Electron donor pool of photosystem II in Tris-washed chloroplasts in a study of low temperature delayed fluorescence

Transient time courses ("induction") and the intensity of thedelayed fluorescence of chlorophyll a (measured between 0.1and 3.9 msec after a 0.9 msec excitation period) were studiedwith a phosphoroscope at temperatures between 40 and –170°Cin Tris-washed chloroplasts. Tris-washing of chloroplasts changed the temperature dependenciesof the induction and the intensity of the delayed fluorescence.From the analysis of the induction each photosystem II reactioncenter appears to be linked to a donor pool which can supplyone electron to the acceptor pool in Tris-washed chloroplasts. An artificial electron donor, diphenylcarbazide affected thedelayed fluorescence above –100°C evidence that electronsare donated to photosystem II in at least two different ways. An electron transport inhibitor, 3-(3',4'-dichlorophenyl)-l,l-dimethylurea,changed the induction of the delayed fluorescence at temperaturesabove –60°C. The temperature dependence of the electron transport in thevicinity of photosystem II was characterized from these results. (Received May 27, 1980; )     

Simultaneous analysis of prompt and delayed chlorophyll a fluorescence in leaves during the induction period of dark to light adaptation

An attempt is made to reveal the relation between the induction curves of delayed fluorescence (DF) registered at 0.35-5.5 ms and the prompt chlorophyll fluorescence (PF). A simple formulation was proposed to link the ratio of the transient values of delayed and variable fluorescence with the redox state of the primary electron acceptor of Photosystem II--QA, and the thylakoid membrane energization. The term luminescence potential (UL) was introduced, defined as the sum of the redox potential of QA and the transmembrane proton gradient. It was shown that UL is proportional to the ratio of DF to the variable part of PF. The theoretical model was verified and demonstrated by analysing induction courses of PF and millisecond DF, simultaneously registered from leaves of barley--wild-type and the chlorophyll b-less mutant chlorina f2. A definitive correlation between PF and DF was established. If the luminescence changes are strictly due to UL, the courses of DF and PF are reciprocal and the millisecond DF curve resembles the first derivative of the PFt function.     

Delayed fluorescence in photosynthesis

Photosynthesis is a very efficient photochemical process. Nevertheless, plants emit some of the absorbed energy as light quanta. This luminescence is emitted, predominantly, by excited chlorophyll a molecules in the light-harvesting antenna, associated with Photosystem II (PS II) reaction centers. The emission that occurs before the utilization of the excitation energy in the primary photochemical reaction is called prompt fluorescence. Light emission can also be observed from repopulated excited chlorophylls as a result of recombination of the charge pairs. In this case, some time-dependent redox reactions occur before the excitation of the chlorophyll. This delays the light emission and provides the name for this phenomenon—delayed fluorescence (DF), or delayed light emission (DLE). The DF intensity is a decreasing polyphasic function of the time after illumination, which reflects the kinetics of electron transport reactions both on the (electron) donor and the (electron) acceptor sides of PS II. Two main experimental approaches are used for DF measurements: (a) recording of the DF decay in the dark after a single turnover flash or after continuous light excitation and (b) recording of the DF intensity during light adaptation of the photosynthesizing samples (induction curves), following a period of darkness. In this paper we review historical data on DF research and recent advances in the understanding of the relation between the delayed fluorescence and specific reactions in PS II. An experimental method for simultaneous recording of the induction transients of prompt and delayed chlorophyll fluorescence and decay curves of DF in the millisecond time domain is discussed.     

Irreversible changes in barley leaf chlorophyll fluorescence detected by the fluorescence temperature curve in a linear heating/cooling regime

The chlorophyll fluorescence (F) temperature curves in a linear time-temperature heating/cooling regime were used to study heat-induced irreversible F changes in primary green leaves of spring barley (Hordeum vulgare L. cv. Akcent). The leaf segments were heated in a stirred water bath at heating rates of 0.0083, 0.0166, 0.0333, and 0.0500 °C s⁻¹ from room temperature up to maximal temperature T _m and then linearly cooled to 35 °C at the same rate. The F intensity was measured by a pulse-modulated technique. The results support the existence of the two critical temperatures of irreversible F changes postulated earlier, at 45–48 and 53–55 °C. The critical temperatures are slightly dependent on the heating rate. Two types of parameters were used to characterize the irreversibility of the F changes: the coefficient of irreversibility μ defined as the ratio of F intensity at 35 °C at the starting/ending parts of the cycle and the slopes of tangents of linear parts of the F temperature curve. The dependence of μ on T _m revealed a maximum, which moved from 54 to 61 °C with the increasing heating/cooling rate v from 0.0083 to 0.0500 °C s⁻¹, showing two basic phases of the irreversible changes. The Arrhenius and Eyring approaches were applied to calculate the activation energies of the initial increase in μ. The values varied between 30 and 50 kJ mol⁻¹ and decreased slightly with the increasing heating rate.     

Floral Initiation of Upland Cotton Gossypium hirsutum L. in Response to Temperatures

The effect of germination temperature, duration of high-intensitylight, and day temperature in modifying the influence of nighttemperature on the flowering process of the M-8 strain of Uplandcotton was examined. In general, night temperatures above 28°C caused the first floral branch to be formed at a higher node.The magnitude of the reaction was conditioned by the other environmentalfactors studied. Germination temperature had a slight but significanteffect on subsequent floral responses to night temperature.Plants given eight-hour periods of high-intensity light eachday were delayed more by high night temperature than those exposedto 14 or 24 hours of high light. At high day temperatures (28–32°C) the inhibiting influence of the high night temperature wasgreatly increased. High day temperatures delayed floral initiationif the night temperature was high (28–32°C) but causeda lowering of position of first floral branch when the nighttemperature was low (20–22°C). The enhancement offlowering by 32°C days and 22°C nights was expressednot only in the low node of first floral branch, but also inthe shorter time from planting to floral initiation.     

Regulation of the photosynthetic electron transport chain

The regulation of electron transport between photosystems II and I was investigated in the plant Silene dioica L. by means of measurement of the kinetics of reduction of P₇₀₀ following a light-to-dark transition. It was found that, in this species, the rate constant for P₇₀₀ reduction is sensitive to light intensity and to the availability of CO₂. The results indicated that at 25 °C the rate of electron transport is down-regulated by approximately 40–50% relative to the maximum rate achievable in saturating CO₂ and that this down-regulation can be explained by regulation of the electron transport chain itself. Measurements of the temperature sensitivity of this rate constant indicated that there is a switch in the rate-limiting step that controls electron transport at around 20 °C: at higher temperatures, CO₂ availability is limiting; at lower temperatures some other process regulates electron transport, possibly a diffusion step within the electron transport chain itself. Regulation of electron transport also occurred in response to drought stress and sucrose feeding. Measurements of non-photochemical quenching of chlorophyll fluorescence did not support the idea that electron transport is regulated by the pH gradient across the thylakoid membrane, and the possibility is discussed that the redox potential of a stromal component may regulate electron transport. Received: 4 March 1999 / Accepted: 25 May 1999     

Effects of chill stress on prompt and delayed chlorophyll fluorescence from leaves

This paper describes the utilization of a portable solid state device for the simultaneous measurement of prompt and delayed fluorescence transients in leaves from a variety of species subjected to temperature lowering. The induction transients of the two phenomena were not identical as the peak in prompt fluorescence yield always preceded that of delayed fluorescence. Temperature lowering delayed the occurrence of peak fluorescence, increased prompt fluorescence yield, decreased delayed fluorescence yield, and caused the occurrence of a new, more rapid delayed fluorescence transient. Leaves from all species had qualitatively the same type of induction curves although the response to temperature differed between species. The delayed fluorescence yield of chill-sensitive species was reduced to a greater extent than that of chill-insensitive species. Cold hardening leaf material did not greatly change the fluorescence response to temperature lowering. Arrhenius plots showed a linear relationship between delayed fluorescence yield and temperature. There were no breaks that would suggest membrane lipid phase changes. The data indicate that thylakoid membranes of chill-sensitive species are less capable of maintaining a light-induced high energy state at low temperatures than are thylakoid membranes of chill-resistant species.     

Supercooling ability of Rhododendron flower buds in relation to cooling rate and cold hardiness

The freezing process and supercooling ability in flower budsof 11 native Rhododendron species were examined with referenceto the cooling rate and cold hardiness by differential thermalanalysis. The freezing patterns of the excised whole buds variedwith the season: in autumn, buds froze as whole units, whilein winter, freezing was initiated in the scales and propagatedto each floret. The supercooling ability of florets was enhancedduring winter. The freezing patterns in winter buds were stronglyinfluenced by the cooling rate (1 to 30°C/hr). Althoughthe first exotherm in scales occurred at –5 to –10°Gand was rate-independent, the occurrence of several floret exothermsshifted considerably to lower subzero temperatures at slowerrates. The most reliable cooling rate for testing maximum supercoolingability was l°C/hr. The exotherm in florets of hardier speciesoccurred at –20 to –25°C and at –7 to–20°C for less hardy ones, and were well correlatedwith their killing temperatures. Water relations within budtissues in response to freezing are briefly discussed. (Received June 26, 1980; )     

Supercooling ability of Rhododendron flower buds in relation to cooling rate and cold hardiness

The freezing process and supercooling ability in flower budsof 11 native Rhododendron species were examined with referenceto the cooling rate and cold hardiness by differential thermalanalysis. The freezing patterns of the excised whole buds variedwith the season: in autumn, buds froze as whole units, whilein winter, freezing was initiated in the scales and propagatedto each floret. The supercooling ability of florets was enhancedduring winter. The freezing patterns in winter buds were stronglyinfluenced by the cooling rate (1 to 30°C/hr). Althoughthe first exotherm in scales occurred at –5 to –10°Gand was rate-independent, the occurrence of several floret exothermsshifted considerably to lower subzero temperatures at slowerrates. The most reliable cooling rate for testing maximum supercoolingability was l°C/hr. The exotherm in florets of hardier speciesoccurred at –20 to –25°C and at –7 to–20°C for less hardy ones, and were well correlatedwith their killing temperatures. Water relations within budtissues in response to freezing are briefly discussed. (Received June 26, 1980; )     

The Freezing Response of an Arctic Cushion Plant, Saxifraga caespitosa L.: Acclimation, Freezing Tolerance and Ice Nucleation

Cold hardiness in actively growing plants of Saxifraga caespitosaL., an arctic and subarctic cushion plant, was examined. Plantscollected from subarctic and arctic sites were cultivated ina phytotron at temperatures of 3, 9, 12 and 21 °C undera 24-h photoperiod, and examined for freezing tolerance usingcontrolled freezing at a cooling rate of 3–4 °C eitherin air or in moist sand. Post-freezing injury was assessed byvisual inspection and with chlorophyll fluorescence, which appearedto be well suited for the evaluation of injury in Saxifragaleaves. Freezing of excised leaves in moist sand distinguishedwell among the various treatments, but the differences werepartly masked by significant supercooling when the tissue wasfrozen in air. Excised leaves, meristems, stem tissue and flowerssupercooled to –9 to –15 °C, but in rosettesand in intact plants ice nucleation was initiated at –4to –7 °C. The arctic plants tended to be more coldhardy than the subarctic plants, but in plants from both locationscold hardiness increased significantly with decreasing growthtemperature. Plants grown at 12 °C or less developed resistanceto freezing, and excised leaves of arctic Saxifraga grown at3 °C survived temperatures down to about –20 °C.Exposure to –3 °C temperature for up to 5 d did notsignificantly enhance the hardiness obtained at 3 °C. Whenwhole plants of arctic Saxifraga were frozen, with roots protectedfrom freezing, they survived –15 °C and –25°C when cultivated at 12 and 3 °C, respectively, althougha high percentage of the leaves were killed. The basal levelof freezing tolerance maintained in these plants throughoutperiods of active growth may have adaptive significance in subarcticand arctic environments. Saxifraga caespitosa L., arctic, chlorophyll fluorescence, cold acclimation, cushion plant, freezing stress, freezing tolerance, ice nucleation, supercooling     

Delayed fluorescence from Rhodopseudomonas sphaeroides following single flashes.

Delayed fluorescence from Rhodopseudomonas sphaeroides chromatophores was studied with the use of short flashes for excitation. Although the delayed fluorescence probably arises from a back-reaction between the oxidized reaction center bacteriochlorophyll complex (P+) and the reduced electron acceptor (X-), the decay of delayed fluorescence after a flash is much faster (tau1/2 approximately 120 mus) than the decay of P+X-. The rapid decay of delayed fluorescence is not due to the uptake of a proton from the solution, nor to a change in membrane potential. It correlates with small optical absorbance changes at 450 and 770 nm which could reflect a change in the state of X-. The intensity of the delayed fluorescence is 11-18-fold greater if the excitation flashes are spaced 2 s apart than it is if they are 30 s apart. The enhancement of delayed fluorescence at high flash repetition rates occurs only at redox potentials which are low enough (less than +240 mV) so that electron donors are available to reduce P+X- to PX- in part of the reaction center population. The enhancement decays between flashes as PX- is reoxidized to PX, as measured by the recovery of photochemical activity. Evidently, the reduction of P+X- to PX- leads to the storage of free energy that can be used on a subsequent flash to promote delayed fluorescence. The reduction of P+X- also is associated with a carotenoid spectral shift which decays as PX- is reoxidized to PX. Although this suggests that the free energy which supports the delayed fluorescence might be stored as a membrane potential, the ionophore gramicidin D only partially inhibits the enhancement of delayed fluorescence. With widely separated flashes, gramicidin has no effect on delayed fluorescence. At redox potentials low enough to keep X fully reduced, delayed fluorescence of the type described above does not occur, but one can detect weak luminescence which probably is due to phosphorescence of a protoporphyrin.     

Heat stress and the photosynthetic electron transport chain of the lichen <Emphasis Type="Italic">Parmelina tiliacea</Emphasis> (Hoffm.) Ach. in the dry and the wet state: differences and similarities with the heat stress response of higher plants

Thalli of the foliose lichen species Parmelina tiliacea were studied to determine responses of the photosynthetic apparatus to high temperatures in the dry and wet state. The speed with which dry thalli were activated by water following a 24 h exposure at different temperatures decreased as the temperature was increased. But even following a 24 h exposure to 50°C the fluorescence induction kinetics OJIP reflecting the reduction kinetics of the photosynthetic electron transport chain had completely recovered within 128 min. Exposure of dry thalli to 50°C for 24 h did not induce a K-peak in the fluorescence rise suggesting that the oxygen evolving complex had remained intact. This contrasted strongly with wet thalli were submergence for 40 s in water of 45°C inactivated most of the photosystem II reaction centres. In wet thalli, following the destruction of the Mn-cluster, the donation rate to photosystem II by alternative donors (e.g. ascorbate) was lower than in higher plants. This is associated with the near absence of a secondary rise peak (~1 s) normally observed in higher plants. Analysing the 820 nm and prompt fluorescence transients suggested that the M-peak (occurs around 2–5 s) in heat-treated wet lichen thalli is related to cyclic electron transport around photosystem I. Normally, heat stress in lichen thalli leads to desiccation and as consequence lichens may lack the heat-stress-tolerance-increasing mechanisms observed in higher plants. Wet lichen thalli may, therefore, represent an attractive reference system for the evaluation of processes related with heat stress in higher plants.     

Freezing Tolerance in Hydrated Lactuca sativa (L) Seed: A Model to Explain Observed Variation Between Seed Lots

Low temperature tolerance was investigated in the imbibed seedof 15 seed lots compnsmg seven cultivars of Lactuca sativa L.During rapid cooling (20 °C h^–1) some seeds of allseed lots survived to –16 °C but none to –20°C. The majority of seed lots retained over 50 per centviability above –14 °C due to isolation of the embryofrom external ice by the endosperm, and subsequent embryo super-cooling.Certain seed lots, including all three seed lots of cv. TomThumb, showed high mortality at temperatures above –10°C. Correlation of mortality with the formation of externalice suggested that the endosperm is not an effective nucleationbarrier in these seed lots. Survival to –20 °C was increased at slower coolingrates (6 to 1 °C h^–1) due to freeze desiccation ofthe embryo, but seed lots varied considerably in their toleranceof specific cooling rates. A model to explain this variationwas developed incorporatmg (1) seed lot super-cooling limittemperature, (2) the rate at which freeze dehydration of thesupercooled embryo took place, (3) the moisture content at whichnucleation (at –20 °C) was no longer certain and (4)the.initial equilibrium moisture content of the fully imbibedseed. Factors (1), (2) and (3) were found to be relatively constant,but low (or artificially reduced) seed moisture content wasclosely correlated with high survival at natural cooling rates.Seed size fractions of similar moisture content from a singlecultivar showed that more small seeds survive cooling at 3 °Ch^–1 to –20 °C than larger seed. Seed with pierced endosperms or ineffective nucleation barrierswere capable of surviving to at least –10 °C if cooledslowly (1 °C h^–1) but were killed by rapid (20 °Ch^–1) cooling. Lactuca sativa L, lettuce, seed germination freezing tolerance, super-cooling     

Studies on chlorophyll fluorescence in chloroplasts II. Effect of ferricyanide on the induction of fluorescence in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea

1. The effect of preincubating spinach chloroplasts with ferricyanideon the time courses of chlorophyll- fluorescence in the presenceof 3-(3,4-dichlorophyl)-1,1-dimethylurea (DCMU) was studied.When DCMU was absent from the preincubation mixture, but wasadded just before the onset of excitation light, preincubationof chloroplasts with ferricyanide markedly affected the fluorescencekinetics. The rise-rate was lowered and consequently the areaabove the induction curve (S/Fv), which is proportional to thepool size of the electron acceptor(s) for photosystem 2, increased.The maximum increase in the S/Fv was attained after 3 min and10 min, respectively, of preincubation with 5?10^–4M and3?10^–5M ferricyanide.
2. When DCMU was present during preincubationwith ferricyanide,the effect of ferricyanide in increasingthe S/Fv, was completelyeliminated.
3. The effect of ferricyanidewas also suppressed by addition offerrocyanide to the preincubationmixture. The redox potentialof the ferri-ferrocyanide mixturewhich produced 50% suppressionof the ferricyanide effect wasabout 360 mV.
4. A similar dependency of the ferricyanide effecton the redoxpotential was observed in Tris-treated chloroplasts.However,the redox potential of cytochrome b-559 was markedlyloweredby Tris-treatment.
5. These results were explained byassuming the occurrence of asecondary electron acceptor, R,between the reaction centerof photosystem 2 and the DCMU-sensitivesite.

(Received February 27, 1973; )     

Some properties of the chlorophyll fluorescence of the diatom Phaeodactylum tricornutum

Fluorescence transients were investigated with the diatom Phaeodactylumtricornutum. Supplementary experiments were done with Chaetocerossp. Under weak excitation ({small tilde}10³ erg/cm²sec), fluorescencetransients were induced simply by die oxidation-reduction reactionof Q, the primary reductant of photosystem II. The action spectraindicated that the electron transfer components between thetwo photosystems were in the most reduced state when fucoxanthinwas excited. The transients were observed with the 681 run emissionand with the 707 nm emission at room temperature. At –196°C,induction due to the reduction of Q. appeared both at the 681and 707 nm emissions. Similar results were also obtained withChaetoceros sp. Under strong excitation (10⁴–10⁵ erg/cm²-sec), the fluorescencetransients due to the interconversion between States 1 and 2of die pigment system (cf. ref. 27, 29) were observed. The transientswere induced by die alternate excitation of chlorophyll a andfucoxanthin or chlorophyll c. Conversion from State 2 to State1 was inhibited by DNP and CCCP, indicating that die processwas energy-dependent. Fluorescence spectra at –196°Cwere not altered by die state-conversion of die pigment system. These results suggest diat all die fluorescence bands whichappeared at room temperature and at –196°C were dueto die chlorophyll a of pigment system II in Phaeodactylum andChaetoceros. (Received September 7, 1972; )     

Primary and Secondary Induction Requirements for Flowering of Contrasting European Varieties of Lolium perenne

The flowering requirements of six European varieties of Loliumperenne L. were studied in controlled environments. In experimentson primary induction, flowering was recorded after transferto long days (LD) in a greenhouse at 12–24°C. In experimentson secondary induction, primary induction was first accomplishedat 6°C/10 h daylength for 12 weeks. When evaluated by the50% heading criterion, the requirement for duration of primaryinduction at 6°C/8 h daylength was <3 weeks in Mediterranean,5–6 weeks in Central European and 7–8 weeks in Scandinavianvarieties. While ‘Veyo’ (Italy) flowered profuselyregardless of temperature or daylength during primary induction,critical temperatures for primary induction in SD and LD were15 and 11°C in ‘Baca’ (Czech Republic) and 11and 7°C in ‘Falster’ (Denmark). The criticalphotoperiod for secondary induction at 15°C ranged from12 h in ‘Veyo’ and 14 h in ‘Baca’ to16.5 h in ‘Falster’ and 17.5 in ‘Kleppe’(Norway). The critical number of LD cycles varied correspondingly.While the Central and North European varieties required fewerLD cycles for 50% heading at 18 than at 12°C, ‘Veyo’showed the opposite response. It is concluded that the requirementsfor both primary and secondary induction of Lolium perenne increasewith increasing latitude of origin of the germplasm. In oneexperiment, 39–87% of the inflorescences came from tillersthat were not visible on transfer from primary to secondaryinduction, thus it is also concluded that there is no juvenilestage in tillers of Lolium perenne. Copyright 2000 Annals ofBotany Company Daylength, flowering, juvenility, perennial ryegrass (Lolium perenne L.), primary induction, secondary induction, temperature, varieties, vernalization     

Delayed fluorescence from Rhodopseudomonas sphaeroides following single flashes

Delayed fluorescence from Rhodopseudomonas sphaeroides chromatophores was studied with the use of short flashes for excitation. Although the delayed fluorescence probably arises from a back-reaction between the oxidized reaction center bacteriochlorophyll complex (P⁺) and the reduced electron acceptor (X^?), the decay of delayed fluorescence after a flash is much faster ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 120 μ}\text{s}$) than the decay of P⁺X^?. The rapid decay of delayed fluorescence is not due to the uptake of a proton from the solution, nor to a change in membrane potential. It correlates with small optical absorbance changes at 450 and 770 nm which could reflect a change in the state of X^?.The intensity of the delayed fluorescence is 11–18-fold greater if the excitation flashes are spaced 2 s apart than it is if they are 30 s apart. The enhancement of delayed fluorescence at high flash repetition rates occurs only at redox potentials which are low enough (< + 240 mV) so that electron donors are available to reduce P⁺X^? to PX^? in part of the reaction center population. The enhancement decays between flashes as PX^? is reoxidized to PX, as measured by the recovery of photochemical activity. Evidently, the reduction of P⁺X^? to PX^? leads to the storage of free energy that can be used on a subsequent flash to promote delayed fluorescence. The reduction of P⁺X^? also is associated with a carotenoid spectral shift which decays as PX^? is reoxidized to PX. Although this suggests that the free energy which supports the delayed fluorescence might be stored as a membrane potential, the ionophore gramicidin D only partially inhibits the enhancement of delayed fluorescence. With widely separated flashes, gramicidin has no effect on delayed fluorescence.At redox potentials low enough to keep X fully reduced, delayed fluorescence of the type described above does not occur, but one can detect weak luminescence which probably is due to phosphorescence of a protoporphyrin.     

Delayed fluorescence from Rhodopseudomonas viridis following single flashes.

Delayed fluorescence from Rhodopseudomonas viridis membrane fragments has been studies using a phosphoroscope employing single, short actinic flashes, under conditions of controlled redox potential and temperature. The emission spectrum shows that delayed fluorescence is emitted by the bulk, antenna bacteriochlorophyll. The energy for delayed fluorescence, however, must be stored in a reaction-center complex including the photooxidized form (P+) of the primary electron-donor (P) and the photoreduced form (X MINUS) of the primary electron-acceptor. This is shown by the following observations: (1) Delayed luminescence is quenched (a) at low redox potentials which allow cytochromes to reduce P+ rapidly after the flash, (b) at higher redox potentials which, by oxidizing P chemically, prevent the photochemical formation of P+X minus, and (c) upon transfer of an electron from X minus to a secondary acceptor, Y. (2) Under conditions that prevent the reduction of P+ by cytochromes and the oxidation of X minus by Y, the decay kinetics of delayed fluorescence are identical with those of P+X minus, as measured from optical absorbance changes. The main decay route for P+X minus under these conditions has a rate-constant of approximately 10-3-s-minus 1. In contrase, a comparison of the intensities of delayed and prompt fluorescence indicates that the process in which P+X minus returns energy to the bulk bacteriochlorophyll has a rate-constant of 3.7 s-minus 1, at 295 degrees K and pH 7.8. The decay kinetics of P+X minus and delayed fluorescence change little with temperature, whereas the intensity of delayed fluorescence increases with increasing temperature, having an activation energy of 12.5 kcal mol-mol- minus 1. We conclude that the main decay route involves tunneling of an electron from X minus to P+, without the promotion of P to an excited state. Delayed fluorescence requires such a promotion, followed by transfer of energy to the bulk bacteriochlorophyll, and this combination of events is rare. The activation energy, taken with potentiometric data, indicates that the photochemical conversion of PX to P+X minus results in increases of both the energy and the entropy of the system, by 16.6 kcal-mol- minus 1 and 8.8 cal-mol- minus 1-deg- minus 1. The intensity of delayed fluorescence depends strongly on the pH; the origin of this effect remains unclear.     

Temperature dependence of delayed ehlorophyll fluorescence in intact leaves of higher plants. A rapid method for detecting the phase transition of thylakoid membrane lipids

The temperature dependence of the yield of in vivo prompt and delayed chiorophyll fluorescence was investigated in maize and barley leaves. In the chilling-sensitive maize, delayed fluorescence at steady-state level showed a maximum near the temperature at which thylakoid membrane lipids undergo a phase transition as revealed by differential scanning calorimetry measurements. In the chilling-resistant barley, no phase transition was detected above 0°C and the delayed light emission varied in a monotonic fashion. It was shown that measurements of delayed luminescence intensity in vivo can provide a rapid and sensitive method for detecting the phase change of membrane lipids in intact leaves of chilling-sensitive plant species such as tomato, cotton, cucumber, castor bean or avocado. In contrast, the use of steady-state prompt chlorophyll fluorescence as an indicator of membrane fluidity change was not successful.     

Temperature Effects on Pea Plants Probed by Simultaneous Measurements of the Kinetics of Prompt Fluorescence,Delayed Fluorescence and Modulated 820 nm Reflection

Simultaneous in vivo measurements of prompt fluorescence (PF), delayed fluorescence (DF) and 820-nm reflection (MR) were made to probe response of pea leaves to 40 s incubation at high temperatures (25–50°C). We interpret our observation to suggest that heat treatment provokes an inhibition of electron donation by the oxygen evolving complex. DF, in a time range from several microseconds to milliseconds, has been thought to reflect recombination, in the dark, between the reduced primary electron acceptor Q_A ^– and the oxidized donor (P680⁺) of photosystem II (PSII). The lower electron transport rate through PSII after 45 and 50°C incubation also changed DF induction. We observed a decrease in the amplitude of the DF curve and a change in its shape and in its decay. Acceleration of P700⁺ and PC⁺ re-reduction was induced by 45°C treatment but after 50°C its reduction was slower, indicating inhibition of photosystem I. We suggest that simultaneous PF, MR and DF might provide useful information on assessing the degree of plant tolerance to different environmental stresses.