We study the scaling of kaon decay amplitudes with the number of colours, $$N_c$$
N
c
, in a theory with four degenerate flavours, $$N_f=4$$
N
f
=
4
. In this scenario, two current-current operators, $$Q^\pm $$
Q
±
, mediate $$\Delta S=1$$
Δ
S
=
1
transitions, such as the two isospin amplitudes of non-leptonic kaon decays for $$K\rightarrow (\pi \pi )_{I=0,2}$$
K
→
(
π
π
)
I
=
0
,
2
, $$A_0$$
A
0
and $$A_2$$
A
2
. In particular, we concentrate on the simpler $$K\rightarrow \pi $$
K
→
π
amplitudes, $$A^\pm $$
A
±
, mediated by these two operators. A diagrammatic analysis of the large-$$N_c$$
N
c
scaling of these observables is presented, which demonstrates the anticorrelation of the leading $${{\mathcal {O}}}(1/N_c)$$
O
(
1
/
N
c
)
and $${{\mathcal {O}}}(N_f/N_c^2)$$
O
(
N
f
/
N
c
2
)
corrections in both amplitudes. Using our new $$N_f=4$$
N
f
=
4
and previous quenched data, we confirm this expectation and show that these corrections are naturally large and may be at the origin of the $$\Delta I=1/2$$
Δ
I
=
1
/
2
rule. The evidence for the latter is indirect, based on the matching of the amplitudes to their prediction in Chiral Perturbation Theory, from which the LO low-energy couplings of the chiral weak Hamiltonian, $$g^\pm $$
g
±
, can be determined. A NLO estimate of the $$K \rightarrow (\pi \pi )_{I=0,2}$$
K
→
(
π
π
)
I
=
0
,
2
isospin amplitudes can then be derived, which is in good agreement with the experimental value.