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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
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本文提出了一个对称性破缺前不仅左、右对称, 而且中微子(或反中微子)与荷电轻子、反轻子的弱作用也相同的SU(3)×U(1)模型. 这一模型无三角反常; 导出了sin2θw≤1/4; 在低能范围内与标准模型一致. 我们反轻子数推广为轻子荷. 证明了只有轻子荷才是严格守恒的, 各代轻子数分别守恒只能近似成立. 夸克不仅带有重子数、电荷, 而且也带有轻子荷. 本模型预言有μR→eR+νeL+νμR, e-+e-→μ-+μ-等现象. 相似文献
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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
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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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本文应用复合粒子量子场论的微扰展开式和相对论性的(π&;#177;μ?)、(K&;#177;μ?)的B.S.波函数,计算了在原子核屏蔽库仑场中高能(π&;#177;μ?)、(K&;#177;μ?)原子的裂解能谱和截面。在极端相对论近似下,对大多数原子核,它们的裂解截面分别约为10-18cm2和10-17cm2。利用同样的波函数,还计算了(π&;#177;μ?)→π0+vμ(vμ),(K&;#177;μ?)→K0+vμ(vμ),以及(π&;#177;μ?)→μ++μ-+vμ(vμ),(K&;#177;μ?)→μ++μ-+vμ(vμ)的衰变几率。 相似文献
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本文在光锥代数的基础上,用层子模型中核子的波函数和计算方法,由vW2P的实验曲线定出参数,并计算了 vG1、v2G2的值,得到了具有一定自旋取向的价层子的分布函数 h(?)(x).其中波函数中的时空函数取类谐振子的形式.文中对具有 SU(6)对称和不具有 SU(6)对称的两种旋量结构进行了讨论.计算得到的 A1P×vW2P 的理论值与实验相符合,对 SU(6)对称情况得到6 integral from 0 to 1{vG1P-vG1n}dx=-1.16,实验支持 SU(6)对称的波函数. 相似文献
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把满足约束Pi2—mi2—U(x2)=0(i=1,2)的二质点组的相对论力学应用于介子的SU(4)层子模型。在U(x2)为无限深球方势阱情况下,导出介子的质量谱。得到一组较精确的线性的质量关系。对于O-介子,代替η’—ηs混合,提出了η’—ηc混合的猜测。指出瑞奇轨迹对J—M2直线有系统地偏离,得到新的轨迹为M2对ξnl2的直线,其中ξneπ为球贝塞尔函数的零点,l为轨道角动量,新轨迹与实验数据符合较好。 相似文献
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本文提出了三个SO(14)规范群大统一模型。它们能容纳四代通常的费米子。模型A预言了第一代和第二代费米子具有V-A型荷电弱流,而第三代和第四代费米子具有y+A型荷电弱流。在模型B中,我们得到和实验接近的Weinberg值:sin2θw=0.225荷电中间玻色子和中性中间玻色子的质量都将比Weinberg-Salam模型中的大1.7倍。模型B预言了另一个质量为100GeV数量级的中性中间玻色子,它与第一、二代费米子的耦合类似于重光子的耦合。模型B的τ—νr耦合和模型C的四代轻费米子的荷电弱流都是V—A型。本文中所有的模型都能容纳质量关系:mα·mμ~md·mτ,mμ~3ms,mr~mb,并给出第一Cabibbo角sinθ1=((md)/(ms))1/2。 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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本文分析了C2群无穷小算子的对易关系,发现C2群的10个无穷小算子可以表示为两组相互对易的角动量算符v1,v0,v-1;τ1,τ0,τ-1,一组秩为(1/2)(1/2)的双不可约张量算符U±1/2±1/2。利用C2群无穷小算子的这个性质,我们求出了C2群的所有有限维不可约表示,C2群的约化系数等等。本文给出了在C2群的不可约表示(λμ)中无穷小算子对应的矩阵,从而完全确定了不可约表示(λμ)及其表示空间Rλμ。我们还给出了C2群约化系数标量因子所满足的方程组,对称关系,并给出了(λμ)(?)(10),(λμ)×(01),(λμ)(?)(20)约化系数标量因子的代数表达式。在本文最后,我们定义了C2群的不可约张量算符并证明了相应的Wigner-Eckart定理。 相似文献
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Based on the nonrelativistic QCD factorization approach, O(αsv2) corrections to J/ψ plus ηc production in m e+e- annihilation at √s=10.6 ≥v are calculated in this work. The numerical results show that the correction at αsv2 order is only about a few percent of the total theoretical result. This indicates that the perturbative expansions become convergent and that a higher order correction will be smaller. The uncertainties from the long-distance matrix elements, renormalization scale and the measurement in the experiment are also discussed. Our result is in agreement with the previous result by Jia. 相似文献
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We investigate the condition that the neutrino energies Ev can be considered to be small enough to be neglected in the energy momentum conservation equation in the reactions d+ve → u+e- and u+e- → d+ve. It can be simply expressed as Ev < 4αcμe/π, where αc is the strong coupling constant and μe is the electron chemical potential. Then for Ev < 4αcμe/π, we generalize the mean free path for nondegenerate neutrinos given by Iwamoto and obtain a formula that is valid for both nondegenerate and degenerate neutrinos. We also model the mean free path for both nondegenerate and degenerate neutrinos with energies Ev < 4αcμe/π. 相似文献
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利用环形固体径迹探测器,通过238U(α,2n)反应,测量了240mPu的半衰期和激发函数.定出半衰期T1/2=3.5±0.5ns.它与基态的能量差Ei=3.2±0.5MeV. 相似文献
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本文在SU(3)极限为转动限的假定下,讨论了N—1个(sd)玻色子和1个(pf)玻色子组成的系统的转动;用群论方法给出负宇称转动谱;导出了v0带(Kπ=0-)到基带E3跃迁约化矩阵元的解析表达式;用(sd)-(sd)相互作用和(sd)-(pf)相互作用强度的不同,定性地解释了正负宇称能带参数的不同。 相似文献
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Depth Dependence of Tetragonal Distortion of a ZnO/Mg0.1Zn0.9O/ZnO Heterostructure Studied by Rutherford Backscattering/Channeling 下载免费PDF全文
Rutherford backscattering and channeling are used to characterize the structure of a ZnO/Mg0.1Zn0.9O/ZnO heterostructure grown on a sapphire (0001) substrate by rf plasma-assisted molecular beam epitaxy. The results show that the Mg0.1Zn0.9O layer has the same hexagonal wurtzite structure as the underlying ZnO layer, and the heterostructure has a good crystalline quality with χmin =5%, which is the ratio of the backscattering yields of aligned and random spectra in the near-surface region. Using the channeling angular scan around an off-normal <12-13> axis in the {101-0} plane of both ZnO and MgZnO layer, the tetragonal distortion eT, which is caused by the elastic strain in the epilayer, is determined. The depth dependence of eT is obtained by using this technique. It can clearly be seen that the elastic strain rapidly decreases with the increase in thickness of the ZnO film in the early growth stage and becomes slightly larger in the region of the Mg0.1Zn0.9O layer. 相似文献