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Crystal Growth & Design is published by the American Chemical Society. 1155Sixteenth Street N.W., Washington, DC 20036Published by American Chemical Society. Copyright © American Chemical Society.However, no copyright claim is made to original U.S. Government works, or worksproduced by employees of any Commonwealth realm Crown government in the courseof their duties.
Article
Cuprous Halide Complexes of a Variable Length Ligand: Helices,Cluster Chains and Nets Containing Large Solvated Channels
William J. Gee, and Stuart Robert BattenCryst. Growth Des., Just Accepted Manuscript • DOI: 10.1021/cg3018858 • Publication Date (Web): 09 May 2013
Downloaded from http://pubs.acs.org on May 19, 2013
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Cuprous Halide Complexes of a Variable Length
Ligand: Helices, Cluster Chains and Nets Containing
Large Solvated Channels
William J. Gee and Stuart R. Batten*
School of Chemistry, Monash University, Clayton, Victoria, 3800, Australia
Supporting Information Placeholder
ABSTRACT: The variable-length azacrown ether bridging ligand N,N'-bis(3-pyridyl-methyl)diaza-18-
crown-6 (b3pmdc) has been reacted with cuprous iodide to give a range of new discrete and polymeric
coordination compounds. Six structurally diverse CuI(b3pmdc) architectures were isolated as well as a
single oxidized CuII(b3pmdc) species. These include the helical 1D chain
[H4b3pmdc][Cu10I14]·CHCl3·2H2O (1), the luminescent linear cluster chain [Cu4I6(H2b3pmdc)] (2), the
guest water containing network [Cu4I4(Hb3pmdc)2](1.5ClO4)(0.5I3)·3.5H2O·2.5MeOH (3), the
luminescent cubane cluster chain [Cu4I4(b3pmdc)2] (4), the 3D net [Cu9I12(Kb3pmdc)3(H2O)4]·9MeOH
(5), the dinuclear mixed halide [Cu2Cl3.4I2.6(H4b3pmdc)] (6) and the cupric 1D chain
[CuCl2(H2b3pmdc)(MeOH)2]·2Cl·2MeCN (7). Manipulation of the ligand conformation was achieved
by the addition of the alkali metal salt potassium and by varying the pH of the solution with a range of
acids (HCl, HClO4). In the case of 2 and 4 green and yellow luminescent emission was observed, as a
result of the varied metal environment.
New molecular tools are needed to foster new developments in the growing field of crystal
engineering, with the goal of accelerating the development of materials with advantageous properties.1
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An emerging tool for the crystal engineer is the variable length ligand, which offers the ability to
manipulate the length and geometry of an organic linker in a predicable manner in response to chemical
stimuli. Proof of principle was recently demonstrated using a para-pyridyl substituted azacrown ether
ligand that exhibited variation in length ranging from ca. 7.7 Å to 16.6 Å as a result of coordination of
alkali, alkaline earth and transition metals.2 That same ligand was recently shown to manipulate spin
crossover properties in FeII compounds as a result of varying the guest molecule which, in turn, afforded
differing packing arrangements.3 Previously, related diazamacrocyclic ligands have shown promise as
molecular tectons, however targeted manipulation of ligand length was not reported.4
This work focuses on a meta-pyridyl variant of the dipyridyl azacrown ether family, namely N,N'-
bis(3-pyridyl-methyl)diaza-18-crown-6 (b3pmdc), reacted in cuprous iodide solution. Cuprous iodide
has been demonstrated to stabilize a diverse array of inorganic architectures, including 1D chains of
cubane clusters linked by organic spacers,5 polymeric CuxIy chains of varying ratios,5a,6 dinuclear
species,5e-g,7 discrete clusters,5c,6b,8 calixarene complexes,9 mixed valence clusters,10 CuI slabs11 and
nanosized wheels.12 These cuprous iodide species have unique properties including
photoluminescence5a-c,5e,5g,6c,13 and electrical conductivity,6a,11 allowing their potential application in
organic light-emitting diodes (OLEDs)5e and hybrid materials with second-order nonlinear optical
(NLO) responses.11
The rich diversity of chemical motif and application has drawn inorganic chemists seeking to put
ligands through a gamut of varying coordination modes and architectures,5f,7b,8a thereby demonstrating
their utility, as we aim to achieve here. Thus we report the synthesis and characterization of six
structurally-diverse CuI(b3pmdc) architectures, as well as a single oxidized CuII(b3pmdc) species.
These include the helical 1D chain [H4b3pmdc][Cu10I14]·CHCl3·2H2O (1), the luminescent linear cluster
chain [Cu4I6(H2b3pmdc)] (2), the guest water containing network
[Cu4I4(Hb3pmdc)2](1.5ClO4)(0.5I3)·3.5H2O·2.5MeOH (3), the luminescent cubane cluster chain
[Cu4I4(b3pmdc)2] (4) and the 3D net [Cu9I12(Kb3pmdc)3(H2O)4]·9MeOH (5). The use of hydrochloric
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acid yielded a dinuclear mixed halide [Cu2Cl3.4I2.6(H4b3pmdc)] (6) and a cupric 1D chain
[CuCl2(H2b3pmdc)(MeOH)2]·2Cl·2MeCN (7). Each of these species has been characterized using
single-crystal X-ray crystallography, supported by infrared spectroscopy, thermogravimetric analysis
and, in the case of 2 and 4, fluorescence spectrometry.
Experimental Section
General Remarks. CAUTION: Metal perchlorates are potentially explosive! Only a small amount of
material should be prepared and handled with great care. The ligand b3pmdc was synthesized
according to a literature procedure14 using chemicals purchased from Sigma-Aldrich. A stock solution
of cuprous perchlorate was created by refluxing cupric perchlorate hydrate with an excess of copper
powder in acetonitrile for two hours. The resultant clear solution was filtered and stored under nitrogen.
Metal salts were purchased from Alfa Aesar. All yields shown are relative to Cu(ClO4)2�6H2O which in
each case is limiting.
Physical Measurements. Solid-state IR spectra were recorded using a Perkin Elmer 1600 series FTIR
or a Bruker Equinox 55 Infrared Spectrometer fitted with a Specac Diamond ATR source. Infrared band
frequencies are reported in wavenumbers (cm-1) and intensities are reported as strong (s), medium (m)
or weak (w). Thermogravimetric analysis was performed using a Mettler Toledo TGA/DSC 1 STARe
System and Software. Elemental analyses were performed by Campbell Microanalytical Laboratory,
Department of Chemistry, University of Otago, Dunedin, New Zealand. Solid-state photoluminescence
measurements were undertaken for single crystals of 2 and 4 using a fibre optic probe coupled to a
Varian Cary Eclipse fluorescence spectrophotometer. Sample emissions were passed through a
monochromator (CVI, dk480) and focused onto a fast response avalanche photodiode detector (APD,
Id-Quantique, Id-100).
Synthesis. [H4b3pmdc][Cu10I14]�CHCl3�2H2O (1). Compound 1 was obtained by slow diffusion of
solutions of cuprous perchlorate (0.06 mmol in 1 mL CH3CN) and b3pmdc (50 mg, 0.11 mmol) in
CHCl3 (1 mL) containing perchloric acid (0.23 mmol) into a buffer layer (1:1 CHCl3:MeOH, 1 mL)
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containing tetraethylammonium iodide (40 mg, 0.15 mmol). A crop of yellow crystals suitable for X-ray
analysis grew in the metal-rich layer after 24 h. The crystals were isolated by decanting the mother
liquor, washing with CH3CN followed by filtration. Yield: 4 mg, 23%. Anal. Calcd for
C25H41Cl3Cu10I14N4O6: C, 9.97; H, 1.37; N, 1.86. Found: C, 10.21; H, 1.50; N, 1.76. IR (ATR): υmax
3156w, 3111w, 3062w, 3014w, 2950w, 2736w, 1628w, 1599w, 1540m, 1462m, 1429w, 1400w, 1349w,
1311w, 1273w, 1251m, 1075s, 990m, 968m, 937m, 914m, 788m, 752m, 672m, 622m.
[Cu4I6(H2b3pmdc)] (2). Crystals were obtained from the same reaction as 1. Crystals grew in the
ligand-rich and buffer regions. Yield: 12 mg, 55%. Anal. Calcd for C12H19Cu2I3N2O2: C, 19.71; H, 2.62;
N, 3.83. Found: C, 19.82; H, 2.64; N, 3.90. IR (ATR): υmax 3158w, 3093w, 3047m, 2993w, 2952w,
2892m, 2631m, 1638w, 1609w, 1545m, 1466m, 1354m, 1258m, 1086s, 1024m, 991w, 970w, 902w,
803m, 678m, 622m.
[Cu4I4(Hb3pmdc)2](1.5ClO4)(0.5I3)·3.5H2O·2.5MeOH (3). Compound 3 was obtained by slow
diffusion of solutions of cuprous perchlorate (0.06 mmol in 1 mL CH3CN) and b3pmdc (50 mg, 0.11
mmol) in CHCl3 (1 mL) containing perchloric acid (0.11 mmol) into a buffer layer (1:1 CHCl3:MeOH, 1
mL) containing tetraethylammonium iodide (40 mg, 0.15 mmol). A small number of red crystals were
manually separated from a large quantity of yellow amorphous material after a period of two weeks.
Yield: 3 mg, 3%. The low yield precluded elemental analysis. υmax 3429w, 2871w, 1601w, 1478w,
1431m, 1353w, 1271w, 1192w, 1074s, 931m, 817w, 781w, 707m, 648w, 622m.
[Cu4I4(b3pmdc)2] (4). Obtained by slow diffusion of solutions of cuprous perchlorate (0.06 mmol in
1 mL CH3CN) and b3pmdc (50 mg, 0.11 mmol) in CHCl3 (1 mL) into a buffer layer (1:1
CHCl3:CH3CN, 1 mL) containing tetraethylammonium iodide (40 mg, 0.15 mmol). Colorless crystals
were observed after several days. Yield: 15 mg, 61%. Anal. Calcd for C48H72Cu4I4N8O8: C, 34.92; H,
4.40; N, 6.79. Found: C, 34.85; H, 4.37; N, 6.59. IR (ATR): υmax 2850m, 1597m, 1474m, 1426s, 1352m,
1299m, 1254m, 1192m, 1119s, 1040s, 992s, 947m, 909m, 836m, 795m, 701s, 649m.
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[Cu9I12(Kb3pmdc)3(H2O)6]�9MeOH (5). Obtained by slow diffusion of solutions of cupric
perchlorate hydrate (43 mg, 0.12 mmol) in CH3OH (1 mL) and b3pmdc (50 mg, 0.11 mmol) in CHCl3
(1 mL) into a buffer layer (1:1 CHCl3:CH3OH, 1 mL) containing potassium iodide (25 mg, 0.15 mmol).
Red crystals were observed after a number of days. Yield: 21 mg, 77%. Anal. Calcd for
C27H32Cu3I4KN4O8 (1 - 5MeOH): C, 25.44; H, 3.66; N, 4.24; I, 38.40. Found: C, 25.31; H, 3.69; N,
4.27; I, 38.67. IR (ATR): υmax 2962w, 2869m, 1598w, 1476w, 1429m, 1350w, 1259m, 1090s, 932m,
797s, 706m, 645w, 622m.
[Cu2Cl3.4I2.6(H4b3pmdc)] (6). Obtained by slow diffusion of solutions of cuprous perchlorate
(0.06 mmol in 1 mL CH3CN) and b3pmdc (50 mg, 0.11 mmol) in CHCl3 (1 mL) containing
hydrochloric acid (0.45 mmol) into a buffer layer (1:1 CHCl3:MeOH, 1 mL) containing
tetraethylammonium iodide (40 mg, 0.15 mmol). Yellow crystals suitable for X-ray analysis grew after
several days. The crystals were isolated by decanting the mother liquor, washing with CH3OH followed
by filtration. Yield: 14 mg, 40%. Anal. Calcd for C24H40Cl3.4Cu2I2.6N4O4: C, 28.09; H, 3.93; N, 5.46; Cl
& I, 43.90. Found: C, 27.87; H, 3.90; N, 5.42; Cl & I, 44.34. IR (ATR): υmax 3047w, 2892w, 2632w,
2346w, 1639w, 1610w, 1545m, 1467m, 1354m, 1316w, 1258w, 1086s, 1024m, 991m, 970m, 925m,
903m, 886m, 840m, 826m, 803s, 762m, 677s.
[CuCl2(H2b3pmdc)(MeOH)2]�2Cl�2MeCN (7). Blue crystals of 7 grew a week after exposing the
mother liquor of 6 to air. The crystals were washed with CH3OH and isolated by filtration. Yield: 11
mg, 40%. Anal. Calcd for C30H52Cl4CuN6O6: C, 45.15; H, 6.57; N, 10.53. Found: C, 45.19; H, 6.57; N,
10.60. IR (ATR): υmax 3399s, 2963m, 2916m, 2631m, 1611m, 1484w, 1432m, 1360m, 1257w, 1197w,
1114s, 1077s, 997w, 966w, 937w, 912w, 851w, 810w, 700w, 657w.
X-ray Studies. Diffraction data for 3, 4 and 7 were collected at 123 K on a Bruker X8 Apex equipped
with a KAPPA CCD detector using Mo Kα radiation (λ = 0.71073 Å). Diffraction data for 1,2,5 and 6
were collected at 123 K at either the MX1 or MX2 beamlines at the Australian Synchrotron using
synchrotron radiation (λ = 0.710698 Å). Adsorption corrections based on multiscan methods were
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applied to 2 and 7.15 Apex structures were solved by direct methods in SHELX-9716 and refined by the
full-matrix method based on F2 with the program SHELXL-97 using the X-SEED software package.17
Data collection and integration for the synchrotron structures were performed within Blu-Ice18 and
XDS19 software programs. All hydrogen atoms attached to carbon were included in the model at
idealized positions and refined using the riding model. A summary of the crystallographic data for
compounds 1-7 is shown in Table 1.
Hydrogen atoms could not be modeled on methanol molecules within the pores of 5 and were omitted
from the model. Similarly, it was found that the methanol molecules within the pores could not sustain
anisotropic refinement, hence they were modeled as isotropic.
Tables of interatomic distances for structures 1-7 are included as Supporting Information.
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Table 1: Crystal data and structure refinement for compounds 1-7.
Complex 1 2 3 4 5 6 7
Chemical formula
C25H41Cl3Cu10I1
4N4O6 C12H19Cu2I3N2
O2 C101H156Cl3Cu8I11
N16O40 C48H72Cu4I4N8
O8 C81H132Cu9I12K3N14O22
C24H40Cu2Cl3.4I2.6
N4O4 C30H52CuCl4N6O6
Formula Mass 3011.97 731.07 4244.99 1650.90 3837.95 1026.15 1068.84
Crystal system Triclinic Triclinic Triclinic Triclinic Trigonal Monoclinic Triclinic
Space group P1� P1� P1� P1� P-3 P21/n P1�
a/Å 10.642(2) 8.4710(17) 13.4834(13) 11.3584(13) 19.275(3) 10.9151(2) 9.1665(6)
b/Å 13.927(3) 8.8950(18) 16.9513(10) 14.054(2) 19.275(3) 11.4972(2) 10.0157(7)
c/Å 22.032(4) 12.919(3) 19.4949(12) 19.535(3) 13.123(3) 13.0904(3) 10.8275(7)
α/° 100.20(3) 107.31(3) 68.035(2) 107.967(8) 90 90 78.835(2)
β/° 90.27(3) 91.80(3) 73.558(2) 97.502(7) 90 91.945(1) 77.128(2)
γ/° 109.39(3) 96.29(3) 71.645(2) 98.108(7) 120 90 75.841(2)
Unit cell volume/Å3
3024.3(10) 921.6(3) 3852.4(4) 2886.0(7) 4222.6(12) 1625.9(2) 929.40(11)
Z 2 2 1 2 3 2 1
Temperature/K 123 123 123 123 123 123 123
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µ/mm-1 10.756 7.336 3.410 3.649 3.422 4.053 1.426
Reflections measured
51915 16250 62624 26701 88031 17255 7871
Independent reflections (Rint)
13743 (0.0350) 4581 (0.0548) 13733 (0.0470) 12328 (0.0705) 8639 (0.0776) 3767 (0.0240) 4203 (0.0127)
Obs. reflections
(I > 2σ(I))
12550 4357 10844 8549 7089 3414 3976
Final R1 (obs., all)
0.0451, 0.05183 0.0322, 0.0343 0.0671, 0.0909 0.0488, 0.0845 0.0720, 0.0813 0.0362, 0.0447 0.0236, 0.0279
Final wR2 (obs., all)
0.1235, 0.1560 0.0796, 0.0810 0.1832, 0.2119 0.1161, 0.1653 0.2372, 0.2487 0.1004, 0.1028 0.0822, 0.1035
GOF on F2 1.063 1.067 1.112 1.024 1.060 1.140 1.212
largest dif. peak/hole/e Å3
2.062/-4.057 1.012/-2.280 2.430/-3.080 1.207/-1.931 2.289/-2.175 1.784/-1.134 0.528/-0.856
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Results and Discussion
Synthesis of CuI and Cu
II Species. Two variables were initially targeted by this study to effect
changes in the ligand geometry of b3pmdc: the inclusion of a potassium cation and the lowering of pH,
each of which will influence the structure and rigidity of the azacrown group (Figure 1). The
incorporation of alkali (i.e. Figure 1a), alkaline earth and selected transition metals were recently
highlighted using a closely related ligand.2 Similarly, the basicity of the azacrown ligand in aqueous
solvent systems was found to facilitate inclusion of a water molecule upon protonation (Figure 1, (b)),
reproducibly giving an 'S' ligand geometry.20 In this work, we sought to control the degree of
protonation of b3pmdc through manipulation of solvent system and acidity. Cuprous iodide species
were generated by slow in situ diffusion of a copper source, typically [CuI(MeCN)4](ClO4), a source of
iodide (KI, NEt4I) and the ligand, b3pmdc. The diffusion gradient typically proceeded from metallic
acetonitrile or methanol, through a buffer layer (1:1 CHCl3:MeOH) containing the iodide source, to a
chloroform solution of b3pmdc. During instances where acid was added, acidification of b3pmdc was
undertaken in the chloroform layer followed by addition of the minimum quantity of methanol required
to resolve turbidity of the resultant mixture. Crystalline material suitable for single crystal X-ray
diffraction studies were found to deposit after several days in the buffer region. The yellow crystals of
1D polymer 1 were found to slowly return to solution as part of an equilibrium favoring eventual
formation of tetranuclear cluster 2. Blue crystals of cupric species 7 grew in the hours subsequent to
exposing the solution of 6 to air.
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Figure 1. Common ligand geometries observed for the azacrown ether group and relevant to b3pmdc.
Hydrogen and coordinative bonds are represented as dashed lines. Examples a, b and c are known from
prior work.2,20
Solid state structures of 1-7. Ten CuI centers were observed within the asymmetric unit of
[H4b3pmdc][Cu10I14]·CHCl3·2H2O (1) linked by fourteen iodides in a spiral conformation. Tetra-
protonated H4b3pmdc balances the charge, with the azacrown ammonium groups hydrogen bonding to
water molecules located above and below the crown ring (N-O distances of 2.827(10) Å and 2.835(11)
Å). The two water molecules are 3.104(12) Å apart and, although the hydrogen atom locations could not
be determined from the electron density map, hydrogen bonding interactions are highly probable
between the water molecules and the crown oxygens. A molecule of chloroform completes the
asymmetric unit (Figure 2). H4b3pmdc sits within the helical ridges of two polymeric [Cu10I14]∞ chains
(Figure 3). The pyridyl proton interacts very weakly with two iodide atoms in a bifurcated manner, with
observed (N)H…I distances of 3.069 Å and 2.999 Å. The majority of Cu-Cu distances within the
[Cu10I14]∞ chain range from 2.780 Å to 3.037 Å, however two contacts, Cu(1)-Cu(2): 2.5598(19) Å and
Cu(6)-Cu(7): 2.5456(19) Å, are extremely close to that of metallic copper (2.56 Å).6a The former range
relates well to other reports of cuprous chains6a and although unusual, Cu-Cu contacts of less than twice
the van der Waals radius of CuI (1.4 Å) have been observed previously in polymeric cuprous iodide
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chains.6b,c Each copper center possesses a tetrahedral CuI4 coordination environment. A helical chain of
this type, formed by face-sharing tetrahedra, has previously been termed a 'tetrahelix'.21 Two iodides
bridge in a µ4 fashion, with six each bridging in µ3 and µ2 manners completing the helical segment. The
chiral 'handedness' of the [Cu10I14]∞ chains alternates along the crystallographic c-axis, yielding an
overall racemic packing arrangement. The closest contact between the chains is an interiodide distance
(I(5)-I(5')) of ca. 4.0 Å. The addition of two equivalents of perchloric acid was essential to ensure 1
exists as the fully protonated species. Increasing the ratio of acid was found to improve the yield of 1
relative to a diprotonated species 2 (vide infra).
Figure 2. Structure of 1 showing the [Cu10I14]∞ chain, H4b3pmdc, chloroform and hydrogen bonded
water molecules. All non-acidic hydrogen atoms have been removed for clarity. Thermal ellipsoids are
shown at 50% probability.
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Figure 3. Positioning of H4b3pmdc between two [Cu10I14]∞ helical chains in 1. All non-acidic hydrogen
atoms, chloroform and water molecules have been removed for clarity.
Helix 1 was found to crystallize only in a high concentration of cuprous iodide, hence the crystals
were later found to dissolve as the metal concentration decreased due to diffusion of the Cu mixture
throughout the mixture. As a result, crystallization of a second yellow cuprous iodide species was later
observed. The structure of [Cu4I6(H2b3pmdc)] 2 is a 1D chain motif, however lack of protonation at the
pyridyl groups allows for H2b3pmdc to participate in coordination to the copper fragments, yielding a
coordination polymer (Figure 4). The [Cu4I6]2- cluster core can be viewed as the fusion of two [Cu2I3]
-
units, with the opposing half generated through an inversion center. Each copper atom retains the
tetrahedral coordination mode seen for 1, with Cu-Cu distances of 2.4574(9) Å (Cu(1)-Cu(2)) and
2.8848(14) Å (Cu(2)-Cu(2')) observed. Pyridyl groups coordinate to the cluster termini (Cu(1)-N(1):
1.988(3) Å) with four µ2 and two µ3 bridging iodides completing the cluster. The ligand adopts an 'S'
conformation with the ammonium protons oriented into the crown (Figure 1, (c)). Minimization of ionic
repulsion appears to largely govern the ligand geometry in this case. The ligand length, measured from
the pyridyl nitrogen donors, was found to be ca. 10.6 Å
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Figure 4. Coordination polymer 2 comprising alternating H2b3pmdc and [Cu4I6] units. Thermal
ellipsoids are shown at 50% probability.
Decreasing the ratio of acid to ligand resulted in monoprotonation the ligand in
[Cu4I4(Hb3pmdc)2](1.5ClO4)(0.5I3)·3.5H2O·2.5MeOH (3), which in combination with Cu4I4 cubane
nodes is incorporated into a ladder-like network. The asymmetric unit, shown in Figure 5, contains an
entire Cu4I4 cubane unit, with each copper atom exhibiting a tetrahedral coordination geometry
completed by pyridyl coordination from Hb3pmdc. Two unique Hb3pmdc ligands are present, each
protonated at a single tertiary amine within the crown and hydrogen bonding to a water molecule. The
charge on the cationic ligands is offset by a perchlorate molecule that is disordered over two positions,
and a molecule of triiodide and a second perchlorate molecule which each possess half occupancy. The
remaining void space is filled by two water molecules, one with full occupancy, one with half
occupancy, and four methanol molecules, one with full occupancy, three with half occupancy.
The overall structure resembles a 1D ladder-like net, with the sides of the ladders defined by Cu4I4
clusters bridged by one type of Hb3pmdc ligand, and the rungs provided by the second type of
Hb3pmdc ligand, which bridges the clusters in pairs to form loops (Figure 6). The Cu4I4 nodes have
Cu-Cu distances varying from 2.6129(19) Å (Cu(1)-Cu(2)) to 2.7113(19) Å (Cu(2)-Cu(3)), with an
average Cu-Cu distance of 2.65 Å. The hydrogen bonded water molecules within the azacrown impart a
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bent ligand geometry that has been observed in prior studies.2 Indeed the bridging lengths were found to
be ca. 9.2 and 10.2 Å, both of which are within the typical range for monoprotonated water-hosting
ligands of 8.9 to 10.2 Å.20 The ammonium hydrogen bond lengths were determined to be closest at
2.734(14) Å (N(2)-O(9)) and 2.689(11) Å (N(4)-O(10)), with the remaining distances observed to be
2.94(2) Å (O(9)-O(3)), 2.841(13) Å (O(9)-O(6)), 2.864(10) Å (O(10)-O(7)) and 2.822(10) Å (O(10)-
O(8)). The triiodide anion possesses a near linear geometry (175.00(14)° I(5)-I(6)-I(7)) and near
equivalent diiodide distances of 2.821(4) Å (I(5)-I(6)) and 2.873(4) Å (I(6)-I(7)).
In the absence of perchloric acid, neutral ligands were incorporated into a 1D coordination polymer of
b3pmdc, both linking and capping cubane [Cu4I4] clusters in the structure of [Cu4I4(b3pmdc)2]∞ (4,
Figure 7). One of the two b3pmdc ligands caps the cluster in an intramolecular fashion whereas the
second ligand serves to bridge between two [Cu4I4] units. The copper atoms are arrayed in a tetrahedron,
each coordinating to a single pyridyl group and three µ3 bridging iodides. The Cu-Cu distances vary
from 2.6035(15) Å (Cu(2)-Cu(3)) to 2.8101(15) Å (Cu(1)-Cu(2)) with an average distance of 2.69 Å.
The bond lengths between the pyridyl groups and copper centers range from 2.054(8) (Cu(4)-N(7)) to
2.021(7) (Cu(2)-N(4)) Å. The capping b3pmdc ligand sits over the cluster core in a fashion reminiscent
of a pair of earmuffs, culminating in a compact bridging length of ca. 6.2 Å. Despite the lack of a
templating force, be it metal inclusion, hydrogen bound water or charge repulsion, the second ligand
exhibits a bridging length of ca. 13.3 Å, more than double that of the capping ligand. This is largely a
result of the size of the [Cu4I4(b3pmdc)] moieties, necessitating the ligand being nearly fully extended
in order to bridge between these units (Figure 7, bottom).
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Figure 5. Structure of 3. The [Cu4I4] cubane unit with to two Hb3pmdc ligands coordinating. Only one
of the two possible disordered positions for the counter anions is shown. Hydrogen atoms and lattice
solvent molecules have been omitted for clarity.
Figure 6. Extended 1D ladder-like motif exhibited by 3. Hydrogen atoms, counter ions and lattice
solvent molecules have been omitted for clarity.
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Figure 7. 1D coordination polymer 4 comprising a bridging and capping b3pmdc ligand and [Cu4I4]
units. Thermal ellipsoids where shown are at 50% probability.
Replacement of tetrabutylammonium iodide with potassium iodide resulted in neutral ligands hosting
potassium cations. The resulting 3D coordination polymer contains both [Cu4I5] and [Cu5I6] cluster
units, with an overall composition of [Cu9I12(Kb3pmdc)3(H2O)4]·9MeOH (5) (Figure 8). The
asymmetric unit contains one third of the cluster core, with I(1), I(3) and Cu(1) each located on a
threefold rotation axis. Half of the b3pmdc ligand is present in the asymmetric unit, with the remainder
generated by an inversion center located at the potassium cation. The potassium cation coordinates to
both iodide and a water molecule, and three molecules of methanol were also located in the lattice. The
presence of an extra cuprous iodide, Cu(3) and I(4), constitutes the difference between the [Cu4I5] and
[Cu5I6] cluster units, and occurs such that the extra atoms show half the expected site occupancy. This
suggests a random arrangement of the two cluster types rather than an ordered arrangement which
would lead to the two clusters being crystallographically distinct. Cu(3) exhibits distorted trigonal
planar coordination with angles of 105.7(3)° (I(2)-Cu(3)-I(4)), 114.6(3)° (I(1)-Cu(3)-I(2)) and 138.4(3)°
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(I(1)-Cu(3)-I(4)) observed. In the absence of Cu(3) and I(4) the void is filled by a water molecule
coordinated to potassium.
Figure 8. Structure of 5. Only the pyridyl groups of two b3pmdc ligands coordinating to the [Cu4I5]
cluster are shown.
Each cluster is coordinated to three Kb3pmdc ligands, and each Kb3pmdc ligand in turn bridges two
clusters, leading to honeycomb-like 2D (6,3) networks (Figure 9) which possess large hexagonal
windows (diameter ca. 13 Å). The layers stack in an eclipsed fashion, leading to large channels. Each
channel is filled by solvent methanol. Two interactions fuse the layers into a 3D network: ionic
interactions between K(1) and the partially occupied I(4), and π-π interactions between the pyridyl
groups of stacked b3pmdc ligands, with an observed π-π distance of 3.88 Å (Figure 10).
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Figure 9. Packing of 5 along the crystallographic c-axis. All hydrogen atoms and methanol molecules
within the hexagonal pore have been removed for clarity.
Substituting hydrochloric acid for the perchloric acid retained the acidic environment for protonation
of b3pmdc observed with 1 and 2, but imparted a new variable in the form of halide exchange. Aside
from the obvious differences in ionic radii, chloride is also more likely to engage in significant
hydrogen bonding interactions, which may then affect the coordination motifs in the cuprous halides
regions. These effects were realized with isolation of ionic pair [Cu2Cl3.4I2.6(H4b3pmdc)] (6), which
contains a tetra-protonated b3pmdc ligand and a mixed halide CuI dimer (Figure 11). The structure
crystallizes in the P1� space group, with the asymmetric unit consisting of half of both the CuI dimer and
H4b3pmdc. The bridging halide exhibits substitutional disorder, with site occupancy factors refined as
0.3 iodide and 0.7 chloride. Hydrogen bonding to the terminal chlorides of the copper dimer occurs
from both pyridinium and tertiary ammonium groups from separate H4b3pmdc molecules. These
interactions are displayed at either terminus of the copper dimer (Figure 12). In this manner, each
H4b3pmdc hydrogen bonds to four distinct copper dimers. As each cluster also interacts with four
crown molecules, a hydrogen bonded 3D cds net22 is formed with alternating H4b3pmdc and cluster
nodes. Hydrogen bond lengths range from 3.160(5) Å (N(1)-Cl(1)) to 3.179(4) Å (N(2)-Cl(1)), however
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the strength of the pyridyl derived N(1) hydrogen bond is likely less, owing to the more angled
directionality (ca. 138°) relative to the tertiary ammonium N(2) derivative (ca. 154°).
Figure 10. Inter-sheet interactions in 5. Only the pyridyl groups of two b3pmdc ligands coordinating to
the [Cu4I5] cluster are shown. Each pyridyl group undergoes offset π-π stacking with neighboring
b3pmdc ligands. Ionic interactions between K(1) and I(4) occur where copper is present.
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Figure 11. Solid-state structure of ionic pair 6 which comprises [H4b3pmdc][Cu2Cl2I2X2] (X = 0.3 I,
0.7 Cl). All non-acidic hydrogen atoms have been removed for clarity.
Figure 12. Hydrogen bonding network observed between a copper dimer of 6 and four separate
H4b3pmdc molecules, which, in turn, are hydrogen bonded to four copper dimers.
After isolation of 6, prolonged exposure of the filtrate to air resulted in dioxygen mediated oxidation
of the remaining CuI to CuII, generating blue crystals of [CuCl2(H2b3pmdc)(MeOH)2]·2Cl·2MeCN (7)
after only twelve hours. The cupric metal center is located on an inversion center and has an octahedral
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conformation, with two methanol molecules present in Jahn-Teller distorted axial positions and para
arrangement of the chloride and pyridyl groups in the equatorial positions (Figure 13). Both of the
coordinated methanol molecules hydrogen bond to a second chloride anion, with protonation of
H2b3pmdc providing an additional hydrogen bond interaction (Figure 13, bottom) and charge
balancing. Hydrogen bond distances of 3.1262(13) Å (O(3)-Cl(2)) and 3.1059(14) (N(2)-Cl(2)) were
observed, suggesting near equivalent interactions between both donor atoms. The three bond lengths
about the copper atom are 2.0167(13) Å (Cu(1)-N(1)), 2.3186(4) Å (Cu(1)-Cl(1)) and 2.5015(13) Å
(Cu(1)-O(3)), each duplicated by symmetry to give the six coordinate geometry. The overall length of
H2b3pmdc was found to be ca. 12.5 Å. The overall structure is 1D polymeric in nature, with H2b3pmdc
covalently linking cupric chloride units. Non-covalent hydrogen bond interactions between ammonium
chloride and coordinated methanol molecules strengthen the chain (Figure 13, bottom). Small lattice
voids are filled by molecules of acetonitrile.
Figure 13. 1D coordination polymer 7 comprises alternating H2b3pmdc and [CuCl2] units. Further
chlorides are hydrogen bonded by coordinated methanol and the tertiary ammonium proton. Thermal
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ellipsoids are shown at 50% probability. One molecule of acetonitrile is also present within the lattice
(not shown).
While attempts were made to oxidize the reaction mixtures containing compounds 1-5 in a similar
manner as yielded crystalline 7, ultimately these efforts proved unsuccessful. Typically precipitates with
low solubility in common organic solvents were isolated and not analyzed further.
Luminescence study of 2 and 4. Previous studies have shown that cuprous iodide species
coordinated by pyridyl groups may exhibit photoluminescence, emitting blue, green or orange light
depending on the motif.5e,23 Clusters 2 and 4 were investigated for photoluminescent behavior, with both
found to emit room temperature, solid-state photoluminescence (Figure 14). Both had comparable
excitation wavelength maxima (338 nm for 2, 342 nm for 4). A second less intense maximum was
observed at ca. 370 nm, which is consistent with previously reported double absorption profiles of other
tetrahedral CuI systems.5a,23 The emission profile of 2 displayed a maximum at λ = 502 nm, giving blue-
green photoluminescence. The emission was observed to tail to ca. 700 nm. By contrast, the emission
spectrum of 4 showed considerable red-shifting relative to 2, with a maximum at λ = 553 nm, imparting
a yellow-green hue. The emission profile also was found to terminate at 720 nm. The cause of
photoluminescent emission in cuprous iodide species is thought to be related to a triplet centered (3CC)
excited state as a result of halide to metal charge transfer and d-s transitions.5a No luminescence
behavior was evident for network 3.
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Figure 14. Photoluminescence profiles for 2 (dashed excitation, green emission traces) and 4 (solid
excitation, orange emission traces).
The replacement of the apical coordinating pyridyl group with an iodide in 5 results in the absence of
photo luminescent behavior, possibly due to the presence of potassium-coordinated water adjacent to the
cuprous clusters. Water derived O-H oscillators are renowned for their ability to quench metal-based
luminescent emission.24 This explanation also explains the lack of luminescent behavior observed for
network 3.
Gas adsorption and thermogravimetric analysis. The structure was analyzed for gas adsorption
characteristics which, disappointingly, were found to be lacking. This evaluation included trialing a
range of activation protocols, including use of supercritical CO2. Thermogravimetric analysis suggested
5 should exhibit thermal stability to a temperature of ca. 200 °C (see Supporting Information).
Consequently we postulate that the single ionic link (Cu(3)-I(4)-K(1)) per every two cluster units offers
insufficient stabilization to the open channel motif upon desolvation. Indeed instability of the cluster
core was evidenced by the observation of sublimed iodine in the experimental apparatus after heating
the sample at 80 °C.
Ligand conformational analysis. A comparison of the various coordination geometries observed for
b3pmdc within this study found that the tetra-protonated ligand adopts an 'S' confirmation within a
narrow range of distances (ca. 10.3 to 10.6 Å (1, 6)) between the pyridyl nitrogens across the ligand.
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Protonation of only the tertiary amine groups of b3pmdc left the pyridyl groups free to participate in
metal coordination, yet retention of the 'S' conformation was still seen. Comparable overall ligand
lengths resulted, provided the ammonium protons were directed into the aza-ring (2, ca. 10.6 Å).
Outward orientation (i.e. Figure 1, (d)) yielded a longer ligand length of ca. 12.5 Å, likely influenced by
the reorientations necessary for hydrogen bonding to chloride in 7. Singular protonation of the
azacrown, resulting in hydrogen bonding of a guest water molecule, yielded two ligand bridging lengths
in structure 3: ca. 9.2 and 10.2 Å. These lengths, as well as the observed bent ligand geometry, are
typical of ligands that exhibit this behaviour.20 The neutral ligands in 4 were found to have the
conformational freedom to adopt either short (6.2 Å) or long (13.3 Å) coordination lengths, as well as
both crescent and elongated trans-pyridyl conformations. The longest observed ligand length was
induced by potassium incorporation in 5 (ca. 14.6 Å) as a result of the alkali metal forcing the azacrown
functionality into a planar, trans-pyridyl conformation, consistent with previous studies.2
In conclusion, we have observed a range of conformations for the bridging b3pmdc ligand, induced
by incorporation of water molecules, potassium ions or variation of reaction pH. Both cuprous and
cupric halide architectures have been utilized as a means of promoting these variations in ligand
geometry. Six separate architectures containing b3pmdc were synthesized and isolated, including a 3D
network containing large solvent filled channels, a racemic mixture of chiral 1D cuprous iodide chains
and two photoluminescent 1D cuprous iodide cluster chains.
ASSOCIATED CONTENT
SUPPORTING INFORMATION
Crystallographic data in CIF format. Further crystallographic details are given in Tables S1 to S6.
Thermogravimetric analytical trace of 5 is given in Figure S1. This material is available free of charge
via the Internet at http://pubs.acs.org.
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AUTHOR INFORMATION
Corresponding Author
* Email: [email protected]
ACKNOWLEDGMENTS
The authors gratefully acknowledge the Australian Research Council, Monash University for financial
support. This research was, in part, undertaken on the macromolecular crystallography (MX1 and MX2)
beamlines at the Australian Synchrotron, Victoria, Australia. The authors acknowledge Dr. Matthew
Hill for determining the gas adsorption characteristics of compound 5.
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SYNOPSIS TOC
The conformational variability of a diaza-18-crown-6 ligand has been restricted by variations to
pH and guest molecules within the scope of cuprous halide chemistry.
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Crystal Growth & Design
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ACS Paragon Plus Environment
Crystal Growth & Design
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ACS Paragon Plus Environment
Crystal Growth & Design
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ACS Paragon Plus Environment
Crystal Growth & Design
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97x94mm (300 x 300 DPI)
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ACS Paragon Plus Environment
Crystal Growth & Design
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49x24mm (300 x 300 DPI)
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ACS Paragon Plus Environment
Crystal Growth & Design
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754x277mm (96 x 96 DPI)
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ACS Paragon Plus Environment
Crystal Growth & Design
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