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Lehrstuhl für Biophysik, Ruhr-Universität Bochum, D-44780 Bochum, Germany
Correspondence: Address reprint requests to Mathias Lübben, Tel.: +49-234-32-24465; Fax: +49-234-32-14626; E-mail: luebben{at}bph.rub.de.
| ABSTRACT |
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| INTRODUCTION |
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Previously applied techniques to study redox-dependent protonation changes suffer from specific limitations, although the recently reported development of the perfusion technique, using attenuated total reflectance (Nyquist et al., 2001
; Rich and Breton, 2002
) appears to be promising. However, the spectro-electrochemical cell requires highly concentrated protein solutions and the addition of redox mediators to secure redox equilibration. Moreover, it requires rather demanding technical equipment. On the other hand, the "caged electron" approach, using FMN as a photoreductant (termed "photoreduction"), allowed the use of highly concentrated samples, which were applied as thin hydrated films (Lübben and Gerwert, 1996
). Nevertheless, the difference signals in the spectral fingerprint region are significantly superimposed due to high background absorptions from the caged compound itself. (We use the term "fingerprint region" operationally to define the region of 11001680 cm1, which provides spectral information on amino acid side chains of proteins.) Slight variations in the photochemical reaction result in great changes and make spectral interpretation in this region a rather complex task. This is because it is intrinsically impossible to subtract the fractional contributions of the caged electron reaction itself from the total absorbance change of the photoreaction, as the light-driven electron transport from the mediator takes place only when a corresponding electron acceptor is present.
Consequently, it is necessary to find a reduction technique that provides reliable insights into the spectral region of 11001650 cm1. As reported earlier, heme proteins, in which the central iron is in the ferric state, can be photoreduced in the absence of external electron donors by irradiation with UV or visible light. Examples for this phenomenon are the one-electron transitions found in met-myoglobin, met-hemoglobin or p-450 hydroxylase and cytochrome c (Pierre et al., 1982
; Bazin et al., 1982
; Gu et al., 1993
; Sakai et al., 2000
). Aerobic light-induced electron transfer has also been examined for mitochondrial cytochrome c oxidase (Salmeen et al., 1978
; Adar and Yonetani, 1978
; Adar and Erecinska, 1979
; Babcock and Salmeen, 1979
; Ogura et al., 1985
; Brooks et al., 1997
).
In this report we use anaerobic auto-photoreduction via internal electron transfer to investigate cytochrome oxidases by means of FTIR spectroscopy, namely the ubiquinol oxidase cytochrome bo3 of Escherichia coli, and the cytochrome c oxidases of mitochondria and of the proteobacterium Rhodobacter sphaeroides. This photochemical autoreduction technique allows the detailed study of the IR fingerprint region, which is known to contain information on absorbances of specific functional groups of proteins.
| EXPERIMENTAL PROCEDURES |
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cyo (KanR), grown in Luria Broth medium in the presence of 50 µg/ml Kanamycin and 50 µg of Ampicillin to select for the cytochrome bo3 overproducer plasmid pHCL. The oligohistidine-tagged protein was isolated by a previously described procedure (Prutsch et al., 2000
R. sphaeroides strain YZ100, kindly donated by S. Ferguson-Miller (East Lansing, MI), was grown as described (Zhen et al., 1998
). The protocol was modified at the following stages: i), ß-n-dodecyl maltoside was used as the sole detergent; ii), membrane homogenization was carried out in 10 mM Tris-Cl, 40 mM KCl, pH 8.0; iii), the oxidase was solubilized in wash buffer (150 mM KCl, 20 mM Tris-Cl, 0.3% ß-n-dodecylmaltoside, pH 7.5) at a membrane protein concentration of 8 mg/ml with 1% detergent; iv), the Ni-NTA column was eluted with 50 mM histidine in wash buffer instead of imidazol; v), the cytochrome c oxidase was stored in 10 mM potassium phosphate buffer, 1 mM EDTA, 0.3% ß-n-dodecylmaltoside, pH 7.5.
Professor Peter Rich (London, UK) kindly donated the mitochondrial cytochrome c oxidase.
Other analytical methods
Protein concentration was determined by the bicinchoninic acid method (Smith et al., 1985
), with serum albumin as standard. Sodium dodecyl sulfate gel electrophoresis was carried out by the Laemmli method (Laemmli, 1970
). Oxidases were quantified with an Aminco (Silver Spring, MD) DW-2 split beam spectrometer using the extinction coefficients (reduced-oxidized enzymes) of 24,000 M1 x cm1 (605630 nm) (Vanneste, 1966
) for cytochrome c oxidase and of 18,700 M1 x cm1 (560580 nm) for ubiquinol oxidase (Kita et al., 1984
). Heme extraction and HPLC analysis were carried out as described above (Lübben and Morand, 1994
). For correction of variable heme recovery, internal standards were added to the samples before extraction; heme B was added to cytochrome c oxidase and heme A was added to ubiquinol oxidase samples. Ubiquinol oxidase activity (Prutsch et al., 2000
) and cytochrome c oxidase activity (Zhen et al., 1998
) were tested as previously reported.
Anaerobic semidry sample preparation
Samples were prepared for optical and for FTIR spectroscopy by applying them onto CaF2 windows and subsequently drying them in vacuo. Aliquots of the oxidases (15 µl) containing a total amount of up to 75 µg protein were pipetted into the center of a CaF2 plate, transferred to a workshop-modified desiccator and dried by membrane pump evacuation for defined time periods (15 min). After rehydration with H2O or D2O solvents, a CaF2 counter plate was pressed on top of the first one by means of a glass piston (details of the apparatus used for anaerobic sample preparation will be published elsewhere). This procedure enabled the adjustment of a sample layer thickness to <5 µm. The plate sandwich was sealed with Apiezon grease and placed in a workshop-made cuvette holder.
Anaerobic preparation of liquid samples
For the measurement of oxidase activity after irradiation, the protein samples were diluted (final concentration 0.2 mg/ml) in vacuum-degassed storage buffer. The sample was added to a stoppered quartz cuvette (0.1 mm pathlength) and exposed for 15 min to an argon atmosphere for removal of residual oxygen.
Optical spectroscopy of auto-photoreduced samples
To monitor cytochrome reduction in the photoreduction and auto-photoreduction experiments, optical spectra were recorded with a diode-array spectrophotometer, operated with monitoring light from a halogen lamp in the range of 3801000 nm. To obtain reasonable signal/noise ratios in the static spectra, 100 scans from an integration period of 0.1 s were averaged. For dynamic measurement of the CO recombination, samples were activated by a flash bulb (20 µs pulse length) and spectra were recorded in logarithmic time intervals over a total observation period of 0.5 s.
Photoirradiation methods
Laser irradiation
The samples were irradiated at 308 nm by a LPX 240i UV excimer laser (Lambda-Physik, Göttingen, Germany) with a pulse energy of 90100 mJ. Subsequently, the samples were placed in the diode-spectrophotometer after each series of flashes.
Lamp irradiation
When photoreduction was carried out with a Xe arc lamp (150 W; Oriel, Stratford, CT), the light source was adjusted to a 35° angle relative to the monitoring beam at a distance of 50 cm from the sample. The photolytic light intensity was greatly enhanced by placing a focusing quartz lens at the central point of the distance between lamp and sample (25 cm each), and this setting was termed "high intensity" conditions. To prevent sample denaturation, the light was heat filtered through an 8-cm cuvette containing water. Photoreduction rates of cytochrome bo3 were calculated after normalization of spectra to the absorbance value at the isosbestic wavelength of 545 nm (Kita et al., 1984
). The degree of reduction was determined from the absorbance difference between 560 and 545 nm of the
-band. For absolute quantification, fully reduced oxidase was prepared by photoreduction with FMN. The photon fluxes of the Xe lamp intensities in the range of 300400 nm (UG 1 filter DIN 58191 from Schott Glaswerke, Mainz, Germany) were determined with the chemical actinometer Aberchrome 540 (Heller and Langan, 1981
).
Recording of the photochemical action spectrum
To correct the wavelength-dependent emission of the Xe lamp, the monochromatic photon fluxes were quantified from actinometric measurements as described above. To achieve the same arbitrarily selected intensity of 5 x 1018 photons per cm2 at all wavelengths, the different irradiation times were adjusted accordingly. During sample irradiation, visible spectra were recorded; the absorbance changes at 560 nm indicated the levels of reduction of cytochrome bo3, which were plotted against the irradiation wavelengths.
FTIR spectroscopy
For routine spectra, 37 µg (samples in H2O) or 50 µg (samples in D2O) of cytochrome bo3 were applied between CaF2 windows as described above. The exact sample amounts were determined by visible redox difference spectra. About 75 µg of bacterial (R. sphaeroides) and mitochondrial cytochrome c oxidase was used. Static FTIR spectra were recorded with a Bruker IFS66v instrument (Karlsruhe, Germany), using a 2600 cm1 cutoff filter during all experiments, except for overview spectra taken to assess the degree of solvent isotope exchange. Nominal resolution was set to 2 cm1; all other conditions were as described above (Lübben et al., 1999
). The samples were thermostated at 4°C. Measurements were taken after irradiation periods of 20 s by a Xe lamp (see above) or a 100-W halogen lamp. Four-hundred scans in the single-sided forward/backward acquisition mode with a 100-kHz sampling rate were recorded. These measuring cycles were repeated until no further spectral changes were observed. To correct for possible temporal drifts in absorbance difference spectra, driftline subtraction was allowed using linear functions, extrapolated from absorbance values at three different wave numbers chosen from different regions of the MIR spectra (2000, 1960, and 1250 cm1). In spectra of cytochrome bo3, the samples yielded absorbance differences at 16961691 cm1 of 0.75 x 103. If minor deviations occurred, these values were used as a reference for scaling the spectra.
| RESULTS |
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1000 laser flashes at 308 nm (not shown) or 5 min continual UV irradiation with a Xe lamp at high light intensity (photon flux: 4.4 x 1015 photons per second per cm2), the oxidase reached almost 100% reduction, whereas prolonged irradiation led to a decrease in absorbance. This is probably due to the damaging effect of high light intensity, which is also accompanied by the photochemical formation of carbon monoxide (see below). Lower light intensity (photon flux: 1.1 x 1015 photons/s/cm2) required longer irradiation times (Fig. 1, A (squares) and B). Light from a halogen lamp (having a rather low UV content) yielded a very slight degree of reduction within the chosen observation time (not shown). The photoreduction effect of cytochrome bo3 and of cytochrome c oxidase has been tested in the presence of 3, 6, and 10 mM tryptophan as a potential external source of electrons, but the aromatic amino acid known to enhance reduction rates with other heme proteins (Pierre et al., 1982
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7.5 (not shown). The data precision does not allow the determination of exact pK values, but it indicates that at least one protonatable group is involved during a certain stage of the photochemical reaction pathway.
Heme composition of photoreduced oxidases
It has been reported that in met-hemoglobin the protein-associated heme group itself is responsible for internal electron transfer (Sakai et al., 2000
). Moreover, it is known that isolated heme B undergoes light-induced reduction in the presence of electron donors (Bartocci et al., 1980
). Cytochrome bo3 carries two heme groups with different chemical structures (Puustinen and Wikström, 1991
; Puustinen et al., 1992
; Rumbley et al., 1997
), namely hemes b (hexa-coordinated, low-spin) and o (penta-coordinated ligand binding, high-spin). To determine the role of these, the heme composition was analyzed after treatment with light at different intensities. The HPLC traces of the extracted hemes are displayed in Fig. 3. Hemes B and O of the untreated control sample were verified with standard compounds (Prutsch et al., 2000
). They exhibited peaks with the expected retention times of 35.6 and 55.3 min. After normalization with respect to their unequal extinction coefficients, the peak areas correspond to a 1:1 ratio of heme B:O (Rumbley et al., 1997
). Samples fully reduced by low intensities of the Xe lamp had the same heme composition as the nontreated reference. Upon irradiation with the focused Xe lamp, heme B was shown to be present in similar amounts, but the heme O peak vanished almost completely. The results are summarized in the inset of Fig. 3. The low-spin heme b of cytochrome bo3 remains unchanged, whereas the high-spin ligand binding heme o appears to be decomposed by very intense UV light. It is proposed that carbon monoxide is formed by the photodecay of heme o. Similar experiments with cytochrome aa3 of R. sphaeroides (not shown) demonstrate heme a degradation of >50% under the same conditions. The data suggest that farnesylated hemes are more susceptible to photochemical decomposition combined with CO release. These data do not allow the exclusion of the low-spin heme a as a possible target in cytochrome aa3.
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10% transmission. Having adjusted this condition (i.e., relatively low sample amounts), due to low signal intensities, it is difficult to evaluate slight absorbance variations outside the amide I spectral region.
General effect of photoirradiation on FTIR spectra (cytochrome bo3)
In the past, several people, including ourselves, have used FMN/EDTA as a caged electron donor for various heme-copper oxidases (Lübben and Gerwert, 1996
; Lübben et al., 1999
; Yamazaki et al., 1999a
) in infrared spectroscopy. The goal of this study is to produce redox FTIR spectra from cytochrome oxidases in the absence of (externally added) artificial electron donors to avoid spectral disturbance from byproducts of the electron transfer reaction. Therefore, redox spectra generated by different techniques were compared. Fig. 5 A displays the redox FTIR spectra of cytochrome bo3 recorded in the range of 16901990 cm1, using different light sources and reaction conditions. At
1960 cm1, the adducts of CO with ferrous high-spin heme (Fiamingo et al., 1986
; Hill et al., 1992
; Shapleigh et al., 1992
; Lemon et al., 1993
; Einarsdottir et al., 1993
; Rich and Breton, 2001
) could be observed. CO release occurs under intense irradiation seen in the laser-induced spectrum (Fig. 5 A, top). The use of lower light intensities from a Xe lamp with and without the presence of FMN (Fig. 5 A, middle and bottom) yields no or insignificant release of CO. The light-induced evolution of difference spectra by photoreduction and auto-photoreduction is compared on an expanded scale in Fig. 5 B. The similarity of spectra generated by both methods above 1680 cm1 is evident. In the photoreduction spectra, the so-called fingerprint region of the spectrum is partially obscured by the reaction products from the chemical electron transfer reaction. In the photoreduction spectra alone, the simple subtraction of absorbance contributions by caged compounds is not possible, because the oxidation of EDTA takes place only in the presence of a suitable electron acceptor, specifically the oxidase itself. In contrast, the auto-photoreduction spectra are remarkably reproducible; they are free of signals from photolytic byproducts (Fig. 5), e.g., the decomposition of EDTA, so in principle the spectra could be used for correction of contributions from caged compounds. Peaks at
1500 cm1 and 1320 cm1 in the auto-photoreduced spectrum are above the noise, and, in the absence of spectral contributions from caged compounds, can now be attributed to the protein itself. Notably, the majority of absorbance bands can be resolved in both types of photo-induced FTIR difference spectra. The spectral region of 16801800 cm1 is especially informative for the analysis of protonated carboxyl groups. All three ways of inducing the redox transition discussed above result in similar patterns at 1744/1735 cm1 (Fig. 5 A), reflecting a redox-driven environmental change, which had been previously assigned to
(C=O) signals from glutamic acid-286 (Lübben et al., 1999
; Hellwig et al., 1998
) located in the center of the D-channel of the catalytic subunit I. The band positions of absorbance maxima and minima from photoreduction were almost identical with those recorded by means of electrochemical equilibration (Hellwig et al., 1999a
). These difference absorbance features were much less pronounced in mutants containing aspartic acid in place of glutamic acid-286 (Lübben et al., 1999
). The different absorbance intensities of glutamic and of aspartic acid had been related to dissimilar interactions of the carboxyl groups with the hydrogen-bonded network located in the proton channel (Puustinen et al., 1997
). At 1198 cm1, there is a fingerprint absorbance feature, which is probably related to the
(C-O) of glutamic acid (Barth, 2000
) and which apparently arises from the same environmental change that was described for the
(C=O) band. This small band disappears upon solvent exchange to D2O (not shown) and it is absent in mutants affecting Glu-286 (e.g., in Glu-286-Asp (Fig. 6) or Glu-286-Gln (not shown)), but it is found reproducibly in other mutant oxidases in which Glu-286 is preserved (Fig. 6).
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16201650 cm1 are evident (Fig. 7), which is a further verification of molecular stability after photoirradiation. The data are highly reproducible, which is especially important for the fingerprint region; the FTIR difference spectra confirm our previous notion that spectral perturbations found with the reductant FMN/EDTA are also absent in this class of heme-copper oxidases. Although both cytochrome c oxidases are functionally equivalent, their redox FTIR spectra are remarkably different, when regions between 1700 and 1750 cm1 are compared. For example, the carbonyl signature band at 1745/1737 cm1 of the R. sphaeroides oxidase is moved to higher wavenumbers in the mitochondrial enzyme, whereas the positive absorbance change of the latter is shifted to 1717 cm1. This could be due to the extra subunits in the mitochondrial oxidase, which provide the enzyme with a number of additional functional groups that may be involved within the redox-induced rearrangement. Clear band shifts are seen in the difference spectra after solvent replacement by D2O, which result from oscillator mass enhancements after proton/deuteron exchange. The fingerprint region is resolved unambiguously; the spectral comparison of Rhodobacter oxidase mutants dissolved in H2O and D2O will elucidate a number of specific band assignments in the respective region. | DISCUSSION |
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Release of carbon monoxide
Auto-photoreduction could be measured at low light intensities; significant release of CO was observed at a much higher radiation. The mechanism of CO production is of particular interest and will be discussed in greater detail elsewhere. In the context of our objectives, i.e., to establish appropriate auto-photoreduction conditions, CO release has to be suppressed to ensure that the protein is in a chemically unperturbed state. The heme a and o groups (i.e., the high-spin hemes) are most probably the source of carbon monoxide, because no other photochemically active additives were present. In the case of cytochrome bo3, the heme o group is preferentially decomposed during high-intensity irradiation, whereas the low-spin heme b group remains unaffected (Fig. 3). One might conclude that farnesylated heme groups are more susceptible to light-induced decomposition than the short-chain substituted iron-protoporphyrin. For the practical setup of noninvasive reaction conditions, we used the liberation of CO as an indicator of irradiation intensities that could photochemically disrupt the oxidase.
Nature of the reduced state
The photoreductive irradiation was usually stopped at
90100% of heme reduction, as it was obtained in parallel samples and quantified by FMN/EDTA as an electron donor. Three (ubiquinol oxidase) or four (cytochrome c oxidase) electrons should fill up the redox sites in their thermodynamically defined order, i.e., the centers CuB, high-spin heme, low-spin heme, and CuA. The degree of reduction was measured by the absorbance of the heme
-band, which is, strictly speaking, indicative of the low-potential redox centers. Thus, at 90% auto-photoreduction, the ubiquinol oxidase (which has no CuA) is three-electron reduced. In cytochrome c oxidase, the photoreduced state of the CuA center cannot be proven by our experiments (the reaction was not monitored at 830 nm), but due to electron equilibration the enzyme should be converted to the four-electron-reduced form. By assuming values of the midpoint potentials for the CuA and heme
centers of +240 mV and +230 mV (Wikström et al., 1981
), 93% of the CuA sites are reduced at a heme reduction level of 90%. Einarsdottir and co-workers have created the oxoferryl state of cytochrome c oxidase by auto-photoreduction in the presence of oxygen (Brooks et al., 1997
). In contrast, our experiments are carried out anaerobically with the enzyme ending up in the fully reduced state.
Which chemical groups could be involved in the photoreaction?
The elucidation of the mechanism of photoinduced electron transfer in cytochrome oxidases far exceeds the scope of this report. A number of different effects may interact mutually.
Isolated porphyrins can act as photosensitizers in various reactions (Reddi et al., 1987
); if bound to heme apoproteins the cofactors have been shown to be involved in auto-photoreduction (Gu et al., 1993
; Sakai et al., 2000
). Photochemical action spectra show a single maximum of 290 nm, which clearly differs from the absorbance at 280 nm of aromatic amino acid side chains. However, this peak maximum of 290 nm cannot unequivocally be assigned to heme absorbance. The light-induced electron transfer may be explained by a complex mechanism, which could be composed of different (cooperating) photochemical events.
We conclude that at least the primary activation process in photo-induced electron transfer is due to the action of heme groups, which leads to a Fe2+/porphyryl radical intermediate state (Sakai et al., 2000
). Due to the high oxidation power of the porphyryl radical generated upon photon absorption, estimated to be from +1.2 to +1.4 V (versus normal hydrogen electrode) (Furhop et al., 1973
; Kadish and Morrison, 1976
), it should readily accept electrons from components that have lower redox potential; i.e., the aromatic amino acids tyrosine and tryptophan have to be taken into account, because their midpoint redox potentials are E0 = +0.94 and +1.05 V (measured in free solution) (DeFelippis et al., 1989
). It should be noted that the spectra of tyrosinate (Edelhoch, 1967
) and of transiently photoactivated tyrosine (Bent and Hayon, 1975
) (triplet state 3Tyr) exhibit absorbance maxima at
290 nm, which corresponds to the peak in our observed photochemical action spectra of cytochrome bo3 oxidase.
The external additives, tris and the detergent decylmaltoside, are excluded from the oxidase reaction center, because the heme groups of the protein are deeply embedded in the membrane and are thus nonaccessible to these small molecules, which are freely dissolved in the aqueous phase. A similar explanation holds for the ineffectiveness of externally added tryptophan to stimulate photoreduction of the cytochrome oxidase. In contrast, addition of this amino acid facilitates reduction of certain heme proteins that have their cofactors more strongly exposed to the solvent (Pierre et al., 1982
; Sakai et al., 2000
). It is deduced that the final electron donor for heme groups arises from the protein interior.
Alternatively, hydroxy or water ligands to the high-spin heme and CuB (Wikström et al., 2000
) may be considered to act as reductants due to their proximity to the internal photoactivated radical groups. It is also probable that the electrons are abstracted from water molecules located in the aqueous internal spaces of the protein. Both the D- and K-proton channels contain bound water (Ostermeier et al., 1997
), which could involve different protein groups/contact sites.
Redox investigation by FTIR spectroscopy
The primary purpose of this study was to probe auto-photoreduction and to record infrared spectra of the fingerprint region. This is a prerequisite for detailed band assignment in the difference spectra and for identification of molecular groups involved in the intramolecular electron transfer, and thus important for understanding the reaction mechanism of the protein. The auto-photoreduction reaction works equally with different heme-copper oxidases of the ubiquinol and cytochrome c subclasses. The MIR spectra have superior quality, because no disruptive spectral contributions from the caged reaction with FMN/EDTA were present after auto-photoreduction. The photolytic conditions can be controlled closely by the FTIR method, because the CO binding to the high-spin heme can be easily monitored. It is possible to identify extremely weak bands in the fingerprint region with this technique, e.g., the absorbance band at 1198 cm1 in cytochrome bo3. An even higher signal/noise ratio may be achieved by further increase of the sample concentration, as long as no quantitative comparisons of the strongly absorbing amide I band are required (see below).
General usability of this novel redox FTIR spectroscopic technique
Anaerobic auto-photoreduction is a phenomenon observed with heme-copper oxidases, which most probably represents a composite of different potential light-driven reactions. At present, these are difficult to explain in detail. Whatever the exact photochemical mechanisms are, it is important to note that the photochemical reaction conditions can be carefully adjusted to avoid disruptive effects on the protein and preserve its structural and functional integrity. Auto-photoreduction is a valuable tool for studying various different heme-copper cytochrome oxidases at the molecular level with FTIR. It allows the observation of absorbance changes of functional protein groups in different spectral ranges. For the purpose of FTIR spectroscopy, band assignments are carried out by comparison of difference spectra generated from wild-type oxidase with those of site-directed mutants or isotopically labeled variants. In any case, molecular events contributing to the photoreaction, which are not observed on the aforementioned structural/functional level, may not leave their imprints in the measured spectra, simply because those would be canceled out by calculation of the double difference spectra.
The described technique allows the light-induced redox spectra to be recorded without the undesirable absorbance contributions from externally added caged compounds, thus facilitating the analysis of absorbance peaks in a wider spectral region. It should be emphasized that this method is very reliable; it can be operated at much lower experimental and financial expenses than the rather intricate electrochemical equilibration techniques. If the sample concentrations were adjusted to result in at least 4% transmission in the observed spectral range, the auto-photoreduction FTIR spectra would be very reproducible and exhibit a high signal/noise ratio, especially in the infrared fingerprint region. This will also help us to resolve in future bands that had low intensity or which were invisible in previous experiments.
In addition to heme-copper oxidases, we have used this method to observe FTIR spectra with the respiratory complex III (the so-called bc1 complex) of bacteria, cytochrome c, met-myoglobin, and met-hemoglobin (to be published elsewhere). Auto-photoreduction therefore seems to be a tool that can be universally applied to study reaction mechanisms of heme proteins at atomic level.
| ACKNOWLEDGEMENTS |
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This work was supported by the Volkswagen-Stiftung and the Fonds der Chemischen Industrie.
| FOOTNOTES |
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Abbreviations used: FTIR, Fourier transform infrared; EDTA, ethylendiamine tetra-acetate; FMN, flavine mononucleotide; HPLC, high-performance liquid chromatography; IR, infrared; MIR, mean infrared (10002000 cm1); Ni-NTA, nickel nitrilo-triacetic acid; UV, ultraviolet.
Submitted on March 8, 2003; accepted for publication December 15, 2003.
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