MA TRẬN KHỐI LƯỢNG NEUTRINO VỚI CẤU TRÚC ZERO TỪ CƠ CHẾ SEESAW VÀ LEPTOGENESIS by Nguyễn Thanh Phong, Lê Tấn Phát

“…Một hệ quả vật lý của cơ chế seesaw đó là các quá trình phân rã phi cân bằng của các RHN tạo ra bất đối xứng số lepton. Nhờ vào quá trình sphaleron, bất đối xứng leptonton chuyển thành bất đối xứng vật chất - phản vật chất của vũ trụ (Baryon Asymmetry of the Universe ? …”
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Dark Matter Candidates with Dark Energy Interiors Determined by Energy Conditions by Irina Dymnikova

“…A nontrivial observational signature of all DM candidates with de Sitter interiors predicted by analysis of dynamical equations is the induced proton decay in an underground detector like IceCUBE, due to non-conservation of baryon and lepton numbers in their GUT scale false vacuum interiors.…”
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NLO QCD predictions for off-shell t t ¯ W $$ t\overline{t}W $$ production in association with a light jet at the LHC by Huan-Yu Bi, Manfred Kraus, Minos Reinartz, Malgorzata Worek

“…We concentrate on the multi-lepton decay channel at the LHC with s $$ \sqrt{s} $$ = 13 TeV. …”
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Deeply virtual Compton scattering in the tensor-pomeron approach by Piotr Lebiedowicz, Otto Nachtmann, Antoni Szczurek

“…Our findings may be checked in future lepton-nucleon scattering experiments in the low-x regime, for instance, at a future Electron-Ion Collider at the BNL (EIC), and, if LHeC is realized, at the LHC.…”
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Searching for sbottom LSP at the LHC by Paulina Knees, Essodjolo Kpatcha, Iñaki Lara, Daniel E. López-Fogliani, Carlos Muñoz

“…The sbottoms are pair produced at the LHC, decaying to a lepton and a top quark or a neutrino and a bottom quark. …”
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Explaining anomalies of B-physics, muon $$g-2$$ g - 2 and W mass in R-parity violating MSSM with seesaw mechanism by Min-Di Zheng, Feng-Zhi Chen, Hong-Hao Zhang

“…Furthermore, this model framework can be tested in future experiments covering, e.g., the predicted lepton flavor violations (LFV) at Belle II and the Future Circular Collider with $$e^+e^-$$ e + e - beams (FCC-ee), as well as the heavy neutrinos at future colliders.…”
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Dark matter from a radiative inverse seesaw majoron model by Cesar Bonilla, A.E. Cárcamo Hernández, Bastián Díaz Sáez, Sergey Kovalenko, Juan Marchant González

“…Furthermore, we provide parameter space regions allowed by current experimental constraints coming from the dark matter relic abundance, (in)direct detection, and charged lepton flavor violation.…”
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The $$R^2$$ R 2 -Higgs inflation with two Higgs doublets by Sung Mook Lee, Tanmoy Modak, Kin-ya Oda, Tomo Takahashi

“…Indirect evidences may also emerge at the LHCb and Belle-II experiments, however, to probe the quasi degenerate mass spectra one would likely require high luminosity LHC or future lepton colliders such as the International Linear Collider and the Future Circular Collider.…”
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Bubble-assisted leptogenesis by Eung Jin Chun, Tomasz P. Dutka, Tae Hyun Jung, Xander Nagels, Miguel Vanvlasselaer

“…Their sudden and violent mass gain allows the neutrinos to become thermally decoupled, and the lepton asymmetry generated from their decay can be, in principle, free from the strong wash-out processes that conventional leptogenesis scenarios suffer from, albeit at the cost of new washout channels. …”
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Lighting up the LHC with Dark Matter by Sebastian Baum, Marcela Carena, Tong Ou, Duncan Rocha, Nausheen R. Shah, Carlos E. M. Wagner

“…Interestingly, “radiative” decays of Wino-like neutralinos into the lightest neutralino and a photon are enhanced, whereas decays into leptons are suppressed. While these decay patterns weaken the reach of multi-lepton searches at the LHC, the radiative decay opens a new window for probing dark matter at the LHC through the exploration of parameter space regions beyond those currently accessible. …”
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Search for a light charged Higgs boson in the decay channel H[superscript +] → c[bar over s] in t[bar over t] events using pp collisions at √s = 7 TeV with the ATLAS detector by Taylor, Frank E

“…The other top quark decays to Wb, where the W boson then decays into a lepton (e/μ) and a neutrino. The data were recorded in pp collisions at √s = 7 TeV by the ATLAS detector at the LHC in 2011, and correspond to an integrated luminosity of 4.7 fb[superscript −1]. …”
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Search for the production of single vector-like and excited quarks in the Wt final state in pp collisions at √s =TeV with the ATLAS detector by Taylor, Frank E

“…Events with one or two leptons, and one, two or three jets are selected with the additional requirement that at least one jet contains a b-quark. …”
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Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in √s=8  TeV proton-proton collisions using the ATLAS detector... by ATLAS Collaboration, Taylor, Frank E

“…The measurement is performed for t[t with a line over it] events in the lepton+jets channel. The cross-section is reported as a function of the hadronically decaying top quark transverse momentum for values above 300 GeV. …”
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Precision measurement of and search for dark matter in the transverse momentum spectra of Z bosons by Hsu, Dylan George.

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Search for resonances decaying to a pair of Higgs bosons in the bb¯$$ \overline{\mathrm{b}} $$qq¯$$ \overline{\mathrm{q}} $$’ℓν final state in proton-proton collisions at s$$ \sqrt... by Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Brandstetter, J., Dragicevic, M., Erö, J., Escalante Del Valle, A., Flechl, M., Frühwirth, R., Jeitler, M., Krammer, N., Krätschmer, I., Liko, D., Madlener, T., Mikulec, I.

“…The search is performed for resonances with a mass between 0.8 and 3.5 TeV using events in which one Higgs boson decays into a bottom quark pair and the other decays into two W bosons that subsequently decay into a lepton, a neutrino, and a quark pair. The Higgs boson decays are reconstructed with techniques that identify final state quarks as substructure within boosted jets. …”
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Search for a charged Higgs boson decaying into top and bottom quarks in events with electrons or muons in proton-proton collisions at s$$ \sqrt{\mathrm{s}} $$ = 13 TeV by Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Brandstetter, J., Dragicevic, M., Erö, J., Escalante Del Valle, A., Flechl, M., Frühwirth, R., Jeitler, M., Krammer, N., Krätschmer, I., Liko, D., Madlener, T., Mikulec, I.

“…Events are selected by the presence of a single isolated charged lepton (electron or muon) or an opposite-sign dilepton (electron or muon) pair, categorized according to the jet multiplicity and the number of jets identified as originating from b quarks. …”
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HE-LHC: The High-Energy Large Hadron Collider by Abada, A., Abbrescia, M., AbdusSalam, S. S, Abdyukhanov, I., Abelleira Fernandez, J., Abramov, A., Aburaia, M., Acar, A. O, Adzic, P. R, Agrawal, P., Aguilar-Saavedra, J. A, Aguilera-Verdugo, J. J, Aiba, M., Aichinger, I., Aielli, G., Akay, A., Akhundov, A., Aksakal, H., Albacete, J. L, Albergo, S.

“…The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. …”
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FCC-hh: The Hadron Collider by Abada, A., Abbrescia, M., AbdusSalam, S. S, Abdyukhanov, I., Abelleira Fernandez, J., Abramov, A., Aburaia, M., Acar, A. O, Adzic, P. R, Agrawal, P., Aguilar-Saavedra, J. A, Aguilera-Verdugo, J. J, Aiba, M., Aichinger, I., Aielli, G., Akay, A., Akhundov, A., Aksakal, H., Albacete, J. L, Albergo, S.

“…The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100 km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. …”
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Search for physics beyond the standard model in multilepton final states in proton-proton collisions at s$$ \sqrt{s} $$ = 13 TeV by Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Dragicevic, M., Erö, J., Escalante Del Valle, A., Flechl, M., Frühwirth, R., Jeitler, M., Krammer, N., Krätschmer, I., Liko, D., Madlener, T., Mikulec, I., Rad, N., Schieck, J.

“…The heavy fermions may be manifested as an excess of events with large values of leptonic transverse momenta or missing transverse momentum. …”
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Strong constraints on the b → sγ photon polarisation from B0 → K*0e+e− decays by Aaij, R., Abellán Beteta, C., Ackernley, T., Adeva, B., Adinolfi, M., Afsharnia, H., Aidala, C. A, Aiola, S., Ajaltouni, Z., Akar, S., Albrecht, J., Alessio, F., Alexander, M., Alfonso Albero, A., Aliouche, Z.

“…The A T Re $$ {A}_{\mathrm{T}}^{\mathrm{Re}} $$ observable, which is related to the lepton forward-backward asymmetry, is measured to be A T Re $$ {A}_{\mathrm{T}}^{\mathrm{Re}} $$ = −0.06 ± 0.08 ± 0.02. …”
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