  We study the production of the stable six-quark $H$ dibaryon via the
$(K^-,K^+)$ reaction on a $^{12}$C target within a covariant effective
Lagrangian model. The calculations are performed within a factorization
approximation, in which the full production amplitude is written as a product
of the amplitudes for the $K^- + p \to K^+ + \Xi^-$ and $\Xi^- + p \to H$
processes. The $K^+\Xi^-$ production vertex is described by excitation,
propagation and decay of $\Lambda$ and $\Sigma$ resonance states in the initial
collision of a $K^-$ meson with a target proton in the incident channel. The
parameters of the resonance vertices are taken to be the same as those
determined previously by describing the available data on total and
differential cross sections for the $p(K^-, K^+)\Xi^-$ reaction within a
similar model. The $\Xi^- + p \to H$ fusion process is treated within a quark
model where the $H$ dibaryon is considered as a stable particle. For the $K^+$
meson angle fixed at 0$^o$, the $H$ production cross-section is found to be
about 2.9 $\mu b/sr$ for $H$ mass just below the $\Lambda \Lambda$ threshold at
a $K^-$ beam momentum of 1.67 GeV/c. This is an order of magnitude larger than
the value for this quantity reported earlier in calculations performed on a
$^3$He target using a different model for the cascade hyperon production. We
have also calculated the beam momentum dependence of the $H$ production cross
section and the energy spectrum of the emitted $K^+$ meson.
