Introduction
Titan’s cryovolcanism may extrude, onto its surface, water-ammonia cryolavas [1]. Once flowing on the surface, these water-ammonia solutions can hydrolyze Titan’s organic aerosols to produce amino acids [2]. This is most likely to occur on Titan’s polar regions, where cryovolcanic geological features are most common [3]. Unfortunately, NASA’s upcoming Dragonfly lander is due to explore equatorial locations [4]. The distance between the high-latitude cryovolcanic features and Dragonfly’s equatorial landing site may prevent the lander from detecting cryo-volcanogenic prebiotic molecules.
Herein, we explore the possibility of cryo-volcanogenic amino acids being transported from Titan’s poles to its equator. This transportation scenario requires two steps. First, the molecules are made airborne when gases dissolved in the cryolavas – such as methane, carbon dioxide, and ammonia – coalesce into bubbles which, reaching the cryolava free surface, burst and project droplets into the atmosphere [5]. These water-ammonia aerosols rapidly freeze, encapsulating the prebiotic molecules. Second, the icy aerosols, bearing the prebiotic molecules, are transported by the pole-to-pole atmospheric Hadley circulation. This atmospheric cell upwells at the summer pole and subsequently circulates towards the opposite pole, through the equator. Amino acids produced in the cryovolcanic regions of the seasonal summer pole can thus accumulate on the equatorial sand dunes.
Concerningly, the upper branch of the Hadley circulation may sit as high as 600 km [6], in Titan’s mesosphere, exposing the aerosols to radiation. The success of the two-step transportation thus depends on the survivability of the amino acids to the irradiation felt throughout. We assessed their survivability by comparing the expected photodegradation rates of the amino acids to the pole-to-equator transportation timescale.
Results
Alanine survivability: We irradiated nanolayers of alanine and glycine kept at 90 K and coated with water-ammonia (95:5) ice layers (∼200-nm thick) with a broadband solar simulator (Figure 1). These conditions mimic the environment of the water-ammonia icy aerosols. Based on atmospheric radiative fluxes modeled by us, we calculated an alanine photodegradation half-life of 38.9 ± 8.5 Titan-days in Titan’s mesosphere.
Whilst the velocity of the meridional circulation on Titan’s mesosphere remains to be measured directly, global circulation models estimate it to be within 3–5 cm s−1 [7], [8]. Dynamical timescales of the meridional circulation are obtained by dividing the meridional scale (equivalent to Titan’s radius) by the mean meridional wind velocity. An average meridional wind velocity of 4 cm−1 translates to a dynamical timescale of about 47 Titan-days, similar to the alanine half-life. The similarity between the two timescales implies that half of the alanine molecules would survive their journey from the pole to the equator through Titan’s mesosphere. Nevertheless, as discussed in reference [9], the aerosols are likely subject to faster meridional winds and lower photodegradation rates than we considered, further increasing the expected survivability of alanine.
Glycine survivability and the role of alanine in it: Under the same conditions, the photodegradation half-life of glycine was 535.0 ± 492.7 Titan-days. Being more photostable than alanine, glycine is very likely to survive the meridional transport towards the equator.
We also irradiated nanolayers made up of a 1:1 mixture of alanine and glycine to understand if a close packing of alanine and glycine in the icy aerosols would influence their individual photodegradation behaviors. The presence of alanine decreased the half-life of glycine to 54.2 ± 13.8 Titan-days, in a ten-times faster photodegradation than in the pure glycine sample. This evolution contrasts with that of the alanine photodegradation half-life, which remained the same in the pure alanine and mixture samples (Figure 2). The contrasting behaviors could not be explained by the alanine-glycine sample deposition morphology, infrared signatures, or electronic properties [10].
Through computational methods, we understood that the accelerated photodegradation rate of glycine is due to a reduction in the environment polarity. A slight decrease in environment polarity from εglycine = 18 to εalanine = 15 – produced by the amino acids co-deposition – stabilizes the transition state of the glycine decarboxylation reaction enough to explain large variations in its photo-decarboxylation rate. The alanine photodegradation rate is not, on the other hand, as sensitive to the environment polarity, which is consistent with the unchanged alanine half-life measured experimentally.
Conclusions
Dragonfly may find alanine and glycine molecules produced in the polar cryovolcanic regions. In Titan’s summer pole, after the water-ammonia cryolavas hydrolyze the atmospheric haze into amino acids, the exsolution of dissolved gases can produce icy aerosols encapsulating the amino acids. The icy aerosols would then be transported to the equator and accumulate within the equatorial dunes.
Further, the co-deposition of alanine and glycine induced the latter to photodegrade ten-times faster. This teaches us that by exclusively considering the effects of inorganic surfaces, we disregard a significant fraction of photochemical fates. The effect of organic interactions in the photochemistry of prebiotic molecules deserves further exploration.
Acknowledgements
The authors acknowledge funding by Fundação para a Ciência e Tecnologia (UIDB/00100/2020, UIDP/00100/2020, LA/P/0056/ 2020, UIDB/04565/2020, UIDP/04565/2020, LA/P/ 0140/2020, and 2021.04932.BD), the Ministry of Economics and Energy, Germany (50WB2023 and 50WB2323), the Einstein Foundation Berlin (IPF-2018-469), the Volkswagen Foundation (Freigeist Program), INAF (RSN3 “ORSO” C63C23001250005), the U.S. Department of Energy (DE-AC52-07NA27344), and the European Research Council (804144, ERC-ALIFE).
References
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[2] Brassé, C. et al. Astrobiology 17, 8–26 (2017)
[3] Wood, C. A. et al. J Geophys Res Planets 125, e2019JE006036 (2020)
[4] Barnes, J. W. et al. Planetary Science Journal 2, 130 (2021)
[5] Cordier, D. et al. J Geophys Res Planets 129, e2023JE008248 (2024)
[6] Teanby, N. A. et al. Nature 491, 732–735 (2012)
[7] Lebonnois, S. et al. in Titan 122–157 (Cambridge University Press, 2014)
[8] Achterberg, R. K. et al. Icarus 194, 263–277 (2008)
[9] Gonçalves, D. et al. ACS Earth Space Chem 9, 715–728 (2025)
[10] Gonçalves, D. et al. ACS Earth Space Chem 9, 356–368 (2025)

Figure 1. Sample structure (A, not to scale), irradiation setup (B), and exploded view of the sample in the sample holder (C).

Figure 2. Relative abundances of alanine and glycine plotted against irradiation time, in the three samples: (pure) alanine, (pure) glycine, and alanine-glycine (1:1 mixture).