Alexander A. Shpilman( sah@nursat.kz )
The author of the data of
lines has done a bit of travelling on much to open
spaces of former
The way of knowledge is
infinite. The creative person always will be than to gift of ambient, and at
the fruitless man and that is present, will not give sprout.
Ferrite-magnetic the Reflector Axion (Spin) of Radiation
The ways are known of
change of a direction of propagation of electromagnetic waves with the help of
mirrors constructed on effect of reflection from border of the unit of
environments of a type dielectric-dielectric and a dielectric-conductor at the
expense of a difference of parameters of refraction, interference and
diffraction on a regular structure of a crystal lattice for x-ray, gamma, beta
and other kinds of radiation. But they can not be applied for reflection axion of radiation (spin waves), since it is direct with a
crystal lattice (known materials) practically does not
cooperate.
As axion
of a field and the radiation cooperate, in basic, only with spin of electrons
and nucleuses of atoms, it is meaningful to try to change a direction of
propagation axion radiation at the expense of
orientation these spins. That is, the change of a direction of propagation of
energy axion radiation is possible to achieve by the
reflector with the induced or internal anisotropy focused perpendicularly to a
direction of propagation of radiation of a source, with deviation from
perpendicularity on a angle which is not exceeding of a angle "precessions"
of spin of active elements of the reflector, rather this anisotropy.
Generally, the axion radiation, penetrating in any material and
cooperating with backs of its making elements, orientates them on a direction
of an axis of radiation. In result the spin channel is formed, along which
there is a propagation of energy axion of radiation. If
of elements of a material are already guided perpendicularly to direction axion of a field, there is absorption of energy axion of radiation and re-emission take place in a
direction of orientation of interacting a spin (in our case within the limits
of a cone of precession a spin). The average change of a direction of
propagation of energy axion radiation makes 90
degrees at such reflection.
In the device described in N3/95 axion the
radiation occurs along rotation axis in both directions (two rays of opposite
polarization).
The device (Reflector)
shown on figure generates unidirectional axion
radiation (See also patent of
In which, hollow the cylinder 2 is made from a
ferromagnetic material with built-in constants by magnets (see N3/95). A cone of the reflector 3 with a
covering ring 4, are made of silver or cadmium, with thickness of walls of 1 mm
(the large thickness is not meaningful, as works in a main surface) both angle
between an axis and forming of a cone equality to 30 degrees.
The offered design as
follows works:
The return ray of axion radiation 5 hollow of the cylinder 2 radiators,
dropping on a surface of a reflecting cone 3 under a angle to it, equal to
precession angle spin of electrons and nucleuses of atoms of a cone concerning
an axis of an anisotropy called by a gradient of concentration on border of the
unit of environments (for example metal - oxide-air), cooperates with last,
therefore energy of axion radiation of a ray 5
re-emit on a direction of the data spin. Thus, is formed axion
radiation (reflected) as a ray 6, which as a result of spatial interaction with
a direct ray 7, forms in space closed axion a field
in the form of the extended ellipsoid of rotation with a main axis conterminous
to an axis of the device (Reflector), in result density of axion
radiation in a near zone considerably grows
At use of the offered
reflector axion the radiation 5 drops on a surface of
metal under a angle to it of 30 degrees and is
reflected concerning it on the average under a angle in 60 degrees (reflected
ray 6), so the full angle of change of trajectory of motion of axion a ray makes 90 degrees.
At use of the offered
reflector the drive of the radiator can be located along an axis of the
radiator 1, inside a cone of the reflector 3 with appropriate electromagnetic
protective.
It is necessary to note,
that the processes, occurring in the given design, are considerably more
complex than the adduced description, and it is natural, demand the further
study.
Translation carrying-out by T.M.Shpilman
(see N3/95 , N2/96 , N3/96 , N2/97 , N1/98 , N2/98 , N1/99 , N2/99)
