Nd:YAP激光辐照对雨生红球藻生理效应的荧光分析

目的：Nd：YAP激光辐照对雨生红球藻生理效应的荧光分析j方法：利用Nd：YAG激光（功率10W,辐照剂量为15s、35s、55s）辐照雨生红球藻,在对辐照细胞进行生长测定以及色素吸收光谱分析的基础上,进一步利用激光共聚焦扫描显微镜（LSCM）,在波长488nm的Ar^＋激发光条件下,对细胞的自体荧光以及吖啶橙染色的细胞核荧光物质进行定位定量分析,获得细胞自发荧光光谱和细胞核荧光物质的荧光光谱。结果：①低剂量的Nd：YAG激光辐照（15s左右）对藻细胞有促长作用,生长速率提高20．3％,色素吸收峰的峰值提高25．3％。较高剂量的Nd：YAG激光辐照（35s、55s）对藻细胞生长有抑制作用,并有明显的致死、致突效应。②对自体荧光的分析结果表明,与对照组相比,低剂量激光辐照组的细胞,在荧光光谱的峰型及峰值上变化不大,在682nm处均有较强的荧光发射,而高剂量激光辐照组的细胞多无明显的荧光发射。③对细胞核荧光物质的分析,雨生红球藻细胞在530nm（DNA）和640nm（RNA）处均有荧光发射峰。与对照组相比,低剂量激光辐照组的DNA荧光发射有所增强,但RNA的荧光发射则有所减弱;高剂量激光辐照组的核物质荧光发射谱,在峰型上与对照组存在差异,荧光强度也明显下降。结论：低剂量的Nd：YAP激光辐照对细胞核的DNA合成与复制有一定的刺激作用,可促进光合色素的合成并提高其对光能的吸收效率,从而增强光合活性,促进细胞的增殖与生长;高剂量激光辐照则对细胞的DNA有损伤作用,是致死率上升并发生突变的可能原因。     

Fe^3＋对雨生红球藻（Haematococcus pluvialis）生长及荧光特性的影响

为探求适宜雨生红球藻CG-06株生长的Fe^3＋浓度和Fe^3＋对藻细胞荧光特性的影响,以BBM为基础培养基,选用EDTA—FeNa（Ⅲ）为Fe^3＋源,设置0、1．79、8．95、17．9、35．8、71．6μmol·L^-1 6种Fe^3＋浓度梯度,实验测定藻的生长并分析不同Fe^3＋对藻细胞叶绿素荧光和77K低温荧光等的影响。结果表明：适合雨生红球藻CG-06株生长的Fe^3＋浓度为8．95μmol·L^-1,Fe^3＋浓度较高时,雨生红球藻的生长受到抑制,Fe^3＋浓度低于1．79μmol·L^-1将产生低铁限制。Walz—PAM测定数据显示,在铁不足或高铁抑制条件下,雨生红球藻光系统Ⅱ活性明显下降,开放态的反应中心数目减少,光合作用受到抑制。77K低温荧光光谱显示,在铁不足或高铁抑制条件下,710nm荧光峰降低,684nm和694nm荧光峰相对增强,说明能量在两个光系统分配上发生变化,能量更多的分配给光系统Ⅱ,限制了光系统Ⅰ的活性。在高铁抑制条件下,CP47蛋白荧光峰降低,CP43蛋白荧光峰增强,推测存在D1蛋白降解。     

Fe3+对雨生红球藻(Haematococcus pluvialis)生长及荧光特性的影响

为探求适宜雨生红球藻CG-06株生长的Fe³⁺浓度和Fe³⁺对藻细胞荧光特性的影响,以BBM为基础培养基,选用EDTA-FeNa(Ⅲ)为Fe³⁺源,设置0、1.79、8.95、17.9、35.8、71.6μmol·L^-16种Fe³⁺浓度梯度,实验测定藻的生长并分析不同Fe³⁺对藻细胞叶绿素荧光和77 K低温荧光等的影响。结果表明:适合雨生红球藻CG-06株生长的Fe³⁺浓度为8.95μmol·L^-1,Fe³⁺浓度较高时,雨生红球藻的生长受到抑制,Fe³⁺浓度低于1·79μmol.L^-1将产生低铁限制。W alz-PAM测定数据显示,在铁不足或高铁抑制条件下,雨生红球藻光系统Ⅱ活性明显下降,开放态的反应中心数目减少,光合作用受到抑制。77 K低温荧光光谱显示,在铁不足或高铁抑制条件下,710 nm荧光峰降低,684 nm和694 nm荧光峰相对增强,说明能量在两个光系统分配上发生变化,能量更多的分配给光系统Ⅱ,限制了光系统Ⅰ的活性。在高铁抑制条件下,CP₄₇蛋白荧光峰降低,CP₄₃蛋白荧光峰增强,推测存在D₁蛋白降解。     

氮源对雨生红球藻绿色生长期细胞生长的影响

【背景】雨生红球藻(Haematococcus pluvialis)细胞能合成积累具有超强抗氧化活性的虾青素,是生产高值天然虾青素的优异藻种。【目的】解析不同氮源对雨生红球藻生长的效应,以期建立优化氮素营养提高雨生红球藻生物量和虾青素产量的技术体系。【方法】选用Na NO3和NH_4Cl为氮源、辅以pH缓冲液Hepes,培养雨生红球藻藻株797,测试2种不同氮源对雨生红球藻藻液pH、营养生长期(绿色生长期)藻细胞生长、叶绿素含量和生物量等的影响。【结果】以Na NO3为氮源培养的雨生红球藻细胞的比生长速率、生物量、叶绿素a和叶绿素b含量均高于以NH_4Cl为氮源培养的藻细胞。不同氮源对雨生红球藻培养液的pH值有显著影响,NH_4Cl氮源导致培养液pH值降低,然而Na NO3氮源则导致培养液pH值上升。添加pH缓冲液Hepes能有效稳定培养液的pH值,并促进雨生红球藻的生长,尤以NH_4Cl为氮源添加Hepes的效果更显著。不同氮源导致雨生红球藻营养生长阶段细胞的生长和生物量等差异主要源于不同氮源引起藻液pH的变化。【结论】添加pH缓冲液Hepes可有效控制藻液pH,进而显著促进以Na NO3和NH_4Cl为氮源的雨生红球藻营养生长阶段细胞的生长和生物量积累。     

CO_2浓度对雨生红球藻生理生化指标的影响

为了探讨雨生红球藻对不同CO_2浓度的响应,利用生理生化测定方法比较了两种CO_2浓度对雨生红球藻生长、色素含量、叶绿素荧光参数和两种碳代谢相关酶的影响。结果显示在雨生红球藻的绿色营养阶段,4倍空气CO_2浓度下培养的藻细胞密度是空气CO_2浓度下的3.08倍(第10天),与空气CO_2相比,较高CO_2培养藻的叶绿素和类胡萝卜素含量、胞外碳酸酐酶(CA)活性降低,非光化学淬灭(NPQ)显著升高,最大光能转化效率(Fv/Fm)、实际光化学量子效率(ФPSII)多显著升高,而光化学淬灭(q P)、核酮糖-1,5-二磷酸羧化酶/加氧酶(Rubisco)活性无显著差异。在雨生红球藻的红色孢子阶段,4倍空气CO_2培养下的藻细胞密度显著降低,但虾青素含量提高了20.23%(第8天)。以上研究表明可以通过适当提高CO_2浓度来促进雨生红球藻的生长和虾青素的积累。     

UV-B辐射对雨生红球藻光合特性和虾青素含量的影响及其响应

实验研究了不同强度的UV-B(280-320 nm)辐射对雨生红球藻(Haematococcus pluvialis)的光合活性、生物量、色素含量、活性氧(ROS)含量和抗氧化酶活性等的影响, 以探讨利用UV-B辐射诱导虾青素生物合成增强的可能性。结果发现, 经UV-B辐射处理后,雨生红球藻的光合活性降低、生物量增长被抑制。UV-B辐射对叶绿素影响不大, 但会改变细胞的类胡萝卜素和虾青素含量:0.1和0.3 W/m2强度的UV-B辐射使细胞中的这两种色素含量升高, 0.5 W/m2组的色素含量短暂升高后恢复到对照水平。中低强度的UV-B可以促进雨生红球藻单细胞虾青素含量的增加, 但由于其对细胞生长的抑制作用, 并不能使虾青素大量积累。随辐射时间延长, 细胞内ROS含量未明显增加,但抗氧化酶(过氧化氢酶和超氧化物歧化酶)活性下降, 雨生红球藻可能主要依靠虾青素来淬灭ROS。以上结果表明, UV-B辐射对雨生红球藻的主要生理生化过程有抑制作用, UV-B辐射既可以诱导虾青素的合成又会消耗一部分虾青素, 对虾青素含量的影响与其强度有关, 而利用虾青素来清除细胞内的ROS可能是雨生红球藻抵御这种不利环境条件的最重要的途径。       

雨生红球藻ZL-1 生长和虾青素积累条件优化

分离鉴定了一株雨生红球藻ZL-1, 比较了不同接种密度和吲哚乙酸浓度对其生长的影响; 在此基础上, 探究了不同浓度水杨酸和盐度对雨生红球藻虾青素积累的影响。结果表明: (1)接种密度为2.00×10⁴ cell·mL^–1 时, 雨生红球藻生长快速, 最终生物量达到最大值0.43 g·L^–1; 不动细胞比游动细胞更快的积累虾青素, 高光诱导不动细胞得到最高虾青素产量为8.44 mg·L^–1; IAA 终浓度为1.5 mg·L^–1 时, 雨生红球藻生长速度最快, 最终细胞密度和干重分别比对照组提高了24.28%和27.11%; (2)水杨酸具有缓解高光胁迫和促进虾青素积累的双重作用, 15 和25 mg·L^–1水杨酸诱导下, 雨生红球藻生物量较高, 虾青素产量分别比对照组提高了18.18%和18.94%; 使用4‰的盐度胁迫雨生红球藻, 虾青素产量较对照组提高了17.42%, 但盐度也会引起藻细胞的漂白、死亡, 导致生物量显著降低。     

氮胁迫对雨生红球藻色素积累与抗氧化系统的影响

选用雨生红球藻CG-06为试验藻株,以BBM为基础培养基,分别设置了0、13.7、27.5、41.2mg·L-1四个硝态氮浓度梯度,分析并探讨在不同硝态氮浓度条件下雨生红球藻生长、生理特性、细胞内主要色素含量的变化以及抗氧化酶活性。结果表明：细胞中色素的积累量和积累速率与初始硝态氮浓度成反比,与抗氧化酶活性呈负相关。缺氮时,培养到第3天的藻细胞中虾青素含量达到4.95μg·mg-1,而对照组在培养到第9天的细胞中才开始产生虾青素,而且在整个培养周期内细胞中的虾青素最大含量仅为4.17μg·mg-1。酶活测定结果显示,虾青素含量较高的红色细胞中,超氧化物歧化酶（SOD）、过氧化氢酶（CAT）和谷胱甘肽过氧化物酶（GSH-Px）的活性明显高于绿色细胞,且GSH-Px活性最高。研究表明,雨生红球藻可能有两种过氧化防御机制,绿色细胞阶段以抗氧化酶作用为主,在培养后期启动虾青素保护机制,两种机制具有协同作用。     

雨生红球藻培养过程中色素动态变化与光合生理特性研究

以雨生红球藻Haematococcus pluvialis CG-06为实验材料,分析测定在正常培养周期内藻细胞主要色素的变化动态、光合生理特性,以及培养基中硝态氮的含量。结果表明,雨生红球藻在绿色细胞阶段的主要色素包括:叶绿素、叶黄素、β-胡萝卜素,培养至红色细胞阶段增加了角黄素、海胆酮、虾青素单酯及双酯等次生类胡萝卜素。硝态氮浓度在培养初期下降迅速,第3 d降至4.875 mg/L,下降了85.3%,至第7 d下降为0.169 mg/L。雨生红球藻培养至第7 d时,细胞中开始检测出虾青素,含量为0.159 mg/g,此时虾青素合成速度较快,至第11 d虾青素含量上升为1.68 mg/g,在虾青素合成初期β-胡萝卜素的含量下降。藻细胞的光合速率、呼吸速率和NPQ在培养前期比较稳定,第7 d细胞光合速率开始下降,而呼吸速率和NPQ则上升,在整个培养周期中,藻细胞的Fv/Fm变化不明显。     

雨生红球藻培养基的改良

近年来,雨生红球藻（ＨａｅｍａｔｏｃｏｃｃｕｓｐｌｕｖｉａｌｉｓＦｌｏｔｅｔＷｉｌｌ）作为一种获取天然虾青素的资源被广泛重视ｌ‘,‘１。目前,有关而生红球藻的研究主要集中于虾青素的积累机制、合成调控及其生物学功能‘）。关于雨生红球资生长调控方面的工作报道较少,还没有一个很理想的红球藻培养基【’］,从而在很大程度上阻碍了对雨生红球藻的深人研究与开发利用。雨生红球藻尤其是它的绿色游动细胞对环境ｐＨ值的改变较敏感,其生长状况与培养液的ｐＨ稳定性关系密切［‘”］,而目前较多采用的ＭＣＭ、ＢＢＭ和Ｂｔｈｌ…     

Multiphoton excitation fluorescence microscopy and spectroscopy of in vivo human skin

Multiphoton excitation microscopy at 730 nm and 960 nm was used to image in vivo human skin autofluorescence from the surface to a depth of approximately 200 microm. The emission spectra and fluorescence lifetime images were obtained at selected locations near the surface (0-50 microm) and at deeper depths (100-150 microm) for both excitation wavelengths. Cell borders and cell nuclei were the prominent structures observed. The spectroscopic data suggest that reduced pyridine nucleotides, NAD(P)H, are the primary source of the skin autofluorescence at 730 nm excitation. With 960 nm excitation, a two-photon fluorescence emission at 520 nm indicates the presence of a variable, position-dependent intensity component of flavoprotein. A second fluorescence emission component, which starts at 425 nm, is observed with 960-nm excitation. Such fluorescence emission at wavelengths less than half the excitation wavelength suggests an excitation process involving three or more photons. This conjecture is further confirmed by the observation of the super-quadratic dependence of the fluorescence intensity on the excitation power. Further work is required to spectroscopically identify these emitting species. This study demonstrates the use of multiphoton excitation microscopy for functional imaging of the metabolic states of in vivo human skin cells.     

Spectroscopic studies on origination of the peak at 730 nm in delayed fluorescence of chloroplasts.

The origination of the peak at 730 nm in the delayed fluorescence (DF) spectrum of chloroplasts was studied using various optical analysis methods. The DF spectrum showed that the main emission peak was at about 685 nm, with a small shoulder at 730 nm when the chloroplast concentration was < 7.8 microg/mL. The intensity of the peak at 685 nm decreased, while the intensity of the peak at 730 nm increased, when the chloroplast concentrations were increased from 7.8 to 31.2 microg/mL. With the concentration increasing, the peak at 730 nm became dominant while the peak at 685 nm finally disappeared. The DF decay kinetic curves showed that the intensity of the peak at 730 nm decayed as the same speed as the intensity of the peak at 685 nm during the entire relaxation process (0.5-30.5 s). With the excitation wavelength at 685 nm, the emission intensity was stronger in the excitation spectrum at 730 nm. The absorption spectrum demonstrated that the ratio A(685):A(730) remained almost constant when the chloroplast concentration increased. The results suggest that the peak at 730 nm appearing in DF is mainly contributed by the fluorescence of photosystem I (PSI), generated by the re-absorption of 685 nm band DF.     

High resolution emission spectra of one second delayed fluorescence from chloroplasts

The first well resolved emission spectra of white light-illuminated spinach chloroplasts at room temperature show that one second delayed fluorescence occurs at 685 nm. We demonstrate that reabsorption of this delayed fluorescence induces the second (probably prompt) emission observed at 730 nm and which we identify with the photosystem I peripheral antenna system.     

Fluorescence emission spectra of photosystem I, photosystem II and the light-harvesting chlorophyll a/b complex of higher plants

Fluorescence emission spectra excited at 514 and 633 nm were measured at -196 degrees C on dark-grown bean leaves which had been partially greened by a repetitive series of brief xenon flashes. Excitation at 514 nm resulted in a greater relative enrichment of the 730 nm emission band of Photosystem I than was obtained with 633 nm excitation. The difference spectrum between the 514 nm excited fluorescence and the 633 nm excited fluorescence was taken to be representative of a pure Photosystem I emission spectrum at -196 degrees C. It was estimated from an extrapolation of low temperature emission spectra taken from a series of flashed leaves of different chlorophyll content that the emission from Photosystem II at 730 nm was 12% of the peak emission at 694 nm. Using this estimate, the pure Photosystem I emission spectrum was subtracted from the measured emission spectrum of a flashed leaf to give an emission spectrum representative of pure Photosystem II fluorescence at -196 degrees C. Emission spectra were also measured on flashed leaves which had been illuminated for several hours in continuous light. Appreciable amounts of the light-harvesting chlorophyll a/b protein, which has a low temperature fluorescence emission maximum at 682 nm, accumulate during greening in continuous light. The emission spectra of Photosystem I and Photosystem II were subtracted from the measured emission spectrum of such a leaf to obtain the emission spectrum of the light-harvesting chlorophyll a/b protein at -196 degrees C.     

Fluorescence emission spectra of Photosystem I,Photosystem II and the light-harvesting chlorophyll a/b complex of higher plants

Fluorescence emission spectra excited at 514 and 633 nm were measured at ?196 °C on dark-grown bean leaves which had been partially greened by a repetitive series of brief xenon flashes. Excitation at 514 nm resulted in a greater relative enrichment of the 730 nm emission band of Photosystem I than was obtained with 633 nm excitation. The difference spectrum between the 514 nm excited fluorescence and the 633 nm excited fluorescence was taken to be representative of a pure Photosystem I emission spectrum at ?196 °C. It was estimated from an extrapolation of low temperature emission spectra taken from a series of flashed leaves of different chlorophyll content that the emission from Photosystem II at 730 nm was 12% of the peak emission at 694 nm. Using this estimate, the pure Photosystem I emission spectrum was subtracted from the measured emission spectrum of a flashed leaf to give an emission spectrum representative of pure Photosystem II fluorescence at ?196 °C. Emission spectra were also measured on flashed leaves which had been illuminated for several hours in continuous light. Appreciable amounts of the light-harvesting chlorophyll a/b protein, which has a low temperature fluorescence emission maximum at 682 nm, accumulate during greening in continuous light. The emission spectra of Photosystem I and Photosystem II were subtracted from the measured emission spectrum of such a leaf to obtain the emission spectrum of the light-harvesting chlorophyll a/b protein at ?196 °C.     

Non-photochemical quenching of Fo in leaves is emission wavelength dependent: consequences for quenching analysis and its interpretation

The effects of light-induced non-photochemical quenching on the minimal F_o, and variable F_v, fluorescence emissions at 690 and 730 nm in leaves were determined. Non-photochemical quenching of F_o, but not F_v, was found to be dependent upon the wavelength of emission, and was greater at 690 nm than at 730 nm. For emission at 730, compared to at 690 nm, approx. 30% of F_o was not affected by non-photochemical quenching processes in leaves of C3 plants; in maize leaves this was found to be approx. 50%. The data indicate that a substantial proportion of the pigments contributing to F_o emission at 730 nm are not quenched by light-induced, non-photochemical quenching processes and that there are large differences in the pigment matrices contributing to F_o and F_v emissions at 730 nm, compared to those at 690 nm. These findings have important implications for the accurate estimation and interpretation of non-photochemical quenching of fluorescence parameters and their use in the calculation of photochemical efficiencies in leaves. Measurements of fluorescence emissions at wavelengths above 700 nm are likely to give rise to significant errors when used for determinations of photochemical and non-photochemical quenching parameters.     

Energy transfer in the photochemical apparatus of flashed bean leaves

Fluorescence and energy transfer properties of bean leaves greened by brief, repetitive xenon flashes were studied at −196 °C. The bleaching of P-700 has no influence on the yield of fluorescence at any wavelength of emission. The light-induced fluorescence yield changes which are observed in both the 690 and 730 nm emission bands in the low temperature fluorescence spectra are due to changes in the state of the Photosystem II reaction centers. The fluorescence yield changes in the 730 nm band are attributed to energy transfer from Photosystem II to Photosystem I. Such energy transfer was also confirmed by measurements of the rate of photooxidation of P-700 at −196 °C in leaves in which the Photosystem II reaction centers were either all open or all closed. It is concluded that energy transfer from Photosystem II to Photosystem I occurs in the flashed bean leaves which lack the light-harvesting chlorophyll a/b protein.     

Polarized photoacoustic, absorption and fluorescence spectra of chloroplasts and thylakoids oriented in polyvinyl alcohol films

The polarized photoacoustic, absorption and fluorescence spectra of chloroplasts and thylakoids in unstretched and stretched polyvinyl alcohol films were measured. The intensity ratios of fluorescence bands at 674 nm, 700 nm, 730 nm and 750 nm, and the polarized fluorescence excitation spectra are strongly dependent on light polarization and film stretching. In stretched films, thylakoids exhibit predominantly 674 nm emission. The ratio of photoacoustic signal to absorption is different for light polarized parallel and perpendicular to film stretching. This difference is large in the region of chlorophyll a and carotenoids absorption in which the fluorescence excitation spectra are also strongly dependent on light polarization and film stretching. The observed spectral changes are explained by reorientation of pigment molecules influencing the yield of excitation transfer between different pigments.     

Qualitative changes in the fluorescence spectra of intact pea leaves after photoinhibition

In high light (1400 W m-2) treated, intact pea leaves, a decrease in the ratio of fluorescence emission at 685 to 730 nm and an increase in fluorescence intensity between 500 and 600 nm were observed. Furthermore, photoacoustically monitored heat emission increased slightly, and O2 evolution decreased significantly. These findings are interpreted as effects of a photoprotective mechanism separating the carotenoid pool from the chlorophylls. This is supported by fluorescence excitation measurements and the results of a study on the reversibility of the process.     

褐藻77 K荧光特异性研究

测定了裙带菜、叉开网地藻、海带、囊藻、海蒿子、鼠尾藻、萱藻和水云等8种褐藻的77K荧光光谱并同菠菜和红藻条斑紫菜作了比较。结果表明与红藻和高等植物明显不同,褐藻没有作为PSⅠ特征的730 nm荧光峰。按荧光主峰的波长,可以分为二种类型：裙带菜、叉开网地藻、海带和囊藻的荧光主峰位于690 nm,海蒿子、萱藻、水云和鼠尾藻的荧光主峰在705-720 nm。这种77K荧光特异性预示褐藻同高等植物之间在PSⅠ结构上的差异。