Journal of the American Chemical Society
Communication
attributed this to the formation of multiple phases, preventing
selective crystallization of fjh. Alternative synthetic conditions
favor the formation of a 2D COF with a defected tth
topology.21 In this 2D COF, the TFB units adopt dihedral
angles between 32 and 51°.
Synthesis and full characterization of COF-790, COF-
791, and COF-792 including EA, FT-IR spectroscopy,
NMR spectra, PXRD data, computational modeling, gas
uptake measurements, TGA, SEM images, and HRTEM
To demonstrate the versatility of our design strategy, we also
report a series of isoreticular structures of COF-790, namely
COF-791 and COF-792, where we replaced the square-planar
ETTA unit of COF-790 with 1,2,4,5-tetrakis(4-aminophenyl)-
benzene (TAPB) and 1,2,4,5-tetrakis(4-aminophenyl)-3′,6′-
dimethylbenzene (TAPB-Me), respectively (Figure 3). COF-
791 ([(TTFB)4(TAPB)3]imine) and COF-792 ([(TTFB)4-
(TAPB-Me)3]imine) were synthesized and characterized as
demonstrated for COF-790 (see SI, section S2). Formation
of COF-791 and COF-792 was corroborated by FT-IR and
CP-MAS 13C NMR spectroscopies. Disappearance of the
X-ray crystallographic data for COF-790 (CIF)
X-ray crystallographic data for COF-791 (CIF)
X-ray crystallographic data for COF-792 (CIF)
X-ray crystallographic data for TAPB-Amine (CIF)
X-ray crystallographic data for TTFP-Aniline (CIF)
AUTHOR INFORMATION
Corresponding Author
■
Omar M. Yaghi − Department of Chemistry, University of
California Berkeley; Kavli Energy Nanoscience Institute at
UC Berkeley; and Berkeley Global Science Institute, Berkeley,
California 94720, United States; Joint UAEU-UC Berkeley
Laboratories for Materials Innovations, Berkeley, California
aldehyde functionality, assigned to the resonances at νC=O
=
1692 cm−1, indicated successful imine formation (νC=N = 1628
cm−1; see SI, section S4). Solid-state 13C NMR spectra of
COF-791 and COF-792 displayed resonances associated with
the imine functionality at 161.5 and 160.6 ppm, respectively.
Moreover, at 18.7 and 18.9 ppm, we observed the resonances
corresponding to the methyl groups in COF-791 and COF-792
Authors
Ha L. Nguyen − Department of Chemistry, University of
California Berkeley; Kavli Energy Nanoscience Institute at
UC Berkeley; and Berkeley Global Science Institute, Berkeley,
California 94720, United States; Joint UAEU-UC Berkeley
Laboratories for Materials Innovations, Berkeley, California
Cornelius Gropp − Department of Chemistry, University of
California Berkeley; Kavli Energy Nanoscience Institute at
UC Berkeley; and Berkeley Global Science Institute, Berkeley,
Yanhang Ma − School of Physical Science and Technology,
ShanghaiTech University, Shanghai 201210, China;
Chenhui Zhu − Advanced Light Source, Lawrence Berkeley
National Laboratory, Berkeley, California 94720, United
States
The atomic compositions of COF-791 and COF-792 were
determined by EA (COF-791: Calcd for C210H150N12
corresponding to [(TTFB)4(TAPB)3]imine: C, 88.76; H, 5.32;
N, 5.92%. Found: C, 86.80; H, 5.51; N, 5.97%. COF-792:
Calcd for C216H162N12 corresponding to [(TTFB)4(TAPB-
Me)3]imine: C, 88.67; H, 5.58; N, 5.75%. Found: C, 86.58; H,
6.02; N, 5.55%). COF-791 and -792 showed an onset in
thermal decomposition under a N2 atmosphere at around 400
°C (see SI, section S6). SEM micrographs indicated a
homogeneous size in crystallites of cube (∼300−400 nm)
and needle shapes (∼200 nm) for COF-791 and -792,
respectively.
The crystal structures of COF-791 and -792 were built
analogously to the fjh net of COF-790. Based on the model
structures, COF-791 and COF-792 displayed pore diameters
of 22.8 and 22.4 Å, respectively. N2 adsorption isotherms at 77
K of COF-791 and COF-792 demonstrated permanent
porosity and a Type I isotherm with mesoporous pore
structures. The BET surface area was calculated to be 1920
m2 g−1 for COF-791 and 2250 m2 g−1 for COF-792. Analysis
of the pore size distribution yielded diameters of 19.0 Å for
COF-791 and 22.6 Å for COF-792, both in good agreement
with their theoretical values estimated from their model
structures.
The lowest angle peaks of COF-791 and -792, as measured
by WAXS, appeared at 1.89° (λ = 1.24 Å). A shift to lower d-
spacing was observed for the isoreticular forms of COF-790
due to the slight enlargement of the unit cell parameters with
increasing linker lengths of the TAPB units (Figure 3).
HRTEM analysis of COF-791 indicated lattice fringes of 25 Å,
which were attributed to the 220 lattice plane. Owing to the
higher relative crystallinity of COF-792, lattice fringes with d-
spacings of 44 Å were identified, which corresponds to the 110
Complete contact information is available at:
Notes
The authors declare no competing financial interest.
ACKNOWLEDGMENTS
■
C.G. is a Leopoldina postdoctoral fellow of the German
National Academy of Science (LPDS 2019-02) and acknowl-
edges the receipt of a fellowship of the Swiss National Science
Foundation (P2EZP2-184380). We acknowledge King Abdu-
laziz City for Science and Technology as part of a joint
KACST−UC Berkeley collaboration and UAE University as
part of a joint UAEU−UC Berkeley collaboration. We thank
Mr. Hao Lyu (Yaghi group, UC Berkeley) for help in obtaining
SEM images and Dr. Tianqiong Ma (Yaghi group, UC
Berkeley) for initial efforts in growing crystals of COF-791.
This research used beamline 7.3.3 of the Advanced Light
Source, which is a DOE Office of Science User Facility under
contract no. DE-AC02-05CH11231. This work is supported by
the National Natural Science Foundation of China (No.
21875140) and CℏEM SPST, ShanghaiTech University
(#EM02161943) for TEM measurements. We acknowledge
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