<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom"><channel><title>Prompts | Olivier Durif</title><link>https://olivier.durif.fr/prompts/</link><atom:link href="https://olivier.durif.fr/prompts/index.xml" rel="self" type="application/rss+xml"/><description>Prompts</description><generator>HugoBlox Kit (https://hugoblox.com)</generator><language>fr-FR</language><lastBuildDate>Tue, 29 Sep 2026 00:00:00 +0000</lastBuildDate><image><url>https://olivier.durif.fr/media/icon.svg</url><title>Prompts</title><link>https://olivier.durif.fr/prompts/</link></image><item><title>Hypothèse du biais expérimental</title><link>https://olivier.durif.fr/prompts/low-temperature-bias-hypothesis/</link><pubDate>Tue, 29 Sep 2026 00:00:00 +0000</pubDate><guid>https://olivier.durif.fr/prompts/low-temperature-bias-hypothesis/</guid><description>&lt;div class="highlight"&gt;&lt;pre tabindex="0" class="chroma"&gt;&lt;code class="language-text" data-lang="text"&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;QUESTION
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Is this statement true?
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;&amp;#34;Gas-phase reactions at very low temperature do not get faster and faster as temperature decreases. The reported increase is a historical experimental bias.&amp;#34;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;ANSWER FORMAT
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Line 1: YES (the statement is true) or NO (the statement is false). One word.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Use UNDECIDABLE only if you can name the one experiment that would decide it.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Then, in this order and nothing else:
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;1. Strongest evidence for your answer: one study, with authors, year, journal, DOI, and &amp;#34;read&amp;#34;, &amp;#34;abstract only&amp;#34; or &amp;#34;not read&amp;#34;.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;2. Strongest evidence against your answer: same format.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;3. Confidence, 0 to 100 %.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;4. The one fact that would flip your answer.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Maximum 200 words. No survey of the field. No hedging.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;Never invent a reference: write &amp;#34;unverified&amp;#34; if you cannot check it.
&lt;/span&gt;&lt;/span&gt;&lt;/code&gt;&lt;/pre&gt;&lt;/div&gt;&lt;h2 id="exécutions"&gt;Exécutions&lt;/h2&gt;
&lt;p&gt;&lt;strong&gt;GPT-6 Pro (interface web), 2026-09-29&lt;/strong&gt;&lt;/p&gt;
&lt;div class="run-frame"&gt;
&lt;p&gt;NO&lt;/p&gt;
&lt;ol&gt;
&lt;li&gt;
&lt;p&gt;&lt;strong&gt;Strongest evidence for NO:&lt;/strong&gt; Hickson, Loison, Nuñez-Reyes and Méreau (2016), &lt;em&gt;Journal of Physical Chemistry Letters&lt;/em&gt;, DOI: &lt;strong&gt;10.1021/acs.jpclett.6b01637&lt;/strong&gt; — &lt;strong&gt;read&lt;/strong&gt;, including supplementary information. For C + H₂O, cooling from 106 to 52 K increases measured removal approximately 7.6-fold. Using the measured H-product yield, the inferred product-forming coefficient at 52 K exceeds even the &lt;strong&gt;total&lt;/strong&gt; removal coefficient at 106 K approximately 4.4-fold. &lt;strong&gt;Inference:&lt;/strong&gt; nonreactive complex stabilization alone cannot explain this acceleration.&lt;/p&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;p&gt;&lt;strong&gt;Strongest evidence against NO:&lt;/strong&gt; Lucas, Guillaume, Heard and Lehman (2024), &lt;em&gt;Journal of Chemical Physics&lt;/em&gt;, DOI: &lt;strong&gt;10.1063/5.0220774&lt;/strong&gt; — &lt;strong&gt;read&lt;/strong&gt;. OCS spectroscopy gives a rotational temperature of &lt;strong&gt;49.5 K&lt;/strong&gt;, versus &lt;strong&gt;32 ± 3 K&lt;/strong&gt; from Pitot measurements. This establishes a thermometry discrepancy supporting concern about systematic errors; it does &lt;strong&gt;not&lt;/strong&gt; demonstrate an artificial rate increase.&lt;/p&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;p&gt;&lt;strong&gt;Confidence:&lt;/strong&gt; &lt;strong&gt;95%&lt;/strong&gt;, subjective confidence in rejecting the blanket artifact explanation.&lt;/p&gt;
&lt;/li&gt;
&lt;li&gt;
&lt;p&gt;&lt;strong&gt;The fact that would flip my answer:&lt;/strong&gt; Demonstration of a common experimental bias that quantitatively eliminates the reported accelerations—including product-resolved results—when temperatures, concentrations and product yields are independently calibrated.&lt;/p&gt;
&lt;/li&gt;
&lt;/ol&gt;
&lt;/div&gt;
&lt;h2 id="commentaire-personnel"&gt;Commentaire personnel&lt;/h2&gt;
&lt;p&gt;C&amp;rsquo;est une réponse logique à partir de la littérature scientifique.&lt;/p&gt;
&lt;p&gt;Mais, le C + H₂O cité par ChatGPT en n°1 pour défendre le NO est l&amp;rsquo;exemple typique qui devrait nous faire dire YES. Anecdote vécue pendant ma thèse : avec mon directeur de thèse Sébastien Le Picard, un ancien thésard du laboratoire devenu professeur à la West Virginia University, Fabien Goulet, et K. C. Caster, nous avons mesuré C + H₂O en tube à écoulement, vers 300 °C, au synchrotron ALS de Berkeley. Sollicités par les deux camps : Kevin Hickson, l&amp;rsquo;expérimentateur qui a publié C + H₂O à très basse température, et
, un théoricien qui soutenait que cette réaction ne marche pas à très basse température. Au spectromètre de masse, nous avons vu directement que la réaction ne se produit pas à 300 °C. Même l&amp;rsquo;étude « produits détectés » de référence peut décrire une réaction qui n&amp;rsquo;existe pas. Alors oui, ce n°1 devrait nous faire dire YES.&lt;/p&gt;
&lt;p&gt;Sur le point 2 : ChatGPT n&amp;rsquo;a pas encore été capable de relier l&amp;rsquo;augmentation de la température avec la chute de densité. Je n&amp;rsquo;ai aucun doute que cela arrivera bientôt et qu&amp;rsquo;il sera capable de faire ces connexions qui vont incroyablement changer la science.&lt;/p&gt;</description></item><item><title>Prompt pour trouver des contre-exemples dans la littérature scientifique à l'universalité de mon hypothèse d'une erreur d'interprétation des résultats CRESU. Tentative pour me donner tort et tenter de sauver la technique !</title><link>https://olivier.durif.fr/prompts/gas-phase-literature-reviewer/</link><pubDate>Tue, 29 Sep 2026 00:00:00 +0000</pubDate><guid>https://olivier.durif.fr/prompts/gas-phase-literature-reviewer/</guid><description>&lt;p&gt;Un prompt de référence : je le garde ici comme trace — la question exacte, figée — pour la retenter plus tard avec de nouveaux modèles, dont les réponses devraient s&amp;rsquo;améliorer. Il porte sur mon affirmation — les réactions en phase gazeuse à très basse température ne sont pas de plus en plus rapides, c&amp;rsquo;est un biais expérimental historique : l&amp;rsquo;augmentation apparente de la réactivité lorsque T baisse est en fait due à une chute de densité. L&amp;rsquo;idée ici est de chercher des contre-exemples à l&amp;rsquo;affirmation que je crois fausse mais malheureusement « orthodoxe » (les cinétiques réactionnelles augmentent quand la température baisse) afin de (dé)montrer que parfois les CRESU ont pu obtenir des résultats « censés », des exceptions à cette folie !&lt;/p&gt;
&lt;div class="highlight"&gt;&lt;pre tabindex="0" class="chroma"&gt;&lt;code class="language-text" data-lang="text"&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;ROLE
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;You are a rigorous literature reviewer in gas-phase chemical kinetics. You never invent references. If you cannot verify something, say so explicitly. Do not assume the claim below is true or false: test it.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;CLAIM TO TEST
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;&amp;#34;In uniform supersonic flow (CRESU-type) kinetics, below ~100 K, the measured bimolecular rate coefficient of neutral-neutral gas-phase reactions increases as temperature decreases, in essentially every system studied, with no exception.&amp;#34;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;TASKS (answer each separately, in this order)
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;1. COUNTEREXAMPLES. Find published CRESU / uniform-supersonic-flow studies (any detection: LIF, chirped-pulse, mass spectrometry, cw-CRDS, frequency comb, etc.) in which a neutral-neutral rate coefficient measured between ~10 and ~150 K is:
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt; (a) flat, or (b) decreasing with decreasing temperature, or (c) not measurable because too slow.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt; For each hit give: authors, year, journal, DOI, reaction, temperature range, what the temperature dependence actually is, and whether the authors report a barrier.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;2. BARRIER TEST. The strongest evidence would be a reaction where theory (ab initio / TST / master equation) predicts an entrance barrier, yet CRESU data show an increase at low T. Find such cases, or state that you found none. For each: the reaction, the theoretical barrier height with reference, the CRESU data reference, the size of the disagreement.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;3. SELECTION BIAS. Estimate, as concretely as the literature allows, what fraction of CRESU-studied reactions are barrierless/capture-type versus barrier-limited. Is the statement &amp;#34;no exception&amp;#34; mostly a consequence of only fast reactions being studied at low T? Cite reviews or compilations (e.g. kinetic databases, review articles on CRESU/low-temperature kinetics) that support or contradict this.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;4. STEELMAN THE OPPOSITE. List the three best arguments a specialist would make to defend that the low-T increase is physical (tunnelling, pre-reactive complexes, capture theory), with references.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;OUTPUT RULES
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;- Separate clearly: (i) facts read in a source, (ii) your inference, (iii) unknown.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;- Every factual statement carries a reference with DOI. If you could not open the paper (paywall), write &amp;#34;not read, abstract only&amp;#34; or &amp;#34;not read&amp;#34;.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;- Do not fill gaps with plausible-sounding citations. &amp;#34;I found no counterexample&amp;#34; is an acceptable answer, but state which databases and search terms you used.
&lt;/span&gt;&lt;/span&gt;&lt;span class="line"&gt;&lt;span class="cl"&gt;- End with a table: reaction | T range | dependence | barrier predicted? | reference | how sure (read / abstract only / not verified).
&lt;/span&gt;&lt;/span&gt;&lt;/code&gt;&lt;/pre&gt;&lt;/div&gt;&lt;h2 id="exécutions"&gt;Exécutions&lt;/h2&gt;
&lt;p&gt;&lt;strong&gt;GPT-6 Pro (interface web), 2026-09-29&lt;/strong&gt; — première exécution : contre-exemples publiés trouvés (N+CN décroissant ; O+OH, N+OH plats ; CN+H₂S plat sur 11,7–45,5 K ; F+H₂ en plateau malgré sa barrière ; CN+C₂H₂/C₂H₄ en retournement ; NH₂+H₂CO trop lent) ; aucune barrière d&amp;rsquo;&lt;em&gt;entrée&lt;/em&gt; positive vérifiée avec augmentation.&lt;/p&gt;
&lt;details&gt;
&lt;summary&gt;Afficher la réponse complète (anglais)&lt;/summary&gt;
&lt;h2 id="1-counterexamples"&gt;1. Counterexamples&lt;/h2&gt;
&lt;p&gt;&lt;strong&gt;The literal &amp;ldquo;no exception&amp;rdquo; claim is contradicted by the published literature.&lt;/strong&gt; Particularly clear examples are the approximately temperature-independent CN + H₂S measurements at 11.7–45.5 K and the positive temperature dependence reported for N + CN. Their experimental references are, respectively, DOI &lt;strong&gt;10.3847/1538-4357/ae421d&lt;/strong&gt; and DOI &lt;strong&gt;10.1073/pnas.1200017109&lt;/strong&gt;.&lt;/p&gt;
&lt;p&gt;Here, &lt;strong&gt;&amp;ldquo;flat&amp;rdquo; means no resolved temperature dependence within the experimental uncertainties&lt;/strong&gt;, not proof that &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;dk/dT&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; is exactly zero. An upper limit is a different category: it establishes limited reactivity under the measurement conditions, but does not establish a temperature derivative.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Search scope.&lt;/strong&gt; I checked publisher records, PubMed/PMC, arXiv, author manuscripts, and NIST/KIDA records, using combinations of &amp;ldquo;CRESU,&amp;rdquo; &amp;ldquo;uniform supersonic,&amp;rdquo; &amp;ldquo;temperature independent,&amp;rdquo; &amp;ldquo;positive temperature dependence,&amp;rdquo; &amp;ldquo;upper limit,&amp;rdquo; &amp;ldquo;barrier,&amp;rdquo; and reaction-specific searches. This is a verified set of hits, not an exhaustive census. Access limitations are identified below.&lt;/p&gt;
&lt;p&gt;All numerical bimolecular coefficients below are in &lt;strong&gt;cm³ molecule⁻¹ s⁻¹&lt;/strong&gt;.&lt;/p&gt;
&lt;h3 id="1a-n--cn--n--c-decreases-on-cooling"&gt;1A. N + CN → N₂ + C: decreases on cooling&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; J. Daranlot, U. Hincelin, A. Bergeat, M. Costes, J.-C. Loison, V. Wakelam and K. M. Hickson, &lt;strong&gt;2012&lt;/strong&gt;, &lt;em&gt;PNAS&lt;/em&gt;, &amp;ldquo;Elemental nitrogen partitioning in dense interstellar clouds.&amp;rdquo; &lt;strong&gt;DOI: 10.1073/pnas.1200017109.&lt;/strong&gt; &lt;strong&gt;Read: full text.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read:&lt;/strong&gt; Measurements cover &lt;strong&gt;56–296 K&lt;/strong&gt;, including Laval-nozzle measurements at 56, 87, 152 and 169 K. The authors report approximately &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;9&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;9\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; at 296 K and &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;5&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;5\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; at 56 K, with the fit&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;8.8&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;3.8&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mn&gt;300&lt;/mn&gt;&lt;msup&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mrow&gt;&lt;mn&gt;0.42&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.09&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k(T)=(8.8\pm3.8)\times10^{-11}(T/300)^{0.42\pm0.09}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;Thus the reported fitted dependence is &lt;strong&gt;positive in temperature&lt;/strong&gt;, meaning slower on cooling. These are relative-rate measurements using N + OH as reference. The paper&amp;rsquo;s 10 K value is an &lt;strong&gt;extrapolation&lt;/strong&gt;, not a measurement.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Barrier status:&lt;/strong&gt; An associated quantum-capture calculation reproduces the positive temperature dependence: J. Ma, H. Guo and R. Dawes, &lt;strong&gt;2012&lt;/strong&gt;, &lt;em&gt;PCCP&lt;/em&gt;, &lt;strong&gt;DOI: 10.1039/C2CP41621B&lt;/strong&gt;. &lt;strong&gt;Not read, abstract only.&lt;/strong&gt; I would not infer a positive entrance barrier merely from the positive temperature exponent.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Qualification:&lt;/strong&gt; The exponent is fitted across 56–296 K; it should not be presented as an independently measured local derivative throughout 10–100 K.&lt;/p&gt;
&lt;h3 id="1b-op--oh--o--h-approximately-flat"&gt;1B. O(³P) + OH → O₂ + H: approximately flat&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; D. Carty, A. Goddard, S. P. K. Köhler, I. R. Sims and I. W. M. Smith, &lt;strong&gt;2006&lt;/strong&gt;, &lt;em&gt;Journal of Physical Chemistry A&lt;/em&gt;, &amp;ldquo;Kinetics of the radical–radical reaction … at temperatures down to 39 K.&amp;rdquo; &lt;strong&gt;DOI: 10.1021/jp054429u.&lt;/strong&gt; &lt;strong&gt;Not read, abstract only.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read in the abstract:&lt;/strong&gt; CRESU measurements over &lt;strong&gt;39–142 K&lt;/strong&gt; give approximately&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;3.5&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;1.0&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k=(3.5\pm1.0)\times10^{-11},
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;with little temperature variation and no observed pressure dependence. This directly qualifies as an experimentally approximately flat case.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Barrier status:&lt;/strong&gt; I did not verify a numerical barrier height from the original paper. Its abstract does not provide one; I therefore do not assign one here.&lt;/p&gt;
&lt;h3 id="1c-n--oh--no--h-approximately-flat"&gt;1C. N + OH → NO + H: approximately flat&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; J. Daranlot et al., &lt;strong&gt;2011&lt;/strong&gt;, &lt;em&gt;Science&lt;/em&gt;, &amp;ldquo;Revealing atom-radical reactivity at low temperature through the N + OH reaction.&amp;rdquo; &lt;strong&gt;DOI: 10.1126/science.1213789.&lt;/strong&gt; &lt;strong&gt;Not read, abstract only.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts:&lt;/strong&gt; The original abstract describes a &lt;strong&gt;barrierless&lt;/strong&gt; reaction investigated using a Laval-nozzle apparatus. The authors&amp;rsquo; subsequent account reports approximately constant experimental coefficients over &lt;strong&gt;56–296 K&lt;/strong&gt;, around &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;4.5&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;4.5\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. That account is A. Bergeat, J. Daranlot, K. M. Hickson and M. Costes, &lt;strong&gt;2012&lt;/strong&gt;, &lt;em&gt;EAS Publications Series&lt;/em&gt;, &lt;strong&gt;DOI: 10.1051/eas/1258046&lt;/strong&gt;. &lt;strong&gt;Read: full account, including the experimental figure.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Interpretation:&lt;/strong&gt; This is another flat measured dependence, including measurements below 100 K—not evidence that its rate must remain constant at still lower, unmeasured temperatures.&lt;/p&gt;
&lt;h3 id="1d-cn--hs-approximately-flat-entirely-below-50-k"&gt;1D. CN + H₂S: approximately flat entirely below 50 K&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; M. Antiñolo, F. Martínez, D. González, A. Lema-Saavedra, E. Martínez-Núñez, A. Fernández-Ramos, M. Agúndez, J. Cernicharo and E. Jiménez, &lt;strong&gt;2026&lt;/strong&gt;, &lt;em&gt;Astrophysical Journal&lt;/em&gt;, &amp;ldquo;Revealing that the Gas-phase Reaction of CN with H₂S Can Be a Source of HSCN in Interstellar Molecular Clouds.&amp;rdquo; &lt;strong&gt;DOI: 10.3847/1538-4357/ae421d.&lt;/strong&gt; &lt;strong&gt;Read: author-posted full text.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read:&lt;/strong&gt; Pulsed-CRESU/PLP-LIF measurements cover &lt;strong&gt;11.7–45.5 K&lt;/strong&gt;. The authors report negligible temperature dependence, with coefficients around &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;4\times10^{-10}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. For example:&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;11.7&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;K&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;3.59&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.42&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;mspace width="2em"/&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;45.5&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;K&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;3.96&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.51&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k(11.7\,{\rm K})=(3.59\pm0.42)\times10^{-10},
\qquad
k(45.5\,{\rm K})=(3.96\pm0.51)\times10^{-10}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;Their calculations predict a weak inverse temperature dependence, but the experimental results are described as nearly temperature-independent.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Barrier status:&lt;/strong&gt; The calculated dominant pathway has &lt;strong&gt;submerged transition states&lt;/strong&gt;, not a positive activation barrier above the separated reactants. HSCN + H is the &lt;strong&gt;theoretically assigned&lt;/strong&gt; dominant product channel; the kinetic measurement follows CN removal.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Inference:&lt;/strong&gt; This is an especially relevant counterexample because the entire measured interval lies well below 100 K and involves a radical plus a stable molecule.&lt;/p&gt;
&lt;h3 id="1e-f--h--hf--h-a-low-temperature-plateau-despite-a-barrier"&gt;1E. F + H₂ → HF + H: a low-temperature plateau despite a barrier&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; M. Tizniti, S. D. Le Picard, F. Lique, C. Berteloite, A. Canosa, M. H. Alexander and I. R. Sims, &lt;strong&gt;2014&lt;/strong&gt;, &lt;em&gt;Nature Chemistry&lt;/em&gt;, &amp;ldquo;The rate of the F + H₂ reaction at very low temperatures.&amp;rdquo; &lt;strong&gt;DOI: 10.1038/nchem.1835.&lt;/strong&gt; &lt;strong&gt;Read: author-posted paper and supplementary material.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read:&lt;/strong&gt; For normal H₂, the CRESU measurements give&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;11.3&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;K&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;2.48&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;1.90&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;mspace width="2em"/&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;20.4&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;K&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;2.18&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.72&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k(11.3\,{\rm K})=(2.48\pm1.90)\times10^{-13},
\qquad
k(20.4\,{\rm K})=(2.18\pm0.72)\times10^{-13}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;These are consistent with a &lt;strong&gt;plateau&lt;/strong&gt;, not a resolved low-temperature acceleration. The reaction has a positive barrier of roughly &lt;strong&gt;&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;E&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mo&gt;∼&lt;/mo&gt;&lt;mn&gt;800&lt;/mn&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;E/R\sim800&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; K&lt;/strong&gt;, or &lt;strong&gt;6.6 kJ mol⁻¹&lt;/strong&gt;. Quantum calculations describe the low-temperature behaviour.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Important qualifications:&lt;/strong&gt; The paper&amp;rsquo;s 77 and 295 K measurements used &lt;strong&gt;subsonic flow&lt;/strong&gt;, so the large decrease between 77 and 20 K is not an exclusively CRESU temperature series. Also, these measurements concern &lt;strong&gt;normal H₂&lt;/strong&gt;, with its approximately 3:1 ortho:para mixture, not equilibrium rotational populations at 11 K.&lt;/p&gt;
&lt;h3 id="1f-cn--ch-and-cn--ch-reported-turnover-below-approximately-44-k"&gt;1F. CN + C₂H₂ and CN + C₂H₄: reported turnover below approximately 44 K&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; I. R. Sims, J.-L. Queffelec, D. Travers, B. R. Rowe, L. B. Herbert, J. Karthäuser and I. W. M. Smith, &lt;strong&gt;1993&lt;/strong&gt;, &lt;em&gt;Chemical Physics Letters&lt;/em&gt;, &amp;ldquo;Rate constants for the reactions of CN with hydrocarbons at low and ultra-low temperatures.&amp;rdquo; &lt;strong&gt;DOI: 10.1016/0009-2614(93)87091-G.&lt;/strong&gt; &lt;strong&gt;Not read, abstract only.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read in the abstract:&lt;/strong&gt; For both acetylene and ethylene, the coefficients increase between ambient temperature and approximately &lt;strong&gt;44 K&lt;/strong&gt;, but the coefficients at &lt;strong&gt;25 K are lower than at 44 K&lt;/strong&gt;. These therefore constitute reported low-temperature turnovers rather than monotonic increases on cooling.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Unknown:&lt;/strong&gt; Without the full numerical tables and uncertainties, I cannot establish the statistical significance of either turnover. I also did not verify a barrier height from this paper. These are &lt;strong&gt;qualified counterexamples&lt;/strong&gt;, not the principal basis for rejecting the universal claim.&lt;/p&gt;
&lt;h3 id="1g-nh--hco-too-slow-to-measure-at-34-k"&gt;1G. NH₂ + H₂CO: too slow to measure at 34 K&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference:&lt;/strong&gt; K. M. Douglas, D. Lucas, C. Walsh, N. A. West, M. A. Blitz and D. E. Heard, &lt;strong&gt;2022&lt;/strong&gt;, &lt;em&gt;Astrophysical Journal Letters&lt;/em&gt;, &amp;ldquo;The gas-phase reaction of NH₂ with formaldehyde (CH₂O) is not a source of formamide (NH₂CHO) in interstellar environments.&amp;rdquo; &lt;strong&gt;DOI: 10.3847/2041-8213/ac8cef.&lt;/strong&gt; &lt;strong&gt;Read: accepted paper and supplementary material.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read:&lt;/strong&gt; Pulsed uniform-supersonic-flow measurements at &lt;strong&gt;34 K&lt;/strong&gt; establish only&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;&amp;lt;&lt;/mo&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k&amp;lt;6\times10^{-12}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;The accompanying calculations give approximately &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;6.2&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;14&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;6.2\times10^{-14}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; at 35 K, consistent with that experimental upper limit but not experimentally validated by it. The reported zero-point-corrected barriers include &lt;strong&gt;18.35 kJ mol⁻¹&lt;/strong&gt; for the addition pathway toward formamide and &lt;strong&gt;23.14 kJ mol⁻¹&lt;/strong&gt; for hydrogen abstraction, relative to separated reactants.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Interpretation:&lt;/strong&gt; This meets your category &lt;strong&gt;(c)&lt;/strong&gt;. It does &lt;strong&gt;not&lt;/strong&gt; establish that &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; decreases on cooling: only one low-temperature upper limit was obtained.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="2-barrier-test"&gt;2. Barrier test&lt;/h2&gt;
&lt;h3 id="first-distinguish-a-positive-barrier-from-a-theoryexperiment-contradiction"&gt;First distinguish a positive barrier from a theory–experiment contradiction&lt;/h3&gt;
&lt;p&gt;For this test, I use a positive barrier to mean&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;E&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;T&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;S&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;E&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;p&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;r&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;d&lt;/mi&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;r&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;n&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;&amp;gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
E_{\rm TS}-E_{\rm separated\ reactants}&amp;gt;0,
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;not merely a transition state above a deep intermediate well.&lt;/p&gt;
&lt;p&gt;The verified examples below involve &lt;strong&gt;formation of a prereactive complex followed by passage through a positive barrier toward products&lt;/strong&gt;. They should not automatically be described as having a barrier to the &lt;em&gt;initial capture step&lt;/em&gt;. This distinction is explicit in the methanol and carbon–water reaction mechanisms. &lt;strong&gt;DOIs: 10.1038/nchem.1692; 10.1021/acs.jpclett.6b01637.&lt;/strong&gt;&lt;/p&gt;
&lt;h3 id="2a-oh--choh-positive-product-forming-barriers-and-a-low-t-increase"&gt;2A. OH + CH₃OH: positive product-forming barriers and a low-T increase&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Theoretical barrier reference:&lt;/strong&gt; S. Xu and M.-C. Lin, &lt;strong&gt;2007&lt;/strong&gt;, &lt;em&gt;Proceedings of the Combustion Institute&lt;/em&gt;, &amp;ldquo;Theoretical study on the kinetics for OH reactions with CH₃OH and C₂H₅OH.&amp;rdquo; &lt;strong&gt;DOI: 10.1016/j.proci.2006.07.132.&lt;/strong&gt; &lt;strong&gt;Not read, abstract only.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Barrier heights verified in the experimental paper&amp;rsquo;s discussion of that potential:&lt;/strong&gt; approximately &lt;strong&gt;4.2 kJ mol⁻¹&lt;/strong&gt; for formation of CH₂OH + H₂O and &lt;strong&gt;15.0 kJ mol⁻¹&lt;/strong&gt; for CH₃O + H₂O, above separated reactants. The experimental paper is R. J. Shannon, M. A. Blitz, A. Goddard and D. E. Heard, &lt;strong&gt;2013&lt;/strong&gt;, &lt;em&gt;Nature Chemistry&lt;/em&gt;, &lt;strong&gt;DOI: 10.1038/nchem.1692&lt;/strong&gt;. &lt;strong&gt;Read: full author manuscript.&lt;/strong&gt; Its new CRESU points were at &lt;strong&gt;63 and 82 K&lt;/strong&gt;; the reported coefficient at 63 K is 72 times that at 210 K. Methoxy formation was also observed directly.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Independent lower-temperature measurements:&lt;/strong&gt; M. Antiñolo et al., &lt;strong&gt;2016&lt;/strong&gt;, &lt;em&gt;Astrophysical Journal&lt;/em&gt;, &lt;strong&gt;DOI: 10.3847/0004-637X/823/1/25&lt;/strong&gt;. &lt;strong&gt;Read: full text.&lt;/strong&gt; Two CRESU apparatuses gave, over &lt;strong&gt;22–64 K&lt;/strong&gt;,&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;x&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;3.6&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.1&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mn&gt;300&lt;/mn&gt;&lt;msup&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;1.0&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.2&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k_{\rm exp}(T)
=(3.6\pm0.1)\times10^{-12}(T/300)^{-(1.0\pm0.2)}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;This directly establishes an inverse measured dependence below 100 K.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;How large is the actual theoretical disagreement?&lt;/strong&gt; A later calculation is L. G. Gao, J. Zheng, A. Fernández-Ramos, D. G. Truhlar and X. Xu, &lt;strong&gt;2018&lt;/strong&gt;, &lt;em&gt;JACS&lt;/em&gt;, &lt;strong&gt;DOI: 10.1021/jacs.7b12773&lt;/strong&gt;. &lt;strong&gt;Not read, abstract only.&lt;/strong&gt; Its low-pressure predictions and their discrepancy with experiment are reproduced and analysed by N. Balucani et al., &lt;strong&gt;2024&lt;/strong&gt;, &lt;em&gt;MNRAS&lt;/em&gt;, &lt;strong&gt;DOI: 10.1093/mnras/stae232&lt;/strong&gt;. &lt;strong&gt;Read: full text.&lt;/strong&gt; Both experiment and this quantum treatment show low-temperature acceleration; the major disagreement concerns magnitude and pressure-dependent interpretation.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;My calculation from the published fits:&lt;/strong&gt; At &lt;strong&gt;50 K&lt;/strong&gt;, the experimental fit gives &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;2.16&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;2.16\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. Summing the two product-channel fits tabulated for Gao&amp;rsquo;s low-pressure theory gives &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;4.49&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;13&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;4.49\times10^{-13}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;, a difference of approximately &lt;strong&gt;48-fold&lt;/strong&gt;. Comparing only methoxy formation gives approximately &lt;strong&gt;77-fold&lt;/strong&gt;, but that requires treating the measured OH loss as methoxy formation. These are comparisons of fitted expressions, not individual experimental points. &lt;strong&gt;DOIs: 10.3847/0004-637X/823/1/25; 10.1093/mnras/stae232.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Inference:&lt;/strong&gt; This is strong evidence against naïve classical Arrhenius extrapolation. However, &lt;strong&gt;a CRESU coefficient versus a zero-pressure calculation is not a matched-pressure test&lt;/strong&gt;, and a positive barrier plus increasing &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; is not by itself a contradiction of quantum reaction theory.&lt;/p&gt;
&lt;h3 id="2b-cp--ho-and-cp--do-substantial-positive-barriers"&gt;2B. C(³P) + H₂O and C(³P) + D₂O: substantial positive barriers&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Reference for both theory and experiment:&lt;/strong&gt; K. M. Hickson, J.-C. Loison, D. Nuñez-Reyes and R. Méreau, &lt;strong&gt;2016&lt;/strong&gt;, &lt;em&gt;Journal of Physical Chemistry Letters&lt;/em&gt;, &amp;ldquo;Quantum Tunneling Enhancement of the C + H₂O and C + D₂O Reactions at Low Temperature.&amp;rdquo; &lt;strong&gt;DOI: 10.1021/acs.jpclett.6b01637.&lt;/strong&gt; &lt;strong&gt;Read: full paper and supplementary material.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Facts read:&lt;/strong&gt; The calculated zero-point-corrected barriers are &lt;strong&gt;+32.9 kJ mol⁻¹ for H₂O&lt;/strong&gt; and &lt;strong&gt;+35.1 kJ mol⁻¹ for D₂O&lt;/strong&gt;. For H₂O, measured C-atom removal increases from&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;4.9&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;2.7&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mspace width="1em"/&gt;&lt;mtext&gt;at 106 K&lt;/mtext&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
(4.9\pm2.7)\times10^{-12}\quad\text{at 106 K}
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;to&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;34.7&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;7.4&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mspace width="1em"/&gt;&lt;mtext&gt;at 50 K&lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
(34.7\pm7.4)\times10^{-12}\quad\text{at 50 K}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;D₂O likewise shows increasing removal on cooling.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Size of disagreement:&lt;/strong&gt; The initial master-equation treatment predicted negligible bimolecular product formation. Reproducing the observations required substantial adjustment, including approximately &lt;strong&gt;halving the barrier width&lt;/strong&gt;. Thus the final fit was not an unadjusted ab initio prediction. I did not extract a defensible single multiplicative discrepancy for the original product-rate prediction; &amp;ldquo;negligible&amp;rdquo; is not a numerical denominator.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Conclusion of the barrier test:&lt;/strong&gt; Positive-barrier reactions with low-temperature acceleration are verified. A stricter example involving a demonstrated barrier to &lt;strong&gt;initial capture itself&lt;/strong&gt;, rather than an above-asymptote inner barrier, was &lt;strong&gt;not verified in this search&lt;/strong&gt;.&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="3-selection-bias"&gt;3. Selection bias&lt;/h2&gt;
&lt;h3 id="what-can-be-quantified"&gt;What can be quantified?&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Historical fact:&lt;/strong&gt; Sabbah et al. describe the preceding low-temperature literature as comprising approximately &lt;strong&gt;45 neutral–neutral reactions&lt;/strong&gt;, all fast at room temperature, with &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;298&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi mathvariant="normal"&gt;K&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;≳&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k(298\,\mathrm K)\gtrsim10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. Reference: H. Sabbah, L. Biennier, I. R. Sims, Y. Georgievskii, S. J. Klippenstein and I. W. M. Smith, &lt;strong&gt;2007&lt;/strong&gt;, &lt;em&gt;Science&lt;/em&gt;, &amp;ldquo;Understanding Reactivity at Very Low Temperatures: The Reactions of Oxygen Atoms with Alkenes.&amp;rdquo; &lt;strong&gt;DOI: 10.1126/science.1142373.&lt;/strong&gt; &lt;strong&gt;Read: opening page/introduction; remaining paper not read, abstract only.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Inference:&lt;/strong&gt; For that historical sample, a concrete selection proxy is approximately &lt;strong&gt;45/45—essentially 100%—already fast at room temperature&lt;/strong&gt;. But that is &lt;strong&gt;not&lt;/strong&gt; equivalent to &amp;ldquo;45/45 have rigorously established barrierless potential-energy surfaces.&amp;rdquo;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Unknown:&lt;/strong&gt; I found no verified, current reaction-by-reaction census that provides the requested fraction of &lt;strong&gt;all CRESU-studied reactions&lt;/strong&gt; divided into barrierless/capture-type and barrier-limited classes. I therefore cannot justify a percentage such as &amp;ldquo;90% barrierless.&amp;rdquo;&lt;/p&gt;
&lt;h3 id="why-the-method-favours-fast-reactions"&gt;Why the method favours fast reactions&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Fact read:&lt;/strong&gt; Fournier, Le Picard and Sims discuss a typical accessible lower rate scale around &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;10^{-12}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; for conventional dilute-coreactant measurements, with sensitivity approaching &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;14&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;10^{-14}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; when the reactant can constitute the bath gas, as in H₂ experiments. Reference: &lt;strong&gt;&amp;ldquo;Low-temperature Chemistry in Uniform Supersonic Flows,&amp;rdquo;&lt;/strong&gt; RSC book chapter, online &lt;strong&gt;2017&lt;/strong&gt;, &lt;strong&gt;DOI: 10.1039/9781782626800-00001&lt;/strong&gt;. &lt;strong&gt;Read.&lt;/strong&gt; These are method-dependent scales, not universal detection limits.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Illustrative calculation, not a reported measurement:&lt;/strong&gt; Under pseudo-first-order conditions,&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;r&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;e&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;d&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;exp&lt;/mi&gt;&lt;mo&gt;⁡&lt;/mo&gt;&lt;mo stretchy="false"&gt;[&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;[&lt;/mo&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;mo stretchy="false"&gt;]&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo stretchy="false"&gt;]&lt;/mo&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
f_{\rm reacted}=1-\exp[-k[B]t].
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;Taking &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mo stretchy="false"&gt;[&lt;/mo&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;mo stretchy="false"&gt;]&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mn&gt;15&lt;/mn&gt;&lt;/msup&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;msup&gt;&lt;mi mathvariant="normal"&gt;m&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;[B]=10^{15}\,\mathrm{cm^{-3}}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;200&lt;/mn&gt;&lt;mtext&gt; &lt;/mtext&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;t=200\,\mu\mathrm{s}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; as an illustrative operating point gives approximately &lt;strong&gt;18% reaction&lt;/strong&gt; for &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k=10^{-12}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;, but only &lt;strong&gt;0.2%&lt;/strong&gt; for &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;14&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k=10^{-14}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. Distinguishing the latter from other losses is plainly harder.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;A concrete additional restriction:&lt;/strong&gt; In the NH₂ + formaldehyde study, increasing formaldehyde concentration was limited by clustering, and the published result remained an upper limit. Thus simply increasing &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mo stretchy="false"&gt;[&lt;/mo&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;mo stretchy="false"&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;[B]&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; is not an unrestricted solution. &lt;strong&gt;DOI: 10.3847/2041-8213/ac8cef.&lt;/strong&gt;&lt;/p&gt;
&lt;h3 id="is-no-exception-mostly-a-selection-effect"&gt;Is &amp;ldquo;no exception&amp;rdquo; mostly a selection effect?&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;My assessment:&lt;/strong&gt; Strong selection toward readily measurable reactions is documented, and it plausibly contributes substantially to the prominence of fast, complex-forming chemistry. But three separate propositions must not be collapsed:&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;First&lt;/strong&gt;, the historical sample was strongly selected toward fast reactions; that is documented by Sabbah et al. &lt;strong&gt;Second&lt;/strong&gt;, &amp;ldquo;only fast reactions are studied&amp;rdquo; is too strong: the F + H₂ measurements and NH₂ + formaldehyde upper limit demonstrate otherwise. &lt;strong&gt;Third&lt;/strong&gt;, selection cannot rescue &amp;ldquo;no exception,&amp;rdquo; because published flat and positive-temperature-dependence results exist. &lt;strong&gt;DOIs: 10.1126/science.1142373; 10.1038/nchem.1835; 10.3847/2041-8213/ac8cef.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;For a quantitative modern fraction, the denominator would need to distinguish &lt;strong&gt;unique reactant pairs, isotopologues, measured temperature intervals, failed measurements, and pressure-dependent association versus product formation&lt;/strong&gt;. A compilation of recommended &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k(T)&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; expressions alone would not answer that question. For example, the N + CN paper explicitly distinguishes its measured 56–296 K interval from its extrapolated 10 K recommendation. &lt;strong&gt;DOI: 10.1073/pnas.1200017109.&lt;/strong&gt;&lt;/p&gt;
&lt;hr&gt;
&lt;h2 id="5-steelman-the-opposite-three-strong-physical-arguments"&gt;5. Steelman the opposite: three strong physical arguments&lt;/h2&gt;
&lt;p&gt;You supplied &lt;strong&gt;one explicit claim&lt;/strong&gt;, not four separately formulated claims. I therefore cannot accurately map these arguments onto &amp;ldquo;your four claims.&amp;rdquo; Instead, I identify the inference each argument challenges, without attributing that inference to you.&lt;/p&gt;
&lt;h3 id="argument-1-tunnelling-permits-reaction-below-a-positive-barrier"&gt;Argument 1: Tunnelling permits reaction below a positive barrier&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Specialist&amp;rsquo;s argument:&lt;/strong&gt; A positive potential-energy barrier does not require a vanishing rate when &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;B&lt;/mi&gt;&lt;/msub&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k_{\mathrm B}T&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; falls below its height. The carbon–water study provides more than reactant disappearance: H/D products were detected, while the modelling also identified a contribution from complex stabilization. &lt;strong&gt;DOI: 10.1021/acs.jpclett.6b01637.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What this undermines:&lt;/strong&gt; The inference &lt;strong&gt;&amp;ldquo;theory predicts a positive barrier, therefore substantial low-temperature chemistry is necessarily unphysical.&amp;rdquo;&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What it does not establish:&lt;/strong&gt; Tunnelling does not require every rate coefficient to increase on cooling. F + H₂ supplies an experimentally relevant low-temperature plateau. &lt;strong&gt;DOI: 10.1038/nchem.1835.&lt;/strong&gt;&lt;/p&gt;
&lt;h3 id="argument-2-prereactive-complex-kinetics-can-reverse-the-apparent-temperature-dependence"&gt;Argument 2: Prereactive-complex kinetics can reverse the apparent temperature dependence&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Specialist&amp;rsquo;s argument:&lt;/strong&gt; The measured reaction rate need not be controlled by one isolated barrier-crossing event. In a minimal kinetic model,&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;mover&gt;&lt;mo stretchy="true" minsize="3.0em"&gt;→&lt;/mo&gt;&lt;mpadded width="+0.6em" lspace="0.3em"&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mpadded&gt;&lt;/mover&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/msup&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;mspace width="2em"/&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/msup&gt;&lt;mover&gt;&lt;mo stretchy="true" minsize="3.0em"&gt;→&lt;/mo&gt;&lt;mpadded width="+0.6em" lspace="0.3em"&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;d&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;i&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mpadded&gt;&lt;/mover&gt;&lt;mi&gt;A&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;B&lt;/mi&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;mspace width="2em"/&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mo&gt;∗&lt;/mo&gt;&lt;/msup&gt;&lt;mover&gt;&lt;mo stretchy="true" minsize="3.0em"&gt;→&lt;/mo&gt;&lt;mpadded width="+0.6em" lspace="0.3em"&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;u&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/mpadded&gt;&lt;/mover&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;mo separator="true"&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
A+B\xrightarrow{k_{\rm cap}}C^*,
\qquad
C^*\xrightarrow{k_{\rm diss}}A+B,
\qquad
C^*\xrightarrow{k_{\rm tun}}P,
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;the effective product coefficient is approximately&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mi&gt;P&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mfrac&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;u&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;d&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;i&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;u&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;s&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;t&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;b&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo stretchy="false"&gt;[&lt;/mo&gt;&lt;mi&gt;M&lt;/mi&gt;&lt;mo stretchy="false"&gt;]&lt;/mo&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k_P=k_{\rm cap}
\frac{k_{\rm tun}}
{k_{\rm diss}+k_{\rm tun}+k_{\rm stab}[M]}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;This equation is a schematic steady-state derivation: a lower redissociation rate can increase the probability of reaction per captured encounter without removing the positive inner barrier. Complex-assisted tunnelling is the mechanism advanced for OH + methanol. &lt;strong&gt;DOI: 10.1038/nchem.1692.&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;An important experimental distinction:&lt;/strong&gt; CN + CH₃CN exhibits strongly increasing low-temperature removal and pressure dependence interpreted through competition between reaction and complex formation. Reference: C. Sleiman, S. González, S. J. Klippenstein, D. Talbi, G. El Dib and A. Canosa, &lt;strong&gt;2016&lt;/strong&gt;, &lt;em&gt;PCCP&lt;/em&gt;, &lt;strong&gt;DOI: 10.1039/C6CP01982J&lt;/strong&gt;. &lt;strong&gt;Not read, abstract only.&lt;/strong&gt; The study spans 23–354 K; the abstract reports a 130-fold increase between 168 and 123 K. I did &lt;strong&gt;not&lt;/strong&gt; verify a positive barrier height, so I do not count it as a strict barrier-test hit.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What this undermines:&lt;/strong&gt; The inference &lt;strong&gt;&amp;ldquo;negative apparent activation energy contradicts an above-asymptote product-forming barrier.&amp;rdquo;&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What it also warns against:&lt;/strong&gt; A coefficient obtained from reactant removal can include stabilized association. It need not equal the zero-pressure coefficient for a particular product channel.&lt;/p&gt;
&lt;h3 id="argument-3-capture-dynamics-can-produce-a-physical-inverse-dependencebut-do-not-require-one"&gt;Argument 3: Capture dynamics can produce a physical inverse dependence—but do not require one&lt;/h3&gt;
&lt;p&gt;&lt;strong&gt;Specialist&amp;rsquo;s argument:&lt;/strong&gt; Entrance-channel capture is a dynamical process, not necessarily a temperature-independent collision frequency. Quantitative capture/statistical theories can reproduce low-temperature behaviour, as illustrated by the oxygen–alkene study and the N + CN quantum-capture calculation. &lt;strong&gt;DOIs: 10.1126/science.1142373; 10.1039/C2CP41621B.&lt;/strong&gt; Access statuses are given above.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Illustrative derivation:&lt;/strong&gt; For ideal classical capture on an isotropic attractive potential &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;V&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/msub&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;msup&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;V(R)=-C_n/R^n&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;,&lt;/p&gt;
&lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML" display="block"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mrow&gt;&lt;mi mathvariant="normal"&gt;c&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;a&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;p&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;∝&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mi mathvariant="normal"&gt;.&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;
k_{\rm cap}(T)\propto T^{1/2-2/n}.
&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;
&lt;p&gt;Thus the model yields &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;T^{-1/6}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; for &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;n=3&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;, but &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;T^{+1/6}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt; for &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;n=6&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;. This is a model calculation, not a fit to the reactions listed here.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What this undermines:&lt;/strong&gt; The inference &lt;strong&gt;&amp;ldquo;an inverse temperature dependence must be an experimental artifact.&amp;rdquo;&lt;/strong&gt;&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;What it does not establish:&lt;/strong&gt; &amp;ldquo;Barrierless&amp;rdquo; does not imply &amp;ldquo;increases on cooling.&amp;rdquo; Indeed, capture theory&amp;rsquo;s ability to accommodate different signs makes it an argument &lt;strong&gt;against universality&lt;/strong&gt;, not for it.&lt;/p&gt;
&lt;p&gt;&lt;strong&gt;Overall inference:&lt;/strong&gt; The literature supports physical low-temperature acceleration in particular systems, including systems with positive product-forming barriers. It does &lt;strong&gt;not&lt;/strong&gt; support a universal sign for &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mi mathvariant="normal"&gt;/&lt;/mi&gt;&lt;mi&gt;d&lt;/mi&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;dk/dT&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;, nor does the present search support a numerical allocation of the observed prevalence between reaction-selection bias and underlying dynamics.&lt;/p&gt;
&lt;h3 id="final-evidence-table"&gt;Final evidence table&lt;/h3&gt;
&lt;p&gt;&amp;ldquo;Flat&amp;rdquo; below means experimentally unresolved or negligible temperature dependence. The table includes both counterexamples and the increasing-rate systems examined in the barrier/mechanism tests.&lt;/p&gt;
&lt;table&gt;
&lt;thead&gt;
&lt;tr&gt;
&lt;th&gt;Reaction&lt;/th&gt;
&lt;th&gt;T range&lt;/th&gt;
&lt;th&gt;Dependence&lt;/th&gt;
&lt;th&gt;Barrier predicted?&lt;/th&gt;
&lt;th&gt;Reference&lt;/th&gt;
&lt;th&gt;How sure&lt;/th&gt;
&lt;/tr&gt;
&lt;/thead&gt;
&lt;tbody&gt;
&lt;tr&gt;
&lt;td&gt;N + CN → N₂ + C&lt;/td&gt;
&lt;td&gt;56–296 K; sub-100 K points at 56 and 87 K&lt;/td&gt;
&lt;td&gt;Fitted &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;∝&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mrow&gt;&lt;mn&gt;0.42&lt;/mn&gt;&lt;mo&gt;±&lt;/mo&gt;&lt;mn&gt;0.09&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k\propto T^{0.42\pm0.09}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;: decreases on cooling&lt;/td&gt;
&lt;td&gt;Associated capture treatment; positive exponent does not establish a barrier&lt;/td&gt;
&lt;td&gt;Daranlot et al., 2012, &lt;em&gt;PNAS&lt;/em&gt;, &lt;strong&gt;10.1073/pnas.1200017109&lt;/strong&gt;; Ma et al., &lt;strong&gt;10.1039/C2CP41621B&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;Experiment &lt;strong&gt;read&lt;/strong&gt;; theory &lt;strong&gt;abstract only&lt;/strong&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;O + OH → O₂ + H&lt;/td&gt;
&lt;td&gt;39–142 K&lt;/td&gt;
&lt;td&gt;Approximately flat, &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;3.5&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;3.5\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Numerical height &lt;strong&gt;not verified here&lt;/strong&gt;&lt;/td&gt;
&lt;td&gt;Carty et al., 2006, &lt;em&gt;JPCA&lt;/em&gt;, &lt;strong&gt;10.1021/jp054429u&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Abstract only&lt;/strong&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;N + OH → NO + H&lt;/td&gt;
&lt;td&gt;56–296 K&lt;/td&gt;
&lt;td&gt;Approximately flat, &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;4.5&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;11&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;4.5\times10^{-11}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Described as barrierless&lt;/td&gt;
&lt;td&gt;Daranlot et al., 2011, &lt;em&gt;Science&lt;/em&gt;, &lt;strong&gt;10.1126/science.1213789&lt;/strong&gt;; author account &lt;strong&gt;10.1051/eas/1258046&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;Original &lt;strong&gt;abstract only&lt;/strong&gt;; author account &lt;strong&gt;read&lt;/strong&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;CN + H₂S&lt;/td&gt;
&lt;td&gt;11.7–45.5 K&lt;/td&gt;
&lt;td&gt;Experimentally near-flat, approximately &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;4\times10^{-10}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Dominant pathway has submerged transition states&lt;/td&gt;
&lt;td&gt;Antiñolo et al., 2026, &lt;em&gt;ApJ&lt;/em&gt;, &lt;strong&gt;10.3847/1538-4357/ae421d&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Read&lt;/strong&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;F + normal-H₂ → HF + H&lt;/td&gt;
&lt;td&gt;11.3–20.4 K, CRESU points&lt;/td&gt;
&lt;td&gt;Plateau within uncertainties&lt;/td&gt;
&lt;td&gt;Yes, approximately 6.6 kJ mol⁻¹&lt;/td&gt;
&lt;td&gt;Tizniti et al., 2014, &lt;em&gt;Nature Chemistry&lt;/em&gt;, &lt;strong&gt;10.1038/nchem.1835&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Read&lt;/strong&gt;, including supplementary material&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;CN + C₂H₂&lt;/td&gt;
&lt;td&gt;25 K to ambient; turnover between 44 and 25 K&lt;/td&gt;
&lt;td&gt;Abstract reports &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;25&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;&amp;lt;&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;44&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k(25)&amp;lt;k(44)&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Height &lt;strong&gt;not verified&lt;/strong&gt;&lt;/td&gt;
&lt;td&gt;Sims et al., 1993, &lt;em&gt;CPL&lt;/em&gt;, &lt;strong&gt;10.1016/0009-2614(93)87091-G&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Abstract only&lt;/strong&gt;; turnover significance unverified&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;CN + C₂H₄&lt;/td&gt;
&lt;td&gt;25 K to ambient; turnover between 44 and 25 K&lt;/td&gt;
&lt;td&gt;Abstract reports &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;25&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;mo&gt;&amp;lt;&lt;/mo&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo stretchy="false"&gt;(&lt;/mo&gt;&lt;mn&gt;44&lt;/mn&gt;&lt;mo stretchy="false"&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k(25)&amp;lt;k(44)&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Height &lt;strong&gt;not verified&lt;/strong&gt;&lt;/td&gt;
&lt;td&gt;Sims et al., 1993, &lt;em&gt;CPL&lt;/em&gt;, &lt;strong&gt;10.1016/0009-2614(93)87091-G&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Abstract only&lt;/strong&gt;; turnover significance unverified&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;NH₂ + H₂CO&lt;/td&gt;
&lt;td&gt;34 K&lt;/td&gt;
&lt;td&gt;Only &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;&amp;lt;&lt;/mo&gt;&lt;mn&gt;6&lt;/mn&gt;&lt;mo&gt;×&lt;/mo&gt;&lt;msup&gt;&lt;mn&gt;10&lt;/mn&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;12&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;k&amp;lt;6\times10^{-12}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;; no measured derivative&lt;/td&gt;
&lt;td&gt;Yes; 18.35 and 23.14 kJ mol⁻¹ for the discussed pathways&lt;/td&gt;
&lt;td&gt;Douglas et al., 2022, &lt;em&gt;ApJL&lt;/em&gt;, &lt;strong&gt;10.3847/2041-8213/ac8cef&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Read&lt;/strong&gt;, including supplementary material&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;OH + CH₃OH&lt;/td&gt;
&lt;td&gt;63 and 82 K initially; later 22–64 K&lt;/td&gt;
&lt;td&gt;Increases on cooling; later fit approximately &lt;span class="katex"&gt;&lt;math xmlns="http://www.w3.org/1998/Math/MathML"&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;msup&gt;&lt;mi&gt;T&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;&lt;annotation encoding="application/x-tex"&gt;T^{-1}&lt;/annotation&gt;&lt;/semantics&gt;&lt;/math&gt;&lt;/span&gt;&lt;/td&gt;
&lt;td&gt;Yes; approximately +4.2 and +15.0 kJ mol⁻¹ toward products&lt;/td&gt;
&lt;td&gt;Shannon et al., &lt;strong&gt;10.1038/nchem.1692&lt;/strong&gt;; Antiñolo et al., &lt;strong&gt;10.3847/0004-637X/823/1/25&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;Experimental papers &lt;strong&gt;read&lt;/strong&gt;; original barrier calculation &lt;strong&gt;abstract only&lt;/strong&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;C(³P) + H₂O&lt;/td&gt;
&lt;td&gt;50–106 K&lt;/td&gt;
&lt;td&gt;C removal increases on cooling; product formation also detected&lt;/td&gt;
&lt;td&gt;Yes, +32.9 kJ mol⁻¹&lt;/td&gt;
&lt;td&gt;Hickson et al., 2016, &lt;em&gt;JPCL&lt;/em&gt;, &lt;strong&gt;10.1021/acs.jpclett.6b01637&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Read&lt;/strong&gt;, including supplementary material&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;C(³P) + D₂O&lt;/td&gt;
&lt;td&gt;52–106 K&lt;/td&gt;
&lt;td&gt;Increases on cooling; upper limit at 106 K&lt;/td&gt;
&lt;td&gt;Yes, +35.1 kJ mol⁻¹&lt;/td&gt;
&lt;td&gt;Hickson et al., 2016, &lt;em&gt;JPCL&lt;/em&gt;, &lt;strong&gt;10.1021/acs.jpclett.6b01637&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Read&lt;/strong&gt;, including supplementary material&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
&lt;td&gt;CN + CH₃CN&lt;/td&gt;
&lt;td&gt;23–354 K, combined methods&lt;/td&gt;
&lt;td&gt;Strong low-T removal enhancement; pressure dependent&lt;/td&gt;
&lt;td&gt;Positive barrier height &lt;strong&gt;not verified&lt;/strong&gt;; association is important&lt;/td&gt;
&lt;td&gt;Sleiman et al., 2016, &lt;em&gt;PCCP&lt;/em&gt;, &lt;strong&gt;10.1039/C6CP01982J&lt;/strong&gt;.&lt;/td&gt;
&lt;td&gt;&lt;strong&gt;Abstract only&lt;/strong&gt;; not counted as a verified positive-barrier hit&lt;/td&gt;
&lt;/tr&gt;
&lt;/tbody&gt;
&lt;/table&gt;
&lt;/details&gt;
&lt;h2 id="commentaire-personnel"&gt;Commentaire personnel&lt;/h2&gt;
&lt;p&gt;Contre-exemples trouvés, tous plats (ou sans dépendance résolue) sauf N + CN (Daranlot et al., 2012), dont le coefficient décroît quand T baisse. Étude très intéressante, bravo ! Mais mesure en méthode de taux relatifs — CN et OH suivis simultanément face au même excès de N, donc toute chute commune de densité s&amp;rsquo;élimine dans le rapport.&lt;/p&gt;</description></item></channel></rss>