The decay $$D \rightarrow K^-\pi ^+$$
D
→
K
-
π
+
is studied in a sample of quantum-correlated $$D{\bar{D}}$$
D
D
¯
pairs, based on a data set corresponding to an integrated luminosity of 2.93 fb$$^{-1}$$
-
1
collected at the $$\psi (3770)$$
ψ
(
3770
)
resonance by the BESIII experiment. The asymmetry between $$C\!P$$
C
P
-odd and $$C\!P$$
C
P
-even eigenstate decays into $$K^-\pi ^+$$
K
-
π
+
is determined to be $${{\mathcal {A}}}_{K\pi } = 0.132 \pm 0.011 \pm 0.007$$
A
K
π
=
0.132
±
0.011
±
0.007
, where the first uncertainty is statistical and the second is systematic. This measurement is an update of an earlier study exploiting additional tagging modes, including several decay modes involving a $$K^0_L$$
K
L
0
meson. The branching fractions of the $$K^0_L$$
K
L
0
modes are determined as input to the analysis in a manner that is independent of any strong phase uncertainty. Using the predominantly $$C\!P$$
C
P
-even tag $$D\rightarrow \pi ^+\pi ^-\pi ^0$$
D
→
π
+
π
-
π
0
and the ensemble of $$C\!P$$
C
P
-odd eigenstate tags, the observable $${{\mathcal {A}}}_{K\pi }^{\pi \pi \pi ^0}$$
A
K
π
π
π
π
0
is measured to be $$0.130 \pm 0.012 \pm 0.008$$
0.130
±
0.012
±
0.008
. The two asymmetries are sensitive to $$r_D^{K\pi }\cos \delta _D^{K\pi }$$
r
D
K
π
cos
δ
D
K
π
, where $$r_D^{K\pi }$$
r
D
K
π
and $$\delta _D^{K\pi }$$
δ
D
K
π
are the ratio of amplitudes and phase difference, respectively, between the doubly Cabibbo-suppressed and Cabibbo-favoured decays. In addition, events containing $$D \rightarrow K^-\pi ^+$$
D
→
K
-
π
+
tagged by $$D \rightarrow K^0_{S,L} \pi ^+\pi ^-$$
D
→
K
S
,
L
0
π
+
π
-
are studied in bins of phase space of the three-body decays. This analysis has sensitivity to both $$r_D^{K\pi }\cos \delta _D^{K\pi }$$
r
D
K
π
cos
δ
D
K
π
and $$r_D^{K\pi }\sin \delta _D^{K\pi }$$
r
D
K
π
sin
δ
D
K
π
. A fit to $${{\mathcal {A}}}_{K\pi }$$
A
K
π
, $${{\mathcal {A}}}_{K\pi }^{\pi \pi \pi ^0}$$
A
K
π
π
π
π
0
and the phase-space distribution of the $$D \rightarrow K^0_{S,L} \pi ^+\pi ^-$$
D
→
K
S
,
L
0
π
+
π
-
tags yields $$\delta _D^{K\pi }= \left( 187.6 {^{+8.9}_{-9.7}}{^{+5.4}_{-6.4}} \right) ^{\circ }$$
δ
D
K
π
=
187.6
-
9.7
+
8.9
-
6.4
+
5.4
∘
, where external constraints are applied for $$r_D^{K\pi }$$
r
D
K
π
and other relevant parameters. This is the most precise measurement of $$\delta _D^{K\pi }$$
δ
D
K
π
in quantum-correlated $$D{\bar{D}}$$
D
D
¯
decays.