Lead Nucleus Hides Gluons express

Original: "Observation of nuclear suppression in coherent $$\Upsilon$$(1S) photoproduction off heavy nuclei at the LHC"
· CMS Collaboration
arXiv:2604.05814 · 2026-04-07 · CC BY 4.0 · 2 min
Heavy particles show that inside a lead nucleus there are fewer gluons than expected.

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Colliding two lead nuclei at the Large Hadron Collider is like throwing two hefty bags of marbles at each other. Usually, the marbles scatter in all directions, but sometimes one bag passes so close that the marbles don't collide: they just exchange glances. That's how, without a direct hit, the nuclei exchanged light, and in that light, an Upsilon particle was born — a heavy cousin of the proton, made of a charm quark and its antiquark.

The Upsilon is 10 times heavier than the proton, so it can only be born in very hard light, like needing a powerful crane to lift a heavy load.

Inside a lead nucleus, gluons, the carriers of the strong force that glue quarks together, behave differently than in a free proton. The measurement showed: in lead, each gluon accounts for only 55% of what it would be in a free proton. This is strong suppression, and it hardly depends on how heavy the produced particle is. Previously, the same suppression was seen for the lighter phi particle, and now it's confirmed for the Upsilon — at an energy 100 times higher.

The number 0.55 is like having only 55 free seats for every 100 passengers on a crowded bus.

This result suggests that inside a lead nucleus, gluons are not just 'smeared out' but form a dense state that scientists call the color glass condensate. This state is hard to see directly, but by the suppression of particle production, we can infer its properties. In the future, such measurements will help us understand how matter behaves at extreme densities — for example, in the first moments after the Big Bang or inside neutron stars.

Original abstract

as written by the authors arXiv:2604.05814

The first measurement of coherent $$\Upsilon$$(1S) meson photoproduction off heavy nuclei is performed using ultraperipheral lead-lead collisions collected by the CMS experiment at a nucleon-nucleon center-of-mass energy of 5.02 TeV. The nuclear gluonic structure is probed at a nucleon momentum fraction of order $$x$$ $$\sim$$ 10$$^{-3}$$, determined by the kinematics of the process. Owing to the large $$\Upsilon$$(1S) mass, the measurement reaches the highest scale accessible so far through coherent vector-meson photoproduction, $$\mu^2$$ = 22.4 GeV$$^2$$, where nonlinear quantum chromodynamics effects are expected to be minimal. In the $$\Upsilon$$(1S) rapidity range $$\lvert y\rvert$$ $$\lt$$ 1, the ratio of the measured photoproduction cross section to a baseline model prediction that neglects nuclear effects is $$S_{\Upsilon\text{(1S)}}$$ = 0.25 $$\pm$$ 0.06 (stat) $$\pm$$ 0.02 (syst), thereby demonstrating nuclear suppression in this process. Expressed in terms of a nuclear gluon suppression factor, the result yields $$R_\text{g}^\text{Pb}$$($$x$$ $$\approx$$ 10$$^{-3}$$, $$\mu^2$$ = 22.4 GeV$$^2$$) = 0.55 $$\pm$$ 0.12 (stat) $$\pm$$ 0.02 (syst). The measured $$R_\text{g}^\text{Pb}$$ is only slightly larger than the values previously reported for coherent $$\phi$$ photoproduction, despite the probed $$\mu^2$$ differing by approximately two orders of magnitude.

The Upsilon meson was discovered in 1977 and was the first evidence for the existence of the fifth quark, the bottom quark.

In Liu Cixin's novel 'The Three-Body Problem', aliens use subatomic particles to create super-dense materials — similar states of matter are studied in heavy-ion experiments.

Scientists
Fritz ZwickyAlbert EinsteinHans BetheLise MeitnerMargaret BurbidgeWolfgang Pauli
Concepts
cms detector neutron mass cms collaboration primordial nucleosynthesis proton mass supernova nucleosynthesis meson nuclear force b meson proton neutrinoless double beta decay nuclear stability z boson deuteron nucleon tau lepton particle creation gluon fermilab solar neutrino