the new fuels with magnecular structure - Institute for Basic Research

182 RUGGERO MARIA SANTILLI
Figure A8. A schematic view of the ground and first-excited state of H + 2 ion. The solid line
traces |000〉, and the dashed line follows |0 -1 0〉. The triangles give the positions of the protons
for the ground state and the squares for the excited state. The magnetic field B = 4.7 · 10 12
Gauss is pointed along the internuclear axis; ζ = 2παz/λ e denotes z in a.u.; 1 a.u. = 0.53 · 10 −8
cm (reproduction of Figure 5 by Heyl and Hernquist [14]).
tion, even at the intensities as high as B = 100B 0 . . . 1000B 0 . The outer domain
appears to be of specific, highly elongated distribution along the direction of the
magnetic field as shown in Fig. A7. The possible interpretation that the inner
electrons remain to have a spherical distribution while outer electrons undergo
the squeeze seems to be not correct unless the spin state of the iron atom is verified
to be partially polarized. So, we can conclude that all the electrons are in
the highly magnetically polarized state (Landau state mixed a little by Coulomb
interaction), and the electronic structure is a kind of Landau multi-electron cylindrical
shell, with the spins of all the electrons being aligned antiparallel to the
magnetic field (fully spin polarized configuration).
Another remark regarding Fig. A7 is that the contours indicating a nearly
spherical distribution will always appear since the Coulomb center (nucleus) is
not totally eliminated from the consideration (non-adiabatic approximation), and
it forces a spherical distribution to some degree, which evidently depends on the
distance from the center (closer to the center, more sphericity). We note that
outer contours in Fig. A7 is in qualitative agreement with Fig. A6 in the sense that
the predicted charge distribution reveals symmetry under the inversion z → −z,
with the characteristic z-elongated Landau-type orbits.