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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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It is clear that the self-adjoint operator rot have fundamental meaning but here we have<br />

only a possibility to find the eigenvalues <strong>of</strong> this operator. We set P = f rotandforthis<br />

operator polarization the following relations hold valid<br />

P = −M 2 1 − M 2 2 − M 2 3 + N 2 1 + N 2 2 + N 2 3 = −M 2 + N 2 , P 2 = −2(M 2 + N 2 ).<br />

This means that eigenvalues <strong>of</strong> the polarization operator equal ±p, where p =2, 3, 4, ....<br />

4. Conclusion. In conclusion, we discuss the new situation with solution <strong>of</strong> spindynamics<br />

equations (6) and (7) and the Maxwell equations (8) and (9). From polynomials<br />

(5) we can construct the orthogonal system <strong>of</strong> vector fields on S 3 (potential and turbulent).<br />

The coefficients <strong>of</strong> expansion <strong>of</strong> the vector and scalar fields over these systems will<br />

be the functions <strong>of</strong> f. Using the properties <strong>of</strong> the harmonic polynomials in question we<br />

can derive from the equations <strong>of</strong> spindynamics and the Maxwell equations the systems<br />

<strong>of</strong> ordinary differential equations for these coefficients. It is natural to suppose that this<br />

system <strong>of</strong> equations will have physical solutions only for quite definite meanings <strong>of</strong> charge<br />

and mass. Thus, at first we have a possibility to find the solution <strong>of</strong> nonlinear system <strong>of</strong><br />

equations that can represent the distinct hadrons and nucleus. It should be noted that<br />

a state <strong>of</strong> strongly interacting particle is characterized by the following orbital quantum<br />

numbers: 0, 1/2, 1, 3/2 ···.<br />

<strong>References</strong><br />

[1] I.B. Pestov, Field Theory and the Essence <strong>of</strong> Time. Horizons in World <strong>Physics</strong>, Volume<br />

series 248, Ed. A. Reimer, pp.1-29, (Nova Science, New York 2005); Preprint<br />

<strong>of</strong> <strong>JINR</strong> E2–2004–105, Dubna, 2004; ArXiv: gr-qc/0507131.<br />

[2] I.B. Pestov, The concept <strong>of</strong> Time and Field Theory . Preprint <strong>of</strong> <strong>JINR</strong> E2–1996–424,<br />

Dubna, 1996; ArXiv: gr-qc/0308073.<br />

[3] I.B, Pestov, Dark Matter and Potential Fields. Dark Matter: New Research, Ed.<br />

Val Blain, pp. 77-97, (Nova Science, New York, 2005); Preprint <strong>of</strong> <strong>JINR</strong> E2–2005–51,<br />

Dubna, 2005; ArXiv: gr-qc/0412096.<br />

[4] I.B. Pestov, Spin and Geometry. Relativistic Nuclear <strong>Physics</strong> and Quantum Chromodynamics,<br />

Eds: A.N. Sissakian, V.V.Burov, A.I.Malakhov. Proc. <strong>of</strong> the XVIII<br />

Intern. Baldin Seminar on High Energy <strong>Physics</strong> Problems (Dubna, September 25-30,<br />

2006).-Dubna: <strong>JINR</strong>, 2008. -V.2, p.289-299; Self-Organization <strong>of</strong> Physical Fields and<br />

Spin. Preprint <strong>of</strong> <strong>JINR</strong> E2–2008–93, Dubna, 2008, 42p.<br />

[5] G. de Rham, Varietes Differentiables.-Paris: Hermann, 1955.<br />

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