We present a new simulation for Higgs boson production in association with bottom quarks ($$ b\overline{b}H $$
b
b
¯
H
) at next-to-leading order (NLO) accuracy matched to parton showers in hadronic collisions. Both contributions, the standard one proportional to the bottom-quark Yukawa coupling and the loop-induced one proportional to the top-quark Yukawa coupling from the gluon-fusion process, are taken into account in a scheme with massive bottom quarks. Therefore, we provide the full simulation of the $$ b\overline{b}H $$
b
b
¯
H
final state in the Standard Model, which constitutes also a crucial background to measurements for Higgs-boson pair (HH) production at the Large Hadron Collider when at least one of the Higgs bosons decays to bottom quarks. So far, the modeling of the $$ b\overline{b}H $$
b
b
¯
H
final state induced one of the dominant theoretical uncertainties to HH measurements, as the gluon-fusion component was described only at the leading order (LO) with uncertainties of $$ \mathcal{O} $$
O
(100%). Including NLO corrections in its simulation allows us to reduce the scale dependence to $$ \mathcal{O} $$
O
(50%) so that it becomes subdominant with respect to other systematic uncertainties. As a case study, we provide an in-depth analysis of the $$ b\overline{b}H $$
b
b
¯
H
background to HH measurements with realistic selection cuts in the 2b2γ channel. We also compare our novel simulation with the currently-employed ones, discussing possible issues and shortcomings of a scheme with massless bottom quarks. Finally, we propagate the effect of the new $$ b\overline{b}H $$
b
b
¯
H
simulation to HH searches in the 2b2γ and 2b2τ final states, and we find an improvement of up to 10% (20%) on the current (HL-LHC) limits on $$ {\sigma}_{\textrm{SM}}^{HH} $$
σ
SM
HH
.