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Article

Transition Metals Meet Scorpiand-like Ligands

by
Salvador Blasco
*,
Begoña Verdejo
,
María Paz Clares
* and
Enrique García-España
Instituto de Ciencia Molecular, Departamento de Química Inorgánica, Universidad de Valencia, C/Catedrático José Beltrán Martínez, 2, 46980 Paterna, Valencia, Spain
*
Authors to whom correspondence should be addressed.
Crystals 2023, 13(9), 1338; https://doi.org/10.3390/cryst13091338
Submission received: 28 July 2023 / Revised: 19 August 2023 / Accepted: 29 August 2023 / Published: 1 September 2023
(This article belongs to the Special Issue The Polyhedral Face of Coordination Chemistry)

Abstract

:
Scorpiand-like ligands combine the preorganization of the donor atoms of macrocycles and the degrees of freedom of the linear ligands. We prepared the complexes of several of these ligands with transition metal ions and made a crystallographic and water solution speciation studies. The analysis of the resulting crystal structures show that the ligands have the ability to accommodate several metal ions and that the coordination geometry is mostly determined by the ligand. Ligand 6-[3,7-diazaheptyl]-3,6,9–triaza-1-(2,6)-pyridinacyclodecaphane (L3) is an hexadentate ligand that affords a family of isostructural crystals with Cu(II), Mn(II), Ni(II) and Zn(II). The attempts to obtain Co(II) crystals afforded the Co(III) structures instead. Ligand 6-[4-(2-pyridyl)-3-azabutyl]-3,6,9-triaza-1(2,6)-pyridinacyclodecaphane (L2) is very similar to L3 and yields structures similar to it, but its behavior in solution is very different due to the different interaction with protons. Ligand 6-(2-aminoethyl)-3,6,9–triaza-1-(2,6)-pyridinacyclodecaphane (L1) is pentadentate and its complexes allow the metal to be more accessible from the solvent. A Zn(II) structure with L1 shows the species [ZnBrHL1] 2 + , which exists in a narrow pH range.

1. Introduction

Macrocyclic ligands offer an interesting framework for the study of coordination chemistry because all their donor atoms come preorganized, arranged geometrically in space. When they coordinate transition metals, the resulting coordination geometry is determined by the combined action of the preferred coordination geometry of the metal and the ability of the ligand to adapt to it. In the case of macrocyclic ligands, they tend to impose their coordination mode. If the ligand is open, linear and flexible, it has many more conformational degrees of freedom and, therefore, it is able to adapt to a wider variety of coordination preferences. It is possible to combine both types in a family of ligands that features a macrocyclic core decorated with a flexible pending arm containing additional donor atoms. Such ligands are often referred to as scorpiands due to its similarity with the body of a scorpion, where the macrocycle would be the scorpion body and the pending arm would be the tail with a sting at the end of it. They were first reported by Lotz and Kaden [1] although the name scorpiand was first coined by Fabrizzi and collaborators [2].
In our research group, we work with a family of ligands of this kind. Some of them are derivatives of L1 (see Figure 1), which can be readily obtained from a modified Richman–Atkins condensation of 2,6-bis(bromomethyl)pyridine with tris[2-(N-tolylsulphonylaminoethyl)]-amine followed by detosylation with HBr/acetic acid to obtain the hydrobromide salt [3]. L1 consists of a 12-membered ring with four nitrogen donor atoms: one is a pyridine nitrogen, two of them are secondary amino groups, and the last one is a tertiary amino group. This macrocycle is too small to equatorially coordinate a metal atom. Instead, when a metal atom goes into the cavity, the macrocycle folds leave two adjacent coordination vacancies as it can be seen in the literature in many examples that contain either L1 or the analog macrocycle without the pending arm [4,5,6,7]. This tendency to fold makes the bonds around N2 and N4 (see numbering in Figure 1) stretched out if it is possible. This feature is relevant in order to understand the structures presented in this work. From the synthetic point of view, L1 contains a primary amino group, which allows to easily introduce additional moieties in that position. A sizable number of derivatives of L1 containing different groups in that position have been synthesized and reported by our group [3,8,9,10]. When L1 is reacted with 2-pyridinecarboxaldehyde, we obtain the ligand L2, which incorporates a sixth donor nitrogen atom in the pending arm. If the reagent is 3-bromopropylphthalimide followed by phthalimide cleavage with hydrazine, we obtain L3, which also features a sixth donor atom but is much more flexible than the analog L2.
These ligands are able to coordinate many types of metal atoms, mainly transition and post-transition metal ions. So far, we reported interactions with Cu, Mn, Zn, Fe and Pb [3,9,11,12,13], and research is underway with other metal ions as well. We focused on the copper and manganese complexes of these ligands because they show very interesting redox properties. When the metal in question is able to catalyze one-electron redox reactions, such as Cu(II) or Mn(II), we report that such complexes are able to mimic the redox cycle of superoxide dismutase (SOD), catalyzing the dismutation of the superoxide anion [8,9,11] Iron complexes of L2 undergo oxidative dehydrogenation by the effect of a pH change [13]. These kinds of metal complexes might seem simple at first glance, but they exhibit a rather complex chemistry. Herein, we aim to present some of the features of this family of complexes by showing both solution and solid-state data in order to illustrate the interesting coordination chemistry that they exhibit.

2. Materials and Methods

2.1. Synthesis and Materials Used

The synthesis of L1, L2 and L3 was carried out as described in the literature [3,8,9] For crystal preparation and potentiometric measurements, stock solutions ca. 0.1 m of either MnSO 4 ·H 2 O, Cu(ClO 4 ) 2 ·6H 2 O, Ni(ClO 4 ) 2 ·6H 2 O, Zn(ClO 4 ) 2 ·6H 2 O or CoCl 2 ·2H 2 O were prepared in Mili-Q water. The metal concentration was standardized by a suitable complexation volumetry method. In the particular case of iron stock solutions, they were prepared from FeSO 4 ·7H 2 O in 0.1 m HCl. In these cases, both the metal concentration and the acid concentration were determined by volumetric titration. The complexes were prepared by the simple mixing of equimolar amounts of both the metal stock solution and the desired ligand in an aqueous solution. Single crystals were prepared by the slow evaporation of a pH neutral water solution of the corresponding complex. Caution: Perchlorates are potentially explosive if they come in contact with organic matter, and they should be handled with extreme care.

2.2. X-ray Single Crystal Diffractometry

Single crystal X-ray diffraction was carried out with either of the following machines: (1) Enraf-Nonius KAPPA CCD single-crystal diffractometer with Mo K α radiation ( λ = 0.71073   Å ) and a graphite monochromator with data collection by COLLECT software with utilities DENZO and SCALEPACK, or (2) Agilent Super-Nova Diffractometer with Mo K α radiation ( λ = 0.71073   Å ) with a mirror monochromator located at the Institute of Molecular Sciences (ICMOL) from the University of Valencia, and data acquisition and treatment performed with CRYSALISPRO software [14]. If an absorption correction needed to be applied, either a spherical absorption correction as implemented in DENZO, or a semi-empirical absorption correction (MULABS [15] as implemented in PLATON [16]) was applied.
Crystals were measured at room temperature (293 K ). The structures were solved initially with SHELXS [17] with direct methods. Then, they were refined with SHELXL [17] using OLEX2 [18] as the frontend. Final figures for publishing were produced using CHIMERA [19] or MERCURY [20].

2.3. Potentiometric Measurements

The potentiometric titrations were carried out in a thermostated bath at 298.1   K , using NaClO 4   0.15 m as the supporting electrolyte, in the pH range 2.5–11.0. The experimental procedure (burette, potentiometer, cell, stirrer, microcomputer, etc.) is fully described elsewhere [21]. The acquisition of the electromotive force emf data was performed with the computer program PASAT [22,23]. The reference electrode was an Ag/AgCl electrode in saturated KCl solution. The glass electrode was calibrated as a hydrogen ion concentration probe by titration of previously standardized amounts of HCl with carbonate-free NaOH solutions and the equivalent point determined by the Gran’s method [24,25], which gives the standard potential E and the ionic product of water (pKw = 13.73 ( 1 ) ). At least two reproducible titrations for each system were recorded. The computer program HYPERQUAD [26] was used to fit protonation and stability constants. The independent titration curves were treated first as separate curves, and then the curves for each system (at least two) were then merged and treated as a single set without significant variations in the values of those treated first as separate curves and then merged and treated as a single set without stability constants. The final values were those obtained from the simultaneous treatment of the merged curves. The HYSS [27] program was used to generate the distribution diagrams.

3. Results and Discussion

3.1. Interaction of L3 with Mn, Fe, Co, Cu, Ni and Zn

L3 has six donor atoms that can be geometrically arranged in an octahedral disposition. When a metal atom is placed inside the ligand cavity, the ligand itself will impose its preferred coordination geometry rather than the metal. We prepared crystals of L3 with several transition and post-transition metals and successfully solved the structures for Mn(II), Cu(II), Ni(II) and Zn(II) with ClO 4 counterions. We named these structures C1 to C4, respectively. Unfortunately, crystals of L3 with iron could not be obtained. Also, for the case of the Co(II) complex, the Co(III) structure was obtained instead. This ligand readily coordinates metal ions. We studied some metal atoms from the first transition series for their biological relevance. We previously reported copper- or manganese-related crystal structures [9,10,11], but we include some of them here again for comparative purposes.
We studied metal complex formation in solution and we fitted the values of the formation constants. The results are summarized in Table 1. The stability constant values follow the expected order: Mn < Fe < Cu > Zn. All of them form stable complexes with L3. In addition to that, several protonation constants for each complex were also found and refined with up to three protons. The values of the first protonation constants lie between 4.59 for Cu(II) and 8.14 for Fe(II). This indicates that above pH ca. 8, the complex should be completely hexacoordinated. Distribution diagrams show that the species [ML] 2 + is completely formed in those conditions. Indeed, we obtained all the crystals for L3 from moderately alkaline solutions. Also, some hydroxylated species were also found in the speciation study, but they only predominate at pH > 11 . Solution studies with Ni(II) were also carried out, but the slow kinetics prevented the fitting of reliable formation constants. Nonetheless, suitable single-crystals were obtained from the solutions used in potentiometric measurements. Similarly, solution studies with Co(II) were also carried out, but the values obtained do not match the expected results probably due to the oxidation that happens during the titration, preventing the collection of reliable data.
Crystals C1C4 are isostructural (Figure 2a–d) with the same orthorhombic crystal system, Pbca space group and atom arrangement, with the only difference being the metal atom coordinated to the ligand. Bond distances and angles are shown in Table A4. We always find that the longest bond distances involve N2 and N4. These two donor atoms are the ones that have to stretch more in order to coordinate a metal located inside the macrocycle. When the metal in question displays Jahn–Teller distortion, such as Cu(II) (crystal C2, Figure 2b), then the elongated axis is N2—M—N4 so that the bonds around N2 and N4 are in a more relaxed conformation. Some others, like Zn(II), do not have Jahn–Teller distortion but still have the axis N2—M—N4 as being slightly longer. This indicates that the coordination geometry is to a large extent imposed by the ligand and only to a lesser extent by the metal atom. The metal atom, though, also exerts some influence; that is why the length difference between the axial and equatorial bonds is larger for Cu(II) than for Zn(II). In these four structures, the packing is mainly ionic. In Figure 2e, details of the packing of C1 show the arrangement of anions and cations in the unit cell. It is worthwhile noting that in all these structures, the metal ion is completely wrapped and enclosed by the ligand, leaving no vacant coordination sites and restricted access to the metal from the solvent. This is best seen in Figure 2f, where the spacefill representation shows that the metal ion is not accessible from the solvent. This feature explains that Mn(II) complexes are not oxidized in alkaline conditions open to air, and crystals containing Mn(II) are obtained. When crystals are prepared from a neutral solution of [MnL1] 2 + , then a structure containing Mn(III) is obtained, which consists of two units of [MnL1] 3 + bridged by an oxo anion [28].

3.2. Cobalt Complexes of L1 and L3

When a pale pink, diluted solution of [CoL3] 2 + in aqueous NaClO 4 was allowed to slowly evaporate, deep blue crystals of [CoL3](ClO 4 ) 3 (H 2 O) were obtained instead of the expected Co(II) ones. As we noted above, the metal atom inside the cavity was completely enclosed by the ligand, which provides protection against air oxidation for the Mn(II) complexes. This seems not to be the case for Co(II), as we consistently obtained the crystal with Co(III). As mentioned above, speciation studies under argon were carried out, but the obtained formation constants are not reported herein, as the oxidation appears to happen to some extent during the titration process, which makes the values unreliable. A similar thing also happens when Co(II) complexes of L1 are allowed to slowly evaporate: single crystals containing the [CoBrL1] 2 + complex are obtained. Two different structures containing this complex were resolved: firstly, crystal C6 with formula [CoBrL1]Br 2 (H 2 O), and crystal C7 with formula [CoBrL1]Na(ClO 4 ) 3 in which sodium perchlorate is co-crystallized along with the complex. In all three examples, the Co(II) atom is easily oxidized to Co(III) by exposure to the atmosphere. The geometry of the complex [CoBrL1] 2 + from C6 and that of the complex [CoL3] 3 + from C5 are shown in Figure 3a,b. The complex from [CoBrL1] 2 + from C7 is not shown, but it is identical to that from C6. In all three structures, the Co(III) complex displays an octahedral coordination geometry, fairly regular with angles close to 90 (see Table A5). In the case of C6 and C7, the sixth coordination site is occupied by a bromide atom, which exhibits a longer bond than the others (ca. 2.3  Å), which is to be expected since it is an atom bigger than the other ones. The complex from structure C7 is essentially identical to that of C6 with bonds and angles that are only slightly different (see Table A5). As occurs for C1C4, the metal atom is deeply embedded, and it has no access from the solvent. In this case, a single water molecule is found in the asymmetric unit along with three perchlorate anions. Structure C6 contains a rich network of hydrogen bonds involving the hydrogen atoms of the amino groups, the water moiety and the bromide atoms (see Figure 3c). This structure is not purely electrostatic, but also the hydrogen bonds contribute to the packing. The water molecule is placed between two bromide atoms, Br2 and Br3, to which it donates hydrogen bonds, while not accepting from any other moiety. All N—H groups are hydrogen bond donors towards the nearest bromide anion. C7 is similar to C6, but it features an anionic moiety of (Na(ClO 4 ) 3 ) n 2 n that grows along the b crystallographic axis. Units of [CoBrL1] 2 + cations are placed in alternating orientation, filling in the gaps (see Figure 3d). This structure has a bigger electrostatic contribution to the packing but still some relevant hydrogen bonds are found (see Table A8).

3.3. Complexes of L2 with Cu(II) and Mn(II)

From the coordination point of view, L2 and L3 are similar because the two of them are hexadentate with the donor atoms in the same positions with the same number of bonds separating one from another. The only difference is that the donor N of L2 is on a rigid aromatic group and, for L3, it is located on a flexible aliphatic amino group. Indeed, the slow evaporation of an aqueous solution of the ligand with one equivalent of either Cu(ClO 4 ) 2 or Mn(ClO 4 ) 2 yields single crystals of either [ML2](ClO 4 ) 2 ] (C1 and C2) and [ML3](ClO 4 ) 2 ] (C8 and C9). The coordination mode is almost identical, as it can be seen comparing Figure 2a,b with Figure 4a,b. C1, C2, C8 and C9 crystallize in an orthorhombic system with very similar asymmetric units containing only one molecule of the complex, two perchlorate anions and no water molecules. The space group is different: C1 and C2, which contain L3, have a Pbca space group, while structures C8 and C9 have Pna21. Indeed, C8 is isostructural with C9 as C1 is to C2. This indicates that the metal exerts little influence outside the complex with regard to the packing. Another similarity is that the packing is mainly electrostatic as it can be seen in Figure 4c. The bond distances and angles are listed in Table A6. We observe, as we did for L3, the recurring feature that the longest metal–nitrogen bond distance involves N2 and N4. This is very clear for C8, which contains Cu(II). For C9, which contains Mn(II), the bond Mn1—N5 is slightly longer than Mn1—N4. A possible explanation for this is that the angles for C9 are more distorted and further from 90 than for C8.
If we explore the chemistry in solution, the similarities end, and we see very different behavior compared to the crystal state. Above, in Table 1, we show the formation constants of L3 with Cu(II). If we study the speciation of L2 with Cu(II), a single constant is found, with value log 10 K CuL = 22.6 ( 1 ) [29]. This value is very close to that from L3 ( log 10 K CuL = 22.93 ( 2 ) , see Table 1). Only this single constant is found, and its large value makes it possible for the species [CuL] 2 + to be formed at low pH values and predominate in a very large pH range (Figure 5left). This is also the reason for the larger error in the constant: only a small set of points at low pH values contain meaningful information about the formation of the complex (see Figure 5left). Nonetheless, the obtained value is confirmed by means of titration with a competing ligand in order to increase the number of data points [29]. For L3, on the other hand, even though the formation constant with Cu(II) is close to that of L2, the primary amino group can protonate more easily. As a result, the Cu(II) atom is introduced at ca. one unit of pH higher, and the species [CuL3] 2 + is not completely formed until pH~6 (Figure 5right).

3.4. Complex of L1 with Zn(II)

L1 is a good ligand for many transition metal atoms, such as Cu(II) [3], Mn(II) [28] or Zn(II) [12]. Usually in all the crystal structures of L1 reported by us, the metal atom is pentacoordinated with all donor atoms bonding the metal. Solution studies indicate that the complex [ZnL1] 2 + can take one or two protons to form species [ZnHL1] 3 + and [ZnH2L1] 4 + [12].
We were able to obtain single crystals of one such species, [ZnHL1] 3 + . This structure, named C10, is shown in Figure 6. The terminal amino group can be protonated more easily than the other amino groups, and that coordination bond can break. In this case, the tip of the tail would be + 1 , while the metal next to it is + 2 . Therefore, the tail would fold away from the metal, giving, as a result, an open conformation, with the metal much more exposed to the solvent. C10 presents a triclinic P 1 ¯ system and space group, and its asymmetric unit contains the complex [ZnBrHL1] 2 + with one water molecule and one ZnBr 4 2 counterion. In the unit of [ZnBrHL1] 2 + , the Zn(II) is pentacoordinated by the nitrogen atoms of L1, except N5, which is protonated, bearing one positive charge and being folded away from the metal atom, thus minimizing the electrostatic repulsion. The macrocycle is only partly folded as if it was trying to equatorially coordinate the metal ion but, being too small to do it, it stops halfway. The aforementioned electrostatic repulsion may also contribute to this conformation. N5 would be the fifth donor atom, but instead, a bromide anion fills this vacancy. The units of [ZnBrHL1] 2 + are grouped in pairs that share two hydrogen bonds between N4 and Br1 (see Figure 6b). A total of six hydrogen bonds can be located around each unit of complex. The details are shown in Table A9. Both electrostatic and hydrogen bonds are the main forces in the packing. The origin of ZnBr 4 2 is the free metal available at pH~5, where the complex is not completely formed and the bromide counterions are from the L1 hydrobromide salt.

4. Conclusions

The ligands presented herein have the ability to coordinate a variety of metal ions. We focused on metals from the first transition series and showed examples of Cu(II), Mn(II), Co(III), and Ni(II), as well as the post-transition metal ion Zn(II). The overall packing is mostly determined by the ligand. The same ligand with different metal atoms tends to yield either isostructural or structurally similar crystals provided that the charge does not change. L2 and L3 have almost the same coordination geometry and, as a consequence, the structures they afford are very similar. However, solid-state structures and solution studies show different pictures about the properties of the complexes due to the different interaction of the ligands with protons as it can be seen by comparing the speciation of Cu(II) and Mn(II) with either L2 or L3. L1, which is pentadentate, leaves the metal atom more exposed to the solvent.

Author Contributions

Conceptualization, S.B.; resources, B.V. and M.P.C.; data curation, S.B.; writing—original draft preparation, S.B.; writing—review and editing, S.B. and E.G.-E.; visualization, S.B.; supervision, E.G.-E.; funding acquisition, E.G.-E. All authors have read and agreed to the published version of the manuscript.

Funding

Financial support from the Spanish Ministerio de Economía y Competitividad (Project PID 2019-110751RD-I00) and the Conselleria de Innovación, Universidades, Ciencia y Sociedad Digital of the Generalitat Valenciana (PROMETEO Grant CIPROM/2021/030) is acknowledged.

Data Availability Statement

Crystallographic data have been deposited in the Cambridge Structural Database. These data can be obtained free of charge via http://www.ccdc.cam.ac.uk/conts/retrieving.html accessed on 25 August 2023 (or from the CCDC, 12 Union Road, Cambridge CB2 1EZ, UK; Fax: +44 1223 336033; E-mail: [email protected]). See deposition numbers in Table A1.

Conflicts of Interest

The authors declare no conflict of interest.

Abbreviations

The following abbreviations are used in this manuscript:
SODSuperoxide dismutase
CCDCCambridge Crystallographic Data Center
emfElectromotive force

Appendix A. Additional Tables

Appendix A.1. Crystallographic Data Tables

Table A1. Deposition numbers of crystal structures C1C10 in the Cambridge Crystallographic Data Center.
Table A1. Deposition numbers of crystal structures C1C10 in the Cambridge Crystallographic Data Center.
StructureCCDC n.Reference(s)
C11020483[9,11]
C2897979[10]
C32281410this work
C42281411this work
C52281412this work
C62281413this work
C72281414this work
C8888624[9]
C91423684[29]
C102281415this work
Table A2. Crystallographic data for structures C3C5. Values in parentheses represent standard deviation of the last significant figure.
Table A2. Crystallographic data for structures C3C5. Values in parentheses represent standard deviation of the last significant figure.
C3C4C5
FormulaC 16 H 30 Cl 2 NiN 6 O 8 C 16 H 30 Cl 2 ZnN 6 O 8 C 16 H 32 Cl 3 CoN 6 O 13
d calc./g cm−31.5961.5991.756
μ /mm−11.1081.3151.053
Formula Weight564.07570.73681.75
Colourpale redcolourlessdark blue
Shapeprismprismblock
Size/mm3 0.20 × 0.11 × 0.09 0.14 × 0.11 × 0.09 0.20 × 0.10 × 0.10
Crystal Systemorthorrhombicorthorrhombicmonoclinic
Space GroupPbcaPbcaP21/c
a17.4035(5)17.3510(4)16.9810(10)
b12.6487(6)12.7480(8)9.2817(4)
c21.3344(9)21.4350(9)21.4350(9)
β 109.954(2)
V/ Å 3 4696.4(3)4741.2(4)2578.5(3)
Z884
θ max 27.42827.08828.101
θ min 3.0213.3341.276
Measured Refl.976696159850
Independent Refl.532551895759
R int 0.05290.05800.0619
Parameters298298356
Restraints005
Largest Peak0.6090.6521.036
Deepest Hole−0.533−0.528−0.614
GooF0.9831.0171.021
w R 2 (all data)0.24600.24090.2367
w R 2 0.20040.17840.1975
R 1 (all data)0.14640.15050.1418
R 1 0.06990.06840.0767
Table A3. Crystallographic data for structures C6, C7 and C10. Values in parentheses represent standard deviation of the last significant figure.
Table A3. Crystallographic data for structures C6, C7 and C10. Values in parentheses represent standard deviation of the last significant figure.
C6C7C10
FormulaC 13 H 25 Br 3 CoN 5 OC 13 H 23 BrCoN 5 Cl 3 NaO 12 C 13 H 24 BrN 5 OZn 2
d calc./g cm−32.0162.0282.224
μ /mm−17.5392.80410.398
Formula Weight566.04709.54798.68
Colourbluevioletcolourless
Shapespearblockprism
Size/mm3 0.70 × 0.44 × 0.32 0.50 × 0.30 × 0.30 0.33 × 0.17 × 0.11
Crystal Systemmonoclinicmonoclinictriclinic
Space GroupP21/cP21/cP 1 ¯
a10.2042(3)10.7720(3)8.1632(2)
b9.3402(2)9.6220(6)10.6612(3)
c19.9239(6)23.2950(11)14.4818(4)
α 107.3420(15)
β 100.9050(14)105.792(3)91.8500(16)
γ 96.3360(18)
V/ Å 3 1864.64(9)2323.4(2)1192.88(6)
Z442
θ max 25.00027.49027.498
θ min 2.4162.2852.017
Measured Refl.18009930926571
Independent Refl.328252715472
R int 0.10450.07080.0733
Parameters225333237
Restraints302
Largest Peak2.0321.6151.372
Deepest Hole−2.621−1.835−1.465
GooF1.0280.9991.022
w R 2 (all data)0.25780.26500.0983
w R 2 0.24190.23210.0881
R 1 (all data)0.08960.14150.0671
R 1 0.07640.08130.0396

Appendix A.2. Tables of Distances and Angles

Table A4. Bond distances (Å) and angles (°) for complexes of L3.
Table A4. Bond distances (Å) and angles (°) for complexes of L3.
Bond/AngleC1 (M=Mn)C2 (M=Cu)C3 (M=Ni)C4 (M=Zn)
M—N12.216(4)2.043(6)2.024(4)2.110(5)
M—N22.298(5)2.389(6)2.203(5)2.246(5)
M—N32.267(5)2.103(5)2.113(4)2.203(5)
M—N42.345(5)2.337(6)2.179(5)2.278(6)
M—N52.255(4)2.028(6)2.105(5)2.150(6)
M—N62.213(5)2.031(6)2.099(5)2.119(5)
N1—M—N271.80(18)76.3(2)79.23(19)76.3(2)
N1—M—N399.98(18)91.4(2)94.95(17)93.9(2)
N1—M—N473.15(18)77.5(2)79.3(2)75.9(2)
N1—M—N5175.81(18)176.1(2)178.2(2)175.6(2)
N1—M—N693.77(19)91.2(2)90.1(2)93.3(2)
N2—M—N378.23(18)79.3(2)81.80(18)81.2(2)
N2—M—N4133.93(19)147.1(2)152.77(19)144.9(2)
N5—M—N2111.05(19)103.0(2)100.94(19)103.2(2)
N6—M—N2106.19(19)97.2(2)96.2(2)103.5(2)
N3—M—N479.42(18)81.9(2)83.53(18)79.7(2)
N5—M—N377.9(2)84.7(2)83.28(19)81.7(2)
N6—M—N3166.25(19)175.0(3)174.1(2)172.2(2)
N5—M—N4102.83(17)101.9(2)100.0(2)102.9(2)
N6—M—N4105.03(19)102.8(2)100.43(19)99.1(2)
N6—M—N588.38(19)92.7(2)91.7(2)91.1(2)
Table A5. Bond distances (Å) and angles (°) for complexes of the Co(III) structures. Values in parentheses represent standard deviation of the last significant figure.
Table A5. Bond distances (Å) and angles (°) for complexes of the Co(III) structures. Values in parentheses represent standard deviation of the last significant figure.
C5C6C7
Co1—N11.913(4)Co1—N11.889(8)Co1—N11.892(6)
Co1—N22.017(4)Co1—N21.983(8)Co1—N22.007(6)
Co1—N31.962(4)Co1—N41.967(8)Co1—N31.985(6)
Co1—N42.026(4)Co1—N31.985(8)Co1—N42.011(6)
Co1—N52.012(4)Co1—N51.951(9)Co1—N51.956(6)
Co1—N61.950(5)Co1—Br42.3371(19)Co1—Br12.3600(13)
N1—Co1—N482.03(17)N1—Co1—Br489.1(2)N1—Co1—Br187.07(17)
N1—Co1—N283.91(17)N1—Co1—N283.1(3)N1—Co1—N283.1(3)
N1—Co1—N396.97(18)N1—Co1—N497.0(3)N1—Co1—N397.1(2)
N1—Co1—N684.41(19)N1—Co1—N383.6(3)N1—Co1—N483.0(3)
N5—Co1—N497.75(18)N2—Co1—Br495.1(2)N2—Co1—Br193.98(18)
N5—Co1—N296.52(18)N4—Co1—N286.1(3)N3—Co1—N286.4(3)
N3—Co1—N486.20(18)N4—Co1—N386.1(3)N3—Co1—N486.5(3)
N3—Co1—N285.41(18)N3—Co1—Br494.1(2)N4—Co1—Br194.24(18)
N3—Co1—N584.18(19)N5—Co1—Br487.4(2)N5—Co1—Br189.91(18)
N6—Co1—N491.4(2)N5—Co1—N296.4(4)N5—Co1—N297.7(3)
N6—Co1—N297.32(19)N5—Co1—N486.6(3)N5—Co1—N385.9(3)
N6—Co1—N594.4(2)N5—Co1—N397.5(3)N5—Co1—N496.7(3)
Table A6. Bond distances (Å) and angles (°) for complexes of L2. Values in parentheses represent standard deviation of the last significant figure.
Table A6. Bond distances (Å) and angles (°) for complexes of L2. Values in parentheses represent standard deviation of the last significant figure.
C8 (M=Cu)C9 (M=Mn)
Cu1—N12.031(11)Mn1—N12.165(6)
Cu1—N22.26(3)Mn1—N22.333(16)
Cu1—N32.114(12)Mn1—N32.256(11)
Cu1—N42.368(18)Mn1—N42.26(2)
Cu1—N51.962(11)Mn1—N52.266(13)
Cu1—N62.011(11)Mn1—N62.173(10)
N1—Cu1—N278.7(11)N1—Mn1—N273.6(6)
N1—Cu1—N393.2(4)N1—Mn1—N3102.7(3)
N1—Cu1—N478.6(10)N1—Mn1—N472.2(7)
N2—Cu1—N4150.8(6)N1—Mn1—N5166.2(6)
N3—Cu1—N284.5(10)N1—Mn1—N6103.9(3)
N3—Cu1—N478.6(9)N3—Mn1—N281.2(6)
N5—Cu1—N1178.7(8)N3—Mn1—N476.9(7)
N5—Cu1—N2100.5(13)N3—Mn1—N579.2(5)
N5—Cu1—N385.7(5)N4—Mn1—N2133.6(4)
N5—Cu1—N4101.8(12)N4—Mn1—N595.2(7)
N5—Cu1—N682.4(5)N5—Mn1—N2120.1(7)
N6—Cu1—N198.8(4)N6—Mn1—N2111.0(7)
N6—Cu1—N297.2(12)N6—Mn1—N3153.0(4)
N6—Cu1—N3168.0(4)N6—Mn1—N4106.9(7)
N6—Cu1—N4104.3(10)N6—Mn1—N573.9(5)

Appendix A.3. Tables of Hydrogen Bonds

Table A7. Hydrogen bond data for C6. Symmetry operations: (i) 1 x , y , 1 z ; (ii) x, 1 2 y , 1 2 + z . Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
Table A7. Hydrogen bond data for C6. Symmetry operations: (i) 1 x , y , 1 z ; (ii) x, 1 2 y , 1 2 + z . Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
DistancesAngle
D—H1D—HHADAD—HA
N5—H5A⋯Br2i0.892.883.659(8)146
O1—H1A⋯Br2i0.83(13)2.86(13)3.355(11)120(10)
O1—H1B⋯Br3i0.81(6)2.58(7)3.368(11)164(7)
N2—H2⋯Br2i0.982.323.295(8)174
N5—H5B⋯Br2ii0.892.573.427(8)160
N4—H4⋯Br2ii0.982.443.384(8)161
N5—H5C⋯Br2i0.892.823.659(8)157
N5—H5D⋯Br2i0.892.643.427(8)147
1 D = donor, H = hydrogen, A = acceptor.
Table A8. Hydrogen bond data for C7. Symmetry operations: (i) 1 x , 1 y , 1 z . Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
Table A8. Hydrogen bond data for C7. Symmetry operations: (i) 1 x , 1 y , 1 z . Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
DistancesAngle
D—H1D—HHADAD—HA
N2—H2A⋯O13i0.982.233.125(10)152
N4—H4A⋯Br1i0.982.393.346(7)165
N5—H5A⋯O13i0.892.112.945(10)155
N5—H5B⋯Br1i0.892.703.476(7)147
1 D = donor, H = hydrogen, A = acceptor.
Table A9. Hydrogen bond data for C10. Symmetry operations: (i) 1 x , y, z; (ii) 1 x , 1 y , z ; (iii) 1 x , 2 y , 1 z ; (iv) 1 x , 1 + y , z. Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
Table A9. Hydrogen bond data for C10. Symmetry operations: (i) 1 x , y, z; (ii) 1 x , 1 y , z ; (iii) 1 x , 2 y , 1 z ; (iv) 1 x , 1 + y , z. Distances in Å, angles in °. Values in parentheses represent standard deviation of the last significant figure.
DistancesAngle
D—H1D—HHADAD—HA
O1—H1C⋯Br3i0.81(4)2.62(8)3.290(14)141(9)
O1—H1D⋯Br5ii0.83(11)2.50(10)3.324(13)175(9)
N2—H2 ⋯Br3i0.982.533.440(4)155
N4—H4 ⋯Br1iii0.982.713.550(4)144
N5—H5A⋯Br2ii0.892.673.364(6)135
N5—H5B⋯Br4iv0.892.483.316(6)158
N5—H5C⋯O10.892.503.277(16)147
N5—H5C⋯Br5ii0.892.933.637(6)138
1 D = donor, H = hydrogen, A = acceptor.

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Figure 1. Ligands used in this work and nitrogen atom numbering.
Figure 1. Ligands used in this work and nitrogen atom numbering.
Crystals 13 01338 g001
Figure 2. (ad) Asymmetric unit of structures C1C4 featuring Mn(II), Cu(II), Ni(II) or Zn(II), respectively. (e) Packing of C1 with [CuL3] 2 + depicted in red, and perchlorate anions in blue. (f) Spacefill of C4 highlighting the inaccessibility of the metal atom from the solvent.
Figure 2. (ad) Asymmetric unit of structures C1C4 featuring Mn(II), Cu(II), Ni(II) or Zn(II), respectively. (e) Packing of C1 with [CuL3] 2 + depicted in red, and perchlorate anions in blue. (f) Spacefill of C4 highlighting the inaccessibility of the metal atom from the solvent.
Crystals 13 01338 g002
Figure 3. (a) Details of the complex [CoBrL1] 2 + from C6. Hydrogen atoms not shown. (b) Detail of the complex [CoL3] 3 + from C5. Hydrogen atoms not shown. (c) Unit cell of C6 shown along the b-axis, displaying the packing and the internal hydrogen bonding structure. Hydrogen atoms not shown. (d) Unit cell of C7 shown along the b-axis with Na atoms displayed in polyhedral, carbon atoms in capped stick representation, and other atoms displayed in ball-and-stick. Hydrogen atoms not shown.
Figure 3. (a) Details of the complex [CoBrL1] 2 + from C6. Hydrogen atoms not shown. (b) Detail of the complex [CoL3] 3 + from C5. Hydrogen atoms not shown. (c) Unit cell of C6 shown along the b-axis, displaying the packing and the internal hydrogen bonding structure. Hydrogen atoms not shown. (d) Unit cell of C7 shown along the b-axis with Na atoms displayed in polyhedral, carbon atoms in capped stick representation, and other atoms displayed in ball-and-stick. Hydrogen atoms not shown.
Crystals 13 01338 g003
Figure 4. (a) Details of the complex [MnL2] 2 + from C8. (b) Details of the complex [CuL2] 2 + from C9. (c) Unit cell of C8 viewed down c axis. Hydrogen atoms omitted. Mn (purple), Cl (green), O (red), N (blue), C (gray).
Figure 4. (a) Details of the complex [MnL2] 2 + from C8. (b) Details of the complex [CuL2] 2 + from C9. (c) Unit cell of C8 viewed down c axis. Hydrogen atoms omitted. Mn (purple), Cl (green), O (red), N (blue), C (gray).
Crystals 13 01338 g004
Figure 5. Species distribution diagram for the system Cu(II) with L2 (left) and L3 (right) with [Cu 2 + ] = [L] = 1 × 10−3 m. Charges omitted.
Figure 5. Species distribution diagram for the system Cu(II) with L2 (left) and L3 (right) with [Cu 2 + ] = [L] = 1 × 10−3 m. Charges omitted.
Crystals 13 01338 g005
Figure 6. (a) Details of the complex [ZnBrHL1] 2 + from C10. (b) Hydrogen bonding network around the complex.
Figure 6. (a) Details of the complex [ZnBrHL1] 2 + from C10. (b) Hydrogen bonding network around the complex.
Crystals 13 01338 g006
Table 1. Formation constants for L3 with some metal ions from the first transition series.
Table 1. Formation constants for L3 with some metal ions from the first transition series.
Reaction 1Mn(II) 2Fe(II)Cu(II)Zn(II)
MH 2 L + H ⇌ MH3L6.35(7)  33.1(2)4.26(6)
MHL + H ⇌ MH 2 L5.79(9)5.87(5)3.59(7)5.32(3)
ML + H ⇌ MHL7.74(1)8.17(2)4.47(2)6.27(3)
M + L ⇌ ML10.93(1)13.29(4)22.90(2)17.72(3)
ML + H 2 O ⇌ LMOH + H−10.74(2)−10.64(4)−10.53(4)
1 Charges omitted. 2 Values from ref [9]. 3 Values represent log 10 K , values in parentheses represent standard deviation of the last significant figure.
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Blasco, S.; Verdejo, B.; Clares, M.P.; García-España, E. Transition Metals Meet Scorpiand-like Ligands. Crystals 2023, 13, 1338. https://doi.org/10.3390/cryst13091338

AMA Style

Blasco S, Verdejo B, Clares MP, García-España E. Transition Metals Meet Scorpiand-like Ligands. Crystals. 2023; 13(9):1338. https://doi.org/10.3390/cryst13091338

Chicago/Turabian Style

Blasco, Salvador, Begoña Verdejo, María Paz Clares, and Enrique García-España. 2023. "Transition Metals Meet Scorpiand-like Ligands" Crystals 13, no. 9: 1338. https://doi.org/10.3390/cryst13091338

APA Style

Blasco, S., Verdejo, B., Clares, M. P., & García-España, E. (2023). Transition Metals Meet Scorpiand-like Ligands. Crystals, 13(9), 1338. https://doi.org/10.3390/cryst13091338

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