ηb decay into charmonium in association with c(c) pair

We calculate the inclusive decay rates of ηb into charmonium via double cc pairs for S- and P-wave states ηc, J/ψ and χcJ within the framework of non-relativistic QCD (NRQCD) factorization at leading order in αs. Besides calculating the contributions of the color-singlet channels ηb→c(c)[2S+1Sl(1)]+c(c), the effects of c(c) pair in the color-octet configurations are also considered. We find that ηb→c(c)[3S1(8)]+c(c) make a small contribution to Br(ηb→J/ψ(ηc)+c(c)). While in ther ηb→χcJ+c(c) case, the color octet contributions are significant, for they are of the same αs4vc5 order as the color-singlet processes. We predict Br(ηb → J/ψ(ηc)+c(c)) = 2.99(2.75) × 10-5 for S-vrave states J/ψ and ηc, and Br(ηb→χcJ +c(c))= (4.37,3.40,2.83)×10-5 (for J = 0,1,2) for P-wave states χcJ. In the end, we also find Br(ηb → c(c)c(c)) is almost saturated by ηb decay into charmonium in association with cc pair from the point of view of duality.     

η_b decay into charmonium in association with c pair

We calculate the inclusive decay rates of ηb into charmonium via double c pairs for S-and P-wave states ηc,J/ψ and χcJ within the framework of non-relativistic QCD(NRQCD) factorization at leading order in αs.Besides calculating the contributions of the color-singlet channels ηb→c[2S+1SL(1)]+c,the effects of c pair in the color-octet configurations are also considered.We find that ηb→c[3S1(8)]+c make a small contribution to Br(ηb→J/ψ(ηc)+c).While in the ηb→χcJ+c case,the color octet contributions are significant,for they are of the same αs4vc5 order as the color-singlet processes.We predict Br(ηb→J/ψ(ηc)+c)=2.99(2.75)×10-5 for S-wave states J/ψ and ηc,and Br(ηb→χcJ+c)=(4.37,3.40,2.83)×10-5(for J =0,1,2) for P-wave states χcJ.In the end,we also find Br(ηb→ cc) is almost saturated by ηb decay into charmonium in association with c pair from the point of view of duality.     

关于ηc粒子及其电磁衰变

本文在势模型的框架内估算了ηc粒子的质量、宽度及几种主要电磁衰变道的分支比.指出禁戒型磁跃迁ηc→J/ψγ的相对论修正结果比简单的非相对论估算有可能大一个量级.讨论了北京正负电子对撞机(BEPC)对级联电磁辐射过程ψ′(3686)→γηc→γγ¹P₁,γγJ/ψ,3γ进行测量的可能性.     

J/ψ→Σ~0 “非汉字符号”~0 衰变研究(英文)

利用北京正负电子对撞机 (BEPC)上的北京谱仪 (BES)收集的 7 8× 1 0 6 个J ψ事例 ,研究了J ψ→Σ0 Σ0 衰变 .其衰变分支比为BR(J ψ→Σ0 Σ0 ) =( 0 97±0 0 4± 0 2 4 )× 1 0 - 3,角分布具有 dNdcosθ=N0 ( 1 +αcos2 θ)的形式 ,α值等于 -0 2 1± 0 2 7± 0 1 3 .     

η、η′和ι的夸克和胶子内容、双光子衰变和J/ψ辐射衰变产生

本文引进q_iq_i→q_jq_j以及q_iq_i→(gg)湮没项^[1],并考虑了对湮没项的SU(3)破坏效应^[2],讨论了η、η′和ι的混合,得到了它们的有声有色和胶子内容.与此同时,引入EPCAC(扩充的部分守恒赝矢流)假设^[3],考察了η、η′和ι的双光子衰变.本文还计算了衰变宽度比R₁=Γ(J/ψ→γη′)/Γ(J/ψ→γη)以及R₂=Γ(J/ψ→γη′)/Γ(J/ψ→γι),指出了实验结果对纯胶子球质量值的限制.     

Measurement of J/ψ→ηcγ at KEDR

We present a study of the inclusive photon spectra from 5.9 million J/ψ decays collected with the KEDR detector at the VEPP-4M e＋e collider. We measure the branching fraction of radiative decay J/ψ→ηcγ, ηc width and mass. Our preliminary results are： M（ηc） = 2979.4± 1.5 ± 1.9 MeV/c^2, Г（ηc） = 27.8±5.1 ±3.3 MeV, B（Jψ→ηcγ） = （2.34±0.15±0.40）%.     

Partial wave analysis of ψ' →γχ_(c0) →γpK-Λ used for searching for baryon resonance

Abundant ψ' events have been collected at the Beijing Electron Positron Collider-Ⅱ (BEPCⅡ) that could undoubtedly provide us with a great opportunity to study the more attractive charmonium decays. As has been noticed before, in the process of J/ψ' decaying to the baryonic final states, pK-Λ, the evident Λ* and N* bands have been observed. Similarly, by using the product of χcJ from ψ' radiative decay, we may confirm this or find some extra new resonances. χc0's data samples will be more than χc1,2, taking into account the larger branching ratio of ψ' →γχc0. Here, we provide explicit partial wave analysis formulae for the very interesting channel ψ' →γχc0 →γpK-Λ.     

ηb decay into charmonium in association with cc pair

We calculate the inclusive decay rates of ηb into charmonium via double c~ pairs for S- and P-wave states ηc, J/ψ and XcJ within the framework of non-relativistic QCD （NRQCD） factorization at leading order in αs. Besides calculating the contributions of the color-singlet channels ηb → cc[2s＋1SL^（1）]＋cc, the effects of cc pair in the color-octet configurations are also considered. We find that ηb → cc[3S1^（8）] ＋cc make a small contribution to Br（ηb →J/ψ（ηc）＋cc）. While in the ηb →XcJ ＋cc case, the color octet contributions are significant, for they are of the same a 5 order as the color-singlet processes. We predict Br（ηb →J/ψ（ηc）＋cc） = 2.99（2.75） × 10^-5 Vc for S-wave states J/ψ and ηc, and Br（ηb → XcJ ＋cc） = （4.37, 3.40, 2.83） × 10^-5 （for J = 0,1, 2） for P-wave states XcJ. In the end, we also find Br（ηb → cccc） is almost saturated by ηb decay into charmonium in association with cc pair from the point of view of duality.     

赝标介子的胶子球分量与它们在J/ψ辐射衰变过程中的产生

本文用微扰论QCD计算了赝标胶子球在J/ψ辐射衰变过程中产生的几率. 指出由于ι(1440)与η、η′的混合, 使η、η′有一个胶子球分量, 这些分量在它们的J/ψ辐射衰变产生中占主导地位. 由此得到的比例Γ(J/ψ→γη′)/Γ(J/ψ→γη)比以前一些理论模型的结果要大, 并且是与实验符合的.     

Charmonium results from BES

Using ～14×106ψ(2S) and ～58×106J/ψ data collected at BESⅡ/BEPC,the branching fraction of ψ(2S) →Ω+Ωˉ+ is measured with about 5σ statistical significance.The Λ electric dipole and Λ decay parameter are studied using the decay J/ψ→ΛΛ→ ppˉπ+π-.Using(106±3)×106 ψ(2S) decays collected at BESⅢ/BEPCⅡ,we have obtained some interesting physics results.The branching fractions of χcJ →π0π0,ηη are measured with precision improved.The mass and width of hc(11P1) state,together with the branching fractions of Br(ψ(2S) →π0hc) and Br(hc →γηc) are the first measurements.Surprisingly,the decays of χc1 →φφ,ωω,and ωφ are firstly observed in BESⅢ data.     

Partial wave analysis of ψ＇ →γχc0→γpK-Λ used for searching for baryon resonance

Abundant ψ＇ events have been collected at the Beijing Electron Positron Collider-Ⅱ （BEPCⅡ） that could undoubtedly provide us with a great opportunity to study the more attractive charmonium decays. As has been noticed before, in the process of J/ψ＇ decaying to the baryonic final states, pK-Λ, the evident Λ＊ and N＊ bands have been observed. Similarly, by using the product of χcJ from ψ＇ radiative decay, we may confirm this or find some extra new resonances. χc0＇s data samples will be more than χc1,2, taking into account the larger branching ratio of ψ＇ →γχc0. Here, we provide explicit partial wave analysis formulae for the very interesting channel ψ＇ →γχc0 →γpK-Λ.     

J/ψ→f_JФ→ππK~+K~- 反应的各种一维角分布是否足以鉴别f_0和f_2?(英文)

基于螺旋度分波分析公式 ,我们探讨在J ψ→fJ(θ1,1)、fJ→ππ(θ2 ,2 )、→K+ K-(θ3 ,3 )级联衰变过程中是否可以通过各种一维角分布投影鉴别出f0 和f2 共振态 .结果表明 ,f0 和f2 可以同时给出完全相同的 (θ1,1,θ2 ,2 )一维投影 ,但不能同时给出完全相同的 (θ1,1,θ2 ,2 ,3 )一维投影 .因此 ,要想保证从角分布的一维投影鉴别出f0 和f2 ,必须同时考虑所有三个衰变顶角的角分布信息 .     

J/ψ→fJФ→ππK＋K－反应的各种一维角分布是否足以鉴别f0和f2?

基于螺旋度分波分析公式,我们探讨在J ψ→fJ(θ1,1)、fJ→ππ(θ2 ,2 )、→K+ K-(θ3 ,3 )级联衰变过程中是否可以通过各种一维角分布投影鉴别出f0 和f2 共振态.结果表明,f0 和f2 可以同时给出完全相同的(θ1,1,θ2 ,2 )一维投影,但不能同时给出完全相同的(θ1,1,θ2 ,2 ,3 )一维投影.因此,要想保证从角分布的一维投影鉴别出f0 和f2 ,必须同时考虑所有三个衰变顶角的角分布信息.     

Search for ψ(4S) → ηJ/ψ in B~±→ ηJ/ψK~± and e~+e~-→ ηJ/ψ processes

We search for the ψ(4S) state in the B~±→ηJ/ψK~± and e~+e~-→ηJ/ψ processes based on the Belle measurements with the assumed mass M =(4230±8) MeV/c~2 and width Γ =(38±12) MeV. No significant signal is observed in the ηJ/ψ mass spectra. The 90% confidence level upper limit on the product branching fraction B(B~±→ψ(4S)K~±)B(ψ(4S)→ηJ/ψ) 6.8×10~(-6) is obtained in the B~±→ηJ/ψK~± decays. By assuming the partial width of ψ(4S)→e~+e~-to be 0.63 ke V, a branching fraction limitB(ψ(4S)→ηJ/ψ) 1.3% is obtained at the 90%confidence level in e~+e~-→ηJ/ψ, which is consistent with the theoretical prediction.     

在BEPCⅡ/BESⅢ上寻找胶子球的Monte Carlo研究

在即将建造的BEPCⅡ BESⅢ上利用MonteCarlo模拟研究了J ψ→γX→γηη′(η′→γρ0 ,ρ0 →π+ π-,η→γγ)过程.研究显示BESⅢ的良好性能和大统计量的J ψ事例样本为寻找胶子球态的一些候选者并确认其存在提供了可能.基于所研究的衰变道,为BESⅢ电磁量能器晶体BGO和CsI的选择及磁场强度的选择提供了数据.     

J/ψ→π~03(π~+π~-)分支比的测定

用BESⅠ的 7.8× 1 0 6 J/ ψ数据更为精确地测定了J/ ψ→π0 3 (π+π- )和J/ ψ→ω2 (π+π- )的分支比 (Br(J/ ψ→π0 3 (π+π- ) ) =( 2 .52± 0 .0 6± 0 .4 3 ) % ,Br(J/ ψ→ω2 (π+π- ) ) =( 1 .3 1± 0 .0 9± 0 .2 1 ) % .同时对 4π不变质量谱和ωππ不变质量谱进行研究分析 ,试图观察是否存在有兴趣的信号 .     

关于πρ(1200MeV/c~2)共振态和SU_3群的27维表示

不久前,由实验发现,在质量m=1200MeV/c~2附近存在一个π~+ρ~0共振态A,其宽度Γ=350MeV/c~2。后来,更细致的实验指出,存在两个π~+ρ~0共振态,一个是A_1(1080MeV/c~2),另一个是A_2(1320MeV/c~2);二者的宽度分别为Γ_1=80±10MeV/c~2和Γ_2=100±10MeV/c~2。本文只考察A_1的分类问题。 由于A_1的宽度较大,而A_1→πρ的衰变动量不太大,因此,A_1→πρ衰变较大的可能是通过S波、P波或D波。这样,A_1的量子数(同位旋T、自旋J、宇称P和G宇称G)只可能是 当S波衰变时,     

J/Ψ衰变的Roper共振态结构的研究

通过J/Ψ→p, p*, N**衰变,研究了Roper共振态的混杂态结构对衰变角分布和分支比的影响. 计算结果表明,如果Roper共振态为纯混杂态,那么J/Ψ→p*, N**的角分布几乎相等, 而J/Ψ衰变到混杂态的衰变宽度还不到J/Ψ→p 的1%, 给出了Γ(J/Ψ→ N* )/Γ(J/Ψ→p)和Γ(J/Ψ→ N**)/Γ(J/Ψ→ p)随混合参数的变化关系, 并讨论了在J/Ψ衰变中研究Roper混杂态结构的可能性.The structure of Roper resonance is studied as hybrid states through decays J/Ψ→p*, N** by calculating the angular distributions and decay widths. The results show that the angular distribution parameters for decays J/Ψ→p*, N** are almost equal if the Roper is identified as a pure hybrid state, while their decay width are less the 1% of that for the decay J/Ψ→p, and the variance of the ratio Γ(J/Ψ→N*p)/Γ(J/Ψ→p) and Γ(J/Ψ→N**)/ Γ(J/Ψ→p) with the mixing parameter are presented,and also the scheme to identify the Roper structure in J/Ψ decays is discussed.     

J/ψ→Nπ衰变中的核子极点贡献

采用πN作用的赝标 (PS)耦合和赝矢 (PV)耦合两种形式 ,计算了J/ ψ→NNπ衰变中核子极点图的贡献 ,并加入各种强子顶角形状因子 ,考察它们的离壳效应。     

On ηc line shape in charmonium transitions

The line shapes to observe ηc in charmonium transitions, i.e., ψ（2S）, J/ψ→γηc, are investigated. The ηc line shapes in exclusive decays or by observing the inclusive photon spectrum are given. The sensitivities to measure the ηc resonance parameters are also evaluated. With more than two thousand ηc events observed, the precision of the ηc decay width measurement will be improved by better than 3%. However, the uncertainties associated with the ηc modified line shapes will dominate the systematic errors and this will prohibit precision mass and width measurements.