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Arthur Schweiger

Publications and source records attributed to Arthur Schweiger.

33 records · Page 2Linked to original sources

Hyperfine decoupling in electron paramagnetic resonance as a powerful tool for unraveling complicated ESEEM spectra of S=1/2, I> or =1/2 systems.

Hyperfine decoupling in electron paramagnetic resonance after strong microwave radiation is studied for S=1/2, I=1/2 and S=1/2, I=1 spin systems. A new 2D pulse sequence based on the hyperfine-decoupled DEFENCE (deadtime-free ESEEM by nuclear coherence-transfer echoes) experiment is introduced, which is distinguished by a remarkable reduction of the residual hyperfine coupling. The efficiency of this new decoupling experiment in comparison to the old pulse sequence is studied by means of numerical simulations. The advantages of the new decoupling experiment and its ability to simplify ESEEM spectra are experimentally demonstrated on two disordered systems.

Journal Article↗

Absorption line CW EPR using an amplitude modulated longitudinal field.

In standard continuous wave electron paramagnetic resonance (CW-EPR) experiments, the first derivative of absorption lines is detected. This type of a line shape is caused by the magnetic field modulation and is usually an undesired feature, since the sensitivity of CW-EPR drastically decreases with increasing linewidth. A new approach is introduced, which allows for the measurement of absorption line EPR spectra in systems with broad inhomogeneous lines. The method makes use of multiple-photon transitions that are induced in spin systems when a transverse microwave and a longitudinal radio frequency field are simultaneously applied. The absorption lines are obtained by using amplitude modulation of the radio frequency field and slight saturation of the spectral lines. The basics of the new approach are discussed and experimental examples are given.

Journal Article↗

Tropad: a new ligand for the synthesis of water-stable paramagnetic [16+1]-electron rhodium and iridium complexes.

The new tetradentate ligand 1,4-bis(5 H-dibenzo[a,d]cyclohepten-5-yl)-1,4-diazabuta-1,3-diene ((H)tropdad) allows the syntheses of the 16-electron cationic rhodium complexes [M((H)tropdad)](O(3)SCF(3)) (M=Rh, Ir). The structure of the rhodium complex was determined by X-ray analysis and points to a description of these as [M(+1)((H)tropdad)(0)] with short Cd-N bonds (av 1.285 A) and a long C-C bond (1.46 A) in the diazabutadiene (dad) moiety, that is the M-->dad charge-transfer is negligible. Both [Rh((H)tropdad)](+) and [Ir((H)tropdad)](+) are reduced at very low potentials (E(1) (1/2)= -0.56 V and E(1) (1/2)=-0.35 V, respectively) which allowed the quantitative synthesis of the neutral paramagnetic complexes [M((H)tropdad)](0) (M=Rh, Ir) by reacting the cationic precursor complexes simply with zinc powder. The [M((H)tropdad)](0) complexes are stable against protic reagents in organic solvents. Continuous wave and pulse EPR spectroscopy was used to characterize the paramagnetic species and the hyperfine coupling constants were determined: [Rh((H)tropdad)](0): A(iso)((14)N)=11.9 MHz, A(iso)((1)H)=14.3 MHz, A(iso)((103)Rh)= -5.3 MHz; [Ir((H)tropdad)](0): A(iso)((14)N)=11.9 MHz, A(iso)((1)H)=14.3 MHz. In combination with DFT calculations, the experimentally determined g and hyperfine matrices could be orientated within the molecular frame and the dominant spin density contributions were determined. These results clearly show that the complexes [M((H)tropdad)](0) are best described as [M(+1)((H)tropdad)(.-)] with a [16+1] electron configuration.

Journal Article↗

Spectroscopic investigations of bis(sulfoximine) copper(II) complexes and their relevance in asymmetric catalysis.

The structure of Cu(II) complex 3 formed within the course of a stereoselective Diels-Alder reaction was investigated by EXAFS, CW-EPR at X- and W-band, HYSCORE, pulsed ENDOR, and UV-vis spectroscopy. The experimental techniques indicate that the chiral bis(sulfoximine) ligand (S,S)-1 and the dienophile form a tetragonally distorted complex in CH(2)Cl(2). The ligand binds to the Cu(II) center via the imine nitrogens, whereas the dienophile interacts via the carbonyl oxygen atoms. The additional sites of the first coordination sphere are occupied by counterions and, presumably, solvent molecules. At the axial position, a triflate anion binds via an oxygen atom.

Journal Article↗

Axial solvent coordination in "base-fff" cob(II)alamin and related co(II)-corrinates revealed by 2D-EPR.

Detailed information on the structure of cobalt(II) corrinates is of interest in the context of studies on the coenzyme B(12) catalyzed enzymatic reactions, where cob(II)alamin has been identified as a reaction intermediate. Cob(II)ester (heptamethyl cobyrinate perchlorate) is found to be soluble in both polar and nonpolar solvents and is therefore very suitable to study solvent effects on Co(II) corrinates. In the literature, Co(II) corrinates in solution are often addressed as four-coordinated Co(II) corrins. However, using a combination of continuous-wave (CW) and pulse electron paramagnetic resonance (EPR) and pulse ENDOR (electron nuclear double resonance) at different microwave frequencies we clearly prove axial ligation for Cob(II)ester and the base-off form of cob(II)alamin (B(12r)) in different solvents. This goal is achieved by the analysis of the g values, and the hyperfine couplings of cobalt, some corrin nitrogens and hydrogens, and solvent protons. These parameters are shown to be very sensitive to changes in the solvent ligation. Density functional computations (DFT) facilitate largely the interpretation of the EPR data. In the CW-EPR spectrum of Cob(II)ester in methanol, a second component appears below 100 K. Different cooling experiments suggest that this observation is related to the phase transition of methanol from the alpha-phase to the glassy state. A detailed analysis of the EPR parameters indicates that this transition induces a change from a five-coordinated (above 100 K) to a six-coordinated (below 100 K) Co(II) corrin. In a CH(3)OH:H(2)O mixture the phase-transition properties alter and only the five-coordinated form is detected for Cob(II)ester and for base-off B(12r) at all temperatures. Our study thus shows that the characteristics of the solvent can have a large influence on the structure of Co(II) corrinates and that comparison with the protein-embedded cofactor requires some caution. Finally, the spectral similarities between Cob(II)ester and base-off B(12r) prove the analogies in their electronic structure.

Cobalt↗

Coenzyme B induced coordination of coenzyme M via its thiol group to Ni(I) of F430 in active methyl-coenzyme M reductase.

Methyl-coenzyme M reductase (MCR) catalyzes the reaction of methyl-coenzyme M (CH3-S-CoM) with coenzyme B (HS-CoB) to methane and CoM-S-S-CoB. At the active site, it contains the nickel porphinoid F430, which has to be in the Ni(I) oxidation state for the enzyme to be active. How the substrates interact with the active site Ni(I) has remained elusive. We report here that coenzyme M (HS-CoM), which is a reversible competitive inhibitor to methyl-coenzyme M, interacts with its thiol group with the Ni(I) and that for interaction the simultaneous presence of coenzyme B is required. The evidence is based on X-band continuous wave EPR and Q-band hyperfine sublevel correlation spectroscopy of MCR in the red2 state induced with 33S-labeled coenzyme M and unlabeled coenzyme B.

Electron Spin Resonance Spectroscopy↗

Novel routes to Cu(salicylaldimine) covalently bound to silica: combined pulse EPR and in situ attenuated total reflection-IR studies of the immobilization.

Several novel routes for the immobilization of modified Cu(salicylaldimine) complexes on commercially available silica are described. New pulse electron paramagnetic resonance (EPR) and electron-nuclear double resonance sequences, which provide more detailed information than that available previously, in combination with continuous wave EPR, allow a definitive assignment of the geometry at the copper center in the immobilized Cu(salicylaldimine). Immobilization of the modified Cu(salicylaldimine) on silica was followed in situ by monitoring the intensity of the characteristic free- and metal-coordinated imine bands as a function of time using attenuated total reflectance IR spectroscopy. On the basis of these studies, the outcome of the Schiff base condensation of Cu-bis(salicylaldehyde) with gamma-aminopropyl-modified silica gel is shown to provide immobilized trans-O(2)N(2)- and O(3)N-coordinated immobilized Cu(salicylaldimine)-type compounds. In addition, trans-O(2)N(2)- or O(3)N-coordinated copper centers are selectively prepared on silica by controlling the aminopropyl modifier loading, thus opening a route to compounds not available by conventional synthesis. The O(3)N-coordinated Cu(salicylaldimine)-type compound on silica was investigated as a precursor for the synthesis of a tethered chiral Cu(salicylaldimine) via reaction of the coordinated carbonyl group with (R)-(+)-alpha-methylbenzylamine. Supported Cu(salicylaldimine) was also prepared via the immobilization of the appropriate silylethoxy-modified homogeneous precursor on silica gel. Precursors and silica-supported Cu(salicylaldimine) materials have been fully characterized. Comparisons are drawn with related Cu(salicylaldimine) immobilized in silica aerogels.

Journal Article↗

Dendritic metalloporphyrins with a distal H-bond donor as mimics of haemoglobin.

We report the synthesis of iron(II) porphyrins functionalised with first- and second-generation dendrons as mimics of haemoglobin. The porphyrin core bears an ethynyl linker pointing towards the centre of the molecule, in an ideal position for the introduction of a series of distal ligands as potential H-bond donors by Pd0-catalysed Sonogashira cross-coupling.

Crystallography, X-Ray↗

Characterization of the MCRred2 form of methyl-coenzyme M reductase: a pulse EPR and ENDOR study.

Methyl-coenzyme M reductase (MCR), which catalyses the reduction of methyl-coenzyme M (CH(3)-S-CoM) with coenzyme B (H-S-CoB) to CH(4) and CoM-S-S-CoB, contains the nickel porphinoid F430 as prosthetic group. The active enzyme exhibits the Ni(I)-derived axial EPR signal MCR(red1) both in the absence and presence of the substrates. When the enzyme is competitively inhibited by coenzyme M (HS-CoM) the MCR(red1) signal is partially converted into the rhombic EPR signal MCR(red2). To obtain deeper insight into the geometric and electronic structure of the red2 form, pulse EPR and ENDOR spectroscopy at X- and Q-band microwave frequencies was used. Hyperfine interactions of the four pyrrole nitrogens were determined from ENDOR and HYSCORE data, which revealed two sets of nitrogens with hyperfine couplings differing by about a factor of two. In addition, ENDOR data enabled observation of two nearly isotropic (1)H hyperfine interactions. Both the nitrogen and proton data indicate that the substrate analogue coenzyme M is axially coordinated to Ni(I) in the MCR(red2) state.

Algorithms↗

Stability and Cu(II) binding of prion protein variants related to inherited human prion diseases.

All inherited forms of human prion diseases are linked with mutations in the prion protein (PrP) gene. Here we have investigated the stability and Cu(II) binding properties of three recombinant variants of murine full-length PrP(23-231)-containing destabilizing point mutations that are associated with human Gerstmann-Sträussler-Scheinker disease (F198S), Creutzfeld-Jakob disease (E200K), and fatal familial insomnia (D178N) by electron paramagnetic resonance and circular dichroism spectroscopy. Furthermore, we analyzed the variants H140S, H177S, and H187S of the isolated C-terminal domain of murine PrP, mPrP(121-231), to test a role of the histidine residues in Cu(II) binding. The F198S and E200K variants of PrP(23-231) differed in Cu(II) binding from the wild-type mPrP(23-231). However, circular dichroism spectroscopy indicated that the variants and the wild type did not undergo conformational changes in the presence of Cu(II). The D178N variant showed a high tendency to aggregate at pH 7.4 both with and without Cu(II). At lower pH values, it showed the same Cu(II) binding behavior as the wild type. The analysis allowed for a better location of the Cu(II) binding sites in the C-terminal part of the protein. Our present data indicate that hereditary forms of prion diseases cannot be rationalized on the basis of altered Cu(II) binding or mutation-induced protein destabilization alone.

Copper↗

The continuous wave electron paramagnetic resonance experiment revisited.

When the modulation frequency used in continuous wave electron paramagnetic resonance (cw EPR) spectroscopy exceeds the linewidth, modulation sidebands appear in the spectrum. It is shown theoretically and experimentally that these sidebands are actually multiple photon transitions, sigma(+)+kxpi, where one microwave (mw) sigma(+) photon is absorbed from the mw radiation field and an arbitrary number k of radio frequency (rf) pi photons are absorbed from or emitted to the modulation rf field. Furthermore, it is demonstrated that both the derivative shape of the lines in standard cw EPR spectra and the distortions due to overmodulation are caused by the unresolved sideband pattern of these lines. The single-photon transition does not even give a contribution to the first-harmonic cw EPR signal. Multiple photon transitions are described semiclassically in a toggling frame and their existence is proven using second quantization. With the toggling frame approach and perturbation theory an effective Hamiltonian for an arbitrary sideband transition is derived. Based on the effective Hamiltonians an expression for the steady-state density operator in the singly rotating frame is derived, completely describing all sidebands in all modulation frequency harmonics of the cw EPR signal. The relative intensities of the sidebands are found to depend in a very sensitive way on the actual rf amplitude and the saturation of single sidebands is shown to depend strongly on the effective field amplitude of the multiple photon transitions. By comparison with the analogous solutions for frequency-modulation EPR it is shown that the field-modulation and the frequency-modulation technique are not equivalent. The experimental data fully verify the theoretical predictions with respect to intensities and lineshapes.

Journal Article↗

Measurement of spin-lattice relaxation times in EPR with enhanced orientation selectivity.

Two schemes for the measurement of orientation-dependent spin-lattice relaxation times are introduced, which combine the inversion-recovery experiment with electron-Zeeman-resolved or right-angle wiggling EPR. The principles of the experiments are outlined and their performance is illustrated by examples of application. With the electron Zeeman-resolved approach the relaxation times of two metal complexes with different g values are unraveled, whereas with right-angle wiggling the orientation-dependent relaxation behavior of a metal complex with large hyperfine anisotropy is analyzed.

Journal Article↗

Rapid construction of solid-state magnetic resonance powder spectra from frequencies and amplitudes as applied to ESEEM.

In many Fourier-transform spectroscopies, such as pulse magnetic resonance (NMR, EPR), time-domain signals are acquired. Parameters are extracted from these signals by fitting numerical simulations to the experimental data. At present, simulations are often performed in frequency domain (FD). These computations generate a list of frequencies and amplitudes associated with the complex exponential components evolving during one or several variable time intervals. In order to compare simulations with experiments, this peak list is converted to a finite-length time-domain (TD) signal. This can be achieved either by directly evoluting the exponentials in time (direct method) or by rounding their frequencies and binning their amplitudes into a frequency-domain array (histogram method). The first approach is equivalent to a brute-force TD simulation and is slow for a large number of peaks. The second approach is a fast, but very crude approximation and is usually applied without considering in detail the errors involved. A third method introduced and illustrated here is based on the convolution and deconvolution of a short finite impulse response filter kernel. This convolution approach is much faster than the direct method and by orders of magnitude more accurate than the histogram method. For both TD and FD signals a detailed analysis of the errors and of the associated computational costs is presented. The convolution approach is applicable to any simulation problem where TD signals consist of a large number of complex exponentials. In particular, it is the method of choice for simulating 1D and 2D electron spin echo envelope modulation (ESEEM) spectra of disordered systems.

Algorithms↗

Effects of the dendrimer cage on O2 binding of dendritic cobalt(II) porphyrins.

Two types of dendritically functionalized cobalt(II) porphyrins were prepared and investigated in the presence of 1,2-dimethylimidazole, pyridine, and 1-methylimidazole. Continuous-wave (CW) and pulse electron paramagnetic resonance (EPR) and electron nuclear double resonance (ENDOR) techniques revealed specific information on the oxygenated forms of these porphyrins. The ENDOR and hyperfine sublevel correlation (HYSCORE) spectra showed that in [1.CoII.1,2.DiMelm]-O2, with secondary amide moieties in the dendritic branching, no hydrogen bond forms between the bound O2 and a dendritic amide NH moiety. This hydrogen bond had earlier been proposed on basis of the large dioxygen affinity of the corresponding FeII complex. For both [1.CoII.1,2-DiMelm]-O2 and the ester derivative [2.CoII.1,2-DiMelm]-O2, which lacks H-donor centers in the periphery of the porphyrin, ENDOR experiments clearly showed that the dendritic branches are closely packed in toluene. The analysis of the g values, the cobalt hyperfine interactions, and the hyperfine and nuclear quadrupole couplings of the directly coordinated nitrogen of the axial base showed an increased ionicity in the cobalt-dioxygen bond for [1.CoII.1,2-DiMelm]-O2. This observation is linked to the packing and the polarity of the dendritic branches and can be related to the O2 and CO affinity of the corresponding FeII complexes.

Journal Article↗

High-resolution EPR spectroscopic investigations of a homologous set of d9-cobalt(0), d9-rhodium(0), and d9-iridium(0) complexes.

The 17-electron complexes [M(tropp(ph))2] (M=Co0, Rh0, Ir0) were prepared and isolated (tropp = tropylidene phosphane). A structural analysis of [Co(tropp(ph))2] revealed this complex to be almost tetrahedral, while the heavier homologues have more planar structures. Partially deuterated tropp complexes [D6][M(tropp(ph))2] were synthesised for M = Rh and Ir in order to enhance the resolution in the EPR spectra. This synthesis involves a four-fold intramolecular C-H activation reaction, whereby alkyl groups are transformed into olefins. Dihydrides were observed as intermediates for M = Ir. The electronic and geometric structures of all complexes [M(tropp(ph))2] (M = Co, Rh, Ir) and [D6][M(tropp(ph))2] (M = Rh, Ir) were investigated by continuous wave (CW) and echo-detected EPR in combination with pulse ENDOR and ESEEM techniques. In accord with their planar structures, cis and trans isomers were detected for [M(tropp(ph))2] (M = Rh0, Ir0) for which a dynamic equilibrium was established. The thermodynamic data show that the cis isomer is slightly preferred by deltaH(o) = -4.7 +/- 0.3 kJ mol(-1) (M = Rh) and delta H(o) = -5.1 +/- 0.5 kJ mol(-1); (M = Ir). The entropies for the process trans-[M(tropp(ph))2] <==> cis-[M(tropp(ph))2] are also negative [deltaS(o) = -5 +/- 1.5 J mol(-1) (M = Rh); deltaS(o) = -17 +/- 3.7 J mol(-1) (M = Rh)], indicating higher steric congestion in the cis isomers. The cobalt(0) and irdium(0) complexes show rather large g anisotropies, while that of the rhodium(0) complex is small (Co: g(parallel) = 2.320, g(perpendicular) = 2.080; cis-Rh: g(parallel) = 2.030, g(perpendicular) = 2.0135; trans-Rh: g(parallel) = 2.050, g(perpendicular) = 2.030; cis-Ir: g(parallel) = 2.030, g(perpendicular) = 2.060; trans-Ir: g(parallel) = 1.980, g(perpendicular) = 2.150). The g matrices of [M(tropp(ph))2] (M = Co, Rh) are axially symmetric with g(parallel) > g(perpendicular), indicating either a distorted square planar structure (SOMO essentially d(x2 - y2) or a compressed tetrahedron (SOMO essentially d(xy)). Interestingly, for [Ir(tropp(ph))2] the inverse ordering, g(perpendicular) > g(parallel) is found; this cannot be explained by simple ligand field arguments and must await a more sophisticated analysis. The hyperfine interactions of the unpaired electron with the metal nuclei, phosphorus nuclei, protons, deuterons and carbon nuclei were determined. By comparison with atomic constants, the spin densities on these centres were estimated and found to be small. However, the good agreement of the distance between the olefinic protons and the metal centres determined from the dipolar coupling parameter indicates that the unpaired electron is primarily located at the metal centre.

Journal Article↗