Raymond T. Pierrehumbert's research while affiliated with University of Oxford and other places

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Publications (227)


Global Chemical Transport on Hot Jupiters: Insights from the 2D VULCAN Photochemical Model
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February 2024

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23 Reads

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4 Citations

The Astrophysical Journal

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The atmospheric dynamics of tidally locked hot Jupiters is characterized by strong equatorial winds. Understanding the interaction between global circulation and chemistry is crucial in atmospheric studies and interpreting observations. Two-dimensional (2D) photochemical transport models shed light on how the atmospheric composition depends on circulation. In this paper, we introduce the 2D photochemical (horizontal and vertical) transport model, VULCAN 2D, which improves on the pseudo-2D approaches by allowing for nonuniform zonal winds. We extensively validate our VULCAN 2D with analytical solutions and benchmark comparisons. Applications to HD 189733 b and HD 209458 b reveal a transition in mixing regimes: horizontal transport predominates below ∼0.1 mbar, while vertical mixing is more important at higher altitudes above 0.1 mbar. Motivated by the previously inferred carbon-rich atmosphere, we find that HD 209458 b with supersolar carbon-to-oxygen ratio (C/O) exhibits pronounced C 2 H 4 absorption on the morning limb but not on the evening limb, due to horizontal transport from the nightside. We discuss when a pseudo-2D approach is a valid assumption and its inherent limitations. Finally, we demonstrate the effect of horizontal transport in transmission observations and its impact on the morning−evening limb asymmetry with synthetic spectra, highlighting the need to consider global transport when interpreting exoplanet atmospheres.

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Modeling Noncondensing Compositional Convection for Applications to Super-Earth and Sub-Neptune Atmospheres

January 2024

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10 Reads

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1 Citation

The Astrophysical Journal

Compositional convection is atmospheric mixing driven by density variations caused by compositional gradients. Previous studies have suggested that compositional gradients of atmospheric trace species within planetary atmospheres can impact convection and the final atmospheric temperature profile. In this work, we employ 3D convection-resolving simulations using Cloud Model 1 (CM1) to gain a fundamental understanding of how compositional variation influences convection and the final atmospheric state of exoplanet atmospheres. We perform 3D initial value problem simulations of noncondensing compositional convection for Earth-air, H 2 , and CO 2 atmospheres. Conventionally, atmospheric convection is assumed to mix the atmosphere to a final, marginally stable state defined by a unique temperature profile. However, when there is compositional variation within an atmosphere, a continuous family of stable end states is possible, differing in the final state composition profile. Our CM1 simulations are used to determine which of the family of possible compositional end states is selected. Leveraging the results from our CM1 simulations, we develop a dry convective adjustment scheme for use in general circulation models (GCMs). This scheme relies on an energy analysis to determine the final adjusted atmospheric state. Our convection scheme produces results that agree with our CM1 simulations and can easily be implemented in GCMs to improve modeling of compositional convection in exoplanet atmospheres.


Figure 1. Temperature maps at 55 mbar for drag-free models with varying planetary equilibrium temperature from 1800 to 2600 K (from top to bottom panels) and varying tidally synchronized rotation periods implied by stellar ef fecti ve temperatures of 5500, 6000, and 6500 K (from left to right panels). Horizontal winds are represented by streamlines and arrows which are normalized separately for each panel. The rotation period of each model is labelled abo v e each panel. These results were obtained by time-averaging over the last 200-d drag-free model outputs. Temperature colour maps of the same planetary equilibrium temperature (e.g. in each row) share the same colour bar on the right.
Figure 2. Same as Fig. 1 but showing temperature maps at 0.6 mbar.
Figure 3. Zonal-mean zonal winds for drag-free models with varying planetary equilibrium temperature from 1800 to 2600 K (from top to bottom panels) and varying stellar effective temperature of 5500, 6000, and 6500 K (from left to right panels). The rotation period of each model is labelled above each panel. These results were obtained by time-averaging over the last 200-d drag-free model outputs.
Figure 4. Left panel: TP profiles from the sub-stellar region (solid lines) and the antisubstellar region (dotted lines) from models with T eq from 1800 to 2600 K and without drag. Different colours represent different planetary equilibrium temperatures. Profiles near the sub-stellar area were averaged within ±20 • in longitude and latitude (where 0 • is the sub-stellar point); profiles near the antisubstellar point were averaged over longitudes > 160 • and < −160 • and latitudes within ±20 • . Right panel: profiles av eraged o v er the west limbs (solid lines) and east limbs (dashed lines). Profiles of the west limbs were av eraged o v er longitudes > −100 • and < −80 • and latitudes within ±75 • , and profiles of the east limbs were averaged over longitudes > 80 • and < 100 • and latitudes within ±75 • . The 'opening angles' in the transit observations should depend on T eq (Caldas et al. 2019 ; Wardenier, Parmentier & Lee 2022 ), and here we fix the sampling longitudinal regions of the limb profiles merely for a demonstration of the heat transport effects. These results were obtained by time-averaging over the last 200-d simulations. The stellar ef fecti ve temperature of these models is 6500 K.
Figure 5. Radiative heating and cooling profiles (solid lines) and H 2 -H heating and cooling profiles (dotted lines) as a function of pressure for the set of models shown in Fig. 4 . Dashed lines are the H 2 -H heating minus the radiative heating rates, and correspond mostly to the dynamical heating rates by the dry components. The left panel contains the dayside profiles averaged over a domain that is [ ± 60 • , ± 60 • ] of longitude and latitude around the sub-stellar point, and those in the right panel are similarly averaged over a domain around the antisubstellar point.

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Modelling the day–night temperature variations of ultra-hot Jupiters: confronting non-grey general circulation models and observations

January 2024

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16 Reads

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2 Citations

Monthly Notices of the Royal Astronomical Society

Ultra-hot Jupiters (UHJs) are natural laboratories to study extreme physics in planetary atmospheres and their rich observational data sets are yet to be confronted with models with varying complexities at a population level. In this work, we update the general circulation model of Tan & Komacek (2019) to include a non-grey radiative transfer scheme and apply it to simulate the realistic thermal structures, phase-dependent spectra, and wavelength-dependent phase curves of UHJs. We performed grids of models over a large range of equilibrium temperatures and rotation periods for varying assumptions, showing that the fractional day–night brightness temperature differences remain almost constant or slightly increase with increasing equilibrium temperature from the visible to mid-infrared wavelengths. This differs from previous work primarily due to the increasing planetary rotation rate with increasing equilibrium temperature for fixed host star type. Radiative effects of varying atmospheric compositions become more significant in dayside brightness temperature in longer wavelengths. Data-model comparisons of dayside brightness temperatures and phase-curve amplitudes as a function of equilibrium temperature are in broad agreement. Observations show a large scatter compared to models even with a range of different assumptions, indicating significantly varying intrinsic properties in the hot Jupiter population. Our cloud-free models generally struggle to match all observations for individual targets with a single set of parameter choices, indicating the need for extra processes for understanding the heat transport of UHJs.


Figure 1. Outgoing longwave radiation (OLR) and shortwave (SW) absorption as a function of surface pressure. The green curve represents the OLR of an H 2 -He atmosphere on a dry adiabat with surface temperature equal to the critical temperature of water. The blue and orange curves show the SW absorption at different instellations relative to solar (S 0 ) for an M star and G star, respectively.
Figure 3. Same as Figure 2 but for the G-star experiments.
Summary of Runaway Instellations
Comparison of Model OLR with Analytical Calculations with a Dry Gas Opacity of 1.6 × 10 −4 kg m −2
The Runaway Greenhouse Effect on Hycean Worlds

August 2023

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43 Reads

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11 Citations

The Astrophysical Journal

Hycean worlds are a proposed subset of sub-Neptune exoplanets with substantial water inventories, liquid surface oceans, and extended hydrogen-dominated atmospheres favorable for habitability. We aim to quantitatively define the inner edge of the Hycean habitable zone (HZ) using a 1D radiative-convective model. As a limiting case, we model a dry hydrogen–helium envelope above a surface ocean. For a 1 bar (10,100 bar) atmosphere, the hydrogen greenhouse effect alone sets the inner edge of the HZ at 0.216 au (0.58, 3.71 au) for a Sun-like G star and at 0.0364 au (0.110, 0.774 au) for an 3500 K M star. Introducing water vapor into the atmosphere, the runaway greenhouse instellation limit is greatly reduced due to the presence of superadiabatic layers where convection is inhibited. This moves the inner edge of the HZ from ≈1 au for a G star to 1.6 au (3.85 au) for a Hycean world with a H 2 –He inventory of 1 bar (10 bar). For an M star, the inner edge is equivalently moved from 0.17–0.28 au (0.54 au). Our results suggest that most of the current Hycean world observational targets are not likely to sustain a liquid water ocean. We present an analytical framework for interpreting our results, finding that the maximum possible outgoing longwave radiation scales approximately inversely with the dry mass inventory of the atmosphere. We discuss the possible limitations of our 1D modeling and recommend the use of 3D convection-resolving models to explore the robustness of superadiabatic layers.


Are single global warming potential impact assessments adequate for carbon footprints of agri-food systems?

July 2023

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199 Reads

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4 Citations

Environmental Research Letters

Environmental Research Letters

The vast majority of agri-food climate-based sustainability analyses use GWP100 as an impact assessment, usually in isolation; however, in recent years, discussions have criticised the ‘across-the-board’ application of GWP100 in Life Cycle Assessments (LCA), particularly of food systems which generate large amounts of methane (CH4) and considered whether reporting additional and/or alternative metrics may be more applicable to certain circumstances or research questions. This paper reports a sensitivity analysis using a pasture-based beef production system (a producer of high CH4 emissions) as an exemplar to compare various climate impact assessments: CO2-equivalents using GWP100 and GTP100, and ‘CO2-warming-equivalents’ using ‘GWP Star’, or GWP*. The inventory for this system was compiled using data from the UK Research and Innovation (UKRI) National Capability, the North Wyke Farm Platform, in Devon, SW England. LCAs can have an important bearing on: (i) policymakers’ decisions; (ii) farmer management decisions; (iii) consumers’ purchasing habits; and (iv) wider perceptions of whether certain activities can be considered ‘sustainable’ or not; it is, therefore, the responsibility of LCA practitioners and scientists to ensure that subjective decisions are tested as robustly as possible through appropriate sensitivity and uncertainty analyses. We demonstrate herein that the choice of climate impact assessment has dramatic effects on interpretation, with GWP100 and GTP100 producing substantially different results due to their different treatments of CH4 in the context of carbon dioxide (CO2) equivalents. Given its dynamic nature and previously proven strong correspondence with climate models, out of the three assessments covered, GWP* provides the most complete coverage of the temporal evolution of temperature change for different GHG emissions. We extend previous discussions on the limitations of static emission metrics and encourage LCA practitioners to consider due care and attention where additional information or dynamic approaches may prove superior, scientifically speaking, particularly in cases of decision support.


Summary of runaway instellations Expermiment Runaway Limit[W m −2 ] ([S 0 ]) HZ inner edge [AU]
Comparison of model OLR with analytical calculations with a dry gas opacity of 1.6 × 10 −4 kg m −2
The Runaway Greenhouse Effect on Hycean Worlds

April 2023

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48 Reads

Hycean worlds are a proposed subset of sub-Neptune exoplanets with substantial water inventories, liquid surface oceans and extended hydrogen-dominated atmospheres that could be favourable for habitability. In this work, we aim to quantitatively define the inner edge of the Hycean habitable zone using a 1D radiative-convective model. As a limiting case, we model a dry hydrogen-helium envelope above a surface ocean. We find that 10 to 20 bars of atmosphere produces enough greenhouse effect to drive a liquid surface ocean supercritical when forced with current Earth-like instellation. Introducing water vapour into the atmosphere, we show the runaway greenhouse instellation limit is greatly reduced due to the presence of superadiabatic layers where convection is inhibited. This moves the inner edge of the habitable zone from $\approx$ 1 AU for a G-star to 1.6 AU (3.85 AU) for a Hycean world with a H$_2$-He inventory of 1 bar (10 bar). For an M-star, the inner edge is equivalently moved from 0.17 AU to 0.28 AU (0.54 AU). Our results suggest that most of the current Hycean world observational targets are not likely to sustain a liquid water ocean. We present an analytical framework for interpreting our results, finding that the maximum possible OLR scales approximately inversely with the dry mass inventory of the atmosphere. We discuss the possible limitations of our 1D modelling and recommend the use of 3D convection-resolving models to explore the robustness of superadiabatic layers.


The Runaway Greenhouse on Sub-Neptune Waterworlds

February 2023

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33 Reads

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18 Citations

The Astrophysical Journal

The implications of the water vapor runaway greenhouse phenomenon for water-rich sub-Neptunes are developed. In particular, the nature of the postrunaway equilibration process for planets that have an extremely high water inventory is addressed. Crossing the threshold from subrunaway to superrunaway conditions leads to a transition from equilibrated states with cold, deep liquid oceans and deep interior ice-X phases to states with hot supercritical fluid interiors. There is a corresponding marked inflation of radius for a given mass, similar to the runaway greenhouse radius inflation effect noted earlier for terrestrial planets, but in the present case the inflation involves the entire interior of the planet. The calculation employs the AQUA equation-of-state database to simplify the internal structure calculation. Some speculations concerning the effect of H 2 admixture, silicate cores, and hot- versus cold-start evolution trajectories are offered. Observational implications are discussed though the search for the mass–radius signature of the phenomena considered is limited by degeneracies and by lack of data.


Model parameters of HD 80606 b for the SPARC/MITgcm.
The climate and compositional variation of the highly eccentric planet HD 80606 b – the rise and fall of carbon monoxide and elemental sulfur

February 2023

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34 Reads

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5 Citations

Monthly Notices of the Royal Astronomical Society

The gas giant HD 80606 b has a highly eccentric orbit (e ∼ 0.93). The variation due to the rapid shift of stellar irradiation provides a unique opportunity to probe the physical and chemical timescales and to study the interplay between climate dynamics and atmospheric chemistry. In this work, we present integrated models to study the atmospheric responses and the underlying physical and chemical mechanisms of HD 80606 b. We first run three-dimensional general circulation models (GCMs) to establish the atmospheric thermal and dynamical structures for different atmospheric metallicities and internal heat. Based on the GCM output, we then adopted a 1D time-dependent photochemical model to investigate the compositional variation along the eccentric orbit. The transition of the circulation patterns of HD 80606 b matched the dynamics regimes in previous works. Our photochemical models show that efficient vertical mixing leads to deep quench levels of the major carbon and nitrogen species and the quenching behavior does not change throughout the eccentric orbit. Instead, photolysis is the main driver of the time-dependent chemistry. While CH4 dominates over CO through most of the orbits, a transient state of [CO]/[CH4] > 1 after periastron is confirmed for all metallicity and internal heat cases. The upcoming JWST Cycle 1 GO program will be able to track this real-time CH4–CO conversion and infer the chemical timescale. Furthermore, sulfur species initiated by sudden heating and photochemical forcing exhibit both short-term and long-term cycles, opening an interesting avenue for detecting sulfur on exoplanets.


The runaway greenhouse on subNeptune waterworlds

December 2022

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3 Reads

The implications of the water vapor runaway greenhouse phenomenon for water-rich subNeptunes are developed. In particular, the nature of the post-runaway equilibration process for planets that have an extremely high water inventory is addressed. Crossing the threshold from sub-runaway to super-runaway conditions leads to a transition from equilibrated states with cold deep liquid oceans and deep interior ice-X phases to states with hot supercritical fluid interiors. There is a corresponding marked inflation of radius for a given mass, similar to the runaway greenhouse radius inflation effect noted earlier for terrestrial planets, but in the present case the inflation involves the entire interior of the planet. The calculation employs the AQUA equation of state database to simplify the internal structure calculation. Some speculations concerning the effect of $\mathrm{H_2}$ admixture, silicate cores and hot vs. cold start evolution trajectories are offered. Observational implications are discussed, though the search for the mass-radius signature of the phenomena considered is limited by degeneracies and by lack of data.



Citations (63)


... To simulate this scenario, we feed the equatorial abundances and wind speeds from the GCMs into the 2D VULCAN photochemical model (Tsai et al. 2024). For both the weak-drag and the strong-drag model, we find that the nightside H 2 O abundances only change substantially (by up to 3 orders of magnitude) in small regions of the atmosphere around 10 −5 bar (see Fig. 15 in Appendix A). ...

Reference:

Phase-resolving the absorption signatures of water and carbon monoxide in the atmosphere of the ultra-hot Jupiter WASP-121b with GEMINI-S/IGRINS
Global Chemical Transport on Hot Jupiters: Insights from the 2D VULCAN Photochemical Model

The Astrophysical Journal

... The SPARC/-MITgcm was first described by Showman et al. (2009). Since, it has been widely used to study the atmospheric physics and chemistry of (ultra-)hot Jupiters (e.g., Fortney et al. 2010;Showman et al. 2013;Kataria et al. 2013;Steinrueck et al. 2021;Tan et al. 2024). ...

Modelling the day–night temperature variations of ultra-hot Jupiters: confronting non-grey general circulation models and observations

Monthly Notices of the Royal Astronomical Society

... But for this balance to hold, convection itself, which can be hindered by other dynamical processes, needs to be able to develop. For example, when there is a compositional gradient in the atmosphere -whether it be caused by condensation or chemical reactions -the resulting mean molecular weight gradient in the gas can affect the thermal gradient needed to initiate convection (Nakajima et al. 2000;Garaud 2018;Daley-Yates et al. 2021;Habib & Pierrehumbert 2024). In a more extreme fashion, when the atmosphere contains enough of a condensable species (hereafter referred to as vapor) that is heavier than the non-condensable background gas (hereafter referred to as air), condensation can completely suppress convection, whatever the thermal gradient (Guillot 1995;Leconte et al. 2017;Markham et al. 2022). ...

Modeling Noncondensing Compositional Convection for Applications to Super-Earth and Sub-Neptune Atmospheres

The Astrophysical Journal

... In fact, the simulation enters runaway greenhouse, which forces the ocean to evaporate and the surface temperatures to rise. This result is compatible with previous calculations of the runaway greenhouse limit for hycean planets (Innes et al. 2023). As the simulation progresses, the amount of water vapor in the atmosphere increases at all altitude layers. ...

The Runaway Greenhouse Effect on Hycean Worlds

The Astrophysical Journal

... GWP* has also been criticized e.g., for being a climate model rather than a metric (Meinshausen and Nicholls, 2022) and for being sensitive to historical emissions of SLCPs, thereby raising questions of equity and fairness when applied on national levels rather than at a global level Schleussner et al., 2019). Since 2021, applications of GWP* in various forms have started to emerge in studies on food and agriculture (e.g., Lesschen, 2021;Pérez-Domínguez et al., 2021;Ridoutt et al., 2022a;McAuliffe et al., 2023;McCabe et al., 2023;Pressman et al., 2023). However, the application of the method is not straight forward and Lesschen (2021) concludes that due to the different weighting of CH 4 , the choice of using GWP 100 (global warming) or GWP* (temperature impact) in the assessment can highly affect which climate mitigation policy options are seen as most beneficial, especially under stringent mitigation scenarios with large cuts of CH 4 emissions. ...

Are single global warming potential impact assessments adequate for carbon footprints of agri-food systems?
Environmental Research Letters

Environmental Research Letters

... These temperate sub-Neptunes have sparked great interest in atmospheric characterization and the assessment of habitability. Given suitable climate conditions (Innes et al. 2023;Pierrehumbert 2023), these water-rich worlds could host surface water oceans below hydrogen-rich atmospheresrecently referred to as "Hycean" (Hydrogen ocean) worlds Nixon & Madhusudhan 2021). Promisingly, their hydrogen-rich envelopes are more favorable for atmospheric characterization in transmission observations due to large scale heights, compared to the higher molecular weight N 2 -or CO 2 -dominated atmospheres. ...

The Runaway Greenhouse on Sub-Neptune Waterworlds

The Astrophysical Journal

... Due to efficient heat redistribution, the nightside on WASP-39b is not cool enough for polysulfur to grow beyond S 2 , nor for S 8 to condense (see Zahnle et al. 2016;Tsai et al. 2023a). The laboratory experiments of Reed et al. (2020) suggest that organosulfur hazes can form in Archean-like atmospheres when CH 4 and unsaturated hydrocarbon are present, but we find that the global abundances of CH 4 and C 2 H x hydrocarbons are significantly reduced when zonal winds are considered. ...

The climate and compositional variation of the highly eccentric planet HD 80606 b – the rise and fall of carbon monoxide and elemental sulfur

Monthly Notices of the Royal Astronomical Society

... Consequently, the instellation at which the runaway greenhouse transition occurs is aptly considered to be the inner boundary of the habitable zone (e.g., Ramirez 2018;. Its prevalent definition refers to the possibility of a sustained liquid water body on the surface of an Earth-like planet with an oxidized CO 2 /H 2 O/N 2 -rich atmosphere (Kasting et al. 1993;Kopparapu et al. 2013Kopparapu et al. , 2014; its exact spatial location and extent may be strongly influenced by the interior and atmosphere oxidation state and resulting atmosphere composition (Pierrehumbert & Gaidos 2011;Ramirez & Kaltenegger 2017, 2018Katyal et al. 2019;Graham & Pierrehumbert 2020;Graham et al. 2022;Hakim et al. 2023). The fundamental concept of a habitable zone dates back centuries (Newton 1687;Whewell 1858;Shapley 1953;Huang 1959), and its modern form has proven popular in the planetary literature 1 . ...

CO2 Ocean Bistability on Terrestrial Exoplanets

... The new line list has been MARVELized and also provides much broader wavelength coverage as it also covers rovibronic transitions. Like MgO, SiO has been suggested as one of the important sources of opacity in lava planets as well as sub-Neptunes [181,186,189,190,398,403,404]. Cross sections of SiO computed using SiOUVenIR are shown in Fig. 2. ...

The impact of ultraviolet heating and cooling on the dynamics and observability of lava planet atmospheres
  • Citing Article
  • May 2022

Monthly Notices of the Royal Astronomical Society

... Due to the non-inflated nature of WASP-43b, we chose an internal temperature of T int = 150 K. For this study, we perform three simulations: one cloudless assuming chemical equilibrium, one cloudless with non-equilibrium kinetic chemistry (using the minichem module Tsai et al. (2022); Lee et al. (2023)) and one with tracer clouds following Tan & Showman (2021) with non-equilibrium chemistry. We take the best fit log-normal distribution cloud particle parameters from the MITgcm simulations from Bell et al. (2024) (r med = 2 µm, σ = 2) with an amorphous MgSiO 3 composition. ...

A mini-chemical scheme with net reactions for 3D general circulation models. I. Thermochemical kinetics

Astronomy and Astrophysics