Lepton scattering is an established ideal tool for studying inner structure of small particles such as nucleons as well as nuclei. As a future high energy nuclear physics project, an Electron-ion collider in China (EicC) has been proposed. It will be constructed based on an upgraded heavy-ion accelerator, High Intensity heavy-ion Accelerator Facility (HIAF) which is currently under construction, together with a new electron ring. The proposed collider will provide highly polarized electrons (with a polarization of ∼80%) and protons (with a polarization of ∼70%) with variable center of mass energies from 15 to 20 GeV and the luminosity of (2–3) × 1033 cm−2 · s−1. Polarized deuterons and Helium-3, as well as unpolarized ion beams from Carbon to Uranium, will be also available at the EicC.The main foci of the EicC will be precision measurements of the structure of the nucleon in the sea quark region, including 3D tomography of nucleon; the partonic structure of nuclei and the parton interaction with the nuclear environment; the exotic states, especially those with heavy flavor quark contents. In addition, issues fundamental to understanding the origin of mass could be addressed by measurements of heavy quarkonia near-threshold production at the EicC. In order to achieve the above-mentioned physics goals, a hermetical detector system will be constructed with cutting-edge technologies.This document is the result of collective contributions and valuable inputs from experts across the globe. The EicC physics program complements the ongoing scientific programs at the Jefferson Laboratory and the future EIC project in the United States. The success of this project will also advance both nuclear and particle physics as well as accelerator and detector technology in China.
Abstract:Results for the antinucleon-nucleon (N N ) interaction obtained at next-to-nextto-next-to-leading order in chiral effective field theory (EFT) are reported. A new local regularization scheme is used for the pion-exchange contributions that has been recently suggested and applied in a pertinent study of the N N force within chiral EFT. Furthermore, an alternative strategy for estimating the uncertainty is utilized that no longer depends on a variation of the cutoffs. The low-energy constants associated with the arising contact terms are fixed by a fit to the phase shifts and inelasticities provided by a phase-shift analysis ofpp scattering data. An excellent description of theN N amplitudes is achieved at the highest order considered. Moreover, because of the quantitative reproduction of partial waves up to J = 3, there is also a nice agreement on the level ofpp observables. Specifically, total and integrated elastic and charge-exchange cross sections agree well with the results from the partial-wave analysis up to laboratory energies of 300 MeV, while differential cross sections and analyzing powers are described quantitatively up to 200-250 MeV. The low-energy structure of theN N amplitudes is also considered and compared to data from antiprotonic hydrogen.
In this paper we perform an amplitude analysis of essentially all published pion and kaon pair production data from two-photon collisions below 1.5 GeV. This includes all the high statistics results from Belle, as well as older data from Mark II at SLAC, CELLO at DESY, and Crystal Ball at SLAC. The purpose of this analysis is to provide as close to a model-independent determination of the γγ to meson pair amplitudes as possible. Having data with limited angular coverage, typically j cos θj < 0.6-0.8, and no polarization information for reactions in which spin is an essential complication, the determination of the underlying amplitudes might appear an intractable problem. However, imposing the basic constraints required by analyticity, unitarity, and crossing symmetry makes up for the experimentally missing information. Above 1.5 GeV multimeson production channels become important, and we have too little information to resolve the amplitudes. Nevertheless, below 1.5 GeV the two-photon production of hadron pairs serves as a paradigm for the application of S-matrix techniques. Final state interactions among the meson pairs are critical to this analysis. To fix these, we include the latest ππ → ππ, KK scattering amplitudes given by dispersive analyses, supplemented in the KK threshold region by the recent precision Dalitz plot analysis from BABAR. With these hadronic amplitudes built into unitarity, we can constrain the overall description of γγ → ππ and KK data sets, both integrated and differential cross sections, including the high statistics charged and neutral pion, as well as K s K s , data from Belle. Since this analysis invokes coupled hadronic channels, having data on both ππ and KK reduces the solution space to essentially a single form in the region where these channels saturate unitarity. For the ππ channel, the separation of isospin-0 and -2 and helicity-0 and -2 components is complete. We present the partial wave amplitudes, show how well they fit all the available data, and give the two-photon couplings of scalar and tensor resonances that appear. These partial waves are important inputs into forthcoming dispersive calculations of hadronic light-by-light scattering. PHYSICAL REVIEW D 90, 036004 (2014) 036004-2 LING-YUN DAI AND M. R. PENNINGTON PHYSICAL REVIEW D 90, 036004 (2014) 036004-4 FIG. 8 (color online). Fit to the γγ → π þ π − differential cross section of CELLO experiment. Here, Cello1 is from Harjes [3] and Cello2 from Behrend et al. [4]. The numbers give the central energy in GeV of each angular distribution listed in order of the cross section at z ¼ 0, where z ¼ cos θ. COMPREHENSIVE AMPLITUDE ANALYSIS OF … PHYSICAL REVIEW D 90, 036004 (2014) 036004-15 FIG. 9 (color online). Fit to the γγ → π þ π − differential cross section of the Belle experiment [13]. The numbers give the central energy in GeV of each angular distribution listed in order of the cross section at z ¼ 0, where z ¼ cos θ. The data are normalized so that the integrated cross section is just a sum of the differential cross sect...
Pole analysis on unitarized SU (3) × SU (3) one loop χPT amplitudes (3) chiral perturbation theory. By fitting phase shift and inelasticity data, we determine pole positions in different channels (f 0 (980), a 0 (980),f 0 (600), K * 0 (800), K * (892), ρ(770)) and trace their N c trajectories. We stress that a couple channel Breit-Wigner resonance should exhibit two poles on different Riemann sheets that reach the same position on the real axis when N c = ∞. Poles are hence classified using this criteria and we conclude that K * (892) and ρ(770) are unambiguous Breit-Wigner resonances. For scalars the situation is much less clear. We find that f 0 (980) is a molecular state rather than a Breit-Wigner resonance, while a 0 (980), though behaves oddly when varying N c , does maintain a twin pole structure.
We study the property of X(4260) resonance by re-analyzing all experimental data available, especially the e + e − → J/ψ π + π − , ωχc0 cross section data. The final state interactions of the ππ, KK couple channel system are also taken into account. A sizable coupling between the X(4260) and ωχc0 is found. The inclusion of the ωχc0 data indicates a small value of Γ e + e − = 23.30 ± 3.55eV. * 0 molecule [16-18], non-resonant explanation [19,20], etc.. Besides, the tetraquark state explanation is also very intersting [21-26], especially when two resonances, Z c (3900) and Z c (4025), are recently found in J/ψπ and D ( * )D( * ) channels in e + e − annihilation near 4.26GeV by BESIII Collaboration [27], and confirmed by Belle [28] and CLEO [29] Collaborations. However the open charm channels such asDD * , DD * , D * D * are not found in the final states of X(4260) decays [30][31][32], making the property of X(4260) to be more mysterious.The present authors have also studied the X(4260) issue in the previous edition of the present paper (Preprint arXiv:1206.6911v2, herewith denoted as V1). Through a careful analysis to experimental data available, it is found that the X(4260) has a sizable coupling to ωχ c0 channel, but not to other (nearby) channels. Inspired by our result, a recent experimental analysis [33,34] shows that there is indeed a sizable ωχ c0 final state signal in e + e − collision at around 4.26GeV,
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.
customersupport@researchsolutions.com
10624 S. Eastern Ave., Ste. A-614
Henderson, NV 89052, USA
This site is protected by reCAPTCHA and the Google Privacy Policy and Terms of Service apply.
Copyright © 2024 scite LLC. All rights reserved.
Made with 💙 for researchers
Part of the Research Solutions Family.