DOI:
10.1039/D5DT00783F
(Paper)
Dalton Trans., 2025,
54, 11232-11245
1D polymeric and 2D layered zinc monoalkyl phosphates bearing long alkyl chains: synthesis, structural transformations and thermal behaviour†
Received
1st April 2025
, Accepted 21st June 2025
First published on 25th June 2025
Abstract
The reactivity of two different alkyl phosphate esters with zinc metal ions has been explored. The reaction of zinc nitrate with n-octyl phosphate leads to a mixture of [(nOctO)PO3Zn(DMF)]n (1) and [(nOctO)PO3Zn(H2O)]n (2a); similarly, the reaction of zinc nitrate with n-hexyl phosphate results in a mixture of [(nHexO)PO3Zn(DMF)]n (3) and [(nHexO)PO3Zn(H2O)]n (4). While the DMF-coordinated compounds 1 and 3 are isolated as single crystals, the water-coordinated compounds 2a and 4 were obtained as polycrystalline samples. Exposure of these mixtures (1 and 2a or 3 and 4) to ambient humid conditions results in the exchange of coordinated DMF molecules by water molecules and the whole mixture transforming into either 2a or 4, respectively. The molecular structures of 1 and 3 have been determined by single-crystal X-ray diffraction studies, revealing them to be one-dimensional coordination polymers. The presence of flexible alkyl chains in 2a and 4 results in structural transformation, where the interlayer distance in 2a decreases over time under ambient conditions to form 2b, and it returns to its initial state on heating at 50 °C for 20 hours in a vacuum. DSC studies for 2a and 4 show two low-enthalpy reversible transitions below room temperature, which could be associated with the 3D organization of alkyl chains in the structure. Thermal decomposition studies reveal that compounds 2a and 4 can be utilized as a single-source precursor for ceramic materials. The water contact angles for 2a and 4 are 100.5° and 98.8°, respectively, which fall within the range of hydrophobic materials, indicating the importance of alkyl chains in imparting the hydrophobicity.
1. Introduction
In recent years, there has been a significant surge in investigations on layered materials due to the exceptional physicochemical properties and versatile applications exhibited by this class of materials.1,2 These materials are used in various domains, such as catalysis,3 ion adsorption,4 electronics,5 gas sensing,6 and energy storage.2,7 Among the broad spectrum of layered materials, layered metal phosphates have garnered attention due to their structural versatility, chemical tunability, and intrinsic stability.2–4,7,8 Zinc phosphates represent a promising class of material, with applications as non-toxic anticorrosive agents in paints,9 support for optical materials,10 dental cement,11 glasses,12 ion exchange materials,13 electrode coatings,14,15 nonlinear optical devices,16,17 and therapeutic applications in cancer treatment.18,19
Layered zinc phosphates (LZPs), though relatively unexplored, hold significant potential for a variety of applications. Recent studies highlight their utility in emerging areas such as the development of phosphors,20 metal ion sensing,21 and proton conduction.22 LZPs can be obtained either by using amines or N-donor ligands as the structure-directing group23,24 or by carefully choosing the organophosphate ligand.25 However, due to the strong interaction between the layers, it is difficult to exfoliate these layers. In recent times, our group has explored the utility of monoalkyl phosphate precursors in the formation of layered metal phosphates.26,27 However, reports on zinc alkyl phosphates remain limited.28–30 Notably, the layered zinc ethyl phosphate reported by Clearfield and coworkers exhibits a structure comprising two-dimensional metal–ligand sheets held together by weak van der Waals interlayer interactions.29 Such weak interactions facilitate exfoliation into single nanosheets,26 which can be further exploited for various applications.
Alkyl phosphates additionally offer a unique advantage in the synthesis of metal phosphates, as their thermally labile alkyl groups enable the formation of ceramic metal phosphates at relatively low temperatures.31,32 Over the past few decades, two groups, Murugavel and coworkers and Tilley and coworkers, have shown the utility of di-tert-butyl phosphate-based metal complexes as synthons for ceramic metal phosphate synthesis.33–42 Recently, we started investigating monoalkyl phosphates for the formation of ceramic phosphates and showed that their exfoliation, followed by thermolysis, yielded metal phosphate materials with enhanced supercapacitance properties.26,43
The alkyl chain undergoes deformation with changes in temperature. Presence of longer alkyl chains, in particular, is anticipated to exhibit temperature-dependent structural transitions.44–48 These transitions find utility in functional applications, including the development of actuators48 and cobalt-based systems with unique spin-crossover behavior.49,50 However, crystallization of charge-neutral complexes with extended alkyl chains remains challenging, limiting detailed structural elucidation of these systems. To investigate structural transitions in the alkyl chain-bearing metal phosphates, we previously studied a calcium ethylhexyl phosphate complex, [(phen)Ca(ehpH)2]n.51 This compound was crystallized by exploiting the robustness imparted by the N-donor chelating ligand 1,10-phenanthroline,51 which helped in crystallization and allowed for the observation of a low-temperature structural transformation. However, the rigidity offered by 1,10-phenanthroline also constrained the extent of the structural transition.
Given the above background, in the current study, we have investigated a new family of zinc alkyl phosphates [(RO)PO3Zn(solvent)]n (where R = n-hexyl or n-octyl; solvent = DMF or water), whose R groups are made of highly flexible long alkyl chains, with the objective to realize the full range of structural transitions/transformations that these alkyl chains can undergo under a variety of conditions. The details of this study are presented in the following contribution.
2. Experimental section
2.1. Materials, methods, and measurements
All the experimental manipulations were carried out under ambient conditions. Zn(NO3)2·6H2O (Spectrochem) was procured from commercial sources and used as received. Dimethylformamide (DMF) (Finar) was dried over CaSO4 and subsequently distilled under reduced pressure and stored over 4 Å molecular sieves. The ligands n-hexyl and n-octyl phosphates were synthesized by following reported procedures.52 Melting points were measured in glass capillaries and are reported uncorrected. Fourier transform infrared (FT-IR) spectra were recorded using a PerkinElmer Spectrum One FT-IR spectrometer with diluted samples prepared as KBr discs. Microanalyses were performed on a Vario MICRO cube microanalyzer (Elementar Analysensysteme, Germany). Solid state 31P CP-MAS NMR (303 MHz) studies were performed by diluting samples with KBr on a Bruker BioSpin Ascend 750 MHz spectrometer (for 1–4) and solid-state 31P single-pulse NMR (162 MHz) on a Bruker 400 MHz spectrometer (for 2a-800 °C and 4-800 °C). Powder X-ray diffraction studies were carried out on a Rigaku SmartLab SE diffractometer using Cu Kα radiation (1.5419 Å). Variable temperature powder XRD measurements were performed in air using a Rigaku HT 1500 high-temperature attachment, with a heating rate of 10 °C min−1. At each measurement temperature, the sample was stabilized for 15 minutes before data collection. Thermogravimetric analyses were performed under a nitrogen gas stream at a heating rate of 10 °C min−1 using a Rigaku STA8122 TGA system. Contact angle measurements were performed at room temperature on an Acam series Apex goniometer (India). Contact angle measurements of 2a and 4 were carried out in triplicate using pellets made on an FT-IR hydraulic press. A total of 5 μL of water was added on the surface of each pellet, and the average contact angles along with the standard deviation were recorded. Differential scanning calorimetric measurements were performed on a Rigaku DSCvesta calorimeter. An empty aluminium pan was used as a reference. 7.9 mg of 2a and 7.1 mg of 4 were used for carrying out the experiment. The measurements were performed in two cycles to confirm the reproducibility. The data obtained in the second cycle were used to calculate the enthalpy and the position of the transition.
Morphologies were studied using FEG-SEM on a ZEISS Ultra 55 field-emission gun-scanning electron microscope operating at an accelerating voltage of 3 kV. EDS mapping was performed on the same samples but at 18 kV using an in-lens detector. The samples for SEM and EDS measurements were prepared by smearing powders of 2a and 4 on carbon paper, whereas samples of the pyrolyzed products were prepared by drop-casting well-dispersed suspensions (in isopropanol) of 2a-800 °C and 4-800 °C on a silicon substrate. The samples were sputtered with gold before imaging. Raman spectra were recorded on a Witec 300 Micro Raman spectrometer equipped with He–Ne (632.8 nm) laser excitation sources. Inductively coupled plasma-atomic emission spectroscopy (ICP-AES) analyses were carried out on a SPECTRO ARCOS Simultaneous ICP instrument.
2.2. Synthesis of [(nOctO)PO3Zn(DMF)]n (1) and [(nOctO)PO3Zn(H2O)]n (2a and 2b)
A solution of n-octyl phosphate (0.5 mmol, 105 mg) in DMF (10 mL) was added to a solution of Zn(NO3)2·6H2O (0.5 mmol, 148.5 mg) in DMF (10 mL) under constant stirring. The resulting clear solution was allowed to evaporate at room temperature to obtain white plate-like crystals of 1 along with a white precipitate of 2a, after two weeks. Single crystals of 1 were separated manually under an optical microscope.
Compound 1.
Yield: 30 mg (19%); Mp. >300 °C; elem. anal. found (calcd) (%) for C11H24NO5PZn (Mr = 346.67): C: 37.25 (38.11), H: 6.5 (6.98), N: 3.64 (4.04); FT-IR (KBr pellet, cm−1): 1120 (s), 1085 (s), 1207 (w), 1386 (w), 1657 (s), 2852 (w), 2925 (m), 2958 (m), 3431 (w), 3562 (w); 31P NMR (CP-MAS, 303 MHz): δ 4.25 ppm; TGA: temp range °C (%, weight loss): 80–160 (observed: 21; calculated: 21, DMF), 260–320 (observed: 35; calculated: 35, octene; 0.5 H2O). Note: the discrepancy observed in the elemental analysis values is due to its dynamic conversion to 2 through DMF–H2O exchange.
Compound 2a.
Yield: 47 mg (32%); Mp. >300 °C; elem. anal. found (calcd) (%) for C8H19O5PZn (Mr = 291.6): C: 32.85 (32.95), H: 6.35 (6.57). FT-IR (KBr pellet, cm−1): 1060 (s), 1113 (s), 1453 (w), 1634 (w), 2859 (w), 2930 (m), 2958 (m), 3431 (w), 3562 (w). 31P NMR (CP-MAS, 303 MHz): δ 5.75 ppm. TGA: temp range °C (%, weight loss): 122–207 (observed: 5; calculated: 6, H2O), 207–304 (observed: 42; calculated: 41, octene; 0.5 H2O).
In situ conversion of 1 into 2b.
On removing crystals of 1 from the reaction mixture and exposing them to an open atmosphere under ambient conditions, DMF molecules in 1 exchange with atmospheric water to form 2a, which eventually transforms to 2b.
Compound 2b (formed by in situ conversion of 1 into 2b).
Yield: 30 mg (2%); Mp. >300 °C; elem. anal. found (calcd) (%) for C8H19O5PZn (Mr = 291.6): C: 33.27 (32.95), H: 6.58 (6.57); FT-IR (KBr pellet, cm−1) 1015 (s), 1028 (s), 1062 (s), 1085 (s), 1113 (s), 1262 (w), 1466 (w), 1631 (w), 2358 (w), 2855 (w), 2927 (m), 2955 (m), 3356 (w); 31P NMR (CP-MAS, 303 MHz): δ 5.17 ppm.
2.3. Synthesis of [(nHexO)PO3Zn(DMF)]n (3) and [(nHexO)PO3Zn(H2O)]n (4)
Compounds 3 and 4 were prepared by following a procedure similar to that for 1 and 2 using n-hexyl phosphate (0.5 mmol, 91 mg) and an equimolar amount of zinc nitrate.
Compound 3.
Yield: 4 mg (2.5%); Mp. >300 °C; elem. anal. found (calcd) (%) for C9H20NO5PZn (Mr = 318.6): C: 32.68 (32.31), H: 6.82 (6.02), N: 2.78 (4.19); FT-IR (KBr pellet, cm−1): 1117 (s), 1077 (s), 1200 (w), 1390 (w), 1664 (s), 2861 (w), 2930 (m), 2958 (m), 3431 (w); 31P NMR (CP-MAS, 303 MHz): δ 0.42 ppm, δ 3.62 ppm; TGA: temp range °C (%, weight loss): 40–160 (observed: 24.3; calculated: 23, DMF), 260–306 (observed: 29; calculated: 29, hexene; 0.5 H2O). Note: the discrepancy observed in the elemental analysis values is due to its dynamic conversion to 4 through DMF–H2O exchange.
Compound 4.
Yield: 75 mg (57%); Mp. >300 °C; elem. anal. found (calcd) (%) C6H15O5PZn (Mr = 263.5): C: 27.88 (27.35), H: 5.70 (5.74). FT-IR (KBr pellet, cm−1): 1060 (s), 1113 (s), 1453 (w), 1634 (w), 2859 (w), 2930 (m), 2958 (m), 3431 (w), 3562 (w); 31P NMR (CP-MAS, 303 MHz): δ 3.47 ppm; TGA: temp range °C (%, weight loss): 122–207 (observed: 7; calculated: 7, H2O), 207–304 (observed: 37; calculated: 35, hexene; 0.5 H2O).
Compound 4 (formed by in situ conversion of 3 into 4).
Yield: 4 mg (2.5%); Mp. >300 °C; elem. anal. found (calcd) (%) C6H15O5PZn (Mr = 263.5): C: 27.09 (27.35), H: 5.73 (5.74); FT-IR (KBr pellet, cm−1): 550 (w), 854 (w), 1015 (s), 1028 (s), 1062 (s), 1085 (s), 1113 (s), 1384 (w), 1467 (w), 1631 (w), 2358 (w), 2855 (w), 2956 (m), 2955 (m), 3356 (w); 31P NMR (CP-MAS, 303 MHz): δ 3.84 ppm.
2.4. Reversibility of DMF–water exchange in 2a and 4
20 mg of 2a was suspended in 10 mL of DMF in a 20 mL glass vial and sonicated under heated conditions (50 °C) for 2 hours. Following sonication, the solid was filtered from the suspension and immediately analyzed by powder XRD. To further assess the reversibility of the solvent exchange, the same sample was treated with a drop of deionized water, dried, and subjected to powder XRD analysis once again.
Similarly, 20 mg of compound 4 was suspended in 10 mL of DMF in a 20 mL glass vial and sonicated at 50 °C for 2 hours. However, in this case, no conversion to DMF-exchanged species was observed as seen by powder XRD. Hence, the next step was not performed.
2.5. Reversibility of 2a to 2b phase change
30 mg of 2b was heated under vacuum at 50 °C for 20 hours, followed by immediate analysis using PXRD and TGA.
2.6. Solid state thermolysis
Compound 2a (84 mg) was placed in an alumina crucible and heated to 800 °C in air at a heating rate of 10 °C min−1 for 24 h followed by cooling the sample to room temperature, yielding crystalline 2a-800 °C. Yield: 31 mg (72%); FT-IR (KBr pellet, cm−1): 1129 (s), 1101 (m), 1078 (m), 1044 (m), 1014 (m), 946 (s), 758 (s), 646 (w), 543 (s); ICP-AES: Zn
:
P ratio: 1
:
0.915.
Similarly, compound 4 (81 mg) was pyrolyzed at 800 °C to obtain 4-800 °C. Yield: 38 mg (81%); FT-IR (KBr pellet, cm−1): 1122 (s), 1101 (m), 1080 (m), 1051 (m), 1014 (m), 958 (s), 753 (s), 640 (w), 543 (s). ICP-AES: Zn
:
P ratio: 1
:
1.32.
2.7. Single-crystal X-ray diffraction studies
Single crystals of compounds 1 and 3 suitable for X-ray diffraction analysis were grown from the reaction mixture and mounted on a BRUKER D8 QUEST diffractometer equipped with an IμS DIAMOND microfocus Mo-Kα radiation source (λ = 0.71073 Å). Data collection, data integration, and indexing were performed with the CrysAlisPro software suite.53 The structures were solved using the SHELXT program and refined with SHELXL54 by the least squares method using the Olex2 package.55 The data collection and refinement processes are summarized in Table 1. CCDC deposition numbers 2350478 and 2350479† for 1 and 3 contain the supplementary crystallographic data for this paper, which can be obtained free of charge from the Cambridge Crystallographic Data Centre.
Table 1 Crystallographic data for [(nOctO)PO3Zn(DMF)]n (1) and [(nHexO)PO3Zn(DMF)]n (3)
Compound number |
1
|
3
|
Sample code |
RM-HA-62 |
RM-HA-61 |
Empirical formula |
C11H24NO5PZn |
C9H20NO5PZn |
Formula weight |
346.65 |
318.60 |
Temperature/K |
150.0(1) |
107.0(4) |
Crystal system |
Triclinic |
Triclinic |
Space group |
P![[1 with combining macron]](https://www.rsc.org/images/entities/char_0031_0304.gif) |
P![[1 with combining macron]](https://www.rsc.org/images/entities/char_0031_0304.gif) |
a/Å |
5.4254(2) |
5.4197(2) |
b/Å |
9.4114(3) |
9.3778(4) |
c/Å |
15.2643(4) |
13.3722(5) |
α/° |
85.187(2) |
83.203(3) |
β/° |
82.270(2) |
88.754(3) |
γ/° |
82.405(3) |
82.318(3) |
Volume/Å3 |
763.81(4) |
668.79(5) |
Z
|
2 |
2 |
ρ
calc, g cm−3 |
1.507 |
1.582 |
μ/mm−1 |
1.726 |
1.964 |
F(000) |
364.0 |
332.0 |
Crystal size/mm3 |
0.62 × 0.154 × 0.026 |
0.595 × 0.103 × 0.095 |
Radiation/Å |
Mo Kα (λ = 0.71073) |
Mo Kα (λ = 0.71073) |
2θ range for data collection/° |
4.376 to 50.05 |
4.412 to 49.996 |
Index ranges |
−6 ≤ h ≤ 6, −11 ≤ k ≤ 11, −18 ≤ l ≤ 18 |
−6 ≤ h ≤ 6, −11 ≤ k ≤ 11, −15 ≤ l ≤ 15 |
Reflections collected |
28 102 |
25 008 |
Independent reflections |
2700 [Rint = 0.0531, Rsigma = 0.0234] |
2358 [Rint = 0.0465, Rsigma = 0.0215] |
Data/restraints/parameters |
2700/0/175 |
2358/0/157 |
Goodness-of-fit on F2 |
1.033 |
1.053 |
Final R indexes [I ≥ 2σ(I)] |
R
1 = 0.0272, wR2 = 0.0655 |
R
1 = 0.0225, wR2 = 0.0516 |
Final R indexes [all data] |
R
1 = 0.0292, wR2 = 0.0670 |
R
1 = 0.0235, wR2 = 0.0521 |
Largest diff. peak/hole/e Å−3 |
0.37/−0.43 |
0.34/−0.34 |
3. Results and discussion
3.1. Synthesis and characterization of zinc alkyl phosphates
The reaction of equimolar quantities of zinc nitrate hexahydrate and n-octyl phosphate (L1) in DMF leads to the formation of a DMF-coordinated polymer [(nOctO)PO3Zn(DMF)]n (1) as the minor product, and a water-coordinated polymer [(nOctO)PO3Zn(H2O)]n (2a) as the major product. Exposing crystals of 1 to air results in rapid exchange of DMF molecules with moisture (H2O), leading to its conversion to 2a (Scheme 1). Similarly, [(nHexO)PO3Zn(DMF)]n (3) and [(nHexO)PO3Zn(H2O)]n (4) were synthesized using n-hexyl phosphate (L2). These reactions were repeated multiple times under identical conditions, consistently yielding the same products, thereby confirming their high reproducibility. These polymers 1–4 were characterized by various spectroscopic and analytical techniques.
 |
| Scheme 1 Synthesis of zinc phosphates 1–4. | |
The FT-IR spectra of 1–4 show strong absorption bands around 1150–1000 cm−1, corresponding to P
O stretching, and M–O–P asymmetric and symmetric vibrations (Fig. S1 and S2†).26,35 The absorption bands observed at 2917 and 2836 cm−1 correspond to C–H stretching of the alkyl groups. The elemental analysis values obtained for 2a and 4 match well with the calculated values. However, the values for both 1 and 3 show a discrepancy between the observed and calculated elemental analysis values due to their tendency to rapidly undergo interconversion to 2a and 4, respectively. The 31P CP-MAS NMR spectra of 1 and 3 exhibit broad peaks due to the dynamic exchange of DMF with moisture, which converges to a single peak at δ 5.75 and 3.47 ppm for 2a and 4, respectively (Fig. 1 and S3†). The additional minor signal observed at δ 7.87 ppm for 4 can be attributed to the presence of minor species of a slightly different environment around the phosphorus centre, probably due to a different conformation of alkyl chains. However, we have not been able to determine conclusively the exact source of this signal.
 |
| Fig. 1
31P CP-MAS NMR spectra of 1 and 2a (303 MHz). | |
3.2. Crystal structure of 1D coordination polymers 1 and 3
Colourless plate-shaped crystals of 1 and 3 were obtained from the reaction mixture after two weeks at room temperature. X-ray diffraction studies reveal that compounds 1 and 3 crystallize in the triclinic P
space group and are isostructural. The asymmetric part of the unit cell of 1 and 3 consists of one zinc ion, one alkyl phosphate anion (ROPO32−, R = n-octyl (1) and n-hexyl (3)) and one coordinated DMF molecule. The zinc ion is coordinated with three oxygen atoms of different alkyl phosphate ligands, while the fourth coordination site is occupied by the oxygen atom of the DMF molecule (Fig. 2a and b). This arrangement results in distorted tetrahedral geometry around the zinc ion with Zn–O(P) bond lengths of 1.925(2) Å for Zn1–O31, 1.910(2) Å for Zn1–O2, and 1.914(2) Å for Zn1–O12 in 1, and 1.928(1) Å for Zn1–O31, 1.912(1) Å for Zn1–O2, and 1.913(1) Å for Zn1–O12 in 3 (#1: −1 + X, +Y, +Z; 2: 1 − X, 1 − Y, 2 − Z; 3: 1 + X, +Y, +Z). The tetrahedral geometry around the zinc atom has also been confirmed by shape analysis (Tables S1 and S2†).56 The Zn–O(P) bond lengths in 1 and 3 are comparable to those observed in earlier reported zinc alkyl and aryl phosphates.29,35,57 The bond length of Zn–O from the DMF molecule is 2.025(2) Å (Zn1–O5) in 1 and 2.023(1) Å (Zn1–O5) in 3, which are significantly longer compared to the Zn–O(P) bonds. The O–Zn–O bond angles for the distorted tetrahedron range from 100.00(7)° to 115.69(7)° in 1 and 99.92(6)° to 115.83(6)° in 3, showcasing the extent of distortion around the tetrahedral zinc centres. Similarly, the O–P–O bond angles vary in the range of 102.42(9)°–112.86(9)° for 1 and 102.39(8)°–112.94(8)° for 3. The observed P–O bond lengths in 1 are P1–O1: 1.505(2), P1–O2: 1.522(2), P1–O3: 1.521(2), and P1–O4: 1.594(2) Å; similar distances were observed in 3: P1–O1: 1.510(1), P1–O2: 1.526(1), P1–O3: 1.521(2), and P1–O4: 1.595(1) Å. The selected bond angles and bond lengths for 1 and 3 have been listed in Tables S3 and S4.†
 |
| Fig. 2 (a and b) Molecular structure of [(nOctO)PO3Zn(DMF)]n (1) and [(nHexO)PO3Zn(DMF)]n (3) showing the section of the polymeric structure and geometry around the zinc atom (asymmetric unit). (c and d) Edge sharing S4R rings forming a 1D coordination polymer for 1 and 3, respectively (hydrogen atoms are omitted for clarity; colour scheme; : Zn, : P, : O, : N, : C). | |
Alkyl phosphate ligands in compounds 1 and 3 are tridentate and exhibit a [3.111] mode of coordination (Fig. 2c and d).26,58 It should be noted that the three ligating oxygen atoms bind three different zinc ions. In other words, the zinc ions are ligated/bridged by three different phosphate oxygen atoms arising from three different phosphate ligands. This leads to the formation of Zn2O4P2 eight-membered rings, which resemble the Single-4-Ring (S4R) zeolitic SBUs (Fig. S4a and S5a†). Moreover, the side-by-side fusion of these S4R rings leads to the formation of 1D polymeric chains whose central core resembles a ‘tape’ made up of indefinite edge-sharing S4R rings extending along the a-axis in both 1 and 3 (Fig. 2c and d). In the 1D polymeric chain, the eight-membered rings of the adjacent S4R rings exhibit different ring conformations, as evidenced by different Zn–Zn diagonal distances. These distances are 4.2278(4) and 4.5003(4) Å for adjacent rings in 1 (Fig. S4b†), and 4.2306(4) and 4.4959(4) Å in 3 (Fig. S5b†). The inorganic tape is capped on both sides by the coordinated DMF molecules on zinc and the long alkoxy chain on phosphorus. The presence of all trans octyloxy and hexyloxy chains (which do not coil around), leads to the stacking of these 1D tape-like polymers adjacent to each other in the crystal lattice (Fig. 3).
 |
| Fig. 3 (a) Variation in the interlayer distance of interdigitated 1D polymer [(nOctO)PO3Zn(DMF)]n (1), upon transformation to [(nOctO)PO3Zn(H2O)]n (2a). (b) Variation in interlayer distance upon the transformation of [(nHexO)PO3Zn(DMF)]n (3) to [(nHexO)PO3Zn(H2O)]n (4), showing the expansion of the interlayer distance on coordination with water [colour scheme; : Zn, : P, : O, : N, : C]. | |
The presence of hydrophobic van der Waals type interactions between the alkoxy groups of the immediate neighbours in these complexes leads to a packing arrangement such as that shown in Fig. 3a and b, where the alkoxy chains of the adjacent polymeric chains are involved in near-perfect interdigitation, as has been normally observed in many other layered metal alkyl phosphates and phosphonates,26,29 albeit in the present case, the crystal packing is due to agglomeration of polymeric chains and not 2D sheets. The packing diagrams of 1 and 3 further reveal that owing to perfect interdigitation, they achieve close packing, exhibiting inter-polymer distances of 15.3 Å in 1 and 13.4 Å in 3. Clearfield and co-workers reported water-coordinated zinc ethyl phosphate that adopts a two-dimensional polymeric structure.29 Similarly, the long-chain phosphonate analogue, calcium hexyl phosphonate, reported by Mallouk also forms a two-dimensional polymeric network.59 These studies suggest that both short- and long-chain alkyl phosphonates and phosphates tend to favor the formation of two-dimensional polymeric architectures. However, in the case of 1 and 3, where DMF is coordinated to the metal centre, the relatively larger steric bulk hinders the growth of the polymer in the perpendicular direction. As a result, one-dimensional DMF-coordinated polymers 1 and 3 were isolated instead.
3.3. Structural evolution by exchange of DMF with water molecules
Although 1D polymers 1 and 3 have been isolated as single crystals and their structures determined by SCXRD, both solids are relatively unstable in open air and readily convert into their secondary polymeric forms 2a and 4, respectively. While the presence of bulky DMF at the fourth coordination site on the zinc ion in 1 and 3 ensures the isolation of 1D polymers, the rapid replacement of DMF by water on standing over a period of time brings about interesting changes in the PXRD pattern. The most intriguing aspect of the structures of 1 and 3 emerges from closer examination of the PXRD patterns of their freshly prepared samples. The powder XRD pattern of 1 shows slight deviations from the simulated pattern obtained from the single-crystal structure (Fig. 4a and S6†). The slight deviations can be attributed to crystal morphology and temperature-dependent changes in the orientation of the alkyl chains. This is because powder XRD patterns were recorded at room temperature, whereas the molecular structure studies were conducted at 150 K and 107 K for 1 and 3, respectively.51 Thus, as has been mentioned above, compound 1 is sufficiently stable for its PXRD pattern to be recorded for its pure form obtained from the single crystals isolated freshly from the mother liquor. However, the PXRD pattern for a similar sample of 3 is entirely different (Fig. 4a and S7†), where one observes additional stronger reflections of compound 4, with only a minor proportion of 3.
 |
| Fig. 4 (a) Powder XRD patterns for 1–4; the interdigitated 1D polymer 1 and 3 shows narrower interlayer spacing compared to 2a and 4, respectively; a pure experimental PXRD pattern for 3 could not be obtained due to rapid solvent exchange. (b and c) SEM images of 1 and 4, respectively. | |
The powder XRD pattern of 2a exhibits reflections at 2θ values of 3.7° (d = 23.8 Å), 7.4° (d = 11.9 Å), and 11.2° (d = 7.9 Å) (Fig. 4a). Likewise, the powder XRD pattern of 4 shows reflections at 2θ = 4.5° (d = 19.5 Å), 9.0° (d = 9.8 Å), and 13.5° (d = 6.5 Å) (Fig. 4a), indicating a layered structure. The lowest angle of reflection has the highest intensity, and this progressively decreases moving towards the higher angles of reflection. Furthermore, the observed d-spacings follow a 1
:
1/2
:
1/3 ratio, suggesting a highly organized layered structure exhibiting reflections corresponding to the 001, 002, and 003 planes.60–62 In case of 2a, the interlayer distance has increased to a higher value (d = 23.8 Å) than that seen for the interdigitated polymer 1 (15.3 Å). Similarly, in the case of 4, the interlayer distance has increased to a higher value (d = 19.6 Å) compared to that observed in the interdigitated 1D polymer 3 (13.4 Å). This difference can be explained by the opening up of interdigitated alkyl chains on exchange of DMF with H2O (Fig. 3a and b) to form 2D layered materials. A similar kind of expanded structure for aluminium alkyl phosphates and calcium hexyl phosphonates has been previously observed by the groups of Tanaka60–62 and Mallouk.59 The interlayer distance in metal alkyl phosphates and phosphonates increases with an increase in the number of carbon atoms in the alkyl chain.60–63 Interlayer distances reported for water-coordinated zinc methyl phosphonate and zinc ethyl phosphonate are 8.73 Å and 10.14 Å, respectively.64 Similarly, water-coordinated zinc ethyl phosphate shows an interlayer spacing of 10.2 Å.29 In this study, when the alkyl chain length increases to six and eight carbon atoms, the interlayer spacing expands significantly to 19.5 Å and 23.8 Å, respectively.
Additionally, SEM analysis was performed to study the morphological features of polymers 1–4 (Fig. 4b, c and S8†). The SEM image of 1 shows a spindle formed by a collection of rod-shaped microcrystals. The SEM images of 4 reveal sheets cleanly stacked one over the other to form a lamellar compound, indicating the significance of alkyl groups for synthesizing compounds having layered morphology.
3.4. Tracking of DMF–water exchange by PXRD studies
The powder XRD patterns recorded after ambient drying of 1 and 3 did not match their respective simulated patterns but instead closely matched the diffraction patterns recorded for 2a and 4, respectively. Time-dependent powder XRD studies were therefore conducted over a period of time to investigate the structural evolution of 2a from 1 and 4 from 3, respectively. The powder XRD patterns were recorded at various intervals after removing crystals of 1 and 3 from the reaction mixture (Fig. 5 and S9†). Initially, a fresh sample of 1 shows an XRD pattern corresponding to 1 with a 001 reflection at 5.6° (Fig. 5, 0 h). After two hours, a new pattern emerged featuring reflections at 3.7°, 7.4°, and 11.1°, indicating the formation of compound 2a. After eight hours, the majority of compound 1 transforms into 2a. A similar observation was reported by Kanoh and co-workers., where a 1D polymer transitioned into a 2D polymer by the loss of coordinated solvent molecules.65 Given that alkyl phosphates have a propensity to form 2D polymers,26,29 the alteration in the powder XRD pattern suggested the conversion of 1D polymer 1 into a 2D polymer 2a. Furthermore, elemental analysis was carried out to verify the exchange of DMF with water, which reveals that the sample is free from nitrogen (of DMF) after 8 hours and correspond to the molecular formula [(nOctO)PO3Zn(H2O)]n.
 |
| Fig. 5 Structural evolution of [nOctOPO3Zn(H2O)]n (2a and 2b) from the freshly prepared [nOctOPO3Zn(DMF)]n (1) monitored by powder XRD. Initially, the XRD pattern shows reflections corresponding to 1, with a 001 reflection peak at 5.6°. As time progresses, new peaks appear corresponding to 2, having a 001 reflection at 3.7°, while the intensity of reflections due to 1 decreases. After eight hours, the reflections associated with 1 are significantly reduced, indicating that most of it has transformed into 2a. After fifteen hours, a new pattern began to appear with a 001 reflection peak at 4.1°, corresponding to a decrease in the interlayer distance of 2a due to the flexible nature of the alkyl chains. Compound 2a completely transforms to 2b in two weeks, exhibiting a decreased d-spacing. | |
Similarly, fresh crystals of 3 exhibit reflection at 6.3°, which is characteristic to 3, along with reflections at 4.5°, 9.0°, and 13.6° that correspond to 4 (Fig. S9†). Reflections corresponding to 4 are dominant, indicating that a significant portion of 3 has already converted into 4 upon removal from the solution. The time-dependent powder XRD measurements show that after forty hours, 3 completely transforms into 4. The elemental analysis of the sample of 3 that has completely transformed into 4 matches well with [(nHexO)PO3Zn(H2O)]n.
To further confirm DMF–water exchange, 31P CP-MAS NMR studies were carried out on the solid samples of 1 and 3. The first set of NMR measurements was performed on a fresh batch of crystals immediately after their removal from solution. Subsequently, another set of measurements was performed after allowing the crystals to remain in air. It was observed that the 31P CP-MAS NMR spectra of the samples immediately removed from solution revealed a broad NMR signal due to the initiation of exchange of DMF with water for both 1 and 3. Upon further exposure to air, distinct resonances corresponding to 2a and 4 began to emerge (Fig. 1 and S3†). To investigate the reversibility of the DMF–water exchange, 2a and 4 were sonicated at 50 °C in DMF for two hours. Powder X-ray diffraction (PXRD) patterns recorded immediately after removing 2a from the suspension showed the appearance of a reflection at 5.5°, characteristic of compound 1, along with reflections corresponding to 2a (Fig. S10†). Furthermore, one drop of water was added to the same sample, which led to the disappearance of the reflection due to 1. This indicates that the transformation from 1 to 2avia DMF–water exchange is a reversible process. However, subjecting 4 to similar conditions did not result in the regeneration of 3 as seem from its powder XRD plot after sonication in DMF for 2 h under the same conditions (Fig. S11†), suggesting that the DMF–water exchange is either not reversible in this case or that any formation of 3 rapidly reverts back to 4 upon removal from solution.
A second dynamic process sets in for a sample of 2a (obtained by in situ conversion from 1) kept under ambient conditions beyond 8 hours (Fig. 5). The PXRD patterns recorded after 15 hours and 21 hours reveal the emergence of a new phase 2b with small shifts in 2θ values from 3.7° to 4.1°, 7.4° to 8.2°, and 11.2° to 12.3° (Fig. 5). This dynamic process is complete after approximately two weeks. During the conversion of 2a to 2b, the interlayer spacing marginally decreases from 23.8 Å to 21.6 Å, which can be attributed to the flexibility in the structure due to ordering and disordering of alkyl chains.44 Although the transformation of 2a to 2b was observed within 15 hours when 2a was generated in situ from 1, the conversion was significantly slower in the case of microcrystalline 2a obtained directly from the reaction mixture, requiring more than two weeks for complete transformation into 2b. Elemental analysis indicated that 2a and 2b share the same chemical composition. Furthermore, 2b was heated at 50 °C under vacuum for 20 hours, resulting in its conversion back to 2a, as evident by the powder XRD pattern (Fig. S12†). The similar composition of 2a and 2b is further supported by the TGA data collected before and after evacuation, which show nearly identical thermal decomposition profiles (Fig. S13†).
The temperature-dependent structural changes were studied using variable temperature powder XRD for 2b and 4. For compound 2b, the reflection appearing at 4.1° at room temperature shifts to a lower 2θ value of 3.7° on heating to 200 °C, signifying expansion of the interlayer distance (d-spacing) (Fig. S15a†), which matches with the interlayer distance of 2a. However, this phase could not be assigned to 2a since the coordinated water will be lost at such a high temperature, as evident from the TGA results (Fig. 6a). However, it can be inferred that the alkyl chains have the same orientation as that of 2a, since water, being a small molecule that is buried within the structure, has little effect on the interlayer distance, which is predominantly governed by the organization of the alkyl chains. While not widely reported, there are a few examples of layered phosphonates in the literature, such as zinc ethyl phosphonate produced by Mallouk and co-workers66 and zinc phenyl phosphonate produced by Clearfield and co-workers,67 where the hydrated and dehydrated phases exhibit similar interlayer spacings. Similarly, variable temperature powder XRD of 4 reveals temperature-dependent phase transformation (Fig. S16a†). The reflection originally appearing at 4.6° shifts to a lower value of 4.0° on heating to 150 °C, indicating an expansion of the interlayer distance from 19.6 Å at room temperature to 22.1 Å at 150 °C. Further cooling cycles were recorded for these transitions, which show the irreversible nature of these temperature-dependent transitions (Fig. S15b and S16b†). These observations indicate the flexible nature of the alkyl chain in 2a and 4 and suggest that the layered metal alkyl phosphates can exist in phases having different interlayer distances due to the flexibility (folding and unfolding) of the alkyl chains. This further explains the huge variation in the interlayer spacing observed in the metal alkyl phosphates having the same alkyl chain length, as can be seen in Table S5.†
 |
| Fig. 6 (a) TGA traces of 2a and 4 recorded under a flow of N2 at a heating rate of 10 °C min−1; (b and c) DSC plots of 2a and 4, respectively, at a scanning rate of 10 °C min−1 under an N2 atmosphere. | |
3.5. Thermal studies
Metal alkyl phosphates undergo β-hydride elimination at elevated temperatures, leading to the formation of metal phosphates at comparatively lower temperatures.68 We have investigated the thermal decomposition of compounds 1–4 using TGA under a nitrogen atmosphere at a heating rate of 10 °C min−1. TGA of 1 and 3 shows initial weight loss of approximately 21.0% and 24.3%, respectively, occurring at around 120 °C (Fig. S17†), consistent with the loss of coordinated DMF molecules. For compound 3, the observed weight loss slightly exceeds the calculated value of 23.0% for the loss of DMF molecules. This minor discrepancy is attributed to the presence of surface-adsorbed water, as also indicated by a slight weight loss beginning at room temperature. Despite this, the first major weight loss event in both compounds occurs near 120 °C, confirming that the majority of the mass loss is due to DMF molecules. Subsequent weight loss of 35% for 1 and 29% for 3 at 300 °C corresponds to the loss of alkene and water molecules via condensation of two P–OH groups, respectively. Compounds 2a and 4 exhibit similar decomposition patterns in TGA (Fig. 6a). An initial weight loss of 5% and 7% at 200 °C for 2a and 4, respectively, indicates the loss of coordinated water molecules. This was followed by another weight loss of 42% for 2a and 37% for 4 at 300 °C, attributed to β-H elimination of the alkyl chains and subsequent water release via condensation of phosphate hydroxyl groups.
To investigate the structural changes associated with decomposition of zinc alkyl phosphates and the formation of ceramic zinc phosphates, we conducted variable temperature powder XRD for compound 2b over a range of temperatures up to 800 °C (Fig. S14†). Upon heating at 300 °C, 2b underwent conversion to an amorphous phase as revealed in the powder XRD profile. This is attributed to the loss of the octyl groups, which can also be confirmed by the weight loss at 300 °C observed in the thermogram (Fig. S13†). The amorphous phase remained until 550 °C, above which a crystalline phase started to appear with complete crystallization occurring at 800 °C.
It has been earlier shown that the temperature-dependent structural transformations in metal complexes are facilitated by the inherent flexibility of their alkyl chains.44,51 Recently, we have shown that these transitions are associated with the folding of alkyl chains, resulting in the change of the crystal system as showcased in [(phen)Ca(ehpH)2]n.51 Due to the presence of flexible alkyl chains in 2a and 4, these compounds are expected to show temperature-dependent phase transitions. These transitions can be observed by DSC measurements in the temperature range of −50 °C to 115 °C under a nitrogen atmosphere. The heat flow versus temperature plot of 2a reveals two low-enthalpy exothermic transitions at 15 °C (ΔH = 1.8 J g−1) and −2.4 °C (ΔH = 3.9 J g−1) during the cooling cycle (Fig. 6b). Corresponding endothermic peaks were observed upon heating at 1.8 °C (ΔH = 3.4 J g−1) and 19.7 °C (ΔH = 1.8 J g−1). The low-enthalpy transition at 19.7 °C explains the observed room temperature structural changes in 2a. In the case of 4, the heat flow vs. temperature plot reveals a low-enthalpy exothermic transition at −20 °C (ΔH = 0.491 J g−1) and a high-enthalpy exothermic transition at −34.8 °C (ΔH = 13.9 J g−1) (Fig. 6c). Upon heating, corresponding endothermic peaks are observed at −26.3 °C (ΔH = 13.6 J g−1) and −2.0 °C (ΔH = 0.8 J g−1).
3.6. Solid-state thermolysis
Bulk thermolysis of compounds 2a and 4 at 800 °C for 24 h in air results in highly crystalline products 2-800 °C and 4-800 °C, respectively. The powder XRD plots of 2a-800 °C and 4-800 °C are identical, indicating that thermolysis of 2a and 4 gives rise to the same ceramic metal phosphate product (Fig. 7a). The observed powder XRD patterns do not match with any of the earlier reported zinc phosphate or pyrophosphate phases. However, monoalkyl phosphate-based metal complexes are known to undergo thermal decomposition to form a metal pyrophosphate product.26,27 ICP-AES reveals the ratio of Zn and P in 2a-800 °C and 4-800 °C to be 1
:
0.915 and 1
:
1.32, respectively, consistent with the stoichiometric range for zinc pyrophosphate.
 |
| Fig. 7 (a) Powder XRD patterns of bulk thermolysis products 2a-800 °C and 4-800 °C recorded upon heating 2a and 4 at 800 °C for 24 h showing the formation of a new phase of zinc phosphate. (b) Raman spectra of 2a-800 °C and 4-800 °C (632 nm laser) showing the presence of residual carbon in 2a-800 °C. | |
The infrared spectra of 2a-800 °C and 4-800 °C show similar profiles, with absorption bands characteristic of Zn2P2O7 (Fig. S18†).69,70 The FT-IR absorption bands at 1180, 1126 and 1075 cm−1 correspond to the asymmetric stretching of the PO32− unit (νas(PO32−)), whereas the absorption bands at 1043 and 1010 cm−1 are assigned to its symmetric stretching (νs(PO32−)). The absorption bands appearing at 951 cm−1 (νas(P–O–P)) and 754 cm−1 (νs(P–O–P)) signifies the presence of the P–O–P bond. The band appearing at 540 cm−1 is assigned to the O–P–O bending vibration (δ(P–O)) of the P2O72− unit.69,70 The Raman spectra of 2a-800 °C and 4-800 °C further complement the formation of the pyrophosphate phase. The Raman peaks at 1180 cm−1 and 1137 cm−1 correspond to νas(PO32−), while peaks at 1069 and 1005 cm−1 are attributed to νs(PO3) (Fig. 7b). The peak observed at 950 cm−1 corresponds to νas(P–O–P) stretching, whereas the peak at 777 cm−1 is assigned to νs(P–O–P). Additionally, the peaks at 601 and 367 cm−1 correspond to the O–P–O bending vibration (δ(PO)) of the P2O72− unit.71,72 Furthermore, the additional peaks observed in the Raman spectra at 1340 and 1610 cm−1 correspond to the D and G bands of carbon, indicating the presence of residual carbon.51,73 The intensity of peaks due to carbon in the Raman spectrum for 4-800 °C is less relative to the peak intensity for 2a-800 °C, suggesting a lower residual carbon content in 4 after thermal treatment. The presence of residual carbon in the pyrolyzed products is further confirmed via SEM-EDS analysis (Fig. S19 and S20†). The single-pulse 31P NMR spectra of 2a-800 °C and 4-800 °C show peaks at δ 5.78, δ 1.36 ppm, and at δ 5.75, δ 1.44 ppm, respectively, indicating the presence of two non-equivalent phosphate centres in the structure (Fig. S21†).
3.7. Contact angle measurements
Corrosion protection materials are coated with functional groups bearing alkyl chains, owing to their hydrophobic nature.52,74,75 The hydrophobicity of alkyl chains prevents the interaction of water molecules with metal surfaces and hence protects them from corrosion.76 Since the structures of 2a and 4 feature alkyl chains, they are expected to show hydrophobic behaviour; hence, contact angle measurements were conducted to examine the surface interaction of 2a and 4 with water droplets. Pellets of 2a and 4 were made by using a hydraulic press and subjected to static contact angle measurements, resulting in observed angles of 100.5° (±0.2) for 2a and 98.8° (±0.2) for 4 (Table 2). These values indicate hydrophobicity and suggest that, although the coordination polymer is hydrated, the surface is enriched with alkyl chains that either extend outward or are oriented near the interface. This surface composition effectively imparts hydrophobic character to the material by minimizing water–surface interactions. These studies imply that 2a and 4 could serve as effective hydrophobic coating materials.77
Table 2 Contact angles of 2a and 4
Sample |
Image |
Contact angle (°) |
2a
|
|
100.5 (±0.2) |
4
|
|
98.8 (±0.2) |
4. Conclusions
Zinc phosphate coordination polymers [(RO)PO3Zn(DMF)]n (R = n-octyl (1) and n-hexyl (3)) and [(RO)PO3Zn(H2O)]n (R = n-octyl (2a) and n-hexyl (4)) have been synthesized by respective facile reactions between zinc nitrate hexahydrate and n-octyl phosphate and n-hexyl phosphate by mixing the reagents. Single-crystal X-ray diffraction studies of 1 and 3 show the formation of 1D railroad-type or tape-like polymeric structures. These 1D polymeric chains arrange themselves to form arrays having interdigitated alkyl chains with an inter-polymer distance of 15.3 Å and 13.4 Å for 1 and 3, respectively. Interestingly, DMF-coordinated polymers 1 and 3 undergo a facile transformation where the DMF molecules are exchanged with water molecules, leading to the formation of 2a and 4, respectively. Powder XRD studies of 2a and 4 indicate the formation of 2D layered structures with interlayer distances of 23.8 Å and 19.6 Å for 2a and 4, respectively, indicating structural expansion as a result of DMF–water exchange. The flexible nature of long alkyl chains in 2a (d = 23.8 Å) leads to the contraction of interlayer spacing over time to form 2b (d = 21.6 Å). The presence of structural transformations at lower temperatures has been confirmed by DSC studies. Thermal decomposition studies reveal that 2a and 4 transition to an amorphous phase at 300 °C, which then transforms to a crystalline phase having an approximate Zn to P ratio of 1
:
1 at 800 °C. Furthermore, contact angle measurements indicate the hydrophobic nature of 2D layered zinc alkyl phosphates.
In conclusion, this work highlights the role of alkyl chains and solvent coordination for shaping the layered structures. The transformation from 1D to 2D structures upon replacement of coordinated DMF with water demonstrates the role of solvent molecules in directing the dimensionality of the framework assembly. Thermal and contact angle studies reveal the utility of zinc alkyl phosphates as single-source precursors for ceramic phosphates and hydrophobic materials, underscoring the potential of these systems in designing functional materials with tailored structural properties.
Conflicts of interest
The authors declare no conflict of interest.
Data availability
The data supporting this article have been included as part of the ESI.† Crystallographic data have been deposited at the CCDC under deposition numbers 2350478 (for 1) and 2350479 (for 3).†
Acknowledgements
This work was supported by SERB, New Delhi (CRG/2022/002406 & SB/S2/JCB-85/2014). Harsha Arya acknowledges CSIR, New Delhi, for the award of a fellowship. The authors thank the Sophisticated Analytical Instrument Facility (SAIF) at IIT Bombay and the IoE-funded central facilities (IOE funding) for providing access to equipment used in this work.
References
- Y. He, X. Shen and Y. Zhang, ACS Appl. Nano Mater., 2024, 7, 27907–27939 CrossRef CAS.
- L. Peng, Y. Zhu, D. Chen, R. S. Ruoff and G. Yu, Adv. Energy Mater., 2016, 6, 1600025 CrossRef.
- H. Liao, Y. Jiang, X. Wei, X. Zhao, W. Lai, N. An, Y. Ma, S. Dai and Z. Hou, ACS Sustainable Chem. Eng., 2024, 12, 2632–2645 CrossRef CAS.
- S. Yadav, J. Das, S. P. Chaurasia, L. Singh and P. Rekha, Chem. Eng. Sci., 2024, 285, 119628 CrossRef CAS.
- T. Dutta, N. Yadav, Y. Wu, G. J. Cheng, X. Liang, S. Ramakrishna, A. Sbai, R. Gupta, A. Mondal and Z. Hongyu, Nano Mater. Sci., 2024, 6, 1–23 CrossRef CAS.
- J. Zhou, C. Wang, X. Zhang, L. Jiang and R. Wu, Mater. Sci. Eng., R, 2024, 161, 100872 CrossRef.
- M. R. A. Karim, W. Shehzad, K. I. Khan, E. U. Haq and Y. Haroon, J. Electrochem. Sci. Technol., 2024, 15, 321–344 CrossRef.
- R. Lin and Y. Ding, Materials, 2013, 6, 217–243 CrossRef CAS PubMed.
- M. Beiro, A. Collazo, M. Izquierdo, X. Nóvoa and C. Pérez, Prog. Org. Coat., 2003, 46, 97–106 CrossRef CAS.
- J. Juárez-Batalla, A. Meza-Rocha, I. Camarillo and U. Caldiño, Opt. Mater., 2016, 58, 406–411 CrossRef.
- N. Attar, L. E. Tam and D. McComb, J. Prosthet. Dent., 2003, 89, 127–134 CrossRef CAS PubMed.
- P. Pascuta, G. Borodi, A. Popa, V. Dan and E. Culea, Mater. Chem. Phys., 2010, 123, 767–771 CrossRef CAS.
- I. R. Sayed, A. M. Farhan, A. A. AlHammadi, M. I. El-Sayed, I. M. Abd El-Gaied, A. M. El-Sherbeeny, W. Al Zoubi, Y. G. Ko and M. R. Abukhadra, J. Mol. Liq., 2022, 360, 119527 CrossRef CAS.
- J. Li, Z. Zheng, Z. Yu, F. She, L. Lai, J. Prabowo, W. Lv, L. Wei and Y. Chen, J. Mater. Chem. A, 2023, 11, 3051–3059 RSC.
- S. Xia, Q. Luo, J. Liu, X. Yang, J. Lei, J. Shao and X. Tang, Small, 2024, 20, 2310497 CrossRef CAS PubMed.
- Q. Jing, M. Zhu, L. Li, X. Ji, H. Duan, H. Chen and M.-H. Lee, Opt. Mater., 2024, 147, 114620 CrossRef CAS.
- Y. L. Sun, G. X. Liu, Y. L. Lv, L. Ma, W. D. Yao and R. L. Tang, J. Solid State Chem., 2023, 325, 124171 CrossRef CAS.
- S. Vafaei, S. A. Sadat Shandiz and Z. Piravar, Biol. Trace Elem. Res., 2020, 198, 109–117 CrossRef CAS PubMed.
- X. Hu, X. Song, Y. Yuan, X. Yao, X. Chen, G. Li and S. Li, J. Mater. Chem. B, 2023, 11, 6404–6411 RSC.
- P. C. Jhang, N. T. Chuang and S. L. Wang, Angew. Chem., Int. Ed., 2010, 25, 4296–4300 CrossRef.
- Z. Fu, D. Song, Y. Zeng, S. Liao and J. Dai, Dalton Trans., 2012, 41, 10910–10912 RSC.
- K. M. Zhang, X. L. Zhong, X. Y. Zhou, X. T. Kuang and H. R. Zhao, Polyhedron, 2024, 264, 117258 CrossRef CAS.
- S. Neeraj, S. Natarajan and C. Rao, Chem. Mater., 1999, 11, 1390–1395 CrossRef CAS.
- J. Fan and B. E. Hanson, Inorg. Chem., 2005, 44, 6998–7008 CrossRef CAS PubMed.
- J. Vallejo, I. R. Salcedo, R. M. Colodrero, A. Cabeza, A. Świtlicka, J. Cano and M. Viciano-Chumillas, Dalton Trans., 2017, 46, 16570–16579 RSC.
- G. A. Bhat, S. Haldar, S. Verma, D. Chakraborty, R. Vaidhyanathan and R. Murugavel, Angew. Chem., 2019, 131, 17000–17005 CrossRef.
- G. A. Bhat, A. C. Kalita and R. Murugavel, CrystEngComm, 2017, 19, 5390–5401 RSC.
- T. Lis, Acta Crystallogr., Sect. C: Cryst. Struct. Commun., 1994, 50, 181–185 CrossRef.
- Y. Ortiz-Avila, P. R. Rudolf and A. Clearfield, Inorg. Chem., 1989, 28, 2137–2141 CrossRef CAS.
- P. Bissinger, O. Kumberger and A. Schier, Chem. Ber., 1991, 124, 509–513 CrossRef CAS.
- S. Verma and R. Murugavel, Inorg. Chem., 2022, 61, 6807–6818 CrossRef CAS PubMed.
- S. Verma and R. Murugavel, Inorg. Chem., 2020, 59, 13233–13244 CrossRef CAS PubMed.
- R. Murugavel and S. Chaudhary, Chem. – Asian J., 2025, e202401177 Search PubMed.
- R. Pothiraja, M. Sathiyendiran, R. J. Butcher and R. Murugavel, Inorg. Chem., 2004, 43, 7585–7587 CrossRef CAS PubMed.
- R. Murugavel, M. Sathiyendiran and M. G. Walawalkar, Inorg. Chem., 2001, 40, 427–434 CrossRef CAS PubMed.
- M. Sathiyendiran and R. Murugavel, Inorg. Chem., 2002, 41, 6404–6411 CrossRef CAS PubMed.
- R. Pothiraja, M. Sathiyendiran, R. J. Butcher and R. Murugavel, Inorg. Chem., 2005, 44, 6314–6323 CrossRef CAS PubMed.
- C. G. Lugmair, T. D. Tilley and A. L. Rheingold, Chem. Mater., 1997, 9, 339–348 CrossRef CAS.
- C. G. Lugmair, T. D. Tilley and A. L. Rheingold, Chem. Mater., 1999, 11, 1615–1620 CrossRef CAS.
- K. L. Fujdala and T. D. Tilley, J. Am. Chem. Soc., 2001, 123, 10133–10134 CrossRef CAS PubMed.
- K. M. Van Allsburg, E. Anzenberg, W. S. Drisdell, J. Yano and T. D. Tilley, Chem. – Eur. J., 2015, 21, 4646–4654 CrossRef CAS PubMed.
- S. Chaudhary and R. Murugavel, Chem. Mater., 2024, 36, 6475–6488 CrossRef CAS.
- G. A. Bhat, S. Verma, A. Rajendran and R. Murugavel, Inorg. Chem., 2018, 57, 7644–7654 CrossRef CAS PubMed.
- K. Omoto, S. Aoyama, T. Galica, E. Nishibori, S. Katao, K. Yasuhara and G. Rapenne, Dalton Trans., 2022, 51, 17967–17972 RSC.
- T. Minami, H. Sato and S. Matsumoto, CrystEngComm, 2018, 20, 2644–2647 RSC.
- Z. S. Yao, M. Mito, T. Kamachi, Y. Shiota, K. Yoshizawa, N. Azuma, Y. Miyazaki, K. Takahashi, K. Zhang and T. Nakanishi, Nat. Chem., 2014, 6, 1079–1083 CrossRef CAS PubMed.
- S. Q. Su, T. Kamachi, Z. S. Yao, Y. G. Huang, Y. Shiota, K. Yoshizawa, N. Azuma, Y. Miyazaki, M. Nakano and G. Maruta, Nat. Commun., 2015, 6, 8810 CrossRef PubMed.
- S. H. Kang, Y. J. Jin and G. Kwak, ACS Appl. Polym. Mater., 2020, 2, 2987–2993 CrossRef CAS.
- S. Hayami, K. Kato, Y. Komatsu, A. Fuyuhiro and M. Ohba, Dalton Trans., 2011, 40, 2167–2169 RSC.
- S. Hayami, R. Moriyama, A. Shuto, Y. Maeda, K. Ohta and K. Inoue, Inorg. Chem., 2007, 46, 7692–7694 CrossRef CAS PubMed.
- N. Matharoo, M. G. Walawalkar and R. Murugavel, Dalton Trans., 2023, 52, 2412–2423 RSC.
- X. Gao, S. Liu, H. Lu, F. Gao and H. Ma, Ind. Eng. Chem. Res., 2015, 54, 1941–1952 CrossRef CAS.
-
CrysAlisPRO, Oxford Diffraction/Agilent Technol. UK Ltd, Yarnton, Oxford, UK Search PubMed.
- G. M. Sheldrick, Acta Crystallogr., Sect. C: Struct. Chem., 2015, 71, 3–8 Search PubMed.
- O. V. Dolomanov, L. J. Bourhis, R. J. Gildea, J. A. K. Howard and H. Puschmann, J. Appl. Crystallogr., 2009, 42, 339–341 CrossRef CAS.
-
M. Llunell, D. Casanova, J. Cirera, P. Alemany and S. Alvarez, SHAPE (Version 2.1), Universitat de Barcelona, Barcelona, 2013 Search PubMed.
- G. A. Bhat and R. Murugavel, J. Chem. Sci., 2020, 132, 1–9 CrossRef.
- R. A. Coxall, S. G. Harris, D. K. Henderson, S. Parsons, P. A. Tasker and R. E. Winpenny, J. Chem. Soc., Dalton Trans., 2000, 2349–2356 RSC.
- G. Cao, V. M. Lynch, J. S. Swinnea and T. E. Mallouk, Inorg. Chem., 1990, 29, 2112–2117 CrossRef CAS.
- H. Tanaka, T. Watanabe, M. Chikazawa, K. Kandori and T. Ishikawa, Colloids Surf., A, 1998, 139, 341–349 CrossRef.
- H. Tanaka and M. Chikazawa, J. Mater. Chem., 1999, 9, 2923–2927 RSC.
- H. Tanaka, K. Masuda and R. Hino, J. Colloid Interface Sci., 2002, 254, 331–337 CrossRef CAS PubMed.
- G. Cao, H. Lee, V. M. Lynch and T. E. Mallouk, Solid State Ionics, 1988, 26, 63–69 CrossRef CAS.
- G. Cao, H. Lee, V. M. Lynch and T. E. Mallouk, Inorg. Chem., 1988, 27, 2781–2785 CrossRef CAS.
- A. Kondo, T. Nakagawa, H. Kajiro, A. Chinen, Y. Hattori, F. Okino, T. Ohba, K. Kaneko and H. Kanoh, Inorg. Chem., 2010, 49, 9247–9252 CrossRef CAS PubMed.
- G. Cao and T. E. Mallouk, Inorg. Chem., 1991, 30, 1434–1438 CrossRef CAS.
- Y. Zhang, K. J. Scott and A. Clearfield, J. Mater. Chem., 1995, 5, 315–318 RSC.
- R. Murugavel, Emergent Mater., 2019, 2, 273–294 CrossRef CAS.
- M. Crobu, A. Rossi, F. Mangolini and N. D. Spencer, Anal. Bioanal. Chem., 2012, 403, 1415–1432 CrossRef CAS PubMed.
- L. Popović, D. De Waal and J. Boeyens, J. Raman Spectrosc., 2005, 36, 2–11 CrossRef.
- G. Stranford, R. Condrate Sr and B. C. Cornilsen, J. Mol. Struct., 1981, 73, 231–234 CrossRef CAS.
- B. Wang, Y. Duan, M. Wei, J. Guo, M. Chao, Q. Gao, Y. Gao, Z. Li, J. Xie and E. Liang, Results Phys., 2024, 61, 107785 CrossRef.
- M. Pimenta, G. Dresselhaus, M. S. Dresselhaus, L. Cancado, A. Jorio and R. Saito, Phys. Chem. Chem. Phys., 2007, 9, 1276–1290 RSC.
- C. C. Pan, X. Z. Wang, Y. Behnamian, Z. Wu, Z. B. Qin, D. H. Xia and W. B. Hu, J. Electrochem. Soc., 2020, 167, 161510 CrossRef CAS.
- C. Zhao, X. Gao, H. Lu, R. Yan, C. Wang and H. Ma, RSC Adv., 2015, 5, 54420–54432 RSC.
- C. Verma, M. Quraishi and K. Rhee, Adv. Colloid Interface Sci., 2022, 306, 102723 CrossRef CAS PubMed.
- S. Ananthapadmanabhan, T. K. Rout, S. Chatterjee, T. Dasgupta and S. Parida, ACS Appl. Mater. Interfaces, 2023, 15, 51737–51752 CrossRef CAS PubMed.
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