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We introduce a model-independent framework to reinterpret Belle II results using only public data, analytically reconstructing the mapping between true and reconstructed kinematic variables within the statistically dominant Inclusive…

High Energy Physics - Phenomenology · Physics 2026-05-08 Merna Abumusabh , Giulio Dujany , Diego Guadagnoli , Axel Iohner , Claudio Toni

We construct the minimal dark matter models in the left-right symmetric extensions of the standard model (SM), where the gauge symmetry SU(3)$_C\times$SU(2)$_L\times$SU(2)$_R\times$U(1)$_{B-L}$ is broken into its subgroup…

High Energy Physics - Phenomenology · Physics 2016-02-17 P. Ko , Takaaki Nomura

Belle II has recently reported the new measurement ${\cal B}(B^+\to K^+\nu\bar\nu)=(2.3\pm0.7)\times 10^{-5}$ \cite{Belle-II:2023esi} which is two times larger than their previous result (although consistent within errors) and about…

High Energy Physics - Phenomenology · Physics 2024-03-25 Xiao-Gang He , Xiao-Dong Ma , German Valencia

$L_\mu -L_\tau$ gauge boson ($Z'$) with a mass in the MeV to GeV region can resolve not only the muon $g-2$ excess, but also the gap in the high-energy cosmic neutrino spectrum at IceCube. It was recently proposed that such a light gauge…

High Energy Physics - Phenomenology · Physics 2017-11-29 Chuan-Hung Chen , Takaaki Nomura

Rare decays mediated by $b \to s \nu \bar \nu$ transitions have been reported by the Belle II experiment. The branching ratio of the decay $B^+ \to K^+ \nu \bar \nu$ is found to be enhanced with respect to the standard model value. If taken…

High Energy Physics - Phenomenology · Physics 2023-12-15 Rigo Bause , Hector Gisbert , Gudrun Hiller

We propose an extension of the standard model with an extra U(1)' abelian symmetry, three Higgs doublets and one Higgs singlet, where the new U(1)' charges are flavour non-universal. As a result, the model introduces an enlarger particle…

High Energy Physics - Phenomenology · Physics 2018-08-29 R. Martinez , F. Ochoa , J. M. Quimbayo

We study scalar and fermionic crossing two-component dark matter (C2CDM) models with $ U(1)_X $ dark gauge symmetry. This $ U(1)_X $ gauge symmetry is broken via the dark Higgs mechanism of a dark Higgs field $\Phi$ and the dark photon…

High Energy Physics - Phenomenology · Physics 2022-02-28 P. Ko , Chih-Ting Lu , Ui Min

We study an effective theory beyond the standard model (SM) where either of two additional gauge singlets, a Majorana fermion and a real scalar, constitutes all or some fraction of dark matter. In particular, we focus on the masses of the…

High Energy Physics - Phenomenology · Physics 2019-05-22 Wen Yin

Dedicated underground experiments searching for dark matter have little sensitivity to GeV and sub-GeV masses of dark matter particles. We show that the decay of B mesons to K(K^*) and missing energy in the final state can be an efficient…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chris Bird , Paul Jackson , Robert Kowalewski , Maxim Pospelov

Theories beyond the standard model often predict the existence of an additional neutral boson, the $Z^{\prime}$. Using data collected by the Belle II experiment during 2018 at the SuperKEKB collider, we perform the first searches for the…

High Energy Physics - Experiment · Physics 2020-04-07 Belle II Collaboration , I. Adachi , P. Ahlburg , H. Aihara , N. Akopov , A. Aloisio , N. Anh Ky , D. M. Asner , H. Atmacan , T. Aushev , V. Aushev , T. Aziz , V. Babu , S. Baehr , P. Bambade , Sw. Banerjee , V. Bansal , M. Barrett , J. Baudot , J. Becker , P. K. Behera , J. V. Bennett , E. Bernieri , F. U. Bernlochner , M. Bertemes , M. Bessner , S. Bettarini , F. Bianchi , D. Biswas , A. Bozek , M. Bračko , P. Branchini , R. A. Briere , T. E. Browder , A. Budano , L. Burmistrov , S. Bussino , M. Campajola , L. Cao , G. Casarosa , C. Cecchi , D. Červenkov , M. -C. Chang , R. Cheaib , V. Chekelian , Y. Q. Chen , Y. -T. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. Cho , S. -K. Choi , S. Choudhury , D. Cinabro , L. Corona , L. M. Cremaldi , S. Cunliffe , T. Czank , F. Dattola , E. De La Cruz-Burelo , G. De Nardo , M. De Nuccio , G. De Pietro , R. de Sangro , M. Destefanis , S. Dey , A. De Yta-Hernandez , F. Di Capua , Z. Doležal , I. Domínguez Jiménez , T. V. Dong , K. Dort , D. Dossett , S. Dubey , S. Duell , G. Dujany , S. Eidelman , M. Eliachevitch , J. E. Fast , T. Ferber , D. Ferlewicz , G. Finocchiaro , S. Fiore , A. Fodor , F. Forti , B. G. Fulsom , E. Ganiev , M. Garcia-Hernandez , R. Garg , V. Gaur , A. Gaz , A. Gellrich , J. Gemmler , T. Geßler , R. Giordano , A. Giri , B. Gobbo , R. Godang , P. Goldenzweig , B. Golob , P. Gomis , W. Gradl , E. Graziani , D. Greenwald , Y. Guan , C. Hadjivasiliou , S. Halder , T. Hara , O. Hartbrich , K. Hayasaka , H. Hayashii , C. Hearty , M. T. Hedges , I. Heredia de la Cruz , M. Hernández Villanueva , A. Hershenhorn , T. Higuchi , E. C. Hill , M. Hoek , C. -L. Hsu , Y. Hu , T. Iijima , K. Inami , G. Inguglia , J. Irakkathil Jabbar , A. Ishikawa , R. Itoh , Y. Iwasaki , W. W. Jacobs , D. E. Jaffe , E. -J. Jang , H. B. Jeon , S. Jia , Y. Jin , C. Joo , K. K. Joo , J. Kahn , H. Kakuno , A. B. Kaliyar , J. Kandra , G. Karyan , Y. Kato , T. Kawasaki , B. H. Kim , C. -H. Kim , D. Y. Kim , K. -H. Kim , S. -H. Kim , Y. K. Kim , Y. Kim , T. D. Kimmel , H. Kindo , C. Kleinwort , P. Kodyš , T. Koga , S. Kohani , I. Komarov , S. Korpar , N. Kovalchuk , T. M. G. Kraetzschmar , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , J. Kumar , M. Kumar , R. Kumar , K. Kumara , S. Kurz , A. Kuzmin , Y. -J. Kwon , S. Lacaprara , C. La Licata , L. Lanceri , J. S. Lange , K. Lautenbach , I. -S. Lee , S. C. Lee , P. Leitl , D. Levit , L. K. Li , Y. B. Li , J. Libby , K. Lieret , L. Li Gioi , Z. Liptak , Q. Y. Liu , D. Liventsev , S. Longo , T. Luo , Y. Maeda , M. Maggiora , E. Manoni , S. Marcello , C. Marinas , A. Martini , M. Masuda , T. Matsuda , K. Matsuoka , D. Matvienko , F. Meggendorfer , J. C. Mei , F. Meier , M. Merola , F. Metzner , M. Milesi , C. Miller , K. Miyabayashi , H. Miyake , R. Mizuk , K. Azmi , G. B. Mohanty , T. Moon , T. Morii , H. -G. Moser , F. Mueller , F. J. Müller , Th. Muller , G. Muroyama , R. Mussa , E. Nakano , M. Nakao , M. Nayak , G. Nazaryan , D. Neverov , C. Niebuhr , N. K. Nisar , S. Nishida , K. Nishimura , M. Nishimura , B. Oberhof , K. Ogawa , Y. Onishchuk , H. Ono , Y. Onuki , P. Oskin , H. Ozaki , P. Pakhlov , G. Pakhlova , A. Paladino , A. Panta , E. Paoloni , H. Park , B. Paschen , A. Passeri , A. Pathak , S. Paul , T. K. Pedlar , I. Peruzzi , R. Peschke , R. Pestotnik , M. Piccolo , L. E. Piilonen , V. Popov , C. Praz , E. Prencipe , M. T. Prim , M. V. Purohit , P. Rados , R. Rasheed , S. Reiter , M. Remnev , P. K. Resmi , I. Ripp-Baudot , M. Ritter , G. Rizzo , L. B. Rizzuto , S. H. Robertson , D. Rodríguez Pérez , J. M. Roney , C. Rosenfeld , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , A. Sangal , L. Santelj , P. Sartori , Y. Sato , V. Savinov , B. Scavino , J. Schueler , C. Schwanda , R. M. Seddon , Y. Seino , A. Selce , K. Senyo , C. Sfienti , C. P. Shen , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , R. J. Sobie , A. Soffer , A. Sokolov , E. Solovieva , S. Spataro , B. Spruck , M. Starič , S. Stefkova , Z. S. Stottler , R. Stroili , J. Strube , M. Sumihama , T. Sumiyoshi , D. J. Summers , S. Y. Suzuki , M. Tabata , M. Takizawa , U. Tamponi , S. Tanaka , K. Tanida , N. Taniguchi , P. Taras , F. Tenchini , E. Torassa , K. Trabelsi , T. Tsuboyama , M. Uchida , K. Unger , Y. Unno , S. Uno , Y. Ushiroda , S. E. Vahsen , R. van Tonder , G. S. Varner , K. E. Varvell , A. Vinokurova , L. Vitale , A. Vossen , M. Wakai , H. M. Wakeling , W. Wan Abdullah , C. H. Wang , M. -Z. Wang , A. Warburton , M. Watanabe , J. Webb , S. Wehle , C. Wessel , J. Wiechczynski , H. Windel , E. Won , B. Yabsley , S. Yamada , W. Yan , S. B. Yang , H. Ye , J. H. Yin , M. Yonenaga , C. Z. Yuan , Y. Yusa , L. Zani , Z. Zhang , V. Zhilich , Q. D. Zhou , X. Y. Zhou , V. I. Zhukova

We report on recent results obtained by the Belle II experiment related to searches for beyond-the-standard-model physics. The $B$ meson decay data sample used corresponds to an integrated luminosity of $L = 189$ fb$^{-1}$. In recent years,…

High Energy Physics - Experiment · Physics 2023-08-15 Roberta Volpe , Belle II Collaboration

We investigate the phenomenology of light GeV-scale fermionic dark matter in $U(1)_{L_\mu - L_{\tau}}$ gauge extension of the Standard Model. Heavy neutral fermions alongside with a $S_1(\overline{3}$,$1$,$1/3$) scalar leptoquark and an…

High Energy Physics - Phenomenology · Physics 2022-02-09 Shivaramakrishna Singirala , Suchismita Sahoo , Rukmani Mohanta

The direct searches for heavy scalar dark matter with a mass of order 100 GeV are much more sensitive than for light dark matter of order 1 GeV. The question arises whether dark matter could be light and has escaped detection so far. We…

High Energy Physics - Phenomenology · Physics 2021-08-30 Markos Maniatis

We study UV complete theories where the Standard Model (SM) gauge group is extended with a new abelian $U(1)$, and the field content is augmented by an arbitrary number of scalar and fermion SM singlets, potentially including dark matter…

High Energy Physics - Phenomenology · Physics 2017-11-29 Yanou Cui , Francesco D'Eramo

We propose a model realizes that a semi-visible dark photon which can contribute to the anomalous magnetic moment ($g-2$) of both electron and muon. In this model, the electron $g-2$ is deviated from the Standard Model (SM) prediction by…

High Energy Physics - Phenomenology · Physics 2024-02-02 Waleed Abdallah , Mustafa Ashry , Junichiro Kawamura , Ahmad Moursy

The Belle II experiment at the SuperKEKB collider is a major upgrade of the KEK "$B$ factory" facility in Tsukuba, Japan. The machine is designed for an instantaneous luminosity of $8\times 10^{35}$~cm$^{-2}$\,s$^{-1}$, and the experiment…

High Energy Physics - Experiment · Physics 2016-07-08 Gianluca Inguglia

The muon g-2 discrepancy between theory and experiment may be explained by a light vector boson Z_d that couples to the electromagnetic current via kinetic mixing with the photon. We illustrate how the existing electron g-2, pion Dalitz…

High Energy Physics - Phenomenology · Physics 2014-05-14 Hooman Davoudiasl , Hye-Sung Lee , William J. Marciano

Dark photons with kinetic mixing are compelling mediators for the interactions between dark matter and Standard Model particles. While most experimental searches focus on fully visible or fully invisible decays of dark photons, we explore…

High Energy Physics - Phenomenology · Physics 2025-08-14 Francesca Acanfora , Felix Kahlhoefer

The possible existence of a new gauge boson U, light and very weakly coupled, allows for Light Dark Matter particles, which could also be at the origin of the 511 keV line from the galactic bulge. Independently of dark matter, and taking…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pierre Fayet

A search for dark matter is performed using events with large missing transverse momentum and a Higgs boson decaying either to a pair of bottom quarks or to a pair of photons. The data from proton-proton collisions at a center-of-mass…

High Energy Physics - Experiment · Physics 2017-11-21 CMS Collaboration