Arrhythmogenesis in heart failure.

In a rabbit model of heart failure produced by combined pressure and volume overload, nonsustained ventricular tachycardias developed in 15 of 23 failing rabbits. Sinus rate was increased in rabbits dying suddenly, but was decreased in survivors. This also was true in isolated preparations. Microelectrode recordings from ventricular trabeculae both from patients with end-stage failure and from failing rabbits showed that in half of the preparations, delayed afterdepolarizations and triggered activity occurred, but only in the presence of norepinephrine and a lowered extracellular K+ concentration of 3 mM. This was due to spontaneous release of Ca2+ from the sarcoplasmic reticulum.

Towards integrating vectors for gene therapy: expression of functional bacteriophage MuA and MuB proteins in mammalian cells.

Bacteriophage Mu has one of the best studied, most efficient and largest transposition machineries of the prokaryotic world. To harness this attractive integration machinery for use in mammalian cells, we cloned the coding sequences of the phage factors MuA and MuB in a eukaryotic expression cassette and fused them to a FLAG epitope and a SV40-derived nuclear localization signal. We demonstrate that these N-terminal extensions were sufficient to target the Mu proteins to the nucleus, while their function in Escherichia coli was not impeded. In vivo transposition in mammalian cells was analysed by co-transfection of the MuA and MuB expression vectors with a donor construct, which contained a miniMu transposon carrying a Hygromycin-resistance marker (Hyg(R)). In all co-transfections, a significant but moderate (up to 2.7-fold) increase in Hyg(R) colonies was obtained if compared with control experiments in which the MuA vector was omitted. To study whether the increased efficiency was the result of bona fide Mu transposition, integrated vector copies were cloned from 43 monoclonal and one polyclonal cell lines. However, in none of these clones, the junction between the vector and the chromosomal DNA was localized precisely at the border of the Att sites. From our data we conclude that expression of MuA and MuB increases the integration of miniMu vectors in mammalian cells, but that this increase is not the result of bona fide Mu-induced transposition.

Ammonium sulphate precipitation of recombinant adenovirus from culture medium: an easy method to increase the total virus yield.

In the majority of the methods for purifying and concentrating recombinant adenoviruses (rAds) the virus that is associated with the helper cells is harvested, while the virus that is present in the cell-culture medium is discarded. During routine propagation of adenovirus type-5 vectors at optimised conditions we noted that, on average, 47% of the total amount of virus is present in the culture medium. To recover and concentrate these rAds from the medium, we devised a method, which is based on ammonium sulphate ((NH4)2SO4) precipitation. At 40% (NH4)2SO4 saturation, 95 +/- 6% of the available virus precipitates from the medium, while the majority of the protein (85%) remains in solution. In contrast to adenovirus precipitation with polyethylene glycol, the (NH4)2SO4 precipitation technique allows collection of precipitated rAds by filtration. We demonstrate here that (NH4)2SO4 precipitation of rAds from cell-culture medium is a simple and fast technique that can be used in combination with standard virus isolation methods to increase the yields of rAds.

Changes in sinus node function in a rabbit model of heart failure with ventricular arrhythmias and sudden death.

BACKGROUND: Heart failure is associated with profound changes in the balance of the autonomic nervous system, such as vagal withdrawal and increased catecholamine levels. It is not known whether the intrinsic sinus node function changes during the progression of heart failure. METHODS AND RESULTS: We implanted transmitters for Holter recording in an established rabbit model of heart failure (n=9) and observed changes in sinus cycle length and the occurrence of arrhythmias during the progression of heart failure. The in vitro sinus cycle length and the responses to acetylcholine and norepinephrine in the isolated right atria were analyzed in 12 rabbits with heart failure and in 6 control rabbits. In vivo cycle length increased in some animals and decreased in others. Sudden death occurred in 3 of 9 rabbits. These rabbits had developed a shorter cycle length than the surviving rabbits. Ventricular tachycardias developed in all but 1 rabbit. The in vitro sinus cycle length increased in heart failure. The response to acetylcholine also increased in heart failure, whereas the response to norepinephrine was unchanged. CONCLUSIONS: Changes in intrinsic sinus node function during the progression of heart failure cannot explain the observed decreases in heart rate variability and/or baroreflex sensitivity in this disease, because increased responsiveness to acetylcholine would be expected to cause the opposite.

Specific tumor-cell killing with adenovirus vectors containing the apoptin gene.

Specificity is an essential prerequisite for cancer gene therapy. Recently we described that apoptin, a protein of 121 amino acids which is derived from the chicken anemia virus, induces programmed cell death or apoptosis in transformed and malignant cells, but not in normal, diploid cells (Danen-van Oorschot AAAM et al, Proc Natl Acad Sci USA 1997; 94: 5843-5847). This protein has an intrinsic specificity that allows it to selectively kill tumor cells, irrespective of the p53 or Bcl-2 status of these cells. Hence, it is attractive to explore the use of the apoptin gene for therapeutic applications, viz cancer gene therapy. In this paper, we describe the generation and characterization of an adenovirus vector, AdMLPvp3, for the expression of apoptin. Despite the fact that apoptin ultimately induces apoptosis in the helper cells, which are transformed by the adenovirus type 5 early region 1 (E1), the propagation kinetics and yields of AdMLPvp3 are similar to those of control vectors. Infection with AdMLPvp3 of normal rat hepatocytes in cell culture did not increase the frequency of apoptosis. In contrast, in the hepatoma cell lines HepG2 and Hep3b, infection with AdMLPvp3, but not with control vectors, led to a rapid induction of programmed cell death. Experiments in rats demonstrated that AdMLPvp3 could be safely administered by intraperitoneal, subcutaneous or intravenous injection. Repeated intravenous doses of AdMLPvp3 were also well tolerated, indicating that the apoptin-expressing virus can be administered without severe adverse effects. In a preliminary experiment, a single intratumoral injection of AdMLPvp3 into a xenogeneic tumor (HepG2 cells in Balb/Cnu/nu mice) resulted in a significant reduction of tumor growth. Taken together, our data demonstrate that adenovirus vectors for the expression of the apoptin gene may constitute a powerful tool for the treatment of solid tumors.

Cellular uncoupling during ischemia in hypertrophied and failing rabbit ventricular myocardium: effects of preconditioning.

BACKGROUND: Patients with heart failure show a very high incidence of arrhythmias and sudden death that is often preceded by ischemia; however, data on electrophysiological changes during ischemia in failing myocardium are sparse. We studied electrical uncoupling during ischemia in normal and failing myocardium. METHODS AND RESULTS: Tissue resistance, intracellular Ca2+ concentration (Indo-1 fluorescence ratio), and mechanical activity were simultaneously determined in arterially perfused right ventricular papillary muscles from 11 normal and 15 failing rabbits. Heart failure was induced by combined volume and pressure overload. Before sustained ischemia, muscles were subjected to control perfusion (non-PC) or ischemic preconditioning (PC). The onset of uncoupling during ischemia was equal in non-PC normal (13.6+/-0.9 minutes of ischemia) and non-PC failing hearts (13.3+/-0.7 minutes of ischemia). PC postponed uncoupling in normal hearts by 10 minutes. In failing hearts, however, PC caused a large variability in the onset of uncoupling during ischemia (mean, 12.2+/-2.1; range, 5 to 22 minutes of ischemia). The duration of uncoupling process was prolonged in failing hearts (12.9+/-0.9 minutes) compared with normal hearts (7.8+/-0.4 minutes). The degree of heart failure and relative heart weight of the failing hearts significantly correlated with the earlier uncoupling after PC and the duration of uncoupling. In every experiment, the start of Ca2+ rise and contracture preceded uncoupling during ischemia. CONCLUSIONS: The duration of the process of ischemia-induced electrical uncoupling in failing hearts is prolonged compared with that in normal hearts. Ischemic PC has detrimental effects in severely failing papillary muscles because it advances the moment of irreversible ischemic damage.

Electrophysiologic and extracellular ionic changes during acute ischemia in failing and normal rabbit myocardium.

The incidence of ventricular arrhythmias is higher in failing hearts than in control hearts, especially during acute ischemia. Electrophysiological and extracellular ionic changes during acute ischemia in normal and failing rabbit myocardium were assessed. Heart failure was induced in rabbits by combined volume and pressure overload. In perfused papillary muscles, the onset of electrical uncoupling and changes in action potential duration and conduction velocity during acute ischemia were determined. In Langendorff-perfused rabbit hearts the changes in extracellular potassium concentration ([K+]o) and pH during acute global ischemia were studied. In perfused papillary muscles, during the first 10 min of ischemia, action potential duration at 80% of repolarization decreased more in preparations from failing than from control hearts (from 174 to 104 ms and from 156 to 119 ms respectively (P < 0.001)). Conduction velocity was significantly lower in failing hearts during ischemia (P < 0.005). The onset of electrical uncoupling was similar in failing and control hearts (mean +/- S.E.M., 17 +/- 1 and 15 +/- 1 min respectively, n.s.). Langendorff-perfused hearts [K+]o, after 10 min of ischemia, was 11.0 +/- 0.4 mM in failing and 9.5 +/- 0.3 mM in control hearts (P < 0.01), while the change in pH was the same. After pretreatment with glibenclamide, an ATP sensitive K+ channel blocker, [K+]o reached lower values after 10 min of ischemia in both failing (8.8 +/- 0.5 mM) and control hearts (7.2 +/- 0.4 mM). During ischemia, action potential duration shortening is more pronounced and conduction velocity is lower in failing myocardium than in control myocardium. [K+]o reaches higher values during acute ischemia in failing compared with normal myocardium. These changes are not caused by an earlier activation of IK.ATP. Increased spatial dispersion in electrophysiological parameters and [K+]o over the ischemic border in failing hearts may explain the higher propensity for reentrant arrhythmias during acute regional ischemia in failing hearts.

The photoreactivity of the copper-NO complexes in cytochrome c oxidase and in other copper-containing proteins.

The complexes of NO with CuB of cytochrome c oxidase in which cytochrome a3 may or may not be ligated to cyanide or fluoride are photodissociable. NO does not appear to react with CuB in complexes of cytochrome c oxidase in which sulphide or mercaptans are ligated to the haem iron of cytochrome a3. A comparison is made between the photoreactivity of the complexes of NO with cytochrome c oxidase and those with ceruloplasmin, ascorbate oxidase, and haemocyanin. It is shown that the photoreactivity of CuB 2+.NO in cytochrome c oxidase is not unique for this enzyme, but may also be observed in the complexes of NO with type-1 copper-containing enzymes. This would suggest that the ligation of CuB in cytochrome c oxidase shows some similarity to type-1 copper in blue oxidases.

The cytochrome c oxidase-azide-nitric oxide complex as a model for the oxygen-binding site.

The complex of cytochrome c oxidase with NO and azide has been studied by EPR at 9.2 and 35 GHz. This complex which shows delta ms = 2 EPR triplet and strong anisotropic signals, due to the interaction of cytochrome a2+3 X NO (S = 1/2) and Cu2+B (S = 1/2), is photodissociable . Its action spectrum is similar to that of cytochrome a2+3 X NO with bands at 430, 560 and 595 nm, but shows an additional band in the near ultraviolet region. The quantum yield of the photodissociation process of cytochrome a2+3 X NO in the metal pair appears to depend on the redox state of CuB. When the photolysed sample was warmed to 77 K, a complex was observed with the EPR parameters of cytochrome a3+3 - N-3 - Cu1 +B (S = 1/2). This process of electron and ligand transfer can be reversed by heating the sample to 220 K. It is suggested that in the triplet species azide is bound to Cu2+B whereas NO is bridged between Cu2+B and the haem iron of the cytochrome a2+3. The complex has a triplet ground state and a singlet excited state with an exchange interaction J = -7.1 cm-1 between both spins. The anisotropy in the EPR spectra is mainly due to a magnetic dipole-dipole interaction between cytochrome a2+3 X NO and Cu2+B. From simulations of the triplet EPR spectra obtained at 9 and 35 GHz, a value for the distance between the nitroxide radical and Cu2+B of 0.33 nm was found. A model of the NO binding in the cytochrome a3-Cu pair shows a distance between the haem iron of cytochrome a3 and CuB of 0.45 nm. It is concluded that the cytochrome a3-CuB pair forms a cage in which the dioxygen molecule is bidentate coordinated to the two metals during the catalytic reaction.

An EPR study of the photodissociation reactions of oxidised cytochrome c oxidase-nitric oxide complexes.

Complexes of oxidised cytochrome c oxidase with NO in the absence and presence of ligands such as formate, fluoride and cyanide are photodissociable. After photodissociation at 10 K the EPR spectrum of the high-spin cytochrome a3+3 in the absence of ligands or in the presence of fluoride or formate disappears - as does the EPR spectrum of the low-spin cytochrome a3+3 in the presence of cyanide. The action spectra of the photodissociation reaction of these complexes show slight differences but all have maxima at 640-660 nm and below 400 nm, and are assigned to a diamagnetic Cu+B-NO+ complex. The differences in the action spectra in the presence of various ligands are due to binding of these anions to the cytochrome (a3-CuB) couple. The disappearance of the cytochrome a3 signal upon photodissociation of the Cu+B-NO+ complex is explained by a magnetic interaction between cytochrome a3+3 and Cu2+B in the photodissociated complex. The temperature at which NO recombines with Cu2+B is about 30 K and slightly affected by the presence of added ligands. It is suggested that in the oxidised ligand-cytochrome c oxidase complexes the coupling ligand between cytochrome a3+3 and Cu2+B is cyanide, fluoride and formate. The observation that two ligands may bind simultaneously to the cytochrome a3-CuB couple leads to further support for the notion that during turnover of cytochrome c oxidase both metal ions are involved in binding and reduction of oxygen.

EPR studies of the photodissociation reactions of cytochrome c oxidase-nitric oxide complexes.

Three complexes of NO with cytochrome c oxidase are described which are all photodissociable at low temperatures as measured by EPR. The EPR parameters of the cytochrome a2+(3)-NO complex are the same both in the fully reduced enzyme and in the mixed-valence enzyme. The kinetics of photodissociation of cytochrome a2+(3)-NO and recombination of NO with cytochrome a2+(3) (in the 30-70 K region) revealed no differences in structure between cytochrome a2+(3) in the fully reduced and the mixed-valence states. The action spectrum of the photodissociation of cytochrome a2+(3)-NO as measured by EPR has maxima at 595, 560 and 430 nm, and corresponds to the absorbance spectrum of cytochrome a2+(3)-NO. Photodissociation of cytochrome a2+(3)-NO in the mixed-valence enzyme changes the EPR intensity at g 3.03, due to electron transfer from cytochrome a2+(3) to cytochrome a3+. The extent of electron transfer was found to be temperature dependent. This suggests that a conformational change is coupled to this electron transfer. The complex of NO with oxidized cytochrome c oxidase shows a photodissociation reaction and recombination of NO (in the 20-40 K region) which differ completely from those observed in cytochrome a2+(3)-NO. The observed recombination occurs at a temperature 15 K lower than that found for the cytochrome a2+(3)-NO complex. The action spectrum of the oxidized complex shows a novel spectrum with maxima at 640 and below 400 nm; it is assigned to a Cu2+B-NO compound. The triplet species with delta ms = 2 EPR signals at g 4 and delta ms = 1 signals at g 2.69 and 1.67, that is observed in partially reduced cytochrome c oxidase treated with azide and NO, can also be photodissociated.

The balance between primary forward and back reactions in bacterial photosynthesis.

The temperature dependence of the bacteriochlorophyll fluorescence and reaction center triplet yield in while cells of Rhodopseudomonas sphaeroides strain 2.4.1 and of the magnetic field-induced fluorescence increase are calculated, taking into account rate constants of losses in the antenna system and of charge separation and recombination in the reaction center. Triplet and singlet yield after recombination in the reaction center are described by the radical pair mechanism. Good fits of the theoretically calculated temperature dependence with published experimental results could be obtained, assuming that ks, the rate constant for recombination of the charges on the primary donor P+ and the reduced intermediate acceptor I- to the lowest excited singlet state P*I of the reaction center bacteriochlorophyll, is temperature-dependent via the Boltzmann factor Kso exp(-delta E/kT), where delta E is the energy difference between P*I and P+I- and kso is the frequency factor. kg and/or kt, the rate constants for recombination to the singlet ground and triplet states, respectively, were assumed to be temperature-independent, or temperature-dependent via their exothermicity factors ki = CiT-1/2 exp(-Ei/kT) with i = g, t. Depending on the particular choice for the temperature dependence of kg and kt, best fits were obtained for delta E = 45-75 meV and recombination rate constants at 300 K of ks = 0.4-0.8 ns-1, kg = 0.08-0.12 ns-1, and kt = 0.3-0.5 ns-1. The model predicts a lifetime of the radical pair P+I- that is somewhat larger than that of delayed fluorescence; a magnetic field increases both.

Transfer and trapping of excitation energy in photosystem II as studied by chlorophyll alpha 2 fluorescence quenching by dinitrobenzene and carotenoid triplet. The matrix model.

1. The curves representing the reciprocal fluorescence yield of chlorophyll alpha of Photosystem II (PS II) in Chlorella vulgaris as a function of the concentration of m-dinitrobenzene in the states P Q and P Q-, are found to be straight parallel lines; P is the primary donor and Q the primary acceptor of PS II. In the weakly trapping state P Q- the half-quenching of dinitrobenzene is about 0.2 mM, in vitro it is of the order of 10 mM. The fluorescence yield as a function of the concentration of a quencher is described for three models for the energy transfer between the units, and the matrix model. If it is assumed that the rate constant of quenching by dinitrobenzene is high and thus the number of dinitrobenzene molecules per reaction center low, it can be concluded that the pigment system of PS II in C. vulgaris is a matrix of chlorophyll molecules in which the reaction centers are embedded. Theoretical and experimental evidence is consistent with such an assumption. For Cyanidium caldarium the zero fluorescence yield phi 0 and its quenching by dinitrobenzene were found to be much smaller than the corresponding quantities for C. vulgaris. Nevertheless, our measurements on C. caldarium could be interpreted by the assumption that the essential properties (rate constants, dinitrobenzene quenching) of PS II are the same for these two species belonging to such widely different groups. 2. The measured dinitrobenzene concentrations required for half-quenching in vivo and other observations are explained by (non-rate-limiting) energy transfer between the chlorophyll alpha molecules of PS II and by the assumptions that dinitrobenzene is approximately distributed at random in the membrane and does not diffuse during excitation. 3. The fluorescence kinetics of C. vulgaris during a 350 ns laser flash of variable intensity could be simulated on a computer using the matrix model. From the observed fluorescence quenching by the carotenoid triplet (CT) and the measurement of the the number of CT per reaction center via difference absorption spectroscopy, the rate constant for quenching of CT is calculated to be kT = 3.3 . 10(11)s-1 which is almost equal to the rate constant of trapping by an open reaction center (Duysens, L.N.M. (1979) CIBA Foundation Symposium 61 (New Series), pp. 323--340). 4. The fluorescence quenching by CT in non-treated spinach chloroplasts after a 500 ns laser flash (Breton, J., Geacintov, N.E. and Swenberg, C.E. (1979) Biochim, Biophys. Acta 548, 616--635) could be explained within the framework of the matrix model when the value for kT is used as given in point 3. 5. The observations mentioned under point 1 indicate that the fluorescence yield phi 0 for centers in trapping state P Q is probably for a fraction exceeding 0.8 emitted by PS II.

Carotenoid triplet yields in normal and deuterated Rhodospirillum rubrum.

Quantum yields of carotenoid triplet formation in Rhodospirillum rubrum wild type and fully deuterated cells and chromatophores were determined in weak laser flashes for excitation wavelength lambda i = 530 nm (mainly absorbed by the carotenoid spirilloxanthin) and for lambda i = 608 nm (mainly absorbed by bacteriochlorophyll) in the presence and absence of magnetic fields. All experiments were performed at room temperature and in the absence of oxygen. The quantum yield of reaction center bacteriochlorophyll oxidation in wild type preparations, in which all reaction centers are in state PIX, at lambda i = 608 nm is close to unity, whereas the quantum yield of antenna carotenoid triplet formation is low (about 5%); P is the primary electron donor, a bacteriochlorophyll dimer, I the primary acceptor, a bacteriopheophytin, and X the secondary acceptor, an iron-ubiquinone complex. In cells in which the reaction centers are in the state P+IX(-), the antenna carotenoid triplet yield is about 0.2. In contrast, at lambda i = 530 nm, the quantum yield of P+ formation is relatively low (0.3) and the yield of the antenna carotenoid triplet state in state PIX unusually high (0.3). At increasing light intensities of 530 nm only about 3 carotenoids per reaction center of the 15 carotenoids present are efficiently photoconverted into the triplet state, which indicates that there are two different pools of carotenoids, one with a low efficiency for transfer of electronic excitation to bacteriochlorophyll and a high yield for triplet formation, the other with a high transfer efficiency and a low triplet yield. The absorption difference spectrum of the antenna carotenoid triplet, excited by 608 or 530 nm light in the state P+IX(-) does not show the peak at 430 nm, that is present in the difference spectrum of the reaction center carotenoid triplet, mainly observed at lambda i = 608 nm with weak flashes. The yield of the reaction center carotenoid triplet, generated in chromatophores in the state PIX(-), is decreased by about 10% by a magnetic field of 0.6 T. In a magnetic field of 0.6 T the yield of the carotenoid triplet, formed by 530 nm excitation in chromatophores at ambient redox potential, is decreased by about 45%. The high quantum yield of formation and the pronounced magnetic field effect for the carotenoid triplet generated by direct excitation at 530 nm can be explained by assuming that this triplet is not formed by intersystem crossing, but by fission of the singlet excitation into two triplet excitations and subsequent annihilation (triplet pair mechanism), or by charge separation and subsequent recombination (radical pair mechanism). Fully deuterated bacteria give essentially the same triplet yields, both in the reaction center and in the antenna carotenoids and show the same magnetic field effects as non-deuterated samples. This indicates that hyperfine interactions do not play a major role in the dephasing of the spins in the radical pair P+I- nor in the formation of the antenna carotenoid triplet.

Chlorophyll a fluorescence as a monitor of nanosecond reduction of the photooxidized primary donor P-680 Of photosystem II.

1. Changes in the fluorescence yield of aerobic Chlorella vulgaris have been measured in laser flashes of 15 ns, 30 ns and 350 ns half time. The kinetics after the first flash given after a 3 min dark period could be simulated on a computer using the hypothesis that the oxidized acceptor Q and primary donor P+ are fluorescence quenchers, and Q- is a weak quencher, and that the reduction time for P+ is 20-35 ns. 2. The P+ reduction time for at least an appreciable part of the reaction centers was found to be longer after the second and subsequent flashes. In the first 5 flashes an oscillation was observed. Under steady state conditions, with a pulse separation of 3 s, a reduction time for P+ of about 400 ns for all reaction centers gave the best correspondence between computed and experimental fluorescence kinetics.

Magnetic field-induced increase of the yield of (bacterio)chlorophyll emission of some photosynthetic bacteria and of Chlorella vulgaris.

In photosynthetic bacteria, in which the iron-ubiquinone complex X is prereduced, a magnetic field induces an increase of the emmission yield, which is correlated with the decrease in reaction center triplet yield reported previously (Hoff, A.J., Rademaker, H., van Grondelle, R. and Duysens, L.N.M. (1977) Biochim. Biophys. Acta 460, 547--554). Our results support the hypothesis that under these conditions charge recombination of the oxidized primary donor and the reduced primary acceptor predominantly generates the excited singlet state of the reaction center bacteriochlorophyll. In Chlorella vulgaris and spinach chloroplasts, at 120 K, the magnetic field has an effect similar to that found in bacteria, which suggests that an intermediary electron acceptor between P-680 and Q is present in Photosystem II also.

Bacteriochlorophyll fluorescence of purple bacteria at low redox potentials. The relationship between reaction center triplet yield and the emission yield.

This work describes fluorescence yield measurements in suspensions of strains of Rhodospirillum rubrum and Rhodopseudomonas sphaeroides in which the iron . quinone complex (X) was chemically reduced (state [PIX-]; P is the reaction center bacteriochlorophyll dimer, I is the long wavelength bacteriopheophytin), and compares these with the fluorescence observed when all the traps are open (state [PIX]) and with the fluorescence observed when all the traps are closed (state [P+IX]). At 77 K the amplitude and the shape of the fluorescence emission spectrum in [PIX-] are identical to those observed in [PIX]. This is a strong indication that all the extra fluorescence observed at room temperature in [PIX-] is, in fact, caused by an efficient back reaction [P+I-X-] leads to [P*IX-]. Using an equation similar to the original Vredenberg-Duysens relationship (Vredenburg, W.J. and Duysens, L.N.M. (1963) Nature 197, 355-357) but now assuming that a single reaction center has a probability pt of trapping an excitation and (1--pt) of re-emitting it to the surroundings, we are able to calculate pt as a function of the temperature by measuring the fluorescence in [PIX], [PIX-] and [P+IX] as a function of the temperature. The calculated pt values agree reasonably well with triplet yields measured in isolated reaction centers. Finally, we have measured the reaction center triplet yield (PTR) in intact systems and we have shown that the sum of the triplet yield and the remaining loss processes (PL) in the antenna bacteriochlorophyll including the bacteriochlorophyll dimer (such as fluorescence, internal conversion or direct triplet formation) is approximately constant; if we assume that at 77 K the only process which occurs in the reaction center is the formation of a reaction center triplet, than PTR + PL=1. The energy barrier between [P*IX-] and [P+I-X-] was estimated to be 0.11--0.15 eV for a set of preparations.

On the magnetic field dependence of the yield of the triplet state in reaction centers of photosynthetic bacteria.

The yield of the triplet state in reaction centers of Rhodopseudomonas sphaeroides is dependent on the strength of an applied magnetic field. Reaction centers of the wild type that lack a functional iron complexed to the primary acceptor ubiquinone show a dependence similar to that of reaction centers of the mutant R-26 in which the iron-ubiquinone complex is intact. Apparently, the iron of the iron-ubiquinone complex is not essential to the effect, but it does exert an influence on its extent. Inchromatophores, the effect is about 2-fold decreased; the value of the magnetic field at which half the effect is found is about 500 G, in contrast to this value for reaction centers, which is 50--100 G. The magnetodependence of the triplet yield is discussed in terms of the Chemically Induced Dynamic Electron Polarization mechanism (CIDEP).