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Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2: Structures of a Precursor [L3CuI(NCCH3)](BF4), L3 = Tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane and of its Oxidation Product [L3CuII(-OH)2CuIIL3](BF4)2 with Strong Antiferromagneti

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Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2:

Structures of a Precursor [L3CuI(NCCH3)](BF4), L3 = Tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane and of its

Oxidation Product [L3CuII(-OH)2CuIIL3](BF4)2 with Strong Antiferromagnetic Spin-Spin Coupling

KAIM, Wolfgang, et al .

Abstract

The molecular structure of the highly oxygen-sensitive complex [L3CuI(NCCH3)](BF4) (1) reveals approximately symmetrical coordination by the fac-tridentate (tripodal) ligand L3 = tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane and a rather short CuI-N(acetonitrile) distance of 1.865(5) Å. In CH2Cl2 at -78 °C the colourless compound reacts with O2 to yield a labile purple intermediate (max 517 nm) - presumably a peroxodicopper(II) complex - which decomposes at -30 °C. No such intermediate was observed on reaction of the CuI complex of bis(2-pyridylmethyl)benzylamine with O2 at -80 °C. However, an EPR spectrum with g = 2.17 and g = 2.03 without 63,65Cu hyperfine splitting was observed at low temperatures. Exposure of the precursor 1 to air under ambient conditions yields dinuclear [L3CuII(-OH)2CuIIL3](BF4)2 (2) which exhibits an EPR detectable dissociation into monomers in CH2Cl2 solution. The structure of the hexakis(dichloromethane) solvate of 2 with Cu-Cu and Cu-O distances of 3.055 and 1.94Å, respectively, is typical for dihydroxo-bridged dicopper compounds with square-pyramidal CuII configuration ( = 0.03), [...]

KAIM, Wolfgang, et al . Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2:

Structures of a Precursor [L3CuI(NCCH3)](BF4), L3 =

Tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane and of its Oxidation Product

[L3CuII(-OH)2CuIIL3](BF4)2 with Strong Antiferromagnetic Spin-Spin Coupling. Zeitschrift für anorganische und allgemeine Chemie , 2005, vol. 631, no. 13-14, p. 2568-2574

DOI : 10.1002/zaac.200500053

Available at:

http://archive-ouverte.unige.ch/unige:3316

Disclaimer: layout of this document may differ from the published version.

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Structures of a Precursor [L

3

Cu

I

(NCCH

3

)](BF

4

), L

3

Tris(3-isopropyl-4,5- trimethylenepyrazolyl)methane and of its Oxidation Product [L

3

Cu

II

(µ- OH)

2

Cu

II

L

3

](BF

4

)

2

with Strong Antiferromagnetic Spin-Spin Coupling

Wolfgang Kaima,*, Christoph Titzea, Thilo Schurra, Monika Siegera, Max Lawsonb, Jeanne Jordanovb, Darı´o Rojasc, Ana M. Garcı´ac, and Jorge Manzurc,*

aStuttgart, Institut für Anorganische Chemie der Universität

bGrenoble/France, Centre d’Etudes Nucle´aires

cSantiago/Chile, Departamento de Ciencia de Materiales, Facultad de Ciencias Fisicas y Matematicas, Universidad de Chile Received February 4th, 2005.

Dedicated to Professor Herbert W. Roesky on the Occasion of his 70. Birthday

Abstract. The molecular structure of the highly oxygen-sensitive complex [L3CuI(NCCH3)](BF4) (1) reveals approximately symme- trical coordination by the fac-tridentate (tripodal) ligand L3 tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane and a rather short CuI-N(acetonitrile) distance of 1.865(5) A˚ . In CH2Cl2 at

78°C the colourless compound reacts with O2to yield a labile purple intermediate (λmax517 nm) presumably a peroxodicop- per(II) complexwhich decomposes at30°C. No such intermedi- ate was observed on reaction of the CuIcomplex of bis(2-pyridyl- methyl)benzylamine with O2 at80°C. However, an EPR spec- trum withg2.17 andg2.03 without63,65Cu hyperfine split- ting was observed at low temperatures. Exposure of the precursor 1to air under ambient conditions yields dinuclear [L3CuII(µ-OH)2-

Introduction

The reaction of copper(I) complexes with dioxygen, O2, has been intensely researched in connection with the essential O2binding role of CuIin biology [1⫺7] and, more recently, in connection with the copper-based utilization of O2 for synthetic purposes such as stoichiometric and catalytic ver- sions of C-H activation reactions [8, 9]. Reversibly O2trans- porting hemocyanin as well as C-H bond activating en- zymes such as tyrosinase or dopamine-β-monooxygenase have been investigated as proteins and with regard to small molecular model complexes. Mononuclear and dinuclear electron transfer intermediates involving superoxo (O2·⫺) or peroxo (O22⫺) complexes of copper(II) have been identified spectroscopically and, in part, structurally [1⫺7]. Sterically hindered ligands proved to be advantageous to stabilize these intermediates, however, electronic and charge effects must also be considered.

* Prof. Dr. Wolfgang Kaim Institut für Anorganische Chemie Universität Stuttgart

Pfaffenwaldring 55 D-70550 Stuttgart Fax:49 711 685-4165

e-mail: [email protected]

CuIIL3](BF4)2 (2) which exhibits an EPR detectable dissociation into monomers in CH2Cl2solution. The structure of the hexakis- (dichloromethane) solvate of2 with CuCu and Cu-O distances of 3.055 and 1.94 A˚ , respectively, is typical for dihydroxo-bridged dicopper compounds with square-pyramidal CuII configuration 0.03), adopting an antiarrangement. In agreement with the relatively wide Cu-O-Cu angles of 103.5°an analysis of the tempe- rature dependence of the magnetic susceptibility revealed a rather strong (J⫽ ⫺633 cm⫺1) antiparallel spin-spin coupling. The effect is ascribed to the steric bulk of the ligand L3.

Keywords:Copper; Crystal structures; Magnetism; Tripodal ligands

Following reports of the successful use of tris(3-organo- pyrazolyl)borato(1-) complexes of copper in stabilizing oxy- genated intermediates [1a, 3⫺6] we have chosen a related neutral tris(3-isopropyl-4,5-trimethylenepyrazolyl)methane ligand L3[10a] in corresponding O2reaction studies using [L3CuI(NCCH3)](BF4) 1 as a precursor. We also describe the structure and magnetism of the final reaction product [L3CuII(µ-OH)2CuIIL3](BF4)2(2) in reference to the numer- ous magneto-structural correlations reported for complexes with the [Cu(µ-OH)2Cu]2⫹core [11⫺13, 14a]. Whereas tris- (pyrazolyl)methane ligands have rarely been used in copper/

dioxygen chemistry [1a, 10, 14], the corresponding product complexes with bis- and tris(2-pyridylmethyl)amine ligands are well established [1a, b, 6c-e, 7c, 13]. We therefore de- scribe EPR and UV-VIS spectroscopic results of low tem- perature reactions between the copper(I) complexes with both L3 and bis(2-pyridylmethyl)benzylamine with dioxy- gen.

Results and Discussion

Characterization of [L3CuI(NCCH3)](BF4) (1) The ligand L3 [10] reacts with [Cu(NCCH3)4](BF4) under argon to yield a very air-sensitive colourless complex [L3CuI(NCCH3)](BF4) (1).

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Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2

L3[Cu(NCCH3)4](BF4)[L3Cu(NCCH3)](BF4)3 CH3CN (1) Other such complexes with substituted tris(pyrazolyl)- borato(1-) or tris(pyrazolyl)methane ligands were found to be more tolerant towards O2[5, 6, 14]. In addition to the crystallographic characterization (Tabs. 1, 2, Fig. 1) the1H- NMR spectra support the composition of the compound, with slightly shifted resonances for the coordinated ligands [10a]. However, the C⬅N stretching band could not be de- tected by IR vibrational spectroscopy, in agreement with previous observations for coordinated nitrile ligands (van- ishing dipole moment change) [15]. Electrochemical oxi- dation of1in CH2Cl2/0.1 M Bu4NPF6occurred irreversibly at ⫹0.81 V vs. ferrocenium/ferrocene. This anodically shifted peak potential in comparison to that of analogous tris(pyrazolyl)borato(1-) complexes [5d] reflects the differ- ent charge (cationic vs. neutral).

Table 1Crystallographic data of compounds1and2·6 CH2Cl2

1 2·6 CH2Cl2

formula C28H40BCuF4N4 C62H82B2Cl12Cu2F8N12O2

mol mass 611.01 1753.5

crystal size /mm 0.10.10.1 0.40.30.1 crystal system monoclinic triclinic

space group P21/n P1

a/A˚ 13.433(4) 12.202(4)

b/A˚ 14.3089(4) 12.392(6)

c/A˚ 17.115(4) 16.732(5)

α/° 90 86.83(1)

β/° 104.61(2) 69.62(1)

γ/° 90 60.60(1)

V/A˚3 3201(2) 2045.4(13)

Z 4 1

ρcalc/g cm⫺3 1.585 1.424

hklrange 10 <h<16 16 <h<9

5 <k<17 16 <k<14

21 <l<20 22 <l<20

2θrange /° 3.552 3.856

µ(Mo Kα) /cm⫺1 9.15 9.77

reflection measured 6562 9902

indep. reflections 6298 9902

parameters 388 901

R1 0.0764 0.0684

wR2 0.1998 0.2128

The structure of the molecule1in the crystal (Fig. 1, Tab.

2) reveals an approximately symmetrical coordination of distorted tetrahedral copper(I) by the tripodal ligand L3. The CuI-N(acetonitrile) distance is rather short at

Z. Anorg. Allg. Chem.2005,631, 25682574 zaac.wiley-vch.de 2005 WILEY-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim 2569 Table 2Selected bond lengths/A˚ and angles/°for compound1in the crystal.

Cu1-N1 2.086(5) Cu1-N7 1.865(5)

Cu1-N5 2.098(5) N7-C2 1.134(7)

Cu1-N3 2.072(5) C2-C3 1.462(8)

N1-Cu1-N5 92.7(2) N7-Cu1-N5 119.6(2)

N5-Cu1-N3 85.2(2) N7-Cu1-N3 125.8(2)

N3-Cu1-N1 87.1(2) Cu1-N7-C2 172.6(5)

N7-Cu1-N1 133.0(2) N7-C2-C3 178.5(7)

Figure 1 Molecular structure of the cation in the crystal of [L3Cu(NCCH3)](BF4) (1).

1.865(5) A˚ [14b, 16], reflecting the good access of small molecules to the metal.

Reaction of copper(I) complexes with O2at low temperature

Addition of dry O2 to a cooled (⫺78°C) solution of1 in CH2Cl2resulted in the slow development of an intense pur- ple colour (λmax⫽517 nm). Such purple colours and corre- sponding absorption maxima between 500 and 600 nm have been observed previously for solution-generated and iso- lated intermediates from reactions between O2 and cop- per(I) model complexes [3⫺6], including a tris(3,5-dimeth- ylpyrazolyl)methane compound [14a], or oxy-hemocyanin [3], they are assigned to ligand-to-metal charge transfer (LMCT) transitions of µ-peroxodicopper(II) species re- sulting from electron transfer between O22⫺and CuII[2, 3].

Intense bands around 340 or 400 nm which are usually found for bis(side-on) coordinated peroxodicopper(II) spec- ies [1, 4⫺6, 14a] or for bis(µ-oxo)-bridged dicopper(III) sys- tems [1a], respectively, were not observed; according to es- tablished correlations [1a] these data would be more com- patible with an end-on coordination despite the merely tri- dentate nature of the ligand L3. The related complex with

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tris(3,5-dimethylpyrazolyl)methane showed bands at 518 and 332 nm [14a].

Attempts to reverse the O2addition reaction by bubbling argon through the system in dilute solutions were unsuc- cessful as evident from the remaining colour, indicating an irreversible O2 binding process in contrast to the reactivity of the hemocyanin proteins. A copper(II) EPR signal at g⫽2.292 (A⫽16.0 mT,63,65Cu with I⫽3/2) and g⫽ 2.063 was observed in frozen solution, suggesting some de- composition to monomers [17]. Removal of the solvent at

⫺60°C gave a purple residue which rapidly decomposed at

⫺30°C to a green material as reported before for related systems [13, 18, 19]. The irreversibility of O2 binding and the thermal lability distinguish the compound described here from related tris(pyrazolyl)borato(1-) complexes [4, 5]

or from the analogue with tris(3,5-dimethylpyrazolyl)meth- ane [14a].

The successful use of tris(2-pyridylalkyl)amine ligands in copper/dioxygen chemistry [6c-g, 18] has prompted us to study the solely tridentate but also established [13] ligand bis(2-pyridylmethyl)benzylamine in a similar experiment.

The final dicopper(II) product with bridging hydroxide li- gands has been characterized with respect to structure and magnetism [13]. While single crystals of a copper(I) com- plex with bis(2-pyridylmethyl)benzylamine could not be ob- tained, such solutions obtained from the ligand and [Cu(NCCH3)4](BF4) in CH2Cl2reacted rapidly with dry O2 even at ⫺90°C without showing typical peroxo-to-cop- per(II) LMCT transitions. The only absorption observed was that of the final bis(hydroxo)bridged product with a ligand-field band at 610 nm (see below). We attribute this high reactivity to a lack of steric shielding or electronic sta- bilization by the bis(2-pyridylmethyl)benzylamine ligand.

However, EPR experiments showed the presence of a new signal at low temperatures (Fig. 2) different from the famil- iar trace spectra resulting from small amounts of mononu- clear CuII.

Figure 2X band EPR spectrum obtained from the reaction of a bis(2-pyridylmethyl)benzylamine-copper(I) solution in CH2Cl2 with O2at90°C.

This EPR signal has a diminishedg anisotropy ofg⫽ 2.17 and g ⫽ 2.03 without detectable 63,65Cu hyperfine splitting, suggesting considerable localization of spin on the ligand rather than on the metal(s) [2, 20, 21]. Tentatively one could attribute the signal to a metastable species formu- lated as either a superoxo complex [19] of dicopper(I) (see (6b)) or a valence-isomeric dicopper(I,II) mixed-valent

complex ofµ-peroxide (see (6c)), as suggested by a 1:3 stoi- chiometry between O2 and CuI compound. Although superoxide [7c] may be considered too oxidizing for cop- per(I) as evident from the function of Cu,Zn-superoxide dismutase enzymes [22] we have shown that the the formally related anion radicals of azo ligands (RN)2(RNZO) can accommodate copper(I) in stable and even structurally characterized dicopper(I)-radical complexes [23]. While the g anisotropies are smaller in these cases as evident from high-field EPR studies [24] they confirm the small metal hyperfine splitting < 2 mT in such a situation.

Formation, structure and magnetism of [L3CuII(µ- OH)2CuIIL3](BF4)2(2)

Reaction of the precursor1 with air at room temperature yields a dinuclear compound [L3Cu(µ-OH)2CuL3](BF4)2 (2).

4 [L3Cu(NCCH3)](BF4)O22 H2O

2 [L3Cu(µ-OH)2CuL3](BF4)24 CH3CN (2) Such species were frequently encountered as final prod- ucts from the reaction of copper(I) complexes with dioxy- gen [13, 14a, 18, 19]. The presence of hydroxo ligands is evident from a relatively narrow IR vibrational band at 3675 cm⫺1 , the tris(3,5-dimethylpyrazolyl)methane ana- logue [14a] shows 3650 cm⫺1. Furthermore, the absorption maxima at 663 nm (ε ⫽ 130 M⫺1 cm⫺1, ligand-field tran- sition) and 326 nm (ε ⫽ 3700 M⫺1 cm⫺1) agree with re- ported data for corresponding tris(3,5-dimethylpyrazo- lyl)methane (641 and 325 nm [14a]), tris(pyrazolyl)bor- ato(1-) [5a] and other such systems [1a, 18], the correspond- ing complex with di(2-pyridylmethyl)benzylamine has λmax⫽610 nm. The broadening of the1H-NMR spectrum and the observation of a copper(II)-type EPR signal with g ⫽ 2.298 (A ⫽ 14.2 mT) and g ⫽ 2.055 suggests dis- sociation (3) of the EPR-silent solid (4 K) in solution to yield [L3Cu(OH)(BF4)] with unknown metal coordination.

Quantitative EPR spectroscopy experiments according to AasaandVanngard[25] yielded about 40 % presence of the monomer in frozen dichloromethane solution.

[L3CuII(µ-OH)2CuIIL3](BF4)2v2 [L3CuII(OH)(BF4)] (3) The dissociation of such bis-hydroxo bridged dimers into mononuclear copper(II) complexes explains the ready con- version betweensynandantiisomers (cf. below).

Single crystals of the dinuclear compound were obtained as the hexakis(dichloromethane) solvate 2·6 CH2Cl2, whereas the dried powder analyzed as the bis(dichlorome- thane) solvate. The large number of partially labile solvent molecules in the crystal is held responsible for the relatively poor structure quality (Tabs. 1,3) which, however, reveals sufficient information to fit the compound into the vast number of bis(µ-hydroxo)dicopper(II) complexes [11⫺14, 19].

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Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2

The molecular structure of2 in the hexakis(dichlorome- thane) solvate crystal (Tab. 3, Fig. 3) shows an essentially planar [Cu2O2] core with the metals in square pyramidal (sqp) configuration. Theantiarrangement (Fig. 4) [14a] in contrast to possiblesynstructures [5a, 13] is observed here which also causes relatively [11⫺13] wide Cu-O-Cu angles at 103.5° and rather long Cu-O and Cu⫺Cu distances at about 1.94 A˚ and at 3.055(1) A˚, respectively.

Table 3Selected bond lengths/A˚ and angles/°for compound2in the crystal of2·6 CH2Cl2.

Cu1-O1 1.947(7) Cu2-N21 2.017(7)

Cu1-O2 1.944(8) Cu2-N31 2.021(9)

Cu2-O1 1.942(8) Cu1-N41 2.022(8)

Cu2-O2 1.949(8) Cu1-N51 2.029(11)

Cu1Cu2 3.0554(12) Cu1-N61 2.339(10)

Cu2-N11 2.356(9)

O1-Cu1-O2 76.5(3) N41-Cu1-N21 119.6(2)

O1-Cu2-O2 76.5(3) O2-Cu2-N11 104.9(3)

O1-Cu1-N41 170.8(4) O2-Cu2-N21 96.5(3)

O1-Cu1-N51 96.2(3) O2-Cu2-N31 170.0(4)

O1-Cu1-N61 104.0(3) N41-Cu1-N61 84.8(4)

O2-Cu1-N41 99.4(4) N41-Cu1-N51 86.5(4)

O2-Cu1-N51 169.0(4) N51-Cu1-N61 86.6(4)

O2-Cu1-N61 103.1(4) N21-Cu2-N11 87.7(3)

O1-Cu2-N11 103.0(4) N21-Cu2-N31 86.6(4)

O1-Cu2-N21 168.4(3) N31-Cu2-N11 84.7(3)

O1-Cu2-N31 98.8(3) Cu1-O2-Cu2 103.4(4)

N41-Cu1-N11 133.0(2) Cu1-O1-Cu2 103.6(3)

Figure 3 Molecular structure of the dication in the crystal of [L3Cu(µ-OH)2CuL3](BF4)2· 6 CH2Cl2.

Theτvalue typically used to assess the square-pyramidal or trigonal-bipyramidal characteristics of five-coordinated arrangements [26] is very low for2 atτ ⫽0.03, indicating essential square-pyramidal configuration.

τ(β-α)/60

β,α: basal angles;τ0 for square-pyramidal,τ1 for trigonal- bipyramidal configuration

Since the hydroxo oxygen atoms participate to make up the basal plane in2 (Fig. 4), the tripodal ligand L3 has to coordinate in a strongly unsymmetrical 2⫹1 fashion with two rather short Cu-N bonds at about 2.02 A˚ and one long

Z. Anorg. Allg. Chem.2005,631, 25682574 zaac.wiley-vch.de 2005 WILEY-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim 2571 Figure 4 Structure of the metal ion coordination spheres in the cation of [L3Cu(µ-OH)2CuL3](BF4)2· 6 CH2Cl2.

bond at ca. 2.35 A˚ as a result of the Jahn-Teller distortion.

Similar effects have been noted previously with unsym- metrical [13] or symmetrical [14a, 27] tripodal ligands.

In comparison to analogous compounds [LCu(µ- OH)2CuL] such as 3 [14a], 4 [4a] and5 [5a] with tris(3,5- dimethylpyrazolyl)methane (3), tris(3,5-dimethylpyrazo- lyl)borato(1-) (4) and tris(3,5-diisopropylpyrazolyl)bor- ato(1-) ligands L (5), respectively, the latter exhibits a syn configuration in the crystallized form isolated. The bonds to the apical nitrogen atoms are shorter in3(2.270(6) A˚ ) or 4(2.277(7) A˚ ) than in2at 2.356(9) A˚ or in5at 2.371(6) A˚ . On the other hand, the Cu⫺Cu distances are more similar for2 at 3.055(1) A˚ and4 (3.059(2) A˚ [4a]) than in 3 with 3.021(2) A˚ [14a] or in5 with 2.937(2) A˚ [5a]. This effect is related to similar angles Cu-O-Cu (ca. 103.4°⫺104.0°) and O-Cu-O (76.0°⫺76.5°) in theanti-configurated compounds 2 and 4 whereas syn-configurated 5 is distinguished by wider angles O-Cu-O at 79.2° and reduced angles Cu-O- Cu at 100.8° [5a]. The tris(3,5-dimethylpyrazolyl)methane analogue 3 [14a] adopts an intermediate position with 77.7(2)°and 102.4(2)°.

The dissociation (3) of bis-hydroxo bridged dimers into mononuclear copper(II) complexes explains the ready con- version between syn and anti isomers and their isolation depending on the solvent of crystallization, as was observed for compounds with di(2-pyridylmethyl)benzylamine [13].

The structural characteristics of2are reflected by the re- sults from a temperature dependence analysis of the mag- netic susceptibility (Fig. 5).

The classical analysis [11⫺14] using the Bleaney-Bowers equation [28] (Fig. 5) yields a very good fit with the ex- change coupling parameter J ⫽ ⫺633 cm⫺1, signifying strong antiferromagnetic coupling in agreement with the absence of EPR signals for the solid even at 4 K. This result is in agreement with reports [13] from related systems and with general guidelines as given in a paper byRuiz et al.

[12a]; the wide Cu-O-Cu angle, the rather long Cu-O bonds and the largely undistorted [Cu2O2] core of 2 all favour

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Figure 5 χT vs T plot for [L3Cu(µ-OH)2CuL3](BF4)2· 6 CH2Cl2: experimental data (o) and best fit (see text for details).

strong antiparallel spin-spin coupling. While the O-H vec- tors could not be determined in the solvate structure due to the insufficient crystal quality, it may be assumed due to steric requirements that they do not point significantly out of plane, which would also favor very negative J values [12a], relative to what might be estimated applying tra- ditional correlations betweenJ and the Cu-O-Cu angle or the Cu⫺Cu distance [11, 14a].

Summary and conclusion

The use of the tripodal ligand L3for copper complexes in- volved in the reactivity towards dioxygen has led to the iso- lation and structural characterization of a copper(I) precur- sor [L3Cu(NCCH3)](BF4) and of a dinuclear copper(II) end product [L3Cu(µ-OH)2CuL3](BF4)2 with strong antiferro- magnetic exchange coupling. A purple compound was ob- served as the intermediate product of an irreversible reac- tion between the precursor and dry O2at⫺78°C in CH2Cl2 however, it could not be characterized in detail because of its high lability. With the less sterically protecting bis(2-pyri- dylmethyl)benzylamine tripodal ligand such an intermedi- ate could not even be detected at ⫺80°C, however, a new kind of EPR signal was observed which was tentatively at- tributed to a superoxo complex of copper(I) (6b). Combin- ing these observations, including the formation of di- hydroxo-bridged final products such as 2 (7), with other literature results [1a, 7a, 18, 29, 30] leads to reaction schemes (4)-(7) for different O2/Cu ratios:

O21 LCuI ———씮LCuII(µ-O2앫⫺) [29] (4) O22 LCuI ———(LCuII)2(µ-O22⫺) (5a) or

O22 LCuI ———(LCuIII)2(µ-O2⫺)2[1a, 30] (5b) O23 LCuI ———씮(LCuII)2(LCuIII)(µ3-O2⫺)2[7a, 30] (6a) or

O23 LCuI ———(LCuI)2(µ-O2앫⫺)LCuII (6b) or

O23 LCuI ———씮(LCu1.5)2(µ-O22⫺)LCuII (6c)

O24 LCuI ———2 (LCuII)2(µ-O2⫺) [18] (7a) or

2 H

O24 LCuI ———(LCuII)2(µ-OH)22 LCuII (7b) or

2 H2O

O24 LCuI ———2 (LCuII)2(µ-OH)2[18] (7c) The lack of charge in both bis(2-pyridylmethyl)benzylam- ine and tris(pyrazolyl)methane as compared to tris(pyrazo- lyl)borato ligands is held responsible for this increased la- bility. In addition, the presence of benzylic/allylic functions in L3 or (2-pyridylmethyl)amine ligands may render these systems susceptible towards CH activation reactions be- cause of possible self-attack.Nevertheless, this study has once again [1a, 4⫺7] revealed that several factors determine the binding and activation of O2 by copper compounds.

New ligands will thus be tested in our laboratories in the directions of stabilizing intermediates or enhancing oxy- genating reactivity.

Experimental Section Instrumentation

EPR spectra were recorded in the X band on a Bruker System ESP 300 equipped with a Bruker ER035M gaussmeter and a HP 5350B microwave counter.1H-NMR spectra were taken on a Bruker AC 250 spectrometer, infrared spectra were obtained using Perkin Elmer 684 and 283 instruments. UV/Vis/NIR absorption spectra were recorded on Shimadzu UV160 and Bruins Instruments Omega 10 spectrophotometers. Cyclic voltammetry was carried out at 100 mV/s scan rate in dichloromethane/0.1 M Bu4NPF6using a three-electrode configuration (glassy carbon electrode, Pt counter electrode, Ag/AgCl reference) and a PAR 273 potentiostat and function generator. The ferrocene/ferrocenium couple served as in- ternal reference. Susceptibility measurements were carried out using previously described set-up and methodology [31]. The fitting was performed using the standard Bleaney-Bowers approach [28]

for dicopper(II) complexes [11⫺14].

Syntheses

The ligand L3 tris(3-isopropyl-4,5-trimethylenepyrazolyl)me- thane was obtained as described [10]. Products isolated from the reaction of bis(2-pyridylmethyl)benzylamine with copper precur- sors were reported [13].

[L3Cu(NCCH3)](BF4) (1)

A solution containing 102 mg (0.326 mmol) [Cu(NCCH3)4](BF4) [32] in 30 ml CH3OH was slowly added dropwise under argon to a solution of 150 mg (0.326 mmol) L3in 15 ml methanol. Following reflux for 2 hours the solvent was removed and the residue recrys- tallized from methanol. After two days at 15°C the colourless product was obtained in 58 % yield (123 mg). Mp 198°C. Calc. for C30H43BCuF4N7(652.1) C, 55.26; H, 6.65; N, 15.04 %. Found. C, 55.11; H, 6.76; N, 14.89 %.

1H-NMR(CDCl3):δ1.20 (d,J7 Hz, 18 H, CH(CH3)2), 2.35 (s, 3H, CH3CN), 2.55 (m, 12H, CH2), 2.96 (m, 6H, CH2, 3H, CH(CH3)2), 7.81 (s,

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Reactivity of Copper(I) Complexes with Tripodal Ligands towards O2

1H, CH).IR(CH2Cl2):ν˜2964 w, 2926 w, 2869 w, 2360 w, 1564 w, 1506 w, 1484 s, 1398 w, 1385 w, 1364 w, 1336 w, 1314 w, 1062 br, 1037 vs, 928 w, 859 w, 850 w, 824 w cm⫺1.

Low-temperature reactions with O2

Dry O2was slowly added to a cooled (78°C) solution of 100 mg (0.153 mmol)1 in 40 ml dichloromethane. The initially colourless solution turned pink and then dark purple within 30 minutes max517 nm). Attempts to reverse the reaction by bubbling ar- gon through the system in more dilute solutions were not success- ful, as evident from the remaining colour. Removal of the solvent at 60°C gave a purple residue which rapidly decomposed at

30°C to a green material. The thermal lability thus precluded further characterization.

In an analogous experiment, dry O2was slowly added to a cooled (90°C) solution of a 1:1 molar mixture of [Cu(NCCH3)4](BF4) [32] and bis(2-pyridylmethyl)benzylamine [13]. Before the initially yellowish solution turned blue at higher temperatures an axial EPR signal withg2.17 andg2.03 was observed.

[L3Cu(µ-OH)2CuL3](BF4)2·2 CH2Cl2(2·2 CH2Cl2)

A solution containing 100 mg (0.153 mmol)1in 20 ml CH2Cl2was stirred under open atmosphere for 5 minutes. After two days in air dark blue single crystals had formed which were collected and then carefully dried (42 mg, 22 %). Calc. for C56H82B2Cu2F8N12O2·2 CH2Cl2(1425.93): C, 48.85; H, 6.08; N, 11.79 %. Found: C, 48.67;

H, 6.08; N, 11.66 %.

UV/Vis (CH2Cl2):λmax (ε) 326 (3700), 663 (130) nm (M⫺1 cm⫺1).IR (KBr):ν˜3674 w, 2966 vs, 2867 s, 1564 w, 1485 vs, 1451 s, 1400 s, 1312 w, 1250 vs, 1060 vs, 924 s, 862 s, 736 s, 520 w, 487 w cm⫺1.

Crystallography

Single crystals were obtained from methanol at 15°C (1) and from the reaction mixture (2). The latter crystallized with six di- chloromethane molecules per formula unit. The X-ray data were collected at 188(2) K on a Siemens P4 diffractometer, using graph- ite monochromated Mo-Kα radiation (λ 0.71073 A˚ ) and em- ploying Wyckoff scans. Further details are given in Table 1. All structures were solved by the Patterson method using the SHELXTL package while refinement was carried out with SHELXL97 employing full-matrix least-squares methods on F2 with F02 ⱖ ⫺2σ(F02) [33]. All non-hydrogen atoms were refined anisotropically, hydrogen atoms were introduced using appropriate riding models.

Crystallographic data have been deposited with the Cambridge Crystallographic Data Centre, CCDC-262408 and 262409. Copies of the information may be obtained free of charge from: The Direc- tor, CCDC, 12 Union Road, Cambridge CB2 1EZ, UK (fax:

(⫹44)1223-336-033; e-mail: [email protected]; www: http://

www.ccdc.cam.ac.uk).

This work was supported by the Deutsche Forschungsgemeinschaft and FONDECYT (projects No. 1020101 and 7020101). We also thank Dr. W. Schwarz for crystallographic data collection.

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