749 research outputs found
QCD sum rules for the anti-charmed pentaquark
We present a QCD sum rule analysis for the anti-charmed pentaquark state with
and without strangeness. While the sum rules for most of the currents are
either non-convergent or dominated by the continuum, the one for the
non-strange pentaquark current composed of two diquarks and an antiquark, is
convergent and has a structure consistent with a positive parity pentaquark
state after subtracting out the continuum contribution. Arguments are
presented on the similarity between the result of the present analysis and that
based on the constituent quark models, which predict a more stable pentaquark
states when the antiquark is heavy.Comment: 19 pages, 8 figures, REVTex, revised version,new figures added and
references update
Pentaquark state in pole-dominated QCD sum rules
We propose a new approach in QCD sum rules applied for exotic hadrons with a
number of quarks, exemplifying the pentaquark Theta^{+} (I=0,J=1/2) in the
Borel sum rule. Our approach enables reliable extraction of the pentaquark
properties from the sum rule with good stability in a remarkably wide Borel
window. The appearance of its valid window originates from a favorable setup of
the correlation functions with the aid of it chirality of the interpolating
fields on the analogy of the Weinberg sum rule for the vector currents. Our
setup leads to large suppression of the continuum contributions which have
spoiled the Borel stability in the previous analyses, and consequently enhances
importance of the higher-dimensional contributions of the OPE, which are
indispensable for investigating the pentaquark properties. Implementing the OPE
analysis up to dimension 15, we find that the sum rules for the chiral-even and
odd parts independently give the Theta^{+} mass of 1.68 pm 0.22 GeV with
uncertainties of the condensate values. Our sum rule indeed gives rather flat
Borel curves almost independent of the continuum thresholds both for the mass
and pole residue. Finally, we also discuss possible isolation of the observed
states from the KN scattering state on view of chiral symmetry.Comment: 8 pages, 7 figure
Pentaquark and diquark-diquark clustering: a QCD sum rule approach
In this work we study the Theta(1540) in the framework of QCD sum rules based
on (ud)^2\bar{s} diquark clustering as suggested by Jaffe and Wilczek. Within
errors, the mass of the pentaquark is compatible with the experimentally
measured value. The mass difference between the Theta and the pentaquark with
the quantum numbers of the nucleon amounts to 70 MeV, consistent with the
interpretation of the N(1440) as a pentaquark.Comment: 10 pages, 3 figures; discussions extended, references added, version
to appear in Phys. Lett.
Spin 3/2 Pentaquarks
We investigate the possible existence of the spin 3/2 pentaquark states using
interpolating currents with K-N color-octet structure in the framework of QCD
finite energy sum rule (FESR). We pay special attention to the convergence of
the operator product expansion
Spin-3/2 pentaquark in the QCD sum rule
We study and pentaquark states with in
the QCD sum rule approach. The QCD sum rule for positive parity states and that
for negative parity are independently derived. The sum rule suggests that there
exist the and the states. These states may be observed as
extremely narrow peaks since they can be much below the -wave threshold and
since the only allowed decay channels are in -wave, whose centrifugal
barriers are so large that the widths are strongly suppressed. The
state may be assigned to the observed and the state
can be a candidate for .Comment: 27 pages, 14 figure
Magnetic Moment of The Pentaquark State
We have calculated the magnetic moment of the recently observed
pentaquark in the framework of the light cone QCD sum rules using the photon
distribution amplitudes. We find that ,
which is quite small. We also compare our result with predictions of other
groups.Comment: 1 eps figure, 13 page
Are the pentaquark sum rules reliable?
We rewiew and scrutinize the existing mass determinations of the pentaquarks
from the exponential Laplace Sum Rules (LSR). We do not find any sum rule
window for extracting optimal and reliable results from the LSR, due to the
unusual slow convergence of the OPE and to the exceptional important role of
the QCD continuum into the spectral function in this channel. Instead, we use
in this channel,for the first time, Finite Energy Sum Rules (FESR), which
exhibit a nice stability in the QCD continuum threshold t_c, at which one can
extract, with a good accuracy, the mass of the lowest resonance. Including the
D=7, 9 condensate contributions in the OPE, we obtain M_Theta=(1513+- 114) MeV,
and the corresponding residue lambda_Theta^2= -(0.14-- 0.49)x 10^{-9} GeV^{12},
which favours the I=0, J=1/2, and negative parity S-wave interpretation of the
Theta (1540). However, our analysis indicates a degeneracy between the unmixed
I=0 and I=1 S-wave states. In the I=0, J=1/2, P-wave channel, we obtain, for
the P-resonance, M_P = (1.99+- 0.19) GeV and lambda_P= -(0.7--7.1)x 10^{-9}
GeV^{14}, which we expect to be discovered experimentally. Our results also
suggest that some intuitive choices of the continuum threshold used in the LSR
literature are inconsistent with the FESR results. Finally, a study of the
Theta-K-N coupling using a vertex sum rule shows that, for the I=0, S-wave
channel, the leading OPE contributions only start to order alpha_s^2 in the
chiral limit m_s=0, indicating that the Theta is very narrow.Comment: Latex file 6 pages, 5 ps.figures. Contribution to the QCD 04
International Conference (Montpellier-5-9th July 2004) and to HEP-MAD 04
International Conference (Antananarivo 27th Sept-2nd Oct. 2004). To appear in
Nucl. Phys. B (Proc. Suppl.) and in SLAC Econf. on-line Proceedings. Comments
and References adde
Spectroscopy of Pentaquark Baryons
A review is given to pentaquark mass predictions in quark models and QCD. It
is pointed out that no successful quark model prediction is available for
low-lying pentaquark states. Some new results of direct application of QCD, QCD
sum rules and lattice QCD, are also presented.Comment: Talk presented at the International Conference on QCD and Hadronic
Physics, June 16-20, 2005, Beijing, China, 6 page
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