Particle physics

Liberating quarks and gluons

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An extraordinary new state of matter, the quark-gluon plasma, may have been produced. In collisions between high-energy heavy nuclei, conditions like those 0.01 seconds after the Big Bang are reproduced — though only on a small scale and briefly. Temperatures of 1012 K or more are achieved, roughly ten million times that at the surface of the Sun, or ten thousand times that in the solar core. Theorists predict that under these conditions there is a drastic change in the structure of nuclear matter. The usual description in terms of baryons (such as protons and neutrons) and mesons (such as pions) must be abandoned in favour of a description involving the truly fundamental particles, quarks and gluons. Experiments last year have provided the first substantial evidence that such a change in fact occurs1,2,3.

To put these developments in perspective, let me sketch some of the background. Quantum chromodynamics (QCD) is the modern theory of the strong interaction4 — the most powerful force of nature, responsible for holding atomic nuclei together, and for most of what goes on in high-energy accelerators. QCD is verified by dozens or perhaps hundreds of experimental tests5,6. But it is a most peculiar theory: its fundamental particles, the quarks and gluons, have never been observed in isolation. Indeed, the theory predicts that they never will be.

According to QCD, particles that carry uncompensated colour charge call forth such strong forces that they spontaneously ionize empty space. One might say that they cause a colour lightning storm. When the storm subsides, all the colour charges have been neutralized. The strongly interacting particles that experimenters can actually observe are composites of several quarks and gluons, arranged into structures with compensating colour charges, so that they are neutral overall. The most important types are baryons, which can be constructed from three quarks; antibaryons, constructed from three antiquarks; and mesons, constructed from a quark and an antiquark.

Quarks and gluons themselves carry uncompensated colour charge, and therefore, according to QCD, cannot exist in isolation — they are ‘confined’. Nevertheless, to modern physicists quarks and gluons are quite real and tangible objects, no less than (say) electrons. Indeed, quarks and gluons have quite distinct signatures (Fig. 1). They can do so, despite being confined, because of the special nature of the forces among them. The powerful confinement forces only come into play when colour charges are taken far apart from one another, and they take some time to set in. When the colour balance is disturbed by sudden, small-scale motions, to begin with the colour forces are much weaker. This property of QCD is called asymptotic freedom. In a high-energy collision, the key events that control the large-scale flow of energy and momentum are brief, violent accelerations of the particles. Because of asymptotic freedom, these events occur almost as if the quarks and gluons were free and unconfined, so the energy and momentum distribution follows a pattern imprinted by the quarks and gluons (Fig.1).

Figure 1: Realization of quarks and gluons as jets.
figure1

A Z-boson decay into quark and antiquark (a) is reflected in the jets of compound particles observed (b). When the Z-boson instead decays into quark, antiquark and gluon (c), the observed energy and angle distribution of the products (d) again follows the pattern set by the underlying quarks and gluons. (Parts b and d from ref. 9.)

In a quark-gluon plasma, liberation of quarks and gluons is taken to a new level. At low particle densities, each coloured particle is bound up with its neutralizing partners, inside some ordinary hadron (Fig. 2a). At high particle densities the hadrons start to overlap, and cease to exist as meaningful individuals. Indeed, a particle needing a mate no longer finds it necessary to stay married to a particular partner, since there are always plenty of eligible singles nearby (Fig. 2b). The meaningful units are then quarks and gluons, not hadrons.

Figure 2: Confinement and deconfinement.
figure2

When the surrounding quarks and gluons are contained in colour-neutral hadrons (a), the charm quark and antiquark that make up a J/ψ particle must also stay paired, so that their colour charges cancel out. But if the surrounding quarks and gluons run free (b), the components of the J/ψ readily make and break bonds with other particles, and the J/ψ particles dissociate much more quickly. A rapid decrease in J/ψ production with effective temperature has been seen by the NA50 experiment10 at CERN (c).

Theorists calculate that this drastic change in the structure of matter sets in over a narrow range of temperatures centred around 1012 K. To gauge the change, it is instructive to compare the degrees of freedom — the number of different particles that energy can go to. On the hadronic side of the transition, the important particles at these temperatures are just the pions (the other hadrons being too heavy). These are spinless particles and come in three types — with positive, negative or zero electric charge. On the quark-gluon side, there are three colours of quarks of three different types (up, down and strange — the other quarks are too massive to play a part) and each has two possible spin directions. Taking into account antiquarks, we find 3×3×2×2 = 36 quark degrees of freedom. In addition, there are eight gluons each with two possible spin directions — thus 54 degrees of freedom altogether, compared with the previous three. A direct consequence is that a given input of energy will raise the temperature of a quark-gluon plasma much less than it would the hadronic gas, as the energy has to be shared by many more particles.

Despite the dramatic nature of these predicted changes, it is not easy to establish experimentally that one has produced a quark-gluon plasma. Difficulties arise because the number of particles reaching the detectors after a heavy ion collision is extremely large, and because the plasma, even if produced, has only a fleeting existence in a very small region.

The experimenters are like inspectors who must examine the residue of a great explosion to determine if it was due to conventional or nuclear weapons (or perhaps a meteorite). Ambitious responses to this challenge are being mounted at CERN and at Brookhaven, where the heavy-ion accelerator RHIC will come into operation next summer.

Already, CERN has seen what might be the first harbinger of the quark-gluon plasma. Charm-quark/charm-antiquark pairs, making up the J/ψ family of particles, seem to find it much more difficult to stay paired once the energy in a fireball exceeds a threshold value (Fig. 2c). This certainly suggests the deconfinement mentioned above. It has been advocated for some time as a signature of the quark-gluon plasma. Even though the issue is muddied by the fact that the J/ψ particles will be buffeted more at higher temperature whether one has hadrons or quark- gluon plasma, nevertheless the apparent sharpness of the threshold, and other details, point towards the plasma. What makes the latest results3 especially intriguing is that they are the first that sceptical theorists7 have not been able to explain without invoking a quark-gluon plasma.

A big question left open by these experiments is whether the transition from normal matter to quark-gluon plasma, as a function of temperature, is continuous or truly abrupt. If it is abrupt (in the language of phase transitions, first order), superheating and supercooling are possible, and could trigger explosive instabilities. If such events occurred in the early Universe, they must have appreciably perturbed its evolution.

We anticipate other relics of the quark- gluon plasma created in accelerators. An especially intriguing possibility is that the quark-antiquark condensate which normally fills space could reassemble incorrectly, forming a domain analogous to domains in magnets. When such a domain snaps back into place, it will release a laser-like pion beam8.

More prosaically, it would be reassuring to see the predicted high specific heat, and the associated increase in multiplicity of particles. In particular, strange quarks and antiquarks are much lighter and therefore much easier to produce than the K mesons in which they are normally confined. So events following the creation of a quark-gluon plasma should be especially strange, in more ways than one.

References

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    Abreu, M. C.et al. Phys. Lett. B 410, 327–343 (1997).

  2. 2

    Satz, H. preprint hep-ph/9711289 on xxx.lanl.gov

  3. 3

    Gonin, M. http://www.cern.ch/NA50/papers/bnl.ps

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    Wilczek, F. Annu. Rev. Nucl. Sci. 32, 177–209 (1982).

  5. 5

    Schmelling, M. preprint hep-ex/971002 on xxx.lanl.gov

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    Burrows, P. preprint hep-ex/9705013 on xxx.lanl.gov

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    Gavin, S. & Vogt, R. Phys. Rev. Lett. 78, 1006–1009 (1997).

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    Rajagopal, K. in Quark-Gluon Plasma 2 (ed. Hwa, R.) 484-554 (World Scientific, Singapore, 1995).

  9. 9

    http://www.cern.ch/Opal/events/qq.gif& http://www.cern.ch/Opal/events/qqg_lego.gif

  10. 10

    http://www.cern.ch/NA50

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