Atomic Physics with Heavy Ions

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Heavy-ion collisions recreate the quark-gluon plasma, the extreme state of matter that is believed to have filled the universe when it was only microseconds old. Besides searching for new fundamental particles, the LHC experiments have substantial physics programmes that study the collective behaviour of quarks and gluons when they form this state.

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From the perspective of the early s, the energies attained by the Tevatron and LHC would have seemed like science-fiction. But, thanks to breakthroughs in accelerator science and technology in subsequent decades, they are now real. Who can anticipate the future progress that may one day give us single nucleons colliding with 1 PeV? In the meantime, while it seems unlikely that the LHC will be renamed the "Pevatron", we can celebrate this week's breaking of a new symbolic energy barrier.

It may be a while before the next such occasion.

Read more: " LHC collides ions at new record energy ". So, for about 5 times the weight of the Bevatron magnet, the LHC provides about 10, times the proton collision energy. This is another measure of the progress of accelerator science and technology in the meantime.

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This year, the LHC experiments requested the same average energy per pair of colliding nucleons as in the run where 4 TeV protons were collided with TeV lead nuclei. This was arranged by lowering the LHC's magnetic field from the value corresponding to 6. That was still just enough to exceed 1 PeV in total collision energy! News Opinion Topic: Physics.

Tevatron heavy ion. Related Articles. A busy week for science. The Tevatron's data continue to excite. At CERN. Also On Physics. NA62 spots two potential instances of rare pa Heavy-ion and proton—proton collisions at ultrarelativistic energies provide a unique system with which to investigate the dynamics of matter in the early universe. Given that the universe did not become transparent until roughly , years after the Big Bang, this epoch in our history lies completely out of reach to observational astronomy.

According to the Standard Model of particle physics, the emergence of elementary particles and forces took place via a succession of symmetry-breaking mechanisms at different energy scales as the universe expanded and cooled. In the early universe, matter was made of freely roaming quarks — which formed the quark—gluon plasma QGP — in addition to leptons and gauge bosons.


The QGP cooled down until hadrons including baryons such as neutrons and protons were formed. During the past 30 years, a succession of collider experiments and impressive theoretical achievements have driven immense progress in the field of high-energy heavy-ion physics.

Explaining Light-Nuclei Production in Heavy-Ion Nuclear Collisions

Not only do these results shed new light on the dynamics of matter in the early universe, they probe fundamental predictions about the strong nuclear force governed by quantum chromodynamics QCD. We have come a long way from the early belief in the s that this early phase in the universe, recreated by colliding heavy ions at continuously increasing energies, comprised a gas of quarks and gluons.

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This is what was expected following asymptotic freedom, a feature of QCD that explains how the interaction between two quarks becomes asymptotically weaker as the distance between them decreases. But it took three major colliders on both sides of the Atlantic to find out what was really going on during these extreme initial moments.

This finding confirmed a fundamental prediction of QCD: above a critical temperature, quarks are no longer confined in hadrons. The CERN announcement was, however, only the beginning of our exploration into strongly interacting matter. Just five years after the CERN announcement, the remarkable data collected at RHIC demonstrated that a change of paradigm for strongly interacting matter was needed. Rather, it showed all the properties of a perfect liquid: a strongly interacting fluid with minimal mean free path.

The LHC also offered new opportunities to explore deconfined matter in great detail, with the goal of understanding how the dynamics of matter emerge from the fundamental properties of the strong interaction and from the quark infrastructure of particles. More recently, and surprisingly, LHC data are pointing to unexpected similarities between observables measured in heavy-ion collisions and those measured in proton—lead or in high-multiplicity proton—proton collisions, perhaps hinting at yet another change of paradigm.

During hadronisation of the QGP, final states range from non-strange and strange mesons and baryons to light nuclei. Image credit: arXiv The past 30 years have been an arduous path where every step both reveals more knowledge to us while simultaneously generating new riddles. To mark the important achievements so far and to discuss the long and thrilling future of heavy-ion physics, more than physicists met at CERN on 9 November last year to review what can be considered as one of the most vigorous fields at the forefront of the high-energy physics programme.

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Despite this, Schopper bravely decided to give heavy-ion physics a chance. He had no direct personal interest and his physics motivation sounded convincing.

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The main argument he put forward was to find the theoretically predicted quark—gluon plasma, which played an important role in the development of the universe. When, in October , oxygen ions were successfully accelerated by the SPS and fired into a fixed target of gold, the heavy-ion programme began with a disparate ensemble of detectors recuperated from earlier high-energy experiments. In , together with the increase of energy and the acceleration of sulphur beams, second-generation experiments containing innovative detector technologies were launched. Among these were: NA49 with an ambitious time projection chamber; CERES and its double ring imaging Cherenkov detectors; NA57 and its silicon tracking; and NA44, which contained a focusing spectrometer that made use of cesium-iodide photocathodes for the first time.

Today, heavy-ion science is a thriving field of research, and it is notable that it is the common denominator in the physics programmes of all four major LHC experiments. On one hand, we have entered a phase of precision measurements of the QGP properties, while on the other hand the surprising similarities between proton—proton and proton—nucleon collisions observed at the LHC lead us to question if the same dynamics are at work in light and heavy systems.

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On the experimental side, these are based on a wealth of high-quality data collected both at LHC and RHIC for a variety of collision systems and energies, coupled with inventive analysis tools. On the theory side, particular progress has been made in relativistic hydrodynamics calculations.

Macroscopic properties of the QGP such as its density and viscosity can now be determined with increasing precision by studying how the QGP, modelled by hydrodynamics, transports a perturbation. On 9 November , more than physicists came to CERN to celebrate three decades of heavy-ion physics.

Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions Atomic Physics with Heavy Ions
Atomic Physics with Heavy Ions

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