R-宇称破缺的相互作用研究

在LHC上，最小超对称标准模型中R-宇称破缺相互作用使LHC上tt对的产生有两种过程，一种是交换slepton粒子的t道的d_Rd_R→t_Lt_L过程，一种是交换squark粒子的u道的d_Rd_R→t_Rt     

探测B_s~0-_s~0混合中的R宇称破缺超对称效应(英文)

最近由CDF合作组和DΦ合作组测量的Bs质量差ΔMs粗略地与标准模型预测值一致,因此这些测量将对限制超出标准模型的新物理信号提供一个机会．考虑Bs0-s0混合中的R宇称破缺超对称效应,并用最近ΔMs的实验结果去限制树图的R宇称破缺耦合．然后,通过从ΔMs实验限制得到R宇称破缺耦合的参数空间,显示在Bs宽度差ΔΓs中的R宇称破缺超对称效应．     

gb→tH-的超对称QCD单圈修正和非退耦效应

在最小超对称标准模型的框架内计算了gb→tH-过程产生截面的单圈超对称QCD修正. 结果发现:若胶子质量和超对称软破缺参数μ或At,Ab同量级且趋于很大,就会出现超对称QCD的非退耦效应. 大的tanβ值可以提高非退耦的贡献,因此大tanβ情况下,较大的修正结果可能在Tevatron和LHC上观测到. 非退耦行为的根本原因在于圈图中的某些耦合顶角正比于超对称质量参数.     

gb→tH－的超对称QCD单圈修正和非退耦效应

在最小超对称标准模型的框架内计算了gb→tH^－过程产生截面的单圈超对称QCD修正.结果发现:若胶子质量和超对称软破缺参数μ或A_t,A_b同量级且趋于很大,就会出现超对称QCD的非退耦效应.大的tanβ值可以提高非退耦的贡献,因此大tanβ情况下,较大的修正结果可能在Tevatron和LHC上观测到.非退耦行为的根本原因在于圈图中的某些耦合顶角正比于超对称质量参数.     

探测B0s—B0s混合中的R宇称破缺超对称效应

最近由CDF合作组和DO合作组测量的B_s质量差ΔM_s粗略地与标准模型预测值一致, 因此这些测量将对限制超出标准模型的新物理信号提供一个机会. 考虑B0s—B0s混合中的R宇称破缺超对称效应, 并用最近ΔM_s的实验结果去限制树图的R宇称破缺耦合. 然后, 通过从ΔM_s实验限制得到R宇称破缺耦合的参数空间, 显示在B_s宽度差ΔΓ_s中的R宇称破缺超对称效应.     

二维超对称模型的超对称破缺和Witten指数

构造了一类超势W=(1/n)gφⁿ的二维O(N)对称超对称模型,详细计算了此类模型的Witten指数△。结果表明,当n为偶数时,超对称一定不能破缺,而当n为奇数时,超对称可以破缺。利用大N展开法,还研究了上述模型的超对称自发破缺机制,同时给出了相应的粒子谱。 关键词：     

暗物质粒子湮没生成的反质子谱

在粒子物理最小超对称标准模型下,计算了X0X0→gg物理过程的反应截面.利用所获得的截面值给出了暗物质粒子Neutralino X0湮没生成的反质子谱.计算表明:反质子谱具有的可观性,为寻找暗物质粒子和超对称粒子提供了一种可能的途径.     

环二硅氨烷的29Si和13C NMR研究

本文报道了十种环二硅氨烷衍生物(R₁=Me、ф;R₂=Me、ф1 R₃=Me;X=Me、ф、OH、OSiMe₃、H和cl)及与此有关的九种聚合物m+n(m=2,3,4,7,10)的²⁹Si和¹³C化学位移,讨论了取代基X、R₁、R₂及硅氧链节数m对化学位移的影响。通过考察化学位移随R₁、R₂的变化,推断环二硅氨烷中N与其周围的三个Si之间存在(p→d)π相互作用。     

TOPCMTC模型中π介子与W±规范玻色子在LHC上的辅助产生

在顶色辅助多标度人工色(TOPCMTC)模型下计算了大动量强子对撞机(LHC)上π介子与W±规范玻色子辅助产生过程pp→bb→W±π的产生截面.发现这个产生截面与最小超对称模型下pp→bb→W±H的相应结果大致相当.在一定的参数范围内,这个过程的产生截面能够达到几十个甚至一百多个fb.W±π的信息可能在LHC上被探测到.     

TOPCMTC模型中π~"非汉字符号"介子与W~±规范玻色子在LHC上的辅助产生(英文)

在顶色辅助多标度人工色 (TOPCMTC)模型下计算了大动量强子对撞机 (LHC)上π 介子与W± 规范玻色子辅助产生过程pp→b b→W±π 的产生截面 .发现这个产生截面与最小超对称模型下pp→b b→W±H 的相应结果大致相当 .在一定的参数范围内 ,这个过程的产生截面能够达到几十个甚至一百多个fb .W±π 的信息可能在LHC上被探测到 .     

Probing R-parity violating interactions from top-quark polarization at LHC

In the minimal supersymmetric standard model the R-parity violating interactions can induce anomalous top pair productions at the LHC through the t-channel process d_Rd̄_R→t_Lt̄_L by exchanging a slepton or by the u-channel process d_Rd̄_R→t_Rt̄_R exchanging a squark. Such top pair productions with a certain chirality cause top-quark polarization in the top pair events. We found that at the LHC, due to the large statistics, the statistical significance of the polarization observable, and thus the probing ability for the corresponding R-parity violating couplings, is much higher than at the Tevatron upgrade. PACS 14.65.Ha; 14.80.Ly     

An effective approach to same sign top pair production at the LHC and the forward-backward asymmetry at the Tevatron

We study the phenomenology of same sign top pair production at the LHC in a model-independent way. The complete set of dimension six operators involving two top (or anti-top) quarks is introduced and the connection with all possible t- or s-channel heavy particle exchanges is established. Only in the former case, same and opposite sign top pair production can be related. We find that while current Tevatron data disfavor t-channel models, other production mechanisms are viable and can be tested at the LHC.     

Effects of R-Parity Violating Supersymmetry in Top Pair Production at Linear Colliders with Polarized Beams

In the minimal supersymmetric standard model with R-parity violation, the lepton number violating top quark interactions can contribute to the top pair production at a linear collider via tree-level u-channel squark exchange diagrams. We calculate such contributions and find that in the allowed range of these R-violating couplings, the top pair production rate as well as the top quark polarization and the forward-backward asymmetry can be significantly altered. By comparing the unpolarized beams with the polarized beams, we find that the polarized beams are more powerful in probing such new physics.     

NNLL threshold resummation for top-pair and single-top production

I discuss threshold resummation at NNLL accuracy in the standard moment-space approach in perturbative QCD for top-pair and single-top production. For top quark pair production I present new approximate NNLO results for the total cross section and for the top quark transverse momentum and rapidity distributions at 8 TeV LHC energy. I discuss the accuracy of the soft-gluon approximation and show that the NLO and NNLO approximate results from resummation are practically indistinguishable from exact NLO and partial NNLO results. For single top production I present new approximate NNLO results for the total cross sections in all three channels at the LHC and also for the top quark transverse momentum distributions in t-channel production and in top-quark associated production with a W boson. For both \(t\bar t\) and single-top production the agreement of theoretical results with LHC and Tevatron data is excellent.     

B s →μ + μ − decay in the R-parity violating minimal supergravity

We study B _s →μ ⁺ μ ^? in the context of the R-parity violating minimal supergravity in the high-tan?β regime. We find that the lowest value of the branching ratio can go well below the present LHCb sensitivity and hence B _s →μ ⁺ μ ^? can even be invisible to the LHC. We also find that the present upper bound on Br?(B _s →μ ⁺ μ ^?) puts strong constraint on the minimal supergravity parameter space. The constraints become more severe if the upper bound is close to its standard model prediction.     

Study of Two Top Production Through FCNC Anomalous Couplings at the LHC

We study the possibility of production of same sign top quark pairs at the LHC as a direct probe of flavor changing neutral current (FCNC) processes in the tqg vertices. In particular, the LHC potential to probe the flavor violating parameter κ/Λ is investigated with 5, 10, 15, and 20 fb^?1 of integrated luminosity of data of 7 and 8 TeV collisions. We find that the LHC can probe it down to 0.13 TeV^?1 via double top production process. Also, we examine the effects of variation of factorization scale and different parton distribution functions on the total cross section of same sign top quark pair at the LHC. The results could be a valid starting point for a more detailed experimental study.     

Measurement of single top production in pp collisions at 7 TeV with the CMS detector

The measurement of t-channel single top cross-section in proton?Cproton collisions at the Large Hadron Collider (LHC) at a centre-of-mass energy of 7 TeV, using data collected with the Compact Muon Solenoid (CMS) experiment during the year 2010 is presented. Both the electron-neutrino and muon-neutrino decay channels of W boson from top decay are considered. Two complementary multivariate analysis methods to separate signal and background and to extract the cross-section for the single top produced in t-channel are explored. The result is compared with the most precise Standard Model theory predictions.     

Top squark and neutralino decays in a <Emphasis Type="Italic">R</Emphasis>-parity violating model constrained by neutrino oscillation data

In a R-parity violating (RPV) model of neutrino mass with three bilinear couplings μ _i and three trilinear couplings λ′ _i33, where i is the lepton index, we find six generic scenarios each with a distinctive pattern of the trilinear couplings consistent with the neutrino oscillation data. These patterns may be reflected in direct RPV decays of the lighter top squark or in the RPV decays of the lightest superparticle, assumed to be the lightest neutralino. Typical signal sizes at the Tevatron RUN II and the LHC have been estimated and the results turn out to be encouraging.      

Neutrino masses in supersymmetry: R-parity and leptogenesis

In the supersymmetric standard model of particle interactions, R-parity nonconservation is often invoked to obtain nonzero neutrino masses. We point out here that such interactions of the supersymmetric particles would erase any pre-existing lepton or baryon asymmetry of the universe before the electroweak phase transition through the B+L violating sphaleron processes. We also point out that all models of radiative generation of neutrino masses suffer from the same problem. We then show how neutrino masses may be obtained in supersymmetry (assuming R-parity conservation) together with successful leptogenesis and predict the possible existence of new observable particles.     

Hydrokinetic predictions for femtoscopy scales in A + A collisions in the light of recent ALICE LHC results

A study of energy behavior of the pion spectra and interferometry scales is carried out for the top SPS, RHIC and for LHC energies within the hydrokinetic approach. The main mechanisms that lead to the paradoxical, at first sight, dependence of the interferometry scales with an energy growth, in particular, a decrease R _out/R _side ratio, are exposed. The hydrokinetic predictions for the HBT radii at LHC energies are compared with the recent results of the ALICE experiment.