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1,488 results on '"vector [resonance]"'

1. Magnetic field interference suppression method based on phase-compensation vector resonance control in near-zero magnetic field environment

Author: Wu, Haoting, Cui, Peiling, Tian, Pengtao, Zhang, Haifeng, and Zhao, Xiuqi
Published: 2025
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2. A direct current control strategy based on vector resonance controller for shunt active power filter

Author: Dongdong Chen, Zhenming Xu, Long Xiao, Wenduan Yan, and Yinbiao Guo
Subjects: Vector resonance, Active power filter(APF), Direct current control, Harmonics compensation, Electrical engineering. Electronics. Nuclear engineering, TK1-9971
Abstract: From the perspective of complex vector, this paper derives the mathematical model of the three-phase three-wire shunt active power filter (SAPF) current control object, and based on it, derives the corresponding vector resonance control expression form coordinate transformation, and the steady-state accuracy, anti-interference ability, and stability of the system are analyzed. The deduction demonstrates the equivalence of the traditional detection load harmonic current control and the direct grid current control in this paper, and the consistency of the current regulator. Then, a direct vector resonance control structure of grid current based on the dq coordinate without detecting harmonic currents is designed, and the digital realization of the vector resonance controller, the adaptive ability to frequency, and the phase lag at the high-order control frequency are designed. And finally experimental verification under different working conditions is presented, the experimental results prove the practicability and effectiveness of the direct current control strategy based on the vector resonance controller proposed in this paper.
Published: 2022
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3. Vector resonance $X_1(2900)$ and its structure

Author: Agaev, S. S., Azizi, K., and Sundu, H.
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment, High Energy Physics - Lattice
Abstract: The new vector resonance $X_1(2900)$ observed recently by LHCb in the $ D^{-}K^{+}$ invariant mass distribution in the decay $B^{+} \to D^{+}D^{-}K^{+}$ is studied to uncover internal structure of this state, and calculate its physical parameters. In the present paper, the resonance $ X_1(2900)$ is modeled as an exotic vector state, $ J^P=1^- $, built of the light diquark $u^{T}C\gamma_5d$ and heavy antidiquark $\overline{c} \gamma_{\mu}\gamma_5C\overline{s}^{T}$. The mass and current coupling of $ X_1(2900)$ are computed using the QCD two-point sum rule approach by taking into account various vacuum condensates up to dimension $10$. The width of the resonance $X_1(2900)$ is saturated by two decay channels $X_1 \to D^{-}K^{+}$ and $X_1 \to \overline{D}^{0}K^{0}$. The strong couplings $g_1$ and $g_2$ corresponding to the vertices $X_1D^{-}K^{+}$ and $X_1\overline{D} ^{0}K^{0}$ are evaluated in the context of the QCD light-cone sum rule method and technical tools of the soft-meson approximation. Results for the mass of the resonance $X_1(2900)$ $m=(2890~\pm 122)~\mathrm{MeV}$, and for its full width $\Gamma _{\mathrm{full}}=(93\pm 13)~\mathrm{MeV}$ are smaller than their experimental values reported by the LHCb collaboration. Nevertheless, by taking into account theoretical and experimental errors of investigations, interpretation of the state $X_1(2900)$ as the vector tetraquark does not contradict to the LHCb data. We also point out that analysis of the invariant mass distribution $D^{+}K^{+}$ in the same decay $ B^{+} \to D^{+}D^{-}K^{+}$ may reveal doubly charged four-quark structures $ [uc][\overline{s}\overline{d}]$., Comment: 8 Pages, 1 Figure and 1 Table
Published: 2021
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4. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at $\sqrt{s} = $ 13 TeV

Author: CMS Collaboration
Subjects: High Energy Physics - Experiment
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb$^{-1}$. Upper limits are derived on the production of a narrow heavy resonance Z', and a mass below 3.5 and 3.7 TeV is excluded at 95% confidence level in models where the heavy vector boson couples exclusively to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z' model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z' mass between 0.8 and 4.6 TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay., Comment: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at http://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-19-006 (CMS Public Pages)
Published: 2021
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5. On the transition form factors of the axial-vector resonance $f_1(1285)$ and its decay into $e^+e^-$

Author: Zanke, Marvin, Hoferichter, Martin, and Kubis, Bastian
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment, Nuclear Theory
Abstract: Estimating the contribution from axial-vector intermediate states to hadronic light-by-light scattering requires input on their transition form factors (TFFs). Due to the Landau-Yang theorem, any experiment sensitive to these TFFs needs to involve at least one virtual photon, which complicates their measurement. Phenomenologically, the situation is best for the $f_1(1285)$ resonance, for which information is available from $e^+e^-\to e^+e^- f_1$, $f_1\to 4\pi$, $f_1\to \rho \gamma$, $f_1\to \phi \gamma$, and $f_1\to e^+e^-$. We provide a comprehensive analysis of the $f_1$ TFFs in the framework of vector meson dominance, including short-distance constraints, to determine to which extent the three independent TFFs can be constrained from the available experimental input, a prerequisite for improved calculations of the axial-vector contribution to hadronic light-by-light scattering. In particular, we focus on the process $f_1\to e^+e^-$, evidence for which has been reported recently by SND for the first time, and discuss the impact that future improved measurements will have on the determination of the $f_1$ TFFs., Comment: 60 pages, 14 figures; v2: Appendix D on alternative $f_1 \to 4\pi$ mechanism added, references updated, version published in JHEP
Published: 2021
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6. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s=13Te

Author: Sirunyan, AM, Tumasyan, A, Adam, W, Bergauer, T, Dragicevic, M, Erö, J, Valle, A Escalante Del, Frühwirth, R, Jeitler, M, Krammer, N, Lechner, L, Liko, D, Mikulec, I, Pitters, FM, Rad, N, Schieck, J, Schöfbeck, R, Spanring, M, Templ, S, Waltenberger, W, Wulz, C-E, Zarucki, M, Chekhovsky, V, Litomin, A, Makarenko, V, Gonzalez, J Suarez, Darwish, MR, De Wolf, EA, Di Croce, D, Janssen, X, Kello, T, Lelek, A, Pieters, M, Sfar, H Rejeb, Van Haevermaet, H, Van Mechelen, P, Van Putte, S, Van Remortel, N, Blekman, F, Bols, ES, Chhibra, SS, D’Hondt, J, De Clercq, J, Lontkovskyi, D, Lowette, S, Marchesini, I, Moortgat, S, Morton, A, Müller, D, Python, Q, Tavernier, S, Van Doninck, W, Van Mulders, P, Beghin, D, Bilin, B, Clerbaux, B, De Lentdecker, G, Dorney, B, Favart, L, Grebenyuk, A, Kalsi, AK, Makarenko, I, Moureaux, L, Pétré, L, Popov, A, Postiau, N, Starling, E, Thomas, L, Vander Velde, C, Vanlaer, P, Vannerom, D, Wezenbeek, L, Cornelis, T, Dobur, D, Gruchala, M, Khvastunov, I, Niedziela, M, Roskas, C, Skovpen, K, Tytgat, M, Verbeke, W, Vermassen, B, Vit, M, Bruno, G, Bury, F, Caputo, C, David, P, Delaere, C, Delcourt, M, Donertas, IS, Giammanco, A, Lemaitre, V, Mondal, K, Prisciandaro, J, Taliercio, A, Teklishyn, M, Vischia, P, Wertz, S, Wuyckens, S, and Alves, GA
Subjects: CMS Collaboration, Atomic, Molecular, Nuclear, Particle and Plasma Physics, Quantum Physics, Nuclear & Particles Physics
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb-1 . Upper limits are derived on the production of a narrow heavy resonance Z' , and a mass below 3.5 and 3.7 Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z' model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z' mass between 0.8 and 4.6 Te , respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

7. Impact of a colored vector resonance on the collider constraints for top-like top partner

Author: Dasgupta, Sayan, Rai, Santosh Kumar, and Ray, Tirtha Sankar
Subjects: High Energy Physics - Phenomenology
Abstract: In this work we reappraise the collider constraints from leptonic final states on the vectorlike colored top partners taking into account the impact of exotic colored vector resonances. These colored states are intrinsic to a broad class of models that employ a strongly interacting sector to drive electroweak symmetry breaking. We translate the recent results in the {\sl monolepton + jets} channel as reported by CMS with an integrated luminosity of 35.8 fb$^{-1}$, and {\sl dilepton + jets} and {\sl trilepton + jets} channels as reported by ATLAS with an integrated luminosity of 36.1 fb$^{-1}$ to constrain the parameter space of these class of models. We also comment on the impact and modification of the derived constraints due to the expected fatness of the colored vector resonance, when accounted for beyond the narrow-width approximation by simulating the full one-particle irreducible resummed propagator., Comment: Extensive changes in text, Matches published version
Published: 2019
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8. Nature of the vector resonance $Y(2175)$

Author: Agaev, S. S., Azizi, K., and Sundu, H.
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment, High Energy Physics - Lattice
Abstract: Spectroscopic parameters and decay channels of the vector resonance $Y(2175)$ are studied by considering it as a diquark-antidiquark state with the quark content $su\overline{s}\overline{u}$. The mass and coupling of the tetraquark $Y(2175)$ are calculated using the QCD two-point sum rules by taking into account various quark, gluon and mixed condensates up to dimension 15. Partial widths of its strong decays to $\phi f_{0}(980)$, $ \phi \eta$, and $\phi \eta^{\prime}$ are computed as well. To this end, we explore the vertices $Y\phi f_{0}(980)$, $Y\phi \eta$, and $Y\phi \eta^{\prime}$, and calculate the corresponding strong couplings by means of the QCD light-cone sum rule method. The coupling $G_{Y\phi f}$ of the vertex $Y\phi f_{0}(980)$ is found using the full version of this method, and by treating the scalar meson $f_{0}(980)$ as a diquark-antidiquark tetraquark state. The couplings $g_{Y\phi \eta }$ and $g_{Y\phi \eta^{\prime}}$, however, are calculated by applying the soft-meson approximation to the light-cone sum rule method. Prediction for the mass of the resonance $m_{Y} =\left( 2173\pm 85\right)~\mathrm{MeV}$ is in excellent agreement with the data of the BaBar Collaboration \cite{Aubert:2006bu}, and within errors of calculations is compatible with the result reported by BESIII \cite {Ablikim:2014pfc}. The full width $\Gamma _{\mathrm{full}}=(91.1\pm 20.5)~ \mathrm{MeV}$ of the $Y(2175)$ saturated by its three strong decay channels is in a reasonable agreement with existing experimental data., Comment: 11 Pages, 4 Figures and 1 Table
Published: 2019
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9. A Dark Vector Resonance at CLIC

Author: Callender, Constanza and Zerwekh, Alfonso R.
Subjects: High Energy Physics - Phenomenology
Abstract: One of the main problems in Particle Physics is to understand the origin and nature of Dark Matter. An exciting possibility is to consider that the Dark Matter belongs to a new complex but hidden sector. In this paper, we assume the existence of a strongly interacting dark sector consisting on a new scalar doublet and new vector resonances, in concordance with a model recently proposed by our group. Since in a previous work it was found that it is very challenging to find the new vector resonances at the LHC, here we study the possibility of finding them at the a future Compact Linear Collider (CLIC) running at $\sqrt{s}=3$ TeV. We consider two distinct scenarios: when the non-standard scalars are heavy, the dark resonance is intense enough to make its discovery possible at CLIC when the resonance mass is in the range $[2000,3000]$ GeV. In the second scenario, when the non-standard scalars are light, the new vector boson is too broad to be recognized as a resonance and is not detectable except when the mass of the scalars is close to (but smaller than) a half of the resonance mass and the scale of the dark sector is high. In all the positive cases, less than a tenth of the maximum integrated luminosity is needed to reach the discovery level. Finally, we also comment about the mono-$Z$ production., Comment: Version accepted in the Chinese Journal C
Published: 2018
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10. Modelling top partner-vector resonance phenomenology

Author: Yepes, Juan and Zerwekh, Alfonso
Subjects: High Energy Physics - Phenomenology
Abstract: We have analysed the observable consequences of the interactions of spin-1 resonances coupled to the invariant fermionic currents that arise in an $SO(5)$ Composite Higgs set-up. The phenomenology entailed by such interactions is thoroughly analysed by studying heavy vector resonances production and decay modes in the viable resonance mass range. Additionally, the production of double and single-composite fermion final states has been scanned along the fermion mass scale. Such production is mediated by the SM gauge and Higgs interactions, and also by charged and neutral vector resonances. The coupling between the new fermions and vector resonances induces a sizeable effect in the production rates. We use the recent 13 TeV LHC searches for vector-like quarks to constrain our parameter space. Specifically, we explore the allowed regions by analysing the decays of a heavy vector-like quark in the $Wb$-channel. We conclude that generically the impact of the couplings between the spin-1 and spin-1/2 resonances will substantially reduce the permitted regions, leading us to test the sensitivity of the parametric dependence in the light of exotic matter interactions., Comment: 30 pages, 40 figures, references added and some sections shortened. arXiv admin note: text overlap with arXiv:1405.1617, arXiv:1211.5663 by other authors. References and footnotes added
Published: 2018
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11. An i2HDM Strongly Coupled to a non-Abelian Vector Resonance

Author: Rojas-Abatte, Felipe, Mora, Maria Luisa, Urbina, Jose, and Zerwekh, Alfonso R.
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment
Abstract: We study the possibility of a Dark Matter candidate having its origin in an extended Higgs sector which, at least partially, is related to a new strongly interacting sector. More concretely, we consider an i2HDM (i.e. a Type-I Two Higgs Doublet Model supplemented with a Z_2 under which the non-standard scalar doublet is odd) based on the gauge group SU(2)_1 x SU(2)_2 x U(1)_Y. We assume that one of the scalar doublets and the standard fermion transform non-trivially under SU(2)_1 while the second doublet transforms under SU(2)_2. Our main hypothesis is that standard sector is weakly coupled while the gauge interactions associated to the second group is characterized by a large coupling constant. We explore the consequences of this construction for the phenomenology of the Dark Matter candidate and we show that the presence of the new vector resonance reduces the relic density saturation region, compared to the usual i2DHM, in the high Dark Matter mass range. In the collider side, we argue that the mono-Z production is the channel which offers the best chances to manifest the presence of the new vector field. We study the departures from the usual i2HDM predictions and show that the discovery of the heavy vector at the LHC is challenging even in the mono-$Z$ channel since the typical cross sections are of the order of 10^{-2} fb.
Published: 2017
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12. The LHC mass limits for the $SU(2)_{L+R}$ vector resonance triplet of a strong extension of the Standard model

Author: Gintner, Mikulas and Juran, Josef
Subjects: High Energy Physics - Phenomenology
Abstract: In this paper, we derive the mass exclusion limits for the hypothetical vector resonances of a strongly interacting extension of the Standard model using the most recent upper bounds on the cross sections for various resonance production processes. The $SU(2)_{L+R}$ triplet of the vector resonances under consideration is embedded into the effective Lagrangian based on the non-linear sigma model with the $125$-GeV $SU(2)_{L+R}$ scalar singlet. No direct interactions of the vector resonance to the SM fermions are assumed. We find that among eleven processes considered in this paper only those where the vector resonances decay to $WW$ and $WZ$ provide the mass exclusion limit. Depending on the values of other parameters of the model the mass limit can be as low as 1 TeV., Comment: 14 pages, 7 figures
Published: 2017
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13. Modelling top partner-vector resonance phenomenology

Author: Yepes, Juan and Zerwekh, Alfonso
Published: 2019
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14. LHC vector resonance searches in the $t\bar{t} Z$ final state

Author: Backović, Mihailo, Flacke, Thomas, Jain, Bithika, and Lee, Seung J.
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment, 81T99, J.2
Abstract: LHC searches for BSM resonances in $l^+ l^-, \, jj, \, t\bar{t}, \gamma \gamma$ and $VV$ final states have so far not resulted in discovery of new physics. Current results set lower limits on mass scales of new physics resonances well into the $\mathcal{O}(1)$ TeV range, assuming that the new resonance decays dominantly to a pair of Standard Model particles. While the SM pair searches are a vital probe of possible new physics, it is important to re-examine the scope of new physics scenarios probed with such final states. Scenarios where new resonances decay dominantly to final states other than SM pairs, even though well theoretically motivated, lie beyond the scope of SM pair searches. In this paper we argue that LHC searches for (vector) resonances beyond two particle final states would be useful complementary probes of new physics scenarios. As an example, we consider a class of composite Higgs models, and identify specific model parameter points where the color singlet, electrically neutral vector resonance $\rho_0$ decays dominantly not to a pair of SM particles, but to a fermionic top partner $T_{f1}$ and a top quark, with $T_{f1} \rightarrow tZ$. We show that dominant decays of $\rho_0 \rightarrow T_{f1} t$ in the context of Composite Higgs models are possible even when the decay channel to a pair of $T_{f1}$ is kinematically open. Our analysis deals with scenarios where both $m_\rho$ and $m_{T_{f1}}$ are of $\mathcal{O}(1)$ TeV, leading to highly boosted $t\bar{t}Z$ final state topologies. We show that the particular composite Higgs scenario we consider is discoverable at the LHC13 with as little as 30 fb$^{-1}$, while being allowed by other existing experimental constraints., Comment: 37 pages, 6 figures, 9 tables. v2: typos corrected, Version published in JHEP
Published: 2016
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15. Tricking Landau-Yang: How to obtain the diphoton excess from a vector resonance

Author: Chala, Mikael, Duerr, Michael, Kahlhoefer, Felix, and Schmidt-Hoberg, Kai
Subjects: High Energy Physics - Phenomenology
Abstract: We show that contrary to naive expectations the recently observed diphoton excess can be explained by a vector resonance, which decays to a photon and a light scalar $s$, followed by a decay of the scalar into two photons: $Z' \rightarrow \gamma s \rightarrow 3 \gamma$. As the two photons from the scalar decay are highly boosted, the experimental signature is an apparent diphoton final state. In fact all the necessary ingredients are naturally present in $Z'$ models: Additional fermions with electroweak quantum numbers are required in order to render the theory anomaly free and naturally induce the required effective couplings, while the hidden Higgs which gives mass to the $Z'$ can be very light. In particular no new coloured states are required in this framework. We also show that in such a setup the width of the resonance can be rather large, while all couplings remain perturbative., Comment: 8 pages, 4 figures, 3 photons; v2: matches published version
Published: 2015
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16. Search for a heavy vector resonance decaying to a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson and a Higgs boson in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$ s = 13 Te

Author: A. M. Sirunyan, A. Tumasyan, W. Adam, T. Bergauer, M. Dragicevic, J. Erö, A. Escalante Del Valle, R. Frühwirth, M. Jeitler, N. Krammer, L. Lechner, D. Liko, I. Mikulec, F. M. Pitters, N. Rad, J. Schieck, R. Schöfbeck, M. Spanring, S. Templ, W. Waltenberger, C.-E. Wulz, M. Zarucki, V. Chekhovsky, A. Litomin, V. Makarenko, J. Suarez Gonzalez, M. R. Darwish, E. A. De Wolf, D. Di Croce, X. Janssen, T. Kello, A. Lelek, M. Pieters, H. Rejeb Sfar, H. Van Haevermaet, P. Van Mechelen, S. Van Putte, N. Van Remortel, F. Blekman, E. S. Bols, S. S. Chhibra, J. D’Hondt, J. De Clercq, D. Lontkovskyi, S. Lowette, I. Marchesini, S. Moortgat, A. Morton, D. Müller, Q. Python, S. Tavernier, W. Van Doninck, P. Van Mulders, D. Beghin, B. Bilin, B. Clerbaux, G. De Lentdecker, B. Dorney, L. Favart, A. Grebenyuk, A. K. Kalsi, I. Makarenko, L. Moureaux, L. Pétré, A. Popov, N. Postiau, E. Starling, L. Thomas, C. Vander Velde, P. Vanlaer, D. Vannerom, L. Wezenbeek, T. Cornelis, D. Dobur, M. Gruchala, I. Khvastunov, M. Niedziela, C. Roskas, K. Skovpen, M. Tytgat, W. Verbeke, B. Vermassen, M. Vit, G. Bruno, F. Bury, C. Caputo, P. David, C. Delaere, M. Delcourt, I. S. Donertas, A. Giammanco, V. Lemaitre, K. Mondal, J. Prisciandaro, A. Taliercio, M. Teklishyn, P. Vischia, S. Wertz, S. Wuyckens, G. A. Alves, C. Hensel, A. Moraes, W. L. Aldá Júnior, E. Belchior Batista Das Chagas, H. Brandao Malbouisson, W. Carvalho, J. Chinellato, E. Coelho, E. M. Da Costa, G. G. Da Silveira, D. De Jesus Damiao, S. Fonseca De Souza, J. Martins, D. Matos Figueiredo, M. Medina Jaime, C. Mora Herrera, L. Mundim, H. Nogima, P. Rebello Teles, L. J. Sanchez Rosas, A. Santoro, S. M. Silva Do Amaral, A. Sznajder, M. Thiel, F. Torres Da Silva De Araujo, A. Vilela Pereira, C. A. Bernardes, L. Calligaris, T. R. Fernandez Perez Tomei, E. M. Gregores, D. S. Lemos, P. G. Mercadante, S. F. Novaes, Sandra S. Padula, A. Aleksandrov, G. Antchev, I. Atanasov, R. Hadjiiska, P. Iaydjiev, M. Misheva, M. Rodozov, M. Shopova, G. Sultanov, A. Dimitrov, T. Ivanov, L. Litov, B. Pavlov, P. Petkov, A. Petrov, T. Cheng, W. Fang, Q. Guo, H. Wang, L. Yuan, M. Ahmad, G. Bauer, Z. Hu, Y. Wang, K. Yi, E. Chapon, G. M. Chen, H. S. Chen, M. Chen, T. Javaid, A. Kapoor, D. Leggat, H. Liao, Z.-A. Liu, R. Sharma, A. Spiezia, J. Tao, J. Thomas-wilsker, J. Wang, H. Zhang, S. Zhang, J. Zhao, A. Agapitos, Y. Ban, C. Chen, Q. Huang, A. Levin, Q. Li, M. Lu, X. Lyu, Y. Mao, S. J. Qian, D. Wang, Q. Wang, J. Xiao, Z. You, X. Gao, M. Xiao, C. Avila, A. Cabrera, C. Florez, J. Fraga, A. Sarkar, M. A. Segura Delgado, J. Jaramillo, J. Mejia Guisao, F. Ramirez, J. D. Ruiz Alvarez, C. A. Salazar González, N. Vanegas Arbelaez, D. Giljanovic, N. Godinovic, D. Lelas, I. Puljak, Z. Antunovic, M. Kovac, T. Sculac, V. Brigljevic, D. Ferencek, D. Majumder, M. Roguljic, A. Starodumov, T. Susa, M. W. Ather, A. Attikis, E. Erodotou, A. Ioannou, G. Kole, M. Kolosova, S. Konstantinou, J. Mousa, C. Nicolaou, F. Ptochos, P. A. Razis, H. Rykaczewski, H. Saka, D. Tsiakkouri, M. Finger, A. Kveton, J. Tomsa, E. Ayala, E. Carrera Jarrin, S. Abu Zeid, Y. Assran, E. Salama, A. Lotfy, M. A. Mahmoud, S. Bhowmik, A. Carvalho Antunes De Oliveira, R. K. Dewanjee, K. Ehataht, M. Kadastik, M. Raidal, C. Veelken, P. Eerola, L. Forthomme, H. Kirschenmann, K. Osterberg, M. Voutilainen, E. Brücken, F. Garcia, J. Havukainen, V. Karimäki, M. S. Kim, R. Kinnunen, T. Lampén, K. Lassila-Perini, S. Lehti, T. Lindén, H. Siikonen, E. Tuominen, J. Tuominiemi, P. Luukka, T. Tuuva, C. Amendola, M. Besancon, F. Couderc, M. Dejardin, D. Denegri, J. L. Faure, F. Ferri, S. Ganjour, A. Givernaud, P. Gras, G. Hamel de Monchenault, P. Jarry, B. Lenzi, E. Locci, J. Malcles, J. Rander, A. Rosowsky, M.Ö. Sahin, A. Savoy-Navarro, M. Titov, G. B. Yu, S. Ahuja, F. Beaudette, M. Bonanomi, A. Buchot Perraguin, P. Busson, C. Charlot, O. Davignon, B. Diab, G. Falmagne, R. Granier de Cassagnac, A. Hakimi, I. Kucher, A. Lobanov, C. Martin Perez, M. Nguyen, C. Ochando, P. Paganini, J. Rembser, R. Salerno, J. B. Sauvan, Y. Sirois, A. Zabi, A. Zghiche, J.-L. Agram, J. Andrea, D. Bloch, G. Bourgatte, J.-M. Brom, E. C. Chabert, C. Collard, J.-C. Fontaine, D. Gelé, U. Goerlach, C. Grimault, A.-C. Le Bihan, P. Van Hove, E. Asilar, S. Beauceron, C. Bernet, G. Boudoul, C. Camen, A. Carle, N. Chanon, D. Contardo, P. Depasse, H. El Mamouni, J. Fay, S. Gascon, M. Gouzevitch, B. Ille, Sa. Jain, I. B. Laktineh, H. Lattaud, A. Lesauvage, M. Lethuillier, L. Mirabito, K. Shchablo, L. Torterotot, G. Touquet, M. Vander Donckt, S. Viret, G. Adamov, Z. Tsamalaidze, L. Feld, K. Klein, M. Lipinski, D. Meuser, A. Pauls, M. Preuten, M. P. Rauch, J. Schulz, M. Teroerde, D. Eliseev, M. Erdmann, P. Fackeldey, B. Fischer, S. Ghosh, T. Hebbeker, K. Hoepfner, H. Keller, L. Mastrolorenzo, M. Merschmeyer, A. Meyer, G. Mocellin, S. Mondal, S. Mukherjee, D. Noll, A. Novak, T. Pook, A. Pozdnyakov, Y. Rath, H. Reithler, J. Roemer, A. Schmidt, S. C. Schuler, A. Sharma, S. Wiedenbeck, S. 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Goldstein, G. P. Heath, H. F. Heath, L. Kreczko, B. Krikler, S. Paramesvaran, T. Sakuma, S. Seif El Nasr-Storey, V. J. Smith, N. Stylianou, J. Taylor, A. Titterton, K. W. Bell, C. Brew, R. M. Brown, D. J. A. Cockerill, K. V. Ellis, K. Harder, S. Harper, J. Linacre, K. Manolopoulos, D. M. Newbold, E. Olaiya, D. Petyt, T. Reis, T. Schuh, C. H. Shepherd-Themistocleous, A. Thea, I. R. Tomalin, T. Williams, R. Bainbridge, P. Bloch, S. Bonomally, J. Borg, S. Breeze, O. Buchmuller, A. Bundock, V. Cepaitis, G. S. Chahal, D. Colling, P. Dauncey, G. Davies, M. Della Negra, G. Fedi, G. Hall, G. Iles, J. Langford, L. Lyons, A.-M. Magnan, S. Malik, A. Martelli, V. Milosevic, J. Nash, V. Palladino, M. Pesaresi, D. M. Raymond, A. Richards, A. Rose, E. Scott, C. Seez, A. Shtipliyski, M. Stoye, A. Tapper, K. Uchida, T. Virdee, N. Wardle, S. N. Webb, D. Winterbottom, A. G. Zecchinelli, J. E. Cole, P. R. Hobson, A. Khan, P. Kyberd, C. K. Mackay, I. D. Reid, L. Teodorescu, S. Zahid, S. Abdullin, A. Brinkerhoff, K. Call, B. Caraway, J. Dittmann, K. Hatakeyama, A. R. Kanuganti, C. Madrid, B. McMaster, N. Pastika, S. Sawant, C. Smith, J. Wilson, R. Bartek, A. Dominguez, R. Uniyal, A. M. Vargas Hernandez, A. Buccilli, O. Charaf, S. I. Cooper, S. V. Gleyzer, C. Henderson, C. U. Perez, P. Rumerio, C. West, A. Akpinar, A. Albert, D. Arcaro, C. Cosby, Z. Demiragli, D. Gastler, J. Rohlf, K. Salyer, D. Sperka, D. Spitzbart, I. Suarez, S. Yuan, D. Zou, G. Benelli, B. Burkle, X. Coubez, D. Cutts, Y. t. Duh, M. Hadley, U. Heintz, J. M. Hogan, K. H. M. Kwok, E. Laird, G. Landsberg, K. T. Lau, M. Narain, S. Sagir, R. Syarif, E. Usai, W. Y. Wong, D. Yu, W. Zhang, R. Band, C. Brainerd, R. Breedon, M. Calderon De La Barca Sanchez, M. Chertok, J. Conway, R. Conway, P. T. Cox, R. Erbacher, C. Flores, G. Funk, F. Jensen, W. Ko, O. Kukral, R. Lander, M. Mulhearn, D. Pellett, J. Pilot, M. Shi, D. Taylor, K. Tos, M. Tripathi, Y. Yao, F. Zhang, M. Bachtis, R. Cousins, A. Dasgupta, D. Hamilton, J. Hauser, M. Ignatenko, M. A. Iqbal, T. Lam, N. Mccoll, W. A. Nash, S. Regnard, D. Saltzberg, C. Schnaible, B. Stone, V. Valuev, K. Burt, Y. Chen, R. Clare, J. W. Gary, G. Hanson, G. Karapostoli, O. R. Long, N. Manganelli, M. Olmedo Negrete, M. I. Paneva, W. Si, S. Wimpenny, Y. Zhang, J. G. Branson, S. Cittolin, S. Cooperstein, N. Deelen, J. Duarte, R. Gerosa, D. Gilbert, V. Krutelyov, J. Letts, M. Masciovecchio, S. May, S. Padhi, M. Pieri, V. Sharma, M. Tadel, F. Würthwein, A. Yagil, N. Amin, C. Campagnari, M. Citron, A. Dorsett, V. Dutta, J. Incandela, B. Marsh, H. Mei, A. Ovcharova, H. Qu, M. Quinnan, J. Richman, U. Sarica, D. Stuart, S. Wang, A. Bornheim, O. Cerri, I. Dutta, J. M. Lawhorn, N. Lu, J. Mao, H. B. Newman, J. Ngadiuba, T. Q. Nguyen, J. Pata, M. Spiropulu, J. R. Vlimant, C. Wang, S. Xie, Z. Zhang, R. Y. Zhu, J. Alison, M. B. Andrews, T. Ferguson, T. Mudholkar, M. Paulini, M. Sun, I. Vorobiev, J. P. Cumalat, W. T. Ford, E. MacDonald, T. Mulholland, R. Patel, A. Perloff, K. Stenson, K. A. Ulmer, S. R. Wagner, J. Alexander, Y. Cheng, J. Chu, D. J. Cranshaw, A. Datta, A. Frankenthal, K. Mcdermott, J. Monroy, J. R. Patterson, D. Quach, A. Ryd, W. Sun, S. M. Tan, Z. Tao, J. Thom, P. Wittich, M. Zientek, M. Albrow, M. Alyari, G. Apollinari, A. Apresyan, A. Apyan, L. A. T. Bauerdick, A. Beretvas, D. Berry, J. Berryhill, P. C. Bhat, K. Burkett, J. N. Butler, A. Canepa, G. B. Cerati, H. W. K. Cheung, F. Chlebana, M. Cremonesi, V. D. Elvira, J. Freeman, Z. Gecse, E. Gottschalk, L. Gray, D. Green, S. Grünendahl, O. Gutsche, R. M. Harris, S. Hasegawa, R. Heller, T. C. Herwig, J. Hirschauer, B. Jayatilaka, S. Jindariani, M. Johnson, U. Joshi, P. Klabbers, T. Klijnsma, B. Klima, M. J. Kortelainen, S. Lammel, D. Lincoln, R. Lipton, M. Liu, T. Liu, J. Lykken, K. Maeshima, D. Mason, P. McBride, P. Merkel, S. Mrenna, S. Nahn, V. O’Dell, V. Papadimitriou, K. Pedro, C. Pena, O. Prokofyev, F. Ravera, A. Reinsvold Hall, L. Ristori, B. Schneider, E. Sexton-Kennedy, N. Smith, A. Soha, W. J. Spalding, L. Spiegel, S. Stoynev, J. Strait, L. Taylor, S. Tkaczyk, N. V. Tran, L. Uplegger, E. W. Vaandering, H. A. Weber, A. Woodard, D. Acosta, P. Avery, D. Bourilkov, L. Cadamuro, V. Cherepanov, F. Errico, R. D. Field, D. Guerrero, B. M. Joshi, M. Kim, J. Konigsberg, A. Korytov, K. H. Lo, K. Matchev, N. Menendez, G. Mitselmakher, D. Rosenzweig, K. Shi, J. Sturdy, X. Zuo, T. Adams, A. Askew, D. Diaz, R. Habibullah, S. Hagopian, V. Hagopian, K. F. Johnson, R. Khurana, T. Kolberg, G. Martinez, H. Prosper, C. Schiber, R. Yohay, J. Zhang, M. M. Baarmand, S. Butalla, T. Elkafrawy, M. Hohlmann, D. Noonan, M. Rahmani, M. Saunders, F. Yumiceva, M. R. Adams, L. Apanasevich, H. Becerril Gonzalez, R. Cavanaugh, X. Chen, S. Dittmer, O. Evdokimov, C. E. Gerber, D. A. Hangal, D. J. Hofman, C. Mills, G. Oh, T. Roy, M. B. Tonjes, N. Varelas, J. Viinikainen, X. Wang, Z. Wu, Z. Ye, M. Alhusseini, K. Dilsiz, S. Durgut, R. P. Gandrajula, M. Haytmyradov, V. Khristenko, O. K. Köseyan, J.-P. Merlo, A. Mestvirishvili, A. Moeller, J. Nachtman, H. Ogul, Y. Onel, F. Ozok, A. Penzo, C. Snyder, E. Tiras, J. Wetzel, O. Amram, B. Blumenfeld, L. Corcodilos, M. Eminizer, A. V. Gritsan, S. Kyriacou, P. Maksimovic, C. Mantilla, J. Roskes, M. Swartz, T. Á. Vámi, C. Baldenegro Barrera, P. Baringer, A. Bean, A. Bylinkin, T. Isidori, S. Khalil, J. King, G. Krintiras, A. Kropivnitskaya, C. Lindsey, N. Minafra, M. Murray, C. Rogan, C. Royon, S. Sanders, E. Schmitz, J. D. Tapia Takaki, J. Williams, G. Wilson, S. Duric, A. Ivanov, K. Kaadze, D. Kim, Y. Maravin, T. Mitchell, A. Modak, A. Mohammadi, F. Rebassoo, D. Wright, E. Adams, A. Baden, O. Baron, A. Belloni, S. C. Eno, Y. Feng, N. J. Hadley, S. Jabeen, G. Y. Jeng, R. G. Kellogg, T. Koeth, A. C. Mignerey, S. Nabili, M. Seidel, A. Skuja, S. C. Tonwar, L. Wang, K. Wong, D. Abercrombie, B. Allen, R. Bi, S. Brandt, W. Busza, I. A. Cali, M. D’Alfonso, G. Gomez Ceballos, M. Goncharov, P. Harris, D. Hsu, M. Hu, M. Klute, D. Kovalskyi, J. Krupa, Y.-J. Lee, P. D. Luckey, B. Maier, A. C. Marini, C. Mcginn, C. Mironov, S. Narayanan, X. Niu, C. Paus, D. Rankin, C. Roland, G. Roland, Z. Shi, G. S. F. Stephans, K. Sumorok, K. Tatar, D. Velicanu, T. W. Wang, Z. Wang, B. Wyslouch, R. M. Chatterjee, A. Evans, P. Hansen, J. Hiltbrand, Sh. Jain, M. Krohn, Y. Kubota, Z. Lesko, J. Mans, M. Revering, R. Rusack, R. Saradhy, N. Schroeder, N. Strobbe, M. A. Wadud, J. G. Acosta, S. Oliveros, K. Bloom, D. R. Claes, C. Fangmeier, L. Finco, F. Golf, J. R. González Fernández, C. Joo, I. Kravchenko, J. E. Siado, G. R. Snow, W. Tabb, F. Yan, G. Agarwal, H. Bandyopadhyay, C. Harrington, L. Hay, I. Iashvili, A. Kharchilava, C. McLean, D. Nguyen, J. Pekkanen, S. Rappoccio, B. Roozbahani, G. Alverson, E. Barberis, C. Freer, Y. Haddad, A. Hortiangtham, J. Li, G. Madigan, B. Marzocchi, D. M. Morse, V. Nguyen, T. Orimoto, A. Parker, L. Skinnari, A. Tishelman-Charny, T. Wamorkar, B. Wang, A. Wisecarver, D. Wood, J. Bueghly, Z. Chen, A. Gilbert, T. Gunter, K. A. Hahn, N. Odell, M. H. Schmitt, K. Sung, M. Velasco, R. Bucci, N. Dev, R. Goldouzian, M. Hildreth, K. Hurtado Anampa, C. Jessop, D. J. Karmgard, K. Lannon, N. Loukas, N. Marinelli, I. Mcalister, F. Meng, K. Mohrman, Y. Musienko, R. Ruchti, P. Siddireddy, S. Taroni, M. Wayne, A. Wightman, M. Wolf, L. Zygala, J. Alimena, B. Bylsma, B. Cardwell, L. S. Durkin, B. Francis, C. Hill, A. Lefeld, B. L. Winer, B. R. Yates, B. Bonham, P. Das, G. Dezoort, P. Elmer, B. Greenberg, N. Haubrich, S. Higginbotham, A. Kalogeropoulos, G. Kopp, S. Kwan, D. Lange, M. T. Lucchini, J. Luo, D. Marlow, K. Mei, I. Ojalvo, J. Olsen, C. Palmer, P. Piroué, D. Stickland, C. Tully, S. Norberg, V. E. Barnes, R. Chawla, S. Das, L. Gutay, M. Jones, A. W. Jung, G. Negro, N. Neumeister, C. C. Peng, S. Piperov, A. Purohit, H. Qiu, J. F. Schulte, M. Stojanovic, N. Trevisani, F. Wang, A. Wildridge, R. Xiao, W. Xie, J. Dolen, N. Parashar, A. Baty, S. Dildick, K. M. Ecklund, S. Freed, F. J. M. Geurts, M. Kilpatrick, W. Li, B. P. Padley, R. Redjimi, J. Roberts, J. Rorie, W. Shi, A. G. Stahl Leiton, A. Bodek, P. de Barbaro, R. Demina, J. L. Dulemba, C. Fallon, T. Ferbel, M. Galanti, A. Garcia-Bellido, O. Hindrichs, A. Khukhunaishvili, E. Ranken, R. Taus, B. Chiarito, J. P. Chou, A. Gandrakota, Y. Gershtein, E. Halkiadakis, A. Hart, M. Heindl, E. Hughes, S. Kaplan, O. Karacheban, I. Laflotte, A. Lath, R. Montalvo, K. Nash, M. Osherson, S. Salur, S. Schnetzer, S. Somalwar, R. Stone, S. A. Thayil, S. Thomas, H. Acharya, A. G. Delannoy, S. Spanier, O. Bouhali, M. Dalchenko, A. Delgado, R. Eusebi, J. Gilmore, T. Huang, T. Kamon, S. Luo, S. Malhotra, R. Mueller, D. Overton, L. Perniè, D. Rathjens, A. Safonov, N. Akchurin, J. Damgov, V. Hegde, S. Kunori, K. Lamichhane, T. Mengke, S. Muthumuni, T. Peltola, S. Undleeb, I. Volobouev, A. Whitbeck, E. Appelt, S. Greene, A. Gurrola, R. Janjam, W. Johns, C. Maguire, A. Melo, H. Ni, K. Padeken, F. Romeo, P. Sheldon, S. Tuo, J. Velkovska, M. W. Arenton, B. Cox, G. Cummings, J. Hakala, R. Hirosky, M. Joyce, A. Ledovskoy, A. Li, C. Neu, B. Tannenwald, E. Wolfe, F. Xia, P. E. Karchin, N. Poudyal, P. Thapa, K. Black, T. Bose, J. Buchanan, C. Caillol, S. Dasu, I. De Bruyn, P. Everaerts, C. Galloni, H. He, M. Herndon, A. Hervé, U. Hussain, A. Lanaro, A. Loeliger, R. Loveless, J. Madhusudanan Sreekala, A. Mallampalli, D. Pinna, A. Savin, V. Shang, W. H. Smith, D. Teague, S. Trembath-reichert, W. Vetens, and CMS Collaboration
Subjects: Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract: Abstract A search is presented for a heavy vector resonance decaying into a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson and the standard model Higgs boson, where the $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 . Upper limits are derived on the production of a narrow heavy resonance $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ , and a mass below 3.5 and 3.7 $$\,\text {Te}\text {V}$$ Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 $$\,\text {fb}$$ fb for a $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ mass between 0.8 and 4.6 $$\,\text {Te}\text {V}$$ Te , respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021
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17. On the transition form factors of the axial-vector resonance f 1(1285) and its decay into e + e −

Author: Marvin Zanke, Martin Hoferichter, and Bastian Kubis
Subjects: Chiral Lagrangians, Effective Field Theories, Nonperturbative Effects, Precision QED, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract: Abstract Estimating the contribution from axial-vector intermediate states to hadronic light-by-light scattering requires input on their transition form factors (TFFs). Due to the Landau–Yang theorem, any experiment sensitive to these TFFs needs to involve at least one virtual photon, which complicates their measurement. Phenomenologically, the situation is best for the f 1(1285) resonance, for which information is available from e + e − → e + e − f 1, f 1 → 4π, f 1 → ργ, f 1 → ϕγ, and f 1 → e + e − . We provide a comprehensive analysis of the f 1 TFFs in the framework of vector meson dominance, including short-distance constraints, to determine to which extent the three independent TFFs can be constrained from the available experimental input — a prerequisite for improved calculations of the axial-vector contribution to hadronic light-by-light scattering. In particular, we focus on the process f 1 → e + e − , evidence for which has been reported recently by SND for the first time, and discuss the impact that future improved measurements will have on the determination of the f 1 TFFs.
Published: 2021
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18. Peak locations and relative phase of different decay modes of the $a_1$ axial vector resonance in diffractive production

Author: Basdevant, Jean-Louis and Berger, Edmond L
Subjects: High Energy Physics - Phenomenology
Abstract: We show that a single $I=1$ spin-parity $J^{PC}= 1^{++}$ $a_1$ resonance can manifest itself as two separated mass peaks, one decaying into an S-wave $\rho\pi$ system and the second decaying into a P-wave $f_0(980)\pi$ system, with a rapid increase of the phase difference between their amplitudes arising mainly from the structure of the diffractive production process. This study clarifies questions related to the mass, width, and decay rates of the $a_1$ resonance raised by the recent high statistics data of the COMPASS collaboration on $a_1$ production in $\pi N \rightarrow \pi \pi \pi N$ at high energies., Comment: 4 pages, 4 figures, to be published in Physical Review Letters. arXiv admin note: substantial text overlap with arXiv:1501.04643
Published: 2015
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19. Search for a heavy vector resonance decaying to a Zs=13Te boson and a Higgs boson in proton-proton collisions at Zs=13Te

Author: Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Erö, J., Valle, A. Escalante Del, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Pitters, F. M., Rad, N., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., Waltenberger, W., Wulz, C.-E., Zarucki, M., Chekhovsky, V., Litomin, A., Makarenko, V., Gonzalez, J. Suarez, Darwish, M. R., De Wolf, E. A., Di Croce, D., Janssen, X., Kello, T., Lelek, A., Pieters, M., Sfar, H. Rejeb, Van Haevermaet, H., Van Mechelen, P., Van Putte, S., Van Remortel, N., Blekman, F., Bols, E. S., Chhibra, S. S., D’Hondt, J., De Clercq, J., Lontkovskyi, D., Lowette, S., Marchesini, I., Moortgat, S., Morton, A., Müller, D., Python, Q., Tavernier, S., Van Doninck, W., Van Mulders, P., Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Dorney, B., Favart, L., Grebenyuk, A., Kalsi, A. K., Makarenko, I., Moureaux, L., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Vander Velde, C., Vanlaer, P., Vannerom, D., Wezenbeek, L., Cornelis, T., Dobur, D., Gruchala, M., Khvastunov, I., Niedziela, M., Roskas, C., Skovpen, K., Tytgat, M., Verbeke, W., Vermassen, B., Vit, M., Bruno, G., Bury, F., Caputo, C., David, P., Delaere, C., Delcourt, M., Donertas, I. S., Giammanco, A., Lemaitre, V., Mondal, K., Prisciandaro, J., Taliercio, A., Teklishyn, M., Vischia, P., Wertz, S., Wuyckens, S., Alves, G. A., Hensel, C., Moraes, A., Júnior, W. L. Aldá, Chagas, E. Belchior Batista Das, Malbouisson, H. Brandao, Carvalho, W., Chinellato, J., Coelho, E., Da Costa, E. M., Da Silveira, G. G., De Jesus Damiao, D., De Souza, S. Fonseca, Martins, J., Figueiredo, D. Matos, Jaime, M. Medina, Herrera, C. Mora, Mundim, L., Nogima, H., Teles, P. Rebello, Rosas, L. J. Sanchez, Santoro, A., Do Amaral, S. M. Silva, Sznajder, A., Thiel, M., Da Silva De Araujo, F. Torres, Pereira, A. 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P., Gandrakota, A., Gershtein, Y., Halkiadakis, E., Hart, A., Heindl, M., Hughes, E., Kaplan, S., Karacheban, O., Laflotte, I., Lath, A., Montalvo, R., Nash, K., Osherson, M., Salur, S., Schnetzer, S., Somalwar, S., Stone, R., Thayil, S. A., Thomas, S., Wang, H., Acharya, H., Delannoy, A. G., Spanier, S., Bouhali, O., Dalchenko, M., Delgado, A., Eusebi, R., Gilmore, J., Huang, T., Kamon, T., Kim, H., Luo, S., Malhotra, S., Mueller, R., Overton, D., Perniè, L., Rathjens, D., Safonov, A., Akchurin, N., Damgov, J., Hegde, V., Kunori, S., Lamichhane, K., Lee, S. W., Mengke, T., Muthumuni, S., Peltola, T., Undleeb, S., Volobouev, I., Wang, Z., Whitbeck, A., Appelt, E., Greene, S., Gurrola, A., Janjam, R., Johns, W., Maguire, C., Melo, A., Ni, H., Padeken, K., Romeo, F., Sheldon, P., Tuo, S., Velkovska, J., Arenton, M. W., Cox, B., Cummings, G., Hakala, J., Hirosky, R., Joyce, M., Ledovskoy, A., Li, A., Neu, C., Tannenwald, B., Wang, Y., Wolfe, E., Xia, F., Karchin, P. E., Poudyal, N., Thapa, P., Black, K., Bose, T., Buchanan, J., Caillol, C., Dasu, S., De Bruyn, I., Everaerts, P., Galloni, C., He, H., Herndon, M., Hervé, A., Hussain, U., Lanaro, A., Loeliger, A., Loveless, R., Sreekala, J. Madhusudanan, Mallampalli, A., Pinna, D., Savin, A., Shang, V., Sharma, V., Smith, W. H., Teague, D., Trembath-reichert, S., and Vetens, W.
Published: 2021
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20. The vector resonance triplet with the direct coupling to the third quark generation

Author: Gintner, Mikulas and Juran, Josef
Subjects: High Energy Physics - Phenomenology
Abstract: The effective Lagrangian with scalar and vector resonances that might result from new strong physics beyond the SM is formulated and studied. In particular, the scalar resonance representing the recently discovered 125-GeV boson is complemented with the SU(2)_{L+R} triplet of hypothetical vector resonances. Motivated by experimental and theoretical considerations, the vector resonance is allowed to couple directly to the third quark generation only. The coupling is chiral-dependent and the interaction of the right top quark can differ from that of the right bottom quark. To estimate the applicability range of the effective Lagrangian the unitarity of the gauge boson scattering amplitudes is analyzed. The experimental fits and limits on the free parameters of the vector resonance triplet are investigated., Comment: 17 pages, 10 figures, to be published in The European Physical Journal C. arXiv admin note: text overlap with arXiv:1301.2124
Published: 2013
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21. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Author: Sirunyan, A.M., Beghin, Diego, Bilin, Bugra, Clerbaux, Barbara, De Lentdecker, Gilles, Dorney, Brian, Favart, Laurent, Grebenyuk, Anastasia, Kalsi, Amandeep Kaur, Makarenko, Inna, Malara, Andrea, Moureaux, Louis, Pétré, Laurent, Popov, Andrey, Postiau, Nicolas, Starling, Elizabeth Rose, Thomas, Laurent, Vander Velde, Catherine, Vanlaer, Pascal, Vannerom, David, Wezenbeek, Liam, Sirunyan, A.M., Beghin, Diego, Bilin, Bugra, Clerbaux, Barbara, De Lentdecker, Gilles, Dorney, Brian, Favart, Laurent, Grebenyuk, Anastasia, Kalsi, Amandeep Kaur, Makarenko, Inna, Malara, Andrea, Moureaux, Louis, Pétré, Laurent, Popov, Andrey, Postiau, Nicolas, Starling, Elizabeth Rose, Thomas, Laurent, Vander Velde, Catherine, Vanlaer, Pascal, Vannerom, David, and Wezenbeek, Liam
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137fb-1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3fb for a Z′ mass between 0.8 and 4.6Te, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay., 0, CMS Collaboration, info:eu-repo/semantics/published
Published: 2021

22. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s = 13TeV

Author: European Organization for Nuclear Research, Principado de Asturias, European Commission, European Research Council, Ministerio de Economía y Competitividad (España), CMS Collaboration, Brochero Cifuentes, J. A., Cabrillo, I. J., Calderon, Alicia, Chazin Quero, B., Duarte Campderros, J., Fernández-García, Marcos, Fernández Manteca, P. J., García Alonso, A., Gómez, Gervasio, Martínez-Rivero, Celso, Martínez Ruiz del Arbol, P., Matorras, Francisco, Piedra, Jonatan, Prieels, C., Ricci-Tam, F., Rodrigo, Teresa, Ruiz Jimeno, Alberto, Scodellaro, Luca, Vila, Iván, Vizán, J., European Organization for Nuclear Research, Principado de Asturias, European Commission, European Research Council, Ministerio de Economía y Competitividad (España), CMS Collaboration, Brochero Cifuentes, J. A., Cabrillo, I. J., Calderon, Alicia, Chazin Quero, B., Duarte Campderros, J., Fernández-García, Marcos, Fernández Manteca, P. J., García Alonso, A., Gómez, Gervasio, Martínez-Rivero, Celso, Martínez Ruiz del Arbol, P., Matorras, Francisco, Piedra, Jonatan, Prieels, C., Ricci-Tam, F., Rodrigo, Teresa, Ruiz Jimeno, Alberto, Scodellaro, Luca, Vila, Iván, and Vizán, J.
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137fb−1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7TeV is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3fb for a Z′ mass between 0.8 and 4.6TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

23. Search for a heavy vector resonance decaying to a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson and a Higgs boson in proton-proton collisions at $$\sqrt{s} = 13\,\text {Te}\text {V} $$ s = 13 Te

Author: Massachusetts Institute of Technology. Department of Physics, Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Erö, J., Valle, A. E. D., Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Pitters, F. M., Rad, N., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., Waltenberger, W., Massachusetts Institute of Technology. Department of Physics, Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Erö, J., Valle, A. E. D., Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Pitters, F. M., Rad, N., Schieck, J., Schöfbeck, R., Spanring, M., Templ, S., and Waltenberger, W.
Abstract: A search is presented for a heavy vector resonance decaying into a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson and the standard model Higgs boson, where the $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 . Upper limits are derived on the production of a narrow heavy resonance $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ , and a mass below 3.5 and 3.7 $$\,\text {Te}\text {V}$$ Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 $$\,\text {fb}$$ fb for a $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ mass between 0.8 and 4.6 $$\,\text {Te}\text {V}$$ Te , respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

24. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Author: Sirunyan, A, Tumasyan, A, Adam, W, Bergauer, T, Dragicevic, M, Ero, J, Valle, A, Fruhwirth, R, Jeitler, M, Krammer, N, Lechner, L, Liko, D, Mikulec, I, Pitters, F, Rad, N, Schieck, J, Schofbeck, R, Spanring, M, Templ, S, Waltenberger, W, Wulz, C, Zarucki, M, Chekhovsky, V, Litomin, A, Makarenko, V, Gonzalez, J, Darwish, M, De Wolf, E, Di Croce, D, Janssen, X, Kello, T, Lelek, A, Pieters, M, Sfar, H, Van Haevermaet, H, Van Mechelen, P, Van Putte, S, Van Remortel, N, Blekman, F, Bols, E, Chhibra, S, D'Hondt, J, De Clercq, J, Lontkovskyi, D, Lowette, S, Marchesini, I, Moortgat, S, Morton, A, Muller, D, Python, Q, Tavernier, S, Van Doninck, W, Van Mulders, P, Beghin, D, Bilin, B, Clerbaux, B, De Lentdecker, G, Dorney, B, Favart, L, Grebenyuk, A, Kalsi, A, Makarenko, I, Moureaux, L, Petre, L, Popov, A, Postiau, N, Starling, E, Thomas, L, Vander Velde, C, Vanlaer, P, Vannerom, D, Wezenbeek, L, Cornelis, T, Dobur, D, Gruchala, M, Khvastunov, I, Niedziela, M, Roskas, C, Skovpen, K, Tytgat, M, Verbeke, W, Vermassen, B, Vit, M, Bruno, G, Bury, F, Caputo, C, David, P, Delaere, C, Delcourt, M, Donertas, I, Giammanco, A, Lemaitre, V, Mondal, K, Prisciandaro, J, Taliercio, A, Teklishyn, M, Vischia, P, Wertz, S, Wuyckens, S, Alves, G, Hensel, C, Moraes, A, Junior, W, Chagas, E, Malbouisson, H, Carvalho, W, Chinellato, J, Coelho, E, Da Costa, E, Da Silveira, G, De Jesus Damiao, D, De Souza, S, Martins, J, Figueiredo, D, Jaime, M, Herrera, C, Mundim, L, Nogima, H, Teles, P, Rosas, L, Santoro, A, Do Amaral, S, Sznajder, A, Thiel, M, Da Silva De Araujo, F, Pereira, A, Bernardes, C, Calligaris, L, Tomei, T, Gregores, E, Lemos, D, Mercadante, P, Novaes, S, Padula, S, Aleksandrov, A, Antchev, G, Atanasov, I, Hadjiiska, R, Iaydjiev, P, Misheva, M, Rodozov, M, Shopova, M, Sultanov, G, Dimitrov, A, Ivanov, T, Litov, L, Pavlov, B, Petkov, P, Petrov, A, Cheng, T, Fang, W, Guo, Q, Wang, H, Yuan, L, Ahmad, M, Bauer, G, Hu, Z, Wang, Y, Yi, K, Chapon, E, Chen, G, Chen, H, Chen, M, Javaid, T, Kapoor, A, Leggat, D, Liao, H, Liu, Z, Sharma, R, Spiezia, A, Tao, J, Thomas-wilsker, J, Wang, J, Zhang, H, Zhang, S, Zhao, J, Agapitos, A, Ban, Y, Chen, C, Huang, Q, Levin, A, Li, Q, Lu, M, Lyu, X, Mao, Y, Qian, S, Wang, D, Wang, Q, Xiao, J, You, Z, Gao, X, Xiao, M, Avila, C, Cabrera, A, Florez, C, Fraga, J, Sarkar, A, Delgado, M, Jaramillo, J, Guisao, J, Ramirez, F, Alvarez, J, Gonzalez, C, Arbelaez, N, Giljanovic, D, Godinovic, N, Lelas, D, Puljak, I, Antunovic, Z, Kovac, M, Sculac, T, Brigljevic, V, Ferencek, D, Majumder, D, Roguljic, M, Starodumov, A, Susa, T, Ather, M, Attikis, A, Erodotou, E, Ioannou, A, Kole, G, Kolosova, M, Konstantinou, S, Mousa, J, Nicolaou, C, Ptochos, F, Razis, P, Rykaczewski, H, Saka, H, Tsiakkouri, D, Finger, M, Kveton, A, Tomsa, J, Ayala, E, Jarrin, E, Zeid, S, Assran, Y, Salama, E, Lotfy, A, Mahmoud, M, Bhowmik, S, De Oliveira, A, Dewanjee, R, Ehataht, K, Kadastik, M, Raidal, M, Veelken, C, Eerola, P, Forthomme, L, Kirschenmann, H, 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W., Attikis A., Erodotou E., Ioannou A., Kole G., Kolosova M., Konstantinou S., Mousa J., Nicolaou C., Ptochos F., Razis P. A., Rykaczewski H., Saka H., Tsiakkouri D., Finger M., Kveton A., Tomsa J., Ayala E., Jarrin E. C., Zeid S. A., Assran Y., Salama E., Lotfy A., Mahmoud M. A., Bhowmik S., De Oliveira A. C. A., Dewanjee R. K., Ehataht K., Kadastik M., Raidal M., Veelken C., Eerola P., Forthomme L., Kirschenmann H., Osterberg K., Voutilainen M., Brucken E., Garcia F., Havukainen J., Karimaki V., Kim M. S., Kinnunen R., Lampen T., Lassila-Perini K., Lehti S., Linden T., Siikonen H., Tuominen E., Tuominiemi J., Luukka P., Tuuva T., Amendola C., Besancon M., Couderc F., Dejardin M., Denegri D., Faure J. L., Ferri F., Ganjour S., Givernaud A., Gras P., de Monchenault G. H., Jarry P., Lenzi B., Locci E., Malcles J., Rander J., Rosowsky A., Sahin M. O., Savoy-Navarro A., Titov M., Yu G. B., Ahuja S., Beaudette F., Bonanomi M., Perraguin A. 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K., Manousakis-katsikakis A., Panagiotou A., Papavergou I., Saoulidou N., Theofilatos K., Tziaferi E., Vellidis K., Vourliotis E., Bakas G., Kousouris K., Papakrivopoulos I., Tsipolitis G., Zacharopoulou A., Evangelou I., Foudas C., Gianneios P., Katsoulis P., Kokkas P., Manitara K., Manthos N., Papadopoulos I., Strologas J., Bartok M., Csanad M., Gadallah M. M. A., Lokos S., Major P., Mandal K., Mehta A., Pasztor G., Suranyi O., Veres G. I., Bencze G., Hajdu C., Horvath D., Sikler F., Veszpremi V., Vesztergombi G., Czellar S., Karancsi J., Molnar J., Szillasi Z., Teyssier D., Raics P., Trocsanyi Z. L., Ujvari B., Csorgo T., Nemes F., Novak T., Choudhury S., Komaragiri J. R., Kumar D., Panwar L., Tiwari P. C., Bahinipati S., Dash D., Kar C., Mal P., Mishra T., Bindhu V. K. M. N., Nayak A., Sahoo D. K., Sur N., Swain S. K., Bansal S., Beri S. B., Bhatnagar V., Chaudhary G., Chauhan S., Dhingra N., Gupta R., Kaur A., Kaur S., Kumari P., Meena M., Sandeep K., Sharma S., Singh J. 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P., Tosi N., Albergo S., Costa S., Di Mattia A., Potenza R., Tricomi A., Tuve C., Barbagli G., Cassese A., Ceccarelli R., Ciulli V., Civinini C., D'Alessandro R., Fiori F., Focardi E., Latino G., Lenzi P., Lizzo M., Meschini M., Paoletti S., Seidita R., Sguazzoni G., Viliani L., Benussi L., Bianco S., Piccolo D., Bozzo M., Ferro F., Mulargia R., Robutti E., Tosi S., Benaglia A., Beschi A., Brivio F., Cetorelli F., Ciriolo V., De Guio F., Dinardo M. E., Dini P., Gennai S., Ghezzi A., Govoni P., Guzzi L., Malberti M., Malvezzi S., Massironi A., Menasce D., Monti F., Moroni L., Paganoni M., Pedrini D., Ragazzi S., de Fatis T. T., Valsecchi D., Zuolo D., Buontempo S., Cavallo N., De Iorio A., Fabozzi F., Fienga F., Iorio A. O. M., Lista L., Meola S., Paolucci P., Rossi B., Sciacca C., Voevodina E., Azzi P., Bacchetta N., Bisello D., Bortignon P., Bragagnolo A., Carlin R., Checchia P., De Castro Manzano P., Dorigo T., Gasparini F., Gasparini U., Hoh S. Y., Layer L., Margoni M., Meneguzzo A. T., Presilla M., Ronchese P., Rossin R., Simonetto F., Strong G., Tosi M., Yarar H., Zanetti M., Zotto P., Zucchetta A., Zumerle G., Aime' C., Braghieri A., Calzaferri S., Fiorina D., Montagna P., Ratti S. P., Re V., Ressegotti M., Riccardi C., Salvini P., Vai I., Vitulo P., Biasini M., Bilei G. M., Ciangottini D., Fano L., Lariccia P., Mantovani G., Mariani V., Menichelli M., Moscatelli F., Piccinelli A., Rossi A., Santocchia A., Spiga D., Tedeschi T., Androsov K., Azzurri P., Bagliesi G., Bertacchi V., Bianchini L., Boccali T., Castaldi R., Ciocci M. A., Dell'Orso R., Di Domenico M. R., Donato S., Giannini L., Giassi A., Grippo M. T., Ligabue F., Manca E., Mandorli G., Messineo A., Palla F., Ramirez-Sanchez G., Rizzi A., Rolandi G., Chowdhury S. R., Scribano A., Shafiei N., Spagnolo P., Tenchini R., Tonelli G., Turini N., Venturi A., Verdini P. G., Cavallari F., Cipriani M., Re D. D., Di Marco E., Diemoz M., Longo E., Meridiani P., Organtini G., Pandolfi F., Paramatti R., Quaranta C., Rahatlou S., Rovelli C., Santanastasio F., Soffi L., Tramontano R., Amapane N., Arcidiacono R., Argiro S., Arneodo M., Bartosik N., Bellan R., Bellora A., Antequera J. B., Biino C., Cappati A., Cartiglia N., Cometti S., Costa M., Covarelli R., Demaria N., Kiani B., Legger F., Mariotti C., Maselli S., Migliore E., Monaco V., Monteil E., Monteno M., Obertino M. M., Ortona G., Pacher L., Pastrone N., Pelliccioni M., Angioni G. L. P., Ruspa M., Salvatico R., Siviero F., Sola V., Solano A., Soldi D., Staiano A., Tornago M., Trocino D., Belforte S., Candelise V., Casarsa M., Cossutti F., Da Rold A., Ricca G. D., Vazzoler F., Dogra S., Huh C., Kim B., Kim D. H., Kim G. N., Lee J., Lee S. W., Moon C. S., Oh Y. D., Pak S. I., Radburn-Smith B. C., Sekmen S., Yang Y. C., Kim H., Moon D. H., Francois B., Kim T. J., Park J., Cho S., Choi S., Go Y., Ha S., Hong B., Lee K., Lee K. 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A., Shah M. A., Shoaib M., Waqas M., Avati V., Grzanka L., Malawski M., Bialkowska H., Bluj M., Boimska B., Frueboes T., Gorski M., Kazana M., Szleper M., Traczyk P., Zalewski P., Bunkowski K., Doroba K., Kalinowski A., Konecki M., Krolikowski J., Walczak M., Araujo M., Bargassa P., Bastos D., Boletti A., Faccioli P., Gallinaro M., Hollar J., Leonardo N., Niknejad T., Seixas J., Shchelina K., Toldaiev O., Varela J., Afanasiev S., Bunin P., Gavrilenko M., Golutvin I., Kamenev A., Karjavine V., Kashunin I., Korenkov V., Lanev A., Malakhov A., Matveev V., Mitsyn V. V., Palichik V., Perelygin V., Savina M., Shalaev V., Shmatov S., Shulha S., Smirnov V., Teryaev O., Trofimov V., Zarubin A., Gavrilov G., Golovtcov V., Ivanov Y., Kim V., Kuznetsova E., Murzin V., Oreshkin V., Smirnov I., Sosnov D., Sulimov V., Uvarov L., Volkov S., Vorobyev A., Andreev Y., Dermenev A., Gninenko S., Golubev N., Karneyeu A., Kirsanov M., Krasnikov N., Pashenkov A., Pivovarov G., Tlisov D., Toropin A., Epshteyn V., Gavrilov V., Lychkovskaya N., Nikitenko A., Popov V., Safronov G., Spiridonov A., Stepennov A., Toms M., Vlasov E., Zhokin A., Aushev T., Bychkova O., Philippov D., Popova E., Rusinov V., Zhemchugov E., Andreev V., Azarkin M., Dremin I., Kirakosyan M., Terkulov A., Belyaev A., Boos E., Bunichev V., Dubinin M., Dudko L., Ershov A., Klyukhin V., Kodolova O., Lokhtin I., Obraztsov S., Perfilov M., Petrushanko S., Savrin V., Blinov V., Dimova T., Kardapoltsev L., Ovtin I., Skovpen Y., Azhgirey I., Bayshev I., Kachanov V., Kalinin A., Konstantinov D., Petrov V., Ryutin R., Sobol A., Troshin S., Tyurin N., Uzunian A., Volkov A., Babaev A., Iuzhakov A., Okhotnikov V., Sukhikh L., Borchsh V., Ivanchenko V., Tcherniaev E., Adzic P., Cirkovic P., Dordevic M., Milenovic P., Milosevic J., Aguilar-Benitez M., Maestre J. 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C., Kotlinski D., Langenegger U., Rohe T., Backhaus M., Berger P., Calandri A., Chernyavskaya N., De Cosa A., Dissertori G., Dittmar M., Donega M., Dorfer C., Gadek T., Espinosa T. A. G., Grab C., Hits D., Lustermann W., Lyon A. -M., Manzoni R. A., Meinhard M. T., Micheli F., Nessi-Tedaldi F., Niedziela J., Pauss F., Perovic V., Perrin G., Pigazzini S., Ratti M. G., Reichmann M., Reissel C., Reitenspiess T., Ristic B., Ruini D., Becerra D. A. S., Schonenberger M., Stampf V., Steggemann J., Olsson M. L. V., Wallny R., Zhu D. H., Amsler C., Bartschi P., Botta C., Brzhechko D., Canelli M. F., Burgo R. D., Heikkila J. K., Huwiler M., Jofrehei A., Kilminster B., Leontsinis S., Macchiolo A., Meiring P., Mikuni V. M., Molinatti U., Neutelings I., Rauco G., Reimers A., Robmann P., Schweiger K., Takahashi Y., Adloff C., Kuo C. M., Lin W., Roy A., Sarkar T., Yu S. S., Ceard L., Chang P., Chao Y., Chen K. F., Chen P. 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Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137fb-1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3fb for a Z′ mass between 0.8 and 4.6Te, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

25. On the disputed $\pi_1(1600)$ resonance and observation of a new iso-vector resonance

Author: Nerling, F.
Subjects: High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract: The COMPASS experiment at CERN delivers new results on the search for exotic mesons. A spin-exotic resonance, the $\pi_1(1600)$, was reported by several experiments in the past. Those observations are, however, still to date highly disputed in the community. Especially the $\rho\pi$ decay channel allows for simultaneous observation of well established and less known resonances in different decay modes. The results from amplitude analysis of diffractively produced $(3\pi)^{-}$ final states show consistently a spin-exotic signal, that appears in agreement with previous observations of the $\pi_1(1600)$. The high-statistics 2008 data sample allows and demands for an extended amplitude analysis method that further disentangles resonant and non-resonant particle production. The present status of analysis of COMPASS data and the observation of a new iso-vector meson $a_1(1420)$ is discussed., Comment: 6 pages, 24 figures, DSPIN-13 Conference Proceedings, to appear in the proceedings of the XV Workshop on High Energy Spin Physics, Dubna, Russia, October 8-12, 2013
Published: 2014

26. Precision spectroscopy with COMPASS and the observation of a new iso-vector resonance

Author: Paul, Stephan
Subjects: High Energy Physics - Experiment, Nuclear Experiment
Abstract: We report on the results of a novel partial-wave analysis based on $50\cdot 10^6$ events from the reaction $\pi^- + p \to \pi^-\pi-^\pi^+ + p_\text{recoil}$ at 190 $\text{GeV/c}$ incoming beam momentum using the COMPASS spectrometer. A separated analysis in bins of $m_{3\pi}$ and four-momentum transfer $t'$ reveals the interference of resonant and non-resonant particle production and allows their spectral separation. Besides well known resonances we observe a new iso-vector meson $a_1(1420)$ at a mass of 1420 $\text{MEV\c}^2$ in the $f_0(980)\pi$ final state only, the origin of which is unclear. We have also examined the structure of the $0^{++}$ $\pi\pi$-isobar in the $J^{PC}=0^{-+}, 1^{++}, 2^{-+}$ three pion waves. This clearly reveals the various $0^{++}$ $\pi\pi$-isobar components and its correlation to the decay of light mesons., Comment: 8 pages, 7 figures
Published: 2013
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27. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at $\sqrt{s}$ = 13TeV

Author: CMS Collaboration, Canelli, Maria Florencia, Kilminster, Benjamin, Caminada, Lea, Botta, Cristina, Bartschi, Pascal, Brzhechko, Danyyl, Wit, Adinda, Del Burgo, Riccardo, Heikkilae, Jaana, Huwiler, Marc, Jofrehei, Arash, Leontsinis, Stefanos, Macchiolo, Anna, Meiring, Peter, Missiroli, Marino, Mikuni, Vinicius, Molinatti, Umberto, Neutelings, Izaak, Rauco, Giorgia, Robmann, Peter, Sanchez Cruz, Sergio, Schweiger, Korbinian, Takahashi, Yuta, et al, CMS Collaboration, Canelli, Maria Florencia, Kilminster, Benjamin, Caminada, Lea, Botta, Cristina, Bartschi, Pascal, Brzhechko, Danyyl, Wit, Adinda, Del Burgo, Riccardo, Heikkilae, Jaana, Huwiler, Marc, Jofrehei, Arash, Leontsinis, Stefanos, Macchiolo, Anna, Meiring, Peter, Missiroli, Marino, Mikuni, Vinicius, Molinatti, Umberto, Neutelings, Izaak, Rauco, Giorgia, Robmann, Peter, Sanchez Cruz, Sergio, Schweiger, Korbinian, Takahashi, Yuta, and et al
Published: 2021

28. Measurements of neutral vector resonance in Higgsless models at the LHC

Author: Asano, Masaki and Shimizu, Yasuhiro
Subjects: High Energy Physics - Phenomenology, High Energy Physics - Experiment
Abstract: In Higgsless models, new vector resonances appear to restore the unitarity of the W_L W_L scattering amplitude without the Higgs boson. In the ideal delocalized three site Higgsless model, one of large prodcution cross section of the neutral vector resonance (Z') at the Large Hadron Collider is the W-associated production, pp \to Z'W \to WWW. Although the dileptonic decay channnel, l\nu l'\nu 'jj, is experimentally clean to search for the Z' signals, it is difficult to reconstruct the Z' invariant mass due to the two neutrinos in the final state. We study collider signatures of Z' using the M_{T2}-Assisted On-Shell (MAOS) reconstruction of the missing neutrino momenta. We show the prospect of the Z' mass determination in the channel, l\nu l'\nu 'jj, at the Large Hadron Collider., Comment: 16 pages, 6 figures, 5 tables; v2: references added, minor corrections, version published in JHEP
Published: 2010
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29. Probing the strong electroweak symmetry breaking in a model with a vector resonance

Author: Gintner, M., Melo, I., and Trpisova, B.
Subjects: High Energy Physics - Phenomenology
Abstract: We systematically study the possibility to probe the physics behind the electroweak symmetry breaking at the LHC assuming new strong interactions being responsible for the effect. The new physics is described by the Higgs-less effective Lagrangian with a vector resonance in the particle spectrum, in addition to the Standard Model fields. We analyze signals of the resonance in the mixing-induced LHC processes pp-> abX, ab=t\bar{t},b\bar{b},t\bar{b},W^+Z,W^+W^-. At this level of our calculations we do not consider further decays of the quarks and of the gauge bosons., Comment: To appear in the proceedings of the 10th Small Triangle Meeting on Theoretical Physics in Medzilaborce, Slovakia, Sep 21-24,2008
Published: 2009

30. Combined analysis of Z' -> t tbar and Z' -> t tbar j production for vector resonance searches at LHC

Author: del Aguila, F., Aguilar-Saavedra, J. A., Moretti, M., Piccinini, F., Pittau, R., and Treccani, M.
Subjects: High Energy Physics - Phenomenology
Abstract: We have implemented a code for Z' + n jets production in ALPGEN, with Z' decays into several final states, including l+ l- and t tbar. The MLM prescription is used for matching the matrix element with the parton shower, including in this way the leading soft and collinear corrections. In order to demonstrate its capabilities, we perform a combined analysis of Z' -> t tbar and Z' -> t tbar j production for a heavy leptophobic gauge boson. It is found that the effect of the extra jet cannot only be accounted for by a K factor multiplying the leading-order cross section. In fact, the combined analysis for Z' -> t tbar and Z' -> t tbar j presented improves the statistical significance of the signal by 25% (8.55 sigma versus 6.77 sigma for a Z' mass of 1 TeV), compared with the results of an inclusive analysis carried out on the same sample of t tbar + t tbar j events., Comment: LaTeX 17 pages, 13 PS figures
Published: 2009
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31. Modelling top partner-vector resonance phenomenology

Author: Juan Yepes and Alfonso Zerwekh
Subjects: Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract: We have analysed the observable consequences of the interactions of spin-1 resonances coupled to the invariant fermionic currents that arise in an SO(5) Composite Higgs set-up. The phenomenology entailed by such interactions is thoroughly analysed by studying heavy vector resonances production and decay modes in the viable resonance mass range. Additionally, the production of double and single-composite fermion final states has been scanned along the fermion mass scale. Such production is mediated by the SM gauge and Higgs interactions, and also by charged and neutral vector resonances. The coupling between the new fermions and vector resonances induces a sizeable effect in the production rates. We use the recent 13 TeV LHC searches for vector-like quarks to constrain our parameter space. Specifically, we explore the allowed regions by analysing the decays of a heavy vector-like quark in the Wb-channel. We conclude that generically the impact of the couplings between the spin-1 and spin-1/2 resonances will substantially reduce the permitted regions, leading us to test the sensitivity of the parametric dependence in the light of exotic matter interactions.
Published: 2019
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32. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Author: Sirunyan, A., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, Milošević, Jovan, Sirunyan, A., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Adžić, Petar, Ćirković, Predrag, Đorđević, Miloš, Milenović, Predrag, and Milošević, Jovan
Abstract: A search is presented for a heavy vector reso- nance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is per- formed in a Lorentz-boosted regime and is based on data col- lected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb−1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7 TeV is excluded at 95% confidence level in models where the heavy vector boson couples predomi- nantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z′ mass between 0.8 and 4.6 TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

33. Rogue waves and mode locking driven by Vector Resonance Multimode instability.

Author: Sergey V. Sergeyev, Hani Kbashi, and Stanislav A. Kolpakov
Published: 2017
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34. A direct current control strategy based on vector resonance controller for shunt active power filter

Author: Chen, Dongdong, Xu, Zhenming, Xiao, Long, Yan, Wenduan, and Guo, Yinbiao
Published: 2022
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35. LHC vector resonance searches in the t t ¯ Z final state

Author: Backović, Mihailo, Flacke, Thomas, Jain, Bithika, and Lee, Seung J.
Published: 2017
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36. Vector-resonance-multimode instability

Author: Sergeyev, S.V., Kbashi, H., Tarasov, N., Loiko, Yu., Kolpakov, S.A., Sergeyev, S.V., Kbashi, H., Tarasov, N., Loiko, Yu., and Kolpakov, S.A.
Abstract: The modulation and multimode instabilities are the main mechanisms which drive spontaneous spatial and temporal patterns formation in a vast number of nonlinear systems ranging from biology to the laser physics. Using Er-doped fiber laser as a test bed, here for the first time we demonstrate both experimentally and theoretically a new type of a low threshold vector resonance multimode instability which inherits features of multimode and modulation instabilities. The same as for the multimode instability, the large number of longitudinal modes can be excited without modes synchronization. To enable modulation instability, we modulate the state of polarization of the lasing signal with the period of the beat length by adjustment of the in-cavity birefringence and the state of polarization of the pump wave. As a result, we show regimes tunability from complex oscillatory to periodic with longitudinal modes synchronization in the case of the resonance matching between beat and cavity lengths. Apart from the interest in laser physics for unlocking tunability and stability of dynamic regimes, the proposed mechanism of the vector resonance multimode instability can be of fundamental interest for nonlinear dynamics of various distributed systems.
Published: 2017

37. Tricking Landau–Yang: How to obtain the diphoton excess from a vector resonance

Author: Mikael Chala, Michael Duerr, Felix Kahlhoefer, and Kai Schmidt-Hoberg
Subjects: Physics, QC1-999
Abstract: We show that contrary to naive expectations the recently observed diphoton excess can be explained by a vector resonance, which decays to a photon and a light scalar s, followed by a decay of the scalar into two photons: Z′→γs→3γ. As the two photons from the scalar decay are highly boosted, the experimental signature is an apparent diphoton final state. In fact all the necessary ingredients are naturally present in Z′ models: Additional fermions with electroweak quantum numbers are required in order to render the theory anomaly free and naturally induce the required effective couplings, while the hidden Higgs which gives mass to the Z′ can be very light. In particular no new coloured states are required in this framework. We also show that in such a setup the width of the resonance can be rather large, while all couplings remain perturbative. Keywords: Mostly weak interactions: beyond standard model
Published: 2016
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38. Search for a heavy vector resonance decaying to a ${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$ boson and a Higgs boson in proton-proton collisions at $\sqrt{s} = 13\,\text {Te}\text {V} $

Author: Matthias Kasemann, Luca Giommi, Cole Lindsey, Paola Salvini, Eddi A De Wolf, Marcos Fernandez, Young-Il Choi, J William Gary, Florian Beaudette, Daniel Arcaro, Christina Wang, Marek Walczak, S. Sánchez Navas, Jose Chinellato, Richard Cavanaugh, Tobias Pook, Jay Hauser, Andrei Starodumov, Isidro Gonzalez Caballero, Marcella Diemoz, Andrea Gelmi, Neil Schroeder, Atanu Modak, Marco Cipriani, Peter Elmer, Olena Hlushchenko, Tomasz Gadek, Marco Rovere, Alexander Richards, Jorge Berenguer Antequera, Marco Toliman Lucchini, Mauricio Thiel, Peter Timothy Cox, Torben Lange, Jason Sang Hun Lee, Michael Mulhearn, P. Klabbers, Alberto Sánchez Hernández, Christophe Royon, Elizabeth Sexton-Kennedy, Bobae Kim, Matthias Wolf, Gabriella Pugliese, Kevin Lannon, Jordan Nash, Sung Keun Park, Bugra Bilin, Kati Lassila-Perini, Mariana Araujo, Luigi Guiducci, Gregory R Snow, Sophie Wuyckens, Edy Ayala, Igor Volobouev, Hirak Bandyopadhyay, Özlem Özçelik, Jie Xiao, Ilya Kravchenko, Jeroen Hegeman, Paolo Ronchese, Badder Marzocchi, Sanjay Kumar Swain, Marc M Baarmand, Silvia Maselli, Rhys Taus, Valeri Valentinovitch Mitsyn, Joseph Taylor, Yi Wang, Mikhail Dubinin, Serguei Afanasiev, Petra Merkel, De Hua Zhu, Si Xie, Natale Demaria, Angelo Giacomo Zecchinelli, Malte Backhaus, Pushpalatha C Bhat, Fatma Aydogmus Sen, Ian Laflotte, Wei Li, Robert Stone, Simone Calzaferri, Angela Giraldi, Mohammad Alhusseini, Maria Teresa Grippo, Anatoli Zarubin, Suat Ozkorucuklu, Kenyi Hurtado Anampa, Younes Otarid, Guenakh Mitselmakher, Ran Bi, Federica Maria Simone, Wei Xie, Rainer Wallny, Yang Yang, Winston Ko, Katarzyna Wichmann, Reza Goldouzian, Mohd Nizam Yusli, Vivan Nguyen, Vinaya Krishnan Muraleedharan Nair Bindhu, Hannes Sakulin, Arnab Purohit, Tilman Rohe, Jing Wang, Sara Nabili, Andrey Popov, Doyeong Kim, Rafael Eduardo Sosa Ricardo, Alibordi Muhammad, Artur Kalinowski, Karla Josefina Pena Rodriguez, Hyejin Kwon, James Wetzel, S. Seif El Nasr-storey, Nicholas Wardle, Matthew Jones, Alexei Raspereza, Christoph Heidecker, Tao Huang, Jordan Damgov, D. Di Croce, Peter Hansen, Basile Vermassen, Davide Zuolo, Giacomo Sguazzoni, Alan Campbell, Johann Rauser, Olivér Surányi, Renato Potenza, Jay Mathew Lawhorn, Claude Amsler, Andrea Bellora, Laurent Favart, Troy Mulholland, Cristian Pena, Seungkyu Ha, Thomas Reis, Martin Lipinski, Luigi Benussi, Daniele Fasanella, Andris Skuja, Salvatore Nuzzo, Philippe Bloch, Martina Vit, Ivica Puljak, Hans Reithler, Guenter Eckerlin, Ben Bylsma, Roberto Tenchini, Meng Xiao, Zhengyun You, Andrew Mehta, Armen Tumasyan, Jacobo Konigsberg, Young Do Oh, Ivan Amos Cali, Bryan Cardwell, Jose M Hernandez, Paula Eerola, Manoj Sharan, Lukas Lechner, Dmitry Philippov, Sridhara Dasu, Emilio Meschi, Peter Robmann, Grace Cummings, Dipika Dash, Norbert Neumeister, Yiwen Wen, Dylan Hsu, Kinga Anna Wozniak, Stephen Sanders, Wesley H Smith, Mauro De Palma, Menglei Sun, Pierre Piroué, Raman Khurana, Jeremy Mans, Aliya Nigamova, Alexandros Attikis, Diego Alejandro Sanz Becerra, Bradley Cox, Laurent Forthomme, Lorenzo Bianchini, Philip Baringer, Roy Montalvo, Hamed Bakhshiansohi, George Stephans, Frank Würthwein, Jordi Duarte Campderros, Angela Taliercio, Paul Kyberd, Sema Zahid, Manas Maity, Alexi Mestvirishvili, Sandra Consuegra Rodríguez, Kristian Harder, Ulrich Goerlach, Vladimir Petrov, Nicolaus Kratochwil, Ravi Janjam, Siddharth Narayanan, Anton Karneyeu, Leonard Apanasevich, Weinan Si, Pritam Palit, Andrew Levin, Anton Stepennov, Andrew Loeliger, Sergei Gleyzer, Simon Christoph Schuler, Steve Nahn, Wren Vetens, Pietro Vischia, Paolo Capiluppi, Frigyes Nemes, James Rohlf, Matti J Kortelainen, Cheng-Chieh Peng, Efe Yazgan, Frank Hartmann, Luciano Orsini, Luca Pacher, Gouranga Kole, Claire Shepherd-Themistocleous, Michael Wassmer, Antonis Agapitos, Alessandro Rossi, Daniel Denegri, Magda Diamantopoulou, Gage Dezoort, Konstantinos Theofilatos, Sandor Czellar, Yasser Assran, Marius Preuten, Dmitry Eliseev, Joao Seixas, Francisco Matorras, Carlos Avila, Nils Faltermann, Duong Nguyen, Vladyslav Danilov, Ricardo Eusebi, Lukas Layer, Zhicai Zhang, Camille Camen, Rui Xiao, Kevin Burkett, Ibrahim Soner Zorbakir, Maksym Titov, Federico Ferri, Douglas Berry, Igor Azhgirey, János Karancsi, Thomas N. Williams, Matthias Schröder, Joosep Pata, Colin Bernet, Vladimir Rusinov, Alexandra Carvalho Antunes De Oliveira, David Vannerom, Nadia Pastrone, Frank Golf, Jochen Schieck, Antonio Cassese, Kevin Flöh, Charalambos Nicolaou, Niki Saoulidou, Zhengcheng Tao, Sercan Sen, Andre Govinda Stahl Leiton, Eduard De La Cruz-Burelo, Christopher Mcginn, Ka Hei Martin Kwok, Theodor Christian Herwig, Filippo Errico, Deepak Kumar Sahoo, Daniel Robert Marlow, Tiziano Camporesi, Ana Ovcharova, Allison Reinsvold Hall, Brent Stone, Seema Sharma, Andrea Venturi, Ta-Wei Wang, Piet Verwilligen, Stefan Spanier, Hartmut Stadie, Natascha Krammer, Andreas Hinzmann, Marcin Konecki, Artur Lobanov, Nathaniel Pastika, Kyle Tos, Antonio Delgado Peris, Ioannis Evangelou, Lisa Borgonovi, Paul Dauncey, Kenichi Hatakeyama, Anna Woodard, Louise Skinnari, Vito Palladino, Nural Akchurin, Daniele Pedrini, Marco Costa, Fan Xia, Dietrich Liko, Manuel Giffels, Ugur Kiminsu, Mykhailo Dalchenko, Tahir Javaid, Pavel Bunin, Quan Wang, Benedikt Maier, Tamás Álmos Vámi, Sungwoong Cho, Catherine Vander Velde, Hannu Siikonen, Gustavo Gil Da Silveira, Jingyu Luo, Guo-Ming Chen, Arabella Martelli, Soureek Mitra, Muhammad Ahmad, Giuseppe Iaselli, Suman Bala Beri, Vincenzo Mastrapasqua, Yves Sirois, Michael Benjamin Andrews, Simone Paoletti, Georgi Sultanov, Armando Bermúdez Martínez, Abhijith Gandrakota, Evan Wolfe, David Cutts, Gian Luca Pinna Angioni, Kevin Stenson, Aurélien Carle, Prafulla Kumar Behera, Nikolai Golubev, Jean-Louis Faure, Gerrit Patrick Van Onsem, Ivan Heredia-De La Cruz, Brian Francis, Paolo Checchia, Alberto Messineo, John Almond, Shirin Chenarani, Martti Raidal, Brian Dorney, Riccardo Andrea Manzoni, Cristina Oropeza Barrera, Christian Veelken, Mariarosaria D'Alfonso, Mario Galanti, Zoltan Szillasi, Jussi Viinikainen, Edoardo Bossini, Andrey Uzunian, Christopher Palmer, Alice Bean, Balazs Ujvari, Yuri Musienko, Damir Lelas, Jozsef Molnar, Valerio Re, Dajeong Jeon, Federico Vazzoler, Subash Chandra Behera, Costas Foudas, Devdatta Majumder, Anna Zacharopoulou, David Hamilton, Nabin Poudyal, Sharon Hagopian, Sarah Freed, Alicia Calderon, Ralf Ulrich, Juliette Alimena, Frank Jensen, Paul Asmuss, Marco Bozzo, Dennis Schwarz, Ekaterina Kuznetsova, Lloyd Stanley Durkin, Hevjin Yarar, Vincenzo Innocente, Mattia Lizzo, Marcel Rieger, Patrick Asenov, Sudeshna Banerjee, Vladimir Andreev, Martina Malberti, Suchandra Dutta, Aruna Nayak, Robert Hirosky, Achim Stahl, Gervasio Gomez, Saikat Karmakar, Diego Matos Figueiredo, Yuan Chen, Guillaume Bourgatte, Demetra Tsiakkouri, Shawn Zaleski, Giulio Mandorli, Anne-Marie Magnan, Wagner Carvalho, Nur Zulaiha Jomhari, Vivian O'Dell, Seyed Mohsen Etesami, Metin Yalvac, Stephan Lammel, Tagir Aushev, Daniel Noonan, Olaf Behnke, Jay Dittmann, Sandra Oliveros, Alfredo Gurrola, Ufuk Guney Tok, Markus Klute, Matteo Maria Defranchis, Alessandro Braghieri, Nicola Minafra, Johannes Schulz, Kyungwook Nam, Maryam Zeinali, Patrick Jarry, Alexander Spiridonov, Vladislav Borshch, Francesca Nessi-Tedaldi, Joel Goldstein, Ron Lipton, Yongho Jeong, Luciano Ristori, Andreas Werner Jung, William Tabb, Chandiprasad Kar, Milena Misheva, Luigi Calligaris, Kevin Pedro, Junho Kim, Anders Ryd, Gavin Davies, Thong Nguyen, Anna Benecke, Suvankar Roy Chowdhury, Alexey Vorobyev, Haifa Rejeb Sfar, Jean-Baptiste Sauvan, Shamik Ghosh, Gigi Rolandi, Thomas Schuh, Hans Van Haevermaet, David Overton, Stefano Argiro, Tiehui Liu, Silvano Tosi, Tom Cornelis, Cristian Baldenegro Barrera, Zhenbin Wu, Bhawna Gomber, Marcello Mannelli, Christian Schwanenberger, Sang Il Pak, Shao Min Tan, Francesco Brivio, Marco Musich, Ryan Heller, Dominique Gigi, Rishi Patel, Maxime Guilbaud, Daniel Treille, Ioannis Papadopoulos, Efstathios Paganis, David Seith, Erica Brondolin, Patricia Rebello Teles, M. Mohammadi Najafabadi, Daniele Ruini, Michail Bachtis, Margaret Eminizer, Francesco Fienga, Geonhee Oh, Tejinder Virdee, Nicolò Tosi, Daniel Tapia Takaki, Pawan Kumar Netrakanti, Evgueni Tcherniaev, Wing Yan Wong, Camilla Galloni, Juan Pablo Fernández Ramos, Fanbo Meng, Jhovanny Mejia Guisao, Caroline Collard, Raffaello D'Alessandro, Slawek Tkaczyk, Hanwen Wang, Roger Rusack, Marc Dejardin, Charles Harrington, Emil Sørensen Bols, Panja-Riina Luukka, Roberto Salerno, Vladimir Makarenko, Scarlet Norberg, Tielige Mengke, Christopher Brew, Gintautas Tamulaitis, Lothar At Bauerdick, Leonardo Giannini, Raghunath Pradhan, Bisnupriya Sahu, Anadi Canepa, Dario Menasce, Kelvin Mei, D. De Jesus Damiao, Sebastian Wuchterl, Olga Kodolova, Ram Krishna Dewanjee, Bora Isildak, Bennett Marsh, Greg Landsberg, Cécile Caillol, Giuseppe Della Ricca, Sw. Banerjee, Burin Asavapibhop, Xunwu Zuo, Andrea Piccinelli, Robert M Harris, James Bueghly, Matthew Nguyen, Elliot Hughes, Gurpreet Singh Chahal, Qiang Li, Andrei Sobol, Gabriella Pasztor, Sebastian Templ, Andrew Buccilli, Garrett Funk, Pedro G Mercadante, Yonghoon Lee, Nabarun Dev, Viacheslav Bunichev, Johan Borg, Dhanush Anil Hangal, Archana Sharma, Sung Won Lee, Vitalii Okhotnikov, Petar Adzic, Irene Dutta, Charis Kleio Koraka, Maria Margherita Obertino, Daniel Winterbottom, Vinay Hegde, Saptaparna Bhattacharya, Samila Muthumuni, David Zou, Finn Feindt, Andrey Korytov, Nairit Sur, Tamas Novak, Min Suk Kim, Vipin Bhatnagar, Daniele Bonacorsi, Nicholas Haubrich, Kevin Nash, Thea Klaeboe Aarrestad, Georgios Anagnostou, Melody A. Swartz, Maxwell Chertok, Danek Kotlinski, Jordan Martins, Antonio María Pérez-Calero Yzquierdo, Yildiray Komurcu, Philippe Busson, Arun Kumar, Marc Huwiler, Alexander Lanev, Colin Fallon, Daniele Spiga, Piotr Traczyk, Susan Dittmer, Georgios Daskalakis, David Jonathan Hofman, Vincenzo Daponte, Andrey Belyaev, Julia Thom, Ece Aşılar, Denis Gelé, Chang-Seong Moon, Catherine Schiber, Mauro Emanuele Dinardo, Carmen Albajar, Sven Dildick, Nhan Viet Tran, Mohammad Abrar Wadud, Christof Roland, Yao Yao, David Colling, Gourab Saha, Valentina Dutta, Finn Rebassoo, Cecilia Elena Gerber, D. Domínguez Damiani, P. Chang, Eduardo De Moraes Gregores, Ashfaq Ahmad, Anna Teresa Meneguzzo, Giovanni Petrucciani, Ernesto Migliore, Hans-Jürgen Simonis, John Alison, Aliakbar Ebrahimi, Hans-Christian Kaestli, Aleksandr Iuzhakov, Shubham Pandey, Wei Shi, Andrea Castro, Thomas Klijnsma, Mikhail Gavrilenko, Nadezda Chernyavskaya, Vladimir Korenkov, Ashim Roy, Andre Frankenthal, Evgueni Vlasov, Karl Ehataht, Qianying Guo, Enrico Robutti, Michael Krohn, Jeremie Alexandre Merlin, Piotr Zalewski, Juska Pekkanen, Xinmei Niu, Diego Beghin, Andrej Saibel, Oleg Teryaev, Vitaly Smirnov, Dragos Velicanu, Rohith Saradhy, Nuno Leonardo, Lucia Silvestris, Neeti Parashar, German Martinez, Cristina Botta, Jonathon Langford, Viesturs Veckalns, David Brunner, Marek Gruchala, Simranjit Singh Chhibra, Ali Eren Simsek, David Barney, Aleksandra Lelek, Eda Eskut, Thorben Quast, Po-Hsun Chen, Stefano Mersi, Mykyta Haranko, Vukasin Milosevic, Nikkie Deelen, Radia Redjimi, Sándor Lökös, Tariq Aziz, Dave M Newbold, Daniel Savoiu, Marko Dragicevic, Willard Johns, Monika Bharti, George Karathanasis, Joern Schwandt, Yen-Jie Lee, Pablo De Castro Manzano, Kevin Black, Kamuran Dilsiz, Seema Bahinipati, Paolo Rumerio, Lorenzo Uplegger, William T. Ford, Alexander Fröhlich, Kenneth Bloom, Pedrame Bargassa, Nick Amin, Kira Burt, Gui Nyun Kim, Hao Qiu, Muhammad Imran Malik Awan, Jennifer Ngadiuba, Miguel Medina Jaime, Claudia Pistone, Wolfgang Adam, Pierre Van Hove, Prasant Kumar Rout, Riccardo Paramatti, Andrea Giammanco, Priyanka Kumari, Doga Gulhan, Louis Lyons, Hugues Lattaud, Alberto Escalante Del Valle, Shivali Malhotra, Gunter Quast, Tanmay Mudholkar, Ennio Monteil, Aldo Penzo, Nicolas Tonon, Artur Gottmann, Aimilios Ioannou, Stephanie Beauceron, Amina Zghiche, Emily MacDonald, Danilo Meuser, Andrew Gilbert, Ridhi Chawla, Meenakshi Narain, Mirena Ivova Paneva, Thomas Eichhorn, Mar Barrio Luna, Alessandro Thea, Cristina Fernandez Bedoya, Isabel Pedraza, Sunil Somalwar, Mark Raymond Adams, Ulrich Husemann, Valentina Sola, Fabio Monti, Matteo Cremonesi, Naimuddin, Jaehoon Lim, Nitish Dhingra, Stephen Butalla, Sudhir Malik, Rizki Syarif, Ia Iashvili, Roberto Seidita, You-ying Li, Monoranjan Guchait, Samuel Bein, Daniel Spitzbart, Jean-Roch Vlimant, Brajesh C Choudhary, Paul David Luckey, Andrea Trapote, A. Álvarez Fernández, Marc Dünser, Janek Bechtel, Kurtis F Johnson, Bayram Tali, Merijn Van De Klundert, Klaus Rabbertz, Sebastiano Albergo, Hui Wang, Tyler Mitchell, Igor Lokhtin, Timothy Koeth, Myriam Schönenberger, Antonio Di Pilato, Jan Krolikowski, Luiz Mundim, Kun Shi, Zachary Lesko, Robert M Brown, Brooks McMaster, Mithat Kaya, Merve Ince, Suyong Choi, Etiennette Auffray, Maurizio Biasini, D. R. Muller, Sinan Sagir, Marta Felcini, Negin Shafiei, Duccio Abbaneo, Matteo Bonanomi, Isa Dumanoglu, Elizabeth Locci, Ilaria Vai, Gabriele Benelli, Somnath Choudhury, Ruchi Chudasama, Todd Adams, Andrew Wightman, Prakash Thapa, Olmo Cerri, Olivier Davignon, Dmitri Konstantinov, Arnd Meyer, Dario Bisello, Pascal Paganini, Francisco Yumiceva, Ritva Kinnunen, Jonas Rembser, Petar Maksimovic, David Stickland, Daniel Pitzl, Joaquin Emilo Siado, Maksat Haytmyradov, Paolo Montagna, Nicola Turini, Cristina Mantilla, Jaana Kristiina Heikkilä, Nikitas Loukas, Pierluigi Paolucci, Manuel Alejandro Segura Delgado, Marcos Cerrada, Eleni Erodotou, Mehar Ali Shah, Michele Gallinaro, Tommaso Isidori, Junquan Tao, Peter Wittich, Francesco Fabozzi, Chad Flores, Stefaan Tavernier, Diego Ciangottini, Kelci Mohrman, Jaebeom Park, Andrea Perrotta, Jose Monroy, Fuqiang Wang, Justin Pilot, David Ja Cockerill, Wolfgang Lange, Gianni Masetti, Erik Gottschalk, Andrea Delgado, Duncan Leggat, Giacomo Bruno, Ian Mcalister, Manuel Calderon De La Barca Sanchez, Michele Bianco, Antoine Lesauvage, Rainer Mankel, Alice Florent, Gregor Kasieczka, Oleksii Toldaiev, Adinda De Wit, Marco Meschini, Lourdes Urda Gómez, Andrea Massironi, Izzeddin Suat Donertas, Livia Soffi, Mariana Shopova, Eric Christian Chabert, Christopher Seez, Andrea García Alonso, Ada Solano, Mehdi Rahmani, Ricardo Lopez-Fernandez, Wolfgang Funk, Thomas Berger, Othmane Bouhali, Barbara Chazin Quero, Hannsjoerg Artur Weber, Gordon H. Hanson, Michel Della Negra, Sandhya Jain, Subir Sarkar, Furong Yan, Zhangqier Wang, Raffaele Gerosa, Huaqiao Zhang, Alexander Ledovskoy, Vincent J Smith, W. A. T. Wan Abdullah, Deshitha Chamikara Wickramarathna Dhammage, Jamal Rorie, Jason Gilmore, Andrei Gritsan, Leszek Grzanka, Marco Paganoni, Saswati Nandan, Mani Tripathi, Rachel Bartek, Marco Peruzzi, Usama Hussain, Owen Rosser Long, Sergei Gninenko, Senka Duric, Benjamin Tannenwald, Guler Karapinar, Sandro Fonseca De Souza, Samuel May, Muzamil Ahmad Bhat, Giuseppe Latino, Mauro Donegà, Igor Bayshev, Yajun Mao, Mikhail Kirsanov, Biagio Rossi, Kirika Uchida, Andrew Beretvas, Otto Hindrichs, Aashaq Shah, T. 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Sanchez Cruz, Harvey B Newman, Jeffrey Berryhill, Lucas Corcodilos, Antonin Kveton, Mauro Menichelli, Clément Grimault, Geetanjali Chaudhary, Luca Perniè, Roland Horisberger, Yuan Chao, Michele Arneodo, Garvita Agarwal, Ka Tung Lau, Leonid Didukh, Brieuc Francois, Paul Edmund Karchin, Thomas Madlener, Christopher Rogan, Akram Khan, Nicolas Chanon, Helena Malbouisson, Camelia Mironov, Tongguang Cheng, Valentina Avati, Brian L Winer, Anton Petrov, Danyer Pérez Adán, Mehmet Özgür Sahin, Donato Creanza, Marc Dobson, Rudy Ceccarelli, Alessandro Giassi, Giacomo Ortona, Benedikt Vormwald, Ilknur Hos, Riccardo Salvatico, Maurizio Pierini, J. N. Butler, Fabiola Vazquez Valencia, Paolo Lariccia, Dmitry Sosnov, Rudolf Fruehwirth, Nick Van Remortel, Chad Freer, Stefan Piperov, Mohit Gola, Wajid Ali Khan, David Cussans, Inna Kucher, Jelena Mijuskovic, Markus Spanring, Soumya Mukherjee, Luis Ignacio Estevez Banos, Daniel R Claes, Tuure Tuuva, Margaret Zientek, Unki Yang, Liam Wezenbeek, Yuta Takahashi, Ozgun Kara, Ramkrishna Sharma, Daniel Gastler, Sioni Summers, Mikko Voutilainen, Sumit Keshri, Alain Givernaud, Seth Moortgat, Giorgia Rauco, Nancy Marinelli, Muhammad Waqas, Izaak Neutelings, Predrag Milenovic, Peter R Hobson, Kin Ho Lo, Vladislav Shalaev, Daniel Diaz, Sudarshan Paramesvaran, Victor Daniel Elvira, Bilal Kiani, Stephane Cooperstein, Plamen Iaydjiev, Minseok Oh, Francesca Cavallari, Stefano Belforte, Massimo Casarsa, Thomas Müller, Andrés G Delannoy, Christopher Hill, Jennifer Chu, Pawel de Barbaro, Viktor Khristenko, Vilius Cepaitis, Gaël Perrin, Anne-mazarine Lyon, Umesh Joshi, Alexander Dermenev, Jared Sturdy, Doris Eckstein, Achim Geiser, Batoul Diab, Dong Ho Moon, Nikolai Krasnikov, Sami Lehti, Adish Vartak, Umberto Molinatti, Matej Roguljic, Javier Cuevas, Marcello Abbrescia, Danila Tlisov, Brandon Bonham, Valentina Mariani, Felipe Torres Da Silva De Araujo, Arash Jofrehei, Samuel Nathan Webb, Giovanni Mocellin, Ivan Shvetsov, Igor Golutvin, Mircho Rodozov, Francesco Pandolfi, Serguei Volkov, Maria Aldaya Martin, Nicola Bacchetta, Attila Racz, Roberta Arcidiacono, Paul Sheldon, Yuichi Kubota, Gilles De Lentdecker, Andreas Albert, Christian Schnaible, Jonathan Fulcher, Anatoli Pashenkov, Avto Kharchilava, Mikhail Ignatenko, Tapio Lampén, Javier Andres Brochero Cifuentes, James Alexander, Lukasz Kreczko, Fabrizio Fabbri, Christoph Wissing, Sanghyun Ko, Norraphat Srimanobhas, Riccardo Di Maria, Dermot Moran, Byung-Sik Hong, Mahmod Moussa Abdelkhalek Gadallah, Michael Hildreth, Oscar Gonzalez Lopez, Seth Cooper, Tanmay Sarkar, Matthew Joyce, Simone Giani, Rosamaria Venditti, Anastasia Karavdina, Bożena Boimska, Kerem Cankocak, Harrison Prosper, Semra Turkcapar, Viktor Kutzner, Linda Finco, Alfredo Castaneda Hernandez, Mingshui Chen, Mario Deile, Stephen Robert Wagner, Kak Wong, Daniele Trocino, David Walter, Alexander Dierlamm, Minna Leonora Vesterbacka Olsson, Michal Szleper, Philippe Gras, Chia-Ming Kuo, Candan Dozen, Scott Thomas, Piero Giorgio Verdini, Ludivine Ceard, Michael Wayne Arenton, Siddhesh Sawant, Xuyang Gao, Shalini Thakur, James John Brooke, Cédric Prieels, Praveen Chandra Tiwari, F. Fiori, Martina Ressegotti, Álvaro Navarro Tobar, Matevz Tadel, Yannik Rath, Oleksii Turkot, Fabrizio Gasparini, Michele Selvaggi, Gulsen Onengut, Viktor Matveev, Predrag Cirkovic, Clemens Lange, Erika Garutti, Santiago Folgueras, George Alverson, Roman Kogler, Satoshi Hasegawa, Andrew Wildridge, Mark Pesaresi, Claudia Ciocca, Jangbae Lee, Didier Contardo, Jeong-Eun Lee, Kaitlin Salyer, Agostino De Iorio, Markus Seidel, Vaia Papadimitriou, Vineet Kumar, Giancarlo Mantovani, Carlo Battilana, Sezen Sekmen, Inseok Yoon, K. Osterberg, Ziheng Chen, Maximilian Heindl, Claus Kleinwort, Alexander Savin, Caleb Fangmeier, Vinicius Massami Mikuni, Quentin Ingram, Igor Vorobiev, Martin Delcourt, Francesco Fallavollita, Julie Managan Hogan, Panos A Razis, John Gabriel Acosta, Samuel Baxter, Sifu Luo, Anne-Catherine Le Bihan, Tyler Lam, Nadja Strobbe, Jean-Laurent Agram, Anthony Moeller, Lauren Hay, Jim Freeman, Brent Yates, Geum Bong Yu, Alberto Bragagnolo, Anthony Lefeld, Begona De La Cruz, Aristotelis Kyriakis, Cecilia Uribe Estrada, Welathantri Gd Dharmaratna, Ferenc Sikler, Dayong Wang, Mauro Verzetti, Antonio Vagnerini, Mario Kadastik, Ashley Parker, Colin Jessop, Manuel Olmedo Negrete, Changwoo Joo, Alessandro Calandri, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg (UNISTRA)-Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA))-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université de Haute-Alsace (UHA) Mulhouse - Colmar (Université de Haute-Alsace (UHA)), Institut de Physique Nucléaire de Lyon (IPNL), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université de Lyon, Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), CMS, Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université de Strasbourg (UNISTRA)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)
Subjects: Physics and Astronomy (miscellaneous), 13000 GeV-cms, Hadron, heavy [vector boson], 01 natural sciences, Vector boson, resonance: heavy, electron: pair production, heavy [resonance], Z': mass: lower limit, scattering [p p], [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], resonance: decay modes, Boson, Physics, Large Hadron Collider, neutrino: pair production, CMS, triplet [model], mass dependence, 3. Good health, channel cross section: branching ratio: upper limit, muon: pair production, mass: lower limit [Z\'], Higgs boson, mass: lower limit [Z'], Neutrino, colliding beams [p p], narrow resonance, vector boson: heavy, Particle Physics - Experiment, Particle physics, p p: scattering, CERN Lab, production [resonance], resonance: vector, pair production [neutrino], Standard Model, vector [resonance], 0103 physical sciences, vector boson: coupling, ddc:530, model: triplet, pair production [electron], pair production [muon], 010306 general physics, coupling [vector boson], S056ZOT, Engineering (miscellaneous), Condensed Matter::Quantum Gases, branching ratio: upper limit [channel cross section], 010308 nuclear & particles physics, Branching fraction, model [Z'], Z': model, High Energy Physics::Phenomenology, leptonic decay [Z0], decay modes [resonance], hadronic decay [Higgs particle], Higgs particle: hadronic decay, Z0: leptonic decay, High Energy Physics::Experiment, model [Z\'], p p: colliding beams, resonance: production, experimental results
Abstract: A search is presented for a heavy vector resonance decaying into a $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson and the standard model Higgs boson, where the $${\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}$$ Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137$$\,\text {fb}^{-1}$$ fb - 1 . Upper limits are derived on the production of a narrow heavy resonance $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ , and a mass below 3.5 and 3.7$$\,\text {Te}\text {V}$$ Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3$$\,\text {fb}$$ fb for a $${\mathrm{{{\mathrm{Z}}_{\mathrm{}}^{\mathrm{}}}}}_{\mathrm{}}^{\mathrm{\prime }}$$ Z ′ mass between 0.8 and 4.6$$\,\text {Te}\text {V}$$ Te , respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

39. Impact of a colored vector resonance on the collider constraints for a toplike top partner

Author: Tirtha Sankar Ray, Santosh Kumar Rai, and Sayan Dasgupta
Subjects: Physics, Particle physics, 010308 nuclear & particles physics, Atlas (topology), Electroweak interaction, High Energy Physics::Phenomenology, Propagator, FOS: Physical sciences, Parameter space, 01 natural sciences, Vector resonance, High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Colored, 0103 physical sciences, High Energy Physics::Experiment, Symmetry breaking, 010306 general physics
Abstract: In this work we reappraise the collider constraints from leptonic final states on the vectorlike colored top partners taking into account the impact of exotic colored vector resonances. These colored states are intrinsic to a broad class of models that employ a strongly interacting sector to drive electroweak symmetry breaking. We translate the recent results in the {\sl monolepton + jets} channel as reported by CMS with an integrated luminosity of 35.8 fb$^{-1}$, and {\sl dilepton + jets} and {\sl trilepton + jets} channels as reported by ATLAS with an integrated luminosity of 36.1 fb$^{-1}$ to constrain the parameter space of these class of models. We also comment on the impact and modification of the derived constraints due to the expected fatness of the colored vector resonance, when accounted for beyond the narrow-width approximation by simulating the full one-particle irreducible resummed propagator., Comment: Extensive changes in text, Matches published version
Published: 2020

40. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at sqrt(s)=13TeV

Author: Sirunyan, A. M., Tumasyan, A., Adam, W., Bergauer, T., Dragicevic, M., Ero, J., Valle, A. E. D., Fruhwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Pitters, F. M., Rad, N., Schieck, J., Schofbeck, R., Spanring, M., Templ, S., Waltenberger, W., Wulz, C. -E., Zarucki, M., Chekhovsky, V., Litomin, A., Makarenko, V., Gonzalez, J. S., Darwish, M. R., De Wolf, E. A., Di Croce, D., Janssen, X., Kello, T., Lelek, A., Pieters, M., Sfar, H. R., Van Haevermaet, H., Van Mechelen, P., Van Putte, S., Van Remortel, N., Blekman, F., Bols, E. S., Chhibra, S. S., D'Hondt, J., De Clercq, J., Lontkovskyi, D., Lowette, S., Marchesini, I., Moortgat, S., Morton, A., Muller, D., Python, Q., Tavernier, S., Van Doninck, W., Van Mulders, P., Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Dorney, B., Favart, L., Grebenyuk, A., Kalsi, A. K., Makarenko, I., Moureaux, L., Petre, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Vander Velde, C., Vanlaer, P., Vannerom, D., Wezenbeek, L., Cornelis, T., Dobur, D., Gruchala, M., Khvastunov, I., Niedziela, M., Roskas, C., Skovpen, K., Tytgat, M., Verbeke, W., Vermassen, B., Vit, M., Bruno, G., Bury, F., Caputo, C., David, P., Delaere, C., Delcourt, M., Donertas, I. S., Giammanco, A., Lemaitre, V., Mondal, K., Prisciandaro, J., Taliercio, A., Teklishyn, M., Vischia, P., Wertz, S., Wuyckens, S., Alves, G. A., Hensel, C., Moraes, A., Junior, W. L. A., Chagas, E. B. B. D., Malbouisson, H. B., Carvalho, W., Chinellato, J., Coelho, E., Da Costa, E. M., Da Silveira, G. G., De Jesus Damiao, D., De Souza, S. F., Martins, J., Figueiredo, D. M., Jaime, M. M., Herrera, C. M., Mundim, L., Nogima, H., Teles, P. R., Rosas, L. J. S., Santoro, A., Do Amaral, S. M. S., Sznajder, A., Thiel, M., Da Silva De Araujo, F. T., Pereira, A. V., Bernardes, C. A., Calligaris, L., Tomei, T. R. F. P., Gregores, E. M., Lemos, D. S., Mercadante, P. G., Novaes, S. F., Padula, S. S., Aleksandrov, A., Antchev, G., Atanasov, I., Hadjiiska, R., Iaydjiev, P., Misheva, M., Rodozov, M., Shopova, M., Sultanov, G., Dimitrov, A., Ivanov, T., Litov, L., Pavlov, B., Petkov, P., Petrov, A., Cheng, T., Fang, W., Guo, Q., Wang, H., Yuan, L., Ahmad, M., Bauer, G., Hu, Z., Wang, Y., Yi, K., Chapon, E., Chen, G. M., Chen, H. S., Chen, M., Javaid, T., Kapoor, A., Leggat, D., Liao, H., Liu, Z. -A., Sharma, R., Spiezia, A., Tao, J., Thomas-wilsker, J., Wang, J., Zhang, H., Zhang, S., Zhao, J., Agapitos, A., Ban, Y., Chen, C., Huang, Q., Levin, A., Li, Q., Lu, M., Lyu, X., Mao, Y., Qian, S. J., Wang, D., Wang, Q., Xiao, J., You, Z., Gao, X., Xiao, M., Avila, C., Cabrera, A., Florez, C., Fraga, J., Sarkar, A., Delgado, M. A. S., Jaramillo, J., Guisao, J. M., Ramirez, F., Alvarez, J. D. R., Gonzalez, C. A. S., Arbelaez, N. V., Giljanovic, D., Godinovic, N., Lelas, D., Puljak, I., Antunovic, Z., Kovac, M., Sculac, T., Brigljevic, V., Ferencek, D., Majumder, D., Roguljic, M., Starodumov, A., Susa, T., Ather, M. W., Attikis, A., Erodotou, E., Ioannou, A., Kole, G., Kolosova, M., Konstantinou, S., Mousa, J., Nicolaou, C., Ptochos, F., Razis, P. A., Rykaczewski, H., Saka, H., Tsiakkouri, D., Finger, M., Kveton, A., Tomsa, J., Ayala, E., Jarrin, E. C., Zeid, S. A., Assran, Y., Salama, E., Lotfy, A., Mahmoud, M. A., Bhowmik, S., De Oliveira, A. C. A., Dewanjee, R. K., Ehataht, K., Kadastik, M., Raidal, M., Veelken, C., Eerola, P., Forthomme, L., Kirschenmann, H., Osterberg, K., Voutilainen, M., Brucken, E., Garcia, F., Havukainen, J., Karimaki, V., Kim, M. S., Kinnunen, R., Lampen, T., Lassila-Perini, K., Lehti, S., Linden, T., Siikonen, H., Tuominen, E., Tuominiemi, J., Luukka, P., Tuuva, T., Amendola, C., Besancon, M., Couderc, F., Dejardin, M., Denegri, D., Faure, J. L., Ferri, F., Ganjour, S., Givernaud, A., Gras, P., de Monchenault, G. H., Jarry, P., Lenzi, B., Locci, E., Malcles, J., Rander, J., Rosowsky, A., Sahin, M. O., Savoy-Navarro, A., Titov, M., G. B., Yu, Ahuja, S., Beaudette, F., Bonanomi, M., Perraguin, A. B., Busson, P., Charlot, C., Davignon, O., Diab, B., Falmagne, G., de Cassagnac, R. G., Hakimi, A., Kucher, I., Lobanov, A., Perez, C. M., Nguyen, M., Ochando, C., Paganini, P., Rembser, J., Salerno, R., Sauvan, J. B., Sirois, Y., Zabi, A., Zghiche, A., Agram, J. -L., Andrea, J., Bloch, D., Bourgatte, G., Brom, J. -M., Chabert, E. C., Collard, C., Fontaine, J. -C., Gele, D., Goerlach, U., Grimault, C., Bihan, A. -C. L., Van Hove, P., Asilar, E., Beauceron, S., Bernet, C., Boudoul, G., Camen, C., Carle, A., Chanon, N., Contardo, D., Depasse, P., El Mamouni, H., Fay, J., Gascon, S., Gouzevitch, M., Ille, B., Jain, S., Laktineh, I. B., Lattaud, H., Lesauvage, A., Lethuillier, M., Mirabito, L., Shchablo, K., Torterotot, L., Touquet, G., Vander Donckt, M., Viret, S., Adamov, G., Tsamalaidze, Z., Feld, L., Klein, K., Lipinski, M., Meuser, D., Pauls, A., Preuten, M., Rauch, M. P., Schulz, J., Teroerde, M., Eliseev, D., Erdmann, M., Fackeldey, P., Fischer, B., Ghosh, S., Hebbeker, T., Hoepfner, K., Keller, H., Mastrolorenzo, L., Merschmeyer, M., Meyer, A., Mocellin, G., Mondal, S., Mukherjee, S., Noll, D., Novak, A., Pook, T., Pozdnyakov, A., Rath, Y., Reithler, H., Roemer, J., Schmidt, A., Schuler, S. C., Sharma, A., Wiedenbeck, S., Zaleski, S., Dziwok, C., Flugge, G., Ahmad, W. H., Hlushchenko, O., Kress, T., Nowack, A., Pistone, C., Pooth, O., Roy, D., Sert, H., Stahl, A., Ziemons, T., Petersen, H. A., Martin, M. A., Asmuss, P., Babounikau, I., Baxter, S., Behnke, O., Martinez, A. B., Anuar, A. A. B., Borras, K., Botta, V., Brunner, D., Campbell, A., Cardini, A., Connor, P., Rodriguez, S. C., Danilov, V., De Wit, A., Defranchis, M. M., Didukh, L., Damiani, D. D., Eckerlin, G., Eckstein, D., Eichhorn, T., Banos, L. I. E., Gallo, E., Geiser, A., Giraldi, A., Grohsjean, A., Guthoff, M., Harb, A., Jafari, A., Jomhari, N. Z., Jung, H., Kasem, A., Kasemann, M., Kaveh, H., Kleinwort, C., Knolle, J., Krucker, D., Lange, W., Lenz, T., Lidrych, J., Lipka, K., Lohmann, W., Madlener, T., Mankel, R., Melzer-Pellmann, I. -A., Metwally, J., Meyer, A. B., Meyer, M., Missiroli, M., Mnich, J., Mussgiller, A., Myronenko, V., Otarid, Y., Adan, D. P., Pflitsch, S. K., Pitzl, D., Raspereza, A., Saggio, A., Saibel, A., Savitskyi, M., Scheurer, V., Schwanenberger, C., Singh, A., Ricardo, R. E. S., Tonon, N., Turkot, O., Vagnerini, A., Van De Klundert, M., Walsh, R., Walter, D., Wen, Y., Wichmann, K., Wissing, C., Wuchterl, S., Zenaiev, O., Zlebcik, R., Aggleton, R., Bein, S., Benato, L., Benecke, A., De Leo, K., Dreyer, T., Ebrahimi, A., Eich, M., Feindt, F., Frohlich, A., Garbers, C., Garutti, E., Gunnellini, P., Haller, J., Hinzmann, A., Karavdina, A., Kasieczka, G., Klanner, R., Kogler, R., Kutzner, V., Lange, J., Lange, T., Malara, A., Niemeyer, C. E. N., Nigamova, A., Rodriguez, K. J. P., Rieger, O., Schleper, P., Schumann, S., Schwandt, J., Schwarz, D., Sonneveld, J., Stadie, H., Steinbruck, G., Vormwald, B., Zoi, I., Bechtel, J., Berger, T., Butz, E., Caspart, R., Chwalek, T., De Boer, W., Dierlamm, A., Droll, A., El Morabit, K., Faltermann, N., Floh, K., Giffels, M., Gottmann, A., Hartmann, F., Heidecker, C., Husemann, U., Katkov, I., Keicher, P., Koppenhofer, R., Maier, S., Metzler, M., Mitra, S., Muller, T., Musich, M., Quast, G., Rabbertz, K., Rauser, J., Savoiu, D., Schafer, D., Schnepf, M., Schroder, M., Seith, D., Shvetsov, I., Simonis, H. J., Ulrich, R., Wassmer, M., Weber, M., Wolf, R., Wozniewski, S., Anagnostou, G., Asenov, P., Daskalakis, G., Geralis, T., Kyriakis, A., Loukas, D., Paspalaki, G., Stakia, A., Diamantopoulou, M., Karasavvas, D., Karathanasis, G., Kontaxakis, P., Koraka, C. K., Manousakis-katsikakis, A., Panagiotou, A., Papavergou, I., Saoulidou, N., Theofilatos, K., Tziaferi, E., Vellidis, K., Vourliotis, E., Bakas, G., Kousouris, K., Papakrivopoulos, I., Tsipolitis, G., Zacharopoulou, A., Evangelou, I., Foudas, C., Gianneios, P., Katsoulis, P., Kokkas, P., Manitara, K., Manthos, N., Papadopoulos, I., Strologas, J., Bartok, M., Csanad, M., Gadallah, M. M. A., Lokos, S., Major, P., Mandal, K., Mehta, A., Pasztor, G., Suranyi, O., Veres, G. I., Bencze, G., Hajdu, C., Horvath, D., Sikler, F., Veszpremi, V., Vesztergombi, G., Czellar, S., Karancsi, J., Molnar, J., Szillasi, Z., Teyssier, D., Raics, P., Trocsanyi, Z. L., Ujvari, B., Csorgo, T., Nemes, F., Novak, T., Choudhury, S., Komaragiri, J. R., Kumar, D., Panwar, L., Tiwari, P. C., Bahinipati, S., Dash, D., Kar, C., Mal, P., Mishra, T., Bindhu, V. K. M. N., Nayak, A., Sahoo, D. K., Sur, N., Swain, S. K., Bansal, S., Beri, S. 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M., Khakzad, M., Najafabadi, M. M., Felcini, M., Grunewald, M., Abbrescia, M., Aly, R., Aruta, C., Colaleo, A., Creanza, D., De Filippis, N., De Palma, M., Di Florio, A., Di Pilato, A., Elmetenawee, W., Fiore, L., Gelmi, A., Gul, M., Iaselli, G., Ince, M., Lezki, S., Maggi, G., Maggi, M., Margjeka, I., Mastrapasqua, V., Merlin, J. A., My, S., Nuzzo, S., Pompili, A., Pugliese, G., Ranieri, A., Selvaggi, G., Silvestris, L., Simone, F. M., Venditti, R., Verwilligen, P., Abbiendi, G., Battilana, C., Bonacorsi, D., Borgonovi, L., Braibant-Giacomelli, S., Campanini, R., Capiluppi, P., Castro, A., Cavallo, F. R., Ciocca, C., Cuffiani, M., Dallavalle, G. M., Diotalevi, T., Fabbri, F., Fanfani, A., Fontanesi, E., Giacomelli, P., Giommi, L., Grandi, C., Guiducci, L., Iemmi, F., Meo, S. L., Marcellini, S., Masetti, G., Navarria, F. L., Perrotta, A., Primavera, F., Rossi, A. M., Rovelli, T., Siroli, G. 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C., Hirschauer, J., Jayatilaka, B., Jindariani, S., Johnson, M., Joshi, U., Klabbers, P., Klijnsma, T., Klima, B., Kortelainen, M. J., Lammel, S., Lincoln, D., Lipton, R., Liu, M., Liu, T., Lykken, J., Maeshima, K., Mason, D., Mcbride, P., Merkel, P., Mrenna, S., Nahn, S., O'Dell, V., Papadimitriou, V., Pedro, K., Pena, C., Prokofyev, O., Ravera, F., Hall, A. R., Ristori, L., Schneider, B., Sexton-Kennedy, E., Smith, N., Soha, A., Spalding, W. J., Spiegel, L., Stoynev, S., Strait, J., Taylor, L., Tkaczyk, S., Tran, N. V., Uplegger, L., Vaandering, E. W., Weber, H. A., Woodard, A., Acosta, D., Avery, P., Bourilkov, D., Cadamuro, L., Cherepanov, V., Errico, F., Field, R. D., Guerrero, D., Joshi, B. M., Kim, M., Konigsberg, J., Korytov, A., K. H., Lo, Matchev, K., Menendez, N., Mitselmakher, G., Rosenzweig, D., Shi, K., Sturdy, J., Zuo, X., Adams, T., Askew, A., Diaz, D., Habibullah, R., Hagopian, S., Hagopian, V., Johnson, K. F., Khurana, R., Kolberg, T., Martinez, G., Prosper, H., Schiber, C., Yohay, R., Zhang, J., Baarmand, M. M., Butalla, S., Elkafrawy, T., Hohlmann, M., Noonan, D., Rahmani, M., Saunders, M., Yumiceva, F., Adams, M. R., Apanasevich, L., Gonzalez, H. B., Cavanaugh, R., Chen, X., Dittmer, S., Evdokimov, O., Gerber, C. E., Hangal, D. A., Hofman, D. J., Mills, C., Oh, G., Roy, T., Tonjes, M. B., Varelas, N., Viinikainen, J., Wang, X., Wu, Z., Ye, Z., Alhusseini, M., Dilsiz, K., Durgut, S., Gandrajula, R. P., Haytmyradov, M., Khristenko, V., Koseyan, O. K., Merlo, J. -P., Mestvirishvili, A., Moeller, A., Nachtman, J., Ogul, H., Onel, Y., Ozok, F., Penzo, A., Snyder, C., Tiras, E., Wetzel, J., Amram, O., Blumenfeld, B., Corcodilos, L., Eminizer, M., Gritsan, A. V., Kyriacou, S., Maksimovic, P., Mantilla, C., Roskes, J., Swartz, M., Vami, T. A., Barrera, C. B., Baringer, P., Bean, A., Bylinkin, A., Isidori, T., Khalil, S., King, J., Krintiras, G., Kropivnitskaya, A., Lindsey, C., Minafra, N., Murray, M., Rogan, C., Royon, C., Sanders, S., Schmitz, E., Takaki, J. D. T., Williams, J., Wilson, G., Duric, S., Ivanov, A., Kaadze, K., Kim, D., Maravin, Y., Mitchell, T., Modak, A., Mohammadi, A., Rebassoo, F., Wright, D., Adams, E., Baden, A., Baron, O., Belloni, A., Eno, S. C., Feng, Y., Hadley, N. J., Jabeen, S., Jeng, G. Y., Kellogg, R. G., Koeth, T., Mignerey, A. C., Nabili, S., Seidel, M., Skuja, A., Tonwar, S. C., Wang, L., Wong, K., Abercrombie, D., Allen, B., Bi, R., Brandt, S., Busza, W., Cali, I. A., D'Alfonso, M., Ceballos, G. G., Goncharov, M., Harris, P., Hsu, D., Hu, M., Klute, M., Kovalskyi, D., Krupa, J., Lee, Y. -J., Luckey, P. D., Maier, B., Marini, A. C., Mcginn, C., Mironov, C., Narayanan, S., Niu, X., Paus, C., Rankin, D., Roland, C., Roland, G., Shi, Z., Stephans, G. S. F., Sumorok, K., Tatar, K., Velicanu, D., Wang, T. W., Wang, Z., Wyslouch, B., Chatterjee, R. M., Evans, A., Hansen, P., Hiltbrand, J., Krohn, M., Kubota, Y., Lesko, Z., Mans, J., Revering, M., Rusack, R., Saradhy, R., Schroeder, N., Strobbe, N., Wadud, M. A., Acosta, J. G., Oliveros, S., Bloom, K., Claes, D. R., Fangmeier, C., Finco, L., Golf, F., Fernandez, J. R. G., Joo, C., Kravchenko, I., Siado, J. E., Snow, G. R., Tabb, W., Yan, F., Agarwal, G., Bandyopadhyay, H., Harrington, C., Hay, L., Iashvili, I., Kharchilava, A., Mclean, C., Nguyen, D., Pekkanen, J., Rappoccio, S., Roozbahani, B., Alverson, G., Barberis, E., Freer, C., Haddad, Y., Hortiangtham, A., Li, J., Madigan, G., Marzocchi, B., Morse, D. M., Nguyen, V., Orimoto, T., Parker, A., Skinnari, L., Tishelman-Charny, A., Wamorkar, T., Wang, B., Wisecarver, A., Wood, D., Bueghly, J., Chen, Z., Gilbert, A., Gunter, T., Hahn, K. A., Odell, N., Schmitt, M. H., Sung, K., Velasco, M., Bucci, R., Dev, N., Goldouzian, R., Hildreth, M., Anampa, K. H., Jessop, C., Karmgard, D. J., Lannon, K., Loukas, N., Marinelli, N., Mcalister, I., Meng, F., Mohrman, K., Musienko, Y., Ruchti, R., Siddireddy, P., Taroni, S., Wayne, M., Wightman, A., Wolf, M., Zygala, L., Alimena, J., Bylsma, B., Cardwell, B., Durkin, L. S., Francis, B., Hill, C., Lefeld, A., Winer, B. L., Yates, B. R., Bonham, B., Das, P., Dezoort, G., Elmer, P., Greenberg, B., Haubrich, N., Higginbotham, S., Kalogeropoulos, A., Kopp, G., Kwan, S., Lange, D., Lucchini, M. T., Luo, J., Marlow, D., Mei, K., Ojalvo, I., Olsen, J., Palmer, C., Piroue, P., Stickland, D., Tully, C., Norberg, S., Barnes, V. E., Chawla, R., Das, S., Gutay, L., Jones, M., Jung, A. W., Negro, G., Neumeister, N., Peng, C. C., Piperov, S., Purohit, A., Qiu, H., Schulte, J. F., Stojanovic, M., Trevisani, N., Wang, F., Wildridge, A., Xiao, R., Xie, W., Dolen, J., Parashar, N., Baty, A., Dildick, S., Ecklund, K. M., Freed, S., Geurts, F. J. M., Kilpatrick, M., Li, W., Padley, B. P., Redjimi, R., Roberts, J., Rorie, J., Shi, W., Leiton, A. G. S., Bodek, A., de Barbaro, P., Demina, R., Dulemba, J. L., Fallon, C., Ferbel, T., Galanti, M., Garcia-Bellido, A., Hindrichs, O., Khukhunaishvili, A., Ranken, E., Taus, R., Chiarito, B., Chou, J. P., Gandrakota, A., Gershtein, Y., Halkiadakis, E., Hart, A., Heindl, M., Hughes, E., Kaplan, S., Karacheban, O., Laflotte, I., Lath, A., Montalvo, R., Nash, K., Osherson, M., Salur, S., Schnetzer, S., Somalwar, S., Stone, R., Thayil, S. A., Thomas, S., Acharya, H., Delannoy, A. G., Spanier, S., Bouhali, O., Dalchenko, M., Delgado, A., Eusebi, R., Gilmore, J., Huang, T., Kamon, T., Luo, S., Malhotra, S., Mueller, R., Overton, D., Pernie, L., Rathjens, D., Safonov, A., Akchurin, N., Damgov, J., Hegde, V., Kunori, S., Lamichhane, K., Mengke, T., Muthumuni, S., Peltola, T., Undleeb, S., Volobouev, I., Whitbeck, A., Appelt, E., Greene, S., Gurrola, A., Janjam, R., Johns, W., Maguire, C., Melo, A., Ni, H., Padeken, K., Romeo, F., Sheldon, P., Tuo, S., Velkovska, J., Arenton, M. W., Cox, B., Cummings, G., Hakala, J., Hirosky, R., Joyce, M., Ledovskoy, A., Li, A., Neu, C., Tannenwald, B., Wolfe, E., Xia, F., Karchin, P. E., Poudyal, N., Thapa, P., Black, K., Bose, T., Buchanan, J., Caillol, C., Dasu, S., De Bruyn, I., Everaerts, P., Galloni, C., He, H., Herndon, M., Herve, A., Hussain, U., Lanaro, A., Loeliger, A., Loveless, R., Sreekala, J. M., Mallampalli, A., Pinna, D., Savin, A., Shang, V., Smith, W. H., Teague, D., Trembath-reichert, S., and Vetens, W.
Subjects: CMS, New Physics Search, Vector Resonance, Z and H final state
Published: 2021

41. Rogue waves and mode locking driven by Vector Resonance Multimode instability

Author: Sergeyev, Sergey V., Kbashi, Hani, Kolpakov, Stanislav A., Sergeyev, Sergey V., Kbashi, Hani, and Kolpakov, Stanislav A.
Abstract: Modulation instabilities discovered more than fifty and hundred fifty years ago created since then a framework for study complexity of different wave phenomena including turbulence and rogue waves. Using Erbium-doped fiber laser without any previously studied mode-locking mechanisms, here for the first time we demonstrate both experimentally and theoretically a new type of modulation instability, namely Vector Resonance Multimode Instability, leading to tunability of the laser dynamics from turbulence including rogue waves to the stable pulse train similar to the laser mode-locking regime.
Published: 2017

42. LHC vector resonance searches in the $t\bar{t} Z$ final state

Author: UCL - SST/IRMP - Institut de recherche en mathématique et physique, Backovic, Mihailo, UCL - SST/IRMP - Institut de recherche en mathématique et physique, and Backovic, Mihailo
Abstract: LHC searches for BSM resonances in $l^+ l^-, \, jj, \, t\bar{t}, \gamma \gamma$ and $VV$ final states have so far not resulted in discovery of new physics. Current results set lower limits on mass scales of new physics resonances well into the $\mathcal{O}(1)$ TeV range, assuming that the new resonance decays dominantly to a pair of Standard Model particles. While the SM pair searches are a vital probe of possible new physics, it is important to re-examine the scope of new physics scenarios probed with such final states. Scenarios where new resonances decay dominantly to final states other than SM pairs, even though well theoretically motivated, lie beyond the scope of SM pair searches. In this paper we argue that LHC searches for (vector) resonances beyond two particle final states would be useful complementary probes of new physics scenarios. As an example, we consider a class of composite Higgs models, and identify specific model parameter points where the color singlet, electrically neutral vector resonance $\rho_0$ decays dominantly not to a pair of SM particles, but to a fermionic top partner $T_{f1}$ and a top quark, with $T_{f1} \rightarrow tZ$. We show that dominant decays of $\rho_0 \rightarrow T_{f1} t$ in the context of Composite Higgs models are possible even when the decay channel to a pair of $T_{f1}$ is kinematically open. Our analysis deals with scenarios where both $m_\rho$ and $m_{T_{f1}}$ are of $\mathcal{O}(1)$ TeV, leading to highly boosted $t\bar{t}Z$ final state topologies. We show that the particular composite Higgs scenario we consider is discoverable at the LHC13 with as little as 30 fb$^{-1}$, while being allowed by other existing experimental constraints.
Published: 2017

43. Hiding the Vector Resonance Signal Hiding the Vector Resonance Signal

Author: Mikulas Gintner and Josef Juran
Subjects: electroweak symmetry breaking, effective lagrangian, vector resonances, new strong interactions, Transportation and communications, HE1-9990, Science, Transportation engineering, TA1001-1280
Abstract: We investigate how the interplay of the direct and mixing-induced couplings of the hypothetical SU(2)L+R vector triplet resonance to the third quark generation can hide the resonance signal in ,tb tb , and / bt tb channels. The vector resonances are assumed to represent bound states of hypothetical strongly-interacting new physics, the extension of the Standard model.
Published: 2014
Full Text: View/download PDF

44. Measurements of neutral vector resonance in Higgsless models at the LHC

Author: Asano, Masaki and Shimizu, Yasuhiro
Published: 2011
Full Text: View/download PDF

45. Peak Locations and Relative Phase of Different Decay Modes of the Axial Vector Resonance in Diffractive Production

Author: Berger, Edmond
Published: 2015
Full Text: View/download PDF

46. Vector resonance X1(2900) and its structure

Author: Agaev, S.S., primary, Azizi, K., additional, and Sundu, H., additional
Published: 2021
Full Text: View/download PDF

47. On the transition form factors of the axial-vector resonance f1(1285) and its decay into e+e−

Author: Zanke, Marvin, primary, Hoferichter, Martin, additional, and Kubis, Bastian, additional
Published: 2021
Full Text: View/download PDF

48. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Author: Cms, Collaboration, Blekman, Freya, Bols, Emil Sørensen, Chhibra, Simranjit Singh, D'Hondt, Jorgen, De Clercq, Jarne Theo, Lontkovskyi, Denys, Lowette, Steven, Marchesini, Ivan, Moortgat, Seth, Morton, Alexander, Müller, Denise, Python, Quentin, Tavernier, Stefaan, Van Doninck, Walter, Van Mulders, Petra, Physics, Elementary Particle Physics, Faculty of Sciences and Bioengineering Sciences, and Vriendenkring VUB
Subjects: Condensed Matter::Quantum Gases, hep-ex, High Energy Physics::Phenomenology, High Energy Physics::Experiment
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137fb-1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3fb for a Z′ mass between 0.8 and 4.6Te, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

49. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at s=13 TeV

Author: The CMS collaboration, Sirunyan, A. M., Tumasyan, A., Eerola, P., Forthomme, Laurent, Kirschenmann, H., Österberg, K., Voutilainen, M., Brücken, Erik, Garcia, F., Havukainen, J., Heikkilä, Jaana, Karimäki, Veikko, Kim, Minsuk, Kinnunen, R., Lampén, T., Lassila-Perini, K., Laurila, S., Lehti, S., Lindén, T., Luukka, P., Pekkanen, Juska, Siikonen, H., Tuominen, E., Tuominiemi, J., Viinikainen, Jussi, Tuuva, T., Department of Physics, and Helsinki Institute of Physics
Subjects: Condensed Matter::Quantum Gases, High Energy Physics::Phenomenology, High Energy Physics::Experiment, PLUS PLUS, 114 Physical sciences
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137 fb-1. Upper limits are derived on the production of a narrow heavy resonance Z ', and a mass below 3.5 and 3.7 Te is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z ' model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3 fb for a Z ' mass between 0.8 and 4.6 Te, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay.
Published: 2021

50. Search for a heavy vector resonance decaying to a Z boson and a Higgs boson in proton-proton collisions at √s=13Te

Author: Sirunyan, AM, Tumasyan, A, Adam, W, Bergauer, T, Dragicevic, M, Erö, J, Valle, AED, Frühwirth, R, Jeitler, M, Krammer, N, Lechner, L, Liko, D, Mikulec, I, Pitters, FM, Rad, N, Schieck, J, Schöfbeck, R, Spanring, M, Templ, S, Waltenberger, W, Wulz, CE, Zarucki, M, Chekhovsky, V, Litomin, A, Makarenko, V, Gonzalez, JS, Darwish, MR, De Wolf, EA, Di Croce, D, Janssen, X, Kello, T, Lelek, A, Pieters, M, Sfar, HR, Van Haevermaet, H, Van Mechelen, P, Van Putte, S, Van Remortel, N, Blekman, F, Bols, ES, Chhibra, SS, D’Hondt, J, De Clercq, J, Lontkovskyi, D, Lowette, S, Marchesini, I, Moortgat, S, Morton, A, Müller, D, Python, Q, Tavernier, S, Van Doninck, W, Van Mulders, P, Beghin, D, Bilin, B, Clerbaux, B, De Lentdecker, G, Dorney, B, Favart, L, Grebenyuk, A, Kalsi, AK, Makarenko, I, Moureaux, L, Pétré, L, Popov, A, Postiau, N, Starling, E, Thomas, L, Vander Velde, C, Vanlaer, P, Vannerom, D, Wezenbeek, L, Cornelis, T, Dobur, D, Gruchala, M, Khvastunov, I, Niedziela, M, Roskas, C, Skovpen, K, Tytgat, M, Verbeke, W, Vermassen, B, Vit, M, Bruno, G, Bury, F, Caputo, C, David, P, Delaere, C, Delcourt, M, Donertas, IS, Giammanco, A, Lemaitre, V, Mondal, K, Prisciandaro, J, Taliercio, A, Teklishyn, M, Vischia, P, Wertz, S, Wuyckens, S, and Alves, GA
Subjects: Condensed Matter::Quantum Gases, High Energy Physics::Phenomenology, High Energy Physics::Experiment
Abstract: A search is presented for a heavy vector resonance decaying into a Z boson and the standard model Higgs boson, where the Z boson is identified through its leptonic decays to electrons, muons, or neutrinos, and the Higgs boson is identified through its hadronic decays. The search is performed in a Lorentz-boosted regime and is based on data collected from 2016 to 2018 at the CERN LHC, corresponding to an integrated luminosity of 137fb−1. Upper limits are derived on the production of a narrow heavy resonance Z′, and a mass below 3.5 and 3.7TeV is excluded at 95% confidence level in models where the heavy vector boson couples predominantly to fermions and to bosons, respectively. These are the most stringent limits placed on the Heavy Vector Triplet Z′ model to date. If the heavy vector boson couples exclusively to standard model bosons, upper limits on the product of the cross section and branching fraction are set between 23 and 0.3fb for a Z′ mass between 0.8 and 4.6TeV, respectively. This is the first limit set on a heavy vector boson coupling exclusively to standard model bosons in its production and decay. SCOAP3
Published: 2021

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