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Reflection of an Unpolarized Beam from the
Surface of a Bulk Magnetic Sample
An unpolarized incident electron beam is [31,32] an incoherent superposition of pure states
representing all directions of the incident spin. Each such
direction can be represented by its spherical polar angle
co-ordinates
. That is to say, the incident beam
contains a flux of electrons
 |
(2.25) |
with polarization direction between
and
, and between
and
.
The flux of such electrons in the reflected beam will, therefore, be
 |
(2.26) |
The reflection from the surface of a bulk sample is to be modelled as
a single reflection, of amplitude reflection coefficient
, in
a situation where
,
, and therefore
, are all zero. In
this case,
 |
(2.27) |
and
 |
(2.28) |
assuming that
is real.
If the spherical polar representation
is used for
the direction of the magnetic flux density in region
, then
 |
(2.29) |
Therefore,
 |
(2.30) |
The polarization of the pure state represented by
,
in the Cartesian co-ordinate system associated with this spherical
polar system, is
 |
(2.31) |
and the average polarization of the reflected beam is
The crucial integrals are
and
This gives a polarization
where
is a unit vector, in the direction of the
magnetic flux density in region 1.
Next: The Experimental Apparatus
Up: PER Theory
Previous: Amplitude Reflection Coefficient
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Daniel Christopher Hatton
2004-11-30