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We study the dark matter particle, the dark photon (DP), in the decay of the Higgs-like boson. The nature of dark matter is maintained through the hidden sector including the effects of breaking of the scale invariance. The model is based…

High Energy Physics - Phenomenology · Physics 2015-07-24 G. A. Kozlov

Many theories about dark matter have emerged due to its strong theoretical appeal in explaining astrophysical phenomena. However, experimental and theoretical particle physics have yet not provided evidence that dark matter is part of the…

High Energy Physics - Phenomenology · Physics 2023-08-08 G. Gil da Silveira , M. S. Mateus

We revisited the decaying dark matter (DDM) model, in which one collisionless particle decays early into two collisionless particles, that are potentially dark matter particles today. The effect of DDM will be manifested in the cosmic…

High Energy Physics - Phenomenology · Physics 2011-07-20 Ran Huo

The similar densities of dark matter and baryons in the universe imply that they might arise from the same ultraviolet model. The B-Mesogenesis, which assumes dark matter is charged under the baryon number, attempts to simultaneously…

High Energy Physics - Phenomenology · Physics 2024-08-20 Yong Zheng , Jian-Nan Ding , Dong-Hao Li , Lei-Yi Li , Cai-Dian Lü , Fu-Sheng Yu

The framework for soft leptogenesis minimally extended with a DM sector is studied. A heavy singlet neutrino superfield acts as the source for (s)lepton asymmetry and by coupling to the singlet DM superfield it produces a DM particle…

High Energy Physics - Phenomenology · Physics 2013-01-04 Heidi Kuismanen , Iiro Vilja

Assuming that the $\Upsilon(10753)$ is a $4S$-$3D$ mixed state, we investigated the hidden-bottom hadronic decays of the $\Upsilon(10753) \to \eta_b(1S)\omega(\eta^{(\prime)})$ via the intermediate meson loops. In a commonly accepted range…

High Energy Physics - Phenomenology · Physics 2024-03-06 Shidong Liu , Zuxin Cai , Zhaosai Jia , Gang Li , Jujun Xie

The freeze-in mechanism describes the out-of-equilibrium production of dark matter (DM) particles via feeble couplings or non-renormalisable interactions with large suppression scales. In the latter case, predictions suffer from a strong…

High Energy Physics - Phenomenology · Physics 2025-04-16 Cristina Benso , Felix Kahlhoefer , Henda Mansour

Cold Dark Matter (CDM) models struggle to match the observations at galactic scales. The tension can be reduced either by dramatic baryonic feedback effects or by modifying the particle physics of CDM. Here, we consider an ultra-light…

Cosmology and Nongalactic Astrophysics · Physics 2016-07-27 Erminia Calabrese , David N. Spergel

The fundamental nature of mass is one of the greatest mysteries in physics. The Higgs mechanism is a theoretically appealing way to account for the different masses of elementary particles and implies the existence of a new, yet unseen…

High Energy Physics - Experiment · Physics 2009-02-13 The BABAR Collaboration , B. Aubert

The growth and virialization of spherical top-hat fluctuations, in coupled Dark Energy models, causes segregation between Dark Matter (DM) and baryons, as the gravitational infall into the potential well proceeds more slowly for the baryons…

Astrophysics · Physics 2009-11-13 Roberto Mainini

Using data corresponding to an integrated luminosity of 1.3 fb^-1, we observe a narrow mass state decaying into Upsilon(1S)+gamma, where the Upsilon(1S) meson is detected by its decay into a pair of oppositely charged muons, and the photon…

High Energy Physics - Experiment · Physics 2013-05-30 D0 Collaboration

Dark matter may form bound states in a dark sector with an attractive force between two dark matter particles. Searches for dark matter at colliders can differ dramatically from routine searches if bound states, dubbed darkonia, are…

High Energy Physics - Phenomenology · Physics 2025-06-19 Yang Bai , Susanne Westhoff

Motivated by concerns regarding possible two-body contributions to the recently-measured inclusive Upsilon(nS)->gamma+X (n=1, 2, 3) direct photon spectra, we report on a new study of exclusive radiative decays of these narrow Upsilon(nS)…

High Energy Physics - Experiment · Physics 2010-04-08 J. L Rosner , CLEO Collaboration

The decay and annihilation cross sections of dark matter particles may depend on the value of a chameleonic scalar field that both evolves cosmologically and takes different values depending on the local matter density. This possibility…

Cosmology and Nongalactic Astrophysics · Physics 2015-03-20 Kimberly K. Boddy , Sean M. Carroll , Mark Trodden

We propose a minimal model for the cosmic coincidence problem $\Omega_{\rm DM}/\Omega_B \sim 5$ and neutrino mass in a type-II seesaw scenario. We extend the standard model of particle physics with a $\rm SU(2)$ singlet leptonic Dirac…

High Energy Physics - Phenomenology · Physics 2021-11-30 Nimmala Narendra , Narendra Sahu , Sujay Shil

We generalize dark matter production to a two-metric framework whereby the physical metric, which couples to the Standard Model (SM), is conformally and/or disformally related to the metric governing the gravitational dynamics. We show that…

High Energy Physics - Phenomenology · Physics 2021-02-03 Philippe Brax , Kunio Kaneta , Yann Mambrini , Mathias Pierre

In this work we examine the possible existence of new physics beyond the standard model which could modify the branching fractions of the leptonic (mainly tauonic) decays of bottomonium vector resonances below the $B\bar{B}$ threshold. The…

High Energy Physics - Phenomenology · Physics 2011-07-19 Miguel-Angel Sanchis-Lozano

We present a model of composite Dark Matter (DM), in which a new QCD-like confining "hypercolor" sector generates naturally stable hyperbaryons as DM candidates and at the same time provides mass to new weakly coupled gauge bosons $H$ that…

High Energy Physics - Phenomenology · Physics 2021-02-24 Alexandre Carvunis , Diego Guadagnoli , Meril Reboud , Peter Stangl

We report evidence for the ground state of bottomonium, eta_b(1S), in the radiative decay Upsilon(3S) --> gamma eta_b in e^+e^- annihilation data taken with the CLEO III detector. Using 6 million Upsilon(3S) decays, and assuming…

Using samples of 102 million $\Upsilon(1S)$ and 158 million $\Upsilon(2S)$ events collected with the Belle detector, we study exclusive hadronic decays of these two bottomonium resonances to the three-body final states $\phi K^+ K^-$,…

High Energy Physics - Experiment · Physics 2012-08-16 Belle Collaboration , C. P. Shen , C. Z. Yuan , T. Iijima , I. Adachi , H. Aihara , D. M. Asner , T. Aushev , A. M. Bakich , A. Bay , K. Belous , B. Bhuyan , M. Bischofberger , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. -C. Chang , P. Chang , A. Chen , P. Chen , B. G. Cheon , K. Chilikin , R. Chistov , I. -S. Cho , K. Cho , S. -K. Choi , Y. Choi , J. Dalseno , Z. Doležal , Z. Drásal , S. Eidelman , J. E. Fast , V. Gaur , N. Gabyshev , Y. M. Goh , B. Golob , J. Haba , H. Hayashii , Y. Horii , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , K. Inami , A. Ishikawa , R. Itoh , M. Iwabuchi , Y. Iwasaki , T. Iwashita , T. Julius , J. H. Kang , T. Kawasaki , C. Kiesling , B. H. Kim , H. O. Kim , J. B. Kim , J. H. Kim , M. J. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , S. Koblitz , P. Kodyš , S. Korpar , R. T. Kouzes , P. Križan , P. Krokovny , R. Kumar , T. Kumita , A. Kuzmin , Y. -J. Kwon , S. -H. Lee , J. Li , Y. Li , J. Libby , C. Liu , Y. Liu , Z. Q. Liu , R. Louvot , S. McOnie , K. Miyabayashi , H. Miyata , G. B. Mohanty , D. Mohapatra , A. Moll , N. Muramatsu , E. Nakano , M. Nakao , Z. Natkaniec , S. Nishida , K. Nishimura , O. Nitoh , S. Ogawa , T. Ohshima , S. Okuno , S. L. Olsen , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , H. K. Park , T. K. Pedlar , R. Pestotnik , M. Petrič , L. E. Piilonen , M. Ritter , H. Sahoo , Y. Sakai , D. Santel , T. Sanuki , Y. Sato , O. Schneider , C. Schwanda , K. Senyo , O. Seon , M. E. Sevior , M. Shapkin , V. Shebalin , T. -A. Shibata , J. -G. Shiu , B. Shwartz , A. Sibidanov , F. Simon , P. Smerkol , Y. -S. Sohn , A. Sokolov , E. Solovieva , M. Starič , M. Sumihama , T. Sumiyoshi , G. Tatishvili , Y. Teramoto , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , P. Vanhoefer , G. Varner , C. H. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , B. D. Yabsley , Y. Yamashita , C. C. Zhang , Z. P. Zhang , V. Zhilich , V. Zhulanov , A. Zupanc