Spectroscopy Qf . & Ight and Heavy Quarks
نویسنده
چکیده
New results on various controversial light mesons are reviewed, including the glueball candidates fs(1720) and ~(1460), the 1 ++-O-+ mass " coincidences " fi(1285)-n(1275) and fi(1420)-q(1420), as well as evidence for the X(3100)+Ap+nx and the p(148O)+&r, which have quantum numbers not allowed for qq. The 77+W dfects move out of the threshold region with data on 77+wp. Statistically weak data on I',(~~) and the search for heavy quark 'Pi states are presented. Pee, B,,, and Ptot for the Y(lS), Y(2S), and Y(3S) are updated using new data and a consistent treatment of the radiative corrections for I',. New data on the mass splittings of the xb(2P) compare favorably with the scalar confinement model, which may however have new trouble. This review was supposed to cover all the spec-troscopy presented in 3 parallel sessions: 77 Interactions , Heavy Bound-Quark States, and a particularly full session on Hadron Spectroscopy. It was too much, even aft,er the usual restriction to things I found interesting and could understand, and in desperation I decided to exclude baryons and Qq mesons. I sincerely hope the next conference offers those fields better treatment (and more time!) 2 KK and qq Resonances The light mesons part of this paper may be more than the casual reader wants to digest. There are many details, and few firm conclusions. However to simplify would be to mislead. Heavy mesons are a lot easier to deal with, and the last pages are devoted with relief to them. 1 New Meson Names Starting this year the Particle Data Group asks us to use their new naming scheme for hadrons [I]. New and old names are compared in Table 1. Much of this talk is devoted to the 3P~ states, which have Jpc = O++, l++, and 2 ++. The new scheme unifies them, with a subscript to label the spin. f stands for I=0 and a for I=l. If you can remember that S' and 6 were O++ mesons with I=0 and 1, you know that they are now fo and a+ The first step is harder than the second, demonstrating the need for new names. However progress is always accompanied by some pain. f' and 0 were a lot easier than fr(1525) and fs(1720). The search for glueballs has occupied many people over the last several years. At first there was hope that a candidate would be found satisfying all the criteria …
منابع مشابه
AROMA 2.2 – A Monte Carlo Generator for Heavy Flavour Events in ep Collisions
A program to simulate the production of heavy quarks through the boson-gluon fusion process in ep collisions is presented. The full electroweak structure of the electron–gluon interaction is taken into account as well as the masses of the produced heavy quarks. Higher order QCD radiation is treated using initial and final state parton showers, and hadronization is performed using the Lund strin...
متن کاملar X iv : h ep - p h / 94 07 22 4 v 1 5 J ul 1 99 4
We review the spectroscopy and some properties of hadrons containing two charmed quarks, or more generally, two heavy quarks. This includes heavy baryons such as (bcu), and possible exotic multiquark states.
متن کاملHadronic Spectroscopy from the Lattice: Glueballs and Hybrid Mesons
Lattice QCD determinations appropriate to hadron spectroscopy are reviewed with emphasis on the glueball and hybrid meson states in the quenched approximation. Hybrids are discussed for heavy and for light quarks. The effects of sea quarks (unquenching) are explored.
متن کاملThe Theory of Heavy Baryons A
I discuss the theory of heavy baryon spectroscopy, emphasizing predictions which follow from light and heavy quark symmetries. The experimental data which are available for the properties of heavy (charmed and bottom) baryons continue to improve steadily in both quantity and quality. As a result, it is important for us to take more seriously the theory of these states, so that these measurement...
متن کاملar X iv : h ep - p h / 97 10 50 2 v 1 2 8 O ct 1 99 7 Hadron Spectroscopy from the Lattice
Lattice QCD determinations appropriate to hadron spectroscopy are reviewed with emphasis on the glueball and hybrid meson states in the quenched approximation. Hybrids are discussed for heavy and for light quarks. The effects of sea quarks (unquenching) are explored. Heavy-light systems are presented particularly excited B mesons.
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 1986