STANFORD Tidying up Charmonium

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STANFORD Tidying up Charmonium The SPEAR electron-positron storage ring at SLAC, After first generation detectors discovered charmonium, new experiments are now uncovering the details of the rich charmonium spectroscopy. (Photo SLAC) tion has been mounting that under different conditions, new forms of nuclear matter are possible (see December 1980 issue, page 404). The behaviour seen in the heavy ion experiments at Berkeley cannot be explained if the secondary frag­ ments are ordinary particles, and one suggestion is that evidence is being seen for a new type of nuclear matter. While still made up of quarks, this new metastable nuclear material has its component quarks in configurations very different to those of normal particles. Experi­ ments are continuing to study the behaviour of these short-lived colli­ sion fragments. STANFORD Tidying up charmonium Charmonium is the family name given to mesons composed of a charmed quark bound to a charmed spectroscopy of triplet charmonium monium. They had definite ideas for antiquark. The discovery in 1 974 of states has been uncovered. the mass of the eta-c, which did not the first charmonium state, the J/ However their singlet counter­ agree with the preliminary informa psi, at Brookhaven and at SLAC parts have proved to be much harder tion from DORIS. heralded the arrival of a new era in to find, and for good reasons. Char­ Then new data began to come the study of elementary particles, monium normally comes from ener­ through from new detectors at the the so-called 'New Physics'. The getic photons, produced for example SPEAR electron-positron ring at existence of this new quantum num­ from the annihilation of colliding SLAC (see September 1979 issue, ber was one vital clue which radically electrons and positrons. Because page 246). Playing a prominent role changed our understanding of the the photon itself carries spin one, the in this search was the Crystal Ball basic forces in Nature. Since then selection rules for these reactions detector (a Caltech / Harvard / the careful study of charmonium say that only spin one charmonium Princeton / SLAC / Stanford colla­ spectroscopy has gone on to provide states can be formed directly. In boration). This spherical array of 672 much valuable information on quark experiments with colliding electron- sodium iodide crystals, each viewed dynamics. positron beams, singlet charmonium by a photomultiplier, gives good Charmed quarks and their antipar- shows up only in the subsequent angular coverage of the electron- ticles each carry intrinsic angular decays of the triplet variety, and is positron collision region, and good momentum (spin) of half a unit, and correspondingly more elusive. measurement of low energy photons according to the rules can combine Preliminary reports of the ground produced in the decay of triplet char­ together either with their spins state spin zero charmonium, now monium. parallel (a triplet state), giving a called the eta-c, came from experi­ These 'radiative' decays can pro­ meson of spin one, or with their spins ments at the DORIS electron-posi­ duce a variety of secondary char­ antiparallel (a singlet state), forming tron ring at DESY. Theoreticians had monium states, and the photon a spin zero particle. The J/psi has already deduced much from the spectrum from the Crystal Ball spin one, and since 1974, a rich unfolding spectrum of triplet char­ showed sharp peaks corresponding 68 CERN Courier, March 1981 to transitions between different tri­ At present, the characteristics of the mediated by the exchange of so- plet charmonium levels, in much the state are highly suggestive of the called gluons, similar in some res­ same way that sharp spectral lines eta-c, but further work is needed. pects to the photon exchange res­ show up when ordinary atoms are Elsewhere in the photon spectrum ponsible for the familiar electromag­ excited. In addition, a small but sta­ from radiative charmonium decays, netic force. As well as transiently tistically significant peak was seen in the Crystal Ball shows evidence for flitting between quarks, these gluons the spectrum corresponding to a decays producing a meson of mass should also be able to stick together new charmonium state of mass 1420 MeV. A small sample of spe­ to form 'gluonium' or 'glueballs'. 2983 MeV. Some months later, the cific decay modes for a meson of this Whether the E-meson signal seen in Mark II group (Berkeley / SLAC), mass was also reconstructed by radiative charmonium decays is a announced the first evidence for a both Mark II and the Crystal Ball. A glueball or not remains to be sett­ specific eta-c decay mode, while spin one meson of this mass, the E, led. another decay mode was found by has been known for some time With Mark II having already the Crystal Ball shortly afterwards. through the analysis of bubble moved to the bigger PEP ring, the This was already sufficient to make chamber exposures to hadron Crystal Ball is presently the only theoreticians feel better, but to pin beams. detector operating at SPEAR. Even down this new candidate charmon­ In the Crystal Ball, the radiative though its move to PEP has been ium state, its quantum numbers first transitions producing E-mesons ap­ approved, this will not take place for had to be fixed. peared to be quite copious, and this at least a year. An important task The Crystal Ball is well suited to led some people to speculate that remaining at SPEAR is to continue to measure electromagnetically show­ the E, rathe/ than being a conven­ search for the F-meson, carrying ering particles like electrons and tional meson built up of a quark and both charm and strangeness. F can­ photons. To handle charged hadrons an antiquark, could be an example of didates have now been reported required more work, and further evi­ a 'glueball' — a new type of matter from experiments at several Labora­ dence in favour of an eta-c assign­ much talked about but never before tories, but as yet none from SPEAR. ment for the new state came from seen. Other objectives include more eta-c analysis of channels containing ap­ Current thinking says that quarks data and a scan of the SPEAR energy propriate combinations of hadrons. interact through the 'colour' force regions so far largely neglected. Physics monitor soon come within the reach of labo­ Various characteristics of the Ultrahigh energy ratory experiments. fragmentation region of inelastic cosmic rays Meanwhile the cosmic ray spe­ hadron-nucleus interactions were cialists continue their studies, and covered, and detailed comparison of Cosmic ray experiments have tradi­ from 20-29 October, the city of the comparable data obtained by all tionally provided physicists with Nakhodka in the Soviet Far East was three groups shows quite reasona­ glimpses of behaviour beyond the host to a Soviet-Japanese sympo­ ble agreement in a number of res­ energy range attainable with artifi­ sium on processes at ultrahigh ener­ pects. cial particle beams. However with gies in cosmic rays, investigated 1. The cross-section of the hadron the CERN antiproton project promis­ using emulsion chambers exposed inelastic interaction with an air ing to provide collision energies at altitude. There were participants nucleus still increases at least up to equivalent to those of 1 55 000 GeV from the Japanese/Brazilian colla­ energies of 1015eV at nearly the beams, and with the prospect of boration at Mount Chacaltaya in the same rate as at accelerator ener­ ISABELLE at Brookhaven going Andes, from the group carrying out gies. even higher, physicists hope that experiments on Mount Fuji, Japan, 2. At ultrahigh energies there is con­ some of the exotic behaviour and from the 'Pamir' Soviet-Polish siderable deviation of scaling not reported from cosmic ray studies will collaboration. only in pionization but also in the CERN Courier, March 1981 69 .
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