在高能e+e－对撞机上探测top-Higgs的可能性

计算了top-Higgsh0t对过程e⁺e^－→tc νeνe,e⁺e^－→γ(Z)tc的贡献,并进一步讨论了在高能线性e⁺e^－对撞机(LC)上探测此粒子的可能性.结果表明:h0t对过程e⁺e^－→tc νeνe的贡献很大,通过此过程可在LC实验中探测top-Higgs;另外e⁺e^－→γtc也是探测h0t的有效过程.     

最小Higgs模型在ILC上可能的味改变物理迹象

在最小Higgs(LH)模型中, 由于引进了类矢量顶夸克T, 对弱作用流产生了新的影响. CKM矩阵从3×3变为4×3, 在树图下出现味改变中性流(FCNC). 本文研究了在国际高能直线对撞机(ILC)上能否通过e⁺e^－→tc+tc和e⁺e^－→WWν_eν_e→(tc+tc) ν_eν_e过程探测到LH模型所预言的FCNC信号.     

τ±→π±+nπ0+ντ(n=0,1,2)衰变分支比测量

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^±ν_τ)=(11.64±0.49^+0.76_－0.73%,Br(τ^±→π^±π⁰ν_τ)=(24.00±1.34^+1.36_－1.30%,Br(τ^±→π^±2π⁰ν_τ)=(9.39±1.68^+1.69_－1.66%.     

J/ψ强子衰变过程的角分布螺旋度形式

本文给出了e⁺e^－→J/ψ→V+X,V→P₁P₂和e⁺e^－→J/ψ→V+X,X→P₄P₅过程的角分布螺旋度形式.为e⁺e^－实验数据分析提供了理论公式.     

Kl3介子衰变

本文通过强作用K-π中间态,利用色散关系理论计算了Г(K_μ3⁺)/Г(K_α3⁺),Г(K₂⁰→πμ⁺ν)/Г(K₂⁰→πe⁺ν),{Г(K₂⁰→πe⁺ν)+Г(K₂⁰→πe^-ν)}/Г(K_α3⁺)分支比及K_μ3⁺衰变中的μ谱,当选择定则|ΔI|=1/2及ΔS=+ΔQ被破坏,并且I_z=1/2及I_z=3/2的振幅f^{3/2 1/2}(0)及f^{3/2 3/2}(0)不等时,上述分支比与实验能很好符合。在本文的理论中,形式因子不是常数。     

TC2理论在LC实验中的可能物理迹象

在高能e⁺e^－碰撞实验(LC)中，研究了顶色辅助的人工色(TC2)理论所预言的中性top介子 的产生. 结果表明，在LC实验中通过过程e⁺e^－→tc, e⁺e^－→γtc和e⁺e^－→Ztc可以探测到πt0的物理迹象.     

e+e－→W+W－→h's过程中的色重组

用色等效哈密顿研究了e⁺e^－→W⁺W^－→h＇s过程中部分子阶段的色重组几率,并与Gustafson和Sjostrand等人的结果作了分析比较,发现色重组几率不能被忽略,并指出研究色重组对发展强子化模型提出了新的要求.     

在LEPⅡ及NLC能量下e+e—→bb Z0 和 tt－Z0过程中Higgs粒子的观测效应

根据最小标准模型及双Higgs二重态的扩展标准模型理论,计算了LEPⅡ以及NLC能量下e⁺e^—→bb Z⁰ 和 tt－Z⁰的总截面和微分截面以探求Higgs粒子的观测效应.我们发现,只要Higgs粒子的质量M_H≤140GeV,对e⁺e^—→bb Z⁰的测量就能清楚地提供Higgs粒子的信息.然而对e⁺e^—→tt－Z⁰,不论Higgs粒子是轻或重,它的效应都被淹没在弱电过程的本底中,没有观测的可能.     

中性top-pion的产生和衰变

研究了顶色辅助的人工色(TC2?)理论预言的中性top-pion π0t的产生和衰变.结果表明:在高能正负电子对撞(LC)实验中,通过e⁺e^－→γπ0t和e⁺e^－→Z π0t过程可以产生大量的π0t粒子,通过e⁺e^－→γπ0t→γtc和e⁺e^－→π0tZ→tcZ过程可以探测中性top-pion π0t?的可能物理迹象.     

强耦合QED相的非拓扑孤子模型和正、负电子对凝聚

在强耦合QED相的非拓扑孤子模型中,讨论了电子动力学质量的生成机制,得到了产生正、负电子对凝聚的临界耦合常数g_crit和临界核电荷数Z_crit,定性地解释了反常e⁺e^－峰的性质.结果表明,正、负电子对凝聚在QED强耦合相中起着重要作用.     

Tree-Level Violation of the Equivalence Principle

Massive particles of spin 0 and 1 violate the equivalence principle (EP) at the tree level. On the other hand, if these particles are massless, they agree with the EP, which leads us to conjecture that from a semiclassical viewpoint massless particles, no matter what their spin, obey the EP. General relativity predicts a deflection angle of 2.63 for a nonrelativistic spinless massive boson passing close to the Sun, while for a massive vectorial boson of spin 1 the corresponding deflection is 2.62.     

Indirect bounds on heavy scalar masses of the two-Higgs-doublet model in light of recent Higgs boson searches

We study an upper bound on masses of additional scalar bosons from the electroweak precision data and theoretical constraints such as perturbative unitarity and vacuum stability in the two-Higgs-doublet model taking account of recent Higgs boson search results. If the mass of the Standard-Model-like Higgs boson is rather heavy and is outside the allowed region by the electroweak precision data, such a discrepancy should be compensated by contributions from the additional scalar bosons. We show the upper bound on masses of the additional scalar bosons to be about 2 (1) TeV for the mass of the Standard-Model-like Higgs boson to be 240 (500) GeV.     

Symmetries of the interacting boson model

This contribution reviews the symmetry properties of the interacting boson model of Arima and Iachello. While the concept of a dynamical symmetry is by now a familiar one, this is not necessarily so for the extended notions of partial dynamical symmetry and quasi dynamical symmetry, which can be beautifully illustrated in the context of the interacting boson model. The main conclusion of the analysis is that dynamical symmetries are scarce while their partial and quasi extensions are ubiquitous.     

Top Quark Pair Production at e^＋e^— Colliders in the Topcolor—Assisted Technicolor Model

In the framework of topcolor-assisted technicolor model we calculate the contributions from the preudo Goldstone bosons and new gauge bosons to e^ e^-→ttk.We find that for reasonable ranges of the parameters,the preudo Goldstone bosons afford dominate contribution,the correction arising from new gauge bosons is negligibly small,the maximum of the relative corrections is-10% with the center-of-mass energy √s=500GeV;whereas in the case of √s=1500 GeV,the relative corrections could be up to 16%.Thus large new physics might be observable at the experiments of next-generation linear colliders.     

Lorentz violation from the Higgs portal

We study bounds and signatures of models where the Higgs doublet has an inhomogeneous mass or vacuum expectation value, being coupled to a hidden sector that breaks Lorentz invariance. This physics is best described by a low-energy effective Lagrangian in which the Higgs speed-of-light is smaller than c; such effect is naturally small because it is suppressed by four powers of the inhomogeneity scale. The Lorentz violation in the Higgs sector is communicated at tree level to fermions (via Yukawa interactions) and to massive gauge bosons, although the most important effect comes from one-loop diagrams for photons and from two-loop diagrams for fermions. We calculate these effects by deriving the renormalization-group equations for the speed-of-light of the Standard Model particles. An interesting feature is that the strong coupling dynamically makes the speed-of-light equal for all colored particles.     

TC2模型下底夸克对产生的研究

在顶色辅助的technicolor模型下, 计算了来自赝标哥得斯通玻色子和新规范玻色子对e⁺e^－→bb的截面贡献. 发现由technipions和新规范玻色子产生截面的修正足够小以至于可以忽略, 在合理的参数范围内, top pions起主要作用, 在质心能量√s=500GeV, 修正的最大值可以达到43%; 在√s=1500GeV, 最大的相对修正却只有3.1%. 这为我们在下一代直线对撞机实验中探测顶色辅助的technicolor模型下(TC2模型)提供了可行的方法.     

The Structure of the Neutron-Rich Nd Isotopes in the IBM

The spectra and E2 transition properties of ^146-156Nd isotopes are studied in the interacting boson model in the light of new experimental data. It is found that ^146-150Nd are in the transition from the vibrational limit to the rotational limit. From ¹⁵²Nd onward, the isotopes are nearly perfect rotors. Possible deformation saturation is discussed in the interacting boson model.     

Hidden sector effects on double Higgs production near threshold at the LHC

In this Letter we study a novel effect of a hidden sector coupling to the standard model Higgs boson: an enhancement of the Higgs pair production cross section near threshold due to bound state effects. After summing the ladder contributions of the hidden sector to the effective ggHH coupling, we find the amplitude for gluon-gluon scattering via a Higgs loop. We relate this amplitude to the double Higgs production cross section via the optical theorem. We find that enhancements of the O(100) for the partonic cross section near the threshold region can be obtained for a hidden sector strongly coupled to the Higgs boson. The corresponding cross section at the LHC can be as large as O(10) times the SM result for extreme values of the coupling. The detection of such an effect could in principle lead to important information about the hidden sector.     

Some Electromagnetic Transition Properties of Odd-A Europium Isotopes

In this work, we analyze the positive parity of states of odd-A Eu isotopes within the framework of interacting boson fermion model （IBFM-1）. The result of an IBFM-1 multilevel calculation with the 3s1/2, 2d3/2, 2d5/2, and 1g7/2 single panicle orbits is reported for the positive parity states of the odd-A Eu isotopes. A/so, an IBM-1 calculation is presented for the low-lying states in the even-even 152-154Sm core nucleus. The energy levels and B（E2） transition probabilities are calculated and compared with the experimental data. It is found that the calculated positive parity low spin state energy spectra of the odd-A Eu isotopes agree quite well with the experimental data.     

Associated Productions of HZZ and HHZ at Linear Colliders in Large Extra Dimension Model

In this paper we investigate the effects of the large extra dimensions on the two processes e⁺e^-→ H⁰Z⁰Z⁰ and e⁺e^-→ H⁰Z⁰Z⁰ at linear colliders in both unpolarized and polarized collision modes. We find that the virtual Kaluza-Klein graviton exchange can significantly enhance the cross section from their standard model expectations for these two processes. The results show that the LED effect on the process e⁺e^-→ H⁰Z⁰Z⁰ allows the observation limits on the effective scale M_S to be probed up to 9.75 TeV and 10.1 TeV in the unpolarized and +-(λ_e⁺=1/2, λ_e^-=-1/2) polarized beam collision modes (with P_e⁺=0.6, P_e^-=0.8), respectively. For the process e⁺e^-→ H⁰Z⁰Z⁰, these limits on M_S can be probed up to 6.06 TeV and 6.38 TeV in the unpolarized and polarized collision modes separately. We find that the λ_e⁺=1/2, λ_e^-=-1/2 polarization collision mode in both process e⁺e^-→ H⁰Z⁰Z⁰ and e⁺e^-→ H⁰Z⁰Z⁰ may provide a possibility to improve the sensitivity in probing the LED effects.