N. Nuñez-Dallos, et al.
InorganicaChimicaActa498(2019)119136
coordination polymer in one dimension (1-D) as an efficient catalyst for
three-component azide-alkyne cycloadditions to obtain 1,4-dis-
ubstituted 1,2,3-triazoles from organic halides, sodium azide and
terminal alkynes under mild reaction conditions (T < 50 °C, 5% mol
catalyst, in air) and short reaction time (t < 3 h).
Table 1
Crystal data and structure refinement for Cu(I) CP.
Empirical formula
C20H16CuIN6
Formula weight
530.83
Temperature/K
293(2)
Crystal system
Monoclinic
Space group
P21/n (no. 14)
2. Experimental section
a/Å
11.2216(11)
b/Å
11.4710(11)
2.1. General
c/Å
15.0558(16)
α/°
90
β/°
92.770(6)
All reagents and solvents were purchased from commercial sources
and used as received. All solvents used in this work were of analytical
grade. The reactions were monitored by thin layer chromatography
(TLC) on silica gel plates and observed under UV lamps (254 nm or
365 nm). The ligand 1,3-bis(1H-benzotriazol-1-ylmethyl)benzene (L)
was prepared by a modified literature procedure [20–22], in one-step
process at reflux, using commercially available reagents (m-xylylene
dibromide and 1H-benzotriazole), and without using an organic base.
Detailed synthesis and characterization are shown in the
Supplementary Information.
γ/°
90
Volume/Å3
1935.8(3)
Z
4
ρcalc g/cm3
1.821
μ/mm−1
14.261
F(0 0 0)
1040.0
Crystal size/mm3
Radiation
0.36 × 0.152 × 0.102
Cu Kα (λ = 1.54178)
2Θ range for data collection/°
Index ranges
9.61 to 131.3
−13 ≤ h ≤ 13, −13 ≤ k ≤ 13, −17 ≤ l ≤ 17
Reflections collected
Independent reflections
Data/restraints/parameters
Goodness-of-fit on F2
Final R indexes [I > = 2σ (I)]
Final R indexes [all data]
Largest diff. peak/hole/e Å−3
42,946
3322 [Rint = 0.1041, Rsigma = 0.0511]
NMR data were recorded on a Bruker Avance 400 spectrometer
(400.13 MHz for 1H; 100.61 MHz for 13C). 1H and 13C NMR chemical
shifts are reported in parts per million (ppm) relative to TMS, with the
residual solvent peak used as an internal reference. High resolution
mass spectra (HRMS) were obtained on an Agilent Technologies Q-TOF
6520 spectrometer via electrospray ionization (ESI) in the positive ion
mode. Infrared spectra (FT-IR) were recorded on a Thermo Nicolet
Nexus 470 ESP FT-IR spectrometer using KBr discs. Elemental analysis
(C, H and N) was performed with a Thermo Scientific™ FLASH 2000
CHNS/O Analyzer. Thermogravimetric analysis (TGA) was performed
on a NETZSCH STA 409 PC/PG instrument in a nitrogen atmosphere
with a continuous flow of 100 mL min−1 and a heating rate of
10 °C min−1, from 30 to 700 °C. Melting points were determined in
open capillary tubes on a Mel-Temp® Electrothermal melting point
apparatus and are uncorrected.
3322/0/254
1.062
R
1 = 0.0591, wR2 = 0.1155
R1 = 0.0984, wR2 = 0.1347
0.65/−1.43
2.3. X-ray crystallography
Single crystals of the Cu(I) CP for X-ray structural analysis were
obtained after a few days by slow evaporation in acetonitrile solution. A
suitable crystal was selected and mounted using
a MiTeGen
MicroMount. Intensity data were collected at room temperature on a
Bruker D8 VENTURE diffractometer equipped with a bidimensional
CMOS Photon100 detector, using graphite monochromated Cu-Kα ra-
diation. The structure solution and refinement were carried out with
OLEX2 [23]. The structure was solved by direct methods using the
SHELXS software [24]. The complete structure was refined by the full
the SHELXL software [25]. All non-hydrogens were refined with ani-
sotropic displacement coefficients, and all hydrogen atoms were placed
in idealized locations. Molecular graphics were generated using Mer-
cury 3.3 [26]. Color codes for molecular graphics were orange (Cu),
blue (N), grey I, white (H) and purple (I). Crystal data and details of
data collection for the Cu(I) CP are reported in Table 1.
The electronic absorption spectra were measured in DMSO solution
with a Varian Cary 100 Conc (Agilent Technologies) spectrophotometer
from 200 to 800 nm, and in a quartz cuvette having a path length of
1 cm. Solid state emission and excitation spectra of the Cu(I) CP (at
λ
ex = 342 nm; λem = 538 nm) were recorded by using a CARY Eclipse
(Agilent Technologies) fluorescence spectrophotometer with the solid
sample holder accessory at room temperature (20 °C). Both the excita-
tion and emission slit widths were 5 nm. During the luminescence
measurements, a low voltage detector was used for the complex due to
its strong solid-state emission.
on a Rigaku Ultima III X-ray diffractometer with Cu-Kα radiation
(λ = 1.54056 Å). The samples were scanned using a step size of 0.02°
2.2. Synthesis of the 1-D Cu(I) coordination polymer catena-poly[bis-μ-
[1,3-bis(1H-benzotriazol-κN3-1-ylmethyl)benzene]dicopper(I)-di-μ-iodo]
and
a scan speed of 2 s per step (Fig. S8, see Supplementary
Information).
CuI (241 mg, 1.24 mmol) was added to a solution of 1,3-bis(1H-
benzotriazol-1-ylmethyl)benzene (400 mg, 1.16 mmol) in acetonitrile
(24 mL). The resulting solution was stirred for 1 h at room temperature,
giving a yellow solid. The precipitate was isolated by vacuum filtration,
washed with acetonitrile, and dried under vacuum. Yield: 510 mg
(82%). mp 236–238 °C. IR (KBr, cm−1): ν 3059 (w), 3029 (w), 2969
(w), 2932 (w), 1611 (w), 1591 (w), 1497 (w), 1454 (m), 1313 (m),
1270 (w), 1224 (s), 1162 (m), 1135 (w), 1114 (m), 1002 (w), 971 (w),
901 (w), 779 (s), 757 (s), 741 (s). 1H NMR (400 MHz, DMSO‑d6): δ
(ppm) 8.05 (d, J = 7.6 Hz, 2H), 7.73 (d, J = 8.1 Hz, 2H), 7.46 (t,
J = 7.4 Hz, 2H), 7.41 – 7.34 (m, 3H), 7.31 (d, J = 7.1 Hz, 1H), 7.25 (d,
J = 7.1 Hz, 2H), 5.94 (s, 4H). Anal. Calcd. for C20H16N6CuI: C, 45.25;
H, 3.04; N, 15.83. Found: C, 44.20; H, 3.27; N, 15.10. HRMS (ESI+) m/
2.4. Computational details
Relativistic density functional theory calculations [27] were carried
Slater basis set, plus two polarization functions (STO-TZ2P) for valence
electrons, within the generalized gradient approximation (GGA) ac-
cording to the Perdew-Burke-Ernzerhof (PBE) exchange-correlation
functional [30,31] because of its improved performance on long-range
core approximation was applied to the [1s2-3p6] shells for Cu, [1s2-4p6]
for I, and [1s2] for C and N, leaving the remaining electrons to be
treated variationally. Geometry optimizations were performed without
any symmetry restraint, via the analytical energy gradient method
z 341.1524 [L + H]+, 592.9076 [Cu2I(L)]+, 743.2182 [Cu(L)2]+
,
933.0518 [Cu2I(L)2]+, 1124.8863 [Cu3I2(L)2]+. UV–vis (DMSO) [λmax
(log ε), nm (M−1 cm−1)]: 263 (4.29), 283 (4.12).
2