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	<title>protons &#8211; Science</title>
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	<title>protons &#8211; Science</title>
	<link>https://scienmag.com</link>
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		<title>Protons Take Command: NMR Reveals Hidden Gatekeeper in Molecular Sieve Growth</title>
		<link>https://scienmag.com/protons-take-command-nmr-reveals-hidden-gatekeeper-in-molecular-sieve-growth/</link>
		
		<dc:creator><![CDATA[Bethany Barker]]></dc:creator>
		<pubDate>Tue, 13 Oct 2026 14:51:55 +0000</pubDate>
				<category><![CDATA[Chemistry]]></category>
		<category><![CDATA[acidity]]></category>
		<category><![CDATA[advanced NMR techniques for crystallization studies]]></category>
		<category><![CDATA[aluminophosphate]]></category>
		<category><![CDATA[aluminophosphates and silicoaluminophosphates]]></category>
		<category><![CDATA[catalysis]]></category>
		<category><![CDATA[catalytic and separation applications of molecular sieves]]></category>
		<category><![CDATA[Chinese research on crystalline porous materials]]></category>
		<category><![CDATA[crystallization]]></category>
		<category><![CDATA[HMQC]]></category>
		<category><![CDATA[hydrogen ions in material synthesis]]></category>
		<category><![CDATA[in situ monitoring of inorganic-organic interactions]]></category>
		<category><![CDATA[molecular sieve formation mechanisms]]></category>
		<category><![CDATA[molecular sieves]]></category>
		<category><![CDATA[molecular sieves crystallization]]></category>
		<category><![CDATA[nucleation]]></category>
		<category><![CDATA[porous materials]]></category>
		<category><![CDATA[proton role in crystal growth]]></category>
		<category><![CDATA[protons]]></category>
		<category><![CDATA[real-time observation of crystal assembly]]></category>
		<category><![CDATA[role of acidity in porous framework materials]]></category>
		<category><![CDATA[SAPO]]></category>
		<category><![CDATA[solid-state NMR]]></category>
		<category><![CDATA[solid-state NMR spectroscopy in materials science]]></category>
		<category><![CDATA[structure-directing agents]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=268123</guid>

					<description><![CDATA[Chinese researchers used ultrafast operando solid-state NMR spectroscopy to reveal a proton-mediated dual-channel gating mechanism that directs nucleation and morphology in molecular sieve crystallization.]]></description>
										<content:encoded><![CDATA[<p>In the world of industrial chemistry, few materials are as quietly indispensable as molecular sieves. These crystalline porous frameworks, known scientifically as aluminophosphates and silicoaluminophosphates, serve as the workhorses of catalysis, separation, and adsorption across the chemical industry, from petroleum refining to gas purification. Yet for decades, one of the most fundamental questions about these materials has stubbornly resisted a clear answer: how, exactly, do their crystals assemble themselves at the molecular level? Now, a team of researchers in China has delivered a striking piece of the puzzle, showing that protons — the humble hydrogen ions that define acidity — act as master regulators of the entire crystallization process.</p>
<p>The study, published in the Journal of the American Chemical Society, was led by Professor Hou Guangjin and Associate Professor Liang Lixin from the Dalian Institute of Chemical Physics of the Chinese Academy of Sciences, in collaboration with Professor Dai Weili of Nankai University. Rather than examining finished crystals and inferring how they formed, the team watched the crystallization as it happened, using an advanced form of solid-state nuclear magnetic resonance spectroscopy that could track the fleeting interactions between inorganic building blocks and the organic molecules that guide their assembly. What they found was a proton-mediated, dual-channel gating mechanism in which two distinct chemical pathways alternately steer the reorganization of precursors and the birth of crystal nuclei.</p>
<p>To appreciate why this matters, it helps to understand the peculiar chemistry of molecular sieve synthesis. Aluminophosphate molecular sieves, designated AlPO4-n, and their silicon-containing cousins, SAPO-n, are typically crystallized under acidic, hydrothermal conditions from a gel containing aluminum, phosphorus, and, in the case of SAPOs, silicon sources. Suspended in this reactive soup are organic structure-directing agents, or OSDAs — carefully chosen organic molecules that act as templates around which the inorganic framework organizes itself. The final framework topology, and with it the catalytic properties that make these materials commercially valuable, depends intimately on how these organic and inorganic partners interact during nucleation and growth. But those interactions are transient, heterogeneous, and notoriously difficult to observe directly.</p>
<p>Conventional analytical methods have long struggled with this problem. X-ray diffraction, the standard tool for determining crystal structures, only becomes informative once crystals are large and ordered enough to diffract, by which point the critical early stages of nucleation are already history. Liquid-phase spectroscopic techniques, meanwhile, lose sensitivity or resolution when applied to the viscous, heterogeneous gels from which molecular sieves grow. The DICP-led team recognized that solid-state nuclear magnetic resonance offered a way through, provided they could push the technique&#8217;s sensitivity and speed far beyond what was previously possible. Their solution was a new ultrafast two-dimensional experiment correlating hydrogen-1 and aluminum-27 nuclei.</p>
<p>The technical innovation at the heart of the study is an ultrafast two-dimensional 1H-27Al heteronuclear multiple-quantum coherence, or HMQC, NMR experiment built on an innovative adiabatic SR4 dipolar-recoupling pulse sequence. In plain terms, the experiment works by deliberately reintroducing the weak magnetic interactions between hydrogen nuclei and nearby aluminum nuclei — interactions that are normally averaged away by the rapid spinning of the sample at the so-called magic angle. Recoupling these dipolar interactions allows the spectrometer to detect which protons sit close to which aluminum sites, producing a two-dimensional correlation map that reveals the local chemical neighborhoods within the reacting gel. The catch has always been that such recoupling sequences are inefficient and slow, often requiring hours of signal averaging to produce usable spectra.</p>
<p>The researchers overcame this bottleneck by introducing tanh/tan adiabatic inversion pulses into the recoupling sequence. Adiabatic pulses sweep through their frequency range in a way that makes them remarkably tolerant of imperfections in radiofrequency field strength and of resonance offsets, meaning they invert spins uniformly across a broad bandwidth. The result was a dramatic improvement in recoupling efficiency, enabling high-quality two-dimensional correlation spectra to be acquired in just 30 seconds. That speed is not merely a convenience; it is what makes the experiment truly operando. Crystallization is a dynamic process, and a technique that requires hours per spectrum can only offer static snapshots. With spectra in half a minute, the team could follow the evolving host-guest interactions in near real time as the gel transformed into crystal.</p>
<p>Combined with theoretical simulations, the spectroscopic data revealed a mechanism with an elegant two-channel structure. In the first channel, hydroxyl-driven hydrolysis takes center stage: protons attack and reorganize the inorganic precursor species, breaking and reforming bonds in the aluminophosphate network. In the second channel, the organic structure-directing agents take over, mediating templating interactions that lock the reorganized precursors into the geometry required for the target framework. Crucially, these two channels do not operate independently or simultaneously in a simple additive way. Instead, they alternate, gating each other&#8217;s activity in a rhythm that regulates precursor reorganization and nucleation. The protons, by toggling the system between hydrolysis-dominated and templating-dominated regimes, effectively conduct the entire assembly process.</p>
<p>The team went on to quantify how protonation accelerates the condensation reactions that build the framework itself. Their findings showed that protonation lowers the activation energy of P-O-Al condensation — the chemical step in which phosphorus and aluminum species link together to form the crystalline network — while simultaneously enhancing the thermodynamic driving force for framework formation. In other words, acidity does not merely speed the reaction along a pre-existing path; it changes both the kinetic barrier and the energetic payoff, making framework formation both easier to initiate and more favorable to complete. This dual effect provides a concrete, mechanistic explanation for a long-observed but poorly understood phenomenon: the strong dependence of molecular sieve crystallization rates and outcomes on the acidity of the synthesis medium.</p>
<p>Perhaps the most visually striking consequence of the mechanism lies in crystal morphology. The researchers found that the synergistic effects of proton-promoted nucleation and facet-selective stabilization — the preferential protection of certain crystal faces during growth — enabled the formation of nanosheet-like and nanorod-like molecular sieves across different framework topologies. Morphology control is far from a cosmetic concern in this field. The shape and aspect ratio of molecular sieve crystals determine their external surface area, the accessibility of their pore systems, and their diffusion characteristics, all of which feed directly into catalytic performance. A rational handle on morphology, grounded in an understanding of proton-mediated gating, could therefore translate into better-designed catalysts and adsorbents without the trial-and-error empiricism that has traditionally dominated synthesis optimization.</p>
<p>Professor Hou summarized the significance of the work by noting that the study provides new insights into the role of acidity in molecular sieve crystallization and establishes an advanced NMR approach for investigating crystallization mechanisms and guiding the rational synthesis of porous materials. The implications extend well beyond the aluminophosphate family. The operando solid-state MAS NMR methodology, with its ultrafast 2D correlation capability, is a general-purpose probe of host-guest interactions in reacting systems, and the conceptual framework of proton-gated dual-channel assembly may find echoes in other solution-grown functional materials. For a field that has spent half a century perfecting the products of crystallization while remaining largely blind to the process itself, the ability to watch protons orchestrate the birth of a crystal — one 30-second spectrum at a time — marks a genuine step change in how molecular sieves will be understood, and ultimately designed, in the years ahead.</p>
<p><strong>Subject of Research:</strong> Proton-mediated crystallization mechanisms of aluminophosphate molecular sieves studied by operando solid-state NMR spectroscopy</p>
<p><strong>Article Title:</strong> Scientists reveal how protons control molecular sieve crystallization</p>
<p><strong>Article References:</strong> Scientists reveal how protons control molecular sieve crystallization. (n.d.). <a href="https://www.eurekalert.org/news-releases/1147329" rel="noopener noreferrer">Original publication</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> Not provided</p>
<p><strong>Keywords:</strong> molecular sieves, aluminophosphate, SAPO, crystallization, protons, acidity, solid-state NMR, HMQC, nucleation, structure-directing agents, catalysis, porous materials</p>
]]></content:encoded>
					
		
		
		<post-id xmlns="com-wordpress:feed-additions:1">268123</post-id>	</item>
		<item>
		<title>Tiny Proton Collisions at the LHC Show Big-System Behavior, ALICE Reports</title>
		<link>https://scienmag.com/tiny-proton-collisions-at-the-lhc-show-big-system-behavior-alice-reports/</link>
		
		<dc:creator><![CDATA[Katie Riggs]]></dc:creator>
		<pubDate>Fri, 02 Oct 2026 05:53:03 +0000</pubDate>
				<category><![CDATA[Space]]></category>
		<category><![CDATA[ALICE]]></category>
		<category><![CDATA[ALICE high-multiplicity event analysis]]></category>
		<category><![CDATA[and proton yields]]></category>
		<category><![CDATA[behavior of small collision systems]]></category>
		<category><![CDATA[charged pion]]></category>
		<category><![CDATA[collective flow in small systems]]></category>
		<category><![CDATA[comparison of small and large collision systems]]></category>
		<category><![CDATA[emergence of quark-gluon plasma signatures in proton collisions]]></category>
		<category><![CDATA[EPOS4]]></category>
		<category><![CDATA[flowing matter in small systems]]></category>
		<category><![CDATA[high multiplicity]]></category>
		<category><![CDATA[high-multiplicity triggers at LHC]]></category>
		<category><![CDATA[Hot]]></category>
		<category><![CDATA[implications for particle physics and Q]]></category>
		<category><![CDATA[kaon]]></category>
		<category><![CDATA[kaons]]></category>
		<category><![CDATA[LHC]]></category>
		<category><![CDATA[particle multiplicity density at 13 TeV]]></category>
		<category><![CDATA[particle production in high-energy collisions]]></category>
		<category><![CDATA[pions]]></category>
		<category><![CDATA[proton-proton collisions]]></category>
		<category><![CDATA[Proton-proton collisions at LHC]]></category>
		<category><![CDATA[protons]]></category>
		<category><![CDATA[PYTHIA 8]]></category>
		<category><![CDATA[quark-gluon plasma]]></category>
		<category><![CDATA[radial flow]]></category>
		<category><![CDATA[strangeness enhancement]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=226002</guid>

					<description><![CDATA[New ALICE measurements of pion, kaon, and proton production in the highest-multiplicity proton-proton collisions ever analyzed at 13 TeV reveal heavy-ion-like patterns that challenge existing models.]]></description>
										<content:encoded><![CDATA[<p>When two protons slam into each other at the Large Hadron Collider, physicists usually expect a messy spray of particles governed by simple fragmentation rules. But a new measurement from the ALICE collaboration, published in The European Physical Journal C, shows that in the rarest and most crowded proton-proton events, the smallest collision system at the LHC begins to behave in ways that echo the giant fireballs formed when lead nuclei collide. The collaboration measured the production of charged pions, charged kaons, and protons in high-multiplicity proton-proton collisions at a center-of-mass energy of 13 TeV, and the results sharpen one of the most intriguing questions in modern particle physics: can a system as small as two protons create a droplet of hot, collectively flowing matter?</p>
<p>The analysis focuses on particles produced at midrapidity, within |y| &lt; 0.5, in three of the highest-multiplicity event classes ever selected in proton-proton collisions. Using a dedicated high-multiplicity trigger that selects roughly the top 0.1 percent of events based on the signal in the V0 scintillator arrays, ALICE pushed the average charged-particle multiplicity density to 35.8 particles per unit of pseudorapidity, about a factor of five higher than in average inelastic proton-proton collisions. That density is comparable to what is seen in peripheral lead-lead collisions at 2.76 TeV per nucleon pair, dramatically narrowing the multiplicity gap between small and large collision systems and providing a crucial bridge for comparing physics across system sizes.</p>
<p>The experimental technique combines two independent particle-identification approaches. At low transverse momentum, between roughly 0.1 and 0.75 GeV/c depending on the particle species, the Inner Tracking System alone identifies hadrons through their specific energy loss in silicon. At higher momenta, from about 0.6 up to 4.0 GeV/c, a two-dimensional fit exploits the correlated information from the Time Projection Chamber and the Time-Of-Flight detector, simultaneously modeling the energy-loss and time-of-flight responses for pions, kaons, and protons while accounting for background from mismatched TOF signals. The data sample, collected in 2016 during LHC Run 2 with an integrated luminosity of 13 inverse picobarns for the high-multiplicity trigger, yielded about 80 million events for the inner-tracking analysis and 8 million for the TPC-TOF analysis.</p>
<p>After correcting the raw yields for tracking efficiency, detector acceptance, and contamination from secondary particles produced in weak decays or interactions with detector material, the collaboration obtained transverse-momentum spectra for each particle species in each multiplicity class. The most striking feature is a hardening of the spectra with increasing multiplicity, and that hardening is mass-dependent: the heavier the particle, the more its spectrum shifts toward higher momenta. This mass ordering is precisely the signature associated with radial flow in heavy-ion collisions, where the hot, dense medium expands outward hydrodynamically and gives heavier particles a bigger boost. Quantitatively, the kaon-to-pion ratio rises by a factor of about six, and the proton-to-pion ratio by a factor of about fifteen, as the transverse momentum increases from roughly 0.3 to 3.0 GeV/c.</p>
<p>The proton-to-pion ratio itself tells a compelling story. At low transverse momentum, below about 1 GeV/c, the ratio is suppressed relative to expectations, while at intermediate momenta around 3 GeV/c it shows a clear enhancement. This baryon-to-meson enhancement at intermediate transverse momentum has long been a hallmark of heavy-ion collisions, where it is attributed either to collective flow or to quark recombination, a process in which thermal quarks from the medium combine to form hadrons. Observing a similar pattern in proton-proton collisions, where no large medium was expected to form, reinforces the accumulating evidence that collective-like phenomena are not exclusive to nucleus-nucleus systems.</p>
<p>Perhaps the most consequential result emerges when the transverse-momentum-integrated kaon-to-pion and proton-to-pion ratios are plotted against the charged-particle multiplicity and compared across proton-proton, proton-lead, and lead-lead collisions at various energies. The measurements from all systems and energies fall on smooth, continuous trends, suggesting that particle production is governed primarily by the final-state charged-particle multiplicity rather than by the collision energy or the size of the colliding system. The kaon-to-pion ratio increases by a factor of 1.39 plus or minus 0.19 from low-multiplicity proton-proton collisions to the highest multiplicities in lead-lead collisions, a hint of strangeness enhancement, while the proton-to-pion ratio decreases by a factor of 1.23 plus or minus 0.15, consistent with antibaryon-baryon annihilation in the hadronic phase of heavy-ion collisions. The new high-multiplicity proton-proton points follow both trends seamlessly.</p>
<p>To probe the underlying mechanism, the collaboration compared its results with several theoretical models. PYTHIA 8, the workhorse Monte Carlo generator based on the Lund string model, was tested with four distinct tunes: the standard Monash 2013 configuration, a Ropes tune in which overlapping strings form higher-tension color ropes that boost baryon and strangeness production, a Shoving tune in which strings repel each other and generate a microscopic transverse pressure, and a CLR-BLC Mode 3 tune that introduces string-junction topologies during color reconnection to enhance baryon production. EPOS4, the latest version of the EPOS generator, takes a different approach, dynamically separating each event into a dense core that undergoes collective expansion and a dilute corona that fragments independently.</p>
<p>The comparison reveals that no single model consistently captures all the observed features. The Monash and Ropes tunes reproduce the pion spectra qualitatively within about 20 percent over the full momentum range, while EPOS4 underestimates them. All model calculations underestimate the kaon-to-pion ratio above 0.5 GeV/c, and none of the PYTHIA 8 tunes captures the low-momentum depletion seen in the highest-multiplicity data. EPOS4 provides a better description of the momentum-dependent kaon-to-pion and proton-to-pion ratios than the PYTHIA 8 tunes, and it reproduces the multiplicity trend of the pion mean transverse momentum across the full range, though it falls short for protons in the highest multiplicity classes. The Shoving tune, notably, gives a quantitatively good description of the pion mean transverse momentum, while all PYTHIA 8 tunes underestimate the kaon and proton values.</p>
<p>The mean transverse momentum itself adds another layer of evidence. For all three particle species, it rises continuously with multiplicity, and the rise is steeper for heavier hadrons, mirroring the pattern seen in heavy-ion collisions and consistent with radial flow. Interestingly, at similar multiplicity the mean transverse momentum in proton-proton collisions is higher than in lead-lead collisions, a difference that models will need to explain. The integrated yields were obtained by fitting the measured spectra with Levy-Tsallis functions, with only 6 to 9 percent of the yield extrapolated from unmeasured momentum regions, and the associated systematic uncertainties on the extrapolations range from 0.9 to 1.8 percent.</p>
<p>These measurements do not claim that a quark-gluon plasma forms in proton-proton collisions, and the nuclear modification factor in small systems remains consistent with unity at high momentum, in contrast to the strong jet suppression seen in lead-lead collisions. But by extending light-flavor hadron measurements to charged-particle densities previously unreachable in proton-proton events, ALICE has delivered exactly the kind of high-precision input that theorists need to constrain and improve their models of collective behavior in small systems. Whether the mass-dependent spectral hardening, the intermediate-momentum baryon enhancement, and the multiplicity-driven scaling of particle ratios ultimately trace back to a tiny droplet of deconfined matter, to dense overlapping strings, or to some other mechanism entirely, the new data make clear that the smallest collisions at the LHC are far from trivial, and that the physics of the very large and the very small is more deeply connected than anyone expected.</p>
<p><strong>Subject of Research:</strong> Pion, kaon, and proton production in high-multiplicity proton-proton collisions at 13 TeV measured by ALICE</p>
<p><strong>Article Title:</strong> &#040;\pi &#041;, K, and p production in high-multiplicity pp collisions at &#040;\mathbf {\sqrt{ s} = 13}&#041; TeV</p>
<p><strong>Article References:</strong> ALICE Collaboration, Abdallah, D. A. H., Abualrob, I. J., Acharya, S., Rinella, G. A., Aglietta, L., Agrawal, N., Ahammed, Z., Ahmad, S., Ahuja, I., Akbar, Z., Akishina, V., Al-Turany, M., Alessandro, B., Molina, R. A., Ali, B., Alici, A., Alme, J., Alocco, G., &#8230; Zurlo, N. (2026). $$\pi $$, K, and p production in high-multiplicity pp collisions at $$\mathbf {\sqrt{ s} = 13}$$ TeV. <em>The European Physical Journal C, 86</em>(9), Article 1127. <a href="https://doi.org/10.1140/epjc/s10052-026-16235-5" rel="noopener noreferrer">https://doi.org/10.1140/epjc/s10052-026-16235-5</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1140/epjc/s10052-026-16235-5" rel="noopener noreferrer">10.1140/epjc/s10052-026-16235-5</a></p>
<p><strong>Keywords:</strong> ALICE, LHC, proton-proton collisions, pions, kaons, protons, high multiplicity, radial flow, strangeness enhancement, PYTHIA 8, EPOS4, quark-gluon plasma</p>
]]></content:encoded>
					
		
		
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