Magnetic field effects on radical pair intermediates in bacterial photosynthesis.

We have investigated the effects of magnetic fields on the formation and decay of excited states in the photochemical reaction centers of Rhodopseudomonae sphaeroides. In chemically reduced reaction centers, a magnetic field decreases the fraction of the transient state PF that decays by way of the bacteriochlorophyll triplet state PR. At room temperature, a 2-kG field decreases the quantum yield of Pr by about 40%. In carotenoid-containing reaction centers, the yield of the carotenoid triplet state which forms via PR is reduced similarly. The effect of the field depends monotonically on field-strength, saturating at about 1 kG. The effect decreases at lower temperatures, when the yield of PR is higher. Magnetic fields do not significantly affect the formation of the triplet state of bacteriochlorophyll in vitro, the photooxidation of P870 in reaction centers at moderate redox potential, or the decay kinetics of states PF and PR. The effect of magnetic fields support in view that state PF is a radical pair which is born in a singlet state but undergoes a rapid transformation into a mixture of singlet and triplet states. A simple kinetic model can account for the effects of the field and relate them to the temperature dependence of the yield of PR.     

Excited states of photosynthetic reaction centers at low redox potentials

In preparations of photochemical reaction centers from Rhodopseudomonas spheroides R-26, lowering the redox potential so as to reduce the primary electron acceptor prevents the photochemical transfer of an electron from bacteriochlorophyll to the acceptor. Measuring absorbance changes under these conditions, we found that a 20-ns actinic flash converts the reaction center to a new state, P^F, which then decays with a half-time that is between 1 and 10 ns at 295 °K. At 25 °K, the decay half-time is approx. 20 ns. The quantum yield of state P^F appears to be near 1.0, both at 295 and at 15 °K. State P^F could be an intermediate in the photochemical electron-transfer reaction which occurs when the acceptor is in the oxidized form.Following the decay of state P^F, we detected another state, P^R, with a decay half-time of 6 μs at 295 °K and 120 μs at 15 °K. The quantum yield of state P^R is approx. 0.1 at 295 °K, but rises to a value nearer 1.0 at 15 °K. The kinetics and quantum yields are consistent with the view that state P^R forms from P^F. State P^R seems likely to be a side-product, rather than an intermediate in the electron-transfer process.The decay kinetics indicate that state P^F cannot be identical with the lowest excited singlet state of the reaction center. One of the two states, P^F or P^R, probably is the lowest excited triplet state of the reaction center, but it remains unclear which one.     

Triplet states of bacteriochlorophyll and carotenoids in chromatophores of photosynthetic bacteria

Chromatophores from photosynthetic bacteria were excited with flashes lasting approx. 15 ns. Transient optical absorbance changes not associated with the photochemical electron-transfer reactions were interpreted as reflecting the conversion of bacteriochlorophyll or carotenoids into triplet states. Triplet states of various carotenoids were detected in five strains of bacteria; triplet states of bacteriochlorophyll, in two strains that lack carotenoids. Triplet states of antenna pigments could be distinguished from those of pigments specifically associated with the photochemical reaction centers. Antenna pigments were converted into their triplet states if the photochemical apparatus was oversaturated with light, if the primary photochemical reaction was blocked by prior chemical oxidation of P-870 or reduction of the primary electron acceptor, or if the bacteria were genetically devoid of reaction centers. Only the reduction of the electron acceptor appeared to lead to the formation of triplet states in the reaction centers.In the antenna bacteriochlorophyll, triplet states probably arise from excited singlet states by intersystem crossing. The antenna carotenoid triplets probably are formed by energy transfer from triplet antenna bacteriochlorophyll. The energy transfer process has a half time of approx. 20 ns, and is about 1 × 10³ times more rapid than the reaction of the bacteriochlorophyll triplet states with O₂. This is consistent with a role of carotenoids in preventing the formation of singlet O₂ in vivo. In the absence of carotenoids and O₂, the decay half times of the triplet states are 70 μs for the antenna bacteriochlorophyll and 6–10 μs for the reaction center bacteriochlorophyll. The carotenoid triplets decay with half times of 2–8 μs.With weak flashes, the quantum yields of the antenna triplet states are in the order of 0.02. The quantum yields decline severely after approximately one triplet state is formed per photosynthetic unit, so that even extremely strong flashes convert only a very small fraction of the antenna pigments into triplet states. The yield of fluorescence from the antenna bacteriochlorophyll declines similarly. These observations can be explained by the proposal that singlet-triplet fusion causes rapid quenching of excited singlet states in the antenna bacteriochlorophyll.     

Magnetic field dependence of radical-pair decay kinetics and molecular triplet quantum yield in quinone-depleted reaction centers

Radical-pair decay kinetics and molecular triplet quantum yields at various magnetic fields are reported for quinone-depleted reaction centers from the photosynthetic bacterium Rhodopseudomonas sphaeroides R26. The radical-pair decay is observed by picosecond absorption spectroscopy to be a single exponential to within the experimental uncertainty at all fields. The decay time increases from 13 ns at zero field to 17 ns at 1 kG, and decreases to 9 ns at 50 kG. The orientation averaged quantum yield of formation of the molecular triplet of the primary electron donor, ³P, drops to 47% of its zero-field value at 1 kG and rises to 126% at 50 kG. Combined analysis of these data gives a singlet radical-pair decay rate constant of 5 · 10⁷s^?1, a lower limit for the triplet radical-pair decay rate constant of 1 · 10⁸s^?1 and a lower limit for the quantum yield of radical-pair decay by the triplet channel of 38% at zero field. The upper limit of the quantum yield of ³P formation at zero field is measured to be 32%. In order to explain this apparent discrepancy, decay of the radical pair by the triplet channel must lead to some rapid ground state formation as well as some ³P formation. It is proposed that the triplet radical pair decays to a triplet charge-transfer state which is strongly coupled to the ground state by spin-orbit interactions. Several possibilities for this charge-transfer state are discussed.     

Kinetic study of PF and CarT states in the LM subunit purified from the wild-type Rhodobacter sphaeroides reaction centers

The kinetics of absorbance changes related to the charge-separated state, P^F, and to the formation and decay of the carotenoid triplet state (Car^T) were studied in the LM reaction center subunit isolated from a wild-type strain of the purple bacterium Rhodobacter sphaeroides (strain Y). The P^F lifetime is lengthened (20±1.5 ns) in the LM complex as compared to the intact reaction centers (11±1 ns). The yield of the carotenoid triplet formation is higher (0.28±0.01) in the LM complex than in native reaction centers. We interpret our results in terms of perturbations of a first-order reaction connecting the singlet and the triplet state of the radical-pair state. Our results, together with those of a recent work (Agalidis, I., Nuijs, A.M. and Reiss-Husson, F. (1987) Biochim. Biophys. Acta (in press)) are consistent with a high I to Q_A electron transfer rate in this LM subunit, which is metal-depleted.The LM complex is considerably more sensitive than the reaction centers to photooxidative damage in the presence of oxygen. This is not readily accounted for simply by the higher carotenoid triplet yield, and may suggest a greater accessibility of the internal structures in the absence of the H-subunit.The lifetime of the carotenoid triplet decay (6.4±0.3 s) in the LM subunit is unchanged compared to the native reaction centers.Abbreviations BChl bacteriochlorophyll - Bph bacteriopheophytin - Car carotenoid - Chl chlorophyll - cyt cytochrome - L, M and H subunits light, medium and heavy subunits of the reaction center complex - P^R triplet electronic state of the primary electron donor - P; Q_A the first stable electron acceptor, a bound quinone - RC reaction center - LDAO lauryldimethylamine N-oxide - SDS sodium dodecyl sulfate - UQ ubiquinone This paper is published in our new format. All future authors are requested to follow our new instructions (see Photosynthesis Research 10:519–526, 1986)—Editor.     

Transient states in reaction centers containing reduced bacteriopheophytin

Photosynthetic reaction centers isolated from Rhodopseudomonas sphaeroides strain R-26 were excited with non-saturating 7-ps, 600-nm flashes under various conditions, and the resulting absorbance changes were measured. If the quinone electron acceptor (Q) is in the oxidized state, flash excitation generates a transient state (P^F), in which an electron has moved from the primary electron donor (P, a dimer of bacteriochlorophylls) to an acceptor complex involving a special bacteriopheophytin (H) and another bacteriochlorophyll (B). P^F decays in 200 ps as an electron moves from H to Q. If Q and the acceptor complex are reduced photochemically before the excitation, the flash generates a different transient state of P with a high quantum yield. This state decays with a lifetime of 340 ps. There is no indication of electron transfer from P to B under these conditions, but this does not rule out the possibility that B is an intermediate electron carrier between P and H. Measurements of the yield of fluorescence from P under various conditions show that the 340 ps state is not the fluorescent excited singlet state of P. The transient state could be a triplet state, a charge-transfer state of P, or another excited singlet state that is not fluorescent.     

Primary photochemical processes in isolated reaction centers of Rhodopseudomonas viridis

Picosecond and nanosecond spectroscopic techniques have been used to study the primary electron transfer processes in reaction centers isolated from the photosynthetic bacterium Rhodopseudomonas viridis. Following flash excitation, the first excited singlet state (P1) of the bacteriochlorophyll complex (P) transfers an electron to an intermediate acceptor (I) in less than 20 ps. The radical pair state (P⁺I^?) subsequently transfers an electron to another acceptor (X) in about 230 ps. There is an additional step of unknown significance exhibiting 35 ps kinetics. P⁺ subsequently extracts an electron from a cytochrome, with a time constant of about 270 ns. At low redox potential (X reduced before the flash), the state P⁺I^? (or P^F) lives approx. 15 ns. It decays, in part, into a longer lived state (P^R), which appears to be a triplet state. State P^R decays with an exponential time of approx. 55 μs. After continuous illumination at low redox potential (I and X both reduced), excitation with an 8-ps flash produces absorption changes reflecting the formation of the first excited singlet state, P1. Most of P1 then decays with a time constant of 20 ps. The spectra of the absorbance changes associated with the conversion of P to P1 or P⁺ support the view that P involves two or more interacting bacteriochlorophylls. The absorbance changes associated with the reduction of I to I^? suggest that I is a bacteriopheophytin interacting strongly with one or more bacteriochlorophylls in the reaction center.     

Influence of magnetic fields on the P-870 triplet state in Rps. sphaeroides reaction centers

Magnetic fields influence two properties of the P-870 triplet state observed in Rps. sphaeroides reaction centers: the yield of formation and the kinetics of decay. These effects have been studied in reaction centers which were prepared in three different states: state Q_A ^–, state Q_A ^2– and state (– Q_A) (Q_A depleted). The triplet yields decrease with increasing magnetic fields, with B1/2's of about 140, 41 and 57 Gauss, respectively. The half-time of ³P-870 decay is not influenced by the field in state Q_A ^–; it increases at increasing fields, in state Q_A ^2– and state (– Q_A), with the same B1/2 as the triplet yield. These results are discussed in the framework of current theories of the radical-pair dynamics and of the mechanism of triplet decay.Abbreviations I primary electron acceptor - LDAO lauryldimethylamine oxide - P-870 primary electron donor - Q_A first quinone acceptor - SDS sodium dodecylsulfate - YAG Yttrium Aluminum Garnet     

Singlet-triplet excitation fission in light-harvesting complexes of photosynthetic bacteria and in isolated carotenoids

Time-resolved electron paramagnetic resonance was used to study the properties of carotenoid triplet states populated in LH2 light-harvesting complexes of phototrophic bacteria Allochromatium minutissimum, Rhodopseudomonas palustris, and in carotenoid films free of bacteriochlorophyll. The study was performed on purified LH2 preparations not contaminated by reaction centers, and under selective pigment excitation. The obtained results enable a conclusion that the carotenoid triplet states, both in LH2 complexes and films, are populated in the process of homofission of singlet excitation into two triplets, which involves only carotenoid molecules. It is observed that the fission process in magnetic field leads to predominant population of the T₀ spin sublevel of the triplet. One molecular spin sublevel of the triplet is demonstrated to possess an increased probability of intersystem crossing to the ground state, independent of the carotenoid configuration. Pigment composition of the LH2 protein heterodimers is discussed, and a conclusion of the possible presence of two interacting carotenoid molecules is made.     

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 emission 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.     

Evidence for a new early acceptor in Photosystem I of plants. An ESR investigation of reaction center triplet yield and of the reduced intermediary acceptors

The yield of the triplet state of the primary electron donor of Photosystem I of photosynthesis (P^T-700) and the characteristic parameters (g value, line shape, saturation behavior) of the ESR signal of the photoaccumulated intermediary acceptor A have been measured for two types of Photosystem I subchloroplast particles: Triton particles (TSF 1, about 100 chlorophyll molecules per P-700) that contain the iron-sulfur acceptors F_X, F_B and F_A, and lithium dodecyl sulfate (LDS) particles (about 40 chlorophyll molecules per P-700) that lack these iron-sulfur acceptors. The results are: (i) In Triton particles the yield of P^T-700 upon illumination is independent of the redox state of A and of F_X,B,A and is maximally about 5% of the active reaction centers at 5 K. The molecular sublevel decay rates are k_x = 1100 s^?1 ± 10%, k_y = 1300 s^?1 ± 10% and k_z = 83 s^?1 ± 20%. In LDS particles the triplet yield decreases linearly with concentration of reduced intermediary acceptors, the maximal yield being about 4% at 5 K assuming full P-700 activity. (ii) In Triton particles the acceptor complex A consists of two acceptors A₀ and A₁, with A₀ preceding A₁. In LDS particles at temperatures below ?30°C only A₀ is photoactive. (iii) The spin-polarized ESR signal found in the time-resolved ESR experiments with Triton particles is attributed to a polarized P-700-A^?₁ spectrum. The decay kinetics are complex and are influenced by transient nutation effects, even at low microwave power. It is concluded that the lifetime at 5 K of P-700A₀A^?₁ must exceed 5 ms. We conclude that P^T-700 originates from charge recombination of P-700A^?₀, and that in Triton particles A₀ and A₁ are both photoaccumulated upon cooling at low redox potential in the light. Since the state P-700AF^?_X does not give rise to triplet formation the 5% triplet yield in Triton particles is probably due to centers with damaged electron transport.     

Nanosecond fluorescence from isolated photosynthetic reaction centers of Rhodopseudomonas sphaeroides

The time-course of fluorescence from reaction centers isolated from Rhodopseudomonas sphaeroides was measured using single-photon counting techniques. When electron transfer is blocked by the reduction of the electron-accepting quinones, reaction centers exhibit a relatively long-lived (delayed) fluorescence due to back reactions that regenerate the excited state (P*) from the transient radical-pair state, P^F. The delayed fluorescence can be resolved into three components, with lifetimes of 0.7, 3.2 and 11 ns at 295 K. The slowest component decays with the same time-constant as the absorbance changes due to P^F, and it depends on both temperature and magnetic fields in the same way that the absorbance changes do. The time-constants for the two faster components of delayed fluorescence are essentially independent of temperature and magnetic fields. The fluorescence also includes a very fast (prompt) component that is similar in amplitude to that obtained from unreduced reaction centers. The prompt fluorescence presumably is emitted mainly during the period before the initial charge-transfer reaction creates P^F from P*. From the amplitudes of the prompt and delayed fluorescence, we calculate an initial standard free-energy difference between P* and P^F of about 0.16 eV at 295 K, and 0.05 eV at 80 K, depending somewhat on the properties of the solvent. The multiphasic decay of the delayed fluorescence is interpreted in terms of relaxations in the free energy of P^F with time, totalling about 0.05 eV at 295 K, possibly resulting from nuclear movements in the electron-carriers or the protein.     

Magnetic field effects on the fluorescence of mutant strains of Rhodopseudomonas capsulata

The magnetic field effects on bacteriochlorophyll fluorescence in six strains of Rhodopseudomonas capsulata were investigated. All strains exhibit an increase in fluorescence upon application of a magnetic field. Large magnetic field effects are shown to arise in mutants which contain the B800–850 complex as the only bacteriochlorophyll-containing protein. These fluorescence increases are observed only with carotenoid excitation and are best described by a carotenoid singlet heterofission mechanism. Variations in the magnitudes of the magnetic field effects for the Rps. capsulata strain arise from energy differences in the excited states of the molecules involved in the process. In order to determine the contribution from reaction centers to the magnetic field effects observed in the mutants which contain all three pigment-protein complexes, reaction centers were isolated from these strains. The reaction center contribution to the magnetic field effect on fluorescence in whole cells was determined to be smaller than the antenna contribution when carotenoid excitation was employed.     

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.     

Carotenoid triplet states in reaction centers from Rhodopseudomonas sphaeroides and Rhodospirillum rubrum

Purified photochemical reaction centers from three strains of Rhodopseudomonas sphaeroides and two of Rhodospirillum rubrum were reduced with Na₂S₂O₄ so as to block their photochemical electron transfer reactions. They then were excited with flashes lasting 5–30 ns. In all cases, absorbance measurements showed that the flash caused the immediate formation of a transient state (P^F) which had been detected previously in reaction centers from Rps. sphaeroides strain R26. Previous work has shown that state P^F is an intermediate in the photochemical electron transfer reaction in the reaction centers of that particular strain, and the present work generalizes that conclusion.

In the reaction centers from two strains that lack carotenoids (Rps. sphaeroides R26 and R. rubrum G9), the decay of P^F yields a longer-lived state (P^R) which is probably a triplet state of the bacteriochlorophyll of the reaction center. In the R26 preparation, the decay of P^F was found to have a half-time of 10±2 ns. The decay kinetics rule out the identification of P^F as the fluorescent excited singlet state of the reaction center.

In the reaction centers from three strains that contain carotenoids (Rps sphaeroides 2.4.1 and Ga, and R. rubrum S1), state P^R was not detected, and the decay of P^F generated triplet states of carotenoids. The efficiency of the coupling between the decay of P^F and the formation of the carotenoid triplet appeared to be close to 100% at room temperature, but somewhat lower at 77 °K. Taken with previous results, this suggests that the coupling is direct and does not require the intermediate formation of state P^R. This conclusion would be consistent with the view that P^F is a biradical which can be triplet in character.     

High-resolution optical absorption-difference spectra of the triplet state of the primary donor in isolated reaction centers of the photosynthetic bacteria Rhodopseudomonas sphaeroides R-26 and Rhodopseudomonas viridis measured with optically detected magnetic resonance at 1.2 K

We have recorded triplet optical absorption-difference spectra of the reaction center triplet state of isolated reaction centers from Rhodopseudomonas sphaeroides R-26 and Rps. viridis with optical absorption-detected electron spin resonance in zero magnetic field (ADMR) at 1.2 K. This technique is one to two orders of magnitude more sensitive than conventional flash absorption spectroscopy, and consequently allows a much higher spectral resolution. Besides the relatively broad bleachings and appearances found previously (see, e.g., Shuvalov V.A. and Parson W.W. (1981) Biochim. Biophys. Acta 638, 50–59) we have found strong, sharp oscillations in the wavelength regions 790–830 nm (Rps. sphaeroides) and 810–890 nm (Rps. viridis). For Rps. viridis these features are resolved into two band shifts (a blue shift at about 830 nm and a red shift at about 855 nm) and a strong, narrow absorption band at 838 nm. For Rps. sphaeroides R-26 the features are resolved into a red shift at about 810 nm and a strong absorption band at 807 nm. We conclude that the appearance of the absorption bands at 807 and 838 nm, respectively, is due to monomeric bacteriochlorophyll. Apparently, the exciton interaction between the pigments constituting the primary donor is much weaker in the triplet state than in the singlet state, and at low temperature the triplet is localized on one of the bacteriochlorophylls on an optical time scale. The fact that for Rps. sphaeroides the strong band shift and the monomeric band found at 1.2 K are absent at 293 K and very weak at 77 K indicates that these features are strongly temperature dependent. It seems, therefore, premature to ascribe the temperature dependence between 293 and 77 K of the intensity of the triplet absorption-difference spectrum at 810 nm (solely) to a delocalization of the triplet state on one of the accessory bacteriochlorophyll pigments.     

Measurement of the extent of electron transfer to the bacteriopheophytin in the M-subunit in reaction centers of Rhodopseudomonas viridis

We have measured the extent of flash-induced electron transfer from the bacteriochlorophyll dimer, P, to the bacteriopheophytin in the M-subunit, H_M, in reaction centers of Rhodopseudomonas viridis. This has been done by measuring the transient states produced by excitation of reaction centers trapped in the PH_L ^–H_M state at 90 K. Under these conditions the normal forward electron transfer to the bacteriopheophytin in the L-subunit, H_L, is blocked and the yield of transient P⁺H_M ^– can be estimated with respect to the lifetime of P^*. Under these conditions flash induced absorbance decreases of the bacteriochlorophyll dimer 990 nm band suggest that a transient P⁺ state is formed with a quantum yield of 0.09±0.06 compared to that formed during normal photochemistry. These transient measurements provide an upper limited on the yield of a transient P⁺ H_M ^– state. An estimate of 0.09 as the yield of the P⁺ H_M ^– state is consistent with all current observations. This estimate and the lifetime of P^* suggest that the electron transfer rate from P^* to H_M, k_M, is about 5 × 10⁹ sec^–1 (_M = 200ps). These measurements suggest that the a branching ratio k_L/k_M is on the order of 200. The large value of the branching ratio is remarkable in view of the structural symmetry of the reaction center. This measurement should be useful for electron transfer calculations based upon the reaction center structure.     

Study of the long-wavelength fluorescence band at 920 nm of isolated reaction centers of the photosynthetic bacterium Rhodopseudomonas spaeroides R-26 with fluorescence-detected magnetic resonance in zero field

The triplet state of isolated reaction centers of Rhodopseudomonas sphaeroides R-26 has been studied by fluorescence-detected electron spin resonance in zero magnetic field (FDMR) at 4.2 K. The sign of the FDMR resonance monitored at the long-wavelength fluorescence band is positive (fluorescence increase); this confirms the earlier interpretation (Hoff, A.J. and Gorter de Vries, H. (1978) Biochim. Biophys. Acta 503, 94–106) that the negative sign of the FDMR resonance of the reaction center triplet state in whole bacterial cells is caused by resonant transfer of the singlet excitations from the antenna pigments to the trap. By monitoring the FDMR response as a function of the wavelength of fluorescence, we have recorded microwave-induced fluorescence spectra. In addition to the positive microwave-induced fluorescence band peaking at 935 nm, at 905 nm a negative band was found. The resonant microwave frequencies for these two bands, i.e., the values of the zero-field splitting parameters |D| and |E| of the triplet state being monitored, were different, those of the 905 nm microwave-induced fluorescence band being identical to the resonant microwave frequencies measured with absorption-detected zero-field resonance (Den Blanken, H.J., Van der Zwet, G.P. and Hoff, A.J. (1982) Chem. Phys. Lett. 85, 335–338), a technique that monitors the bulk properties of the sample. From this result and its negative sign, we tentatively attribute the 905 nm microwave-induced fluorescence band to a small (possibly less than 1%) fraction of antenna bacteriochlorophylls that are in close contact with the trap. The positive 935 nm microwave-induced fluorescence band with resonant microwave frequencies deviating from the bulk material is ascribed to a minority of primary donor bacteriochlorophyll dimers, which have a higher than normal fluorescence yield because of a somewhat slower charge-separation reaction. Is it likely that practically all long-wavelength fluorescence of isolated reaction centers stems from such impaired reaction centers.