共查询到20条相似文献,搜索用时 275 毫秒
1.
本文提出一个证认宇宙线中新X粒子的分析原则:筛比较法。对目前全部已知乳胶室事例进行了判定。其中结果有D介子和∑c+重子的平均寿命和质量,τ(D&;#177;)=5.8×10-13秒,τ(D0)=2.0×10-13秒,τ(∑c+)(?)2.4×10-14秒。支持△I=1的选择规则。 相似文献
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基于北京谱仪收集的4.03GeV质心系能量下e+e-对撞数据,分析τ±τ±→e±+π±+nπ0+ν's(n=0,1,2)事例,给出分支比值Br(τ±→π±ντ)=(11.64±0.49+0.76-0.73%,Br(τ±→π±π0ντ)=(24.00±1.34+1.36-1.30%,Br(τ±→π±2π0ντ)=(9.39±1.68+1.69-1.66%. 相似文献
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P. Pakhlov 《中国物理 C》2008,32(6):488-491
We present a search for new charmonium like states in e+e- annihilation using the initial-state radiation and the process e+e-J/ψD(*)D(*). The analyses are based on a huge data sample recorded near the Υ(4s) resonance with the Belle detector at the KEKB e+e- asymmetric-energy collider. 相似文献
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M. Ablikim et al 《中国物理 C》2012,36(11)
Based on 58 million J/ψ events collected by the BESⅡ detector at the BEPC, J/ψ→ΛΛ π+π- is observed for the first time. The branching fraction is measured to be Br(J/ψ→ΛΛ π+π-)=(4.30±0.13±0.99)×10-3, excluding the decays to intermediate states, namely J/ψ→Ξ-Ξ+, J/ψ→Σ(1385)-Σ(1385)+, and J/ψ→Σ(1385)+Σ(1385)-. The branching fractions for these intermediate resonance channels are measured to be:Br(J/ψ→Ξ-Ξ+)=(0.90±0.03±0.18)×10-3, Br(J/ψ→Σ(1385)-Σ(1385)+)=(1.23±0.07±0.30)×10-3,and Br(J/ψ→Σ(1385)+Σ(1385)-)=(1.50±0.08±0.38)×10-3, respectively. The angular distribution is of the form dN/d(cosθ)α(1+αcos2θ) with α=(0.35±0.29±0.06) for J/ψ→Ξ-Ξ+, α=(-0.54±0.22±0.10) for J/ψ→Σ(1385)-Σ(1385)+, and α=(-0.35±0.29±0.06) for J/ψ→Σ(1385)+Σ(1385)-. 相似文献
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分析北京谱仪(BES)收集的4.03GeV质心系能量下e+e-对撞数据,选出e+e-→τ±τ+→e±X+v′S事例,X±可以为μ±,τ±,ρ±,拟合τ→ev′s中电子的能谱,得到τ→ev′s中Michel参数为ρτ→e=0.705,此结果与标准模型的预言相符合. 相似文献
6.
提出了一种亚层子模型. 层子和轻子是由rishon T和V组成的. T和V是SUH(3)×SUC(3)×SUG(2)×U(1)群的多重态. 由这些多重态可以自然地得到三代层子和轻子. 在此模型中质子衰变为μ-e+e+或e-μ+μ+. 相似文献
7.
利用北京谱仪在北京正负电子对撞机上采集的350万(2S)事例,通过ψ(2S)→γπ+π-和γK+K-反应道测量了χc0的总宽度.由Monte Carlo模拟给出的质量分辨函数,利用拟合χc2谱形得到的质量分辨作标定后,用于χc0宽度的拟合,得到χc0的宽度为(15.0)MeV.同时定出了χcJ(J=0,2)到π+π-+K-的衰变分支比.结果为B(χc0→π+π-)=(4.27±0.23±0.60)×10-3,B(χc0→K+K-)=(3.44±0.21±0.47)×10-3,B(χc2→π+π-)=(1.52±0.17±0.29)×10-3 和 B(χc2→K+K-)=(5.2±1.1±1.8)×10-4,其中第一项误差为统计误差,第二项为系统误差. 相似文献
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We report results of experiments performed with the KEDR detector at the VEPP-4M e+e- collider. They include precise measurement of the D0 and D± meson masses, determination of the ψ(3770) resonance parameters, and a search for narrow resonances in e+e- annihilation at center-of-mass energies between 1.85 and 3.1 GeV. 相似文献
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In this paper we study the semileptonic decays of Bc-→(ηc,J/Ψ)l-vl. We first evaluate the Bc→(ηc,J/Ψ) transition form factors F0(q2), F+(q2), V(q2) and A0,1,2(q2) by employing the pQCD factorization approach, and then we calculate the branching ratios for all considered semileptonic decays. Based on the numerical results and the phenomenological analysis, we find that: (a) the pQCD predictions for the values of the Bc→ηc and Bc→J/Ψ transition form factors agree well with those obtained by using other methods; (b) the pQCD predictions for the branching ratios of the considered decays are Br(Bc-→ηc e-ve(μ-vμ)=(4.41-1.09+1.22)×10-3, Br(Bc-→ηcτ-vτ) =(1.37-0.34+0.37)×10-3, Br(Bc-→J/Ψ e-ve(μ-vμ)) =(10.03-1.18+1.33)×10-3, and Br(Bc-→J/Ψτ-vτ) =(2.92-0.34+0.40)×10-3; and (c) we also define and calculate two ratios of the branching ratios Rηc and RJ/Ψ, which will be tested by LHCb and the forthcoming Super-B experiments. 相似文献
13.
M. Ablikim et al 《中国物理 C》2012,36(11)
The decay ψ(2S)→Ω-Ω+ is analyzed using 14×106 ψ(2S) events recorded by the Beijing Spectrometer Ⅱ (BESⅡ) at the Beijing Electron Positron Collider (BEPC). Based upon events with no missing charged tracks and a satisfactory four-constraint kinematic t, we determine the upper limit for the branching fraction of ψ(2S)→Ω-Ω+ to be 1.5×104 at a 90% confidence level. By including events with one missing charged track, we are able to report the first evidence of an Ω+ signal with a statistical signi cance of 3.1|σ. The branching fraction of ψ(2S)Ω+ is determined to be (4.80±1.56(stat)±1.30(sys))105. 相似文献
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LI Jiang LIAO Xiao-Tao YANG Ming YANG Hong-Xun XU Min ZHANG Bing-Xin SHEN Xiao-Yan YANG Yong-Xu 《中国物理快报》2010,27(4)
The decays of J/φ→μ+μ- and J/φ→ e+e- are studied by Monte-Carlo simulation, based on the Beijing Spectrometer (BES)Ⅲ offline software system. The methods of determination of the J/φ event number via J/φ→μ+μ- and J/φ→ e+e- are presented, respectively. These methods can be used to determine the J/φevent number for the coming BESⅢ J/φ data sample. 相似文献
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Using data samples collected at center-of-mass energies of √s=4.009, 4.230, 4.260, and 4.360 GeV with the BES0 detector operating at the BEPC/ collider, we perform a search for the process e+e-→γχc,j (J =0, 1, 2) and find evidence for e+e-→γχc1 and e+e-→γχc2 with statistical significances of 3.0σ and 3.4σ, respectively. The Born cross sections σB(e+e-→γχc,j), as well as their upper limits at the 90% con dence level (C.L.) are determined at each center-of-mass energy. 相似文献
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The cross sections for e+e-→π+π-J/ψ, π+π-ψ(2S), K+K-J/ψ, DD, D0D-+π++c.c., D*D+c.c., and D*D* are measured using data sample collected on or near the Υ(4S) resonance with the Belle detector at KEKB. A peak near 4.25GeV/c2, corresponding to the so called Y(4260), is observed in π+π-J/ψ final state. In addition, there is another cluster of events at around 4.05GeV/c2. Two resonant structures are observed in the π+π-ψ(2S) invariant mass distribution, one at 4361±9±9MeV/c2 with a width of 74±15±10MeV/c2, and another at 4664±11±5MeV/c2 with a width of 48±15± 3MeV/c2. The rich structures observed in all these final states indicate that our understanding of the vector charmonium states above the open charm threshold is still poor, let alone the other possible dynamics such as charmonium hybrids or final state re-scattering and so on. 相似文献
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本文建议轻子电磁自能通过((δm)/m)=(1/(2π))n-b 与量子数 n 联系起来,其中 b 为待定常数.并建议动量截断值 M 与引力常数 k 和精细结构常数α的联系为 M=(?).得到了带电轻子质量公式(?).利用 e-和μ-质量的实验值和α值作输入,给出计算值 k=(6.67231±0.00026)×10-8 cm3g-lsec-2和mτ=(1782.306±0.078)MeV,与观察值 k=(6.6720±0.0041)×10-8cm3 g-1sec-2和 mτ=(1782-4+3)MeV 很好符合.公式预言第四个带电轻子质量应为 m=(11725.47±0.51)MeV 可以在最近的实验中检验。本文还对所建议的质量公式和结果进行了讨论. 相似文献
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利用北京谱仪(BES)上取得的ψ(2S)数据,对ψ(2S)→π+π-J/ψ,J/ψ→1+1-和J/ψ→任意末态两个过程进行了细致的研究,得到J/ψ的轻子道衰变分支比为B(J/ψ→e+e-)=(5.90±0.07±0.16)%和B(J/ψ→μ+μ-)=(5.96±0.08±0.16)%,由此给出Be/Bμ的值为0.990±0.018±0.024.假定Be=Bμ,J/ψ的轻子道衰变分支比为B(J/ψ→1+1-)=(5.93±0.05±0.16)%.上述结果可用来估计强相互作用耦合常数αs和QCD减除参数∧. 相似文献
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本文描述了拟合Z0峰线形的整个过程;讨论了Z0能区e+e-→ff反应截面的各种辐射修正;给出了截面测量中系统误差的主要来源及其在拟合中的考虑;并以Z0的一个轻子衰变道τ+τ-(γ)为例,说明拟合Z0峰线形得到Z0质量、衰变总宽度及τ+τ-(γ)道衰变分宽度的方法.文中还对不同的理论计算程序作了简单的分析和比较. 相似文献