Mostrando 15,161 - 15,180 Resultados de 16,682 Para Buscar '"quarks"', tiempo de consulta: 0.26s Limitar resultados
  1. 15161
    por Ali, Ahmed, Braun, Vladimir M., Simma, H.
    Publicado 1994
    “…We give a detailed discussion of the dependence of the form factors on the $b$-quark mass and on the momentum transfer, as well as their interrelation with the CKM-suppressed semileptonic decay form factors in $B\to \rho+\ell+\nu$ which we also calculate in our approach.…”
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  2. 15162
    por Scheid, Horst Sebastian
    Publicado 2018
    “…Low-mass dielectron measurements play an essential role in the study of the Quark- Gluon Plasma (QGP) created in ultra-relativistic heavy-ion collisions. …”
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  3. 15163
    “…After defining physical (pole) top quark mass $M_t$, by including QCD self-energies, and physical Higgs mass $M_H$, by including the electroweak self-energies $\Pi\left(M_H~2\right)-\Pi(0)$, we obtain the upper limit on $M_H$ as a function of supersymmetric parameters. …”
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  4. 15164
    por Tripathy, Sushanta
    Publicado 2019
    “…Having different masses, quantum numbers and quark content, hadronic resonancesHadronic resonances carry a wealth of information on different aspects of ion-ion collisions, including the processes that determine the shapes of particle momentum spectra, insight into strangeness productionStrangeness production and collective effects in small collision systems. …”
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  5. 15165
    por Sas, Mike
    Publicado 2020
    “…The production of light neutral mesons in AA collisions probes the physics of the Quark-Gluon Plasma (QGP), which is formed in heavy-ion collisions at the LHC. …”
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  6. 15166
    por Guittière, Manuel
    Publicado 2020
    “…At the LHC collision energies, multiple parton interactions (MPI) are a key ingredient for particle production models including hard scale processes like heavy-quark production (charm and beauty). Quarkonium measurements in high-multiplicity proton-proton (pp) collisions can shed light on the role of MPI at such hard momentum scales, as well as on the interplay between hard and soft particle production mechanisms. …”
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  7. 15167
    “…We report the physics and computational performance of the MLPF algorithm on a Monte Carlo dataset of top quark–antiquark pairs produced in proton–proton collisions in conditions similar to those expected for the high-luminosity LHC. …”
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  8. 15168
    por Wolf, Anton
    Publicado 2021
    “…Within the minimal Buchmüller-Rückl-Wyler model and assuming a branching ratio for the decay into a charged lepton and a quark of 50%, leptoquarks with masses up to $1.20\ \text{TeV}$ are excluded with a confidence level of 95%. …”
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  9. 15169
    “…Therefore, leptons from heavy flavor quark is the major source of background. We closely follow a search for displaced electron plus muon search at CMS and study their control regions, which is related to our signal regions, in great detail to develop a robust estimation of the background for our signals. …”
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  10. 15170
    “…In this study, we employ a support vector machine with a quantum kernel estimator (QSVM-Kernel method) to a recent LHC flagship physics analysis: <math><mrow><mi>t</mi><mover accent="true"><mi>t</mi><mo>¯</mo></mover><mi>H</mi></mrow></math> (Higgs boson production in association with a top quark pair). In our quantum simulation study using up to 20 qubits and up to <math><mrow><mn>50</mn><mspace width="0.16em"/><mn>000</mn></mrow></math> events, the QSVM-Kernel method performs as well as its classical counterparts in three different platforms from Google Tensorflow Quantum, IBM Quantum, and Amazon Braket. …”
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  11. 15171
    “…Furthermore, it inextricably links the origin of the neutrino mass to the experimentally observed difference between the down-type quark and charged lepton masses. The main predictions of the model are that (i) the neutrinos are Majorana particles, (ii) one neutrino is massless, (iii) the neutrinos have normal mass ordering, and (iv) there are four new scalar multiplets at or below a 120 TeV mass scale. …”
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  12. 15172
    por Abdalla, E., Abdalla, M.C.B.
    Publicado 1995
    “…QCD_2 as a field theory 2.1 The 1/N expansion and spectrum, 2.2 Ambiguity in the self-energy of the quark, 2.3 Polyakov--Wiegmann formula and gauge interactions, 2.4 Strong coupling analysis, 2.5 A Lagrangian realization of the coset construction, 2.6 Chiral interactions. 3. …”
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  13. 15173
    por Li, Zhi
    Publicado 2022
    “…The Yukawa coupling between Higgs and top quark - which is the heaviest Standard Model (SM) fermion - is one of the most interesting constants which can be probed from the cross section measurement of associated production of a Higgs boson with a top-quark pair ($t\bar{t}H$). …”
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  14. 15174
    por Boroun, G R, Rezaei, B
    Publicado 2022
    “…The obtained results are comparable with others by considering the effect of the charm quark mass to the longitudinal structure function, which leads to rescaling the variable for nf=4. …”
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  15. 15175
    por The ALICE collaboration
    Publicado 2022
    “…These results and the corresponding comparisons with calculations of transport and statistical models address questions on the existence and properties of charmonium states in the quark–gluon plasma formed in nuclear collisions at the LHC.…”
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  16. 15176
    por Allanach, Ben, Davighi, Joe
    Publicado 2022
    “…This limit is rather loose, meaning that a good fit to data does not require ‘alignment’ in either quark Yukawa matrix. No curtailment of the s$_{L}$− b$_{L}$ mixing angle is evident in the S$_{3}$ model.…”
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  17. 15177
    “…We assess the potential of future electron-positron linear colliders operating in the $e^\pm\gamma$ mode in detecting charged Higgs bosons with mass around and larger than the top quark mass, using Compton back-scattered photons from laser light. …”
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  18. 15178
    por Ali, A., Parkhomenko, A.Ya.
    Publicado 2003
    “…We work in the approximation in which only one non-leading Gegenbauer moment for both the quark-antiquark and the gluonic light-cone distribution amplitudes for the $eta^prime$-meson is kept. …”
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  19. 15179
    por Feldmann, Thorsten, Hurth, Tobias
    Publicado 2004
    “…The latter vanish in the heavy-quark limit, $m_b \to \infty$, and are treated as unknown hadronic parameters. …”
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  20. 15180
    por Jadach, S., Skrzypek, M.
    Publicado 2005
    “…The type of the parton (quark, gluon) and the energy fraction x of the parton exiting emission chain (entering hard process) are predefined, i.e. constrained throughout the evolution. …”
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