§ Current address: Laboratoire de Physique et Chimie des Nano-Objets, Institut National des Sciences Appliquées, 135 avenue de Rangueil, 31077 Toulouse Cedex 4, France
Associate Editor: S. A. Claridge
Beilstein J. Nanotechnol. 2018, 9, 2775–2787. https://doi.org/10.3762/bjnano.9.259
Received 15 Aug 2018, Accepted 11 Oct 2018, Published 30 Oct 2018
The synthesis and characterization of six new lanthanide networks [Ln(L)(ox)(H2O)] with Ln = Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+ is reported. They were synthesized by solvo-ionothermal reaction of lanthanide nitrate Ln(NO3)3·xH2O with the 1,3-bis(carboxymethyl)imidazolium [HL] ligand and oxalic acid (H2ox) in a water/ethanol solution. The crystal structure of these compounds has been solved on single crystals and the magnetic and luminescent properties have been investigated relying on intrinsic properties of the lanthanide ions. The synthetic strategy has been extended to mixed lanthanide networks leading to four isostructural networks of formula [Tb1−xEux(L)(ox)(H2O)] with x = 0.01, 0.03, 0.05 and 0.10. These materials were assessed as luminescent ratiometric thermometers based on the emission intensities of ligand, Tb3+ and Eu3+. The best sensitivities were obtained using the ratio between the emission intensities of Eu3+ (5D0→7F2 transition) and of the ligand as the thermometric parameter. [Tb0.97Eu0.03(L)(ox)(H2O)] was found to be one of the best thermometers among lanthanide-bearing coordination polymers and metal-organic frameworks, operative in the physiological range with a maximum sensitivity of 1.38%·K−1 at 340 K.
Keywords: coordination network; imidazolium salt; lanthanides; magnetism; thermometry
Metal-organic coordination networks have been the subject of considerable research in the last years as evidenced by the increasing number of papers published in the field . Indeed, the possibility of combining different properties by judicious choice of the organic and inorganic moieties makes these systems good candidates for the elaboration of (multi)functional architectures [2,3]. Among the various functionalities that can be envisioned for this class of hybrid compounds, the elaboration of luminescent networks is interesting in term of potential applications in lighting, display, sensing, biomedicine and for optical devices [4-12].
Luminescent coordination networks can be obtained either by the use of specific luminescent organic ligands or by the use of main-group elements, d10 transition metals or of trivalent lanthanide ions for the inorganic moiety [13,14]. The luminescent properties of the trivalent lanthanide ions are particularly interesting since they cover a large range of emission from the ultraviolet (Gd3+) to near-infrared (Pr3+, Nd3+, Ho3+, Er3+, Yb3+) through the visible domain (Pr3+, Sm3+, Eu3+, Tb3+, Dy3+, Tm3+). It confers to lanthanide-based networks a large tunability of emission properties, which is very useful for the elaboration of light-emitting devices or for biomedical applications . Moreover, due to the narrowness and the hypersensitivity of their transitions, lanthanide-based networks can also find utility for the sensing of gases, vapors or small molecules [9,16]. In the case of mixed lanthanide coordination networks, the luminescent properties can be used to synthesize temperature probes with possible applications in the aerospace area, safety and health [17,18].
Beside luminescent properties, lanthanide ions exhibit large magnetic moment and strong magnetic anisotropy, which might have potential applications of lanthanide-based networks in information storage, quantum computing and spintronics [19-23].
Most of these lanthanide-based networks are obtained with neutral organic ligands such as benzene-1,4-dicarboxylate (1,4-bdc) , benzene-1,3,5-tricarboxylate (TMA) , pyridine-2,5-dicarboxylate (2,5-H2pdc)  or 1H-2-propyl-4,5-imidazoledicarboxylate (pimda) . Only few examples of lanthanide-based networks obtained with charged ligands are reported in the literature [27-30]. Following this last point, we have chosen to synthesize lanthanide-based networks from positively charged imidazolium dicarboxylate salts [31-34]. Contrarily to the classical imidazolium salts or ionic liquids used in ionothermal syntheses [35-40], the functionalization of imidazolium moieties with coordinating functions reduces the influence of the imidazolium salt on the ligand for a better rationalization of the synthesis [31-34].
We report in this paper the synthesis and the characterization of six new networks obtained from an imidazolium dicarboxylate salt, oxalic acid and lanthanide ions. The structure of these networks has been solved by single crystal X-ray diffraction and their physical properties (magnetism and luminescence) have been investigated. We establish that these networks show antiferromagnetic interactions. The study of the luminescent properties evidences the presence of well-defined transitions characteristic for the considered lanthanide. These results have prompted us to extend our strategy to the synthesis of mixed lanthanide networks with four different ratios Tb3+/Eu3+. The powder X-ray diffraction analysis indicates that these mixed lanthanide networks are isostructural to the parent homolanthanide compounds. The temperature-resolved photo-luminescent properties of the latter indicate possible applications in thermometry.
The 1,3-bis(carboxymethyl-)-imidazolium ligand [HL] was synthesized according to protocols published in the literature [41,42].
Single crystals and homogeneous powders of [Ln(L)(ox)(H2O)] were obtained with Ln = Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+ by reacting a water/ethanol solution of the lanthanide nitrate and oxalic acid (H2ox) with [HL]. The mixture was sealed in a Teflon-lined stainless steel autoclave and heated at 393 K for 72 h. After cooling to room temperature, the autoclaves were opened and crystals were filtered and washed with ethanol. The yields of the reactions range from 36 to 59 %. Similar reactions were carried out with Nd3+ and Sm3+ ions leading to different structures . In addition, in the case of Nd3+ and Sm3+, various crystalline compounds were obtained depending on whether oxalic acid was added or not. When oxalic acid was not added in situ formation of the oxalate ligand has been observed. The peculiar behavior of these two ions compared to others can be explained by their place in the first part of the lanthanide series . In the case of Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+, described in the present work, the direct reaction between lanthanide nitrate and [HL], without addition of oxalic acid, did not give crystalline compounds.
Single crystal X-ray analysis of the [Ln(L)(ox)(H2O)] compounds with Ln = Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+ reveal that the six compounds are isostructural. All compounds are obtained as colorless crystals and crystallize in the monoclinic space group P21/a (no. 14). Crystal data for these series of compounds are collected in Table 1 and Table 2.
Table 1: Crystallographic data for [Ln(L)(ox)(H2O)] compounds with Ln = Eu3+, Gd3+ and Tb3+.a
|molar mass [g·mol−1]||441.14||446.43||448.10|
|μ (Mo Kα) [mm−1]||5.044||5.366||5.716|
|R1, wR2 [I > 2σ(I)]||0.0358, 0.0690||0.0268, 0.0458||0.0427, 0.0769|
|R1, wR2 [all data]||0.0579, 0.0770||0.0430, 0.0501||0.0627, 0.0850|
|largest diff. peak and hole (e·Å−3)||1.297, −1.365||0.681, −0.689||1.868, −1.838|
aThe relatively high values of the residual density can be explained by the difficulty to isolate single crystals. Indeed SEM images reveal the presence of relatively small and entangled crystals (see Figure S3, Supporting Information File 1).
Table 2: Crystallographic data for [Ln(L)(ox)(H2O)] compounds with Ln = Dy3+, Ho3+ and Yb3+.a
|molar mass [g·mol−1]||451.68||454.11||462.22|
|μ (Mo Kα) [mm−1]||6.137||6.479||7.843|
|R1, wR2 [I > 2σ(I)]||0.0336, 0.0573||0.0494, 0.0751||0.0516, 0.1119|
|R1, wR2 [all data]||0.0517, 0.0624||0.0854, 0.0840||0.0914, 0.1319|
|largest diff. peak and hole (e·Å−3)||0.742, −1.382||1.164, −1.034||2.751, −2.662|
aThe relatively high values of the residual density can be explained by the difficulty to isolate single crystals. Indeed SEM images reveal the presence of relatively small and entangled crystals (see Figure S3, Supporting Information File 1).
The asymmetric unit contains one Ln3+ ion, one [L]− ligand, two half-oxalate ligands and one coordinating water molecule (Figure 1). Ln3+ ions are surrounded by nine oxygens with four oxygen atoms coming from one and same carboxylate function of two different [L]− ligands, one from the water molecule and four from two different oxalate ligands. The coordination environment of Ln3+ ions is a tricapped trigonal prism (Figure S1, Supporting Information File 1) with Ln–O distances similar to those observed in structurally related compounds [44,45]. These distances decrease progressively with the size of the lanthanide ion in agreement with the lanthanide contraction effect (Table S1, Supporting Information File 1). The same tendency is observed with the shortest Ln–Ln distances, which correspond to two Ln3+ ions connected by an oxalate ligand (Table S1, Supporting Information File 1).
Two separate Ln3+ ions are connected through an oxalate ligand in a bis-bidentate bridging coordination mode forming undulating chains along the a-axis (Figure 2). The Ln3+ ions are connected to the carboxylate functions of the [L]− ligand in a bidentate chelate mode. The cohesion between these chains is realized through H bonding between H atoms of the coordinated water molecules and O atoms of the carboxylate functions.
Beside the single crystal analysis, the homogeneity of the six samples was checked by powder X-ray diffraction. As shown in Figure S2 (Supporting Information File 1), the experimental powder patterns fit well with the patterns calculated from the single crystal structure and show no additional phases.
In order to investigate the thermal stability, thermogravimetric analysis (TGA) was realized under air stream from 25 to 900 °C (Figure S4, Supporting Information File 1). The weight loss corresponding to the elimination of the coordinated water molecule occurs between 130 and 310 °C (step 1). The second weight loss between 310 and 750 °C (step 2) is associated to the combustion of the organic moieties (oxalate and [L]− ligands), concomitant with the formation of oxide (Ln2O3 was identified by powder X-ray diffraction in the final product). The total weight loss is in good agreement with the calculated values (Table S2, Supporting Information File 1).
The infrared spectra of the six compounds are similar (Figure S5, Supporting Information File 1). The broad band around 3250 cm−1 and the one at 1672 cm−1 are ascribed to the coordinated water (stretching and bending vibration modes, respectively). The vibration bands of the aromatic and aliphatic C–H bonds are observed in the range 3150–3050 cm−1 and 3050–2950 cm−1, respectively. The characteristic frequencies of the coordinating carboxylate functions are observed at 1627 and 1571 cm−1 (antisymmetric vibration bands) and at 1411 and 1431 cm−1 (symmetric vibration bands). It leads to Δν (Δν = νantisym − νsym) equal to 216 and 140 cm−1 in agreement with a bis-bidentate bridging coordination mode of the oxalate ligand and a bidentate chelate coordination mode of the carboxylate functions of the [L]− ligand, respectively [46,47].
The magnetic behavior of the six compounds [Ln(L)(ox)(H2O)] have been studied in the temperature range of 1.8–300 K under a 0.5 T dc magnetic field. The magnetic susceptibilities and products χT are presented as functions of the temperature in Figure 3.
At 300 K, the value of χT for the compound [Gd(L)(ox)(H2O)] is 7.88 emu·K·mol−1, which agrees well with the theoretical value for spin-only S = 7/2 Gd3+ ions. The χT product remains almost constant above 30 K and then decreases down to 6.7 emu·K·mol−1 at 1.8 K. This decrease suggests the occurrence of antiferromagnetic coupling between neighboring gadolinium centers. Since [Gd(L)(ox)(H2O)] is constituted of linear chains of Gd3+ ions with large spin moment, S = 7/2, we evaluated the magnetic coupling, J, between neighboring Gd3+ ions by using the Fisher expression for classical spin chains [48,49]:
In the above expression, N is the Avogadro number, g is the Landé factor, β is the Bohr magneton, k is the Boltzmann constant, S is the spin moment, J is the magnetic coupling constant and T is the temperature. The simultaneous fitting of the susceptibility and the χT product with the Fischer expression above lead to refined values of g = 2.00(1) and J = −0.026 cm−1. The g value was left free during fitting and is in line with the tabulated g values for Gd ions . The absolute value and the sign of J support the presence of weak antiferromagnetic interactions in [Gd(L)(ox)(H2O)], in agreement with results reported in previous works [51-53]. The magnetic exchange coupling between lanthanide ions is usually weak, due to limited extension of the 4f orbitals.
For [Eu(L)(ox)(H2O)], the χT product decreases continuously from 1.4 emu·K·mol−1 at 300 K to 0 emu·K·mol−1 at 1.8 K. This behavior is typical for Eu3+ ions for which the 7F ground term is split in seven 7FJ (0 ≤ J ≤ 6) states because of spin–orbit coupling [54,55]. The spin–orbit coupling constant, λ, can be evaluated considering isotropic isolated Eu3+ ions parametrized with the appropriate expression (E1 in Supporting Information File 1) for the isotropic susceptibility of Eu3+ ions [54,55].
A very good fit of the experimental susceptibility and the χT product of [Eu(L)(ox)(H2O)] was obtained above 25 K giving the refined value of λ = 309.00(4) cm−1. This value is consistent with the value determined from the luminescence measurements (see below) and confirms that considering only the isotropic component of the susceptibility is a good approximation to analyze the magnetic data .
The behavior of [Tb(L)(ox)(H2O)] is also typical for quasi-isolated Tb3+ ions with χT = 11.75 emu·K·mol−1 at 300 K (expected value: 11.82 emu·K·mol−1 with g = 1.5) [48,50]. When decreasing the temperature, the χT product remains constant until 100 K and then decreases to 4.50 emu·K·mol−1 at 1.8 K. This decay is due to the depopulation of the low-lying J states arising from the splitting of the 7F ground term under spin–orbit coupling. In order to determine the spin–orbit coupling, λ, it was necessary to take into account an antiferromagnetic interaction between neighboring Tb3+ ions using a mean-field approach, in addition to the intrinsic behavior of isolated Tb3+ ions (E5 in Supporting Information File 1) .
Subsequently, a good fit of the magnetic data was obtained on the whole temperature range with λ = −303(75) cm−1 and zJ′ = −0.106(1) cm−1. The obtained λ value is consistent with other values reported in the literature for compounds containing isolated Tb3+ ions [57,58].
In the case of [Dy(L)(ox)(H2O)], [Ho(L)(ox)(H2O)] and [Yb(L)(ox)(H2O)] the χT values at 300 K are 13.82, 13.61 and 2.48 emu·K·mol−1, in line with the theoretical values for isolated Dy3+ ions (14.17 emu·K·mol−1 with g = 1.33)  Ho3+ ions (14.07 emu·K·mol−1 with g = 1.25) [50,59], and Yb3+ ions (theoretical value of 2.57 emu·K·mol−1 with g = 1.14) [48,50]. Upon cooling, the χT product of [Dy(L)(ox)(H2O)] remains nearly constant until 170 K and then decreases to 9.90 emu·K·mol−1 at 1.8 K. For the Ho analogue [Ho(L)(ox)(H2O)], the χT product decreases slowly between 300 and 100 K, and a steeper decrease is observed from 13.67 emu·K·mol−1 at 100 K to 2 emu·K·mol−1 at 1.8 K. Finally, for the Yb analogue [Yb(L)(ox)(H2O)], the χT product decreases slowly as the temperature decreases to reach 1.61 emu·K·mol−1 at 1.8 K. This behavior is ascribed to the depopulation of the low lying states (mJ states) arising from the 6H5/2 (Dy3+), 5I8 (Ho3+) and 2F7/2 (Yb3+), ground states split through the action of the crystal field (for these ions, the ground state is well below the first excited J state). Using the free-ion approach and the isotropic (z) component of the susceptibility, the value of the zero-field splitting (ZFS), Δ, was evaluated for each ion using the expressions E2, E3 and E4 in Supporting Information File 1, leading to Δ = 0.169(3), 0.284(4) and 3.25(1) cm−1 for Dy, Ho and Yb, respectively. These values are in the range of those reported in the literature . It can be noticed that the introduction of a zJ′ term to fit the magnetic curves down to low temperatures for [Dy(L)(ox)(H2O)], [Ho(L)(ox)(H2O)] and [Yb(L)(ox)(H2O)] compounds did not lead to better results.
The excitation spectra of [Gd(L)(ox)(H2O)], [Eu(L)(ox)(H2O)] and [Tb(L)(ox)(H2O)] were recorded at room temperature (ca. 297 K) and 12 K monitoring the ligand emission at 520 nm, and the strongest Eu3+ 5D0→7F2 and Tb3+ 5D4→7F5 transitions (Figure 4). The [Gd(L)(ox)(H2O)] excitation spectra consist of three distinct broad UV bands, ranging from 230 to 400 nm, attributed to the S0→S3,2,1 excited transitions of the organic ligand. For [Eu(L)(ox)(H2O)], these ligand transitions are partially superimposed with the intra-4f6 7F0,1→5D1-4, 5L6, 5G2-6, 5H3-7 and 5F1-5 transitions of Eu3+, which dominate the corresponding excitation spectra. Finally, the [Tb(L)(ox)(H2O)] excitation spectra feature a strong and broad UV band ranging from 220 to ca. 300 nm, with a maximum at 267 nm, which has no counterpart in the [Gd(L)(ox)(H2O)] excitation spectra. Thus, this band is attributed to the inter-configurational spin-forbiden 4f8→4f75d1 transition of Tb3+ because its energy is similar to the energy reported for layered Tb3+ silicates . The additional sharp lines in the spectra of [Tb(L)(ox)(H2O)] are ascribed to the intra-4f8 7F6→5D2-4, 5GJ and 5H7 transitions of Tb3+. Although with a lower relevance, the excited states of the ligands also contribute to the entire excitation spectra of Tb3+, as shown below.
The emission spectra of [Gd(L)(ox)(H2O)], [Eu(L)(ox)(H2O)] and [Tb(L)(ox)(H2O)] recorded at 297 K and 12 K are given in Figure 5. [Gd(L)(ox)(H2O)] displays two broad bands from 390 to ca. 650 nm attributed to the S1→S0 (peaking at ca. 415 nm) fluorescence and T1→S0 (peaking at 503 nm) ligand phosphorescence. This assignment is supported by the time-resolved emission spectra recorded at 12 K excited at 350 nm (Figure S6, Supporting Information File 1), which demonstrates a much faster time dependence of the S1→S0 transition compared to the transition T1→S0. Under 364 nm excitation, a relative minimum for the Eu3+ and Tb3+ auto-absorption, [Eu(L)(ox)(H2O)] and [Tb(L)(ox)(H2O)] show mainly the typical sharp Eu3+ and Tb3+ emission lines assigned to the 5D0→7F0-4 and 5D4→7F6-0 transitions, respectively. In addition, both compounds also exhibit a broad band from 400 to ca. 550 nm, particularly weak in the case of the former, attributed to the S1→S0 transition of the ligand. Accordingly, as exemplified in Figure S7 (Supporting Information File 1) with the [Tb(L)(ox)(H2O)] time-resolved 12 K emission spectra, the broad band has a very fast time dependence totally suppressed by a time delay of only 0.05 ms. The suppression of the low-energy T1→S0 ligand emission denotes an energy transfer from the triplet excited state to the Eu3+ and Tb3+ excited levels. This energy transfer is more effective for the Eu3+ compound, which almost suppresses also the S1→S0 emission. Under excitation at their corresponding maxima, 270 and 395 nm for Tb3+ and Eu3+, respectively, both [Eu(L)(ox)(H2O)] and [Tb(L)(ox)(H2O)] show only the respective sharp emission lines (Figure S8; Supporting Information File 1).
The emission of Eu3+ is highly sensitive to slight changes in the first coordination sphere of the metal, and because of this it is widely used as a local probe . For [Eu(L)(ox)(H2O)], the emission spectra recorded at 297 K and 12 K show i) a single 5D0→7F0 transition and a local-field splitting of the 7F1,2 levels into three and five Stark components, respectively; ii) and the predominance of the 5D0→7F2 transition relatively to the 5D0→7F1 one, witnessing the presence of a single low-symmetry Eu3+ environment, in accordance with the crystal structure. Additionally, the room-temperature Eu3+ 5D0 and Tb3+ 5D4 decay curves were well fitted by single exponential functions, yielding lifetimes of 0.60 ± 0.01 and 0.98 ± 0.01 ms for [Eu(L)(ox)(H2O)] and [Tb(L)(ox)(H2O)], respectively (Figure S9, Supporting Information File 1), corroborating the presence of a unique Ln3+ crystallographic site.
Consideration of these luminescence results prompted the study of isostructural mixed lanthanide networks. In particular, our interest was focused on networks bearing Tb3+ and Eu3+ in view of their potential application in optical thermometry [17,62]. Accordingly, four Tb3+/Eu3+ mixed lanthanide networks of formula [Tb1−xEux(L)(ox)(H2O)] with x = 0.01, 0.03, 0.05 and 0.10 have been synthesized using the same protocol but varying the molar ratio of Tb(NO3)3·6H2O and Eu(NO3)3·6H2O. As expected, these mixed lanthanide networks are isostructural with the parent compound [Ln(L)(ox)(H2O)] (Figure S10, Supporting Information File 1) and show the presence of Tb and Eu in the expected ratio and homogeneously distributed in the crystals (Figure S11, Supporting Information File 1).
Consider the emission spectra of the four Tb3+/Eu3+ mixed lanthanide networks measured at room temperature (Figure S12, Supporting Information File 1). To maximize the relative poor ligand emission, 364 nm excitation was used since it corresponds to a maximum of the ligand excitation and to relative minima of both Eu3+ and Tb3+ auto-absorptions, as demonstrated by the selective 12 K excitation spectra of [Tb0.90Eu0.10(L)(ox)(H2O)] (Figure S13, Supporting Information File 1). The room-temperature emission spectra of [Tb0.90Eu0.10(L)(ox)(H2O)] under ambient pressure and after exposure to high vacuum (5 × 10−3 mbar, Figure S14, Supporting Information File 1) demonstrates the good stability of the emission of the sample against UV irradiation and pressure change.
Among the four mixed Tb3+/Eu3+ mixed lanthanide networks, [Tb0.97Eu0.03(L)(ox)(H2O)] presents at room temperature the best balance between the emissions of ligand, Tb3+ and Eu3+. Based on the integrated areas of the ligand (IL), Tb3+ 5D4→7F5 (ITb) and Eu3+ 5D0→7F2 (IEu) emissions, three distinct thermometric parameters may be defined, Δ1 = ITb/IEu, Δ2 = ITb/IL and Δ3 = IEu/IL, allowing for the conversion of the emission intensities into absolute temperature values. The temperature dependence of the [Tb0.97Eu0.03(L)(ox)(H2O)] emission in the range of 250–340 K is presented in Figure 6a. Four consecutive emission spectra were collected for each temperature and used to determine the average thermometric parameter, with the errors calculated from the corresponding standard deviation (95% confidence). IL, ITb and IEu were determined by integrating the emission spectra in the ranges of 392–478 nm, 536–556 and 606–630 nm, respectively. Figure 6b depicts the temperature dependence of the three integrated emissions. The emission of the ligand decreases by 58% from 250 to 340 K, the Tb3+ and Eu3+ emissions decrease by 31% and by 20%, respectively.
The temperature dependence of the thermometric parameters Δ1, Δ2 and Δ3 in the range of 250–340 K is shown in Figure 7a. The corresponding relative sensitivity, defined as Sr = |∂Δ/∂T|/Δ , a figure of merit used to compare the performance of ratiometric luminescent thermometers, is plotted in Figure 7b. Δ2 and Δ3 exhibit very good sensitivities in the range of 250–340 K with maximum relative sensitivities, Sm, of 1.14% and 1.38%·K−1 at 340 K, respectively. For Δ1, Sm is only 0.18%·K−1. The Sr values obtained for Δ3, in particular, are among the highest reported for metal-organic frameworks or MOF-based luminescent thermometers operative in the physiological range. Indeed, to the best of our knowledge, only eight such visible luminescent ratiometric LnMOF thermometers have been reported [64-71], among which two outperform our material [Tb0.97Eu0.03(L)(ox)(H2O)]: Tb0.995Eu0.005@In(OH)(2,2′-bipyridine-5,5′-dicarboxylate) with Sm = 4.47%·K−1 at 333 K  and Eu@UiO-(2,2′-bipyridine-5,5′-dicarboxylate) with Sm = 2.19%·K−1 at 293 K  (value recalculated and corrected using the published calibration curve). Two other thermometers have a performance similar to ours, Eu0.089Tb0.9911[2,6-di(2′,4′-dicarboxylphenyl)pyridine] with Sm = 1.39%·K−1 at 328 K  and [(Eu0.231Tb0.769(adipate)0.5(phthalate)(H2O)2] with Sm = 1.21%·K−1 at 303 K . These systems are, thus, appealing for potential application as biological sensors [63,72]. The Tb3+-to-Eu3+ energy transfer plays an important role in the higher sensitivity of Δ3 (IEu/IL). On the one hand, the Tb3+ lifetimes obtained for [Tb0.97Eu0.03(L)(ox)(H2O)] from single exponential functions (Figure S15, Supporting Information File 1) decrease from 0.98 ± 0.01 ms obtained for the Tb3+-only sample at 297 K to 0.62 ± 0.01 ms (250 K) and 0.57 ± 0.01 ms (340 K). On the other hand, the Eu3+ lifetimes for the mixed compound (Figure S15, Supporting Information File 1), 0.86 ± 0.02 ms (250 K) and 0.78 ± 0.01 ms (340 K), increases relatively to the one obtained at 297 K for the Eu3+-only compound (0.60 ± 0.01 ms). In addition, the Eu3+ decay curves also exhibit a rise, to 0.81 ± 0.08 ms (250 K) and 0.93±0.06 ms (340 K), most probably originating from the population of the Eu3+ 5D0 emitting level trough the Tb3+ 5D4 donor level.
Six novel coordination networks based on an imidazolium dicarboxylate 1,3-(biscarboxymethyl)imidazolium and Ln3+ ions (Ln = Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+) in the presence of oxalate have been obtained by solvothermal reaction and totally characterized. These coordination networks are isostructural and present a monoclinic structure (space group P21/a). They exhibit magnetic and luminescent properties that are characteristic for the considered lanthanide ions (except for compounds based on Gd3+ ions). The possibility to obtain Tb3+/Eu3+ mixed lanthanide networks has been exploited for potential application in thermometry. Accordingly, four mixed lanthanide networks [Tb1−xEux(L)(ox)(H2O)] (x = 0.01, 0.03, 0.05 and 0.10) were synthesized with different Tb3+/Eu3+ ratios. Using as the thermometric parameter the ratio between the Eu3+, 5D0→7F2 transition, and the ligand emissions, [Tb0.97Eu0.03(L)2(ox)(H2O)] was found to be one of the best three luminescent ratiometric LnMOF thermometers, operative in the physiological range with a maximum sensitivity of 1.38%·K−1 at 340 K. The fact that the structure and properties of these coordination networks can be predicted by design constitutes a promising approach to new multifunctional materials, especially magnetic and luminescent, materials.
Glycine, paraformaldehyde, oxalic acid, Nd(NO3)3·6H2O, Sm(NO3)3·6H2O, Eu(NO3)3·6H2O, Gd(NO3)3·6H2O, Tb(NO3)3·6H2O, Dy(NO3)3·5H2O, Ho(NO3)3·5H2O and Yb(NO3)3·xH2O were purchased from Alfa Aesar and were used as received.
[HL] was synthesized according protocols published in the literature [41,42]. Synthesis method and characterizations (elemental analysis, 1H and 13C NMR) can be found in a previously published paper .
[Ln(L)(ox)(H2O)] compounds with Ln = Eu3+, Gd3+, Tb3+, Dy3+, Ho3+ and Yb3+ were prepared by solvothermal reaction by mixing [HL] (0.5 mmol), lanthanide nitrate (0.5 mmol) and oxalic acid (0.25 mmol) in a water/ethanol solution (1.5 mL). The solution was sealed in a Teflon-line stainless steel bomb (6 mL) and heated at 393 K for 72 h. After cooling to room temperature, the bomb was opened and colorless crystals were filtered and washed with ethanol and dried at room temperature. Yields were between 41% and 59%. Elemental analysis confirmed the composition of each compounds. [Eu(L)(ox)(H2O)]: Anal. calcd for C9H9N2O9Eu (440.96 g·mol−1): C, 24.49; H, 2.04; N, 6.35; found: C, 24.01; H, 2.06; N, 6.00; [Gd(L)(ox)(H2O)]: anal. calcd for C9H9N2O9Gd (446.25 g·mol−1): C, 24.20; H, 2.02; N, 6.27; found: C, 23.96; H, 2.05; N, 6.24; [Tb(L)(ox)(H2O)]: anal. calcd for C9H9N2O9Tb (447.92 g·mol−1): C, 24.11; H, 2.01; N, 6.25; found: C, 23.68; H, 2.07; N, 6.10; [Dy(L)(ox)(H2O)]: anal. calcd for C9H9N2O9Dy (451.50 g·mol−1): C, 23.92; H, 1.99; N, 6.20; found: C, 23.47; H, 2.05; N, 6.15; [Ho(L)(ox)(H2O)]: anal. calcd for C9H9N2O9Ho (453.93 g·mol−1): C, 23.79; H, 1.98; N, 6.17; found: C, 23.16; H, 2.03; N, 6.05; [Yb(L)(ox)(H2O)]: anal. calcd for C9H9N2O9Yb (462.04 g·mol−1): C, 23.37; H, 1.95; N, 6.06; found: C, 23.08; H, 2.10; N 5.95.
[Tb1−xEux(L)(ox)(H2O)] compounds with x = 0.01, 0.03, 0.05 and 0.10 were prepared in a similar manner but terbium nitrate and europium nitrate were introduced with the adapted stoichiometry. Yields were between 32% and 34%.
Elemental analyses for C, H, N were carried out at the Service de Microanalyses of the Institut de Chimie de Strasbourg. The SEM images were obtained with a JEOL 6700F (scanning electron microscope (SEM) equipped with a field-emission gun (FEG), operating at 3 kV in the SEI mode instrument. FTIR spectra were collected on a Perkin Elmer Spectrum Two UATR-FTIR spectrometer. TGA-TDA experiments were performed using a TA instrument SDT Q600 (heating rates of 5 °C·min−1 under air stream). NMR spectra in solution were recorded using a Bruker AVANCE 300 (300 MHz) spectrometer. The emission and excitation spectra were recorded on a modular double grating excitation spectrofluorometer with a TRIAX 320 emission monochromator (Fluorolog-3, Horiba Scientific) coupled to a R928 or a H9170 Hamamatsu photomultiplier, for the detection on the visible and near-infrared spectral ranges, respectively, using the front-face acquisition mode. The excitation source was a 450 W Xe arc lamp. The emission spectra were corrected for detection and optical spectral response of the spectrofluorometer and the excitation spectra were corrected for the spectral distribution of the lamp intensity using a photodiode reference detector. Time-resolved measurements were carried out with the pulsed Xe–Hg lamp excitation, in front-face acquisition mode. The temperature was controlled with a helium closed-cycle cryostat with vacuum system (ca. 5 × 10−6 mbar) and a Lakeshore 330 auto-tuning temperature controller with a resistive heater. The temperature can be adjusted from ca. 12 to 450 K with a maximum accuracy of 0.1 K. The sample temperature was fixed to a particular value using the auto-tuning temperature controller; after waiting 5 min to thermalize the sample, four consecutive steady-state emission spectra were measured for each temperature; the maximum temperature difference detected during the acquisitions was 0.1 K, the temperature accuracy of the controller. Magnetic measurements were performed using a Quantum Design SQUID-VSM magnetometer. The static susceptibility measurements were performed in the temperature range of 1.8–300 K with an applied field of 0.5 T. Samples were blocked in eicosane to avoid orientation under magnetic field. Magnetization measurements at different fields and at given temperature confirm the absence of ferromagnetic impurities. Data were corrected for the sample holder and eicosane and diamagnetism was estimated from Pascal constants. The powder XRD patterns were collected with a Bruker D8 diffractometer (Cu Kα1, λ = 1.540598 Å) operating at 40 kV and 40 mA equipped with a LynxEye detector. The X-ray diffraction data on single crystal were collected with graphite-monochromatized Mo Kα radiation (λ = 0.71073 Å) with a Kappa Nonius CCD diffractometer at room temperature. Intensity data were corrected for Lorenz-polarization and absorption factors. The structures were solved by direct methods using SIR92 , and refined against F2 by full-matrix least-squares methods using SHELXL-2014 with anisotropic displacement parameters for all non-hydrogen atoms [74,75]. All calculations were performed by using the crystal structure crystallographic software package WINGX . The structure was drawn using Mercury or Diamond [77,78]. Hydrogen atoms were located on a difference Fourier map and introduced into the calculations as a riding model with isotropic thermal parameters. Crystallographic data for the structures reported have been deposited in the Cambridge Crystallographic Data Centre with CCDC reference numbers 1541843, 1541844, 1541845, 1541846, 1541847, 1541848 for [Gd(L)(ox)(H2O)], [Yb(L)(ox)(H2O)], [Dy(L)(ox)(H2O)], [Ho(L)(ox)(H2O)], [Tb(L)(ox)(H2O)], [Eu(L)(ox)(H2O)].
Supporting Information contains a representation of the coordination polyhedron, a table of selected bonds, a comparison of the experimental powder X-ray diffraction patterns of the different compounds and the simulated pattern from single crystals X-ray data, SEM analysis, TGA/TDA analysis, a summary of the weight loss values for the different compounds, infrared spectra, luminescence measurement and magnetic expression.
|Supporting Information File 1: Additional experimental data.|
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The authors thank the Centre National de la Recherche Scientifique (CNRS), the Université de Strasbourg (Idex), the Labex NIE (ANR-11-LABX-0058_NIE within the Investissement d’Avenir program ANR-10-IDEX-0002-02), the Agence Nationale de la Recherche (ANR contract no. ANR-15-CE08-0020-01) and the icFRC (http://www.icfrc.fr) for funding. Part of the present work comes from the thesis of Pierre Farger  and is part of the research activity supported by the European COST action MP1202: HINT (Rational design of hybrid organic–inorganic interfaces: the next step towards advanced functional materials. http://www.cost-hint.cnrs.fr). This work was also developed within the scope of the project CICECO-Aveiro Institute of Materials, POCI-01-0145-FEDER-007679 (Fundação para a Ciência e a Tecnologia, FCT, Ref. UID/CTM/50011/2013), financed by national funds through the FCT/MEC (Ministério da Educação e Ciência) and when appropriate co-financed by FEDER under the PT2020 Partnership Agreement. D.A. (SFRH/BPD/95032/2013) thanks FCT for a postdoctoral grant. The authors are grateful to Didier Burger for technical assistance.