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For the linear baryon string model with three massive points (three quarks) connected sequentially by the relativistic strings the initial-boundary value problem is stated and solved in general. This problem implies defining a classical…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. P. Petrov , G. S. Sharov

For the relativistic string with massive ends, the three-string baryon model and other string models of the baryon the small disturbances of well known rotational motions are considered. For the string meson model the two types of these…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. S. Sharov

For the relativistic string with massive ends (the meson model) and four various string baryon models (q-qq, q-q-q, Y and $\Delta$) we consider the classical quasirotational motions, which are small disturbances of the planar uniform…

High Energy Physics - Phenomenology · Physics 2010-11-19 G. S. Sharov

We consider various hadron models with a string carrying $n=3$ massive points (quarks): Y configuration, linear baryon model $q$-$q$-$q$ and the closed string. For these models classical rotational states (planar uniform rotations) are…

High Energy Physics - Phenomenology · Physics 2010-04-12 G. S. Sharov

For the linear string baryon model $q$-$q$-$q$ the small disturbances of its rotational motion (quasirotational states) are investigated. The spectrum of these states is obtained in the form of Fourier series and the complex…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. S. Sharov

Various string models of mesons and baryons include a string carrying 2 or 3 massive points (quarks or antiquarks). Rotational states (planar uniform rotations) of these systems generate quasilinear Regge trajectories and may be used for…

High Energy Physics - Phenomenology · Physics 2013-05-20 G. S. Sharov

The relativistic string with massive ends (the meson model) and four various string baryon models: q-qq, q-q-q, Y and $\Delta$ are considered. In particular, the rotational motions for all these systems are applied to describing the leading…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. S. Sharov

For the linear string baryon model with three material points (three quarks) joined sequentially by the relativistic strings, the class of motions admitting linearizable boundary conditions is investigated. These motions may be represented…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. P. Petrov , G. S. Sharov

We extend the model for QCD string with quarks to consider the Mercedes Benz string configuration describing the three-quark baryon. Under the assumption of adiabatic separation of quark and string junction motion we formulate and solve the…

High Energy Physics - Phenomenology · Physics 2019-08-17 Yu. S. Kalashnikova , A. V. Nefediev

Rotational motions for the quark-diquark (q-qq), linear (q-q-q) "three-string" (Y) and "triangle" string baryon models are considered and applied to description of baryonic orbitally exited states on the Regge trajectories. For the model…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. S. Sharov

The considered model of baryon consists of three pointlike masses (quarks) bounded pairwise by relativistic strings forming a curvilinear triangle. Classic analytic solutions for this model corresponding to a planar uniform rotation about…

High Energy Physics - Theory · Physics 2010-11-19 G. S. Sharov

For the closed string carrying 2 or 3 point-like masses the stability problem for central and linear rotational states is considered. This problem is important for applications of these model to describing baryons, glueballs or other exotic…

High Energy Physics - Phenomenology · Physics 2009-07-09 G. S. Sharov

A simple model is discussed in which baryons are represented as pieces of open string connected at one common point. There are two surprises: one is that, in the conformal gauge, the relative lengths of the three arms cannot be kept…

High Energy Physics - Theory · Physics 2007-05-23 Gerard 't Hooft

The closed string carrying $n$ point-like masses is considered as the model of a baryon ($n=3$), a glueball ($n=2$ or 3) or another exotic hadron. For this system the rotational states are obtained and classified. They correspond to exact…

High Energy Physics - Phenomenology · Physics 2007-12-27 G. S. Sharov

We provide a systematic construction of string junctions in curved backgrounds which are relevant in computing, within the gauge/gravity correspondence, the interaction energy of heavy dyons, notably of quark-monopole pairs, in strongly…

High Energy Physics - Theory · Physics 2008-11-26 Konstadinos Sfetsos , Konstadinos Siampos

We consider the phenomenological consequences of the assumption that the baryons are the systems of three quarks and string junction. The process of baryon number transfer due to string junction propagation in rapidity space is considered…

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

It is argued that the internal dynamics of a baryon, as a bound state of QCD-strings and quarks, may be captured by a theory of matrix coordinates.

High Energy Physics - Phenomenology · Physics 2009-11-10 Amir H. Fatollahi

In this review we describe our current understanding of the properties of open string tachyons on an unstable D-brane or brane-antibrane system in string theory. The various string theoretic methods used for this study include techniques of…

High Energy Physics - Theory · Physics 2009-09-15 Ashoke Sen

The correction to the string junction three-quark potential in a baryon due to the proper moment of inertia of the QCD string is calculated. The magnitudes of the string corrections in P-wave heavy baryons are estimated.

High Energy Physics - Phenomenology · Physics 2011-04-27 O. N. Driga , I. M. Narodetskii , A. I. Veselov

Field-correlator method is used to calculate nonperturbative dynamics of quarks in a baryon. General expression for the 3q Green's function is obtained using Fock-Feynman-Schwinger (world-line) path integral formalism, where all dynamics is…

High Energy Physics - Phenomenology · Physics 2014-11-17 Yu. A. Simonov
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