Stabilization of O–Mn–O clusters (Mn5) in three dimensionally extendedMOF structures: synthesis, structure and properties{
Saurav Bhattacharya,a K. V. Ramanujachary,c S. E. Lofland,d Travis Magdalenoc and Srinivasan Natarajan*ab
Received 18th October 2011, Accepted 10th April 2012
DOI: 10.1039/c2ce06386g
Four new three-dimensional Mn2+ ion-containing compounds have been prepared by employing a
hydrothermal reaction between Mn(CH3COO)2?4H2O, sulfodibenzoic acid (H2SDBA), imidazole,
alkali hydroxide and water at 220 uC for 1 day. The compounds have Mn5 (1–4) clusters connected by
SDBA, forming the three-dimensional structure. A time and temperature dependent study on the
synthesis mixture revealed the formation of a one-dimensional compound, Mn(SDBA)(H2O)2, at
lower temperatures (T ¡ 180 uC). The stabilization of the fcu related topology in the compounds is
noteworthy. Magnetic studies indicate strong anti-ferromagnetic interactions between the Mn2+ ions
within the clusters in the temperature range 75–300 K. The rare participation of a sulfonyl group in
the bonding is important and can pave way for the design of new structures.
Introduction
Metal organic framework compounds (inorganic coordination
polymers) provide new pathways for exploring the formation of
–M–O–M– clusters and networks.1 Isolated –M–O–M– clusters
were investigated with great interest for their unique physical
properties, especially their single molecule magnetism.2 Of these
molecules, those containing manganese are important and were
studied extensively during the last two decades.3 The synthesis of
isolated Mn clusters and their derivatives was achieved by
carefully controlling the experimental parameters.3
The formation of extended –M–O–M– networks within MOFs
appears to be facilitated, in general, by higher reaction
temperatures.4 Simple –M–O–M– clusters, however, can be
stabilized as part of a MOF structure at lower temperatures as
well.5 Ferey and coworkers have isolated and extensively
investigated M3 (M = Fe, Cr, Al etc) clusters stabilized as part
of a MOF structure.6 In addition to exhibiting interesting
magnetic properties, the observation of breathing-like behavior
in these compounds is noteworthy.7
From the available literature, it is clear that nitrogen-
containing ligands help the formation of –M–X–M– (X = O,
N) clusters.8 Pyridine and bipyridine-based dicarboxylic acids
have been employed to stabilize new types of metal–oxygen/
nitrogen clusters within MOFs.8 Of the many dicarboxylic acids
employed in the literature, terephthalic acid appears to be the
most dominant.9 A variant of terephthalic acid is 4,49-oxybis-
benzoic acid, OBA, (HOOC–(C6H4)–O–(C6H4)–COOH), the use
of which has resulted in many interesting compounds.10
We propose that the closely related acid, viz-sulfonyldibenzoic
acid, H2SDBA, (HOOC–(C6H4)–SO2–(C6H4)–COOH), could
also give rise to a variety of new compounds with novel
structures. To this end, we have reacted a mixture of a Mn-salt,
H2SDBA and imidazole along with a number of alkali
hydroxides (Na+, K+, Cs+ and NH4+) under hydrothermal
conditions. Our efforts were successful and we have isolated four
three-dimensional framework compounds possessing Mn5 clus-
ters as part of the framework, [Mn5(C14H8O6S)4(C14H9O6S)2]?
4.5H2O, 1, [Mn5K2(H2O)2(C14H8O6S)6], 2, [Mn5Cs2(C14H8O6S)6],
3 and [Mn5(NH4)2(C14H8O6S)6]?2H2O, 4. In this paper, the
synthesis, structure and properties of these compounds are
described and discussed.
Experimental
Synthesis
The chemicals, Mn(CH3COO)2?4H2O, 4,49-sulfonyldibenzoic
acid (H2SDBA) and CsOH were obtained from Sigma Aldrich
(Germany) and imidazole, NaOH, KOH and NH4OH were
obtained from Merck (India) and were used as received. All the
compounds were prepared via a hydrothermal method. In a
typical synthesis for [Mn5(C14H8O6S)4(C14H9O6S)2]?4.5H2O, 1,
Mn(CH3COO)2?4H2O (0.245 g, 1 mmol), H2SDBA (0.306 g,
aFramework Solids Laboratory, Solid State and Structural ChemistryUnit, Indian Institute of Science, Bangalore, 560012, IndiabDivision of Advanced Materials Science, Pohang University of Scienceand Technology (POSTECH), San 31, Hyoja-Dong, Pohang, 790-784,South Korea. E-mail: [email protected] of chemistry and Biochemistry, University, 201 Mullica HillRoad, Glassboro, New Jersey 08028, USAdDepartment of Physics and Astronomy, Rowan University, 201 MullicaHill Road, Glassboro, New Jersey 08028, USA{ Electronic supplementary information (ESI) available: Tables forselected bond distances, bond angles, hydrogen bonds, magnetic data,IR spectra, PXRD patterns, additional figures for structural description,TGA, UV, PL and magnetic plots of the compounds. CCDC referencenumbers 834723–834725, 864134. For ESI and crystallographic data inCIF or other electronic format see DOI: 10.1039/c2ce06386g
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1 mmol), imidazole (0.068 g, 1 mmol) and NaOH (0.080 g,
2 mmol) were mixed in 10 mL of water. The mixture was
homogenized for 30 min at room temperature, transferred into a
23 mL PTFE lined stainless steel autoclave, sealed and heated at
220 uC for 1 day under autogenous pressure. The final product
contained large quantities of colorless block-shaped crystals,
which were filtered under vacuum, washed with deionized water
and dried under ambient conditions. Similar synthesis proce-
dures were employed for the preparation of compounds 2–4
(Table 1).
Time and temperature variation investigations
The same reaction mixture with the composition
Mn(CH3COO)2?4H2O (1 mmol), H2SDBA (1 mmol), imidazole
(1 mmol) and NaOH/KOH/CsOH/NH4OH (2 mmol) in 10 mL
of water was reacted in a 23 mL Teflon lined stainless steel
autoclave at 75, 110, 150, 180, 200, 220 uC for varying periods of
time (typically 1–3 days). The products in each case were
separated by the usual methods of filtration, dried at ambient
conditions and subjected to PXRD analysis.
Characterizations
Initial characterizations were carried out by elemental analysis,
powder X-ray diffraction (PXRD), thermogravimetric analysis
(TGA), IR and UV-Vis spectroscopic studies. Elemental analysis
(C, H, N) was recorded in a Thermo Finnigan EA Flash 1112
Series. Powder X-ray diffraction patterns were recorded in the 2h
range of 5–50u using Cu–Ka radiation (Philips X’pert Pro). The
observed PXRD patterns were new and the patterns entirely
consistent with the simulated XRD patterns generated, based on
the structures determined using single crystal XRD (Fig. S1,
ESI{). Simulated XRD patterns of all the compounds were
generated using Mercury software (version 1.4.1). The PXRD
studies also revealed that the microcrystalline powders obtained
during the synthesis also belonged to the respective compounds.
IR spectra of all the compounds were recorded on KBr pellets
(PERKIN ELMER SPECTRUM 1000). IR spectra for all the
compounds gave sharp characteristic bands (Fig. S2, ESI{). The
presence of a peak at y3227 and 3099 cm21 in 4 suggests the
presence of symmetric and asymmetric stretching frequencies
from the ammonium ion (Table S1, ESI{).11
The thermal stability of the prepared compounds was
investigated using thermogravimetric analysis (TGA). The
studies were carried out on all the samples (1–4) in flowing air
(flow rate = 20 ml min21) in the temperature range of 30–850 uCusing a heating rate of 5 uC min21 (Fig. S3, ESI{). Details of the
TGA analysis have been tabulated (Table S2, ESI{) and the
PXRD patterns of the final products are given in Figure S4
(ESI{). The general trend appears to be consistent for all
compounds, although the individual compounds exhibit subtle
differences which depend on the amount of water molecules
present within the structure. All the compounds appear to be
stable up to 350 uC. The final product contained Mn2O3
(JCPDS: 89-4836) and MnS0.4O2.6 (JCPDS: 21-0557), along
with K3(MnO4)(MnO4) (JCPDS:79-2320) for 2 and Cs2O3
(JCPDS: 65-3154) for 3 and several other unidentifiable peaks,
as seen in the PXRD spectra (Fig. S4, ESI{).
The diffuse reflectance UV-Vis spectra was recorded at room
temperature for the Na2SDBA anion and for the as-synthesized
compounds using a UV-Vis spectrophotometer (Perkin Elmer
Lambda 35, USA). Room temperature solid state photolumines-
cence studies were carried out on the powdered samples of
Na2SDBA and compounds 1–4 using a luminescence spectro-
photometer (Perkin Elmer LS 55, USA).
To probe the magnetic behavior of the present compounds, we
carried out magnetic studies in the temperature range of 5–300 K
using a SQUID magnetometer (Quantum Design Inc., USA).
The presence of Mn5 clusters in the present compounds suggest a
possibility of interesting magnetic behavior. Single molecule
magnets based on Mn clusters have been investigated and
modeled extensively.3 The studies on extended structures
containing manganese clusters have been quite limited thus far,
as it is difficult to understand the various exchange pathways and
the interactions between the Mn clusters.
Single crystal structure determination
A suitable single crystal of each compound was carefully selected
under a polarizing microscope and glued to a glass fiber. The
data from the single crystals of the compounds were collected on
a Bruker AXS smart Apex CCD diffractometer at 120(2) K for
compound 1 and 293(2) K for compounds 2–4. The X-ray
generator was operated at 50 kV and 35 mA using Mo–Ka (l =
0.71073 A) radiation. Data was collected with a v scan width of
0.3u. A total of 606 frames were collected at three different
settings for Q (0, 90, 180u) whilst keeping the sample-to-detector
distance fixed at 6.03 cm and the detector position (2h) fixed at
225u. The data was reduced using SAINTPLUS12 and an
empirical absorption correction was applied using the SADABS
program.13 The structure was solved and refined using
Table 1 Synthesis composition and conditions employed for compounds 1–4
S no. Composition T/uC Time (h) Product Yield (%)a
1 Mn(CH3COO)2?4H2O + H2SDBA + imidazole+ 2.0 NaOH + 556?0H2O
220 24 [Mn5(C14H8O6S)4(C14H9O6S)2]?4.5H2O, 1 60
2 Mn(CH3COO)2?4H2O + H2SDBA + imidazole+ 2.0 KOH + 556?0H2O
220 24 [Mn5K2(H2O)2(C14H8O6S)6], 2 50
3 Mn(CH3COO)2?4H2O + H2SDBA + imidazole+ 2.0 CsOH + 556?0H2O
220 24 [Mn5Cs2(C14H8O6S)6], 3 75
4 Mn(CH3COO)2?4H2O + H2SDBA + imidazole+ 2.0 NH4OH + 556?0H2O
220 24 [Mn5(NH4)2(C14H8O6S)6]?2H2O, 4 60
a Yields are calculated based on the respective metals. Compositions given are molar compositions.CHN analysis for 1: Calc(%) C 46.2; H 2.6; N0.0; Found(%) : C 45.8; H 2.4; N 0.0 ; for 2: Calc(%) C 45.6; H 2.3; N 0.0; Found(%): C46; H 2.1; N 0.0; for 3: Calc(%) C 42.6; H 2.02; N 0.0;Found(%): C 43.1; H 1.9; N 0.0; for 4: Calc(%) C 46.6; H 2.70; N 1.3; Found: C 47.3; H 2.15; N 1.2.
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SHELXL97,14 present in the WinGx suit of programs (Version
1.63.04a).15 All non-hydrogen positions were initially located in
the difference Fourier maps and for the final refinement, the
hydrogen atoms were placed in geometrically ideal positions and
refined in the riding mode. Restraints for the bond distances
were used during the refinement to keep the hydrogen atoms
bonded to the protonated carboxylate oxygen and the nitrogen
in the ammonium ion in compounds 1 and 4, respectively. DFIX
and DANG restraints were used to fix the hydrogens onto the
nitrogen atom in 4 in order to model the ammonium ion
properly. Final refinements included atomic positions of all the
atoms, anisotropic thermal parameters for all the non-hydrogen
atoms and isotropic thermal parameters for all the hydrogen
atoms. One of the water molecules, O(21), in compound 1 was
found to be disordered and hence only the isotropic refinement
was carried out. A full-matrix least squares refinement against
|F2| was carried out using the WinGx package of programs.15
Details of the structural parameters and final refinements for the
compounds are presented in Table 2. Crystallographic data for
compounds 1–4 (CCDC No. 864134 for 1 and 834723–834725
for 2–4) are available in the ESI.{
Results and discussion
Structure of [Mn5(C14H8O6S)4(C14H9O6S)2]?4.5H2O, 1
The asymmetric unit of 1 consists of 69 non-hydrogen atoms.
For the purpose of describing the structure, the acid is
designated as H2SDBA, the partially deprotonated acid as
HSDBA and the fully deprotonated acid as SDBA. This
nomenclature will be employed hereafter in the manuscript.
There are three Mn2+ ions, which are crystallographically
independent with Mn(1) occupying a special position (1h) with
a site multiplicity of 0.5 and thus lying on an inversion center,
along with two SDBA anions, one HSDBA anion and three
water molecules. Of the three Mn2+ ions, Mn(1) has a distorted
octahedral geometry while Mn(2) and Mn(3) have a distorted
square pyramidal geometry formed by the carboxylate oxygens
(Fig. S5, ESI{). The Mn–O bond distances are in the range
2.051(2)–2.249(2) A while the O–Mn–O bond angles are in the
range 75.83(7)–180.00u. The selected bond distances and bond
angles are listed in the ESI (Table S3 and S4).{ The close
proximity of the lattice water molecules, O(19), to the
carboxylate oxygen, O(12), gives rise to a O–H…O hydrogen
bond interaction. The O…O distance is 3.092(4) A and the
O–H…O bond angle is 164u, which suggests that the hydrogen
bond interaction is medium to strong (Table S5, ESI{).16
The structure of 1 has two types of SDBA anion connectivities:
one in which the HSDBA anion bonds with the three metal centers
via a monodentate and bidentate chelating mode and the other in
which the SDBA anions are bonded via a bidentate and tridentate
mode (Fig. 1a). The formation of the pentameric clusters can be
understood by considering the connectivity between the Mn
centers. Mn(2) and Mn(3) form a paddlewheel arrangement while
the Mn(1) octahedra connects the paddlewheel through the three
coordinate oxygen atoms, O(2) and O(3), forming the trimer. As
Mn(1) occupies a special position, the other paddlewheel is
generated automatically by the symmetry, giving rise to the
pentamer (Fig. 2a). Thus, two paddlewheel units (Mn(2) and
Mn(3)) are joined at the edges by the Mn(1) octahedra (Fig. 2a).
The Mn5 cluster units are connected through the carboxylate
bridges, giving rise to the three-dimensional structure (Fig. 2b and
2c). The lattice water molecules occupy spaces between the clusters
and form hydrogen bond interactions, giving rise to one-
dimensional units (Fig. 2b). The protonated carboxylate oxygen,
O(12), participates in the hydrogen bond interactions involving
the lattice water molecules to bridge the pentanuclear units.
Structures of [Mn5K2(H2O)2(C14H8O6S)6], 2,
[Mn5Cs2(C14H8O6S)6], 3 and [Mn5(NH4)2(C14H8O6S)6]?2H2O, 4
The structures of 2, 3 and 4 are similar where the alkali metal
ions were also found to be part of the network. There are 68
Table 2 Crystal data and structure refinement parameters for compounds 1–4
1 2 3 4
Empirical formula C84H59S6O40.5Mn5 C84H52S6O38K2Mn5 C84H48S6O36Cs2Mn5 C84H60 N2S6O38Mn5
Formula weight 2183.30 2214.48 2366.10 2172.37Crystal system Triclinic Triclinic Triclinic TriclinicSpace group P1 (no.2) P1 (no.2) P1 (no.2) P1 (no.2)a/A 12.700(5) 12.7407(3) 12.5500(6) 12.7609(6)b/A 12.714(5) 12.7787(3) 12.9301(6) 12.7682(6)c/A 15.990(5) 15.9960(4) 16.1279(7) 16.0315(7)a (u) 72.773(5) 86.701(2) 106.080(4) 87.646(4)b (u) 88.047(5) 72.142(2) 93.353(4) 72.508(4)c (u) 60.583(5) 60.438(3) 118.627(5) 60.477(5)Volume/A3 2128.8(14) 2142.27(9) 2149.86(17) 2149.71(17)Z 1 1 1 1T/K 120(2) 293(2) 293(2) 293(2)rcalcd (g cm23) 1.696 1.714 1.828 1.675m/mm21 0.968 1.056 1.787 0.957Wavelength (A) 0.71073 0.71073 0.71073 0.71073h range (deg) 1.35 to 27.63 2.40 to 26.00 2.44 to 26.00 2.42 to 26.00R index [I . 2s(I)] R1 = 0.0416 R1 = 0.0334 R1 = 0.0576 R1 = 0.0425
wR2 = 0.0948 wR2 = 0.0859 wR2 = 0.1334 wR2 = 0.0845R (all data) R1 = 0.0611 R1 = 0.0462 R1 = 0.0930 R1 = 0.0675
wR2 = 0.1036 wR2 = 0.0919 wR2 = 0.1469 wR2 = 0.0971
R1 = S|| Fo | 2 | Fc ||/S | Fo |; wR2 = {S [w (Fo2 2 Fc
2)]/S [w (Fo2) 2]}1/2. w = 1/[r2(Fo)2 + (aP)2 + bP]. P = [max (Fo, O) + 2(Fc)
22]/3, where a =0.0384 and b = 3.6886 for 1, a = 0.0419 and b = 0.6507 for 2, a = 0.0529 and b = 1.4829 for 3, and a = 0.030 and b = 0.0000 for 4.
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Fig. 1 The various connectivities of the SDBA molecule observed in compounds (a) 1, (b) 2, (c) 3, (d) 4.
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Fig. 2 (a) The Mn5 pentamer in compound 1. (b) The bridging of the Mn5 pentamers by hydrogen bonded lattice water molecules and protonated
carboxylates. (c) The overall three-dimensional structure of 1.
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non-hydrogen atoms in the asymmetric unit of 2, 67 in 3 and 68
in 4. There are three Mn2+ ions which are crystallographically
independent, with Mn(1) occupying a special position (1c for 2
and 3 and 1h for 4) with a site multiplicity of 0.5 as it lies on an
inversion center, along with three SDBA anions and one
potassium ion for 2, a cesium ion for 3 and an ammonium ion
for 4 as well as water molecules in 2 and 4 (Fig. S6–S8, ESI{). Of
the three Mn+2 ions, Mn(1) has a distorted octahedral geometry,
while Mn(2) and Mn(3) have distorted square pyramidal
geometries formed by the carboxylate oxygens. The potassium
atom in 2 has a distorted octahedral geometry formed by the
carboxylate and sulfonyl oxygen atoms and it also possesses a
coordinated water molecule, O(19) (Fig. S6, ESI{). The cesium
atom in 3 on the other hand, has a distorted seven coordinate
geometry formed from the carboxylate and sulfonyl oxygen
atoms (Fig. S7, ESI{). The ammonium ion in 4 forms N–H…O
type hydrogen bond interactions with N…O distances ranging
from 2.799(5)–3.134(6) A and N–H…O bond angles ranging
from 146–167u (Fig. S8, Table S5, ESI{ ).
Here, as a representative structure, we present the structure of
the potassium-containing compound (2) in detail. There are three
types of SDBA anion connectivity observed in 2. The first acid
has one of the carboxylate groups coordinated to two Mn2+ ions
in a chelating fashion while the other carboxylate unit is bonded
to two K+ and one Mn+2 ions, with the sulfonyl group bonded to
one K+ ion. The second acid has the carboxylate group bonded
with two Mn2+ ions in a chelating fashion, the other carboxylate
group bonded with three Mn+2 ions and the sulfonyl group
bonded to one K+ ion. The third acid has one of the carboxylates
bonded with two Mn+2 and one K+ ions and the other
carboxylate bonded with three Mn2+ ions while the sulfonyl
group remains uncoordinated (Fig. 1b). It is interesting to note
that the sulfonyl unit, which connects the two benzoic acid
groups, participates in bonding. The polydentate bonding
behavior of the carboxylate groups observed in the present
compounds 1–4 (Fig. 1b), have been observed previously.17
The connectivity between the Mn2+ ions and the carboxylate
groups lead to the formation of Mn5 pentameric clusters
(Fig. 3a). Similar to the structure of 1, the pentameric cluster
contains paddlewheel arrangements connected by the Mn(1)
octahedra. Thus, Mn(2) and Mn(3) form the paddlewheel
arrangement which are connected by the Mn(1) octahedra
through the two three-coordinated oxygen atoms (Fig. 3a).
The role of the K+ ion in the structure is important as it bridges
the pentanuclear units to form a one dimensional unit. The K+
ions are connected through the carboxylate and sulfonyl
oxygens, forming an eight membered ring which links the Mn5
pentamer units (Fig. 3b). As can be seen, the K+ ions occupy the
spaces occupied by the water molecules in the structure of 1. The
one dimensional –Mn5–K2–Mn5– chains are crosslinked by the
carboxylate units, forming the observed three-dimensional
structure (Fig. 3c).
The pentamer cluster units can be considered as nodes, similar
to the structure of 1, in the consideration of the network with
SDBA and the M+ ion dimers (M = K, Cs, NH4] as linkers. A
TOPOS analysis18a,b would then give a uninodal 12 connected
net with an fcu (cubic closed packing) topology, with the Schlafli
symbol [324.436.56]18c (Fig. 3d), while having 3, 4 and 5-mem-
bered circuits originating from the node. The superscripts in the
Schlafli symbol denote the number of such circuits originating
from a particular node.18d The distances between the Mn5
clusters (inter-cluster) range from 12.74(1)–17.12(2) A in 2,
12.55(1)–17.66(4) A in 3 and 12.77(1)–17.78(1) A in 4 (center of
the cluster to the neighbor). MOFs with an fcu topology from
cluster-ligand connectivity have been previously observed.19 For
example, in the case of the [Cu3(pdt)2(CN)] compound,19b if we
consider the Cu6S4 cluster as the node and eight pyridinethiolate
and four cyanide groups as the linkers, one could observe the
emergence of a fcu topology (Fig. 4). Mn5 clusters are not
uncommon and have been observed before. The connectivity
differences between the clusters give rise to unique topologies. In
the present structures, a fcu topology has been observed whereas
bct, hxl and bcu topologies have been observed previously.
Table 3 summarizes the different topologies observed within the
Mn5 clusters.
Four three-dimensional compounds have been prepared by the
use of different alkali metals. All the compounds have similar
Mn5 building units, connected by the acid and alkali metal ions,
forming the observed three-dimensional structure. The present
study suggests that the larger alkali metal ions are incorporated
as part of the structure, though the exact role played by the alkali
metal ions is not clear. It is likely that the subtle differences in the
basic nature of the different alkali ions might have played a role
in the outcome of the structures.
Time and temperature dependent studies on the synthesis
The role of time and temperature in the preparation of MOFs
has not been investigated in great detail in previous studies. Our
earlier studies on the role of time and temperature in
the formation of MOFs clearly points out the formation of
–M–O–M– extended networks or clusters either at higher
temperature or by prolonged heating at a relatively lower
temperature.4d The present series of compounds have been
prepared by heating the reaction mixture at 220 uC for 1 day,
which resulted in the formation of Mn5 clusters bonded through
the ligands. It occurred to us that a greater insight on the
formation of the phases could be obtained by exploring the
formation, using the same reaction mixture, at lower tempera-
tures as well as by varying the periods of time. A study of this
nature might provide valuable clues towards the formation of
other related phases. This is a labour intensive experiment and
the products in most cases were powder samples admixed with
single crystals. The single crystals were analyzed using single
crystal XRD. The powder and the single crystals were crushed
and analyzed using PXRD (Fig. S9–S12, ESI{).
From the PXRD patterns, the following observations can be
made. In all cases, a one dimensional solid, Mn(SDBA)(H2O)2,
was the only product, especially at lower temperatures (Fig. S13,
ESI{). The single crystal structure of the 1D compound was
already known21a and a careful study of the PXRD patterns
indicated that the 1D compound is generally stable up to 180 uC,
using the synthesis composition for the preparation of 1. A small
transient unidentifiable impurity phase was observed at 110 uCafter 2 days (Fig. S13a, ESI{). In spite of our best efforts, we
could not isolate suitable single crystals necessary for identifying
this unknown phase. The 3D compound (1) was the only phase
isolated at higher temperatures as well as at longer durations
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(200–220 uC) (Fig. S13a, ESI{). In the case of compound 2, the
reaction mixture yielded only the 1D21a and 3D (2) phase. We
did not observe the formation of any additional phase, though a
mixture of the 1D and 3D phases was observed at 180 uC at 1
and 2 days during the reaction (Fig. S13b, ESI{). In the case of
compound 3, we observed the formation of the 3D phase even at
75 uC after 3 days (Fig. S13c, ESI{). In addition, at 180 uC a new
unidentified product was observed. The formation of the 3D
phase (3) after prolonged heating (3 days) suggests that it could
be thermodynamically more stable. In the case of compound 4,
again, we observed only two compounds (the 1D and 3D phases)
(Fig. S13d, ESI{). A mixture of the 1D and 3D (4) phases was
observed at 150 uC after 2 and 3 days (Fig. S13d, ESI{).
During the present study, we have observed the formation of two
distinct unidentifiable phases in addition to isolating the reported
1D21a and 3D compounds (1–4). Such observations have been
made before.4a,b Although it is difficult to predict the formation of
phases under hydrothermal conditions, the repetitive formation of
two distinct phases (1D and 3D) as a function of time and
temperature suggests that, for the composition employed, they
could be the stable phases. It is likely that one could observe other
phases by varying the composition and performing further
reactions as a function of temperature and time. Such studies have
led to the formation of interesting new structures.5b
Earlier studies on the effect of time and temperature indicated
the facile formation of –M–O–M– linkages and clusters at higher
synthesis temperatures.10a The formation of –Mn–O–Mn–
clusters at 220 uC suggests that one could observe extended
–Mn–O–Mn– connectivities at even higher reaction temperatures
(T . 220 uC). Similar observations have been made previously
during the synthesis of MOFs.10a We have reacted the 1D Mn
compound, Mn(SDBA)(H2O)2, under hydrothermal conditions
at 220 uC to observe whether the 1D compound undergoes
any transformation to the 3D phase reported here. The
1D compound, however, decomposes under these reaction
Fig. 3 (a) The Mn5 pentamers in compounds 2–4. (b) The one
dimensional chains formed from the connectivity between the Mn5
clusters and the potassium dimers in 2. Similar chains are observed in
compounds 3–4. (c) The overall three dimensional structure formed from
the connectivity between the Mn5 clusters, SDBA and the potassium
dimers in 2. The green polyhedra represent the 12 connected cluster node
while the cyan spheres represent the potassium ions. (d) The connectivity
of the clusters leading to a fcu topology in compounds 2–4, compound 2
taken as a model. The purple spheres represent the Mn5 clusters while the
green spheres represent the potassium ion dimers in 2, cesium ion dimers
in 3 and ammonium ion dimers in 4.
Fig. 4 The fcu topology observed in [Cu3(pdt)2(CN)].19b The net
topology was arrived at by considering the Cu6S4 cluster as the node
and the pyridinethiolate groups and the cyano groups as the linkers. Each
red sphere indicates the 12 connected node.
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Ta
ble
3C
om
pari
son
of
the
Mn
5cl
ust
ers
rep
ort
edin
the
lite
ratu
rew
ith
the
pre
sen
tco
mp
ou
nd
s1–4
Co
mp
ou
nd
sC
lust
erU
nit
Co
nn
ecti
vit
yw
ith
inth
eM
n5
clu
ster
un
itL
ink
ers
an
dto
po
log
y(u
sin
gM
n5
clu
ster
as
no
de)
Illu
stra
tio
ns
(Mn
5cl
ust
era
nd
Fra
mew
ork
top
olo
gy
)
Co
mp
ou
nd
s1–4
[Mn
5(m
3-C
OO
) 4-
(m-C
OO
) 6]
Dis
tort
edsq
ua
rep
yra
mid
al
Mn
are
edg
eco
nn
ecte
dw
ith
oct
ah
edra
lM
nfo
rmin
ga
trim
erco
nn
ecte
dfu
rth
erb
yca
rbo
xy
late
ox
yg
ens
wit
htw
oo
ther
squ
are
py
ram
ida
lM
n.
SD
BA
an
dh
yd
rog
enb
on
ded
wa
ter
(1)
or
alk
ali
ion
dim
ers
(2–4)
con
nec
tsth
eM
n5
clu
ster
no
des
form
ing
a1
2co
nn
ecte
dn
etw
ith
fcu
top
olo
gy
.
[Mn
5(H
trz)
2-
(SO
4) 4
(OH
) 2]2
0a
[Mn
5(m
3-O
H) 2
(m-
SO
4) 4
(m2-H
trz)
2]
Oct
ah
edra
lm
an
gan
ese
con
nec
ted
thro
ugh
the
edg
esS
ulf
ate
con
nec
tsth
eM
n5
clu
ster
no
des
form
ing
a1
0co
nn
ecte
dn
etw
ith
bct
top
olo
gy
.
[Mn
5(m
3-O
H) 2
-(s
db
a) 4
(2,2
9-b
py
) 2-
(H2O
) 2]?
H2O
20b
[Mn
5(m
3-O
H) 2
(m-
CO
O) 6
]O
ctah
edra
lm
an
gan
ese
con
nec
ted
thro
ugh
the
edg
esa
nd
corn
ers.
SD
BA
con
nec
tsth
eM
n5
clu
ster
no
des
form
ing
atw
od
imen
sio
na
l6
con
nec
ted
net
wit
hh
xl
top
olo
gy
.
[Mn
5O
2(H
ND
T) 2
-(N
DT
) 2(D
MF
) 820c
[Mn
5(m
3-O
) 2(t
et) 8
]M
an
ga
nes
eo
ctah
edra
con
nec
ted
thro
ugh
thei
rco
rner
s.
ND
Tan
dH
ND
Tco
nn
ects
the
Mn
5cl
ust
ern
od
esfo
rmin
ga
n8
con
nec
ted
net
wit
hb
cuto
po
log
y
Htr
z=
1,2
,4-t
ria
zole
;b
py
=b
ipy
rid
ine;
Me 3
-TB
zIm
=1,3
,5-t
ris(
ben
zim
idazo
yl-
1-y
lmet
hyl)
-2,4
,6-t
rim
eth
ylb
enze
ne;
bp
d=
1,4
-bis
(4-p
yri
dyl)
-2,3
-d
iaza
-1,3
-bu
tad
ien
e;H
2N
DT
=2
,6-d
i(1H
-tet
razo
l-5
-y
l)n
ap
hth
ale
ne;
tet
=te
rta
zoly
lg
rou
p.
4330 | CrystEngComm, 2012, 14, 4323–4334 This journal is � The Royal Society of Chemistry 2012
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conditions, giving rise to the H2SDBA acid (Fig. S14, ESI{).
This suggests that the 1D compound may not be the direct
precursor for the 3D compounds and the formation of the three-
dimensional compounds, reported here, might be through a
dissolution and re-crystallization pathway. Such mechanistic
pathways have been proposed previously.5d The question of
kinetic versus thermodynamic stability during the formation of
framework compounds under hydrothermal conditions is not yet
fully understood. It has been suggested that the removal of water
molecules from the system (bonded as well as free) is a
thermodynamic process4a,d,10a and there have been some reports
conforming this theory. The present understanding of the hydro-
thermal process is that the phases generally form under kinetic
control. The formation of many well known zeolites and other
related framework compounds conform to this theory.21b–d In the
present case, the 1D compound has water molecules bound to the
Mn centers. In addition, except for 3, all the other 3D compounds
contain water molecules. This suggests that the possible formation
pathway of these phases could be somewhere in between the kinetic
and the thermodynamic routes. Further investigations would be
necessary to understand and unravel this observation.
Optical studies
UV-Vis spectroscopic studies indicated that Na2SDBA exhibited
only one broad absorption peak at y298 nm, which may be due
to an intraligand charge transfer transition (Fig. S15, ESI{). For
all the compounds, five absorption bands were observed at
y254 nm, y294–298 nm, 335–365 nm, 381–420 nm and 507–
511 nm, respectively. The bands may correspond to the
transitions from the 6A1g ground state of the Mn+2 ions to the4A2g(F), 4T1g(P), 4T2g(D), 4Eg(G) or 4A1g and 4T2g exited states,
respectively.22 Similar observations for Mn(II) complexes have
been reported in the literature.22b The bands observed at y294–
298 nm could be the superposition of the charge transfer band of
the ligand as well as the 6A1g to 4T1g(P) transitions.
Fig. 5 (a) Field cooled (FC) and zero field cooled (ZFC) data for compound 1 (H = 0.1 T). (b) xmT vs. T plot and 1/xm vs. T plot (inset) for compound
1. (c) xmT vs. T plots at different fields for compound 1.
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All the compounds, as well as Na2SDBA, were excited using
an excitation wavelength of 255 nm to obtain the luminescence
spectra (Fig. S16, ESI{). A weak emission band was observed at
y330 nm for Na2SDBA and at y308 nm, y392 nm, y423 nm,
y484 nm, y530 nm for compounds 1–4. The various emission
bands could be assigned to the d–d transitions, 4T1g(P), 4T2g(D),4Eg(G), 4A1g and 4T2g to the 6A1g ground state.23 Similar
observations have been made previously in the literature.23b
Magnetic studies
For 1, the room temperature value of xmT (1000 O.e.) was found
to be 16.8 emu mol21 K, which is smaller than the expected value
of 21.2 emu mol21 K for five magnetically isolated high-spin
MnII (S = 5/2) ions with g = 2.00 (Fig. 5). This suggests that the
Mn2+ ions are strongly coupled.24 The 1/xm vs. T plot exhibits a
linear decrease as the temperature is reduced in the range of 300–
75 K, below which it shows a steep drop. A Curie–Weiss fit in the
range of 75–300 K gives values of C = 24.63 emu mol21 K and
hp = 2138.96 K (Fig. 5b inset). The xmT value also exhibits a
continuous decrease with a decrease in the temperature to a
minimum of 7.57 emu mol21 K at y48 K. On cooling below
this, the xmT values exhibit a sharp rise, reaching a maximum of
11.4 emu mol21 K at y38 K. The gradual decrease of the xmT
values with a decrease in the temperature to y48 K, along with
the negative value of hp, suggests that the interactions between
the metal centers are strongly antiferromagnetic.24,25 The rapid
increase in the value of xmT below 48 K, coupled with the steep
drop in the 1/xm vs. T plot, suggests the possibility of long range
magnetic ordering.25,26 The sharp drop in the xmT value below
y38 K may be due to the magnetic field saturation effect.25 This
behavior can also be seen in the FC–ZFC plot (Fig. 5a), where
the FC and ZFC behavior exhibits a divergence at y42 K. This
also suggests the possibility of long range magnetic correlations
between the Mn centers. The possible origin for this behavior
was investigated using a field dependent study (Fig. 5c). The
xmT–T values as a function of different applied fields exhibits
pronounced field dependent behavior. As can be noted from
Fig. 5c, at lower applied fields the increase in xmT values are
larger when compared to higher fields. This behavior is typically
observed in compounds exhibiting canted antiferromagnetism. A
similar trend has been observed previously in compounds
possessing –Mn–O–Mn– clusters and extended linkages.26–28
The M vs. H study on 1 does not exhibit any saturation up to 5 T
(Fig. S17, ESI{). The maximum magnetization value of 4.35 Nb
observed at 5 T, is considerably smaller than the expected
saturation value of 15 Nb for three unpaired Mn+2 ions. The lack
of saturation at high fields also confirms that the low
temperature magnetic ground state could be canted antiferro-
magnetic.25,26c AC magnetic studies were carried out at low
temperatures to probe the magnetic state further (Fig. 6). The
field dependent in phase (x9) and out of phase (x99) AC
susceptibilities exhibit only a single peak and no field depen-
dency was observed in the out of phase (x99) AC susceptibility.
The critical temperature (Tc) was found to be y42 K,
determined from the maximum of the x9 vs. T plot. We did not
observe any other variations either in the x9 or x99 behavior as a
function of temperature, suggesting that the present compounds
do not have any spin-glass like state. Similar behavior has also
been previously observed.27
For the compounds 2–4, the magnetic behavior and the values
of the magnetic parameters observed are similar and are given in
Table 4. The respective magnetic plots are given in the ESI (Fig.
S18–S20).{ For compounds 2–4, the Weiss constants were found
to be negative. The gradual decrease in the observed xmT values
with the decrease in temperature to y48 K, indicates that the
interactions between the metal centers could be antiferromag-
netic (Fig. S18a–S20a, ESI{). A rapid increase in the values of
xmT below y48 K, along with a steep drop in the 1/xm vs. T
behavior, suggests the possibility of long range magnetic
ordering in the compounds.25 The observed field dependence
behavior in the compounds indicates spin canted antiferromag-
netic behavior (Fig. S18c–S20c, ESI{).26–28 The saturation
magnetizations for all the compounds from the M vs. H studies
Fig. 6 (a) xm9 vs. T plot for compound 1 at a zero DC field and 10 O.e AC field at different frequencies. (b) xm99 vs. T plot for compound 1 at a zero
DC field and 10 O.e AC field at different frequencies.
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were found to be considerably smaller ((y4–4.5 Nb), Table 4)
than the expected value of 15 Nb for three unpaired Mn+2 ions,
which confirms that the low temperature magnetic ground state
of all the compounds could be canted antiferromagnetic.25 AC
magnetic susceptibility studies also do not indicate the possibility
of any spin-glass behavior in the compounds. The critical
temperature (Tc) for all the compounds was found to be y42 K
(Table 4).
Conclusions
The synthesis and structures of four manganese sulfonyldibenzo-
ates (SDBA) have been accomplished. All the compounds have
Mn–O–Mn linkages, giving rise to Mn5 clusters which are
connected to the SDBA acid, forming the three-dimensional
structure. The observation of fcu topology in all compounds is
noteworthy. Magnetic studies indicate canted antiferromagnetic
behavior. The SDBA acid, though closely related to the
terephthalic and oxy-bisbenzoic acids, has not been investigated
in detail and the present study indicates the possibilities of
forming new types of structures with interesting properties. The
participation of the sulfonyl group is interesting and we are
presently pursuing this behaviour.
Acknowledgements
The authors thank Prof. G. R. Desiraju for many insightful
discussions on the crystallographic aspects of the structures. SN
thanks the Department of Science and Technology (DST),
Government of India, for the award of a RAMANNA
Fellowship. The authors also thank the Council of Scientific
and Industrial Research, Government of India, for the award of
a research grant and a fellowship.
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Table 4 The various magnetic parameters for compounds 1–4
Compounds
CriticalTemperature(Tc) (K)
Room temperaturevalue of xmT(emu mol 21 K) hp (K)
C(emu mol21 K)
Maximummagnetizationvalues in M vs.H Plots (Nb)
Field dependencein AC susceptibilityplots
[Mn5(C14H8O6S)4-(C14H9O6S)2]?4.5H2O , 1
y42 16.83 2138.9 24.624 4.35 No
[Mn5K2(H2O)2(C14H8O6S)6], 2 y42 15.91 2204.4 26.533 4.24 No[Mn5Cs2(C14H8O6S)6], 3 y42 16.04 2315.1 32.776 4.12 No[Mn5(NH4)2(C14H8O6S)6]?2H2O, 4 y42 14.94 2210.1 25.432 4.46 No
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4334 | CrystEngComm, 2012, 14, 4323–4334 This journal is � The Royal Society of Chemistry 2012
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