The observation of CP violation in decays would greatly enrich
our understanding of this, still mysterious, phenomenon.
CP violation in , even at the level where
mass-mixing effects only are observed, is very interesting, because
any deviation of
from
is a direct signal of
CPT violation. On the other side, CP-odd charge asymmetries in
decays would give a univocal sign of the milliweak nature of CP violation.
If current Standard Theory estimates are correct, the direct CP violation
parameter for
,
, tends to be quite
small because of a cancellation of the dominant gluon penguin diagram
contribution with the one arising from the electroweak penguin diagrams,
made competitive by the large value of the t quark mass [1].
The same two classes of contributions do not cancel in the asymmetry of
decays, which then could provide the crucial test of the
scheme. Furthermore, while
is essentially
suppressed by the
rule as being proportional to the small
ratio of the
to the
amplitude, in
there are two independent
amplitudes whose CP-violating
interference can avoid this suppression, and in principle could be expected to
produce an enhanced effect.
Unfortunately, in general the predicted Dalitz-plot slope asymmetries are in
the order of few units per million (subject to a theoretical error which
could be perhaps of a factor ten). In particular, the
interference between the
two amplitudes turns out to occur only in higher orders in the
chiral perturbation theory expansion (
), and the corresponding
enhancement is therefore somewhat reduced. On purely statistical grounds,
DA
NE experiments can reach the level of a few units in
and
therefore are
rather far from the crucial region, with presently foreseen luminosities.
Concerning neutral kaon decays, DA
NE experiments can observe a few
decays [2], enough to establish the effect, but
to a precision unlikely to reveal any CPT anomaly in
.
Nonetheless, since DANE should significantly improve presently existing
data and/or bounds on
decays, it is appropriate to
discuss in this Handbook the present status-of-the-art of this field.