{"id":477219,"date":"2026-05-10T03:35:16","date_gmt":"2026-05-10T03:35:16","guid":{"rendered":"https:\/\/www.europesays.com\/ie\/477219\/"},"modified":"2026-05-10T03:35:16","modified_gmt":"2026-05-10T03:35:16","slug":"a-single-power-law-for-the-trappist-1-flare-distribution-across-four-orders-of-magnitude-in-energy","status":"publish","type":"post","link":"https:\/\/www.europesays.com\/ie\/477219\/","title":{"rendered":"A Single Power Law For The TRAPPIST-1 Flare Distribution Across Four Orders Of Magnitude In Energy"},"content":{"rendered":"<p>                                    <img decoding=\"async\" src=\"https:\/\/www.europesays.com\/ie\/wp-content\/uploads\/2026\/05\/A-single-power-law.png\" alt=\"A Single Power Law For The TRAPPIST-1 Flare Distribution Across Four Orders Of Magnitude In Energy\"\/><\/p>\n<p>\n                                                                                                            Cumulative flare-frequency distribution of TRAPPIST-1. The cumulative occurrence rate \u03bd(\u2265 ETESS) is shown as a function of TESS-band flare energy. The K2 FFD from this work is shown in blue, the observed JWST FFD in magenta, and the JWST FFD after applying the injection\u2013recovery completeness correction in purple. The light green curve shows the solar soft X-ray flare distribution, derived from the catalog of N. Plutino et al. (2023) and converted to the TESS band assuming Tflare = 9000 K (M. Kretzschmar 2011). The corrected JWST and K2 samples are consistent with a single power law in ETESS over \u223c4 orders of magnitude (dashed black line), with the gray band indicating the 1\u03c3 bootstrap uncertainty. At flare energies above \u223c 1029 erg, the flare occurrence rate of TRAPPIST-1 exceeds that of the Sun. \u2014 astro-ph.SR                                                                                                    <\/p>\n<p><a href=\"https:\/\/astrobiology.com\/trappist-1\" rel=\"nofollow noopener\" target=\"_blank\">TRAPPIST-1 <\/a>is an ultra-cool dwarf that flares frequently. These flares shape the surrounding planets\u2019 high-energy irradiation environments, with consequences for atmospheric chemistry and escape, and they can contaminate transmission spectroscopy of those planets.<\/p>\n<p><img fetchpriority=\"high\" decoding=\"async\" width=\"1024\" height=\"582\" src=\"https:\/\/www.europesays.com\/ie\/wp-content\/uploads\/2026\/05\/Between-eternal-night-and-day-1024x582.png\" alt=\"This artist\u2019s impression displays TRAPPIST-1 and its planets reflected in a surface. The potential for water on each of the worlds is also represented by the frost, water pools, and steam surrounding the scene. \u00a9 NASA\/R. Hurt\/T. Pyle\" class=\"wp-image-38073\"  \/>This artist\u2019s impression displays TRAPPIST-1 and its planets reflected in a surface. The potential for water on each of the worlds is also represented by the frost, water pools, and steam surrounding the scene. \u00a9 NASA\/R. Hurt\/T. Pyle<\/p>\n<p>A quantitative flare-frequency distribution (FFD) spanning the full energy range is therefore essential for both interpreting JWST spectra and modeling the planets\u2019 irradiation histories.<\/p>\n<p>Here we present a unified FFD over four orders of magnitude in energy by jointly analyzing \u224887 hr of JWST\/NIRISS and JWST\/NIRSpec time-series spectroscopy together with \u224874 days of Kepler\/K2 photometry. To enable a consistent comparison across these heterogeneous datasets, we convert all events to energies in the TESS bandpass. For the Kepler-to-TESS conversion we adopt a cooler flare continuum appropriate for ultra-cool dwarfs (Tflare=3500,K).<\/p>\n<p>After correcting for flare-detection sensitivities, the combined JWST+K2 cumulative FFD is consistent with a single power law, N(\u2265ETESS)\u221dE\u2212\u03b2TESS, with \u03b2=0.753 over ETESS\u22431029-1033 erg. The slope of the distribution indicates that the time-averaged flare energy budget is dominated by rare, high-energy events rather than by the more numerous low-energy flares. This bandpass-consistent FFD provides a practical basis for JWST transit-spectroscopy planning and for modeling the flare-driven irradiation environment of the TRAPPIST-1 planets.<\/p>\n<p>Valeriy Vasilyev, Alexander I. Shapiro, Nadiia Kostogryz, Chia-Lung Lin, Greg Kopp, Benjamin V. Rackham, Astrid M. Veronig, Olivia Lim, Julien de Wit, Daniel Apai, Laurent Gizon, Sami K. Solanki<\/p>\n<p>Comments: submitted to ApJL<br \/>Subjects: Solar and Stellar Astrophysics (astro-ph.SR); Earth and Planetary Astrophysics (astro-ph.EP)<br \/>Cite as: arXiv:2605.05468 [astro-ph.SR] (or arXiv:2605.05468v1 [astro-ph.SR] for this version)<br \/><a href=\"https:\/\/doi.org\/10.48550\/arXiv.2605.05468\" target=\"_blank\" rel=\"noreferrer noopener nofollow\">https:\/\/doi.org\/10.48550\/arXiv.2605.05468<\/a><br \/>Focus to learn more<br \/>Submission history<br \/>From: Valeriy Vasilyev<br \/>[v1] Wed, 6 May 2026 21:48:44 UTC (492 KB)<br \/><a href=\"https:\/\/arxiv.org\/abs\/2605.05468\" target=\"_blank\" rel=\"noreferrer noopener nofollow\">https:\/\/arxiv.org\/abs\/2605.05468<\/a><br \/>Astrobiology, heliophysics, space weather,<\/p>\n","protected":false},"excerpt":{"rendered":"Cumulative flare-frequency distribution of TRAPPIST-1. The cumulative occurrence rate \u03bd(\u2265 ETESS) is shown as a function of TESS-band&hellip;\n","protected":false},"author":2,"featured_media":477220,"comment_status":"","ping_status":"","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[77],"tags":[209017,10210,18,18060,19340,209018,71388,11511,203932,19,17,25443,209019,209020,57790,133,98307,51060,209021],"class_list":{"0":"post-477219","1":"post","2":"type-post","3":"status-publish","4":"format-standard","5":"has-post-thumbnail","7":"category-science","8":"tag-astro-ph-sr","9":"tag-atmosphere","10":"tag-eire","11":"tag-exoplanet","12":"tag-flare","13":"tag-flare-frequency-distribution","14":"tag-habitability","15":"tag-heliophysics","16":"tag-https-astrobiology-com-2026-05-radiation","17":"tag-ie","18":"tag-ireland","19":"tag-jwst","20":"tag-jwst-niriss","21":"tag-jwst-nirspec","22":"tag-kepler","23":"tag-science","24":"tag-tess","25":"tag-trappist-1","26":"tag-ultra-cool-dwarfs"},"share_on_mastodon":{"url":"https:\/\/pubeurope.com\/@ie\/116548189095152071","error":""},"_links":{"self":[{"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/posts\/477219","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/comments?post=477219"}],"version-history":[{"count":0,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/posts\/477219\/revisions"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/media\/477220"}],"wp:attachment":[{"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/media?parent=477219"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/categories?post=477219"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.europesays.com\/ie\/wp-json\/wp\/v2\/tags?post=477219"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}