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Article

Closing the Circle of the Lanthanide-Murexide Series: Single-Molecule Magnet Behavior and Near-Infrared Emission of the NdIII Derivative

by
Gang Huang
,
Guillaume Calvez
,
Yan Suffren
,
Carole Daiguebonne
,
Stéphane Freslon
,
Olivier Guillou
and
Kevin Bernot
*
Univ Rennes, INSA Rennes, CNRS, UMR 6226 (Institut des Sciences Chimiques de Rennes), F-35000 Rennes, France
*
Author to whom correspondence should be addressed.
Magnetochemistry 2018, 4(4), 44; https://doi.org/10.3390/magnetochemistry4040044
Submission received: 18 July 2018 / Revised: 19 September 2018 / Accepted: 21 September 2018 / Published: 3 October 2018
(This article belongs to the Special Issue Multifunctional Molecule-based Magnetic Materials)
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Abstract

:
Up to now, even if murexide-based complexometric studies are performed with all 3d or 4f ions, the crystal structures of the light-lanthanide derivatives of the lanthanide-murexide series are unknown. In this work, we report the crystal structure of the NdIII derivative named NdMurex. Contrary to all known complexes of the 3d or 4f series, a dimeric compound was obtained. As for its already reported DyIII and YbIII parents, the NdIII complex responsible for the color-change behaves as a single-molecule magnet (SMM). This behavior was observed on both the crystalline (NdMurex: Ueff = 6.20(0.80) K, 4.31 cm−1; τ0 = 2.20(0.92) × 10−5 s, Hdc = 1200 Oe) and anhydrous form (NdMurexAnhy: Ueff = 6.25(0.90) K, 4.34 cm−1; τ0 = 4.85(0.40) × 10−5 s, Hdc = 1200 Oe). The SMM behavior is reported also for the anhydrous CeIII derivative (CeMurexAnhy: Ueff = 5.40(0.75) K, 3.75 cm−1; τ0 = 3.02(1.10) × 10−5 s, Hdc = 400 Oe). The Near-Infrared Emission NIR emission was observed for NdMurexAnhy and highlights its bifunctionality.

Graphical Abstract

1. Introduction

The interest for multifunctional magnetic material has been boosted by the (re)introduction of lanthanide ions [1] in the field of molecular magnetism [2,3,4]. Indeed, in addition to their appealing magnetic properties they have also intrinsic assets such as catalytic activity or photo-luminescent properties [5,6,7,8,9,10]. This last point opens the way to magnetic and luminescent materials that can be of particular interest [11,12,13].
Murexide ligand (Scheme 1) is also known as purpuric acid or ammonium salt of 2,6-dioxo-5-[(2,4,6-trioxo-5-hexahydropyrimidinylidene)amino]-3H-pyrimidin-4-olate, abbreviated (NH4L) [14,15]. This ligand has been widely used in complexometric studies with 3d or 4f ions [16,17,18,19]. The complexation triggered a very strong color-change from purple to red-orange either in water or in organic solvent [14,16,17,18,19]. The crystal structure of the complex responsible of this color-change is known for 3d ions [20,21,22,23,24,25,26,27], but this is only very recently that some of us managed to determine it for lanthanides from SmIII to LuIII [28,29]. The obtained neutral Ln(L)3·xH2O complexes were found to behave as single-molecule magnets (SMM) for Ln = Dy [28] or Yb [29] (respectively DyMurex and YbMurex). For DyMurex, the original N3O6 environment of the DyIII ion permitted to demonstrate the crucial role played by the local symmetry of the oxygen surrounding over the nitrogen one. It shows also how the dipolar electrostatic field around the DyIII (and not the local charge) is the governing factor of its magnetic behavior [28]. For YbMurex, significant near-infrared (NIR) emissions have been observed that permitted to perform one of the first NIR magneto-luminescent correlations. It evidenced also that the contribution of the YbIII excited-states to the emissions have to be carefully considered in such procedures [29].
In this study, we have been able to obtain information on the crystal structure of two of the missing light lanthanide ions from the series (Ln = CeIII and NdIII). Light lanthanide ions have so far drawn less attention than heavier ones in the field of molecular magnetism [30]. This is somewhat intriguing as most permanent magnets are made of NdIII or SmIII ions [31]. We report here the synthesis and magnetic properties of the CeIII (CeMurex) and NdIII derivatives (NdMurex). For the later a bifunctional compound was obtained as NIR emission was observed.

2. Results

2.1. Crystal Structure

NdMurex crystallizes in the triclinic system, P-1 space group (n°2, see Table S1). The asymmetric unit is made of one NdIII ion coordinated by two murexide ligands and three water molecules. The murexide ligand acts a tri-dentate ligand and a capped N2O7 coordination environment around the NdIII ion formed. Nd-O and Nd-N distances are in the 2.42 Å–2.67 Å and 2.74 Å–2.86 Å range, respectively (Table S2). SHAPE analysis revealed that the coordination polyhedron was either a distorted capped square antiprism (C4v) or a spherical capped square antiprism (C4d) (Figure 1, Table S3) [32,33]. One free murexide ligand ensures the electroneutrality of the asymmetric unit and seven uncoordinated water molecules were found. An inversion center located close to one of the two murexide ligands creates a dimeric structure [34] with Nd-Nd distance of 7.55 Å (see Figure 1 and Figure 2, Figures S1–S3) and fourteen water molecules in the intermolecular space. The overall formula of NdMurex is then [Nd2(L)4(H2O)6](L)2(H2O)14 (Figure 1). The shortest intermolecular Nd-Nd distance is 9.58 Å.
It is interesting to compare this compound with the ones obtained with heavier lanthanide ions (Ln = Sm to Lu), such as DyMurex [28] and YbMurex [29] where neutral monomeric complex of formula Ln(L)3·xH2O where formed. The striking originality in NdMurex is the ability of the murexide ligand to bind two different NdIII ions either via its tris-dentate clamp but also via one of the two external carbonyl group that were left uncoordinated in the case of Ln(L)3·xH2O. This extra coordination is made via the longest Nd-O distance (Nd-O6 = 2.67 Å) and is stabilized via strong stacking between two symmetry-related murexide ligand (Figure 2). It is likely that the ionic size of the lanthanide ion is the governing factor in stabilizing the dimeric crystalline structure over the monomeric one.

2.2. Thermal Stability

The purple crystals of NdMurex are stable for some hours out of their mother solution. Then, cracks appear on the crystal’s surfaces associated with the loss of crystallization water molecules. This has been confirmed by thermogravimetric analysis (TGA/DTA) where 18% weight loss, compatible with the loss of 14 water molecules, was observed between 20 and 200 °C (Figure 3). The anhydrous derivative formed, named NdMurexAnhy, was stable up to 300 °C. Similar dehydration was observed for an overnight room-temperature drying of NdMurex crystals. A crystalline powder was obtained and powder X-ray diffraction evidenced a clear phase transition upon dehydration (Figure S4). The CeIII derivative was obtained only as this anhydrous form named CeMurexAnhy and was isostructural to NdMurexAnhy (Figure S4).

2.3. Magnetic Characterization

Static magnetic measurements of NdMurex have been performed at 1000 Oe on fresh crystals crushed into teflon pellets. The room temperature χMT value was 3.16 emu·K·mol−1 in good agreement with the theoretical value expected for two isolated NdIII ion (4I9/2, gJ = 8/11, J = 9/2, χMT300K = 2 × 1.64 emu·K·mol−1). This confirms that most of crystallization water molecules were retained at this point (all crystallization water molecules considered in NdMurex molecular weight). As the temperature was lowered, χMT decreased to reach 1.11 emu·K·mol−1 at 2 K (Figure 4). This decrease was attributed to a standard depopulation of NdIII Stark’s sub-levels as long intra- and intermolecular distances preclude the occurrence of Nd-Nd magnetic interactions.
A pellet of overnight dried NdMurexAnhy was measured and the room temperature χMT value was 3.22 emu·K·mol−1. Temperature dependence of its magnetic behavior was then highly similar to the one of NdMurex (Figure 4). Same procedures were used with CeMurexAnhy with a room temperature χMT value of 1.82 emu·K·mol−1 in agreement with the expected value (2F5/2, gJ = 6/7, J = 5/2, χMT300K = 2 × 0.80 emu·K·mol−1) (Figure 4).
Dynamic magnetic measurements were performed on NdMurex and NdMurexAnhy and the optimum external Hdc field to observe magnetic slow relaxation was found to be 1200 Oe (Figures S5 and S6). For both samples, frequency dependence of the out-of-phase susceptibility was observed in the 1.8–4.4 K region (Figure 5 and Figure S7). The temperature dependence of the relaxation was found to be close to a linear regime and was estimated considering an Orbach relaxation where τ = τ0exp(−Ueff/kBT) with τ0 the characteristic relaxation time and Ueff the energy barrier for spin reversal. On both samples, very small variations were observed, and Ueff almost identical (Ueff = 6.20(0.80) K, 4.31 cm−1 (τ0 = 2.20(0.92) × 10−5 s) and Ueff = 6.25(0.90) K, 4.34 cm−1 (τ0 = 4.85(0.40) × 10−5 s) for NdMurex and NdMurexAnhy respectively). Indeed, the dehydration of NdMurex impacts only, and in a moderate way, the characteristic relaxation time (Figure 6 and Figure 7). On both samples the distribution of the relaxation times α was investigated using normalized Cole-Cole plots and an extended Debye equation (Figure 6 and Figure 7). On both samples, stable α values around 0.2 were observed that indicate a moderate distribution of the relaxation times. Large relaxing fractions were observed with (1 − χS/χT) = 91% and 80% at 2 K for NdMurex and NdMurexAnhy, respectively (with χS = adiabatic susceptibility, χT isothermal susceptibility, see Tables S4–S7). Overall, these behaviors highlight that the magnetic behavior of NdMurex was not sensitive to dehydration, and consequently that intermolecular interactions play a minor role in its magnetic slow relaxation.
The cerium derivative, CeMurexAnhy, has been was measured with an optimum external Hdc field of 400 Oe (Figure S8). Frequency dependence of the out-of-phase susceptibility was observed between 1.8 K and 4 K (Figure S9). The magnetic relaxation was also governed by Orbach process with Ueff = 5.40(0.75) K, 3.75 cm−1 and τ0 = 3.02(1.10) × 10−5 s (Figure 7). As for the NdIII derivatives, stable α values around 0.15 were observed, with 92% relaxing fraction at 2 K (Figure 6, Tables S8 and S9).
All three samples were rare examples of SMMs that involved light lanthanide ions [30]. Whereas several CeIII-based SMMs have been reported [30,35,36,37,38,39,40], only few examples of NdIII-SMMs are known. We will detail them here.
The first report of an Nd-SMM was a NdIII with a full nitrogen environment N9 with an almost perfect D3h symmetry, but its effective energy barrier was low (Ueff = 2.8 cm−1) (Table 1) [41]. Other examples on sandwich complexes from the COT family (COT = bis(trimethylsilyl)cyclooctatetraenyl dianion) where the NdIII was in C16 environment shows SMM behavior (Ueff = 14.6 cm−1) [39]. Another organometallic NdIII SMM was reported with Cp* as main ligands (Ueff = 29 cm−1) [42]. Macrocyclic complexes of NdIII ions show mixed magnetic relaxation processes in which Ueff ≈ 21 cm−1 or Ueff ≈ 51 cm−1 depending on the crown-ether that is considered (O12 or O10N2 environment) [37]. Cadmium-based metalacrowns stabilize hexagonal bipyramidal environment (O8) for NdIII ions with Ueff ≈ 15 cm−1 but strong influence of Raman-like relaxation process was observed [40]. NdIII derivatives from the polyoxometallates family have also been studied and energy barriers of Ueff = 51.4 cm−1 [43] and Ueff = 34 cm−1 [44] were reported. A detailed study [35] of the magnetic anisotropy of complexes with light lanthanide ions highlights that Ising-type anisotropy can be found in the well-known N2O6 environment that is very common for Dy-based SMMs and Ueff ≈ 20 cm−1 for the NdIII derivative is reported.
To the best of our knowledge only two polynuclear Nd-SMMs (dimers in these cases) have been reported. The first one is made of 2-fluorobenzoate ligands that bridges two phenantroline-chelated NdIII ions [45]. The N2O8 environment that is created, induces a mixed Orbach and Raman-like relaxation with Ueff = 9.5 cm−1. NdIII luminescence is observed but no magneto-luminescent correlation has been possible. On the contrary, such correlation has been possible on the second example [46] that is a carboxylate-bridged dimer with terminal bipyridine ligands (N2O7 environment, mixed Orbach and Raman-like relaxation with Ueff = 8 cm−1). The splitting of the lowest five Stark levels of the J = 9/2 state of the 4I9/2 level is clearly visible. The separation between the ground and first excited mJ state is significantly bigger than Ueff and confirms the presence of a mixed Orbach and Raman relaxation.
Several one-dimensional compounds made of NdIII display SMM behavior. These are one-dimensional assembly of NdIII in O9 environment (Ueff = 18.8 cm−1) [47] or benzene carboxylate-based chains with NdIII in O8 environment that shows mixed Orbach and Raman relaxation processes and Ueff values in the 18–21 cm−1 range [36,48].
It is interesting to note that all these examples have been measured using an external static field Hdc that ranges from 100 Oe to 3500 Oe. The only examples of zero-field Nd-SMMs reported so far are based on complexes made of phosphonic diamide- or phosphine oxide-based ligands [49,50]. The extremely strong geometric constrain [51] imposed by the ligands around the NdIII ions imposes a highly symmetric D5h pentagonal bipyramid environment (O7) with the apical oxygen atoms from the phosphine groups closer of the NdIII ions than the five equatorial water molecules. This induces a suitable electrostatic surrounding of the NdIII ion that is an oblate ion [52]. However the nature of the magnetic relaxation in these two compounds is debated as the initial Orbach mechanisms identified in the first report (Ueff = 17.2 cm−1) [50] has been revised to pure Raman or mixed Raman and QTM processes with no evidence of Orbach magnetic relaxation [49]. It can be noted that some examples may also be considered as relaxing via field-induced paramagnetism and not via standard SMM relaxation pathways. We cannot totally discard this possibility for the three samples we report here.
Last, it is worth noting that Ueff values have always been found significantly lower than ab-initio energy gaps when available. Such discrepancy is also visible when magneto-luminescence correlations have been targeted [41]. The most striking example is found on the previously cited trispyrazolylborate-based Nd-SMM where Ueff = 2.8 cm−1 is observed while a 115 cm−1 energy gap is extrapolated from low-temperature absorption measurements. This indicates that under-barrier fast magnetic relaxation mechanisms can bevery efficient on Nd-SMMs.

2.4. Luminescence Measurements

The investigation of the luminescent properties of Ln-SMM [53] is now a common procedure to establish magneto-luminescent correlations [54]. However these have been mainly performed on TbIII and DyIII ions because of their efficient SMM behaviors coupled with good emission properties (see ref [54] for full review) [55,56,57,58,59]. The approach has been less developed on NIR emissive Ln-SMM where mainly ErIII-SMM [60,61,62,63,64,65] and YbIII-SMM [29,66,67,68,69,70,71,72,73] have been investigated. The drawback of these ions is that their emission is not always strong enough to allow for reliable magneto-luminescent correlations.
In this study, we have measured the luminescence properties of NdMurexAnhy as NdMurex is not suitable for NIR emission because of its numerous crystallization water molecules (Figure 8). At room temperature no emission has been detected, once again the remaining three coordination water molecules are very likely to quench NdIII emission. At 77 K and under λexc = 629 nm (f-f sensitization) the broad and weak 4F3/2 → 4I9/2 transition centered on 870 nm is observed together with the characteristic 4F3/2 → 4I11/2 transition at 1050 nm. For this emission peak, it has not been possible to deconvoluate the different crystal-field contributions of the Stark sub-levels. NdMurexAnhy is thus a NIR-emissive SMM where no magneto- luminescent correlations can be performed [54].

3. Materials and Methods

3.1. General Procedures and Methods

All chemicals and reagents were of reagent grade (TCI chemicals) and used without further purification. Powder X-ray diffraction patterns were measured with a Panalytical X-Pert Pro diffractometer equipped with an X’celerator detector. Recording condition were 45 kV, 45 mA with Cu Kα (λ = 1.542 Å) in θ-θ mode. Simulated patterns from X-ray crystal structure have been obtained with Mercury 3.0 from CCDC. Thermogravimetric and thermodifferential analyses were performed under nitrogen atmosphere (heating rate 5 °C/min) with a PerkinElmer Pyris-Diamond thermal analyzer. Magnetic measurements were performed with a quantum design Magnetic properties Measurement System (MPMS) magnetometer on Teflon pellets. Diamagnetic corrections were applied using Pascal’s constants [74]. Luminescence measurements performed using a Horiba-Jobin-Yvon Florolog-3 spectrometer equipped with a 450 W Xe lamp and an infrared photodiode cooled by nitrogen liquid (InGaAs, sensitivity 800–1600 nm). Recording conditions were T = 77 K, integration time 300 ms (10 accumulation ) for excitation spectrum and T = 77 K, integratio. time 300 ms (50 accumulation).

3.2. Synthetic Procedure

0.1 mmol of murexide (ammonium purpurate, “NH4L”, 28.42 mg) was solubilized in 20 mL of water under strong stirring and a deep purple solution was obtained. 0.1 mmol of Nd(NO3)3·6H2O (45.78 mg) was dissolved in 2 mL of water and quickly added to the NH4L solution. A color change was visible from dark to light purple after stirring for 5 min. At that point, the solution was filtered on sintered glass N°3 for some minutes and left undisturbed for one month at room temperature. Small prismatic purple crystals were then obtained. The CeIII derivative was obtained using a similar procedure but it was not possible to obtain X-ray quality single crystals. Therefore, only its anhydrous derivative was studied here. Elem anal. Calcd for NdMurex C48H64N30Nd2O56: C, 25.71; H, 2.88; N, 18.75. Found: C, 25.63, H, 2.82; N, 18.63. Calcd for NdMurexAnhy C48H36N30Nd2O42: C, 28.97; H, 1.83; N, 21.13. Found: C, 28.69, H, 1.91; N, 20.94. Calcd for CeMurexAnhy C48H36N30Ce2O42: C, 29.03; H, 1.83; N, 21.17. Found: C, 28.71, H, 1.91; N, 20.96.

3.3. Crystal Structure

Crystals were mounted on a Bruker AXS diffractometer (APEXII) and crystal structures were collected at 150 K with Mo Kα (λ = 0.71073 Å) radiation. Data reduction and cell refinement were performed with Denzo and Scalepack [70,71]. Crystal structures were solved by SIR97 [72] and refined by SHELX97 [70] via WINGX [73] interface. Hydrogen atoms were located on ideal positions. Crystal data can be found free of charge from Cambridge Crystallographic Data Center (www.ccdc.cam.ac.uk/data_request/cif) under reference (CCDC-1856342).

4. Conclusions

In this study, we report the synthesis and crystal structure of the light lanthanide adducts of the murexide ligand (“NH4L”). Whereas lanthanide ions from SmIII to LuIII crystallize as mononuclear complexes of formula Ln(L)3·xH2O, for Ln = NdIII dinuclear complexes of formula [Nd2(L)4(H2O)6](L)2(H2O)14 are formed. Their dimeric nature is due to the original binding mode of the murexide ligand that involves not only its tri-dentate clamp but also one of its external carbonyl group to coordinate the NdIII ion. The obtained compounds show SMM behavior either in their hydrated (NdMurex: Ueff = 6.20(0.80) K, 4.31 cm−1; τ0 = 2.20 × 10−5 s) or anhydrous form (NdMurexAnhy: Ueff = 6.25(0.90) K, 4.34 cm−1; τ0 = 4.85 × 10−5 s; CeMurexAnhy: Ueff = 5.40(0.75) K, 3.75 cm−1; τ0 = 3.02(1.10) × 10−5 s). NdMurexAnhy is an NIR-emitting SMM. Each NdIII ion is coordinated by three water molecules whose substitution by terminal ligands may offer interesting possibilities for further optimization of the SMM behavior (tuning of the electrostatic surrounding) and NIR emission (removing of OH vibrators).

Supplementary Materials

The following are available online at https://www.mdpi.com/2312-7481/4/4/44/s1, Table S1. Main crystallographic parameters for NdMurex. Table S2. Selected bond distance and angles of NdMurex. Table S3. Continuous Shape Measurements (CSM) extracted from analysis of NdMurex with SHAPE. Figure S1. Representation of the crystal packing of NdMurex along the a axis. Water molecules and hydrogen atoms are omitted for clarity. Figure S2. Representation of the crystal packing of NdMurex along the b axis. Water molecules and hydrogen atoms are omitted for clarity. Figure S3. Representation of the crystal packing of NdMurex along the c axis. Water molecules and hydrogen atoms are omitted for clarity. Figure S4. Powder X-ray diffraction pattern for NdMurexAnhy and CeMurexAnhy measured at 300 K with simulation from the structural data file of NdMurex at 150 K. Figure S5. Field dependence of the in-phase and out-of phase susceptibility measured at 2 K for NdMurex. Figure S6. Field dependence of the in-phase and out-of phase susceptibility measured at 2 K for NdMurexAnhy. Table S4. Table of the values extracted from the fitting of X” vs frequency curves for NdMurex. Table S5. Table of the values extracted from the Argand plot for NdMurex. Table S6. Table of the values extracted from the fitting of X” vs. frequency curves for NdMurexAnhy. Table S7. Table of the values extracted from the Argand plot for NdMurexAnhy. Figure S7. Frequency dependence of the in-phase susceptibility of NdMurex and NdMurexAnhy with Hdc = 1200 Oe for temperatures from 1.8 (blue) to 4.4 K (red). Lines are guide to the eye. Figure S8. Field dependence of the out-of phase susceptibility measured at 2 K for CeMurexAnhy. Figure S9. Frequency dependence of the in-phase (top) and out of phase susceptibility (bottom) measured with Hdc = 400 Oe for CeMurex for temperatures from 1.8 (blue) to 5 K (red). Table S8. Table of the values extracted from the fitting of X” vs. frequency curves for CeMurex. Table S9. Table of the values extracted from the Argand plot for CeMurex.

Author Contributions

Conceptualization, K.B. and O.G.; Methodology, K.B.; Investigation, K.B., G.H., S.F., Y.S., G.C., C.D.

Funding

This research is funded by Institut Universitaire de France (IUF).

Acknowledgments

T. Roisnel (CDifX) is acknowledged for help in crystal structure data collection. T. Guizouarn (Centre de Mesures Physiques, ISCR) is acknowledged for help in magnetic measurements.

Conflicts of Interest

The authors declare no conflict of interest.

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Magnetochemistry 04 00044 sch001 550
Scheme 1. The murexide ligand (also known as ammonium salt of 2,6-dioxo-5-[(2,4,6-trioxo-5-hexahydropyrimi-dinylidene)amino]-3H-pyrimidin-4-olate).
Scheme 1. The murexide ligand (also known as ammonium salt of 2,6-dioxo-5-[(2,4,6-trioxo-5-hexahydropyrimi-dinylidene)amino]-3H-pyrimidin-4-olate).
Magnetochemistry 04 00044 sch001
Magnetochemistry 04 00044 g001 550
Figure 1. The best view of NdMurex with one of the two free murexide molecules and labeling scheme. Inset view of the Nd1 coordination polyhedron. Hydrogen atoms and water molecules are omitted for clarity.
Figure 1. The best view of NdMurex with one of the two free murexide molecules and labeling scheme. Inset view of the Nd1 coordination polyhedron. Hydrogen atoms and water molecules are omitted for clarity.
Magnetochemistry 04 00044 g001
Magnetochemistry 04 00044 g002 550
Figure 2. Best views of the NdMurex dimeric structure with (a) the asymmetric unit highlighted, and (b) a view parallel to the stacking of murexide ligands. Hydrogen atoms and water molecules are omitted for clarity.
Figure 2. Best views of the NdMurex dimeric structure with (a) the asymmetric unit highlighted, and (b) a view parallel to the stacking of murexide ligands. Hydrogen atoms and water molecules are omitted for clarity.
Magnetochemistry 04 00044 g002
Magnetochemistry 04 00044 g003 550
Figure 3. Thermogravimetric (right axis) and thermodifferential (left axis) analysis of NdMurex performed under N2 atmosphere.
Figure 3. Thermogravimetric (right axis) and thermodifferential (left axis) analysis of NdMurex performed under N2 atmosphere.
Magnetochemistry 04 00044 g003
Magnetochemistry 04 00044 g004 550
Figure 4. Temperature dependence of χMT for NdMurex, NdMurexAnhy, and CeMurexAnhy measured with Hdc = 1000 Oe.
Figure 4. Temperature dependence of χMT for NdMurex, NdMurexAnhy, and CeMurexAnhy measured with Hdc = 1000 Oe.
Magnetochemistry 04 00044 g004
Magnetochemistry 04 00044 g005 550
Figure 5. Frequency dependence of the out-of-phase susceptibility of NdMurex (a) and NdMurexAnhy (b) with Hdc = 1200 Oe for temperatures from 1.8 (blue) to 4.4 K (red). Lines are guide to the eye.
Figure 5. Frequency dependence of the out-of-phase susceptibility of NdMurex (a) and NdMurexAnhy (b) with Hdc = 1200 Oe for temperatures from 1.8 (blue) to 4.4 K (red). Lines are guide to the eye.
Magnetochemistry 04 00044 g005
Magnetochemistry 04 00044 g006 550
Figure 6. Cole-Cole plots measured for temperatures from 1.8 (blue) to 5 K (red) and for NdMurex (Hdc = 1200 Oe, a), NdMurexAnhy (Hdc = 1200 Oe, b), and CeMurexAnhy (Hdc = 400 Oe, c) with selected fits and simulation of the ideal distribution of the magnetic relaxation as red curve.
Figure 6. Cole-Cole plots measured for temperatures from 1.8 (blue) to 5 K (red) and for NdMurex (Hdc = 1200 Oe, a), NdMurexAnhy (Hdc = 1200 Oe, b), and CeMurexAnhy (Hdc = 400 Oe, c) with selected fits and simulation of the ideal distribution of the magnetic relaxation as red curve.
Magnetochemistry 04 00044 g006
Magnetochemistry 04 00044 g007 550
Figure 7. Arrhenius plot with best fits for NdMurex (full circles), NdMurexAnhy (empty circles), and CemurexAnhy (full squares).
Figure 7. Arrhenius plot with best fits for NdMurex (full circles), NdMurexAnhy (empty circles), and CemurexAnhy (full squares).
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Magnetochemistry 04 00044 g008 550
Figure 8. Emission spectrum of NdMurexAnhy measured at 77 K (excitation spectrum in inset).
Figure 8. Emission spectrum of NdMurexAnhy measured at 77 K (excitation spectrum in inset).
Magnetochemistry 04 00044 g008
Table
Table 1. Table of NdIII-based Single-Molecule Magnets with Ueff values and references associated.
Table 1. Table of NdIII-based Single-Molecule Magnets with Ueff values and references associated.
CompoundHdcUeff (cm−1)Reference
NdTp31002.8[41]
Li(DME)3][Nd(COT″)2] 100015[39]
[Nd(NO3)3(18-crown-6)] 100021[37]
[Nd(NO3)3(1,10-diaza-18-crown-6)] 100051[37]
[NdCd3(Hquinha)3(n-Bu3PO)2I3]·3EtOH·2H2O100015[40]
[Nd(W5O18)2]9−100051[43]
Nd2(2-FBz)4−(NO3)2(phen)215009.5[45]
Nd(fdh)3(bpy)50020[35]
{[Nd(μ2-L1)3·(H2O)2]·H2O}n 200019.5[36]
[Nd(μ2-L2)2·(CH3COO)·(H2O)2]n200014[36]
Nd2(μ2–9-AC)4(9-AC)2(bpy)220008[46]
{[Nd2(CNCH2COO)6(H2O)4]·2H2O}n150019[47]
[Nd(μ2-L1)3(H2O)2]·C2H3N}n200019[48]
[Nd(μ2-L2)(L2) (CH3COO)(H2O)2]n350015[48]
(NH2Me2)3{[Nd(Mo4O13)(DMF)4]3(BTC)2}·8DMF Cp*2Nd(BPh4)50034[44]
100029[42]
[Nd(CyPh2PO)2(H2O)5]I3·2(CyPh2PO)·3EtOH 0n.a. *[49]
{[tBuPO(NHiPr)2Nd(H2O)5]-[I]3·tBuPO(NHiPr)2·(H2O)}011/17[50]
-100027[50]
-2000n.a. **[49]
NdMurex12004.3This study
NdMurexAnhy12004.3This study
CeMurexAnhy4003.75This study
Tp− = trispyrazolylborate, COT” = bis(trimethylsilyl)cyclooctatetraenyl dianion, H2quinha = quinaldichydroxamic acid, DME = dimethoxyethane, FBz = 2-fluorobenzoate, phen = phenantroline, fdh = 1,1,1-fluoro-5,5-dimethyl-hexa-2,4-dione, bpy = 2,2′-bipyridine, L1 = 3,5-dinitrobenzoate, L2 = 2,4-dinitrobenzoate, BTC = 1,3,5-benzenetricarboxylate), [Cp*]− pentamethylcyclopentadienyl anion, 9-AC = anthracenecarboxylate, bpy = 2,2′-bipyridine, CyPh2PO = cyclohexyl(diphenyl)phosphine oxide). * Dual Raman and quantum tunneling processes observed with no evidence of Orbach magnetic relaxation; ** Original report has been revised in the cited reference for one with no evidence of Orbach magnetic relaxation.

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Huang, G.; Calvez, G.; Suffren, Y.; Daiguebonne, C.; Freslon, S.; Guillou, O.; Bernot, K. Closing the Circle of the Lanthanide-Murexide Series: Single-Molecule Magnet Behavior and Near-Infrared Emission of the NdIII Derivative. Magnetochemistry 2018, 4, 44. https://doi.org/10.3390/magnetochemistry4040044

AMA Style

Huang G, Calvez G, Suffren Y, Daiguebonne C, Freslon S, Guillou O, Bernot K. Closing the Circle of the Lanthanide-Murexide Series: Single-Molecule Magnet Behavior and Near-Infrared Emission of the NdIII Derivative. Magnetochemistry. 2018; 4(4):44. https://doi.org/10.3390/magnetochemistry4040044

Chicago/Turabian Style

Huang, Gang, Guillaume Calvez, Yan Suffren, Carole Daiguebonne, Stéphane Freslon, Olivier Guillou, and Kevin Bernot. 2018. "Closing the Circle of the Lanthanide-Murexide Series: Single-Molecule Magnet Behavior and Near-Infrared Emission of the NdIII Derivative" Magnetochemistry 4, no. 4: 44. https://doi.org/10.3390/magnetochemistry4040044

APA Style

Huang, G., Calvez, G., Suffren, Y., Daiguebonne, C., Freslon, S., Guillou, O., & Bernot, K. (2018). Closing the Circle of the Lanthanide-Murexide Series: Single-Molecule Magnet Behavior and Near-Infrared Emission of the NdIII Derivative. Magnetochemistry, 4(4), 44. https://doi.org/10.3390/magnetochemistry4040044

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