Wavelength dependence of the time course of fluorescence enhancement and photobleaching during irradiation of ethidium bromide-stained nuclei

The variation of fluorescence during irradiation of ethidium bromide-stained nuclei with the 458 nm argon laser line was measured at different wavelengths throughout the emission spectrum. When glycerol was used as a mountant, photoenhancement of fluorescence was observed at all wavelengths, but was greater at the shorter wavelengths. Fluorescence increased by almost one order of magnitude at 500 nm after 40 s of irradiation, compared with only about 10% at wavelengths longer than 600 nm after 2-3 s. In nuclei mounted in phosphate buffer, an initial photoenhancement of fluorescence was detected only at the shorter wavelengths, while continuous photobleaching was observed in the rest of the emission spectrum. When the spectra are normalized to maximum, so as to eliminate the effect of the concurrent photobleaching, it appears that the difference between the time course of fluorescence variation in buffer and glycerol depends largely on the lower photobleaching rate in glycerol. The photoenhancement of fluorescence at shorter wavelengths was found to consist of a band peaking at 485-491 nm in glycerol and at 495-496 nm in buffer. Attenuation of the inner-filter effect contributes minimally to the enhancement of fluorescence at shorter wavelengths. Since the dimer is known to be non fluorescent, the light-induced disaggregation of dimers to monomers cannot be an explanation for the large increase of fluorescence at the shorter wavelengths. The same laser beam that was used to excite the fluorescence of stained nuclei was also used for monitoring the concomitant variation of transmitted light, from which the variation of absorptance during irradiation was computed. While the expected decrease of absorptance was observed in glycerol, reflecting the photodestruction of the fluorophore, in buffer solution an unexpected initial increase was found, which may reflect the accumulation of an absorbing photoproduct.     

Stomatal closure by ultraviolet radiation

The effect of ultraviolet radiation (UV) (255–325 nm) on stomatal closure was investigated on tef [ Eragrostis tef (Zucc) Trotter] in the presence of white light (ca 50 ·mol m⁻² s⁻¹). The action spectrum showed that UV (ca 2 ·mol m⁻² s⁻¹, half band width about 10 nm) of 285 nm or shorter wavelengths was very efficient in causing stomatal closure. The effectiveness decreased sharply towards longer wavelengths. Radiation of 313 nm or longer wavelengths was practically without effect. Increasing UV intensity increased stomatal resistance. When stronger white light (5 to 9 times stronger than the one used during irradiation) was administered, stomates re-opened rapidly irrespective of whether the UV was on or off, although a subsequent gradual closing tendency was observed when the UV was on.     

The influence of season on adenine nucleotide concentrations and energy charge in four marsh plant species

Unilateral pulse ultraviolet irradiation caused positively phototropic coiling (> 180°) and curvature (≤ 180°) in the growth zone of dark-grown broom sorghum ( Sorghum bicolor Moench, cv. Acme Broomcorn and Sekishokuzairai Fukuyama) first internodes. Coiling was induced by irradiation at 257 to 302 nm, and proceeded to develop almost linearly during 72 h or more involving new tissue produced after irradiation. Curvature, caused at 308 to 413 nm and by red light, developed rapidly during the first several hours then slowly to cease by about 24 h, and did not surpass 120° even at the optimum photon fluences. Action spectra were higher towards shorter wavelengths, having a shoulder at about 287 nm, and could not separate the two photoresponses. The curvature was partially but markedly suppressed by far-red following the ultraviolet irradiation, whereas the coiling was not affected. Possible involvement of a specific UV-B photoreceptor and phytochrome in curvature and of a UV-C photoreceptor in coiling is discussed.     

Is There a Third Photoreceptor Involved in the Control of Chloroplast Movements in Mougeotia?

The photometric method was used to test a possibility proposed recently that a new photoreceptor with maximum activity at 620 nm is involved in mediating chloroplast rotation in Mougeotia (Z Lechowski, J Bialczyk [1988] Plant Physiol 88: 189-193). The hypothesis was tested under conditions of continuous dichromatic unilateral or mutually perpendicular irradiation with red light of wavelengths 620 or 660 (680) nanometers and far-red. When the red light was polarized parallel to the long cell axis, chloroplast response could be monitored by changing the direction of far-red irradiation. The level of the response obtained with red and far-red applied from the same direction depended on far-red intensity: at higher fluence rates the maximum response was shifted to longer wavelengths of red light. A high fluence rate of far-red inhibited the response. The absorption coefficients of Mougeotia chloroplasts were measured for the studied wave-lengths using the microphotometric method. Possible impact of absorption by the chloroplast on photoreception has been discussed. Current and previous results can be interpreted in terms of phytochrome action and do not support the involvement of the hypothetical 620 nanometer photoreceptor.     

Activating effect of light irradiation at various wavelength on the respiration in sperm of the echiuroid, Urechis unicinctus, in the presence of carbon monoxide.

In sperm of the echiuroid, Urechis unicinctus, respiration in the presence of CO was reversibly augmented by light irradiation in an examined range of wavelengths between 350 and 650 nm. The respiratory rate of sperm in the presence of CO was enhanced by light irradiation in proportion to the light fluence rate. A sharp and large peak was obtained at the wavelength of 430 nm in the action spectrum of photo-activated respiration of sperm in the presence of CO. Broad and small peaks were also found at around 530 and 570 nm. This action spectrum is similar in its profile to the absorption spectrum of reduced cytochrome b. Absorption of photon energy by reduced b-type cytochrome probably activates the redox reaction of this cytochrome to enhance the respiratory rate. Photo-activated respiration in the presence of CO was inhibited by antimycin A and cyanide. In this respiratory system, an electron equivalent is probably transferred through the mitochondrial respiratory chain between cytochrome b and cytochrome c and finally to molecular oxygen in the reaction catalyzed by the CO-insensitive terminal oxidase.     

Phototaxis in a dinoflagellate: Action spectra as evidence for a two-pigment system

Summary Action spectra were determined in the UV region of the spectrum for the first phase of the phototactic response (stop response) and for the phytochrome pigment associated with this response in the dinoflagellate Gyrodinium dorsum Kofoid. Differences between these action spectra indicate the participation of two pigments in phototaxis. Following R (620 nm) irradiation of the phytochrome, the stop response maxima occur at 470 and 280-nm; after FR irradiation they shift to 490 and 300–310 nm. These maxima suggest that the photoreceptor pigment for phototaxis is a carotenoprotein. The action spectrum shift following the different phytochrome conversions may represent a trans to cis isomer change by the carotenoid. The absorption maximum of P_R in the UV appears to be at 320 nm, which is consistent with the shift of the R absorption maximum to shorter wavelengths (620 nm) as compared to higher plants. The P_FR absorption maximum appears as a broad band between 360 and 390 nm. Comparison of P_R to P_FR conversions by different intensities of 620-nm and 320-nm light indicates that at lower intensities the logarithm of the threshold for the stop response is inversely proportional to the logarithm of the intensity of the sensitizing light. The ratio of response activation by R and UV light is about 4:1.Abbreviations FR far-red - R red - P_FR far-red-absorbing form of phytochrome - P_R red-absorbing form of phytochrome - UV ultraviolet     

Motility of the microtubular axostyle in Pyrsonympha

The rhythmic movement of the microtubular axostyle in the termite flagellate, Pyrsonympha vertens, was analyzed with polarization and electron microscopy. The protozoan axostyle is birefringent as a result of the semi-crystalline alignment of approximately 2,000 microtubules. The birefringence of the organelle permits analysis of the beat pattern in vivo. Modifications of the beat pattern were achieved with visible and UV microbeam irradiation. The beating axostyle is helically twisted and has two principal movements, one resembling ciliary and the other flagellar beating. The anterior portion of the beating axostyle has effective and recovery phases with each beat thereby simulating the flexural motion of a beating cilium. Undulations develop from the flexural flipping motion of the anterior segment and travel along the axostyle like flagellar waves. The shape of the waves differs from that of flagellar waves, however, and are described as sawtooth waves. The propagating sawtooth waves contain a sharp bend, approximately 3 micron in length, made up of two opposing flexures followed by a straight helical segment approximately 23 micron long. The average wavelength is approximately 25 micron, and three to four sawtooth waves travel along the axostyle at one time. The bends are nearly planar and can travel in either direction along the axostyle with equal velocity. At temperatures between 5 degrees and 30 degrees C, one sees a proportionate increase or decrease in wave propagation velocity as the temperature is raised or lowered. Beating stops below 5 degrees C but will resume if the preparation is warmed. A microbeam of visible light shone on a small segment of the axostyle causes the typical sawtooth waves to transform into short sine-like waves that accumulate in the area irradiated. Waves entering the affected region appear to stimulate waves already accumulated there to move, and waves that emerge take on the normal sawtooth wave pattern. The effective wavelengths of visible light capable of modifying the wave pattern is in the blue region of the spectrum. The axostyle is severed when irradiated with an intense microbeam of UV light. Short segments of axostyle produced by severing it at two places with a UV microbeam can curl upon themselves into shapes resembling lockwashers. We propose that the sawtooth waves in the axostyle of P. vertens are generated by interrow cross-bridges which are active in the straight regions.     

Inhibition of photosynthetic activity by UV-B radiation in radish seedlings

Inhibition of primary photosynthetic reactions by UV-B radiation (280 nm-320 nm) was demonstrated in radish leaves ( Raphanus sativus cv. Saxa Treib). Detached radish cotyledons from 10-day-old seedlings were irradiated with continuous white light and increasing UV-B irradiances using cut-off filters with increasing transmission for shorter wavelengths (WG 360, WG 345, WG 320, WG 305, WG 295, WG 280). Photosynthetic activity measured in terms of chlorophyll fluorescence induction (Kautsky effect) after 2, 4, 6, 8 and 24 h irradiation decreased in a wavelength dependent way with increasing UV-B irradiance and irradiation time.
Radish seedlings grown for 10 days from the time of germination under the same UV-B irradiation conditions exhibited similar reductions of the variable fluorescence as detached cotyledons irradiated for short time periods. They additionally had lower initial fluorescence at high UV-B radiation levels, although the chlorophyll content per leaf area increased. In contrast to short term experiments, the plastoquinone and flavonoid content increased with increasing UV-B irradiance when based on leaf area.     

Optical trapping for chromosome manipulation: a wavelength dependence of induced chromosome bridges.

Using a tunable titanium-sapphire laser, we have compared different wavelengths (from 700 to 840 nm) for their utility in optical trapping of chromosomes in mitotic rat kangaroo Potorous tridactylus (PtK2) cells. It was found that irradiation with a near-infrared light induces the sticking together of chromosome shoulders. The attached chromatids failed to separate, or separated with significant delay and formed a chromosome bridge during anaphase. Using this bridge (and induced c-mitosis) as a reference, we compared the action of different wavelengths (from 700 to 840 nm). Chromosomes were irradiated at metaphase and the cells were observed until the end of cytokinesis. Chromosomes were irradiated for different periods of time, using 130 mW of power at the objective focal plane. The biological responses observed after optical trapping were: (1) normal cell division, (2) formation of a temporary chromosome bridge, (3) formation of a permanent chromosome bridge, (4) complete blockage of chromosome separation (c-mitosis). The chromosomes were found to have a maximal sensitivity to 760-765 nm light and minimal sensitivity to 700 and 800-820 nm light. Cells with chromosomes irradiated for a long time, using wavelength 760-765 nm, generally were incapable of going through anaphase and remained in c-mitosis. We conclude that the optimal wavelengths for optical trapping are 700 and 800-820 nm.     

Action spectra of phototactic responses of the flea beetle, Phyllotreta striolata

Abstract.  Adult flea beetles, Phyllotreta striolata , show a strong positive phototactic response. The action spectrum of phototaxis of dark-adapted beetles was measured with minimal required light intensity between the wavelength range of 300 nm and 600 nm. Male and female flea beetles showed identical phototacitc behaviours. The beetles were most sensitive to light with peak wavelengths between 350 nm and 430 nm in the morning. In the afternoon and evening, the sensitivity to wavelengths shorter than 430 nm decreased, but they remained most sensitive to 430 nm. These results suggest that changes in sensitivity of the photoreceptors or nervous integration influence the phototactic responses, and that the blue wavelengths are more attractive than others.     

Action Spectrum for the Timing of Photo-Induced Cell Division in Adiantum Gametophytes

The photo-induced cell division in single-celled protonemata of the fern Adiantum capillus-veneris was studied. When the protonemata were exposed to monochromatic light at 50 nm intervals between 350 and 750 nm, irradiations in the blue and near-ultraviolet regions effectively induced cell division, while wavelengths longer than 550 nm showed no such effect. As reciprocity between duration and intensity was observed within the range of incident energy used, the action spectrum for the frequency of the photo-induced cell divisions 24 h after irradiation was determined between 360 and 510 nm at 10 nm intervals. Furthermore, the previously known effect of phytochrome on the timing of the cell division was minimized by a short exposure to red light given immediately after the monochromatic irradiation. The resulting action spectra showed a peak in the neighborhood of 460 nm with shoulders and another peak in the near-ultraviolet region.     

Temporal dynamics of ROS biogenesis under simulated solar radiation in the cyanobacterium Anabaena variabilis PCC 7937

We studied the temporal generation of reactive oxygen species (ROS) in the cyanobacterium Anabaena variabilis PCC 7937 under simulated solar radiation using WG 280, WG 295, WG 305, WG 320, WG 335, WG 345, and GG 400 nm cut-off filters to find out the minimum exposure time and most effective region of the solar spectrum inducing highest level of ROS. There was no significant generation of ROS in all treatments in comparison to the samples kept in the dark during the first 8 h of exposure; however, after 12 h of exposure, ROS were significantly generated in samples covered with 305, 295, or 280 nm cut-off filters. In contrast with ROS, the fragmentation of filaments was predominantly seen in 280 nm cut-off filter covered samples after 12 h of exposure. After 24 h of exposure, ROS levels were significantly higher in all samples than in the dark; however, the ROS signals were more pronounced in 320, 305, 295, or 280 nm cut-off filter covered samples. In contrast, the length of filaments was reduced in 305, 295, or 280 nm cut-off filter covered samples after 24 h of exposure. Thus, fragmentation of the filament was induced by all wavelengths of the UV-B region contrary to the UV-A region where only shorter wavelengths were able to induce the fragmentation. In contrast, ROS were generated by all wavelengths of the solar spectrum after 24 h of exposure; however, shorter wavelengths of both the UV-A and the UV-B regions were more effective in generating ROS in comparison to their higher wavelengths and photosynthetic active radiation (PAR). Moreover, lower wavelengths of UV-B were more efficient than the lower wavelengths of the UV-A radiation. Findings from this study suggest that certain threshold levels of ROS are required to induce the fragmentation of filaments.     

Hyperactivation is the mode conversion from constant-curvature beating to constant-frequency beating under a constant rate of microtubule sliding

Flagellar beating of hyperactivated golden hamster spermatozoa was analyzed in detail using digital image analysis and was compared to that of nonhyperactivated (activated) spermatozoa in order to understand the change in flagellar beating during hyperactivation and the active microtubule sliding that brought about the change in flagellar beating. Hyperactivated flagellar beating, which was characterized by a sharp bend in the proximal midpiece and low beat frequency, was able to alter the waveform with little change in beat frequency (constant-frequency beating), whereas activated flagellar beating, which was characterized by a slight bend in the proximal midpiece and high beat frequency, was able to alter beat frequency with little change in the waveform (constant-curvature beating). These results demonstrate that flagellar beating of hyperactivated and activated spermatozoa were essentially different modes and that hyperactivation was the mode conversion from constant-curvature beating to constant-frequency beating. Detailed analysis of flagellar bends revealed that the increase in curvature in the proximal midpiece during hyperactivation was due to the increase in total length of microtubule sliding in a nearly straight region between bends, while the rate of microtubule sliding remained almost constant.     

Photo-activation of respiration in the presence of CO in sperm of several marine invertebrates

• 1.1. The light irradiation at examined wavelengths between 360 and 630 nm enhanced the respiratory rate in the presence of CO in sperm, as well as eggs, of the sea urchins, Anthocidaris crassispina and Hemicentrotus pulcherrimus, the starfish, Asterina pectinifera, and the echiuroid, Urechis unicinctus.
• 2.2. The maximum peaks of stimulating effects of light irradiation on CO-insensitive respiration were found at wavelengths of 430, 530 and 570 nm in sperm of these species.
• 3.3. The respiration in the presence of CO was insensitive to light irradiation in sperm and eggs of the oyster, Crassostrea gigas and the tunicate, Ciona intestinaris.

     

Resolution of low-energy chlorophylls in Photosystem I of Synechocystis sp. PCC 6803 at 77 and 295 K through fluorescence excitation anisotropy

Fluorescence excitation spectra of highly anisotropic emission from Photosystem I (PS I) were measured at 295 and 77 K on a PS II-less mutant of the cyanobacterium Synechocystis sp. PCC 6803 (S. 6803). When PS I was excited with light at wavelengths greater than 715 nm, fluorescence observed at 745 nm was highly polarized with anisotropies of 0.32 and 0.20 at 77 and 295 K, respectively. Upon excitation at shorter wavelengths, the 745-nm fluorescence had low anisotropy. The highly anisotropic emission observed at both 77 and 295 K is interpreted as evidence for low-energy chlorophylls (Chls) in cyanobacteria at room temperature. This indicates that low-energy Chls, defined as Chls with first excited singlet-state energy levels below or near that of the reaction center, P700, are not artifacts of low-temperature measurements.If the low-energy Chls are a distinct subset of Chls and a simple two-pool model describes the excitation transfer network adequately, one can take advantage of the low-energy Chls' high anisotropy to approximate their fluorescence excitation spectra. Maxima at 703 and 708 nm were calculated from 295 and 77 K data, respectively. Upper limits for the number of low-energy Chls per P700 in PS I from S. 6803 were calculated to be 8 (295 K) and 11 (77 K).Abbreviations Chl - chlorophyll - BChl - bacteriochlorophyll - LHC - light-harvesting chlorophyll - PS - Photosystem - RC - reaction center - S. 6803 - Synechocystis sp. PCC 6803     

Action Spectrum for Photobleaching of Human Lenses by Short Wavelength Visible Irradiation

Purpose

Cataract is the world-leading cause of blindness. In search for a new treatment of cataract we have found that the yellow discolouration of aged human lenses can be photobleached using a non-invasive, infra-red, femtosecond laser treatment. These results were presented in an earlier PlosOne publication. The objective of the study was to characterize the single-photon photobleaching action spectrum of the aged human lens in vitro.

Methods

Ninety-one human donor lenses were irradiated with continuous wave laser light at 375, 405, 420, 445, 457 or 473 nm. Photobleaching was monitored by photography and transmission measurements.

Results

The action spectrum peaked at 420 nm followed by, in order of decreasing effect, 445, 457, 473, 405 and 375 nm. Younger and less absorbent lenses showed smaller changes than older and more absorbent lenses. There was a dose-dependent increase in lens transmission with increasing laser irradiation.

Conclusions

For a 75 year old lens an effect corresponding to elimination of 15 years or more of optical ageing was obtained. This study of the spectral characteristics and intensity needed to bleach the human lens with single-photon laser effects found an action-spectrum peak at 420 nm tailing gradually off toward longer wavelengths and more steeply toward shorter wavelengths. The results may be used to guide experiments with two-photon bleaching.     

The effects of light quality and intensity on the synthesis of ribulose-1,5-bisphosphate carboxylase and its mRNAs in the green alga Chlorogonium elongatum

In the green alga Chlorogonium elongatum the promoting effect of light on the synthesis of ribulose bisphosphate carboxylase/oxygenase (RuBPCase) is mainly caused by blue light of wavelengths between 430 nm and 510 nm, with a maximum effect at about 460 nm. Blue light also causes an increase in the amounts of the mRNAs for the large and the small subunits of the enzyme. Furthermore, the concentration of RuBPCase is affected by the light energy fluence rate. The rate of synthesis as well as the maximal obtainable concentration of the enzyme are functions of the light energy fluence rate up to 26 W·m^-2. No further increase occurs beyond that intensity. The quantity of irradiation also alters the concentrations of the subunit mRNAs. The results indicate that the changes in the mRNA levels are the major regulatory steps in the light-dependent synthesis of the RuBPCase enzyme.Abbreviations LSU large subunit - pSSU precursor of the small subunit - RuBPCase ribulose bisphosphate carboxylase/oxygenase EC 4.1.1.39 Dedicated to Prof. Dr. E. Bünning on the occasion of his 80 th birthday     

Spectral sensitivity studies on the visual system of the praying mantis, Tenodera sinensis

In these studies a constant ERG response was used as a measure of visual sensitivity to different wavelengths of light. The dark-adapted compound eye of Tenodera sinensis is dominated by a single class of photoreceptors. with a major peak of sensitivity at about 510–520 nm, and with a minor peak of sensitivity in the near-ultraviolet region at about 370 nm. The dark-adapted dorsal ocellus does not contain a homogeneous population of sensory receptors. The sensitivity function of the dark-adapted ocellus to longer wavelength light (yellow and red) is determined by a single receptor with a major peak of sensitivity in the green at 510–520 nm with some sensitivity in the near-ultraviolet. Sensitivity at shorter wavelengths (near-ultraviolet and blue), however, involves the stimulation of both this and a near-ultraviolet-sensitive receptor with a maximum sensitivity at about 370 nm. Anatomically, the sensory cells of the dorsal ocellus of Tenodera were determined histologically to be grouped into two distinct regions, each group making its own separate contribution to the ocellar nerve. This may represent the separation of two different photoreceptor types in the ocellus of the mantis.     

Photoisomerization of lycopene during carotenogenesis in mutant C-6D of Scenedesmus obliquus

Mutant C-6D of the unicellular green alga Scenedesmus obliquus has lost the ability to form cyclic carotenoids during heterotrophic growth in the dark. In the dark it accumulates acyclic intermediates, i.e. lycopene, neurosporene and ζ-carotene. The lycopene and two neurosporene forms were identified to be cis-isomers. Upon transfer to light, intermediates decrease and a normal set of carotenoids is synthesized. Inhibition of the cyclization reaction by nicotine reveals a lightinduced isomerization of cis-lycopene to trans-lycopene. Since the spectral characteristics of these two isomers differ drastically the isomerization can be followed in vivo by measuring a light-induced absorbance change. This absorbance change has its maximum at 520 nm and shows fast kinetics under high light intensities reaching a saturation level after about 2 min. Fluence-response curves for this absorbance change were performed for different wavelengths of actinic light. From the linear parts of these curves an action spectrum was caculated showing maxima at 670, 630 and 440 nm originating from chlorophyll and a maximum at shorter wavelengths (400–510 nm) which is interpreted to derive from ζ-carotene. A model for the light regulation of carotenogenesis in mutant C-6D is presented and the relation to the so-called 520-change observed in many plants is discussed.