{"title":"Impact of oxygen fugacity on atmospheric structure and emission spectra of ultra hot rocky exoplanets","authors":"Fabian L. Seidler, Paolo A. Sossi, Simon L. Grimm","doi":"arxiv-2408.16548","DOIUrl":null,"url":null,"abstract":"Atmospheres above lava-ocean planets (LOPs) hold clues as to the properties\nof their interiors, owing to the expectation that the two reservoirs are in\nchemical equilibrium. Here we consider `mineral' atmospheres produced in\nequilibrium with silicate liquids. We treat oxygen fugacity ($f$O$_2$) as an\nindependent variable, together with temperature ($T$) and composition ($X$), to\ncompute equilibrium partial pressures ($p$) of stable gas species at the\nliquid-gas interface. Above this boundary, the atmospheric speciation and the\npressure-temperature structure are computed self-consistently to yield emission\nspectra. We explore a wide array of plausible compositions, oxygen fugacities\n(between 6 log$_{10}$ units below- and above the iron-w\\\"ustite buffer, IW) and\nirradiation temperatures (2000, 2500, 3000 and 3500 K) relevant to LOPs. We\nfind that SiO(g), Fe(g) and Mg(g) are the major species below $\\sim$IW, ceding\nto O$_2$(g) and O(g) in more oxidised atmospheres. The transition between the\ntwo regimes demarcates a minimum in total pressure ($P$). Because $p$ scales\nlinearly with $X$, emission spectra are only modest functions of composition.\nBy contrast, $f$O$_2$ can vary over orders of magnitude, thus causing\ncommensurate changes in $p$. Reducing atmospheres show intense SiO emission,\ncreating a temperature inversion in the upper atmosphere. Conversely, oxidised\natmospheres have lower $p$SiO and lack thermal inversions, with resulting\nemission spectra that mimic that of a black body. Consequently, the intensity\nof SiO emission relative to the background, generated by MgO(g), can be used to\nquantify the $f$O$_2$ of the atmosphere. Depending on the emission spectroscopy\nmetric of the target, deriving the $f$O$_2$ of known nearby LOPs is possible\nwith a few secondary occultations observed by JWST.","PeriodicalId":501209,"journal":{"name":"arXiv - PHYS - Earth and Planetary Astrophysics","volume":"50 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Earth and Planetary Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.16548","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Atmospheres above lava-ocean planets (LOPs) hold clues as to the properties
of their interiors, owing to the expectation that the two reservoirs are in
chemical equilibrium. Here we consider `mineral' atmospheres produced in
equilibrium with silicate liquids. We treat oxygen fugacity ($f$O$_2$) as an
independent variable, together with temperature ($T$) and composition ($X$), to
compute equilibrium partial pressures ($p$) of stable gas species at the
liquid-gas interface. Above this boundary, the atmospheric speciation and the
pressure-temperature structure are computed self-consistently to yield emission
spectra. We explore a wide array of plausible compositions, oxygen fugacities
(between 6 log$_{10}$ units below- and above the iron-w\"ustite buffer, IW) and
irradiation temperatures (2000, 2500, 3000 and 3500 K) relevant to LOPs. We
find that SiO(g), Fe(g) and Mg(g) are the major species below $\sim$IW, ceding
to O$_2$(g) and O(g) in more oxidised atmospheres. The transition between the
two regimes demarcates a minimum in total pressure ($P$). Because $p$ scales
linearly with $X$, emission spectra are only modest functions of composition.
By contrast, $f$O$_2$ can vary over orders of magnitude, thus causing
commensurate changes in $p$. Reducing atmospheres show intense SiO emission,
creating a temperature inversion in the upper atmosphere. Conversely, oxidised
atmospheres have lower $p$SiO and lack thermal inversions, with resulting
emission spectra that mimic that of a black body. Consequently, the intensity
of SiO emission relative to the background, generated by MgO(g), can be used to
quantify the $f$O$_2$ of the atmosphere. Depending on the emission spectroscopy
metric of the target, deriving the $f$O$_2$ of known nearby LOPs is possible
with a few secondary occultations observed by JWST.