* [S.sub.1] = [[([v.sup.0.sub.e], e-, E-) [producto cruzado] e+ [producto cruzado] E+].sub.L] with

quantum numbers (1, 3,-2/3); (1, 1, 1) and (1, 1, 1) respectively.

In this formula, Lande introduced a fourth

Quantum Number with a half-integer number value (S = 1/2).

a canonical linear harmonic oscillator with a quadratic dependence of the potential energy on the displacement from an equilibrium condition, 2) a rotor with a fixed axis that produced an energy proportional to the square of a

quantum number, 3) a rigid rotor with a free axis that produced a rotational energy based on functional J (J + 1) and 4) a non-rigid rotor as a model of a diatomic molecule that produced again an energy dependent on the same functional.

In our numerical work, we solve (6) with the adiabatic potential (7) by using the numerical trigonometric sweep method [23] and we find electron energies [E.sub.m,n] for twenty different magnetic

quantum numbers m = 0,-1, -2, ..., -19 and two different axial

quantum numbers n= 1,2.

where n is an integer principal

quantum number, [zeta] is the screening constant, and [S.sub.lm] ([theta], [phi]) is a complex or real spherical harmonic (see [27-29] for exact definitions).

For the first time settlement and experimentally investigated for a round galvanized steel wires, is confirmed the important fundamentals of the theory of electricity electrophysical the fact that in this metal conductor used with aperiodic pulsed axial current conduction time form 9 ms/160 ms and high density (about 0.37 kA/[mm.sup.2]) in the longitudinal direction extend quantized coherent electronic half-wave of de Broglie length [[lambda].sub.enz]/2 defined during the investigations by the

quantum numbers n=1,3,9.

The value of the angular momentum

quantum number L as well as the curvature of the surface of these complex carbon structures clearly plays a crucial role in shaping the effective potential.

The rotational

quantum number j for the diatom is found from:

Quantum physics is usually considered to be the theory of extremely lightweight objects, such as atoms or photons, or of exceptionally small units, namely very small

quantum numbers.

[MATHEMATICAL EXPRESSION NOT REPRODUCIBLE IN ASCII] are the spin and pseudo-spin spherical harmonics functions, respectively, [F.sub.nk] (r) and [G.sub.nk] (r) are the radial wave functions of the upper- and the lower-spinor components respectively, m is the projection of the total angular momentum on the z-axis, n is the radial

quantum number. The orbital and the pseudo-orbital angular momentum

quantum numbers for spin symmetry l and pseudo-spin symmetry [??] refer to the upper- and lowercomponent respectively.

From this idea, he postulated the azimuthal

quantum number. He later introduced the magnetic

quantum number as well.

From now on, the

quantum number m (the canonical angular momentum number) will be considered fixed unless stated otherwise in a explicit way.