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Related papers: Dibaryons cannot be the dark matter

200 papers

We find expressions for the weak decay amplitudes of baryons containing two b quarks (or one b and one c quark -- many relationship are the same) in terms of unknown reduced matrix elements. This project was originally motivated by the…

High Energy Physics - Phenomenology · Physics 2011-01-27 David A. Egolf , Roxanne P. Springer , Joerg Urban

We study a class of dark matter models in which the dark matter is a baryon-like composite particle of a confining gauge group and also a pseudo-Nambu-Goldstone boson associated with the breaking of an enhanced chiral symmetry group. The…

High Energy Physics - Phenomenology · Physics 2013-02-08 Matthew R. Buckley , Ethan T. Neil

If the next fundamental level of matter occurs (preons) then dark matter must consist of familons containing a "hot" component from massless particles and a "cold" component from massive particles. During evolution of the Universe this dark…

High Energy Physics - Phenomenology · Physics 2009-11-13 V. Burdyuzha , O. Lalakulich , Yu. Ponomarev , G. Vereshkov

Recent lattice QCD calculations from the HAL and NPLQCD Collaborations have reported evidence for the existence of a bound state with strangeness -2 and baryon number 2 at quark masses somewhat higher than the physical values. A controlled…

Nuclear Theory · Physics 2013-08-09 P. E. Shanahan , A. W. Thomas , R. D. Young

The apparent discrepancy between abundances of light nuclides predicted by the standard Big-Bang and observational data is explained, by assuming the presence of metastable H dibaryons at the nucleosynthesis era. These dibaryons could be…

Astrophysics · Physics 2009-10-31 J. A. de Freitas Pacheco , S. Stoica , F. Thevenin , J. E. Horvath

The inferred values of the cosmological baryon and dark matter densities are strikingly similar, but in most theories of the early universe there is no true explanation of this fact; in particular, the baryon asymmetry and thus density…

High Energy Physics - Phenomenology · Physics 2009-11-10 Dan Hooper , John March-Russell , Stephen M. West

Strangness production processes can balance natural strangeness decay in the early hadronic Universe. Comparing to the characteristic Hubble time $1/H$, the reaction rates for $\mu^\pm+\nu_{\mu}\rightarrow K^\pm$, $l^-+l^+\rightarrow\phi$,…

High Energy Physics - Phenomenology · Physics 2022-03-08 Johann Rafelski , Cheng Tao Yang

We discuss a simple model of thermal relic dark matter whose mass can be much larger than the so-called unitarity limit on the mass of point-like particle dark matter. The model consists of new strong dynamics with one flavor of fermions in…

High Energy Physics - Phenomenology · Physics 2016-09-21 Keisuke Harigaya , Masahiro Ibe , Kunio Kaneta , Wakutaka Nakano , Motoo Suzuki

We propose a novel scenario to explain the observed cosmological asymmetry between matter and antimatter, based on nonperturbative QCD physics. This scenario relies on a mechanism of separation of quarks and antiquarks in two coexisting…

High Energy Physics - Phenomenology · Physics 2009-11-10 David H. Oaknin , Ariel Zhitnitsky

Based on a dynamical model on particle production, the production and fraction of exotic components in neutron star matter are analyzed. It is found that there exists a small fraction of strangeness in twice saturation density matter. For…

Nuclear Theory · Physics 2023-11-30 Gao-Chan Yong

All presently known stellar-dynamical constraints on the size and mass of the supermassive compact dark object at the Galactic center are consistent with a ball of self-gravitating, nearly non-interacting, degenerate fermions with mass…

Astrophysics · Physics 2007-05-23 Neven Bilic , Gary B. Tupper , Raoul D. Viollier

It was shown in ref. [1] that cold dark matter axions reach thermal contact with baryons, and therefore cool them, shortly after the axions thermalize among themselves and form a Bose-Einstein condensate. The recent observation by the EDGES…

Cosmology and Nongalactic Astrophysics · Physics 2018-08-02 Pierre Sikivie

Strangeon is proposed to be the constituent of bulk strong matter, as an analogy of nucleon for an atomic nucleus. The nature of both nucleon matter (2 quark flavors, u and d) and strangeon matter (3 flavors, u, d and s) is controlled by…

High Energy Astrophysical Phenomena · Physics 2019-08-20 Renxin Xu

Our world is wonderful because of the normal but negligibly small baryonic part (i.e., atoms) although unknown dark matter and dark energy dominate the Universe. A stable atomic nucleus could be simply termed as ``strong matter'' since its…

High Energy Physics - Phenomenology · Physics 2022-11-08 Xiaoyu Lai , Chengjun Xia , Renxin Xu

It is a puzzle why the densities of dark matter and dark energy are nearly equal today when they scale so differently during the expansion of the universe. This conundrum may be solved if there is a coupling between the two dark sectors. In…

High Energy Physics - Phenomenology · Physics 2009-07-09 D. Comelli , M. Pietroni , A. Riotto

Universe heating in $R^2$-modified gravity is considered. The rates of particle production by the scalaron are calculated for different decay channels. Freezing of massive stable relics with the interaction strength typical for…

Cosmology and Nongalactic Astrophysics · Physics 2022-07-15 E. V. Arbuzova , A. D. Dolgov

We introduce a model for matters-genesis in which both the baryonic and dark matter asymmetries originate from a first-order phase transition in a dark sector with an $SU(3)\times SU(2)\times U(1)$ gauge group and minimal matter content. In…

High Energy Physics - Phenomenology · Physics 2023-03-10 Eleanor Hall , Thomas Konstandin , Robert McGehee , Hitoshi Murayama

Strange Quark Nuggets are the relics of the microsecond old universe after the big bang. The universe having experienced a mini inflation of 7-e folding has gone through supercooling leading to a first order phase transition from quark to…

General Physics · Physics 2020-08-17 Bikash Sinha

We investigate the symmetry property and construct the wave function of the dibaryon states containing two strange quarks with S=0 in both the flavor SU(3) symmetric and breaking cases. We discuss how the color $\otimes$ isospin $\otimes$…

High Energy Physics - Phenomenology · Physics 2016-04-13 Woosung Park , Aaron Park , Su Houng Lee

If quark matter is energetically favored over nuclear matter at zero temperature and pressure then it has long been expected to take the form of strange quark matter (SQM), with comparable amounts of $u$, $d$, $s$ quarks. The possibility of…

High Energy Physics - Phenomenology · Physics 2018-06-06 Bob Holdom , Jing Ren , Chen Zhang