共查询到20条相似文献,搜索用时 0 毫秒
1.
2.
YUE Chong-Xing 《理论物理通讯》2001,(7)
[1]C.T. Hill, Phys. Lett. B345 (1995) 483; K. Lane and E.Eichten, Phys. Lett. B352 (1995) 382; K. Lane, Phys.Lett. B433 (1998) 96.
[2]R. Raja, presented at the XXXII Rencontres de Moriond on Electroweak Interactions and Unified Theories, les Arcs, Savoie, France, March 15-22, (1997).
[3]M.E. Peskin, “Physics and Experiments with Linear Collider“, Proceedings of the Workshop, Saarilka, Finland (1991), eds R. Orava, P. Eerala and M. Nordberg, World Scientific, Singapore (1992); A.P. Heinson, Talk given at the XXXIst Rencontres de Moriond, “QCD and High Energy Hadronic Interactions“, les Arcs, Savoie, France,23rd-30th March (1996), Fermilab-Conf. 96/116-E, May (1996).
[4]R.D. Peccei and X. Zhang, Nucl. Phys. B337 (1990) 269;R.D. Peccei, S. Peris and X. Zhang, Nucl. Phys. B349(1991) 305.
[5]S. Dawson, Nucl. Phys. B249 (1985) 42; S. Willenbrock and D. Dicus, Phys. Rev. D34 (1986) 155; S. Dawson and S. Willenbrock, Nucl. Phys. B284 (1987) 449; C.-P.Yuan, Phys. Rev. D41 (1990) 42; F. Anselmo, B. van Eijk and G. Bordes, Phys. Rev. D45 (1992) 2312; R.K. Ellis and S. Parlce, Phys. Rev. D46 (1992) 3875; D. Carlson and C.-P. Yuan, Phys. Lett. B306 (1993) 386; G. Bordes and B. van Eijk, Nucl. Phys. B435 (1995) 23; A. Heinson,A. Belyaev and E. Boos, Phys. Rev. D56 (1997) 3114.
[6]S. Cortese and R. Petronzio, Phys. Lett. B306 (1993) 386;T. Stelzer and S. Willenbrock, Phys. Lett. B357 (1995)125.
[7]M. Smith and S. Willenbrock, Phys. Rev. 954 (1996)6696.
[8]T.G. Rizzo, Phys. Rev. D53 (1996) 6218; G. Mahlon and S. Parke, Phys. Rev. D55 (1997) 7249.
[9]E.H. Simmons, Phys. Rev. D55 (1997) 5494.
[10]A. Datta and X. Zhang, Phys. Rev. D55 (1997) 2530.
[11]YUE Chong-Xing, KUANG Yu-Ping and LU Gong-Ru,Phys. Rev. D56 (1997) 291.
[12]G. Buchalla, G. Burdman, C.T. Hill and D. Kominis,Phys. Rev. D53 (1996) 5185.
[13]K. Lane, Phys. Lett. B357 (1995) 624; YUE ChongXing, ZHOU Hong-Yi, KUANG Yu-Ping and LU GongRu, Phys. Rev. D55 (1997) 5541.
[14]L. Randall and E.H. Simmons, Nucl. Phys. B3S0 (1992)3; V. Lubicz, Nucl. Phys. B404 (1993) 559; V. Lubicz and P. Santorclli, Nucl. Phys. B460 (1996) 3.
[15]G.H. WU, Phys. Rev. Lett. 74 (1995) 4173; C.X. YUE,Y.P. KUANG, et al., Phys. Rev. D52 (1995) 5314; K.Hagiwara and N. Kitazawa, Phys. Rev. D52 (1995) 5374.
[16]C.X. YUE, Y.P. KUANG and G.R. LU, J. Phys. G23(1997) 163.
[17]W. Loinaz and T. Takuchi, Phys. Rev. D60 (1999)015005.
[18]M.B. Popovic and E.H. Simmons, Phys. Rev. D58 (1998)095007.
[19]B. Balaji, Phys. Rev. D53 (1996) 1699.
[20]K. Eicbten and K. Lane, Phys. Lett. B222 (1989) 129; K.Lane and M.V. Ramana, Phys. Rev. D44 (1991) 2678.
[21]Z.J. XIAO, L.D. WAN, G.R. LU, J.M. YANG, X.L.WANG, L.B. GAO and C.X. YUE, J. Phys. G20 (1994)901.
[22]G. Burdman and D. Kominis, Phys. Lett. B403 (1997)101.
[23]C.X. YUE, Y.P. KUANG, X.L. WANG and W.B. LI, hepph/0001133, Phys. Rev. D62 (2000) 055005.
[24]J.H. Field, UGVA-DPNC (120-173) hep-ph/9801413(1997); D. Chang and E. Ma, hep-ph/9909537.
[25]A.P. Heinson, “Future Top Physics at the Tevatron and LHC“, hep-ex/9605010; A.P. Heinson, A.S. Belayev and E.E. Boos, Phys. Rev. D56 (1997) 3114; M. Bohm, W.Hollik and H. Spiesbergerm, Fortschr. Phys. 34 (1986)687.
[26]G.R. LU, et al., Phys. Rev. D54 (1996) 1083.
[27]J. Morfin and W.K. Tung, Z. Phys. C52 (1991) 13.
[28]A. Axelrod, Nucl. Phys. B209 (1982) 349; G. Passarino and M. Veltman, ibid. B160 (1979) 151; M. Clements, et al., Phys. Rev. D27 (1983) 570. 相似文献
3.
在TC2理论框架下,计算了在高能正负电子对撞机(LC)上,TC2动力学对味改变中性流过程e+e-→tc产生截面的修正和TC2理论预言的中性top–pionπ0t对该过程产生截面的贡献.计算结果表明:TC2理论对LC实验中tc夸克联合产生的贡献主要来自中性top-pion π0t.在TC2理论的绝大部分参数空间内,可达10-2ph.若假设LC的积分亮度为500fb-1,则每年可产生数千个tc事例.因此,将来的LC实验可作为检验TC2理论的重要工具. 相似文献
4.
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. 相似文献
5.
6.
Flavor-Changing Neutral-Current Production of t-c in Association with a Neutral Top-Higgs at LHC in the Topcolor-Assisted Technicolor Model 下载免费PDF全文
In the framework of the topcolor-assisted technicolor (TC2) model we investigate the flavor-changing neutral-current production pp→ t-chto at the Large Hadron Collider (LHC), which proceeds through the parton-level processes gg→ t-chto , uu→ t-chto and d-d → t-chto . We calculate the production rate and present the distributions of the transverse momenta and the invarient mass of the neutral top-higgs. It is found that the cross section of pp→ t-chto can reach a few hundreds of fb in a large part of the allowed parameter space. Considering the main decay mode of top-higgs for mht〈2mt, we find that such a production may provide copious events. In the case of unobservation, the LHC can set meaningful constraints on the TC2 model. 相似文献
7.
8.
9.
Based. On the effective Hamiltonian with the generalized factorization approach, we calculate the branchingratios and CP asymmetries of B → VV decays in the Topcolor-assisted Technicolor (TC2) model. Within the consideredparameter space we find that: (a) for the penguin-dominated B → K* φ and K*0 φ decays, the new physics enhancementsto the branching ratios are around 40%; (b) the measured branching ratios of B →K* φ and K*0φ decays prefer therange of 3 Neffc 5; (c) the SM and TC2 model predictions for the branching ratio B(B →ρ ρ0) are only about halfof the Belle‘s measurement; and (d) for most B → VV decays, the new physics corrections on their CP asymmetries are generally small or moderate in magnitude and insensitive to the variation of mπ and Neffc. 相似文献
10.
在顶色辅助的人工色(TC2)理论框架下,研究了顶夸克稀有衰变t→cV过程.结果表明TC2模型预言的标量粒子top-pions和top-Higgs对顶夸克稀有衰变分支比的贡献可以使其比标准模型预言值大6—9个数量级.在大多数参数范围内,分支比的数量级为:Br(t→cg)~10-5,Br(t→cZ)~10-5,Br(t→cγ)~10-7.在合理的参数范围内,顶夸克稀有衰变t→cV过程能够被未来的对撞机实验探测到.因此,顶夸克稀有衰变过程为我们提供了一种检验TC2理论的方法. 相似文献
11.
We calculate one-loop PGB (pseudo-Goldstone bosons) corrections to the cross section for the single-topquarkproduction via qq' → tb at the Fermilab Tevatron in the MWTCM (multiscale walking technicolor model) and topcolor assisted MWTCM. The corrections from PGB in the topcolor assisted MWTCM decrease the production cross section only a few percent, and the corrections from PGB in the MWTCM are found to exceed -l0%, which might be observable at a high-luminosity Tevatron.d:\PDF\.pdf 相似文献
12.
We calculate PGB (pseudo-Goldstone boson) corrections to the decays B → Xsγ and B → K*γ in the MWTCM (multiscale walking technicolor model). The presence of PGBs in the MWTCM leads to large enhancements in the rates of B → Xsγ and B → K*γ. But these results are in conflict with the recent CLEO data on the branching ratios BR (B → Xsγ) and BR(B → K*γ). If topcolor is further introduced, the calculated results in the topcolor assisted MWTCM can be suppressed and be in agreemet with the CLEO data for a certain range of parameters. We also estimate the branching ratio BR (B → Xsg) in the topcolor assisted MWTCM, and this estimate is roughly one order higher than that in the standard model. 相似文献
13.
14.
In this paper, we study the single neutral top-higgs (h0t) production processes at the CERN Large Hadron Collider (LHC) and the International Linear Collider (ILC). At the LHC, the production rates of processes pp→Z(W)h0t are too small to detect h0t . However, with the reasonable parameter values, the cross sections can reach the level of 102 fb for qq→qqh0t process and 103 fb for top quark associated production process pp→th0t+X, respectively. At the ILC, we study the single top-higgs production processes e-γ→νeW-h0t and γγ→W+W-h0t in e-γ and γγ collisions. It is found that the production cross sections can reach the level of a few fb with reasonable parameter values. Furthermore, such processes with the flavor-changing decay mode h0t→tc might provide typical signatures to detected the top-higgs. Therefore, it is hopeful to find the signal of top-higgs at the LHC and ILC experiments via theses processes and test the TC2 model directly. 相似文献
15.
The inclusive production of the doubly heavy baryon [I]bb is investigated with a polarized and unpolarized photon collider. The bb pair in both a color triplet and sextet has been considered to transform into [I]bb. The results indicate that the contribution from the color sextet is about 8% for [I]bb production. For the international linear collider collision energy ranging from 91 GeV to 1000 GeV, the total cross section of 3bb shows a downtrend, i.e., the production Of [I]bb has the maximal rate at x/S=91 GeV. Our results indicate that the initial beam polarization may be an important asset for the production of 3bb. At some collision point, the production rate of [I]bb can be increased by about 17% with an appropriate choice of the initial beam polarization. 相似文献
16.
We calculate the non-oblique correction on Zbb vertex arising from extended technicolor dynamics in one-family technicolor model. We show that this correction is rather large and clearly disfavored by the recently experimental data. 相似文献
17.
XU Wen-Na WANG Xue-Lei XIAO Zhen-Jun 《理论物理通讯》2008,49(1):193-198
In the framework of topcolor-assisted technicolor (TC2) model, there exist tree-level flavor-changing (FC) couplings, which can result in the loop-level FC coupling tcg. Such tcg coupling can contribute significant clues at the forthcoming Large Hadron Collider (LHC) experiments. In this paper, based on the TC2 model, we study some single t-quark production processes involving tcg coupling at the Tevatron and LHC: pp(pp) → tq (q = u, d, s), tg. We calculate the cross sections of these processes. The results show that the cross sections at the Tevatron are too small to observe the signal, but at the LHC it can reach a few pb. With the high luminosity, the LHC has considerable capability to find the single t-quark signal produced via some FC processes involving coupling tcg. On the other hand, these processes can also provide some valuable information of the coupling tcg with detailed study of the processes and furthermore provide the reliable evidence to test the TC2 model 相似文献
18.
19.
Applying perturbative QCD, we study the process Bc → Dsγ in the technicolor with a massless scalar doublet model (TCMLSM). There are mainly two mechanisms contributing to the Bc → D*sγ process. One proceeds through the short distance b → sγ transition and the other through weak annihilation accompanied by a photon emission.We find that, compared with the standard model, the modification of Bc → D*sγ from πρ (the physical pions in the TCMLSM) is so small that can be neglected for the allowed mass ofπρ. The weak-annihilation contribution is found to be about one order larger than that of the electromagnetic penguin diagrams. 相似文献
20.
At LEPⅡ (the energy: √s = 200 GeV), we carry out precise calculations on the process e+e-→tc in the framework of technicolor model with a massless scalar doublet. The results show that the process is unmeasurably small in this TC model. 相似文献