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Atmospheric evaporation in super-Earth exoplanet systems
Spencer R. Moller1, Brendan Miller1, Elena Gallo2, Jason Wright3, Katja Poppenhaeger4
1College of St. Scholastica 2University of Michigan 3Pennsylvania State University 4Queens University Belfast
Can Stellar Activity Transform Planets?
• We wish to investigate how high-energy stellar radiation can
heat, inflate, and evaporate planetary atmospheres of close-in
exoplanets (Lammer+03; see also Jackson+16)
• X-ray observations measure the flux incident at the planet, and
can be used to estimate the mass loss rate (Poppenhaeger+12)
• Test whether inner planets may be transformed into higher-
density cores (Lammer+09; Jackson+10; Lopez+12; Salz+15)
• We consider nearby planets with both transit and radial-velocity
measurements (hence known densities) constructed from the
Exoplanet Orbit Database (Wright+12; Han+14; Figure 1)
We investigate the influence of stellar activity on atmospheric heating and evaporation in four super-Earth exoplanets: HD 97658 b, GJ 1214 b, 55 Cnc e, and CoRoT-7 b. We use X-ray observations of the
host stars to estimate planetary mass loss. We extracted net count rates from a soft band image, converted it to flux using PIMMS for a standard coronal model, calculated the intrinsic stellar luminosity,
and estimated the current-epoch mass-loss rate and the integrated mass lost. Our aim is to determine under what circumstances current super-Earths will have experienced significant mass loss
through atmospheric irradiation over the system lifetime. We hypothesize that closely-orbiting exoplanets receiving the greatest amount of high-energy stellar radiation will also tend to be sculpted into
lower mass and more dense remnant cores.
X-ray data observations
• Use Chandra ACIS-S3 for low background and relatively high soft
X-ray sensitivity; all targets were detected (Figure 2)
• The net counts within a 2’’ extraction radius are used to
determine net rates per ks of 1.51 for 55 Cnc e and 1.22 for HD
97658, which are then converted into flux (at Earth) for a
standard coronal model using PIMMS
• We also use archival Chandra or XMM-Newton data, including for
CoRoT-7 (Poppenhaeger+10, 12; Lalitha+14)
• At distances of 12.34, 150, 12.95 and 21.11 pc, these indicate 0.2-
3 keV X-ray luminosities of log Lx = 26.1, 28.5, 25.8, and 26.5, for
55 Cnc e, CoRoT-7 b, GJ 1214 and HD 97658, respectively
Stellar irradiation and estimated mass loss
• The 0.2-3 keV X-ray fluxes at the planetary orbital radii are, in log values, 2.27,
4.58, 2.04 and 1.25 erg s-1 cm-2 for 55 Cnc e, CoRoT-7 b, GJ 1214 and HD 97658
• We estimate the EUV luminosity using the relationship from Sanz-Forcata+11
(but see Salz+15); our upcoming Swift UV observations will help refine values
• The XUV flux is then used to estimate the current mass loss rate (Figure 3)
following Poppenhaeger+12 and Lalitha+14 (see also Erkaev+07; Jackson+10)
Erkaev, N. V., et al. 2007, A&A, 472, 329
Han, E., Wang, S. X., Wright, J. T., et al. 2014, PASP, 126, 827
Jackson, B., et al. 2010, MNRAS, 407, 910
Jackson, B., et al. 2016, ApJ, 2016, arXiv:1612.04332
Lalitha, S., et al. 2014, ApJ, 790, L11
Lammer, H., et al. 2003, ApJ, 598, L121
Lammer, H., et al. 2009, A&A, 506, 399
We gratefully acknowledge support for this work from Chandra Award GO5-16012X
Figure 1: Nearby (<150 pc) transiting exoplanets with radial-velocity
established masses; only a handful are super Earths
Figure 2: Chandra X-ray images of 55 Cnc e (left) and HD 97658 (right).
Figure 3: Estimated mass loss rates versus Lx values for Super-Earth systems
Figure 4: Integrated mass loss for CoRoT-7 b, GJ 1214 b,55 Cnc e, and HD 97658 b.
Lopez, E. D., Fortney, J. J., & Miller, N. 2012, ApJ, 761, 59
Poppenhaeger, K., et al. 2010, A&A, 515, A98
Poppenhaeger, K., et al. 2012, A&A, 541, A26
Ribas, I., et al. 2005, ApJ, 622, 680
Salz, M., et al. 2015, A&A, 576, 42
Sanz-Forcada, J., et al. 2011, A&A, 532, A6
Wright, J. T., et al. 2012, ApJ, 753, 160
Key:
● Fxuv = incident XUV flux at the
planetary orbit
● G = gravitational constant
● Pp= planetary density
● ε = heating efficiency (0.4)
● K= Roche Lobe overflow (1)
NAME Dists(pc) rates lx Orbit(au) fx fxuv Rho
(g/cm^3)
mdot0 Stellar
ages(Gyr)
HD 97658 b 21.11 0.00122 26.461 0.0796 1.210 2.182e+02 3.44 2.851e+08 6
GJ 1214 b 12.95 XMM 25.820 0.01433 2.058 1.867e+03 1.87 4.488e+9 6
55 Cnc e 12.34 0.00151 26.087 0.01544 2.261 2.7434e+03 4.17 2.957e+09 8
CoRoT-7 b 150 XMM 28.480 0.01719 4.570 1.661e+05 6.20 1.204e+11 1.5

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Detection of an atmosphere around the super earth 55 cancri e
 

Spencer_AAS

  • 1. Atmospheric evaporation in super-Earth exoplanet systems Spencer R. Moller1, Brendan Miller1, Elena Gallo2, Jason Wright3, Katja Poppenhaeger4 1College of St. Scholastica 2University of Michigan 3Pennsylvania State University 4Queens University Belfast Can Stellar Activity Transform Planets? • We wish to investigate how high-energy stellar radiation can heat, inflate, and evaporate planetary atmospheres of close-in exoplanets (Lammer+03; see also Jackson+16) • X-ray observations measure the flux incident at the planet, and can be used to estimate the mass loss rate (Poppenhaeger+12) • Test whether inner planets may be transformed into higher- density cores (Lammer+09; Jackson+10; Lopez+12; Salz+15) • We consider nearby planets with both transit and radial-velocity measurements (hence known densities) constructed from the Exoplanet Orbit Database (Wright+12; Han+14; Figure 1) We investigate the influence of stellar activity on atmospheric heating and evaporation in four super-Earth exoplanets: HD 97658 b, GJ 1214 b, 55 Cnc e, and CoRoT-7 b. We use X-ray observations of the host stars to estimate planetary mass loss. We extracted net count rates from a soft band image, converted it to flux using PIMMS for a standard coronal model, calculated the intrinsic stellar luminosity, and estimated the current-epoch mass-loss rate and the integrated mass lost. Our aim is to determine under what circumstances current super-Earths will have experienced significant mass loss through atmospheric irradiation over the system lifetime. We hypothesize that closely-orbiting exoplanets receiving the greatest amount of high-energy stellar radiation will also tend to be sculpted into lower mass and more dense remnant cores. X-ray data observations • Use Chandra ACIS-S3 for low background and relatively high soft X-ray sensitivity; all targets were detected (Figure 2) • The net counts within a 2’’ extraction radius are used to determine net rates per ks of 1.51 for 55 Cnc e and 1.22 for HD 97658, which are then converted into flux (at Earth) for a standard coronal model using PIMMS • We also use archival Chandra or XMM-Newton data, including for CoRoT-7 (Poppenhaeger+10, 12; Lalitha+14) • At distances of 12.34, 150, 12.95 and 21.11 pc, these indicate 0.2- 3 keV X-ray luminosities of log Lx = 26.1, 28.5, 25.8, and 26.5, for 55 Cnc e, CoRoT-7 b, GJ 1214 and HD 97658, respectively Stellar irradiation and estimated mass loss • The 0.2-3 keV X-ray fluxes at the planetary orbital radii are, in log values, 2.27, 4.58, 2.04 and 1.25 erg s-1 cm-2 for 55 Cnc e, CoRoT-7 b, GJ 1214 and HD 97658 • We estimate the EUV luminosity using the relationship from Sanz-Forcata+11 (but see Salz+15); our upcoming Swift UV observations will help refine values • The XUV flux is then used to estimate the current mass loss rate (Figure 3) following Poppenhaeger+12 and Lalitha+14 (see also Erkaev+07; Jackson+10) Erkaev, N. V., et al. 2007, A&A, 472, 329 Han, E., Wang, S. X., Wright, J. T., et al. 2014, PASP, 126, 827 Jackson, B., et al. 2010, MNRAS, 407, 910 Jackson, B., et al. 2016, ApJ, 2016, arXiv:1612.04332 Lalitha, S., et al. 2014, ApJ, 790, L11 Lammer, H., et al. 2003, ApJ, 598, L121 Lammer, H., et al. 2009, A&A, 506, 399 We gratefully acknowledge support for this work from Chandra Award GO5-16012X Figure 1: Nearby (<150 pc) transiting exoplanets with radial-velocity established masses; only a handful are super Earths Figure 2: Chandra X-ray images of 55 Cnc e (left) and HD 97658 (right). Figure 3: Estimated mass loss rates versus Lx values for Super-Earth systems Figure 4: Integrated mass loss for CoRoT-7 b, GJ 1214 b,55 Cnc e, and HD 97658 b. Lopez, E. D., Fortney, J. J., & Miller, N. 2012, ApJ, 761, 59 Poppenhaeger, K., et al. 2010, A&A, 515, A98 Poppenhaeger, K., et al. 2012, A&A, 541, A26 Ribas, I., et al. 2005, ApJ, 622, 680 Salz, M., et al. 2015, A&A, 576, 42 Sanz-Forcada, J., et al. 2011, A&A, 532, A6 Wright, J. T., et al. 2012, ApJ, 753, 160 Key: ● Fxuv = incident XUV flux at the planetary orbit ● G = gravitational constant ● Pp= planetary density ● ε = heating efficiency (0.4) ● K= Roche Lobe overflow (1) NAME Dists(pc) rates lx Orbit(au) fx fxuv Rho (g/cm^3) mdot0 Stellar ages(Gyr) HD 97658 b 21.11 0.00122 26.461 0.0796 1.210 2.182e+02 3.44 2.851e+08 6 GJ 1214 b 12.95 XMM 25.820 0.01433 2.058 1.867e+03 1.87 4.488e+9 6 55 Cnc e 12.34 0.00151 26.087 0.01544 2.261 2.7434e+03 4.17 2.957e+09 8 CoRoT-7 b 150 XMM 28.480 0.01719 4.570 1.661e+05 6.20 1.204e+11 1.5