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The vast bulk of visible mass emerges from nonperturbative dynamics within quantum chromodynamics (QCD) -- the strong interaction sector of the Standard Model. The past decade has revealed the three pillars that support this emergent hadron…

High Energy Physics - Phenomenology · Physics 2023-07-12 Craig D. Roberts

In this note we describe hadrons: mesons and baryons as strings with electric charges on their endpoints. We consider here only the neutral system with opposite charges coupled to an external constant electric and magnetic fields. We derive…

High Energy Physics - Theory · Physics 2020-07-24 Jacob Sonnenschein , Dorin Weissman , Shimon Yankielowicz

In most models of dark energy the structure formation stops when the accelerated expansion begins. In contrast, we show that the coupling of dark energy to dark matter may induce the growth of perturbations even in the accelerated regime.…

Astrophysics · Physics 2009-11-07 Luca Amendola , Domenico Tocchini-Valentini

We compare the numerical results for antibaryon/baryon production ratios in high energy heavy ion collisions with some theoretical models.

High Energy Physics - Phenomenology · Physics 2007-05-23 Yu. M. Shabelski

Experimental data on inclusive cross sections of the hadrons produced in high energy proton-(anti)proton collisions are analyzed in the z-scaling approach. Saturation of the scaling function PSI(z) for z<0.1 (low transverse momenta) was…

High Energy Physics - Phenomenology · Physics 2011-01-19 I. Zborovský , M. V. Tokarev

In high energy p+p(bar) interactions the mean multiplicity and transverse mass spectra of neutral mesons from eta to Upsilon (m = 0.5 - 10 GeV/c^2) and the transverse mass spectra of pions (m_T > 1 GeV/c^2) reveal a remarkable behaviour:…

High Energy Physics - Phenomenology · Physics 2009-11-07 Marek Gazdzicki , Mark I. Gorenstein

The string melting version of a multi-phase transport model is often applied to high-energy heavy-ion collisions since the dense matter thus formed is expected to be in parton degrees of freedom. In this work we improve its quark…

Nuclear Theory · Physics 2017-07-26 Yuncun He , Zi-Wei Lin

In this two part series a chiral confining model of baryons is used to describe low--lying negative parity resonances $N^*$, $\Delta^*$, $\Lambda^*$ and $\Sigma^*$ in the mean field approximation. A physical baryon in this model consists of…

Nuclear Theory · Physics 2007-05-23 Y. Umino , M. K. Banerjee

We have addressed the study of non-leptonic weak decays of heavy hadrons ($\Lambda_b, \Lambda_c, B$ and $D$), with external and internal emission to give two final hadrons, taking into account the spin-angular momentum structure of the…

High Energy Physics - Phenomenology · Physics 2018-08-01 Wei-Hong Liang , E. Oset

Recent measurements of the asymmetries between Feynman $x$ distributions of strange and antistrange hadrons in $\pi^- A$ interactions show a strong effect as a function of $x_F$. We calculate strange hadron production in the context of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 T. D. Gutierrez , R. Vogt

The mechanism of string creation for light quarks developed earlier is considered for nonzero quark chemical potential. A strong modification of the confining string due to finite quark density (chemical quark potential $\mu$) is observed.…

High Energy Physics - Phenomenology · Physics 2009-08-25 Yu. A. Simonov , M. A. Trusov

Baryon charge radii and quadrupole moments are calculated in a quark model generalized to an arbitrary number (N_c) of colors. Several relations among the charge radii and quadrupole moments are found. In particular, a previously derived…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. J. Buchmann

We examine the generation of baryon asymmetry at the weak scale from a primordial lepton asymmetry. If the electroweak phase transition is first order, partial reflection of tau leptons off the bubble walls and the resulting hypercharge…

High Energy Physics - Phenomenology · Physics 2009-10-28 S. A. Abel , K. E. C. Benson

We study the effect on leptogenesis due to $B-L$ cosmic strings of a $U(1)_{B-L}$ extension of the Standard Model. The disappearance of closed loops of $B-L$ cosmic strings can produce heavy right handed neutrinos, $N_R$'s, whose…

High Energy Physics - Phenomenology · Physics 2008-11-26 Narendra Sahu , Pijushpani Bhattacharjee , Urjit A Yajnik

In this paper we present the description of the production of strange and mulistrange baryons in a wide energy region, from CERN SpS up to LHC, in the framework of the Quark-Gluon String model.

High Energy Physics - Phenomenology · Physics 2015-02-25 G. H. Arakelyan , C. Merino , Yu. M. Shabelski

In recent years, unprecedented progress in observational cosmology has revealed a great deal of information about the formation and evolution of structures in the universe. This, in turn, has raised many challenging issues for the…

Astrophysics · Physics 2010-12-09 T. Roy Choudhury

Measurements of production cross-sections of inclusive $b$-hadrons pairs, bottom mesons and baryons, and quarkonia at LHC will be shown. Recent measurements of branching fractions of bottom baryons, bottom mesons with baryons in the final…

High Energy Physics - Experiment · Physics 2019-11-12 P. Ronchese

Grand unified theories can admit cosmic strings with fermion zero modes which result in the string carrying a current and the formation of stable remnants, vortons. We consider theories in which the zero modes do not survive a subsequent…

High Energy Physics - Phenomenology · Physics 2009-10-30 Anne-Christine Davis , Warren B. Perkins

We report on a scaling behaviour in the transverse momentum ($p_{T}$) distributions for charged hadrons produced in proton-proton ($pp$) collisions with different center of mass energies ($\sqrt{s}$ = 0.9, 2.76 and 7 TeV) at the Compact…

High Energy Physics - Phenomenology · Physics 2014-09-11 W. C. Zhang , C. B. Yang

The baryon junction exchange mechanism recently proposed to explain valence baryon number transport in nuclear collisions is extended to study midrapidity anti-hyperon production. Baryon junction-anti-junction (J anti-J) loops are shown to…

Nuclear Theory · Physics 2009-10-09 Stephen E. Vance , Miklos Gyulassy