Characterization of the low temperature thermoluminescence band Zv in leaf: an explanation for its variable nature

Out of the six thermoluminescence bands reported for a mature leaf, one band (Zv) appearing at the lowest temperatures is dependent on the temperature of illumination. The characteristics of this band in fresh leaf are compared with those is a leaf heated to 60 degrees C for 5 min. It is concluded here that this band, following illumination at temperatures lower than 173 K, is part of Arnold and Azzi's Z band (Arnold, W. and Azzi, J.R. (1971) Photochem. Photobiol. 14, 233--240). However, it is part of peak I when observed subsequent to illumination beyond 173 K. An explanation for the appearance of this band at different temperatures is proposed.     

Characteristics of thermoluminescence bands of intact leaves and isolated chloroplasts in relation to the watersplitting activity in photosynthesis

Plant materials (intact leaves, chloroplasts or subchloroplast particles) preilluminated at a low temperature (e.g. −60°C) were rapidly cooled to −196°C and then the luminescence emitted from the sample on raising the temperature was measured as a function of temperature, by means of a sensitive photo-electron counting technique. Mature spinach leaves showed five luminescence bands at different temperatures which were denoted as Z_v, A, B₁, B₂ and C bands. The A, B₁, B₂ and C bands appeared at constant temperatures, −10, +25, +40 and +55°C, respectively, being independent of the illumination temperature, but the Z_v band appeared at a variable temperature slightly higher than the illumination temperature. The B₁ and B₂ bands were absent in the thermoluminescence profiles of samples devoid of the oxygenevolving activity, such as heat-treated spinach leaves, wheat leaves greened under intermittent illumination and photosystem-II particles prepared with Triton X-100. It was deduced that these luminescence bands arise from the energy stored by the electron flow in photosystem II to evolve oxygen, and other bands were ascribed to charge-separation in some other sites not related to the oxygen evolving system.     

The effect of temperature on the primary reaction of chloroplast Photosystem II Evidence for a temperature-dependent back reaction

The primary reaction of Photosystem II has been studied over the temperature range from −196 to −20 °C. The photooxidation of the reaction-center chlorophyll (P680) was followed by the free-radical electron paramagnetic resonance signal of P680⁺, and the photoreduction of the Photosystem II primary electron acceptor was monitored by the C-550 absorbance change.

At temperatures below −100 °C, the primary reaction of Photosystem II is irreversible. However, at temperatures between −100 and −20 °C a back reaction that is insensitive to 3-(3′,4′-dichlorophenyl)-1,1′-dimethylurea (DCMU) occurs between P680⁺ and the reduced acceptor.

The amount of reduced acceptor and P680⁺ present under steady-state illumination at temperatures between −100 and −20 °C is small unless high light intensity is used to overcome the competing back reaction. The amount of reduced acceptor present at low light intensity can be increased by adjusting the oxidation-reduction potential so that P680⁺ is reduced by a secondary electron donor (cytochrome b₅₅₉) before P680⁺ can reoxidize the reduced primary acceptor. The photooxidation of cytochrome b₅₅₉ and the accompanying photoreduction of C-550 are inhibited by DCMU. The inhibition of C-550 photoreduction by DCMU, the dependence of P680 photooxidation and C-550 photoreduction on light intensity, and the effect of the availability of reduced cytochrome b₅₅₉ on C-550 photoreduction are unique to the temperature range where the Photosystem II primary reaction is reversible and are not observed at lower temperatures.     

Kinetics of chlorophyll fluorescence at 77 K in Chlorella and chloroplasts. Effects of CCCP,ferricyanide and DCMU

The kinetics of chlorophyll fluorescence at 77 K were studied in Chlorella cells and spinach chloroplasts.During a first illumination, the rise is polyphasic with at least three phases. The slowest one is irreversible and corresponds to the cytochrome oxidation.The dark regeneration of half the variable fluorescence is biphasic, the fast phase being inhibited by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) both in Chlorella and chloroplasts.The fluorescence rise during a second illumination is still biphasic.Carbonyl cyanide m-chlorophenylhydrazone (CCCP) slows down the fluorescence rise in Chlorella but has no effect on the dark regeneration. It does not affect the fluorescence of chloroplasts.Ferricyanide which oxidizes cytochrome b-559 at room temperature produces a quenching of the variable fluorescence and an acceleration of the fluorescence rise during the first illumination.Our results fit the idea of the heterogeneity of the Photosystem II centers at low temperature.     

The effect of temperature on the formation and decay of the multiline EPR signal species associated with photosynthetic oxygen evolution

We have investigated the effects of temperature on the formation and decay of the light-induced multiline EPR signal species associated with photosynthetic oxygen evolution (Dismukes, G.C. and Siderer, Y. (1980) FEBS Lett. 121, 78–80). (1) The decay rate following illumination is temperature dependent: at 295 K the half-time of decay is about 40 s, at 253 K the half-time is approx. 40 min. (2) A single intense flash of light becomes progressively less effective in generating the multiline signal below about 240 K. (3) Continuous illumination is capable of generating the signal down to almost 160 K. (4) Continuous illumination after a preilluminating flash generates less signal above 200 K than at lower temperatures. Our results support the conclusion of Dismukes and Siderer that the S₂ state gives rise to this multiline signal; we find that the S₁ state can be fully advanced to the S₂ state at temperatures as low as 160 K. The S₂ state is capable of further advancement at temperatures above about 210 K, but not below that temperature.     

Factors affecting energy transfer from phycobilisomes to thylakoids in Anacystis nidulans

Short illumination with white light of dark-maintained Anacystis nidulans prior to immersion in liquid nitrogen resulted in a marked change of fluorescence emission characteristics at 77 K. The fluorescence of Photosystem II-associated membrane bound pigments increases, while the emission due to phycobilins decreases. This effect seems to be due to a light-dependent alteration in the extent of contact between phycobilisomes and thylakoids, since the effect is reversible in the dark and is abolished by short glutaraldehyde fixation. The preillumination effect is not inhibited by DCMU. Emission spectra obtained with actively growing and CO₂-starved cells indicate that the light-dependent increase in energy transfer from phycobilins to chlorophyll depends upon the physiological state of the cells.     

Photooxidation pathway of chlorophyll Z in photosystem II as Studied by Fourier transform infrared spectroscopy

The oxidation pathway of chlorophyll Z (ChlZ) in photosystem II (PSII) at cryogenic temperatures was studied by means of light-induced Fourier transform infrared (FTIR) difference spectroscopy. To examine the involvement of redox-active beta-carotene (Car) in the pathway, two Car molecules in Mn-depleted PSII membranes of spinach were selectively bleached by illumination at 250 K in the presence of ferricyanide and silicomolybdate. Successful bleaching of Car was demonstrated by disappearance of the light-induced FTIR signals of Car+ at 1465, 1440, and 1147 cm(-1) at 80 K under an oxidative condition. Even in the Car-bleached PSII, the ChlZ+/ChlZ signal at 1713/1687 cm(-1), which is attributed to the upshift of the 9-keto C=O band of ChlZ upon its oxidation, was induced by illumination at 80 K retaining about 80% of the intensity of the control PSII sample. The concomitant appearance of shoulders at 1727/1699 cm(-1) may indicate that both of the two ChlZ molecules on the D1 and D2 sides are photooxidized. The multiphasic kinetics of formation of the ChlZ+/ChlZ signal by continuous illumination at 80 K were mostly unchanged by Car depletion, while the formation rates at 210 K were appreciably reduced in Car-bleached PSII. These results indicate that there are electron-transfer pathways from ChlZ to P680+ that do not involve Car, and they are indeed dominant at 80 K. Although the pathways via Car are mostly blocked at this temperature, the contribution of such pathways to ChlZ oxidation becomes significant at higher temperatures.     

Mechanism of formation of the C‐terminal β‐hairpin of the B3 domain of the immunoglobulin‐binding protein G from Streptococcus. IV. Implication for the mechanism of folding of the parent protein

A 34‐residue α/β peptide [IG(28–61)], derived from the C‐terminal part of the B3 domain of the immunoglobulin binding protein G from Streptoccocus, was studied using CD and NMR spectroscopy at various temperatures and by differential scanning calorimetry. It was found that the C‐terminal part (a 16‐residue‐long fragment) of this peptide, which corresponds to the sequence of the β‐hairpin in the native structure, forms structure similar to the β‐hairpin only at T = 313 K, and the structure is stabilized by non‐native long‐range hydrophobic interactions (Val47–Val59). On the other hand, the N‐terminal part of IG(28–61), which corresponds to the middle α‐helix in the native structure, is unstructured at low temperature (283 K) and forms an α‐helix‐like structure at 305 K, and only one helical turn is observed at 313 K. At all temperatures at which NMR experiments were performed (283, 305, and 313 K), we do not observe any long‐range connectivities which would have supported packing between the C‐terminal (β‐hairpin) and the N‐terminal (α‐helix) parts of the sequence. Such interactions are absent, in contrast to the folding pathway of the B domain of protein G, proposed recently by Kmiecik and Kolinski (Biophys J 2008, 94, 726–736), based on Monte‐Carlo dynamics studies. Alternative folding mechanisms are proposed and discussed. © 2010 Wiley Periodicals, Inc. Biopolymers 93: 469–480, 2010. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Quality control of Photosystem II under light stress – turnover of aggregates of the D1 protein in vivo

When photodamaged under excessive light, the D1 protein is digested and removed from Photosystem (PS) II to facilitate turnover of the protein. In vitro studies have shown that part of the photodamaged D1 protein forms aggregates with surrounding polypeptides before being digested by a protease(s) in the stroma [Yamamoto Y (2001) Plant Cell Physiol 42: 121–128]. The aim of this study was to examine whether light-induced aggregation of the D1 protein also occurs in vivo. The following results were obtained: (1) PS II activity in spinach leaves was significantly inhibited by weak illumination (light intensity, 20–100 μE m⁻² s⁻¹), as monitored by chlorophyll fluorescence Fv/Fm, when the leaves were kept at higher temperatures (35–40 °C); (2) aggregation of the D1 protein, as well as cleavage of the protein, was detected in thylakoids isolated from spinach leaves that had been subjected to heat/light stress; (3) aggregates of the D1 protein disappeared after incubation of the leaves at 25 °C in the dark or under illumination with weak light. Since it is dependent on the presence of oxygen, aggregation of the D1 protein is probably induced by reactive oxygen species produced in thylakoids upon illumination at elevated temperatures. Consistent with this notion, singlet oxygen production in thylakoid samples under illumination was shown to be stimulated significantly at higher temperatures.     

A slow component of delayed light emission as a function of temperature mimics glow peaks in photosynthetic membranes. Evidence for identity

Evidence for a correlation between a slow component of delayed light emission and thermoluminescence from photosynthetic membranes is presented. It was observed that the intensity of delayed light measured 2.5 s subsequent to illumination at different temperatures when plotted as a function of temperature reproduces the glow curve pattern. The slow component of delayed light emission is also quantitatively related to the yield of thermoluminescence, the sum of the two remaining constant.     

Temperature and preillumination dependence of delayed fluorescence of spinach chloroplasts

Delayed fluorescence (luminescence) from spinach chloroplasts, induced by short saturating flashes, was studied in the temperature region between 0 and ?40 °C. At these temperatures, in contrast to what is observed at room temperature, luminescence at 40 ms after a flash was strongly dependent, with period four, on the number of preilluminating flashes (given at room temperature, before cooling). At ?35 °C luminescence of chloroplasts preilluminated with two flashes (the optimal preillumination) was about 15 times larger than that of dark-adapted chloroplasts. The intensity of luminescence obtained with preilluminated chloroplasts increased steeply below ?10 °C, presumably partly due to accumulation of reduced acceptor (Q^?), and reached a maximum at ?35 °C.In the presence of 50 mM NH₄Cl the temperature optimum was at ?15 °C; at this temperature luminescence was increased by NH₄Cl; at temperatures below ?20 °C luminescence at 40 ms was decreased by NH₄Cl. At room temperature a strongly enhanced 40-ms luminescence was observed after the third and following flashes. The results indicate that both the S₂ to S₃ and the S₃ to S₄ conversion are affected by NlH₄Cl.Inhibitors of Q^? reoxidation, like 3-(3, 4-dichlorophenyl)-1, 1- dimethylurea, did only slightly affect the preillumination dependence of luminescence at sub-zero temperatures if they were added after the preillumination. This indicates that these substances by themselves do not accelerate the deactivation of S₂ and S₃.     

Sub-microsecond chlorophyll A delayed fluorescence from Photosystem I Magnetic field-induced increase of the emission yield

(1) In photosystem I (PS I) particles in the presence of dithionite and intense background illumination at 290 K, an external magnetic field (0–0.22 T) induced an increase, ΔF, of the low chlorophyll a emission yield, F ($\text{ΔF}\text{F}\text{? 1–1.5\%}$). Half the effect was obtained at about 35–60 mT and saturation occurred for magnetic fields higher than about 0.15 T. In the absence of dithionite, no field-induced increase was observed. Cooling to 77 K decreased ΔF at 685 nm, but not at 735 nm, to zero. Measuring the emission spectra of F and ΔF, using continuous excitation light, at 82, 167 and 278 K indicated that the spectra of F and ΔF have about the same maximum at about 730, 725 and 700 nm, respectively. However, the spectra of ΔF show more long-wavelength emission than the corresponding spectra of F. (2) Only in the presence of dithionite and with (or after) background illumination, was a luminescence (delayed fluorescence) component observed at 735 nm, after a 15 ns laser flash (530 nm), that decayed in about 0.1 μs at room temperature and in approx. 0.2 μs at 77 K. A magnetic field of 0.22 T caused an appreciable increase in luminescence intensity after 250 ns, probably mainly caused by an increase in decay time. The emission spectra of the magnetic field-induced increase of luminescence, ΔL, at 82, 167 and 278 K coincided within experimental error with those of ΔF mentioned above. The temperature dependence of ΔF and ΔL was found to be nearly the same, both at 685 and at 735 nm. (3) Analogously to the proposal concerning the 0.15 μs luminescence in photosystem II (Sonneveld, A., Duysens, L.N.M. and Moerdijk, A. (1980) Proc. Natl. Acad. Sci. U.S.A. 77, 5889–5893), we propose that recombination of the oxidized primary donor P-700⁺ and the reduced acceptor A^?, probably A^?₁, of PS I causes the observed fast luminescence. The effect of an external magnetic field on this emission may be explained by the radical pair mechanism. The field-induced increase of the 0.1–0.2 μs luminescence seems to be at least in large part responsible for the observed increase of the total (prompt + delayed) emission measured during continuous illumination in the presence of a magnetic field.     

Triplet state EPR of reaction centers from the HisL173→LeuL173 mutant of Rhodobacter sphaeroides which contains a heterodimer primary donor

Electron paramagnetic resonance (EPR) spectroscopy has been used to examine the triplet states in reaction centers of Rhodobacter sphaeroides which have undergone a genetic modification affecting the primary donor. Reaction centers containing the His^L173Leu^L173 substitution in the amino acid sequence have a primary donor which consists of a BChl-BPh heterodimer. The triplets formed in this heterodimer reaction center were compared with those formed in the wild-type reaction center which contains the BChl-BChl homodimer. Both reaction centers transfer triplet energy to the carotenoid under illumination at liquid nitrogen temperatures (90 K). However, the intensity of the carotenoid triplet signal is significantly decreased in the Leu^L173 mutant compared with the wild-type reaction center. At 12 K, in wild-type reaction centers only the primary donor triplet is observed. The Leu^L173 mutant exhibits a signal similar to that observed by Bylina et al. (1990) in His^M200Leu^M200 mutant reaction centers from Rb. capsulatus. The values of the zero-field splitting parameters of this triplet are discussed within the context of various models for the primary donor triplet state. No alteration in the ability of the carotenoid to quench the primary donor triplet state results from mutations at these sites.Abbreviations BChl bacteriochlorophyll - BPh bacteriopheophytin - EPR electron paramagnetic resonance - LDAO lauryl-dimethylamine N-oxide     

Genetic and physical interaction of Ssp1 CaMKK and Rad24 14-3-3 during low pH and osmotic stress in fission yeast

The Ssp1 calmodulin kinase kinase (CaMKK) is necessary for stress-induced re-organization of the actin cytoskeleton and initiation of growth at the new cell end following division in Schizosaccharomyces pombe. In addition, it regulates AMP-activated kinase and functions in low glucose tolerance. ssp1⁻ cells undergo mitotic delay at elevated temperatures and G₂ arrest in the presence of additional stressors. Following hyperosmotic stress, Ssp1-GFP forms transient foci which accumulate at the cell membrane and form a band around the cell circumference, but not co-localizing with actin patches. Hyperosmolarity-induced localization to the cell membrane occurs concomitantly with a reduction of its interaction with the 14-3-3 protein Rad24, but not Rad25 which remains bound to Ssp1. The loss of rad24 in ssp1⁻ cells reduces the severity of hyperosmotic stress response and relieves mitotic delay. Conversely, overexpression of rad24 exacerbates stress response and concomitant cell elongation. rad24⁻ does not impair stress-induced localization of Ssp1 to the cell membrane, however this response is almost completely absent in cells overexpressing rad24.     

Primary charge separation within P870* in wild type and heterodimer mutants in femtosecond time domain

Primary charge separation dynamics in the reaction center (RC) of purple bacterium Rhodobacter sphaeroides and its P870 heterodimer mutants have been studied using femtosecond time-resolved spectroscopy with 20 and 40fs excitation at 870nm at 293K. Absorbance increase in the 1060-1130nm region that is presumably attributed to P(A)(δ+) cation radical molecule as a part of mixed state with a charge transfer character P*(P(A)(δ+)P(B)(δ-)) was found. This state appears at 120-180fs time delay in the wild type RC and even faster in H(L173)L and H(M202)L heterodimer mutants and precedes electron transfer (ET) to B(A) bacteriochlorophyll with absorption band at 1020nm in WT. The formation of the P(A)(δ+)B(A)(δ-) state is a result of the electron transfer from P*(P(A)(δ+)P(B)(δ-)) to the primary electron acceptor B(A) (still mixed with P*) with the apparent time delay of ~1.1ps. Next step of ET is accompanied by the 3-ps appearance of bacteriopheophytin a(-) (H(A)(-)) band at 960nm. The study of the wave packet formation upon 20-fs illumination has shown that the vibration energy of the wave packet promotes reversible overcoming of an energy barrier between two potential energy surfaces P* and P*(P(A)(δ+)B(A)(δ-)) at ~500fs. For longer excitation pulses (40fs) this promotion is absent and tunneling through an energy barrier takes about 3ps. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: from Natural to Artificial.     

Light Suppresses Sporulation and Epidemics of Peronospora belbahrii

Peronospora belbahrii is a biotrophic oomycete attacking sweet basil. It propagates asexually by producing spores on dichotomously branched sporophores emerging from leaf stomata. Sporulation occurs when infected plants are incubated for at least 7.5h in the dark in moisture-saturated atmosphere at 10-27°C. Exposure to light suppresses spore formation but allows sporophores to emerge from stomata. Incandescent or CW fluorescent light of 3.5 or 6 µmoles.m².s^-1 respectively, caused 100% inhibition of spore formation on lower leaf surface even when only the upper leaf surface was exposed to light. The inhibitory effect of light failed to translocate from an illuminated part of a leaf to a shaded part of the same leaf. Inhibition of sporulation by light was temperature-dependent. Light was fully inhibitory at 15-27°C but not at 10°C, suggesting that enzyme(s) activity and/or photoreceptor protein re-arrangement induced by light occur at ≥15°C. DCMU or paraquat could not abolish light inhibition, indicating that photosystem I and photosystem II are not involved. Narrow band led illumination showed that red light (λmax 625 nm) was most inhibitory and blue light (λmax 440 nm) was least inhibitory, suggesting that inhibition in P. belbahrii, unlike other oomycetes, operates via a red light photoreceptor. Nocturnal illumination of basil in the field (4-10 µmoles.m².s^-1 from 7pm to 7am) suppressed sporulation of P. belbahrii and reduced epidemics of downy mildew, thus reducing the need for fungicide applications. This is the first report on red light inhibition of sporulation in oomycetes and on the practical application of light for disease control in the field.     

External electric field effects on prompt and delayed fluorescence in chloroplasts

An electric field pulse was applied to a suspension of osmotically swollen spinach chloroplasts after illumination with a saturating flash in the presence of DCMU. In addition to the stimulation of delayed fluorescence by the electric field, discovered by Arnold and Azzi (Arnold, W.A. and Azzi, R. (1971) Photochem. Photobiol. 14, 233–240) a sudden drop in fluorescence yield was observed. The kinetics of this fluorescence change were identical to those of the integrated delayed fluorescence emission induced by the pulse. The S-state dependence of the stimulated emission was very similar to that of the normal luminescence. We assume that the membrane potential generated by the pulse changes the activation energy for the back reaction in Photosystem II. On this basis, and making use of data we obtained earlier from electrochromic absorbance changes induced by the pulse, the kinetics of the field-induced prompt and delayed fluorescence changes, and also the amplitude of the fluorescence decrease, which was about 12% for a nearly saturating pulse, are explained. Our results indicate that in those reaction centers where a decrease of the activation energy occurs the effect of a pulse can be quite spectacular: the back reaction, which normally takes seconds, is completed in a few hundred microseconds when a sufficiently strong pulse is applied. Measurements of the polarization of the stimulated luminescence supported the interpretation given above.Only 2.8% of the back reaction was found to proceed via transition of reexcited chlorophyll to the ground state, both during the field pulse and in the absence of the field.     

Effect of low temperature (−30 to −60°C) on the reoxidation of the Photosystem II primary electron acceptor in the presence and absence of 3(3,4-dichlorophenyl)-1,1-dimethylurea

The fluorescence yield has been measured on spinach chloroplasts at low temperature (−30 to −60°C) for various dark times following a short saturating flash. A decrease in the fluorescence yield linked to the reoxidation of the Photosystem II electron acceptor Q is still observed at −60°C. Two reactions participate in this reoxidation: a back reaction or charge recombination and the transfer of an electron from Q⁻ to Pool A. The relative competition between these two reactions at low temperature depends upon the oxidation state of the donor side of the Photosystem II center:

1. (1) In dark-adapted chloroplasts (i.e. in States S₀+S₁ according to Kok, B., Forbush, B. and McGloin, M. (1970) Photochem. Photobiol. 11, 457–475), Q, reduced by a flash at low temperature, is reoxidized by a secondary acceptor and the positive charge is stabilized on the Photosystem II donor Z. Although this reaction is strongly temperature dependent, it still occurs very slowly at −60°C.

2. (2) When chloroplasts are placed in the S₂+S₃ states by a two-flash preillumination at room temperature, the reoxidation of Q⁻ after a flash at low temperature is mainly due to a temperature-independent back reaction which occurs with non-exponential kinetics.

3. (3) Long continuous illumination of a frozen sample at −30°C causes 6–7 reducing equivalents to be transferred to the pool. Thus, a sufficient number of oxidizing equivalents should have been generated to produce at least one O₂ molecule.

4. (4) A study of the back reaction in the presence of 3(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) shows the superposition of two distinct non-exponential reactions one temperature dependent, the other temperature independent.

Effect of Oxygen on Temporary Stabilization of Photoreduced Quinone Acceptors in Rhodobacter sphaeroides Reaction Centers

The effect of molecular oxygen on the photochemical activity of the Rhodobacter sphaeroides reaction centers frozen to 160 K under actinic illumination was investigated by the ESR method. About 90% of initially photochemically active bacteriochlorophyll (P) were fixed at 160 K for a long time in aerobic samples in an inactive form. In anaerobic samples, not more than 65% were fixed in an inactive form under the same conditions. In aerobic preparations, a small portion of photochemically active bacteriochlorophyll (about 10%) that retains its photochemical activity at 160 K after freezing under illumination has dark reduction kinetics similar to that of samples at room temperature after several seconds of actinic illumination. In anaerobic samples frozen under illumination, the remaining photochemically active reaction centers (35%) have the same dark reduction kinetics as samples illuminated at 295 K for 1-2 min. The conclusion is that the irreversible stabilization of bacteriochlorophyll P in the oxidized inactive state formed in the reaction centers frozen under illumination is brought about by light-induced conformational changes fixed under low temperatures.     

Inhibitory effect of p-nitrothiophenol in the light on the Photosystem II activity of spinach chloroplasts

The treatment of spinach chloroplasts with p-nitrothiophenol in the light at acidic and neutral pH's caused specific inhibition of the Photosystem II activity, whereas the same treatment in the dark did not affect the activity at all. The photosystem I activity was not inhibited by p-nitrothiophenol both in the light and in the dark. The inhibition was accompanied by changes of fluorescence from chloroplasts. As observed at room temperature, the 685-nm band was lowered by the p-nitrothiophenol treatment in the light and, at liquid nitrogen temperature, the relative height of the 695-nm band to the 685-nm band increased and the 695-nm band shifted to longer wavelengths. The action spectra for these effects of p-nitrothiophenol on the activity and fluorescence showed a peak at 670 nm with a red drop at longer wavelengths. It was concluded that the light absorbed by Photosystem II is responsible for the chemical modification of chloroplasts with p-nitrothiophenol to causing the specific inhibition of Photosystem II.