We find the leading electroweak corrections to the Lagrangians of heavy-quark effective theory and non -relativistic QCD. These corrections appear in the Wilson coefficients of the two-and four-quark operators and are considered here at one-loop order through O(1/m3) and O(1/m2), respectively. The two-quark operators through this order include new parity violating terms, which we derive analogously to the parity preserving QCD result at one-loop order.(c) 2023 Published by Elsevier B.V. This is an open access article under the CC BY license (http:// creativecommons .org /licenses /by /4 .0/). Funded by SCOAP3.