–1– Pentaquarks

ثبت نشده
چکیده

(3100), and for the early unsuccessful attempts to confirm them. The table below lists papers published since then giving results of further unsuccessful searches. There are experiments at high energies and low; in new reactions and old; there are experiments—some by the same groups that claimed the original discoveries—with orders-of-magnitude greater statistics than before; there are experiments that find 100,000 Λ(1520)s in ¯ KN , but no hint of a Θ(1540) in KN. Many of the experiments search over large ranges of mass. The limits on production of a pentaquark given in the last column of the table are at 90 or 95% confidence level; the cross-section limits are in some cases now fractions of a nanobarn. The limits often involve assumptions about the width of the pentaquark, its production angular distribution, or other matters. There is not room (or reason) to give here all the details—for which, see the papers. There are two or three recent experiments that find weak evidence for signals near the nominal masses, but there is simply no point in tabulating them in view of the overwhelming evidence that the claimed pentaquarks do not exist. The only advance in particle physics thought worthy of mention in the American Institute of Physics " Physics News in 2003 " was a false alarm. The whole story—the discoveries themselves, the tidal wave of papers by theorists and phenomenologists that followed, and the eventual " undiscovery " —is a curious episode in the history of science.

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Mass spectrum of spin-1/2 pentaquarks with a cc̄ component and their anticipated discovery modes in b-baryon decays

The LHCb discovery of the two baryonic states P c (4380) and P + c (4450), having J P = 3/2− and J = 5/2, respectively, in the process pp → bb̄ → ΛbX, followed by the decay Λb → J/ψ p K−, has motivated a number of theoretical models. Interpreting them as compact {c̄ [cu] [ud];LP = 0, 1} objects, the mass spectroscopy of the J = 3/2− and J = 5/2 pentaquarks was worked out by us for the pentaquarks...

متن کامل

44 2 v 1 2 5 M ar 1 99 8 Positive parity pentaquarks in a Goldstone boson exchange model

We study the stability of the pentaquarks uuddQ, uudsQ and udssQ (Q = c, b, or t) of positive parity in a constituent quark model based on Goldstone boson exchange interaction between quarks. The pentaquark parity is the antiquark parity times that of a quark excited to a p-shell. We show that the Goldstone boson exchange interaction favors these pentaquarks much more than the negative parity o...

متن کامل

The Discovery and Properties of Pentaquarks

The pentaquarks are exotic baryons formed of four quarks and an antiquarks. Their existence has been discussed in the literature over the last 30 years or more, first in connection with kaon nucleon scattering data. The subject has been revived by the end of 2002 when experimental evidence of a narrow baryon of strangeness S = + 1, and mass M ≃ 1530 MeV has been found. This is interpreted as th...

متن کامل

Magnetic moments of antidecuplet pentaquarks

We analyze the magnetic moments of the exotic pentaquarks of the flavor antidecuplet in the constituent quark model for the case in which the ground state is in an orbital L = 0 or a L = 1− state. We derive sum rules for the magnetic moments. The magnetic moment of the Θ(1540) is found to be 0.38, 0.09 and 1.05 μN for J p = 1/2−, 1/2 and 3/2, respectively, which is compared with the results obt...

متن کامل

Spectrum of the Y=2 Pentaquarks

By assuming a mass formula for the spectrum of the Y = 2 pentaquarks, where the chromo-magnetic interaction plays a main role, and identifying the lightest state with the Θ + (1540), we predict a spectrum in good agreement with the few I = 0 and I = 1 candidates proposed in the past.

متن کامل

Positive parity pentaquarks in a Goldstone boson exchange model

We study the stability of the pentaquarks uuddQ, uudsQ and udssQ (Q = c, b, or t) of positive parity in a constituent quark model based on Goldstone boson exchange interaction between quarks. The pentaquark parity is the antiquark parity times that of a quark excited to a p-shell. We show that the Goldstone boson exchange interaction favors these pentaquarks much more than the negative parity o...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2008