AbstractWe study the quantum structure of four-dimensional $${{\mathcal {N}}}=2$$
N
=
2
superfield sigma-model formulated in harmonic superspace in terms of the omega-hypermultiplet superfield $$\omega $$
ω
. The model is described by harmonic superfield sigma-model metric $$g_{ab}(\omega )$$
g
ab
(
ω
)
and two potential-like superfields $$L^{++}_{a}(\omega )$$
L
a
+
+
(
ω
)
and $$L^{(+4)}(\omega )$$
L
(
+
4
)
(
ω
)
. In bosonic component sector this model describes some hyper-Kähler manifold. The manifestly $${{\mathcal {N}}}=2$$
N
=
2
supersymmetric covariant background-quantum splitting is constructed and the superfield proper-time technique is developed to calculate the one-loop effective action. The one-loop divergences of the superfield effective action are found for arbitrary $$g_{ab}(\omega ), L^{++}_{a}(\omega ), L^{(+4)}(\omega )$$
g
ab
(
ω
)
,
L
a
+
+
(
ω
)
,
L
(
+
4
)
(
ω
)
, where some specific analogy between the algebra of covariant derivatives in the sigma-model and the corresponding algebra in the $${{\mathcal {N}}}=2$$
N
=
2
SYM theory is used. The component structure of divergences in the bosonic sector is discussed.