After publication of Ref. 1, it has been brought to our attention that Hochstrasser and co-workers have studied essentially the same molecular system (i.e.,

${\rm N}_3^-$
N3 in H2O instead of D2O) by two-color 2D IR spectroscopy before us.2 A cross peak is also observed, which less likely is due to population transfer because of the even larger energy gap from the
${\rm N}_3^-$
N3
asymmetric stretch vibration to the H2O band. We had based our conclusion, that population transfer is the dominant coupling mechanism, mostly on the large frequency separation of the 0-1 and the 1-2 transition in the 2D IR spectra, which reflects the large anharmonicity of the OD vibrator itself.1 The 1-2 transition is not shown in Ref. 2, so we cannot decide whether an alternative coupling mechanism might be responsible for the cross-peak between
${\rm N}_3^-$
N3
in H2O. Nonetheless, Ref. 2 found a tilt in the cross-peak, evidencing a correlation in the vibrational frequencies the of
${\rm N}_3^-$
N3
and the H2O vibrations, which is another consequence of the coupling to azide-bound water.

1.
J.
Borek
,
F.
Perakis
,
F.
Kläsi
,
S.
Garrett-Roe
, and
P.
Hamm
,
J. Chem. Phys.
136
,
224503
(
2012
).
2.
C.-H.
Kuo
,
D. Y.
Vorobyev
,
J.
Chen
, and
R. M.
Hochstrasser
,
J. Phys. Chem. B
111
,
14028
(
2007
).