Ted Barnes
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The organizations / institutes from the scholar's other articles in the past ten years
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Ted Barnes has a total of 15 co-authors. Here are the top co-authors by number of shared publications:
- Xiaoguang Li
Department of Physics and Astronomy University of Tennessee 37996-1200 Knoxville TN USA
6 shared publications - Eric Scott Swanson
University of Pittsburgh
5 shared publications - Stephen Godfrey
Ottawa-Carleton Institute for Physics, Carleton University, 1125 Colonel By Drive, Ottawa, Ontario K1S 5B6, Canada
4 shared publications - Winston Roberts
Department of Physics Florida State University 32306 Tallahassee FL USA
4 shared publications - A. Lundborg
Uppsala University, Department of Radiation Sciences, SE-75121 Uppsala, Sweden
2 shared publications - Frank E. Close
Rudolf Peierls Centre for Theoretical Physics University of Oxford 1 Keble Road OX1 3NP Oxford
2 shared publications
Latest Publications
- Open Access
Update on Charmonium Theory
In this invited presentation I review some recent developments in the theory of charmonium that appear likely to be of importance for future experimental studies in this field. The specific areas considered are double charmonium production, LQCD studies of charmonium, recent results for hadron loops, c-cbar production cross sections at PANDA, charm molecules, and two recent developments, "charmiscelleny".
Open AccessUpdate on Charmonium Theory
In this invited presentation I review some recent developments in the theory of charmonium that appear likely to be of importance for future experimental studies in this field. The specific areas considered are double charmonium production, LQCD studies of charmonium, recent results for hadron loops, c-cbar production cross sections at PANDA, charm molecules, and two recent developments, "charmiscelleny".
- 19 February 2010
- Published by American Physical Society (APS) in Physical Review D
- Vol. 81 (3)
Meson emission model ofcharmonium strong decaysIn this paper we consider a sequential ``meson emission'' mechanism for charmonium decays of the type $\Psi${}$\rightarrow${}NN\ifmmode\bar\else\textasciimacron\fi{}m, where $\Psi${} is a generic charmonium state, N is a nucleon, and m is a light meson. This decay mechanism, which may not be dominant in general, assumes that an NN\ifmmode\bar\else\textasciimacron\fi{} pair is created during charmonium annihilation, and the light meson m is emitted from the outgoing nucleon or antinucleon line. A straightforward generalization of this model can incorporate intermediate N* resonances. We derive Dalitz plot event densities for the cases $\Psi${}=$\eta${}c, J/$\psi${}, $\chi${}c0, $\chi${}c1, and $\psi${}$'${}; and m=$\pi${}0, f0, and $\omega${} (and implicitly, any 0-+, 0++, or 1-- final light meson). It may be possible to separate the contribution of this decay mechanism to the full decay amplitude through characteristic event densities. For the decay subset $\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 the two model parameters are known, so we are able to predict absolute numerical partial widths for $\Gamma${}($\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0). In the specific case J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 the predicted partial width and Mp$\pi${} event distribution are intriguingly close to experiment. We also consider the possibility of scalar meson and glueball searches in $\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}f0. If the meson emission contributions to $\Psi${}$\rightarrow${}NN\ifmmode\bar\else\textasciimacron\fi{}m decays can be isolated and quantified, they can be used to estimate meson-nucleon strong couplings {gNNm}, which are typically poorly known, and are a crucial input in meson exchange models of the NN interaction. The determination of gNN$\pi${} from J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 and the (poorly known) gNN$\omega${} and the anomalous ``strong magnetic'' coupling $\kappa${}NN$\omega${} from J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\omega${} are considered as examples.
- 19 February 2010
- Published by American Physical Society (APS) in Physical Review D
- Vol. 81 (3)
Meson emission model ofcharmonium strong decaysIn this paper we consider a sequential ``meson emission'' mechanism for charmonium decays of the type $\Psi${}$\rightarrow${}NN\ifmmode\bar\else\textasciimacron\fi{}m, where $\Psi${} is a generic charmonium state, N is a nucleon, and m is a light meson. This decay mechanism, which may not be dominant in general, assumes that an NN\ifmmode\bar\else\textasciimacron\fi{} pair is created during charmonium annihilation, and the light meson m is emitted from the outgoing nucleon or antinucleon line. A straightforward generalization of this model can incorporate intermediate N* resonances. We derive Dalitz plot event densities for the cases $\Psi${}=$\eta${}c, J/$\psi${}, $\chi${}c0, $\chi${}c1, and $\psi${}$'${}; and m=$\pi${}0, f0, and $\omega${} (and implicitly, any 0-+, 0++, or 1-- final light meson). It may be possible to separate the contribution of this decay mechanism to the full decay amplitude through characteristic event densities. For the decay subset $\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 the two model parameters are known, so we are able to predict absolute numerical partial widths for $\Gamma${}($\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0). In the specific case J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 the predicted partial width and Mp$\pi${} event distribution are intriguingly close to experiment. We also consider the possibility of scalar meson and glueball searches in $\Psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}f0. If the meson emission contributions to $\Psi${}$\rightarrow${}NN\ifmmode\bar\else\textasciimacron\fi{}m decays can be isolated and quantified, they can be used to estimate meson-nucleon strong couplings {gNNm}, which are typically poorly known, and are a crucial input in meson exchange models of the NN interaction. The determination of gNN$\pi${} from J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\pi${}0 and the (poorly known) gNN$\omega${} and the anomalous ``strong magnetic'' coupling $\kappa${}NN$\omega${} from J/$\psi${}$\rightarrow${}pp\ifmmode\bar\else\textasciimacron\fi{}$\omega${} are considered as examples.
- Open Access
Meson Emission Model of Psi to N Nbar m Charmonium Strong Decays
In this paper we consider a sequential "meson emission" mechanism for charmonium decays of the type Psi -> N Nbar m, where Psi is a generic charmonium state, N is a nucleon and m is a light meson. This decay mechanism, which may not be dominant in general, assumes that an NNbar pair is created during charmonium annihilation, and the light meson m is emitted from the outgoing nucleon or antinucleon line. A straightforward generalization of this model can incorporate intermediate N* resonances. We derive Dalitz plot event densities for the cases Psi = eta_c, J/psi, chi_c0, chi_c1} and psi' and m = pi0, f0 and omega (and implicitly, any 0^{-+}, 0^{++} or 1^{--} final light meson). It may be possible to separate the contribution of this decay mechanism to the full decay amplitude through characteristic event densities. For the decay subset Psi -> p pbar pi0 the two model parameters are known, so we are able to predict absolute numerical partial widths for Gamma(Psi -> p pbar pi0). In the specific case J/psi -> p pbar pi0 the predicted partial width and M_{p pi0} event distribution are intriguingly close to experiment. We also consider the possibility of scalar meson and glueball searches in Psi -> p pbar f0. If the meson emission contributions to Psi -> N Nbar m decays can be isolated and quantified, they can be used to estimate meson-nucleon strong couplings {g_NNm}, which are typically poorly known, and are a crucial input in meson exchange models of the NN interaction. The determination of g_NNpi from J\psi -> p pbar pi0 and the (poorly known) g_NNomega and the anomalous "strong magnetic" coupling kappa_{NNomega} from J/psi -> p pbar omega are considered as examples.
Open AccessMeson Emission Model of Psi to N Nbar m Charmonium Strong Decays
In this paper we consider a sequential "meson emission" mechanism for charmonium decays of the type Psi -> N Nbar m, where Psi is a generic charmonium state, N is a nucleon and m is a light meson. This decay mechanism, which may not be dominant in general, assumes that an NNbar pair is created during charmonium annihilation, and the light meson m is emitted from the outgoing nucleon or antinucleon line. A straightforward generalization of this model can incorporate intermediate N* resonances. We derive Dalitz plot event densities for the cases Psi = eta_c, J/psi, chi_c0, chi_c1} and psi' and m = pi0, f0 and omega (and implicitly, any 0^{-+}, 0^{++} or 1^{--} final light meson). It may be possible to separate the contribution of this decay mechanism to the full decay amplitude through characteristic event densities. For the decay subset Psi -> p pbar pi0 the two model parameters are known, so we are able to predict absolute numerical partial widths for Gamma(Psi -> p pbar pi0). In the specific case J/psi -> p pbar pi0 the predicted partial width and M_{p pi0} event distribution are intriguingly close to experiment. We also consider the possibility of scalar meson and glueball searches in Psi -> p pbar f0. If the meson emission contributions to Psi -> N Nbar m decays can be isolated and quantified, they can be used to estimate meson-nucleon strong couplings {g_NNm}, which are typically poorly known, and are a crucial input in meson exchange models of the NN interaction. The determination of g_NNpi from J\psi -> p pbar pi0 and the (poorly known) g_NNomega and the anomalous "strong magnetic" coupling kappa_{NNomega} from J/psi -> p pbar omega are considered as examples.
- Open Access
Hadron Loops: General Theorems and Application to Charmonium
In this paper we develop a formalism for incorporating hadron loops in the quark model. We derive expressions for mass shifts, continuum components and mixing amplitudes of "quenched" quark model states due to hadron loops, as perturbation series in the valence-continuum coupling Hamiltonian. We prove three general theorems regarding the effects of hadron loops, which show that given certain constraints on the external "bare" quark model states, the valence-continuum coupling, and the hadrons summed in the loops, the following results hold: (1) The loop mass shifts are identical for all states within a given N,L multiplet. (2) These states have the same total open-flavor decay widths. (3) Loop-induced valence configuration mixing vanishes provided that ${\L}_i \neq \L_f$ or $\S_i \neq \S_f$. The charmonium system is used as a numerical case study, with the $^3\P_0$ decay model providing the valence-continuum coupling. We evaluate the mass shifts and continuum mixing numerically for all 1S, 1P and 2S charmonium valence states due to loops of D, D$^*$, D$_s$ and D$_s^*$ meson pairs. We find that the mass shifts are quite large, but are numerically similar for all the low-lying charmonium states, as suggested by the first theorem. Thus, loop mass shifts may have been "hidden" in the valence quark model by a change of parameters. The two-meson continuum components of the physical charmonium states are also found to be large, creating challenges for the interpretation of the constituent quark model.Open AccessHadron Loops: General Theorems and Application to Charmonium
In this paper we develop a formalism for incorporating hadron loops in the quark model. We derive expressions for mass shifts, continuum components and mixing amplitudes of "quenched" quark model states due to hadron loops, as perturbation series in the valence-continuum coupling Hamiltonian. We prove three general theorems regarding the effects of hadron loops, which show that given certain constraints on the external "bare" quark model states, the valence-continuum coupling, and the hadrons summed in the loops, the following results hold: (1) The loop mass shifts are identical for all states within a given N,L multiplet. (2) These states have the same total open-flavor decay widths. (3) Loop-induced valence configuration mixing vanishes provided that ${\L}_i \neq \L_f$ or $\S_i \neq \S_f$. The charmonium system is used as a numerical case study, with the $^3\P_0$ decay model providing the valence-continuum coupling. We evaluate the mass shifts and continuum mixing numerically for all 1S, 1P and 2S charmonium valence states due to loops of D, D$^*$, D$_s$ and D$_s^*$ meson pairs. We find that the mass shifts are quite large, but are numerically similar for all the low-lying charmonium states, as suggested by the first theorem. Thus, loop mass shifts may have been "hidden" in the valence quark model by a change of parameters. The two-meson continuum components of the physical charmonium states are also found to be large, creating challenges for the interpretation of the constituent quark model. - Open Access
- 14 May 2008
- Published by American Physical Society (APS) in Physical Review C
- Vol. 77 (5) , 055206
Hadron loops: General theorems and application to charmonium
In this paper, we develop a formalism for incorporating hadron loops into the quark model. We derive expressions for mass shifts, continuum components, and mixing amplitudes of “quenched” quark model states due to hadron loops, as perturbation series in the valence-continuum coupling Hamiltonian. We prove three general theorems regarding the effects of hadron loops, which show that given certain constraints on the external “bare” quark model states, the valence-continuum coupling, and the hadrons summed in the loops, the following results hold: (1) The loop mass shifts are identical for all states within a given multiplet. (2) These states have the same total open-flavor decay widths. (3) Loop-induced valence configuration mixing vanishes provided that or . The charmonium system is used as a numerical case study, with the decay model providing the valence-continuum coupling. We evaluate the mass shifts and continuum mixing numerically for all , and charmonium valence states due to loops of , and meson pairs. We find that the mass shifts are quite large but numerically similar for all the low-lying charmonium states, as suggested by the first theorem. Thus, loop mass shifts may have been “hidden” in the valence quark model by a change of parameters. The two-meson continuum components of the physical charmonium states are also found to be large, creating challenges for the interpretation of the constituent quark model.- 14 May 2008
- Published by American Physical Society (APS) in Physical Review C
- Vol. 77 (5) , 055206
Open AccessHadron loops: General theorems and application to charmonium
In this paper, we develop a formalism for incorporating hadron loops into the quark model. We derive expressions for mass shifts, continuum components, and mixing amplitudes of “quenched” quark model states due to hadron loops, as perturbation series in the valence-continuum coupling Hamiltonian. We prove three general theorems regarding the effects of hadron loops, which show that given certain constraints on the external “bare” quark model states, the valence-continuum coupling, and the hadrons summed in the loops, the following results hold: (1) The loop mass shifts are identical for all states within a given multiplet. (2) These states have the same total open-flavor decay widths. (3) Loop-induced valence configuration mixing vanishes provided that or . The charmonium system is used as a numerical case study, with the decay model providing the valence-continuum coupling. We evaluate the mass shifts and continuum mixing numerically for all , and charmonium valence states due to loops of , and meson pairs. We find that the mass shifts are quite large but numerically similar for all the low-lying charmonium states, as suggested by the first theorem. Thus, loop mass shifts may have been “hidden” in the valence quark model by a change of parameters. The two-meson continuum components of the physical charmonium states are also found to be large, creating challenges for the interpretation of the constituent quark model. - 6 March 2008
- Published by American Physical Society (APS) in Physical Review D
- Vol. 77 (5) , 056001
Evidence for aPauli strong coupling?The couplings of charmonia and charmonium hybrids (generically ) to are of great interest in view of future plans to study these states using an antiproton storage ring at GSI. These low to moderate energy couplings are not well understood theoretically, and currently must be determined from experiment. In this paper we note that the two independent Dirac () and Pauli () couplings of the and can be constrained by the angular distribution of on resonance. A comparison of our theoretical results to recent unpolarized data allows estimates of the couplings; in the better determined case the data is inconsistent with a pure Dirac () coupling, and can be explained by the presence of a term. This Pauli coupling may significantly affect the cross section of the PANDA process near threshold. There is a phase ambiguity that makes it impossible to uniquely determine the magnitudes and relative phase of the Dirac and Pauli couplings from the unpolarized angular distributions alone; we show in detail how this can be resolved through a study of the polarized reactions.- 6 March 2008
- Published by American Physical Society (APS) in Physical Review D
- Vol. 77 (5) , 056001
Evidence for aPauli strong coupling?The couplings of charmonia and charmonium hybrids (generically ) to are of great interest in view of future plans to study these states using an antiproton storage ring at GSI. These low to moderate energy couplings are not well understood theoretically, and currently must be determined from experiment. In this paper we note that the two independent Dirac () and Pauli () couplings of the and can be constrained by the angular distribution of on resonance. A comparison of our theoretical results to recent unpolarized data allows estimates of the couplings; in the better determined case the data is inconsistent with a pure Dirac () coupling, and can be explained by the presence of a term. This Pauli coupling may significantly affect the cross section of the PANDA process near threshold. There is a phase ambiguity that makes it impossible to uniquely determine the magnitudes and relative phase of the Dirac and Pauli couplings from the unpolarized angular distributions alone; we show in detail how this can be resolved through a study of the polarized reactions.- Open Access
Evidence for a J/psi-ppbar Pauli Strong Coupling ?
The couplings of charmonia and charmonium hybrids (generically Psi) to ppbar are of great interest in view of future plans to study these states using an antiproton storage ring at GSI. These low to moderate energy Psi-ppbar couplings are not well understood theoretically, and currently must be determined from experiment. In this letter we note that the two independent Dirac (gamma_mu) and Pauli (sigma_munu) ppbar couplings of the J/psi and psi' can be constrained by the angular distribution of e+e- -> (J/psi, psi') -> ppbar on resonance. A comparison of our theoretical results to recent unpolarized data allows estimates of the ppbar couplings; in the better determined J/psi case the data is inconsistent with a pure Dirac (gamma_mu) coupling, and can be explained by the presence of a sigma_munu term. This Pauli coupling may significantly affect the cross section of the PANDA process p pbar -> pi0 J/psi near threshold. There is a phase ambiguity that makes it impossible to uniquely determine the magnitudes and relative phase of the Dirac and Pauli couplings from the unpolarized angular distributions alone; we show in detail how this can be resolved through a study of the polarized reactions.
Open AccessEvidence for a J/psi-ppbar Pauli Strong Coupling ?
The couplings of charmonia and charmonium hybrids (generically Psi) to ppbar are of great interest in view of future plans to study these states using an antiproton storage ring at GSI. These low to moderate energy Psi-ppbar couplings are not well understood theoretically, and currently must be determined from experiment. In this letter we note that the two independent Dirac (gamma_mu) and Pauli (sigma_munu) ppbar couplings of the J/psi and psi' can be constrained by the angular distribution of e+e- -> (J/psi, psi') -> ppbar on resonance. A comparison of our theoretical results to recent unpolarized data allows estimates of the ppbar couplings; in the better determined J/psi case the data is inconsistent with a pure Dirac (gamma_mu) coupling, and can be explained by the presence of a sigma_munu term. This Pauli coupling may significantly affect the cross section of the PANDA process p pbar -> pi0 J/psi near threshold. There is a phase ambiguity that makes it impossible to uniquely determine the magnitudes and relative phase of the Dirac and Pauli couplings from the unpolarized angular distributions alone; we show in detail how this can be resolved through a study of the polarized reactions.
- Open Access
- 15 March 2007
- Published by American Physical Society (APS) in Physical Review D
- Vol. 75 (5) , 054018
Associated charmonium production in low energypp¯annihilation
The QCD mechanisms underlying the exclusive strong decays and hadronic production amplitudes of charmonium remain poorly understood, despite decades of study and an increasingly detailed body of experimental information. One set of hadronic channels of special interest are those that include baryon-antibaryon states. These are being investigated experimentally at BES and CLEO-c in terms of their baryon resonance content, and are also of interest for the future PANDA experiment, in which charmonium and charmonium hybrids will be produced in annihilation in association with light mesons. In this paper we develop a simple initial-state light meson emission model of the near-threshold associated charmonium production processes , and evaluate the differential and total cross sections for these reactions in this model. (Here we consider the states , , , and .) The predicted near-threshold cross section for is found to be numerically similar to two previous theoretical estimates, and is roughly comparable to the (sparse) existing data for this process. The theoretical charmonium angular distributions predicted by this model are far from isotropic, which may be of interest for PANDA detector design studies.- 15 March 2007
- Published by American Physical Society (APS) in Physical Review D
- Vol. 75 (5) , 054018
Open AccessAssociated charmonium production in low energypp¯annihilation
The QCD mechanisms underlying the exclusive strong decays and hadronic production amplitudes of charmonium remain poorly understood, despite decades of study and an increasingly detailed body of experimental information. One set of hadronic channels of special interest are those that include baryon-antibaryon states. These are being investigated experimentally at BES and CLEO-c in terms of their baryon resonance content, and are also of interest for the future PANDA experiment, in which charmonium and charmonium hybrids will be produced in annihilation in association with light mesons. In this paper we develop a simple initial-state light meson emission model of the near-threshold associated charmonium production processes , and evaluate the differential and total cross sections for these reactions in this model. (Here we consider the states , , , and .) The predicted near-threshold cross section for is found to be numerically similar to two previous theoretical estimates, and is roughly comparable to the (sparse) existing data for this process. The theoretical charmonium angular distributions predicted by this model are far from isotropic, which may be of interest for PANDA detector design studies. - Open Access
Associated Charmonium Production in p-pbar Annihilation
In this paper we summarize our recent results for low energy associated charmonium production cross sections, using 1) crossing symmetry, and 2) an explicit hadronic model. These predictions are of relevance to the planned charmonium and charmonium hybrid production experiment PANDA at GSI.
Open AccessAssociated Charmonium Production in p-pbar Annihilation
In this paper we summarize our recent results for low energy associated charmonium production cross sections, using 1) crossing symmetry, and 2) an explicit hadronic model. These predictions are of relevance to the planned charmonium and charmonium hybrid production experiment PANDA at GSI.
- Open Access
Associated Charmonium Production in Low Energy p-pbar Annihilation
The QCD mechanisms underlying the exclusive strong decays and hadronic production amplitudes of charmonium remain poorly understood, despite decades of study and an increasingly detaled body of experimental information. One set of hadronic channels of special interest are those that include baryon-antibaryon states. These are being investigated experimentally at BES and CLEO-c in terms of their baryon resonance content, and are also of interest for the future PANDA experiment, in which charmonium and charmonium hybrids will be produced in p-pbar annihilation in association with light mesons. In this paper we develop a simple initial-state light meson emission model of the near-threshold associated charmonium production processes p pbar -> pi0 ccbar, and evaluate the differential and total cross sections for these reactions in this model. (Here we consider the ccbar states eta_c, J/psi, psi', chi_0 and chi_1.) The predicted near-threshold cross section for p pbar -> pi0 J/psi is found to be numerically similar to two previous theoretical estimates, and is roughly comparable to the (sparse) existing data for this process. The theoretical charmonium angular distributions predicted by this model are far from isotropic, which may be of interest for PANDA detector design studies.
Open AccessAssociated Charmonium Production in Low Energy p-pbar Annihilation
The QCD mechanisms underlying the exclusive strong decays and hadronic production amplitudes of charmonium remain poorly understood, despite decades of study and an increasingly detaled body of experimental information. One set of hadronic channels of special interest are those that include baryon-antibaryon states. These are being investigated experimentally at BES and CLEO-c in terms of their baryon resonance content, and are also of interest for the future PANDA experiment, in which charmonium and charmonium hybrids will be produced in p-pbar annihilation in association with light mesons. In this paper we develop a simple initial-state light meson emission model of the near-threshold associated charmonium production processes p pbar -> pi0 ccbar, and evaluate the differential and total cross sections for these reactions in this model. (Here we consider the ccbar states eta_c, J/psi, psi', chi_0 and chi_1.) The predicted near-threshold cross section for p pbar -> pi0 J/psi is found to be numerically similar to two previous theoretical estimates, and is roughly comparable to the (sparse) existing data for this process. The theoretical charmonium angular distributions predicted by this model are far from isotropic, which may be of interest for PANDA detector design studies.