Low energy scattering and charmonium radiative decay from lattice QCD

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Presentation transcript:

Low energy scattering and charmonium radiative decay from lattice QCD Institute of Theoretical Physics Peking University Chuan Liu

Outline J/psi radiative decay to scalar glueball (still going…) Low-energy D*D1 scattering and the nature of Z(4430)(PRD80:034503, 2009) J/psi radiative decay to scalar glueball (still going…) Other works… Summary

Basic status of the collaboration People Y. Chen (IHEP, CAS) C. Liu (Peking University) Y.B. Liu (Nankai University) J.P. Ma (ITP, CAS) J.B. Zhang (Zhejiang University) Postdocs(Yi-bo Yang)+students Funding Funded by NSFC, etc. Computing facilities: Shanghai, Tianjin, Beijing…

D*D1 scattering and Z(4430)

Signal for Z(4430) Resonance structure Z(4430) Q=+1, JP=0-,1-,2- S.K. Choi et al., PRL 100,142001 (2008) Resonance structure Z(4430) Close to threshold Q=+1, JP=0-,1-,2- M=4433 MeV G=45 MeV

Theoretical investigations Phenomenology Shallow bound state (S.L. Zhu et al, PRD77,034003) Tetra-quark resonance above threshold (X.-H Liu et al, PRD77, 094005) Threshold enhancement (J.L. Rosner, PRD76,114002) Need to study scattering near threshold Scattering length a0 and effective range r0 Lattice QCD study (quenched)

Utilizing Lüscher’s formalism Consider two hadrons in a finite box interaction:shift of two-particle energy interaction: scattering phase shifts Lüscher’s formula:

Basic formulae A box of size L, periodic in all three spatial directions: Two interacting hadrons

Taking advantage of asymmetric box Use asymmetric volumes: L×(h2 L)×(h3 L) Take: h2=1, h3>1 The symmetry for the box is D4

Single hadron operators Single particle operators Angular momentum decomposition D*+

Double hadron operators

Correlation matrix Only the correlation matrix in A1 channel shows signal We have computed 5 lowest non-zero momentum modes together with the zero momentum mode.

Simulation setup Tadpole improved clover action on anisotropic lattices

Checking single particle states

Extract two-hadron energy Appropriate ratios are taken:

Obtaining a0 & r0 Scattering length a0 & effective range r0

extrapolations After all the extrapolations

discussions Possible bound state? For shallow bound state, But our scattering lengths are all positive On the verge of developing a bound state Using the square well potential model to estimate, the potential well is V0=70(10) MeV, R=0.7fm. Our results is not in favor of a shallow bound state

Glueballs in J/psi radiative decays

QCD predicts the existence of glueballs I. Introduction QCD predicts the existence of glueballs Quenched LQCD predicts glueball spectrum in the range 1~3GeV candidates: f0(1370), f0(1500), f0(1710) etc. J/psi radiative decay can be the best hunting ground. BESIII is producing 1010 J/psi events Y. Chen et al, Phys. Rev. D 73, 014516 (2006)

Hadronic matrix element The computation of J/psi radiative decay into glueballs breaks up into perturbative part (QED part) and non-perturbative part The non-perturbative part requires the computation of matrix element J/Y state Glueball state EM current

Three-point function Scalar glueball operator Electromagnetic current operator Charmonium operator

After the intermediate state insertion, the three-point function can be written as Two-point function of vector meson

II. Numerical details 1. Lattice and parameters Anisotropic lattice: Strong coupling: 2. Actions

5000 gauge configurations, separated by 100 HB sweeps 3. Configurations and quark propagators In order to get fair signals of the three point functions, a large enough statistics is required. 5000 gauge configurations, separated by 100 HB sweeps Charm quark mass is set by the physical mass of J/psi On each configuration, 96 charm quark propagators are calculated with point sources on all the 96 time slices. The periodic boundary conditions are used both for the spatial and temporal directions.

4. The glueball operators Building prototypes (various Wilson loops) Smearing: Single link scheme (APE) and double link scheme (fuzzying) The essence of the VM is to find a set of combinational coefficients such that the operator couples mostly to a specific state.

The horizontal line is the theoretical prediction with . It is seen that the deviations are less than 5% The energies of 27 momentum modes of scalar glueballs are calculated. Plotted are the plateaus using the optimized operators

5. Three point functions Temporarily, we only analyze the following cases:

The plots for the ratios Exponential fit by taking the glueball energies as known parameters

These are known functions

Preliminary ! 6. The form factor and the decay width Polynomial fit: The branch ratio is

6. Renormalization constant In this study, naïve local current operator is used which needs a multiplicative renormalization ZV

6. Renormalization constant (cont.)

Summary Quenched lattice QCD study on J P = 0 – channel scattering yields scattering length a0 and effective range r0. Two meson interaction is attractive, but unlikely to form a bound state. Unquenched study desired Preliminary quenched study on J/psi radiative decay to scalar glueball is performed with the result: G=0.030(5)keV. More to be checked (current renormalization, extrapolations, other channels etc.) Larger lattices (12^3*144, working…)