首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 0 毫秒
1.
讨论了顶色辅助的人工色理论预言的赝标量Goldstones粒子(TC介子和Top介子)在LC实验中对顶夸克产生的贡献,发现Top介子对顶夸克产生截面σtt的贡献是主要的,在大部分参数空间中荷电Top介子的贡献非常大.当取合理的参数时,荷电Top介子对的σtt贡献可以达到8%左右,能够被LC的实验探测到.  相似文献   

2.
The amt2/m2w order supersymmetric electroweak corrections arising from loops of chargino, neu tralino and squark to top quark pair production by gg fusion at LHC are calculated in the minimal supersymmetric model. We found that the corrections amount about a few percent.  相似文献   

3.
The topcolour-assisted technicolour (TC2) model is an interesting dynamical theory among the various new physics models. We cMculate the total tt cross section and the relative correction of the TC2 model to the cross section at Tevatron Run Ⅱ and LHC. At the Tevatron Run Ⅱ, the cross section predicted by the standard model (SM) is consistent with the experimental data, and in most parameter spaces of the TC2 model, the relative correction of the TC2 model to the cross section is too small to be detectable. We find that the tt cross section is more sensitive to the parameters of the TC2 model at the LHC and the relative correction of the TC2 model to the cross section is over 10% in general. Such a value of the relative correction should be large enough to be detectable at the LHC. Therefore, it is promising to find the clue of the TC2 model via the tt production at the LHC.  相似文献   

4.
The top triangle moose (TTM) model, which can be seen as the deconstructed version of the topcolor-assisted technicolor (TC2) model, predicts the existence of the charged top-pions πt± in low energy spectrum. In the context of this model, we consider photoproduction of πt± via the subprocesses γb → tπt- and γb → tπt+ at the large hadron-electron collider (LHeC), in which high energy photon beams are generated by using the Compton backscatting method. We find that, as long as the charged top-pions are not too heavy, they can be abundantly produced via γb collision.  相似文献   

5.
The littlest Higgs (LH) model is the most economical one among various little Higgs models, which predicts the existence of the charged scalars Φ^±. In this paper, we study the production of the charged Higgs boson Φ^- with single top quark via the process gb →tΦ^- at the CERN Large Hadron Collider (LHC). The numerical results show that the production cross section is sma/ler than 0.2 pb in most of the parameters space, it is very difficult to observe the signatures of the charged scalars via the process pp → gb + X → tΦ^- + X at the LHC experiments. However, it can open a window to distinguish the top-pions in the TC2 model or charged Higgs in the MSSM from Φ^±.  相似文献   

6.
7.
The top triangle moose (TTM) model, which can be seen as the deconstructed version of the topcolor-assisted technicolor (TC2) model, predicts the existence of the charged top-pions πt± in low energy spectrum. In the context of this model, we consider photoproduction of πt± via the subprocesses γb→tπ-and γ→πt+ at the large hadron-electron collider (LHeC), in which high energy photon beams are generated by using the Compton backscatting method. We find that, as long as the charged top-pions are not too heavy, they can be abundantly produced via γb collision.  相似文献   

8.
9.
The dominant decay modes of charged top-pions (π±t ) are tb or ~b. We consider the single production ofcharged top-pions in association with a top quark via e+ e- annihilation and calculate the production cross section of theprocesses e+ e- → t-bπ+ (tb-π-) at the leading order. We find that it can reach 1.2 fb with reasonable parameter values.The charged top-pions may be detected via the channel tbπ± in the future high energy e+ e- colliders.  相似文献   

10.
The twin Higgs mechanism has recently been proposed to solve the little hierarchy problem. In the context of the left-right twin Higgs (LRTH) model, we discuss single production of the new charged gauge boson WH^- , which is predicted by the left-right twin Higgs model, in association with top quark at the CERN Large Hadron Collider (LHC). It is found that, for a typical nonzero value of mass mixing parameter M = 150 GeV in the LRTH model, the production cross section is in the range of 3 ×10^-2 - 6.07×10^3 fb at the LHC. As long as the WH^- is not too heavy, the possible signatures of the heavy charged gauge boson might be detected at the LHC experiments.  相似文献   

11.
The unparticle effects on tt^- production at the future photon collider are investigated. Distributions of tt^- invariant mass and that for transverse momentum of top quark with respect to Standard Model and unparticle production are predicted. An odd valley with scalar unparticle contribution appears for some values of du, which is due to the big cancellation between the contribution from SM and that from unparticle. This character may be used to study the properties of scalar unparticle. Our investigations also show that scalar unparticle may play a significant role in tt^- production at the photon collider if it exists.  相似文献   

12.
13.
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   

14.
We calculate the leading supersymmetric electroweak corrections to t → t1xj0 using dimensional reduction scheme within an approximation of low tan β, which can easily be extended to t→xjbi. The numerical results show that such corrections can exceed -12% for tan β = 2 and -6% for tan β = 11, respectively. And these corrections vary insensitively with mi, in the region allowed by the kinematics except for ones near the threshold.  相似文献   

15.
[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   

16.
Given the null results of searches for new physics at the LHC,we investigate the one-loop effects SUSY QCD in the process e~+e~-→tg at the ILC in Minimal Supersymmetric Standard Model(MSSM).We find that the relative SUSY-QCD corrections to the cross section of e~+e~-→ tg can maximally reach 6.5%(3.2%) at the ILC with (1/2)s= 1000 GeV when m__1= 313.4 GeV and m_g =500(1500) GeV.  相似文献   

17.
Given the null results of searches for new physics at the LHC, we investigate the one-loop effects SUSY QCD in the process e+e-→ttg at the ILC in Minimal Supersymmetric Standard Model (MSSM). We find that the relative SUSY-QCD corrections to the cross section of e+e-→ttg can maximally reach 6.5%(3.2%) at the ILC with √s=1000 GeV when m=313:4 GeV and m=500(1500) GeV.  相似文献   

18.
在Topcolor辅助的多标度人工色(TOPMTC)模型框架下计算了扩充人工色(ETC)相互作用对顶夸克对产生过程中CP破坏参数δ的贡献(δ=σ[e–e→t(–)–t(–)]–σ[e–e→t(+)–t(+)]/σ(e–e→t–t)).计算结果表明,对于合理的参数取值,ETC相互作用可对参数δ产生较大的修正(8.65×10-3≤δ≤1.09×10-2).期望在将来的NLC实验中能观测到此修正效应.  相似文献   

19.
在顶色辅助的人工色模型下计算了高能e^ e^-对撞机上top介子辅助的b夸克对产生过程e^ e^-→bb^-π^0t的产生截面.发现在一定的参数范围内,这个过程的产生截面大于lOfb,比标准模型下标量Higgs粒子辅助的b夸克对产生过程大许多,与最小超对称模型下标量和赝标量Higgs粒子h^0,H^0,A^0的相应产生截面大致相当.人工色理论的信息可能在下一代正负电子对撞实验中探测到.  相似文献   

20.
We investigate the spin correlations in top quark pair production near the threshold at the e^ e^- linear collider. Comparing with the results above the threshold region, we find that near the threshold region the off-diagonal basis, the optimized decomposition of the top quark spins above the threshold region, does not exist, and the beamline basis is the optimal basis, in which there are the dominant spin components: the up-down (UD) component for e^-le^ scattering and the down-up (DU) component for eR^-e^ scattering can make up more than 50% of the total cross section,respectively.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号