The nucleon-nucleon center-of-mass frame is ideal for deriving the
relations between spin observables and the interaction matrix, but it is
not always a useful way to conduct experiments. Intermediate energy
nuclear physics experiments are typically fixed target experiments,
so it is necessary
to convert the expressions for 
to be in terms of laboratory frame
polarization transfer observables.
The laboratory frame will be defined as:
and
The axes are typically referred to as longitudinal 
,
normal 
, and sideways 
.
and
represent
right-handed Cartesian coordinate frames [BBW82]. In terms of the
laboratory frame coordinates equation
can be expressed as [Che93]
The analyzing power associated with the out-of-plane component 
is
still referred to as 
by convention. Therefore, the laboratory frame
polarization observables can be obtained by measuring both the initial and
final polarization.
In order to determine the Bleszynski, et al. observables, 
,
[BBW82] it is necessary to express the laboratory frame observables
(i.e. 
) in terms of the center-of-mass spin observables
(i.e. 
). This requires a transformation of the reference frame
which includes a relativistic effect on the spin rotation. This
transformation is presented in detail by [IcK92].
Figure: Scattering kinematics in the center-of-mass and laboratory
reference frames including the relativistic effect on the spin rotation
explicitly [IcK92].
First of all, the unit vector normal to the scattering plane will remain
unchanged 
, so 
.
For the in-plane components the final state coordinates, 
and 
, will be rotated by an angle, 
, which is the
relativistic spin rotation as is shown in figure .
is given by
where 
is the velocity of the particle, 
is the
velocity of the c.m. frame with respect to the laboratory frame,
, and 
and 
are the
scattering angles in the c.m. and laboratory frames, respectively.
If we take 
to be the angle between the incident beam direction,
, and the unit vector 
as defined in equation
(see fig. ) then the transformations look like
Given these expressions between the coordinates the relations between in-plane spin observables is
where 
.
Using equation , equations to can be
rewritten as [Lut93]
where
Note: It is also possible to define 
as [Che93]:
