Page 3 of 5
Journal of the American Chemical Society
a function of uptake, indicating the presence of cooperativity
of host-guest and guest-guest binding.
–CH bond of the NO -decorated phenyl ring [–
CH···CC(centroid) = 3.11(4) Å]. Moreover, there is a weak
2
21
1
2
3
4
5
6
7
8
9
π···π interaction between CC bond of C D (IV) and the
To establish the role of these functional groups on C H2
2
2
2
NO2-decorated phenyl ring [ring centroid···CC(centroid) =
.46(8) Å]. Site V (occupancy = 0.16) is at the window be-
binding, adsorption of CH , as a non-interacting gas probe,
4
4
was also measured. At 298 K and 20 bar, MFM-102 shows a
3
-1
tween the cylindrical and spherical cages involving similar
CH4 uptake of 236 cm g , which is higher than that for
MFM-102-NO , MFM-102-NH and MFM-111 (188, 179 and 173
side-on mode interactions with the –CH group of the NO2-
2
2
3
-1
decorated phenyl ring [–CH···CC(centroid) = 2.63(5) Å] and
cm g , respectively). The trend in uptake of CH is con-
4
the hydrogen bond to the -NO group [D···ONO2 = 3.05(10),
sistent with the variation of BET surface areas of these mate-
rials, and suggests potential binding interactions between the
2
3.17(7) Å]. Site VI (occupancy = 0.09) is located in the center
of the elongated cage, interacting directly with the -NO2
-
NO functional group and unsaturated C H .
2 2 2
1
1
1
1
1
1
1
1
1
1
2
2
2
2
2
2
2
2
2
2
3
3
3
3
3
3
3
3
3
3
4
4
4
4
4
4
4
4
4
4
5
5
5
5
5
5
5
5
5
5
6
0
1
2
3
4
5
6
7
8
9
0
1
2
3
4
5
6
7
8
9
0
1
2
3
4
5
6
7
8
9
0
1
2
3
4
5
6
7
8
9
0
1
2
3
4
5
6
7
8
9
0
group from three surrounding ligands with D···ONO dis-
2
tances ranging from 2.37(1) to 2.56(3) Å. Overall, C D mole-
2
2
cules at sites III-VI are all directly associated with the –NO2
groups in the pore, confirming the positive effect of -NO2
group on achieving optimal acetylene binding.
-1)
Neutron energy loss (cm
0
200 400 600 800 1000 1200 1400 1600
Diff-C H
2
2
Solid C H
2
2
0
25
50
75
100 125 150 175 200
Neutron energy loss (meV)
Figure 4. INS spectra for MFM-102-NO
son of difference INS plots derived by subtracting INS spectra for
-loaded MFM-102-NO and bare MFM-102-NO spectra (black),
with condensed C in the solid state (red).
2 2 2
with C H loading. Compari-
C
2
H
2
2
2
2 2
H
Figure 3. View of the binding sites for adsorbed C
D
2 2
molecules in
The binding dynamics of C H -loaded MFM-102-NO were
2 2 2
MFM-102-NO . (C, dark grey; O, red; N, blue; Cu, turquoise and C D
2
2 2
also studied by in situ inelastic neutron scattering (INS). The
INS spectrum of bare MOF shows excellent agreement with
that obtained from DFT calculations, thus allowing assign-
ment of vibrational modes (Figure S12). The INS spectrum of
C H -loaded MFM-102-NO shows a significant increase in
2 2 2
intensity (Figures 4 and S11). The INS peaks at 80 and 95 meV
(assigned as the asymmetric and symmetric C-H bending
molecules at site I (light blue), site II (orange), site III (light green),
site IV (dark green), site V (purple) and site VI (sapphire).
Six independent binding sites (I to VI) for adsorbed C D2
2
molecules in MFM-102-NO have been determined by in situ
2
neutron powder diffraction (NPD) (Figure 3). Sites I and II
(
occupancies of 0.41 and 0.40, respectively) are located at the
open Cu(II) sites with a side-on interaction between the CC
bond and Cu(II) [Cu···CC(centroid) = 3.98(5) and 2.93(8) Å
for site I and II, respectively]. Interestingly, sites I and II have
very different bonding distance to the open Cu(II) site. A
closer examination revealed that site I also forms supramo-
lecular interactions to two aromatic –CH groups from two
adjacent phenyl rings [–CH···CC(centroid) = 3.23(2), 3.48(3)
Å] and becomes the most populated location owing to this
cooperativity between sites. Site III (occupancy 0.31) is stabi-
lised by a combination of three types of interactions to the
mode of C
adsorption of C
sides and a shift to lower energy. In addition, the translation-
al modes of C molecules, represented by the INS peaks at
low energy region (below 25 meV), show restricted motion
on adsorption, with adsorbed C molecules well-ordered in
the pore as these peaks all shift to lower energy but still re-
main a three-fold feature as found in solid C . Moreover,
in the difference spectra, peaks at 164 and 189 meV (Figure
S12) develop upon inclusion of C molecules in the pore,
and this enhancement of both symmetrical and anti-
symmetrical stretching modes of -NO groups confirms the
formation of host-guest interactions between the -NO
groups and adsorbed C molecules. Overall, these results
are highly consistent with the crystallographic studies show-
H , respectively) show significant broadening on
2 2
H
2 2
with the appearance of shoulders on both
H
2 2
H
2 2
H
2 2
H
2 2
+
host: (i) hydrogen bonds between the D(δ ) of C D mole-
2
2
-
cules and O(δ ) center of the –NO group [D···O = 1.99(9),
2
2
2.35(6) Å]; (ii) supramolecular interactions between the CC
2
bond and the –CH group on adjacent NO -decorated phenyl
H
2 2
2
rings [–CH···CC(centroid) = 2.47(9), 2.80(4) Å]; (iii) inter-
molecular dipole interactions between π-electrons on CC
bond (site III) and D-atoms of C D at site IV. Site IV (occu-
ing various binding sites (I-VI) of C
action between the –NO group and C
VI) in the pore of MFM-102-NO
D
and the strong inter-
2
2
D
2
molecules (site III-
2
2
2
2
pancy 0.26) is also stabilised by hydrogen bonds between
C D molecules and –NO groups [D···O = 1.69(2) Å] and a
.
2
2
2
2
NO2
3
ACS Paragon Plus Environment