Next: Effects of Final-State Interactions
Up: 4.2.3 Observables
Previous: B) Decay of Top
Detailed studies of the decay of free polarized top quarks have
already been available including the full
corrections
[12,13,14].
The best example is the energy-angular distribution of charged
leptons l+ in the semi-leptonic decay of the top quark.
At leading order, the l+ distribution
has a form where the energy and angular dependences are factorized
[15,16]:
![$\displaystyle \frac{d\Gamma_{t \to bl^+\nu}
({\bf {S}})}
{dE_l d\Omega_l}
= h(E...
...}\vert \cos \theta_l ) ~~ + ~~
[ \, {\cal O}(\alpha_s)~\mbox{correction} \, ] .$](img1201.gif) |
|
|
(4.4) |
Here El,
,
and
denote, respectively, the l+ energy, the solid angle of l+,
and the angle between the l+ direction and the
top polarization vector
,
all of which
are defined in the top-quark rest frame.
Hence, we may measure the top-quark polarization
with maximal sensitivity using the l+ angular
distribution.
ACFA Linear Collider Working Group
E-Mail:acfareport@acfahep.kek.jp