85 results on '"Guo, Si"'
Search Results
2. Precise evaluation of And Axion-like Particle Production
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Zong-Guo Si, Peng-Cheng Lu, Shi-Yuan Li, and Z. Li
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Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Particle physics ,High Energy Physics::Lattice ,Physics beyond the Standard Model ,High Energy Physics::Phenomenology ,Electroweak interaction ,Yukawa potential ,Astronomy and Astrophysics ,Bottom quark ,Charm quark ,Higgs boson ,High Energy Physics::Experiment ,Instrumentation ,Axion - Abstract
We study the decay of the SM Higgs boson to a massive charm quark pair at the next-to-next-to-leading order QCD and next-to-leading order electroweak. At the second order of QCD coupling, we consider the exact calculation of flavour-singlet contributions where the Higgs boson couples to the internal top and bottom quark. Helpful information on the running mass effects related to Yukawa coupling may be obtained by analyzing this process. High precision production for within the SM makes it possible to search for new physics that may induce relatively large interactions related to the charm quark. As an example, we evaluate the axion-like particle associate production with a charm quark pair in the Higgs decay and obtain some constraints for the corresponding parameters under some assumptions.
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- 2021
3. Heavy Majorana neutrino production at future ep colliders
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Zong-Guo Si, Shi-Yuan Li, and Xing-Hua Yang
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Photon ,010308 nuclear & particles physics ,Physics::Instrumentation and Detectors ,Physics beyond the Standard Model ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,01 natural sciences ,Physics::History of Physics ,lcsh:QC1-999 ,law.invention ,MAJORANA ,High Energy Physics - Phenomenology ,Seesaw mechanism ,High Energy Physics - Phenomenology (hep-ph) ,law ,0103 physical sciences ,High Energy Physics::Experiment ,Neutrino ,010306 general physics ,Collider ,lcsh:Physics - Abstract
The heavy singlet Majorana neutrinos are introduced to generate the neutrino mass in the so-called phenomenological type-I seesaw mechanism. The phenomena induced by the heavy Majorana neutrinos are important to search for new physics. In this paper, we explore the heavy Majorana neutrino production and decay at future $e^{-}p$ colliders. The corresponding cross sections via $W$ and photon fusion are predicted for different collider energies. Combined with the results of the heavy Majorana neutrino production via single $W$ exchange, this work can provide helpful information to search for heavy Majorana neutrinos at future $e^{-}p$ colliders., 15 pages, 16 figures
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- 2019
4. Exclusive production ratio of neutral to charged kaon pair in e+e− annihilation continuum via a relativistic quark model
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Tao Yao, Zhao-Xia Meng, Shi-Yuan Li, Yan-Rui Liu, Zong-Guo Si, and Yi Jin
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Quark ,Physics ,Particle physics ,Annihilation ,Bethe–Salpeter equation ,Valence (chemistry) ,010308 nuclear & particles physics ,Electron–positron annihilation ,Nuclear Theory ,Quark model ,01 natural sciences ,0103 physical sciences ,High Energy Physics::Experiment ,010306 general physics - Abstract
A completely relativistic quark model in the Bethe-Salpeter framework is employed to calculate the exclusive production ratio of the neutral to charged kaon pair in ${e}^{+}{e}^{\ensuremath{-}}$ annihilation continuum region below the $J/\mathrm{\ensuremath{\Psi}}$ mass. The valence quark charge plays the key role. The cancellation of the diagrams for the same charge case (${K}_{S}+{K}_{L}$) and the noncancellation of the diagrams for the different charge case (${K}^{\ensuremath{-}}+{K}^{+}$) lead to the ratio as ${({m}_{s}\ensuremath{-}{m}_{d})}^{2}/{M}_{kaon}^{2}\ensuremath{\approx}1/10$.
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- 2020
5. Top quark as a probe of heavy Majorana neutrino at the LHC and future colliders
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Lei Wu, Bin Zhu, Zong-Guo Si, Hang Zhou, and Ning Liu
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Physics ,Top quark ,Particle physics ,Large Hadron Collider ,Physics::Instrumentation and Detectors ,High Energy Physics::Phenomenology ,Hadron ,Dark matter ,FOS: Physical sciences ,High Energy Physics - Experiment ,law.invention ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,MAJORANA ,High Energy Physics - Phenomenology (hep-ph) ,law ,Double beta decay ,High Energy Physics::Experiment ,Neutrino ,Nuclear Experiment ,Collider - Abstract
Right-handed (RH) Majorana neutrinos play a crucial role in understanding the origin of neutrino mass, the nature of dark matter and the mechanism of matter-antimatter asymmetry. In this work, we investigate the observability of heavy Majorana neutrino through the top quark neutrinoless double beta decay process $t \to b \ell^+ \ell^+ j j$ at hadron colliders. By performing detector level simulation, we demonstrate that our method can give stronger limits on the light-heavy neutrino mixing parameters $|V_{eN, \mu N}|$ in the mass range of 15 GeV $< m_N, Comment: 6 pages, discussions added, version published in PRD (rapid communication)
- Published
- 2020
6. Spectrum and rearrangement decays of tetraquark states with four different flavors
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J. Cheng, Shi-Yuan Li, Tao Yao, Yu-Nan Liu, Zong-Guo Si, and Yan-Rui Liu
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Particle physics ,Nuclear Theory ,Isoscalar ,FOS: Physical sciences ,01 natural sciences ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,symbols.namesake ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Lattice ,Hadron spectroscopy ,0103 physical sciences ,Nuclear Experiment (nucl-ex) ,010306 general physics ,Nuclear theory ,Nuclear Experiment ,Stable state ,Physics ,010308 nuclear & particles physics ,High Energy Physics - Lattice (hep-lat) ,High Energy Physics::Phenomenology ,High Energy Physics - Phenomenology ,Mass spectrum ,symbols ,Tetraquark ,High Energy Physics::Experiment ,Hamiltonian (quantum mechanics) - Abstract
We have systematically investigated the mass spectrum and rearrangement decay properties of the exotic tetraquark states with four different flavors using a color-magnetic interaction model. Their masses are estimated by assuming that the $X(4140)$ is a $cs\bar{c}\bar{s}$ tetraquark state and their decay widths are obtained by assuming that the Hamiltonian for decay is a constant. According to the adopted method, we find that the most stable states are probably the isoscalar $bs\bar{u}\bar{d}$ and $cs\bar{u}\bar{d}$ with $J^P=0^+$ and $1^+$. The width for most unstable tetraquarks is about tens of MeVs, but that for unstable $cu\bar{s}\bar{d}$ and $cs\bar{u}\bar{d}$ can be around 100 MeV. For the $X(5568)$, our method cannot give consistent mass and width if it is a $bu\bar{s}\bar{d}$ tetraquark state. For the $I(J^P)=0(0^+),0(1^+)$ double-heavy $T_{bc}=bc\bar{u}\bar{d}$ states, their widths can be several MeVs., Version published in PRD. 18 pages, 1 figure, 9 tables
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- 2020
7. Double-heavy tetraquark states with heavy diquark-antiquark symmetry
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J. Cheng, Shi-Yuan Li, Zong-Guo Si, Tao Yao, and Yan-Rui Liu
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Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,Hadron ,FOS: Physical sciences ,01 natural sciences ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Lattice ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Nuclear Experiment (nucl-ex) ,010306 general physics ,Instrumentation ,Nuclear theory ,Nuclear Experiment ,Physics ,010308 nuclear & particles physics ,High Energy Physics - Lattice (hep-lat) ,Astronomy and Astrophysics ,State (functional analysis) ,Diquark ,High Energy Physics - Phenomenology ,Tetraquark ,Symmetry (geometry) ,Color structure ,Bar (unit) - Abstract
We calculate the masses of the $QQ\bar{q}\bar{q}$ ($Q=c,b$; $q=u,d,s$) tetraquark states with the aid of heavy diquark-antiquark symmetry (HDAS) and the chromomagnetic interaction (CMI) model. The masses of the highest-spin ($J=2$) tetraquarks that have only the $(QQ)_{\bar{3}_c}(\bar{q}\bar{q})_{3_c}$ color structure are related with those of conventional hadrons using HDAS. Thereafter, the masses of their partner states are determined with the mass splittings in the CMI model. Our numerical results reveal that: (i) the lightest $cc\bar{n}\bar{n}$ ($n=u,d$) is an $I(J^P)=0(1^+)$ state around 3929 MeV (53 MeV above the $DD^*$ threshold) and none of the double-charm tetraquarks are stable; (ii) the stable double-bottom tetraquarks are the lowest $0(1^+)$ $bb\bar{n}\bar{n}$ around 10488 MeV ($\approx116$ MeV below the $BB^*$ threshold) and the lowest $1/2(1^+)$ $bb\bar{n}\bar{s}$ around 10671 MeV ($\approx20$ MeV below the $BB_s^*/B_sB^*$ threshold); and (iii) the two lowest $bc\bar{n}\bar{n}$ tetraquarks, namely the lowest $0(0^+)$ around 7167 MeV and the lowest $0(1^+)$ around 7223 MeV, are near-threshold states. Moreover, we discuss the constraints on the masses of double-heavy hadrons. Specifically, for the lowest nonstrange tetraquarks, we obtain $T_{cc}, 19 pages, 4 figures, and 11 tables
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- 2020
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8. Central-edge asymmetry as a probe of Higgs-top coupling in tt¯h production at the LHC
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Jinmian Li, Lei Wu, Zong-Guo Si, and Jason Tsz Shing Yue
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,media_common.quotation_subject ,Elementary particle ,Coupling (probability) ,01 natural sciences ,Asymmetry ,Standard Model ,Nuclear physics ,0103 physical sciences ,Higgs boson ,Grand Unified Theory ,CP violation ,010306 general physics ,Boson ,media_common - Abstract
The Higgs-top coupling plays a central role in the hierarchy problem and the vacuum stability of the Standard Model (SM). We propose a central-edge asymmetry ( A C E ) to probe the CP violating Higgs-top coupling in dileptonic channel of t t ¯ h ( → b b ¯ ) production at the LHC. We demonstrate that the CP-violating Higgs-top coupling can affect the central-edge asymmetry through distorting Δ y l + l − distribution because of the contribution of new top charge asymmetric term. Since Δ y l + l − distribution is frame-independent and has a good discrimination even in boosted regime, we use the jet substructure technique to enhance the observability of the dileptonic channel of t t ¯ h production. We find that (1) the significance of dileptonic channel of t t ¯ h production can reach 5 σ for CP phase ξ = 0 , π / 4 , π / 2 when the luminosity L = 795 , 993 , 1276 fb − 1 at 14 TeV LHC. (2) the central-edge asymmetry A C E show a good discrimination power of CP phase of t t ¯ h interaction, which are − 40.26 % , − 26.60 % , − 9.47 % for ξ = 0 , π / 4 , π / 2 respectively and are hardly affected by the event selections. Besides, by performing the binned- χ 2 analysis of Δ y l + l − distribution, we find that the scalar and pseudo-scalar interactions can be distinguished at 95% C.L. level at 14 TeV HL-LHC.
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- 2018
9. Constraints on dark matter interactions from the first results of DarkSide-50
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Yu-Feng Zhou, Chun-Yuan Li, and Zong-Guo Si
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Argon ,010308 nuclear & particles physics ,Dark matter ,chemistry.chemical_element ,FOS: Physical sciences ,DarkSide ,Parameter space ,Kinetic energy ,01 natural sciences ,Dark photon ,High Energy Physics - Phenomenology ,Xenon ,High Energy Physics - Phenomenology (hep-ph) ,chemistry ,Isospin ,0103 physical sciences ,lcsh:QC770-798 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics - Abstract
In an extended effective operator framework of isospin violating interactions with light mediators, we investigate the compatibility of the candidate signal of the CDMS-II-Si with the latest constraints from DarkSide-50 and XENON-1T, etc. We show that the constraints from DarkSide-50 which utilizes Argon as the target is complementary to that from XENON-1T which utilizes Xenon. Combining the results of the two experiments, we find that for isospin violating interaction with light mediator there is no parameter space which can be compatible with the positive signals from CDMS-II-Si. As a concrete example of this framework, we investigate the dark photon model in detail. We obtain the combined limits on the dark matter mass $m_{\chi}$, the dark photon mass $m_{A'}$, and the kinetic mixing parameter $\varepsilon$ in the dark photon model. The DarkSide-50 gives more stringent upper limits in the region of mediator mass from 0.001 to 1 GeV, for $m_{\chi} \lesssim 6$ GeV in the ($m_{A'}$,$\varepsilon$) plane, and more stringent constraints for $m_{\chi}\lesssim 8$ GeV and $\varepsilon \thicksim 10^{-8}$ in the ($m_{\chi}$,$m_{A'}$) plane., Comment: 22 pages, 5 figures
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- 2019
- Full Text
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10. Pentaquark states with the $$QQQq\bar{q}$$ Q Q Q q q ¯ configuration in a simple model
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Yu-Nan Liu, Jing Wu, Zong-Guo Si, Shi-Yuan Li, and Yan-Rui Liu
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Physics ,Particle physics ,Conjecture ,Physics and Astronomy (miscellaneous) ,Meson ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,State (functional analysis) ,01 natural sciences ,Pentaquark ,Interpretation (model theory) ,Baryon ,Simple (abstract algebra) ,0103 physical sciences ,High Energy Physics::Experiment ,Nuclear Experiment ,010306 general physics ,Engineering (miscellaneous) ,Bar (unit) - Abstract
We discuss the mass splittings for the $S$-wave triply heavy pentaquark states with the $QQQq\bar{q}$ $(Q=b,c;q=u,d,s)$ configuration which is a mirror structure of $Q\bar{Q}qqq$. The latter configuration is related with the nature of $P_c(4380)$ observed by the LHCb Collaboration. The considered pentaquark masses are roughly estimated with a simple method. One finds that such states are probably not narrow even if they do exist. This leaves room for molecule interpretation for a state around the low-lying threshold of a doubly heavy baryon and a heavy-light meson, e.g. $\Xi_{cc}D$, if it were observed. As a by product, we conjecture that upper limits for the masses of the conventional triply heavy baryons can be determined by the masses of the conventional doubly heavy baryons.
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- 2019
11. Production and constraints for a massive dark photon at electron-positron colliders *
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Jun Jiang, Shankar Dayal Pathak, Shi-Yuan Li, Zong-Guo Si, Xing-Hua Yang, and Chun-Yuan Li
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Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Scalar (mathematics) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Electron ,01 natural sciences ,Dark photon ,Luminosity ,Standard Model ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Positron ,0103 physical sciences ,High Energy Physics::Experiment ,Production (computer science) ,010306 general physics ,Instrumentation - Abstract
Dark sector may couple to the Standard Model via one or more mediator particles. We discuss two types of mediators: the dark photon $A^{\prime}$ and the dark scalar mediator $\phi$. The total cross-sections and various differential distributions of the processes $e^{+} e^{-} \rightarrow q \bar{q} A^{\prime}$ and $e^{+} e^{-} \rightarrow q \bar{q} \phi$ ($q=u,~d,~c,~s$ and $b$ quarks) are discussed. We focus on the study of the invisible $A^{\prime}$ due to the cleaner background at future $e^{+} e^{-}$ colliders. It is found that the kinematic distributions of the two-jet system could be used to identify (or exclude) the dark photon and the dark scalar mediator, as well as to distinguish between them. We further study the possibility of a search for dark photons at a future CEPC experiment with $\sqrt{s}=$ 91.2 GeV and 240 GeV. With CEPC running at $\sqrt{s}=$ 91.2 GeV, it would be possible to perform a decisive measurement of the dark photon (20 GeV $< m_{A^{\prime}}, Comment: 17 pages, 10 figures, to be published in Chinese Physics C
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- 2020
12. Study Standard Model and Majorana Neutrino Contributions to $B^{+} \to K^{(*)\pm}\mu^+\mu^{\mp}$
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Cong-Feng Qiao, Zong-Guo Si, Peng-Cheng Lu, Ying Wang, and Hong-Lei Li
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Astronomy and Astrophysics ,Type (model theory) ,01 natural sciences ,Lepton number ,Standard Model ,MAJORANA ,High Energy Physics - Phenomenology ,Seesaw mechanism ,0103 physical sciences ,B meson ,Invariant mass ,High Energy Physics::Experiment ,Neutrino ,010306 general physics ,Instrumentation - Abstract
Lepton number violation processes can be induced by the Majorana neutrino exchange, which provide evidence for the Majorana nature of neutrinos. In addition to the natural explanation of the small neutrino masses, Type-I seesaw mechanism predicts the existence of Majorana neutrinos. The aim of this work is to study the B meson rare decays $B^{+} \to K^{(*)+}\mu^+\mu^-$ in the standard model and its extensions, and then to investigate the same-sign decay processes $B^{+}\to K^{(*)-}\mu^{+}\mu^+$. The corresponding dilepton invariant mass distributions are predicted. It is found that the dilepton angular distributions illustrate the properties of new interactions induced by the Majorana neutrinos., Comment: 17 pages, 6 figures
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- 2018
13. Differential decay rates of CP-even and CP-odd Higgs bosons to top and bottom quarks at NNLO QCD
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Werner Bernreuther, Long Chen, and Zong-Guo Si
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Quark ,Nuclear and High Energy Physics ,Particle physics ,Higgs Physics ,Astrophysics::High Energy Astrophysical Phenomena ,High Energy Physics::Lattice ,FOS: Physical sciences ,Jet (particle physics) ,01 natural sciences ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Heavy Quark Physics ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,ddc:530 ,010306 general physics ,Boson ,Physics ,Quantum chromodynamics ,Energy distribution ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Perturbative QCD ,High Energy Physics - Phenomenology ,Beyond Standard Model ,Higgs boson ,lcsh:QC770-798 ,High Energy Physics::Experiment ,Differential (mathematics) - Abstract
We consider the decay of a neutral Higgs boson of arbitrary CP nature to a massive quark antiquark pair at next-to-next-to-leading order in perturbative QCD. Our analysis is made at the differential level using the antenna subtraction framework. We apply our general set-up to the decays of a CP-even and CP-odd heavy Higgs boson to a top-quark top-antiquark pair and to the decay of the 125 GeV Higgs boson to a massive bottom-quark bottom-antiquark pair. In the latter case we calculate, in particular, the two-jet, three-jet, and four-jet decay rates and, for two-jet events, the energy distribution of the leading jet., Latex, 23 pages, a reference added
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- 2018
14. A precise determination of the top-quark pole mass
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Zong-Guo Si, Sheng-Quan Wang, Stanley J. Brodsky, and Xing-Gang Wu
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Particle physics ,Top quark ,Physics and Astronomy (miscellaneous) ,media_common.quotation_subject ,Tevatron ,FOS: Physical sciences ,lcsh:Astrophysics ,Scale (descriptive set theory) ,01 natural sciences ,Asymmetry ,law.invention ,Renormalization ,High Energy Physics - Phenomenology (hep-ph) ,law ,lcsh:QB460-466 ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Nuclear Experiment ,010306 general physics ,Collider ,Engineering (miscellaneous) ,media_common ,Quantum chromodynamics ,Physics ,Large Hadron Collider ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,High Energy Physics - Phenomenology ,lcsh:QC770-798 ,High Energy Physics::Experiment - Abstract
The Principle of Maximum Conformality (PMC) provides a systematic way to eliminate the renormalization scheme and renormalization scale uncertainties for high-energy processes. We have observed that by applying PMC scale-setting, one obtains comprehensive and self-consistent pQCD predictions for the top-quark pair total cross-section and the top-quark pair forward-backward asymmetry in agreement with the measurements at the Tevatron and LHC. As a step forward, in the present paper, we determine the top-quark pole mass via a detailed comparison of the top-quark pair cross-section with the measurements at the Tevatron and LHC. The results for the top-quark pole mass are $m_t=174.6^{+3.1}_{-3.2}$ GeV for the Tevatron with $\sqrt{S}=1.96$ TeV, $m_t=173.7\pm1.5$ GeV and $174.2\pm1.7$ GeV for the LHC with $\sqrt{S} = 7$ TeV and $8$ TeV, respectively. Those predictions agree with the average, $173.34\pm0.76$ GeV, obtained from various collaborations via direct measurements. The consistency of the pQCD predictions using the PMC with all of the collider measurements at different energies provides an important verification of QCD., Comment: 10 pages, 6 figures. Revised version to be published in Eur.Phys.J.C
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- 2018
15. Higgs production in association with bottom quark pair at LHC
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Ying Wang, Hong-Lei Li, Zong-Guo Si, Peng-Cheng Lu, Wen-Tao Huang, Shi-Yuan Li, and Zhong-Juan Yang
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,Computer Science::Information Retrieval ,Physics beyond the Standard Model ,High Energy Physics::Lattice ,Hadron ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Computer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing) ,Astronomy and Astrophysics ,Yukawa interaction ,Bottom quark ,Atomic and Molecular Physics, and Optics ,Standard Model ,Two-Higgs-doublet model ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Higgs boson ,Computer Science::General Literature ,High Energy Physics::Experiment - Abstract
The direct observation of the Yukawa interaction related to Standard Model Higgs and the bottom quark is obtained from the $h\to b\bar{b}$ process recently. The b-tagging becomes an important tool to search for new heavy resonance production at LHC. We use the b-tagging method to investigate the neutral Higgs production in association with a bottom quark pair, and perform the detector simulation for the signal process with the Higgs decaying into $b\bar{b}$ or $\tau^+\tau^-$ together with the dominant backgrounds. Our results show that $b\bar{b}b\bar{b}$ and $b\bar{b}\tau^+\tau^-$ processes will play an important role to search for the exotic heavy Higgs production at LHC and future hadron colliders., Comment: 21 pages, 12 figures
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- 2018
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16. Production of heavy Higgs bosons and decay into top quarks at the LHC. II: top-quark polarization and spin correlation effects
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Zong-Guo Si, Peter Galler, Peter Uwer, and Werner Bernreuther
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Quark ,Particle physics ,Top quark ,High Energy Physics::Lattice ,FOS: Physical sciences ,Elementary particle ,Weak interaction ,01 natural sciences ,Nuclear physics ,symbols.namesake ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Physics::Atomic and Molecular Clusters ,010306 general physics ,QC ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Computer Science::Computers and Society ,Higgs field ,High Energy Physics - Phenomenology ,Pair production ,Higgs boson ,symbols ,High Energy Physics::Experiment ,Higgs mechanism - Abstract
We analyze, within several parameter scenarios of type-II two-Higgs doublet extensions of the standard model, the impact of heavy neutral Higgs-boson resonances on top-quark pair production and their subsequent decay to dileptonic final states at the LHC (13 TeV). In particular, we investigate the effects of heavy Higgs bosons on top-spin observables, that is, the longitudinal top-quark polarization and top-quark spin correlations. We take into account NLO QCD as well as weak interaction corrections and show that top-spin observables, if evaluated in judiciously chosen top-quark pair invariant mass bins, can significantly enhance the sensitivity to heavy Higgs resonances in top-quark pair events., 36 pages, 9 figures
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- 2017
17. Hidden-charm Pentaquark Production at $e^+e^-$ Colliders
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Xiao-Feng Zhang, Yan-Rui Liu, Yu-Nan Liu, Zong-Guo Si, and Shi-Yuan Li
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Physics ,Particle physics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Physics and Astronomy (miscellaneous) ,010308 nuclear & particles physics ,0103 physical sciences ,FOS: Physical sciences ,010306 general physics ,01 natural sciences ,Pentaquark ,B-factory - Abstract
We study one possible production mechanism for hidden charm pentaquark in e+e- collision, where it is produced via a color-octet c \bar c pair fragmentation. The pentaquark production at B factory energy is dominated by e+e- to c \bar c g to Pc + X. At Z^0 pole, for the pentaquark production, there are several partonic processes playing significant role. Our results show that it is possible to search for the direct pentaquark production signal at e+e- colliders, which is important to understand the properties of pentaquark., Comment: 8 pages, 4 figures, 2 tables
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- 2017
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18. Running of the Charm-Quark Mass from HERA Deep-Inelastic Scattering Data
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Johannes Blümlein, Amanda Cooper-Sarkar, Laurent Favart, Grzegorz Nowak, R. Plačakytė, A. Buniatyan, S. Schmitt, J. Hladkỳ, E. Elsen, A. Garfagnini, Klaus Rabbertz, B. B. Levchenko, M. Lisovyi, D. Haidt, Aleksander Filip Żarnecki, Z. P. Zhang, R. Brugnera, I. Abt, T. Tymieniecka, K. Wichmann, O. Zenaiev, J. Feltesse, K. Daum, Andrii Verbytskyi, S. Mikocki, Katerina Lipka, E. Paul, L. M. Shcheglova, Peter Bussey, L. Stanco, Achim Geiser, I. A. Korzhavina, Zong-Guo Si, Maria Vittoria Garzelli, Andrii Gizhko, M. Kapichine, Matthew Wing, P. Truöl, Olaf Behnke, Sven Moch, Th. Naumann, A. Longhin, Roberto Carlin, A. W. Jung, J. Gayler, H. Spiesberger, A. Bertolin, B. Foster, S. Dusini, D. Britzger, Département de Physique des Particules (ex SPP) ( DPP ), Institut de Recherches sur les lois Fondamentales de l'Univers ( IRFU ), Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ) -Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ) -Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire ( LAL ), Université Paris-Sud - Paris 11 ( UP11 ) -Institut National de Physique Nucléaire et de Physique des Particules du CNRS ( IN2P3 ) -Centre National de la Recherche Scientifique ( CNRS ), Département de Physique des Particules (ex SPP) (DPP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de l'Accélérateur Linéaire (LAL), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Sud - Paris 11 (UP11), and Département de Physique des Particules (ex SPP) (DPhP)
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Nuclear and High Energy Physics ,Particle physics ,Photon ,High Energy Physics::Lattice ,FOS: Physical sciences ,Context (language use) ,01 natural sciences ,Charm quark ,renormalization ,Nuclear physics ,High Energy Physics - Phenomenology (hep-ph) ,deep inelastic scattering ,0103 physical sciences ,ddc:530 ,Charm (quantum number) ,quantum chromodynamics: perturbation theory ,010306 general physics ,Physics ,Quantum chromodynamics ,010308 nuclear & particles physics ,Scattering ,High Energy Physics::Phenomenology ,higher-order: 1 ,charm: production ,HERA ,Deep inelastic scattering ,lcsh:QC1-999 ,quark: mass ,High Energy Physics - Phenomenology ,DESY HERA Stor ,scale dependence ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,High Energy Physics::Experiment ,[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,charm ,lcsh:Physics - Abstract
Physics letters / B 775, 233 - 238 (2017). doi:10.1016/j.physletb.2017.11.002, Combined HERA data on charm production in deep-inelastic scattering have previously been used to determine the charm-quark running mass $m_{c}(m_{c})$ in the $\overline{MS}$renormalisation scheme. Here, the same data are used as a function of the photon virtuality $Q^2$ to evaluate the charm-quark running mass at different scales to one-loop order, in the context of a next-to-leading order QCD analysis. The scale dependence of the mass is found to be consistent with QCD expectations., Published by Elsevier, Amsterdam
- Published
- 2017
19. Study Majorana neutrino contribution to B -meson semi-leptonic rare decays
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Zong-Guo Si, Y. G. Wang, Shou-Shan Bao, Nan Zhu, and Zuo-Hong Li
- Subjects
Physics ,Lepton number violation ,Nuclear and High Energy Physics ,Sterile neutrino ,Particle physics ,Physics::Instrumentation and Detectors ,Branching fraction ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Perturbative QCD ,Lepton number ,lcsh:QC1-999 ,Nuclear physics ,High Energy Physics - Phenomenology ,MAJORANA ,High Energy Physics - Phenomenology (hep-ph) ,B-meson rare decay ,New physics beyond standard model ,High Energy Physics::Experiment ,Neutrino ,Neutrino oscillation ,lcsh:Physics ,Majorana neutrino ,Majorana equation - Abstract
B meson semi-leptonic rare decays are sensitive to new physics beyond standard model. We study the $B^{-}\to \pi^{-}\mu^{+}\mu^{-}$ process and investigate the Majorana neutrino contribution to its decay width. The constraints on the Majorana neutrino mass and mixing parameter are obtained from this decay channel with the latest LHCb data. Utilizing the best fit for the parameters, we study the lepton number violating decay $B^{-}\to \pi^{+}\mu^{-}\mu^{-}$, and find its branching ratio is about $6.4\times10^{-10}$, which is consistent with the LHCb data reported recently., Comment: 10 pages, 3 figures
- Published
- 2014
20. Top-quark pair production at next-to-next-to-leading order QCD in electron positron collisions
- Author
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Werner Bernreuther, Oliver Dekkers, Dennis Heisler, Long Chen, and Zong-Guo Si
- Subjects
Particle physics ,Top quark ,Nuclear and High Energy Physics ,media_common.quotation_subject ,Computation ,High Energy Physics::Lattice ,FOS: Physical sciences ,Electron ,pair production [top] ,01 natural sciences ,Asymmetry ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,Positron ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,quantum chromodynamics ,ddc:530 ,010306 general physics ,media_common ,Quantum chromodynamics ,Physics ,electron positron ,pair [quark antiquark] ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,top: production ,Observable ,quark antiquark: pair ,High Energy Physics - Phenomenology ,Pair production ,production [top] ,High Energy Physics::Experiment ,antiquark ,top: pair production ,asymmetry - Abstract
We set up a formalism, within the antenna subtraction framework, for computing the production of a massive quark-antiquark pair in electron positron collisions at next-to-next-to-leading order in the coupling $\alpha_s$ of quantum chromodynamics at the differential level. Our formalism applies to the calculation of any infrared-safe observable. We apply this set-up to the production of top-quark top antiquark pairs in the continuum. We compute the production cross section and several distributions. We determine, in particular, the top-quark forward-backward asymmetry at order $\alpha_s^2$. Our result agrees with previous computations of this observable., Comment: Latex, 33 pages, reference added
- Published
- 2016
21. Heavy Higgs boson resonances and their decay into top quarks at the LHC
- Author
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Werner Bernreuther, Clemens Mellein, Peter Uwer, Zong-Guo Si, and Peter Galler
- Subjects
Quantum chromodynamics ,Quark ,Physics ,Particle physics ,Large Hadron Collider ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,Yukawa potential ,Resonance ,FOS: Physical sciences ,Observable ,High Energy Physics - Phenomenology ,Pair production ,High Energy Physics - Phenomenology (hep-ph) ,Higgs boson ,High Energy Physics::Experiment ,QC - Abstract
We investigate, within the type-II two-Higgs-doublet extension of the standard model (SM), the impact of heavy neutral Higgs boson resonances with unsuppressed Yukawa couplings to top quarks on top-quark pair production at the LHC at next-to-leading order (NLO) in the strong coupling constant. We take into account the resonant Higgs boson contributions, the non-resonant SM $t\bar{t}$ continuum and the interference of these two contributions. The NLO QCD corrections to heavy Higgs production and the interference contributions are calculated in the large top-quark mass ($m_t$) limit, including an effective K-factor rescaling. Our evaluation of the QCD-Higgs interference is focused on the Higgs resonance region. Using representative CP-conserving as well as CP-violating parameter scenarios phenomenological results are presented for different observables., 10 pages, 4 figures, contribution to the proceedings of the Fourth Annual Large Hadron Collider Physics conference, 13-18 June 2016, Lund, Sweden
- Published
- 2016
22. Exotic Hadron Bound State Production at Hadronic Colliders
- Author
-
Yan-Rui Liu, Xiao-Feng Zhang, Shi-Yuan Li, Lu Meng, Zong-Guo Si, and Yi Jin
- Subjects
Physics ,Nuclear and High Energy Physics ,High energy ,Particle physics ,Nuclear Theory ,010308 nuclear & particles physics ,Hadron ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Astronomy and Astrophysics ,Exotic hadron ,01 natural sciences ,Nuclear Theory (nucl-th) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Bound state ,Production (economics) ,High Energy Physics::Experiment ,010306 general physics ,Wave function ,Nuclear Experiment ,Instrumentation ,Event (particle physics) - Abstract
The non-relativistic wave function framework is applied to study the production and decay of the exotic hadrons which can be effectively described as bound states of other hadrons. Employing the factorized formulation, we investigate the production of exotic hadrons in the multiproduction processes at high energy hadronic colliders with the help of event generators. This study provides crucial information for the measurements of the relevant exotic hadrons., This paper also serves partially as the long write-up for the paper arXiv:1603.03250, to be published in Chinese Physics C
- Published
- 2016
23. Color connections of the four-quark QQ¯Q′Q¯′ system and doubly heavy baryon production in e+e− annihilation
- Author
-
Shi-Yuan Li, Zong-Guo Si, Yi Jin, Zhong-Juan Yang, and Tao Yao
- Subjects
Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Annihilation ,Electron–positron annihilation ,Nuclear Theory ,High Energy Physics::Phenomenology ,Hadron ,Hadronization ,Baryon ,Diquark ,Nuclear physics ,High Energy Physics::Experiment ,Tetraquark ,Nuclear Experiment - Abstract
The hadronization effects induced by various color connections of the four-quark system in e + e − annihilation are briefly reviewed. A special color connection of the four-heavy-quark system with no color separation favors the production of doubly heavy baryons. For the related three-jet case, the corresponding hadronization has not yet been considered. We argue that it can be effectively described as two-string fragmentation in addition to the leading heavy diquark fragmentation. The production rate and the properties of the final-state hadron systems are discussed. Emphasis is placed on the string effect as a fingerprint of this hadronization procedure.
- Published
- 2013
24. Production of heavy Higgs bosons and decay into top quarks at the LHC
- Author
-
Clemens Mellein, Peter Galler, Zong-Guo Si, Peter Uwer, and Werner Bernreuther
- Subjects
Quark ,Physics ,Quantum chromodynamics ,Top quark ,Particle physics ,Large Hadron Collider ,010308 nuclear & particles physics ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,01 natural sciences ,Standard Model ,Nuclear physics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Higgs boson ,High Energy Physics::Experiment ,Nuclear Experiment ,010306 general physics ,QC ,Lepton ,Boson - Abstract
We investigate the production of heavy, neutral Higgs boson resonances and their decays to top-quark top-antiquark ($t\bar{t}$) pairs at the Large Hadron Collider (LHC) at next-to-leading order (NLO) in the strong coupling of quantum chromodynamics (QCD). The NLO corrections to heavy Higgs boson production and the Higgs-QCD interference are calculated in the large $m_t$ limit with an effective K-factor rescaling. The nonresonant $t\bar{t}$ background is taken into account at NLO QCD including weak-interaction corrections. In order to consistently determine the total decay widths of the heavy Higgs bosons, we consider for definiteness the type-II two-Higgs-doublet extension of the standard model and choose three parameter scenarios that entail two heavy neutral Higgs bosons with masses above the $t\bar{t}$ threshold and unsuppressed Yukawa couplings to top quarks. For these three scenarios we compute, for the LHC operating at 13 TeV, the $t\bar{t}$ cross section and the distributions of the $t\bar{t}$ invariant mass, of the transverse top-quark momentum and rapidity, and of the cosine of the Collins-Soper angle with and without the two heavy Higgs resonances. For selected $M_{t\bar{t}}$ bins we estimate the significances for detecting a heavy Higgs signal in the $t\bar{t}$ dileptonic and lepton plus jets decay channels., Comment: 54 pages, 23 figures, v2: typos corrected, minor stylistic changes, matches published version
- Published
- 2016
25. Heavy Higgs boson production and decay into top quarks at the LHC
- Author
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Peter Galler, Clemens Mellein, Werner Bernreuther, Zong-Guo Si, and Peter Uwer
- Subjects
Quantum chromodynamics ,Physics ,Quark ,Particle physics ,Large Hadron Collider ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Resonance (particle physics) ,Standard Model ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Higgs boson ,High Energy Physics::Experiment ,QC ,Spin-½ ,Boson - Abstract
In this contribution we report on the calculation of the next-to-leading order (NLO) QCD corrections to the hadro-production of heavy neutral Higgs bosons and their decay into top-quark pairs within the type-II two-Higgs-doublet extension of the standard model (SM). We take into account the contributions from resonant Higgs boson production, the non-resonant SM $t\bar{t}$ background as well as the interference of these two contributions. The NLO corrections to the signal and interference contributions are calculated by applying the heavy top-quark mass ($m_t$) limit including an effective rescaling. In our NLO calculation the QCD-Higgs interference is evaluated in the resonance region that provides the dominant part of the heavy Higgs-boson contributions. Evaluating representative $CP$-conserving and $CP$-violating parameter scenarios within the two-Higgs-doublet model (2HDM) we present results for different distributions and, in addition, for observables that depend on the top-quark spin., Comment: 6 pages, 2 figures, contribution to the proceedings of the 38th International Conference on High Energy Physics, 3-10 August 2016, Chicago, USA
- Published
- 2016
- Full Text
- View/download PDF
26. Z′ particles and e + e − → τ +µ−
- Author
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Tai-Fu Feng, Tie-Jun Gao, Zong-Guo Si, Shu-Min Zhao, and Xue-Qian Li
- Subjects
Nuclear physics ,Physics ,Tree (descriptive set theory) ,Particle physics ,Cross section (physics) ,High Energy Physics::Phenomenology ,General Physics and Astronomy ,High Energy Physics::Experiment ,Extension (predicate logic) ,Neutrino ,Lepton - Abstract
We analyze the cross section of e+e− → τ+µ− within the frameworks of SM and its Z′ extension. The theoretical prediction of the SM on the total cross section is suppressed by the tiny neutrino masses. On the other hand, the contributions from Z′ to the cross section are enhanced drastically because of the tree level FCNC couplings among Z′ and leptons.
- Published
- 2010
27. Distributions and correlations for top quark pair production and decay at the Tevatron and LHC
- Author
-
Werner Bernreuther and Zong-Guo Si
- Subjects
Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Top quark ,Particle physics ,Large Hadron Collider ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Tevatron ,FOS: Physical sciences ,Asymmetry ,Helicity ,Nuclear physics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Pair production ,CP violation ,High Energy Physics::Experiment ,media_common - Abstract
We investigate a number of observables that are and will be instrumental in the exploration of $\tbart$ production and decay at the Tevatron and the LHC. For this analysis we made a computer program that incorporates besides the NLO QCD corrections to $\tbart$ production and decay also mixed weak-QCD corrections to the production amplitudes, and that allows for studies of correlated versus uncorrelated $\tbart$ events. In this paper we analyze and compute observables mostly for dileptonic $\tbart$ final states to next-to-leading order in the strong and weak gauge couplings (NLOW), with selection cuts. We calculate charge asymmetries of the top quark and of $\ell=e,\mu$ and we compare, where possible, with experimental results. We show that top-quark spin correlations affect a leptonic pair asymmetry (which has not been measured so far) by $\sim 7%$. We determine several dileptonic angular correlations, which reflect $\tbart$ spin correlations, namely the beam, off-diagonal and helicity correlation, and the opening angle distribution (defined in the $t$, $\bar t$ rest frames) when selection cuts are applied. Our NLOW predictions for the beam, off-diagonal, and helicity correlation for the Tevatron agree with recent measurements by the CDF and D0 experiments. In addition we make predictions for estimators of these correlations as functions of $\mtt$. These estimators may prove useful for the Tevatron and also in the early rounds of LHC data-analyses, where the event numbers will probably not be abundant. Furthermore, we compute to NLOW in the gauge couplings two dilepton angular correlations that are defined in the laboratory frame, for correlated and uncorrelated $\tbart$ events at the LHC. Finally, based on our SM results, we identify several observables that allow to search for non-standard parity- and CP-violating interactions, especially with future LHC data., Comment: Latex, 39 pages, 39 figures, 4 tables
- Published
- 2010
28. Search for W′ signal in single top quark production at the LHC
- Author
-
Zhong-Juan Yang, Fei Huang, Hong-Lei Li, Wei Su, Shi-Yuan Li, and Zong-Guo Si
- Subjects
Physics ,Nuclear and High Energy Physics ,Top quark ,Gauge boson ,Particle physics ,Missing energy ,Large Hadron Collider ,010308 nuclear & particles physics ,Physics beyond the Standard Model ,High Energy Physics::Phenomenology ,Astronomy and Astrophysics ,Observable ,01 natural sciences ,Standard Model ,0103 physical sciences ,High Energy Physics::Experiment ,010306 general physics ,Instrumentation ,Lepton - Abstract
Heavy charged gauge bosons are proposed in some theories beyond the standard model. We explore the discovery potential for W' -> t (b) over bar with top quark semi-leptonic decay at the LHC. We concentrate on the new physics signal search with the deviation from the standard model prediction if the resonance peak of W' cannot be observed directly. Signal events with two jets plus one charged lepton and missing energy are simulated, together with the dominant standard model backgrounds. In this paper, it is found that suitable cuts on the kinematic observables can effectively suppress the standard model backgrounds, so that it is possible to search for a W' signal at the LHC if its mass is less than 6.6 TeV.
- Published
- 2018
29. Testing the realistic seesaw model with two heavy Majorana neutrinos at the CERN Large Hadron Collider
- Author
-
Shun Zhou, Ya-juan Zheng, Wei Chao, and Zong-Guo Si
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Sterile neutrino ,Large Hadron Collider ,High Energy Physics::Phenomenology ,Pontecorvo–Maki–Nakagawa–Sakata matrix ,FOS: Physical sciences ,Lepton number ,Nuclear physics ,High Energy Physics - Phenomenology ,MAJORANA ,High Energy Physics - Phenomenology (hep-ph) ,Seesaw molecular geometry ,Higgs boson ,High Energy Physics::Experiment ,Neutrino - Abstract
In the conventional type-(I+II) seesaw model, the effective mass matrix of three known light neutrinos is given by M_nu = M_L - M_D M^{-1}_R M^T_D in the leading-order approximation. We propose an intriguing scenario, in which the structural cancellation condition M_D M^{-1}_R M^T_D = 0 is guaranteed by the A_4 x Z_2 flavor symmetry. As a consequence, neutrino masses are mainly generated by the Higgs triplet M_nu = M_L, while the neutrino mixing matrix is non-unitary and takes on the nearly tri-bimaximal pattern. A discriminating feature of this scenario from the pure type-II seesaw model is that the lepton-number-violating signatures induced by the heavy Majorana neutrinos can be discovered at the CERN Large Hadron Collider. We calculate the total cross section of the same-sign dilepton events pp to l^+(-)_alpha N_i to l^+(-)_alpha l^+(-)_beta jj (for i=1, 2 and alpha, beta = e, mu, tau), and emphasize the significant interference of the contributions from two different heavy Majorana neutrinos. The background from the standard model and the kinematic cuts used to reduce it have been considered. The possible way to distinguish between the signals from heavy Majorana neutrinos and those from doubly-charged Higgs bosons is briefly discussed., Comment: 18 pages, 3 figures, discussions about the SM background added, references updated. Accepted for publication in Phys. Lett. B
- Published
- 2010
30. Broken S 3L × S 3R flavor symmetry and leptonic CP violation
- Author
-
Xing-Hua Yang, Shun Zhou, and Zong-Guo Si
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Physics beyond the Standard Model ,Astronomy and Astrophysics ,01 natural sciences ,Symmetry (physics) ,Leptogenesis ,0103 physical sciences ,CP violation ,010306 general physics ,Neutrino oscillation ,Instrumentation ,Flavor - Published
- 2017
31. Unparticle Effects on Top Quark Pair Production at Photon Collider
- Author
-
Zhong-Juan Yang, Hai-Feng Li, Hong-Lei Li, and Zong-Guo Si
- Subjects
Physics ,Top quark ,Particle physics ,Photon ,Physics and Astronomy (miscellaneous) ,Scalar (mathematics) ,Unparticle physics ,FOS: Physical sciences ,law.invention ,Standard Model ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Pair production ,law ,High Energy Physics::Experiment ,Invariant mass ,Collider - Abstract
The unparticle effects on $t\bar t$ production at the future photon collider are investigated. Distributions of $t\bar t$ 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 $d_{\U}$, 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 $t \bar t$ production at photon collider if it exists., 13 pages, 5figures
- Published
- 2009
32. Doubly heavy baryon production at γγ collider
- Author
-
Zong-Guo Si, Shi-Yuan Li, and Zhong-Juan Yang
- Subjects
Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,High Energy Physics::Phenomenology ,Xi baryon ,law.invention ,Nuclear physics ,Baryon ,law ,Heavy quark effective theory ,Baryon number ,Nuclear Experiment ,Collider - Abstract
The inclusive production of doubly heavy baryons Ξ c c and Ξ b b at γγ collider is investigated. It is found that the contribution from the heavy quark pair QQ in color triplet and color sextet are important.
- Published
- 2007
33. Associated Production of Higgs Boson and $t\bar t$ at LHC
- Author
-
Peng-Cheng Lu, Zong-Guo Si, Hong-Lei Li, and Ying Wang
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Top quark ,Large Hadron Collider ,010308 nuclear & particles physics ,Physics beyond the Standard Model ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,Scalar (physics) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Yukawa interaction ,01 natural sciences ,Higgs sector ,Pseudoscalar ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Higgs boson ,High Energy Physics::Experiment ,010306 general physics ,Instrumentation - Abstract
One of the future goals of the LHC is to precisely measure the properties of Higgs boson. The associated production of Higgs boson and the top quark pair is a promising process to investigate the related Yukawa interaction and the properties of Higgs. Compared with the pure scalar sector in the Standard Model, the Higgs sector contains both scalar and pseudoscalar in many new physics models, which makes the $t\bar t H$ interaction more complex and provides a variety of phenomena. To investigate the $t\bar t H$ interaction and the properties of Higgs, we study the top quark spin correlation observables at the LHC.
- Published
- 2015
34. Predictions for the Top-Quark Forward-Backward Asymmetry at High Invariant Pair Mass Using the Principle of Maximum Conformality
- Author
-
Sheng Quan Wang, Zong-Guo Si, Xing-Gang Wu, and Stanley J. Brodsky
- Subjects
Quantum chromodynamics ,Quark ,Physics ,Particle physics ,Top quark ,010308 nuclear & particles physics ,media_common.quotation_subject ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Renormalization group ,01 natural sciences ,Asymmetry ,High Energy Physics - Experiment ,Renormalization ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Invariant mass ,High Energy Physics::Experiment ,Abelian group ,010306 general physics ,media_common - Abstract
The D0 collaboration at FermiLab has recently measured the top-quark pair forward-backward asymmetry in $\bar p p \to t \bar{t} X$ reactions as a function of the $t\bar{t} $ invariant mass $M_{t\bar{t}}$. The D0 result for $A_{\rm FB}(M_{t\bar{t}}>650\, {\rm GeV})$ is smaller than $A_{\rm FB}(M_{t\bar{t}})$ obtained for small values of $M_{t\bar{t}}$, which may indicate an "increasing-decreasing" behavior for $A_{\rm FB}(M_{t\bar{t}}>M_{\rm cut})$. This behavior is not explained using conventional renormalization scale-setting, even by a next-to-next-to-leading order (N$^2$LO) QCD calculation -- one predicts a monotonically increasing behavior. In the conventional scale-setting method, one simply guesses a single renormalization scale $��_r$ for the argument of the QCD running coupling and then varies it over an arbitrary range. However, the conventional method has inherent difficulties. ...... In contrast, if one fixes the scale using the Principle of Maximum Conformality (PMC), the resulting pQCD predictions are renormalization-scheme independent since all of the scheme-dependent $\{��_i\}$-terms in the QCD perturbative series are resummed into the QCD running couplings at each order. ...... In this paper we show that if one applies the PMC to determine the top versus anti-top quark forward-backward asymmetry by properly using the pQCD predictions up to N$^2$LO level, one obtains the predictions without renormalization scheme or scale ambiguities. ...... In addition, the PMC prediction for $A_{\rm FB}(M_{t\bar{t}}> M_{\rm cut})$ shows an "increasing-decreasing" behavior for increasing values of $M_{\rm cut}$ which is not observed in the NLO and N$^2$LO predictions for $A_{\rm FB}(M_{t\bar{t}}> M_{\rm cut})$ with conventional scale-setting. This behavior could be tested by the future more precise measurements at the LHC., 7 pages, 2 figures. Revised version to be published in Phys.Rev.D
- Published
- 2015
35. Studying color connection effects ofe+e−→cc¯cc¯→Ξcc+Xprocess within quark combination model
- Author
-
Tao Yao, Hui Li, Yi Jin, Zong-Guo Si, Shi-Yuan Li, and X. F. Zhang
- Subjects
Quantum chromodynamics ,Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Phenomenology ,Hadron ,Lund string model ,Parton ,Hadronization ,Baryon ,High Energy Physics::Experiment ,Tetraquark ,Nuclear Experiment - Abstract
The color connection of the parton system is an important bridge to connect the perturbative process and the hadronization one. The special color connection of four-heavy-quark system in e + e annihilation, which is the necessary one for the doubly heavy baryon and tetraquark productions is revisited. The hadronization effects, investigated with the help of the Quark Combination Model are compared with the corresponding results employing the Lund String Model in our previous work. The global properties related to a certain color connection are not sensitive to various hadronization models. In high energy collisions, hadronization is one of the most important processes for understanding the nonperturbative quantum chromodynamics and the confinement mechanism. e + e − annihilation has the advantage that the hadronization results can be compared with the experimental data directly to extract informations of hadronization because of no hadrons in the initial states. To embed the parton system into a hadronization model, it is necessary to specify the concrete color connection. However, the color connection for multi-parton system is not unique. Some clues can be obtained by analyzing the decomposition of the color space of the final partons [1– 5]. One of the interesting and important examples is the four-heavy-quark system (QQ ′ ¯ Q ¯
- Published
- 2015
36. A set of top quark spin correlation and polarization observables for the LHC: Standard Model predictions and new physics contributions
- Author
-
Dennis Heisler, Zong-Guo Si, and Werner Bernreuther
- Subjects
Quantum chromodynamics ,Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,Top quark ,Large Hadron Collider ,High Energy Physics::Lattice ,Physics beyond the Standard Model ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Hadron ,FOS: Physical sciences ,Asymmetry ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,ddc:530 ,High Energy Physics::Experiment ,media_common ,Lepton - Abstract
We consider top-antitop quark ($t{\bar t}$) production at the Large Hadron Collider (LHC) with subsequent decay into dileptonic and lepton plus jets final states. We present a set of leptonic angular correlations and distributions with which experiments can probe all the independent coefficient functions of the top-spin dependent parts of the $t{\bar t}$ production spin density matrices. We compute these angular correlations and distributions for LHC center-of-mass energies 8, 13, and 14 TeV within the Standard Model at next-to-leading order in the QCD coupling including the mixed QCD-weak corrections and for the transverse top-quark polarization and the $t{\bar t}$ charge asymmetry also the mixed QCD-QED corrections. In addition we analyze and compute the effects of new interactions on these observables in terms of a gauge-invariant effective Lagrangian which contains all operators relevant for hadronic $t{\bar t}$ production up to mass dimension six., Latex, 35 pages, sevaral comments and 2 tables added, version to be published in JHEP
- Published
- 2015
- Full Text
- View/download PDF
37. Colour connection and diquark fragmentation in e+e−→cc¯qq¯→h′s process
- Author
-
Zong-Guo Si, Wei Han, Zhong-Juan Yang, and Shi-Yuan Li
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Annihilation ,Toy model ,Nuclear Theory ,High Energy Physics::Phenomenology ,Hadronization ,Nuclear physics ,Baryon ,Diquark ,Charmed baryons ,Fragmentation (mass spectrometry) ,High Energy Physics::Experiment ,Nuclear Experiment ,s-process - Abstract
The hadronization effects induced by different colour connections of c c ¯ q q ¯ system in e + e − annihilation are investigated by a toy model where diquark fragmentation is employed based on Pythia. It is found that the correlations between the charm baryons and charm antibaryons produced via diquark pair fragmentation are much stronger, and their momentum spectra are harder than those from the standard colour connection in Pythia.
- Published
- 2006
38. MIXED QCD AND WEAK CORRECTIONS TO $t\bar{t}$ PRODUCTION BY QUARK-ANTIQUARK ANNIHILATION
- Author
-
Zong-Guo Si, M. Fücker, and Werner Bernreuther
- Subjects
Quantum chromodynamics ,Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,Annihilation ,Bar (music) ,Computation ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Astronomy and Astrophysics ,Atomic and Molecular Physics, and Optics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Condensed Matter::Strongly Correlated Electrons ,High Energy Physics::Experiment ,Production (computer science) ,Spin-½ - Abstract
We report on our computation of the mixed QCD and weak corrections to $q {\bar q} \to t\bar{t}$ including $t, \bar t$ spin effects, in particular on single top spin asymmetries., Talk given at "International Conference on QCD and Hadronic Physics", Beijing, China, 16-20 Jun 2005
- Published
- 2006
39. Application of the Principle of Maximum Conformality to the Top-Quark Charge Asymmetry at the LHC
- Author
-
Stanley J. Brodsky, Zong-Guo Si, Sheng-Quan Wang, and Xing-Gang Wu
- Subjects
Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Top quark ,Particle physics ,Large Hadron Collider ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Tevatron ,FOS: Physical sciences ,Asymmetry ,Statistics::Computation ,High Energy Physics - Experiment ,Renormalization ,Nuclear physics ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Pair production ,High Energy Physics::Experiment ,Invariant mass ,media_common - Abstract
The Principle of Maximum Conformality (PMC) provides a systematic and process-independent method to derive renormalization scheme- and scale- independent fixed-order pQCD predictions. In Ref.\cite{pmc3}, we studied the top-quark charge asymmetry at the Tevatron. By applying the PMC, we have shown that the large discrepancies for the top-quark charge asymmetry between the Standard Model estimate and the CDF and D0 data are greatly reduced. In the present paper, with the help of the Bernreuther-Si program, we present a detailed PMC analysis on the top-quark pair production up to next-to-next-to-leading order level at the LHC. After applying PMC scale setting, the pQCD prediction for the top-quark charge asymmetry at the LHC has very small scale uncertainty; e.g., $A_{\rm C}|_{\rm 7 TeV;PMC} =\left(1.15^{+0.01}_{-0.03}\right)\%$, $A_{\rm C}|_{\rm 8 TeV;PMC} =\left(1.03^{+0.01}_{+0.00}\right)\%$, and $A_{\rm C}|_{\rm 14 TeV;PMC} =\left(0.62^{+0.00}_{-0.02}\right)\%$. The corresponding predictions using conventional scale setting are: $A_{\rm C}|_{\rm 7 TeV;Conv.} =\left(1.23^{+0.14}_{-0.14}\right)\%$, $A_{\rm C}|_{\rm 8 TeV;Conv.} =\left(1.11^{+0.17}_{-0.13}\right)\%$, and $A_{\rm C}|_{\rm 14 TeV;Conv.} =\left(0.67^{+0.05}_{-0.05}\right)\%$. In these predictions, the scale errors are predicted by varying the initial renormalization and factorization scales in the ranges $\mu^{\rm init}_r\in[m_t/2,2m_t]$ and $\mu_f\in[m_t/2,2m_t]$. The PMC predictions are also in better agreement with the available ATLAS and CMS data. In addition, we have calculated the top-quark charge asymmetry assuming several typical cuts on the top-pair invariant mass $M_{t\bar{t}}$. For example, assuming $M_{t\bar{t}}>0.5 ~ {\rm TeV}$ and $\mu_f=\mu^{\rm init}_r =m_t$, we obtain $A_{\rm C}|_{\rm 7 TeV;PMC}=2.67\%$, $A_{\rm C}|_{\rm 8 TeV;PMC}=2.39\%$, and $A_{\rm C}|_{\rm 14 TeV;PMC}=1.28\%$., Comment: 10 pages, 4 figures. Discussion improved
- Published
- 2014
40. Top quark pair production and decay at hadron colliders
- Author
-
Werner Bernreuther, Peter Uwer, Zong-Guo Si, and A. Brandenburg
- Subjects
Physics ,Quark ,Nuclear and High Energy Physics ,Top quark ,Particle physics ,High Energy Physics::Lattice ,Nuclear Theory ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Top quark condensate ,Omega baryon ,Lambda baryon ,Bottom quark ,Standard Model ,Sigma baryon ,Nuclear physics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics::Experiment ,Particle Physics - Phenomenology - Abstract
In ongoing and upcoming hadron collider experiments, top quark physics will play an important role in testing the Standard Model and its possible extensions. In this work we present analytic results for the differential cross sections of top quark pair production in hadronic collisions at next-to-leading order in the QCD coupling, keeping the full dependence on the spins of the top quarks. These results are combined with the corresponding next-to-leading order results for the decay of polarized top quarks into dilepton, lepton plus jets, and all jets final states. As an application we predict double differential angular distributions which are due to the QCD-induced top quark spin correlations in the intermediate state. In addition to the analytic results, we give numerical results in terms of fit functions that can easily be used in an experimental analysis., Comment: 58 pages, 12 figures
- Published
- 2004
41. QCD-corrected spin analysing power of jets in decays of polarized top quarks
- Author
-
Zong-Guo Si, Peter Uwer, and A. Brandenburg
- Subjects
Quantum chromodynamics ,Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,Top quark ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,Thrust ,Polarization (waves) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Physics::Atomic and Molecular Clusters ,Radiative transfer ,High Energy Physics::Experiment - Abstract
We present results for the differential distributions of jets from non-leptonic decays of polarized top quarks within the Standard Model, including QCD radiative corrections. Our work extends existing results which are only available for semileptonic top quark decays at the parton level. For $t(\uparrow)$ -> b-jet + 2 light jets we compute in particular the QCD-corrected top-spin analysing power of the b-quark jet and the least energetic light jet. The dependence of the results on the choice of the jet recombination scheme is found to be small. In addition we compute the spin analysing power of the thrust axis. Our results constitute a so far missing ingredient to analyse top quark production and subsequent non-leptonic decay at next-to-leading order in alpha_s, keeping the full information on the top quark polarization., 11 pages
- Published
- 2002
42. Search for a doubly charmed hadron atBfactories
- Author
-
Shi-Yuan Li, Zong-Guo Si, Yi Jin, Yan-Rui Liu, and Tao Yao
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Phenomenology ,Hadron ,Lambda ,Hadronization ,B-factory ,Nuclear physics ,Mass spectrum ,High Energy Physics::Experiment ,Production (computer science) ,Nuclear Experiment ,Event (particle physics) - Abstract
The doubly charmed hadron production at B factories is of special importance for the study of the hadron structure and the color connections before hadronization. To suppress the combination background fluctuations of the reconstructed hadron mass spectra, we suggest a three-jet event shape trigger. After these three jets are identified by their energy and angular distributions, it is found that: 1) The background process $e^+ e^- \to c\bar {c} \to h's$ in consideration of the final hadron system $\Lambda_c^+K^-\pi^+ +X$ are significantly suppressed. 2) For the selected events, about half of the particles, $\Lambda_c^+$, $K^-$, $\pi^+$, which obviously can not belong to the decay products of doubly charmed hadron, can be vetoed. The relevant hadronization is investigated.
- Published
- 2014
43. Search forW′signal viatW′associated production at the LHC
- Author
-
Hong-Lei Li, Cong-Feng Qiao, Zhong-Juan Yang, Zong-Guo Si, and Xue Gong
- Subjects
Quark ,Physics ,Nuclear and High Energy Physics ,Gauge boson ,Particle physics ,Top quark ,Large Hadron Collider ,Physics beyond the Standard Model ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Asymmetry ,Standard Model ,Nuclear physics ,High Energy Physics::Experiment ,Lepton ,media_common - Abstract
A variety of new physics models predict the existence of extra charged gauge bosons ( W ′ ). It is verified that W ′ and top quark associated production is a promising process to search for the W ′ signal at the LHC. We study the collider signatures of multijets + lepton + E T by reconstructing the t W ′ intermediate state through the decay modes of W ′ → t b , W ′ → q q ¯ ′ , and W ′ → l ν , respectively. An angular distribution related to charged lepton and top quark moving direction is provided to distinguish alternative left-handed or right-handed chiral couplings of W ′ to quarks in the hadronic decay modes. The superiority on the search of W ′ is demonstrated in the leptonic decay channel for the left-handed type interaction, which is forbidden for the right-handed type interaction in the most theories. To be more realistic, the relevant standard model backgrounds are simulated. We adopt various kinematic cuts to suppress the backgrounds and collect the integral luminosity needed for the corresponding process detected at the LHC with 3 σ sensitivity. We also provide a forward-backward asymmetry which is related to the chirality of W ′ . The successive studies can shed light on the potential searching for the W ′ signal as well as distinguishing typical new physics models.
- Published
- 2014
44. Light Top Squark in Precision Top Quark Sample
- Author
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Guohuai Zhu, Liucheng Wang, Liangliang Zhang, Kai Wang, Zong-Guo Si, and Xue-Qian Li
- Subjects
Physics ,Left handed ,Nuclear and High Energy Physics ,Particle physics ,Top quark ,Large Hadron Collider ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Nuclear physics ,High Energy Physics - Phenomenology ,Pair production ,High Energy Physics - Phenomenology (hep-ph) ,Statistical analysis ,High Energy Physics::Experiment - Abstract
The uncertainty of $t\bar{t}$ production cross section measurement at LHC is at a-few-percent level which still allows the stop pair production $\tilde{t}\tilde{t}^{*}$ with identical final states $2b+\ell+nj+{E}_{T}$. In this paper, we attempt to use the existing measurement of $W$-polarization in top quark decay to improve the distinction between stop and top quark states. We apply the ATLAS $\chi^2$ method of $W$-polarization measurement in semi-leptonic $t\bar{t}$ final state to semi-leptonic stop pair samples and study its prediction. We find that the faked top events from stop mostly contribute to the left-handed polarized $W$ due to the reconstruction. The benchmark point with maximal contribution to top events only changes $F_{L}$ by 1%. After comparing with the current experiments, we conclude that the current measurement of $W$-polarization in $t$ decay cannot exclude the light stop scenario., Comment: 5 pages, 7 figures, a short version, conclusion unchanged, reference added
- Published
- 2013
45. Next-to-leading order QCD corrections to top quark spin correlations at hadron colliders: the reactions
- Author
-
W. Bernreuther, A. Brandenburg, and Zong-Guo Si
- Subjects
Physics ,Quantum chromodynamics ,Quark ,Nuclear and High Energy Physics ,Top quark ,Particle physics ,Annihilation ,Large Hadron Collider ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,Hadron ,Tevatron ,Quantization (physics) ,Condensed Matter::Strongly Correlated Electrons ,High Energy Physics::Experiment - Abstract
Future hadron collider experiments are expected to record large to huge samples of $t\bar t$ events. The analysis of these data with respect to $t\bar t$ spin-spin correlations requires precise predictions of the production of these quark pairs in a general spin configuration. Therefore we have computed, at next-to-leading order (NLO) in the QCD coupling, the spin density matrices describing $t\bar t$ production by quark antiquark annihilation, which is the dominant production process at the Tevatron. Moreover we have computed the strength of the $t\bar t$ spin correlation at NLO, using various spin quantization axes.
- Published
- 2000
46. Fourth generation Majorana neutrino, dark matter and Higgs physics
- Author
-
Yu-Feng Zhou, Zong-Guo Si, Shou-Shan Bao, and Xue Gong
- Subjects
Physics ,Quark ,High Energy Astrophysical Phenomena (astro-ph.HE) ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,Dark matter ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Astronomy and Astrophysics ,Fermion ,Atomic and Molecular Physics, and Optics ,Standard Model ,MAJORANA ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Higgs boson ,High Energy Physics::Experiment ,Neutrino ,Astrophysics - High Energy Astrophysical Phenomena - Abstract
We consider extensions of the standard model with fourth generation fermions (SM4) in which extra symmetries are introduced such that the transitions between the fourth generation fermions and the ones in the first three generations are forbidden. In these models, the stringent lower bounds on the masses of fourth generation quarks from direct searches are relaxed, and the lightest fourth neutrino is allowed to be stable and light enough to trigger the Higgs boson invisible decay. In addition, the fourth Majorana neutrino can be a subdominant but highly detectable dark matter component. We perform a global analysis of the current LHC data on the Higgs production and decay in this type of SM4. The results show that the mass of the lightest fourth Majorana neutrino is confined in the range $\sim 41-59$ GeV. Within the allowed parameter space, the predicted effective cross-section for spin-independent DM-nucleus scattering is $\sim 3\times 10^{-48}-6\times 10^{-46} \text{cm}^{2}$, which is close to the current Xenon100 upper limit and is within the reach of the Xenon1T experiment in the near future. The predicted spin-dependent cross sections can also reach $\sim 8\times 10^{-40}\text{cm}^{2}$., arXiv admin note: substantial text overlap with arXiv:1110.2930
- Published
- 2013
47. Search forZ′viaZHassociated production at the LHC
- Author
-
Zhong-Juan Yang, Ya-Juan Zheng, Xiu-Yi Yang, Hong-Lei Li, and Zong-Guo Si
- Subjects
Physics ,Quark ,Nuclear and High Energy Physics ,Gauge boson ,Particle physics ,Large Hadron Collider ,High Energy Physics::Lattice ,Physics beyond the Standard Model ,High Energy Physics::Phenomenology ,Higgs boson ,High Energy Physics::Experiment ,Lepton ,Boson - Abstract
Many new physics models predict the existence of extra neutral gauge bosons ($Z'$). Inspired by the recent development on Higgs search, we study the properties of $Z'$ via the Higgs and $Z$ boson associated production. The couplings of $Z'$ to quarks can be investigated through $pp \to Z'\to ZH\to l^+l^-b \bar b$ process, which also provides extraordinary signal for understanding the properties of $Z'ZH$ interaction. The standard model background processes can be significantly suppressed by adopting appropriate kinematic cuts. The charged lepton angular distributions are related to the ratio of chiral couplings of $Z'$ to quarks via $Z'ZH$ interaction.
- Published
- 2013
48. Publisher’s Note: Lepton number violation andW′chiral couplings at the LHC [Phys. Rev. D87, 035011 (2013)]
- Author
-
Ian M. Lewis, Richard Ruiz, Tao Han, and Zong-Guo Si
- Subjects
Physics ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,Lepton number - Published
- 2013
49. Lepton number violation andW′chiral couplings at the LHC
- Author
-
Richard Ruiz, Ian M. Lewis, Zong-Guo Si, and Tao Han
- Subjects
Physics ,Quark ,Coupling ,Nuclear and High Energy Physics ,Gauge boson ,Particle physics ,Large Hadron Collider ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Lepton number ,High Energy Physics - Experiment ,Nuclear physics ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,MAJORANA ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics::Experiment ,Neutrino ,Nuclear Experiment ,Lepton - Abstract
We study the observability for a heavy Majorana neutrino N along with a new charged gauge boson W' at the LHC. We emphasize the complementarity of these two particles in their production and decay to unambiguously determine their properties. We show that the Majorana nature of N can be verified by the lepton-number violating like-sign dilepton process, and by polar and azimuthal angular distributions. The chirality of the W' coupling to leptons and to quarks can be determined by a polar angle distribution in the reconstructed frame and an azimuthal angle distribution., 44 pages, 17 Figures; v2 journal version
- Published
- 2013
50. Top quark spin correlations and polarization at the LHC: standard model predictions and effects of anomalous top chromo moments
- Author
-
Zong-Guo Si and Werner Bernreuther
- Subjects
Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Top quark ,Physics beyond the Standard Model ,media_common.quotation_subject ,High Energy Physics::Lattice ,Hadron ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Asymmetry ,Helicity ,High Energy Physics - Experiment ,Nuclear physics ,High Energy Physics - Phenomenology ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,CP violation ,High Energy Physics::Experiment ,Lepton ,media_common - Abstract
A number of top-spin observables are computed within the Standard Model (SM), at next-to-leading order in the strong and weak gauge couplings for hadronic top-quark anti-quark (ttbar) production and decay at the LHC for center-of-mass energies 7 and 8 TeV. For dileptonic final states we consider the azimuthal angle correlation, the helicity correlation, and the opening angle distribution; for lepton plus jets final states we determine distributions and asymmetries that trace a longitudinal and transverse polarization, respectively, of the t and t-bar samples. In addition, we investigate the effects of a non-zero chromo-magnetic and chromo-electric dipole moment of the top quark on these and other top-spin observables and associated asymmetries. These observables allow to disentangle the contributions from the real and imaginary parts of these moments., Comment: 22 pages, numbers of transverse top polarization corrected
- Published
- 2013
- Full Text
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