9,344 research outputs found

    The hidden-charm pentaquark and tetraquark states

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    In the past decade many charmonium-like states were observed experimentally. Especially those charged charmonium-like ZcZ_c states and bottomonium-like ZbZ_b states can not be accommodated within the naive quark model. These charged ZcZ_c states are good candidates of either the hidden-charm tetraquark states or molecules composed of a pair of charmed mesons. Recently, the LHCb Collaboration discovered two hidden-charm pentaquark states, which are also beyond the quark model. In this work, we review the current experimental progress and investigate various theoretical interpretations of these candidates of the multiquark states. We list the puzzles and theoretical challenges of these models when confronted with the experimental data. We also discuss possible future measurements which may distinguish the theoretical schemes on the underlying structures of the hidden-charm multiquark states.Comment: Review accepted by Physics Reports, 152 pages, 66 figures, and 29 table

    Isospin symmetry breaking of K and K* mesons

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    We use the method of QCD sum rules to investigate the isospin symmetry breaking of K and K* mesons. The electromagnetic effect, difference between up and down current-quark masses and difference between up and down quark condensates are important. We perform sum rule analyses of their masses and decay constant differences, which are consistent with experimental values. Our results yield Delta f_K = f_{K^0} - f_{K^\pm} = 1.5 MeV.Comment: 9 pages, 7 figures, one reference adde

    Light Scalar Mesons in the QCD Sum Rule

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    We study the light scalar mesons in the QCD sum rule. We find that there are five independent scalar tetraquark currents in the local form, and we perform QCD sum rule analysis using both these currents and their combinations. Compared with the sum rules by conventional \bar{q} q currents, our result supports a tetraquark structure for low-lying scalar mesons.Comment: 4 pages, 1 figure. Talk given at the Yukawa International Seminar (YKIS) 2006, "New frontiers in QCD", Kyoto, Japan, 20 Nov. - 8 Dec. 200

    Mass spectra of Zc and Zb exotic states as hadron molecules

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    We construct charmonium-like and bottomonium-like molecular interpolating currents with quantum numbers J(PC)=1(+-) in a systematic way, including both color singlet-singlet and color octet-octet structures. Using these interpolating currents, we calculate two-point correlation functions and perform QCD sum rule analyses to obtain mass spectra of the charmonium-like and bottomonium-like molecular states. Masses of the charmonium-like q_bar c c_bar q molecular states for these various currents are extracted in the range 3.85-4.22 GeV, which are in good agreement with observed masses of the Zc resonances. Our numerical results suggest a possible landscape of hadronic molecule interpretations of the newly-observed Zc states. Mass spectra of the bottomonium-like q_bar b b_bar q molecular states are similarly obtained in the range 9.92-10.48 GeV, which support the interpretation of the Zb(10610) meson as a molecular state within theoretical uncertainties. Possible decay channels of these molecular states are also discussed.Comment: 15 pages, 3 figures, 2 tables, accepted by PR

    The Possible J^{PC}=0^{--} Exotic State

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    In order to explore the possible existence of the exotic 0−−0^{--} state, we have constructed the tetraquark interpolating operators systematically. As a byproduct, we notice the 0+−0^{+-} tetraquark operators without derivatives do not exist. The special Lorentz structure of the 0−−0^{--} currents forbids the four-quark correction to the spectral density. Now the gluon condensate is the dominant power correction. Within the framework of the finite energy sum rule, none of the seven interpolating currents supports a resonant signal. Therefore we conclude that the exotic 0−−0^{--} state does not exist below 2 GeV, which is consistent with the current experimental observations.Comment: 12 pages, 27 figure

    Light vector meson and heavy baryon strong interaction

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    We calculate the coupling constants between the light vector mesons and heavy baryons within the framework of the light-cone QCD sum rule in the leading order of heavy quark effective theory. Most resulting sum rules are stable with the variations of the Borel parameter and the continuum threshold. The extracted couplings will be useful in the study of the possible heavy baryon molecular states

    Establishing low-lying doubly charmed baryons

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    We systematically study the SS-wave doubly charmed baryons using the method of QCD sum rules. Our results suggest that the Ξcc++\Xi_{cc}^{++} recently observed by LHCb can be well identified as the SS-wave Ξcc\Xi_{cc} state of JP=1/2+J^P = 1/2^+. We study its relevant Ωcc\Omega_{cc} state, whose mass is predicted to be around 3.7 GeV. We also systematically study the PP-wave doubly charmed baryons, whose masses are predicted to be around 4.1 GeV. Especially, there can be several excited doubly charmed baryons in this energy region, and we suggest to search for them in order to study the fine structure of the strong interaction.Comment: 6 pages, 2 figures, 1 table; A mistake was found when evaluating decay constants of the S-wave charmed baryons. The conclusion is not change

    Light Scalar Meson sigma(600) in QCD Sum Rule with Continuum

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    The light scalar meson sigma(600) is known to appear at low excitation energy with very large width on top of continuum states. We investigate it in the QCD sum rule as an example of resonance structures appearing above the corresponding thresholds. We use all the possible local tetraquark currents by taking linear combinations of five independent local ones. We ought to consider the pi-pi continuum contribution in the phenomenological side of the QCD sum rule in order to obtain a good sum rule signal. We study the stability of the extracted mass against the Borel mass and the threshold value and find the sigma(600) mass at 530 MeV +- 40 MeV. In addition we find the extracted mass has an increasing tendency with the Borel mass, which is interpreted as caused by the width of the resonance.Comment: 9 pages, 7 figures, comments and suggestions welcom
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