Phytochrome Control of Anthocyanin Biosynthesis in Tomato Seedlings: Analysis Using Photomorphogenic Mutants

Anthocyanin biosynthesis has been studied in hypocotyls and whole seedlings of tomato (Lycoperskon esculentum Mill.) wild types (WTs) and photomorphogenic mutants. In white light (WL)/dark (D) cycles the fri¹ mutant, deficient in phytochrome A (phyA), shows an enhancement of anthocyanin accumulation, whereas the tri¹ mutant, deficient in phytochrome Bl (phyBl) has a WT level of anthocyanin. Under pulses of red light (R) or R followed by far-red light (FR) given every 4 h, phyA is responsible for the non-R/FR reversible response, whereas phyBl is partially responsible for the R/FR reversible response. From R and blue light (B) pretreatment studies, B is most effective in increasing phytochrome responsiveness, whereas under R itself it appears to be dependent on the presence of phyBl. Anthocyanin biosynthesis during a 24 h period of monochromatic irradiation at different flu-ence rates of 4 day-old D-grown seedlings has been studied. At 660 nm the fluence rate-response relationships for induction of anthocyanin in the WT are similar, yet complex, showing a low fluence rate response (LFRR) and a fluence rate-dependent high irradiance response (HIR). The high-pigment-1 (hp-1) mutant exhibits a strong amplification of both the LFRR and HIR. The fri¹ mutant lacks the LFRR while retaining a normal HIR. In contrast, a transgenic tomato line overexpressing the oat PHYA3 gene shows a dramatic amplification of the LFRR. The tri¹ mutant, retains the LFRR but lacks the HIR, whereas the fri¹, tri¹ double mutant lacks both components. Only an LFRR is seen at 729 nm in WT; however, an appreciable HIR is observed at 704 nm, which is retained in the tri¹ mutant and is absent in the fri¹ mutant, indicating the labile phyA pool regulates this response component.     

PHOTOCONTROL OF ANTHOCYANIN SYNTHESIS IN TOMATO SEEDLINGS: A GENETIC APPROACH*

The photocontrol of anthocyanin synthesis in dark-grown seedlings of tomato (Lycopersicon esculentum Mill.) has been studied in an aurea (au) mutant which is deficient in the labile type of phytochrome, a high pigment (hp) mutant which has the wild-type level of phytochrome and the double mutant au/hp , as well as the wild type. The hp mutant demonstrates phytochrome control of anthocyanin synthesis in response to a single red light (RL) pulse, whereas there is no measurable response in the wild type and au mutant. After pretreatment with 12 h blue light (BL) the phytochrome regulation of anthocyanin synthesis is 10-fold higher in the hp mutant than in the wild type, whilst no anthocyanin is detectable in the au mutant, thus suggesting that it is the labile pool of phytochrome which regulates anthocyanin synthesis. The au/hp double mutant exhibits a small (3% of that in the hp mutant) RL/far-red light (FR)-reversible regulation of anthocyanin synthesis following a BL pretreatment. It is proposed that the hp mutant is hypersensitive to the FR-absorbing form of phytochrome (P_fr) and that this (hypersensitivity) establishes response to the low level of P_fl. (below detection limits in phytochrome assays) in the au/hp double mutant.     

SPECTRAL PROPERTIES,PHOTOTRANSFORMATION KINETICS AND PELLETABILITY OF PHYTOCHROME IN Pharbitis nil Chois*

Abstract— An examination has been made of the involvement of phytochrome in the circadian rhythm of flowering in Pharbitis nil Chois. The peak position of P_fr absorption changes with time after a red light pulse. The shortest absorption wavelength of P_fr occurs at the same time as flowering is inhibited by red light in dark grown, red light pretreated plants. Pelletable and supernatant phytochrome show a similar trend with lowest values found at the time of flower inhibition. Neither phototransformation kinetics nor intermediates of phytochrome which accumulate in white light show such a relationship to the circadian rhythm found in flowering of dark grown P. nil.     

KINETICS OF Pfr APPEARANCE IN Amaranthus caudatus‡

Abstract— The kinetics of the far-red absorbing form of phytochrome (P_fr) appearance from intermediates in the pathway from the red absorbing form of phytochrome (P_r) to P_fr that accumulate under high fluence rate white light have been investigated in 3-day old dark grown Amaranthus caudatus seedlings. The appearance of P_(r after a 5 s white light pulse was measured over the temperature range -8 to 25^°C in samples flushed with O₂ or N₂. Over the whole temperature range under anaerobic conditions the kinetics of the slowest component of P_fr appearance are faster than in the presence of O₂. Arrhenius plots are linear over this temperature range and indicate the activation energy for the slowest component of P_fr appearance is 44.05 ± 1.97 kJ mol^?1 for O₂ and 53.69 ± 4.86 kJ mol^?1 for N₂.     

PHYTOCHROME INTERMEDIATES IN VIVO–II. CHARACTERISATION OF INTERMEDIATES BY DIFFERENCE SPECTROPHOTOMETRY

Abstract— In epicotyl tissue of Pisum , irradiation of P_r at – 196°C forms a stable product P₆₉₈, whereas P_fr forms a stable product P₆₅₀. On warming P₆₉₈, dark transformation to P_r predominates. On warming P₆₅₀ to – 70°C an intermediate P₆₉₀ is formed which bleaches on further warming to –10°C. When tissue is cooled to –196°C during actinic irradiation, difference spectra for subsequent warming to –10°C indicate that P_r, P_fr and an intermediate P₇₁₀ are formed from weakly absorbing intermediates. Complete photoconversion of P_r to P_fr is not possible at temperatures below –5°C. As the temperature is reduced, the amount of P_fr produced from P_r decreases, while P₇₁₀ increases. P₇₁₀ can be photoconverted at –20°C and above, ultimately forming P_r, but in contrast to P_fr it is not photoconvertible at –196°C.     

STUDIES OF ADHESION OF METAL PARTICLES TO SILICA PARTICLES BASED ON ZETA POTENTIAL MEASUREMENTS

The zeta-potentials of silica, copper, platinum and gold particles have been measured as a function of pH. The isoelectric points were found to be at pH 3.0, 5.8, 3.0 and 3.5, respectively. In the pH range 3.0 to 5.8 copper and silica particles are oppositely charged and accordingly the coating of silica with copper particles could be demonstrated. In the case of gold and platinum the sign of the charge is such that direct adhesion to silica particles cannot be expected and this was also demonstrated in the case of platinum.