}}$| percentile range indicating 1σ uncertainty. Additionally, the derived parameters, as explained in section 7.3, are also included in this table. The maximum equilibrium temperature is calculated assuming an albedo (A|$_{B}$|) of 0 and isotropic re-emission and uniform equilibrium temperature.
Parameter . | Symbol . | Unit . | HD48948 b . | HD48948 c . | HD48948 d . |
---|---|---|---|---|---|
Three Keplerians-only analysis on YV2 RVs | |||||
Orbital period | P | days | |$7.33982_{-0.00085}^{+0.00082}$| | |$37.998_{-0.019}^{+0.018}$| | |$151.12_{-0.49}^{+0.56}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$1.35_{-0.17}^{+0.18}$| | |$1.71_{-0.22}^{+0.20}$| | |$1.09\pm 0.19$| |
Eccentricity | e | |$0.06_{-0.05}^{+0.10}$| | |$0.06_{-0.05}^{+0.09}$| | |$0.10_{-0.09}^{+0.18}$| | |
Argument of periastron | |$\omega$| | rad | |$0.83_{-1.28}^{+1.27}$| | |$-1.06_{-1.00}^{+1.24}$| | |$-1.02_{-1.11}^{+1.43}$| |
|$\sqrt{e}\cos \omega$| | |$0.07_{-0.16}^{+0.19}$| | |$0.04_{-0.20}^{+0.15}$| | |$0.04_{-0.30}^{+0.17}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.09_{-0.15}^{+0.20}$| | |$-0.11_{-0.19}^{+0.13}$| | |$-0.14_{-0.27}^{+0.18}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456574.05_{-1.49}^{+1.53}$| | |$2456570.22_{-7.11}^{+5.98}$| | |$2456564.06_{-31.89}^{+18.67}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$3.18\pm 0.41$| | |$6.97_{-0.89}^{+0.82}$| | |$6.93_{-1.24}^{+1.21}$| |
One-dimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34012_{-0.00046}^{+0.00052}$| | |$37.99_{-0.22}^{+0.16}$| | |$150.28\pm 0.69$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.07_{-0.17}^{+0.15}$| | |$1.06\pm 0.69$| | |$1.55_{-0.38}^{+0.35}$| |
Eccentricity | e | |$0.08_{-0.05}^{+0.06}$| | |$0.23_{-0.19}^{+0.14}$| | |$0.15_{-0.10}^{+0.17}$| | |
Argument of periastron | |$\omega$| | rad | |$0.55_{-0.92}^{+0.95}$| | |$-0.48_{-1.40}^{+1.81}$| | |$-1.05{-0.79}^{+0.96}$| |
|$\sqrt{e}\cos \omega$| | |$0.16_{-0.18}^{+0.13}$| | |$0.13_{-0.40}^{+0.34}$| | |$0.10_{-0.33}^{+0.20}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.11_{-0.18}^{+0.14}$| | |$-0.11_{-0.33}^{+0.46}$| | |$-0.25_{-0.20}^{+0.23}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456573.74_{87}^{+1.05}$| | |$2456571.71_{-9.80}^{+10.5}$| | |$2456571.52\pm 15.3$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.86_{-0.39}^{+0.35}$| | |$3.94_{-2.85}^{+3.02}$| | |$9.72_{-2.56}^{+2.26}$| |
Multidimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34013_{-0.00040}^{+0.00040}$| | |$37.920_{-0.024}^{+0.026}$| | |$150.95_{-0.41}^{+0.45}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.11\pm 0.13$| | |$1.75\pm 0.25$| | |$1.72\pm 0.22$| |
Eccentricity | e | |$0.078_{-0.050}^{+0.058}$| | |$0.22_{-0.11}^{+0.10}$| | |$0.12_{-0.08}^{+0.12}$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
|$\sqrt{e}\cos \omega$| | |$0.17_{-0.18}^{+0.13}$| | |$-0.08_{-0.22}^{+0.23}$| | |$0.01\pm 0.24$| | ||
|$\sqrt{e}\sin \omega$| | |$0.14_{-0.17}^{+0.13}$| | |$0.41_{-0.21}^{+0.13}$| | |$0.21_{-0.19}^{+0.25}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2459003.44 _{ -0.83 }^{+ 1.06}$| | |$2459019.8 _{ -2.7 }^{+ 3.5}$| | |$2459107 _{ -42 }^{+ 24}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.96\pm 0.32$| | |$6.9\pm 1.0$| | |$11.0\pm 1.5$| |
tweaksanalysis ontweaksRVs | |||||
Orbital period | P | days | |$7.34013 \pm 0.00040$| | |$38.06 \pm 0.06$| | |$151.92 \pm 0.44$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.28\pm 0.15$| | |$1.48\pm 0.39$| | |$1.55\pm 0.34$| |
Eccentricity | e | |$0.055 \pm 0.043$| | |$0.11 \pm 0.08$| | |$0.13 \pm 0.11$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
Time of periastron | |$t_{\rm p}$| | BJD | |$2456567.026 \pm 1.72$| | |$2456557.14 \pm 12.5$| | |$2456494.34 \pm 20.1$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$5.43\pm 0.30$| | |$6.33\pm 1.6$| | |$10.05\pm 2.27$| |
Derived parameters | |||||
Semimajor axis | a | au | |$0.0652\pm 0.0005$| | |$0.1951\pm 0.0016$| | |$0.4894\pm 0.0042$| |
Semimajor axis | a | arcsec | 0.0039 | 0.0116 | 0.0291 |
Scaled semimajor axis | |$a/R_\star$| | |$20.65\pm 0.21$| | |$61.79\pm 0.62$| | |$154.97\pm 1.61$| | |
Incident flux | |$F_{\rm inc}$| | |$F_{\rm inc,{\oplus }}$| | |$43.33\pm 2.41$| | |$4.84\pm 0.27$| | |$0.77\pm 0.04$| |
Equilibrium temperature | |$T_{\rm eq}$| | K | |$715\pm 10$| | |$413\pm 6$| | |$261\pm 4$| |
Parameter . | Symbol . | Unit . | HD48948 b . | HD48948 c . | HD48948 d . |
---|---|---|---|---|---|
Three Keplerians-only analysis on YV2 RVs | |||||
Orbital period | P | days | |$7.33982_{-0.00085}^{+0.00082}$| | |$37.998_{-0.019}^{+0.018}$| | |$151.12_{-0.49}^{+0.56}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$1.35_{-0.17}^{+0.18}$| | |$1.71_{-0.22}^{+0.20}$| | |$1.09\pm 0.19$| |
Eccentricity | e | |$0.06_{-0.05}^{+0.10}$| | |$0.06_{-0.05}^{+0.09}$| | |$0.10_{-0.09}^{+0.18}$| | |
Argument of periastron | |$\omega$| | rad | |$0.83_{-1.28}^{+1.27}$| | |$-1.06_{-1.00}^{+1.24}$| | |$-1.02_{-1.11}^{+1.43}$| |
|$\sqrt{e}\cos \omega$| | |$0.07_{-0.16}^{+0.19}$| | |$0.04_{-0.20}^{+0.15}$| | |$0.04_{-0.30}^{+0.17}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.09_{-0.15}^{+0.20}$| | |$-0.11_{-0.19}^{+0.13}$| | |$-0.14_{-0.27}^{+0.18}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456574.05_{-1.49}^{+1.53}$| | |$2456570.22_{-7.11}^{+5.98}$| | |$2456564.06_{-31.89}^{+18.67}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$3.18\pm 0.41$| | |$6.97_{-0.89}^{+0.82}$| | |$6.93_{-1.24}^{+1.21}$| |
One-dimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34012_{-0.00046}^{+0.00052}$| | |$37.99_{-0.22}^{+0.16}$| | |$150.28\pm 0.69$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.07_{-0.17}^{+0.15}$| | |$1.06\pm 0.69$| | |$1.55_{-0.38}^{+0.35}$| |
Eccentricity | e | |$0.08_{-0.05}^{+0.06}$| | |$0.23_{-0.19}^{+0.14}$| | |$0.15_{-0.10}^{+0.17}$| | |
Argument of periastron | |$\omega$| | rad | |$0.55_{-0.92}^{+0.95}$| | |$-0.48_{-1.40}^{+1.81}$| | |$-1.05{-0.79}^{+0.96}$| |
|$\sqrt{e}\cos \omega$| | |$0.16_{-0.18}^{+0.13}$| | |$0.13_{-0.40}^{+0.34}$| | |$0.10_{-0.33}^{+0.20}$| | ||
|$\sqrt{e}\sin \omega$| | |$0.11_{-0.18}^{+0.14}$| | |$-0.11_{-0.33}^{+0.46}$| | |$-0.25_{-0.20}^{+0.23}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2456573.74_{87}^{+1.05}$| | |$2456571.71_{-9.80}^{+10.5}$| | |$2456571.52\pm 15.3$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.86_{-0.39}^{+0.35}$| | |$3.94_{-2.85}^{+3.02}$| | |$9.72_{-2.56}^{+2.26}$| |
Multidimensional GP analysis on YVA RVs | |||||
Orbital period | P | days | |$7.34013_{-0.00040}^{+0.00040}$| | |$37.920_{-0.024}^{+0.026}$| | |$150.95_{-0.41}^{+0.45}$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.11\pm 0.13$| | |$1.75\pm 0.25$| | |$1.72\pm 0.22$| |
Eccentricity | e | |$0.078_{-0.050}^{+0.058}$| | |$0.22_{-0.11}^{+0.10}$| | |$0.12_{-0.08}^{+0.12}$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
|$\sqrt{e}\cos \omega$| | |$0.17_{-0.18}^{+0.13}$| | |$-0.08_{-0.22}^{+0.23}$| | |$0.01\pm 0.24$| | ||
|$\sqrt{e}\sin \omega$| | |$0.14_{-0.17}^{+0.13}$| | |$0.41_{-0.21}^{+0.13}$| | |$0.21_{-0.19}^{+0.25}$| | ||
Time of periastron | |$t_{\rm p}$| | BJD | |$2459003.44 _{ -0.83 }^{+ 1.06}$| | |$2459019.8 _{ -2.7 }^{+ 3.5}$| | |$2459107 _{ -42 }^{+ 24}$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$4.96\pm 0.32$| | |$6.9\pm 1.0$| | |$11.0\pm 1.5$| |
tweaksanalysis ontweaksRVs | |||||
Orbital period | P | days | |$7.34013 \pm 0.00040$| | |$38.06 \pm 0.06$| | |$151.92 \pm 0.44$| |
RV amplitude | K | |$\rm m\, s^{-1}$| | |$2.28\pm 0.15$| | |$1.48\pm 0.39$| | |$1.55\pm 0.34$| |
Eccentricity | e | |$0.055 \pm 0.043$| | |$0.11 \pm 0.08$| | |$0.13 \pm 0.11$| | |
Argument of periastron | |$\omega$| | rad | |$0.68_{-0.77}^{+0.84}$| | |$1.76_{-0.54}^{+0.66}$| | |$4.69_{-1.21}^{+1.19}$| |
Time of periastron | |$t_{\rm p}$| | BJD | |$2456567.026 \pm 1.72$| | |$2456557.14 \pm 12.5$| | |$2456494.34 \pm 20.1$| |
Minimum mass | |$m\sin (i)$| | M|$_{{\oplus }}$| | |$5.43\pm 0.30$| | |$6.33\pm 1.6$| | |$10.05\pm 2.27$| |
Derived parameters | |||||
Semimajor axis | a | au | |$0.0652\pm 0.0005$| | |$0.1951\pm 0.0016$| | |$0.4894\pm 0.0042$| |
Semimajor axis | a | arcsec | 0.0039 | 0.0116 | 0.0291 |
Scaled semimajor axis | |$a/R_\star$| | |$20.65\pm 0.21$| | |$61.79\pm 0.62$| | |$154.97\pm 1.61$| | |
Incident flux | |$F_{\rm inc}$| | |$F_{\rm inc,{\oplus }}$| | |$43.33\pm 2.41$| | |$4.84\pm 0.27$| | |$0.77\pm 0.04$| |
Equilibrium temperature | |$T_{\rm eq}$| | K | |$715\pm 10$| | |$413\pm 6$| | |$261\pm 4$| |
Author notes
STFC Ernest Rutherford Fellow